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Aniello Mennella


aniello.mennella@fisica.unimi.it

Books

2004
A Mennella, C Baccigalupi, A Balbi, M Bersanelli, C Burigana, C Butler, B Cappellini, G De Gasperis, F Hansen, D Maino, N Mandolesi, M Maris, G Morgante, P Natoli, F Pasian, F Perrotta, P Platania, L Valenziano, F Villa, A Zacchei (2004)  Imaging the First Light : experimental challenges and future perspectives in the observation of the Cosmic Microwave Background Anisotropy   KERALA – IND: Research Signpost  
Abstract: Measurements of the cosmic microwave background (CMB) allow high precision observation of the Last Scattering Surface at redshift $z\sim$1100. After the success of the NASA satellite COBE, that in 1992 provided the first detection of the CMB anisotropy, results from many ground-based and balloon-borne experiments have showed a remarkable consistency between different results and provided quantitative estimates of fundamental cosmological properties. During 2003 the team of the NASA WMAP satellite has released the first improved full-sky maps of the CMB since COBE, leading to a deeper insight into the origin and evolution of the Universe. The ESA satellite Planck, scheduled for launch in 2007, is designed to provide the ultimate measurement of the CMB temperature anisotropy over the full sky, with an accuracy that will be limited only by astrophysical foregrounds, and robust detection of polarisation anisotropy. In this paper we review the experimental challenges in high precision CMB experiments and discuss the future perspectives opened by second and third generation space missions like WMAP and Planck.
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Journal articles

2011
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, C M Cantalupo, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, Y Doi, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, E Falgarone, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, N Ikeda, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, Y Kitamura, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, J Malinen, N Mandolesi, R Mann, M Maris, D J Marshall, P Martin, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, A Melchiorri, L Mendes, A Mennella, C Meny, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, F Nati, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, L Pagani, F Pajot, R Paladini, F Pasian, G Patanchon, V -M Pelkonen, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, V Toth, M Tristram, J Tuovinen, G Umana, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, N Ysard, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XXII. The submillimetre properties of a sample of Galactic cold clumps   Astronomy & Astrophysics 536: A22 December  
Abstract: (abridged) We perform a detailed investigation of sources from the Cold Cores Catalogue of Planck Objects (C3PO). Our goal is to probe the reliability of the detections, validate the separation between warm and cold dust emission components, provide the first glimpse at the nature, internal morphology and physical characterictics of the Planck-detected sources. We focus on a sub-sample of ten sources from the C3PO list, selected to sample different environments, from high latitude cirrus to nearby (150pc) and remote (2kpc) molecular complexes. We present Planck surface brightness maps and derive the dust temperature, emissivity spectral index, and column densities of the fields. With the help of higher resolution Herschel and AKARI continuum observations and molecular line data, we investigate the morphology of the sources and the properties of the substructures at scales below the Planck beam size.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, T M Dame, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, K Dobashi, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, E Falgarone, F Finelli, O Forni, P Fosalba, M Frailis, E Franceschi, Y Fukui, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, I A Grenier, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, A Kawamura, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, P Martin, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, T Onishi, S Osborne, F Pajot, R Paladini, D Paradis, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XIX. All-sky temperature and dust optical depth from Planck and IRAS. Constraints on the “dark gas” in our Galaxy   Astronomy & Astrophysics 536: A19 December  
Abstract: We construct an all-sky map of the apparent temperature and optical depth of thermal dust emission using the Planck-HFI and IRAS data. The optical depth maps are correlated to tracers of the atomic and molecular gas. The correlation is linear in the lowest column density regions at high galactic latitudes. At high NH, the correlation is consistent with that of the lowest NH. In the intermediate NH range, we observe departure from linearity, with the dust optical depth in excess to the correlation. We attribute this excess emission to thermal emission by dust associated with a Dark-Gas phase, undetected in the available HI and CO measurements. We show the 2D spatial distribution of the Dark-Gas in the solar neighborhood and show that it extends around known molecular regions traced by CO. The average dust emissivity in the HI phase in the solar neighborhood follows roughly a power law distribution with beta = 1.8 all the way down to 3 mm, although the SED flattens slightly in the millimetre. The threshold for the existence of the Dark-Gas is found at NH = (8.0$$pm 0.58) 10\^$$20$$ Hcm-2. Assuming the same dust emissivity at high frequencies for the dust in the atomic and molecular phases leads to an average XCO = (2.54$$pm0.13) 10\^$$20$$ H2cm-2/(K km s-1). The mass of Dark-Gas is found to be 28% of the atomic gas and 118% of the CO emitting gas in the solar neighborhood. A possible origin for the Dark-Gas is the existence of a dark molecular phase, where H2 survives photodissociation but CO does not. The observed transition for the onset of this phase in the solar neighborhood (AV = 0.4 mag) appears consistent with recent theoretical predictions. We also discuss the possibility that up to half of the Dark-Gas could be in atomic form, due to optical depth effects in the HI measurements.
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Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, C M Cantalupo, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, L -Y Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, K Dobashi, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, E Falgarone, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, G Joncas, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, N Mandolesi, R Mann, M Maris, D J Marshall, P Martin, E MartĂ­nez-González, G Marton, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, A Melchiorri, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, F Nati, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, R Paladini, F Pasian, G Patanchon, T J Pearson, V -M Pelkonen, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, V Toth, M Tristram, J Tuovinen, G Umana, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, N Ysard, D Yvon, A Zacchei, S Zahorecz, A Zonca (2011)  Planck early results. XXIII. The first all-sky survey of Galactic cold clumps   Astronomy & Astrophysics 536: A23 December  
Abstract: We present the statistical properties of the first version of the Cold Core Catalogue of Planck Objects (C3PO), in terms of their spatial distribution, temperature, distance, mass, and morphology. We also describe the statistics of the Early Cold Core Catalogue (ECC, delivered with the Early Release Compact Source Catalogue, ERCSC) that is the subset of the 915 most reliable detections of the complete catalogue. We have used the CoCoCoDeT algorithm to extract 10783 cold sources. Temperature and dust emission spectral index $$$$beta$$ values are derived using the fluxes in the IRAS 100 $$mum band and the three highest frequency Planck bands. Temperature spans from 7K to 17K, and peaks around 13K. Data are not consistent with a constant value of $$$$beta$$ over the all temperature range. $$$$beta$$ ranges from 1.4 to 2.8 with a mean value around 2.1, and several possible scenarios are possible, including $$$$beta$$(T) and the effect of multiple T components folded into the measurements. For one third of the objects the distances are obtained. Most of the detections are within 2 kpc in the Solar neighbourhood, but a few are at distances greater than 4 kpc. The cores are distributed from the deep Galactic plane, despite the confusion, to high latitudes (\gt30$\^$$$$circle$$$). The associated mass estimates range from 1 to $10\^5$ solar masses. Using their physical properties these cold sources are shown to be cold clumps, defined as the intermediate cold sub-structures between clouds and cores. These cold clumps are not isolated but mostly organized in filaments associated with molecular clouds. The Cold Core Catalogue of Planck Objects (C3PO) is the first unbiased all-sky catalogue of cold objects. It gives an unprecedented statistical view to the properties of these potential pre-stellar clumps and offers a unique possibility for their classification in terms of their intrinsic properties and environment.
Notes:
Planck Collaboration, A Abergel, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, T M Dame, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, I A Grenier, A Gruppuso, F K Hansen, D Harrison, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, T R Jaffe, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, N Mandolesi, R Mann, M Maris, D J Marshall, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, R Paladini, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, R Rebolo, W Reich, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, N Ysard, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XXI. Properties of the interstellar medium in the Galactic plane   Astronomy & Astrophysics 536: A21 December  
Abstract: This paper presents the first results of comparison of Planck along with IRAS data with Green Bank Telescope 21 cm observations in 14 fields covering more than 800 square degrees at high Galactic latitude. Galactic dust emission for fields with average column density lower than 2 x 10\^20 cm\^-2 is well correlated with 21 cm emission. The residual emission in these fields, once the HI-correlated emission is removed, is consistent with the expected statistical properties of the cosmic infrared background fluctuations. Fields with larger average column densities show significant excess dust emission compared to the HI column density. Regions of excess lie in organized structures that suggest the presence of hydrogen in molecular form, though they are not always correlated with CO emission. Dust emission from intermediate-velocity clouds is detected by this correlation analysis with high significance. Its spectral properties are consistent with, compared to the local ISM values, significantly hotter dust (T ~ 20 K), lower emission cross-section and a relative abundance of very small grains to large grains about four times higher. These results are consistent with expectations for clouds that are part of the Galactic fountain in which there is dust shattering and fragmentation. Correlated dust emission in high-velocity clouds is detected only marginally at the 1 to 3.5 sigma level. It has a dust emissivity a factor of ten lower compared to the local ISM, in accordance with the lower metallicity of these clouds. Unexpected anti-correlated variations of the dust temperature and emission cross section per H atom are identified in the local ISM and IVCs, a trend that continues into molecular environments. This suggests that dust growth through aggregation, seen in molecular clouds and then in circumstellar disks, is active much earlier in the cloud condensation and star formation processes.
Notes:
Aniello Mennella (2011)  The microwave sky after one year of Planck operations   arXiv:1110.2051v1  
Abstract: The ESA Planck satellite, launched on May 14th, 2009, is the third generation space mission dedicated to the measurement of the Cosmic Microwave Background (CMB), the first light in the Universe. Planck observes the full sky in nine frequency bands from 30 to 857 GHz and is designed to measure the CMB anisotropies with an unprecedented combination of sensitivity, angular resolution and control of systematic effects. In this presentation we summarise the Planck instruments performance and discuss the main scientific results obtained after one year of operations in the fields of galactic and extragalactic astrophysics.
Notes: Invited presentation at the 13th ICATPP Conference on Astroparticle, Particle, Space Physics and Detectors for Physics Applications (Villa Olmo, Como 3-7 October 2011)
Planck Collaboration, A Abergel, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, K Blagrave, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, C M Cantalupo, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, G Joncas, A Jones, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, M Linden-Vørnle, F J Lockman, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, D J Marshall, P Martin, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, F Nati, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, R Paladini, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, D Pinheiro Gonçalves, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XXIV. Dust in the diffuse interstellar medium and the Galactic halo   Astronomy & Astrophysics 536: A24 December  
Abstract: This paper presents the first results from a comparison of Planck dust maps at 353, 545 and 857GHz, along with IRAS data at 3000 (100 μm) and 5000GHz (60 μm), with Green Bank Telescope 21-cm observations of Hi in 14 fields covering more than 800deg2 at high Galactic latitude. The main goal of this study is to estimate the far-infrared to sub-millimeter (submm) emissivity of dust in the diffuse local interstellar medium (ISM) and in the intermediate-velocity (IVC) and high-velocity clouds (HVC) of the Galactic halo. Galactic dust emission for fields with average Hi column density lower than 2 × 1020 cm-2 is well correlated with 21-cm emission because in such diffuse areas the hydrogen is predominantly in the neutral atomic phase. The residual emission in these fields, once the Hi-correlated emission is removed, is consistent with the expected statistical properties of the cosmic infrared background fluctuations. The brighter fields in our sample, with an average Hi column density greater than 2 × 1020 cm-2, show significant excess dust emission compared to the Hi column density. Regions of excess lie in organized structures that suggest the presence of hydrogen in molecular form, though they are not always correlated with CO emission. In the higher Hi column density fields the excess emission at 857 GHz is about 40% of that coming from the Hi, but over all the high latitude fields surveyed the molecular mass faction is about 10%. Dust emission from IVCs is detected with high significance by this correlation analysis. Its spectral properties are consistent with, compared to the local ISM values, significantly hotter dust (T ~ 20 K), lower submm dust opacity normalized per H-atom, and a relative abundance of very small grains to large grains about four times higher. These results are compatible with expectations for clouds that are part of the Galactic fountain in which there is dust shattering and fragmentation. Correlated dust emission in HVCs is not detected; the average of the 99.9% confidence upper limits to the emissivity is 0.15 times the local ISM value at 857 and 3000GHz, in accordance with gas phase evidence for lower metallicity and depletion in these clouds. Unexpected anti-correlated variations of the dust temperature and emission cross-section per H atom are identified in the local ISM and IVCs, a trend that continues into molecular environments. This suggests that dust growth through aggregation, seen in molecular clouds, is active much earlier in the cloud condensation and star formation processes.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, B Cappellini, J -F Cardoso, S Casassus, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, X Chen, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, C Dickinson, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, T R Jaffe, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, D J Marshall, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, R Paladini, B Partridge, F Pasian, G Patanchon, T J Pearson, M Peel, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, P Procopio, S Prunet, J -L Puget, W T Reach, R Rebolo, W Reich, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, J Varis, L Verstraete, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, R Watson, A Wilkinson, N Ysard, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XX. New light on anomalous microwave emission from spinning dust grains   Astronomy & Astrophysics 536: A20 December  
Abstract: Anomalous microwave emission (AME) has been observed by numerous experiments in the frequency range ~10-60 GHz. Using Planck maps and multi-frequency ancillary data, we have constructed spectra for two known AME regions: the Perseus and Rho Ophiuchus molecular clouds. The spectra are well fitted by a combination of free-free radiation, cosmic microwave background, thermal dust, and electric dipole radiation from small spinning dust grains. The spinning dust spectra are the most precisely measured to date, and show the high frequency side clearly for the first time. The spectra have a peak in the range 20-40 GHz and are detected at high significances of 17.1sigma and 10.4sigma, respectively. In Perseus, spinning dust in the dense molecular gas can account for most of the AME; the low density neutral gas appears to play a minor role. In Rho Ophiuchus, the ~30 GHz peak is dominated by dense molecular gas, but there is an indication of an extended tail at frequencies 50-100 GHz, which can be accounted for by irradiated low density atomic gas. The dust parameters are consistent with those derived from other measurements. We have also searched the Planck map at 28.5 GHz for candidate AME regions, by subtracting a simple model of the synchrotron, free-free, and thermal dust. We present spectra for two of the candidates: bright HII regions that show evidence for AME, and are well fitted by spinning dust models.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, L -Y Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, S Madden, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, B Partridge, F Pasian, G Patanchon, M Peel, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, M TĂĽrler, G Umana, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XVI. The Planck view of nearby galaxies   Astronomy & Astrophysics 536: A16 December  
Abstract: The all-sky coverage of the Planck Early Release Compact Source Catalogue (ERCSC) provides an unsurpassed survey of galaxies at submillimetre (submm) wavelengths, representing a major improvement in the numbers of galaxies detected, as well as the range of far-IR/submm wavelengths over which they have been observed. We here present the first results on the properties of nearby galaxies using these data. We match the ERCSC catalogue to IRAS-detected galaxies in the Imperial IRAS Faint Source Redshift Catalogue (IIFSCz), so that we can measure the spectral energy distributions (SEDs) of these objects from 60 to 850 microns. This produces a list of 1717 galaxies with reliable associations between Planck and IRAS, from which we select a subset of 468 for SED studies, namely those with strong detections in the three highest frequency Planck bands and no evidence of cirrus contamination. The SEDs are fitted using parametric dust models to determine the range of dust temperatures and emissivities. We find evidence for colder dust than has previously been found in external galaxies, with T\lt20K. Such cold temperatures are found using both the standard single temperature dust model with variable emissivity beta, or a two dust temperature model with beta fixed at 2. We also compare our results to studies of distant submm galaxies (SMGs) which have been claimed to contain cooler dust than their local counterparts. We find that including our sample of 468 galaxies significantly reduces the distinction between the two populations. Fits to SEDs of selected objects using more sophisticated templates derived from radiative transfer models confirm the presence of the colder dust found through parameteric fitting. We thus conclude that cold (T\lt20K) dust is a significant and largely unexplored component of many nearby galaxies.
Notes:
Planck Collaboration, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, M L Brown, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, L -Y Chiang, C Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, J M Diego, K Dolag, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, I Flores-Cacho, O Forni, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, R Piffaretti, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, B M Schaefer, D Scott, M D Seiffert, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sunyaev, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, B D Wandelt, S D M White, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. X. Statistical analysis of Sunyaev-Zeldovich scaling relations for X-ray galaxy clusters   Astronomy & Astrophysics 536: A10 December  
Abstract: All-sky data from the Planck survey and the Meta-Catalogue of X-ray detected Clusters of galaxies (MCXC) are combined to investigate the relationship between the thermal Sunyaev-Zeldovich (SZ) signal and X-ray luminosity. The sample comprises ~ 1600 X-ray clusters with redshifts up to ~ 1 and spanning a wide range in X-ray luminosity. The SZ signal is extracted for each object individually and the statistical significance of the measurement is maximised by averaging the SZ signal in bins of X-ray luminosity, total mass or redshift. The SZ signal is detected at very high significance over more than 2 decades in X-ray luminosity (10\^43 erg/s \lt L_500 E(z)\^-7/3 \lt 2 X 10\^45 erg/s). The relation between intrinsic SZ signal and X-ray luminosity is investigated and the measured SZ signal is compared to values predicted from X-ray data. Planck measurements and X-ray based predictions are found to be in excellent agreement over the whole explored luminosity range. No significant deviation from standard evolution of the scaling relations is detected. For the first time the intrinsic scatter in the scaling relation between SZ signal and X-ray luminosity is measured and found to be consistent with the one in the luminosity - mass relation from X-ray studies. There is no evidence for a deficit in SZ signal strength in Planck data relative to expectations from the X-ray properties of clusters, underlining the robustness and consistency of our overall view of intra-cluster medium properties.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, F ArgĂĽeso, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, J -P Bernard, M Bersanelli, R Bhatia, A Bonaldi, L Bonavera, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, P Cabella, B Cappellini, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, X Chen, L -Y Chiang, P R Christensen, D L Clements, S Colafrancesco, S Colombi, F Couchot, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, A Lasenby, R J Laureijs, C R Lawrence, S Leach, J P Leahy, R Leonardi, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, B Maffei, M Magliocchetti, D Maino, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, M Massardi, S Matarrese, F Matthai, P Mazzotta, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, R Paladini, B Partridge, F Pasian, G Patanchon, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, R Rebolo, M Reinecke, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, A Sajina, M Sandri, D Scott, M D Seiffert, S Serjeant, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, M TĂĽrler, G Umana, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XIII. Statistical properties of extragalactic radio sources in the Planck Early Release Compact Source Catalogue   Astronomy & Astrophysics 536: A13 December  
Abstract: The data reported in Planck’s Early Release Compact Source Catalogue (ERCSC) are exploited to measure the number counts (dN/dS) of extragalactic radio sources at 100, 143 and 217 GHz. Due to the full-sky nature of the catalogue, this measurement extends to the rarest and brightest sources in the sky. At lower frequencies (30, 44, and 70 GHz) our counts are in very good agreement with estimates based on WMAP data, being somewhat deeper at 30 and 70 GHz, and somewhat shallower at 44 GHz. Planck’s source counts at 143 and 217 GHz join smoothly with the fainter ones provided by the SPT and ACT surveys over small fractions of the sky. An analysis of source spectra, exploiting Planck’s uniquely broad spectral coverage, finds clear evidence of a steepening of the mean spectral index above about 70 GHz. This implies that, at these frequencies, the contamination of the CMB power spectrum by radio sources below the detection limit is significantly lower than previously estimated.
Notes:
Planck Collaboration, A Abergel, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, K Dobashi, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, V Guillet, F K Hansen, D Harrison, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, A Jones, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, N Mandolesi, R Mann, M Maris, D J Marshall, P Martin, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, R Paladini, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, L Verstraete, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XXV. Thermal dust in nearby molecular clouds   Astronomy & Astrophysics 536: A25 December  
Abstract: Planck allows unbiased mapping of Galactic sub-millimetre and millimetre emission from the most diffuse regions to the densest parts of molecular clouds. We present an early analysis of the Taurus molecular complex, on line-of-sight-averaged data and without component separation. The emission spectrum measured by Planck and IRAS can be fitted pixel by pixel using a single modified blackbody. Some systematic residuals are detected at 353 GHz and 143 GHz, with amplitudes around â’7% and +13%, respectively, indicating that the measured spectra are likely more complex than a simple modified blackbody. Significant positive residuals are also detected in the molecular regions and in the 217 GHz and 100 GHz bands, mainly caused by the contribution of the J = 2 → 1 and J = 1 → 0 12CO and 13CO emission lines. We derive maps of the dust temperature T, the dust spectral emissivity index β, and the dust optical depth at 250 μm Ï„250. The temperature map illustrates the cooling of the dust particles in thermal equilibrium with the incident radiation field, from 16 â’ 17 K in the diffuse regions to 13 â’ 14 K in the dense parts. The distribution of spectral indices is centred at 1.78, with a standard deviation of 0.08 and a systematic error of 0.07. We detect a significant T ⒠β anti-correlation. The dust optical depth map reveals the spatial distribution of the column density of the molecular complex from the densest molecular regions to the faint diffuse regions. We use near-infrared extinction and Hi data at 21-cm to perform a quantitative analysis of the spatial variations of the measured dust optical depth at 250 μm per hydrogen atom Ï„250/NH. We report an increase of Ï„250/NH by a factor of about 2 between the atomic phase and the molecular phase, which has a strong impact on the equilibrium temperature of the dust particles.
Notes:
Planck Collaboration, N Aghanim, M Arnaud, M Ashdown, F Atrio-Barandela, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, H Böhringer, A Bonaldi, J R Bond, S Borgani, J Borrill, F R Bouchet, M L Brown, C Burigana, P Cabella, C M Cantalupo, B Cappellini, P Carvalho, A Catalano, L CayĂłn, L -Y Chiang, C Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, O D ’Arcangelo, R J Davis, P de Bernardis, G de Gasperis, G de Zotti, J Delabrouille, J -M Delouis, J DĂ©moclès, F -X DĂ©sert, C Dickinson, J M Diego, H Dole, S Donzelli, O DorĂ©, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, I Flores-Cacho, O Forni, P Fosalba, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, J González-Nuevo, R González-Riestra, K M GĂłrski, A Gregorio, A Gruppuso, F K Hansen, D Harrison, P Heinämäki, C Hernández-Monteagudo, S R Hildebrandt, E Hivon, M Hobson, G Hurier, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, C R Lawrence, M Le Jeune, S Leach, R Leonardi, C Leroy, A Liddle, P B Lilje, M LĂłpez-Caniego, G Luzzi, J F MacĂ­as-PĂ©rez, D Maino, N Mandolesi, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, P Mazzotta, P R Meinhold, A Melchiorri, J -B Melin, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, P Naselsky, P Natoli, J Nevalainen, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, R Paladini, F Pasian, G Patanchon, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, E Pierpaoli, R Piffaretti, P Platania, E Pointecouteau, G Polenta, N Ponthieu, L Popa, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, J A Rubiño-MartĂ­n, E Saar, M Sandri, G Savini, B M Schaefer, D Scott, G F Smoot, J -L Starck, D Sutton, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, M Tristram, M TĂĽrler, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, J Weller, S D M White, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XXVI. Detection with Planck and confirmation by XMM-Newton of PLCK G266.6–27.3, an exceptionally X-ray luminous and massive galaxy cluster at z ~ 1   Astronomy & Astrophysics A26. December  
Abstract: We present first results on PLCK G266.6-27.3, a galaxy cluster candidate detected at a signal-to-noise ratio of 5 in the Planck All Sky survey. An XMM-Newton validation observation has allowed us to confirm that the candidate is a bona fide galaxy cluster. With these X-ray data we measure an accurate redshift, z = 0.94 +/- 0.02, and estimate the cluster mass to be M_500 = (7.8 +/- 0.8)e+14 solar masses. PLCK G266.6-27.3 is an exceptional system: its luminosity of L_X(0.5-2.0 keV)=(1.4 +/- 0.05)e+45 erg/s, equals that of the two most luminous known clusters in the z > 0.5 universe, and it is one of the most massive clusters at z~1. Moreover, unlike the majority of high-redshift clusters, PLCK G266.6-27.3 appears to be highly relaxed. This observation confirms Planck's capability of detecting high-redshift, high-mass clusters, and opens the way to the systematic study of population evolution in the exponential tail of the mass function.
Notes:
F de Gasperin, A Mennella, D Maino, L Terenzi, S Galeotta, B Cappellini, G Morgante, M Tomasi, M Bersanelli, N Mandolesi, A Zacchei (2011)  Effect of Fourier filters in removing periodic systematic effects from CMB data   Astronomy & Astrophysics 529: A141 May  
Abstract: We consider the application of high-pass Fourier filters to remove periodic systematic fluctuations from full-sky survey CMB datasets. We compare the filter performance with destriping codes commonly used to remove the effect of residual 1/f noise from timelines. As a realistic working case, we use simulations of the typical Planck scanning strategy and Planck Low Frequency Instrument noise performance, with spurious periodic fluctuations that mimic a typical thermal disturbance. We show that the application of Fourier high-pass filters in chunks always requires subsequent normalisation of induced offsets by means of destriping. For a complex signal containing all the astrophysical and instrumental components, the result obtained by applying filter and destriping in series is comparable to the result obtained by destriping only, which makes the usefulness of Fourier filters questionable for removing this kind of effects.
Notes:
Planck Collaboration, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, M L Brown, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, J M Diego, K Dolag, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, I Flores-Cacho, O Forni, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, S Mei, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, R Piffaretti, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, R Sunyaev, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, B D Wandelt, S D M White, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XII. Cluster Sunyaev-Zeldovich optical scaling relations   Astronomy & Astrophysics 536: A12 December  
Abstract: We present the Sunyaev-Zeldovich (SZ) signal-to-richness scaling relation (Y500-N200) for the MaxBCG cluster catalogue. Employing a multi-frequency matched filter on the Planck sky maps, we measure the SZ signal for each cluster by adapting the filter according to weak-lensing calibrated mass-richness relations (N200-M500). We bin our individual measurements and detect the SZ signal down to the lowest richness systems (N200=10) with high significance, achieving a detection of the SZ signal in systems with mass as low as M500~5e13 Msolar. The observed Y500-N200 relation is well modeled by a power law over the full richness range. It has a lower normalisation at given N200 than predicted based on X-ray models and published mass-richness relations. An X-ray subsample, however, does conform to the predicted scaling, and model predictions do reproduce the relation between our measured bin-average SZ signal and measured bin-average X-ray luminosities. At fixed richness, we find an intrinsic dispersion in the Y500-N200 relation of 60% rising to of order 100% at low richness. Thanks to its all-sky coverage, Planck provides observations for more than 13,000 MaxBCG clusters and an unprecedented SZ/optical data set, extending the list of known cluster scaling laws to include SZ-optical properties. The data set offers essential clues for models of galaxy formation. Moreover, the lower normalisation of the SZ-mass relation implied by the observed SZ-richness scaling has important consequences for cluster physics and cosmological studies with SZ clusters.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, H Bourdin, M L Brown, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, J M Diego, K Dolag, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, I Flores-Cacho, O Forni, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, J Lanoux, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, A Liddle, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, R Piffaretti, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, R Sunyaev, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, S D M White, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XI. Calibration of the local galaxy cluster Sunyaev-Zeldovich scaling relations   Astronomy & Astrophysics 536: A11 December  
Abstract: We present precise Sunyaev-Zeldovich (SZ) effect measurements in the direction of 62 nearby galaxy clusters (z \lt0.5) detected at high signal-to-noise in the first Planck all-sky dataset. The sample spans approximately a decade in total mass, 10\^14 \lt M_500 \lt 10\^15, where M_500 is the mass corresponding to a total density contrast of 500. Combining these high quality Planck measurements with deep XMM-Newton X-ray data, we investigate the relations between D_A\^2 Y_500, the integrated Compton parameter due to the SZ effect, and the X-ray-derived gas mass M_g,500, temperature T_X, luminosity L_X, SZ signal analogue Y_X,500 = M_g,500 * T_X, and total mass M_500. After correction for the effect of selection bias on the scaling relations, we find results that are in excellent agreement with both X-ray predictions and recently-published ground-based data derived from smaller samples. The present data yield an exceptionally robust, high-quality local reference, and illustrate Planck’s unique capabilities for all-sky statistical studies of galaxy clusters.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, K Blagrave, J J Bock, A Bonaldi, L Bonavera, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, P Fosalba, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, J Grain, S Gratton, A Gregorio, A Gruppuso, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, P B Lilje, M Linden-Vørnle, F J Lockman, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, P Martin, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, A Melchiorri, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, D Novikov, I Novikov, I J O’Dwyer, S Oliver, S Osborne, F Pajot, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, D Pinheiro Gonçalves, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, M Reinecke, M Remazeilles, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, R Sunyaev, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XVIII. The power spectrum of cosmic infrared background anisotropies   Astronomy & Astrophysics 536: A18 December  
Abstract: Using Planck maps of six regions of low Galactic dust emission with a total area of about 140 square degrees, we determine the angular power spectra of Cosmic Infrared Background (CIB) anisotropies from multipole l = 200 to l = 2000 at 217, 353, 545 and 857 GHz. We use observations of HI emission as a tracer of thermal dust emission in order to reduce the already low level of Galactic dust emission and use the 143 GHz Planck maps in these fields to clean out cosmic microwave background anisotropies. Both of these cleaning processes are necessary in order to avoid significant contamination of the CIB signal. We measure correlated CIB structure across frequencies. As expected, the correlation decreases with increasing frequency separation as the contribution of high-redshift galaxies to CIB anisotropies increases with wavelengths. We find no significant difference between the frequency spectrum of the CIB anisotropies and the CIB mean, with dI/I=15% from 217 to 857 GHz. In terms of clustering properties, the Planck data alone ruled out the linear scale- and redshift- independent bias model. Non-linear corrections are important. Consequently, we develop an alternative model that couples a dusty galaxy, parametric evolution model with a simple halo model approach. It provides an excellent fit to the measured anisotropy angular power spectra and suggests that a different halo occupation distribution is required at each frequency, which is consistent with the fact that we expect each frequency to be dominated by contributions from different redshifts. In our best-fit model, half of the anisotropies power at l=2000 comes from redshifts z\lt0.8 at 857 GHz and z\lt0.9 at 545 GHz, while about 1/5 and 2/3 come from redshifts z\gt3.5 at 353 and 217 GHz, respectively.
Notes:
Planck Collaboration, J Aatrokoski, P A R Ade, N Aghanim, H D Aller, M F Aller, E Angelakis, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, A Berdyugin, J -P Bernard, M Bersanelli, R Bhatia, A Bonaldi, L Bonavera, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, D N Burrows, P Cabella, M Capalbi, B Cappellini, J -F Cardoso, A Catalano, E Cavazzuti, L CayĂłn, A Challinor, A Chamballu, R -R Chary, L -Y Chiang, P R Christensen, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, S Cutini, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, C Dickinson, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, O Forni, M Frailis, E Franceschi, L Fuhrmann, S Galeotta, K Ganga, F Gargano, D Gasparrini, N Gehrels, M Giard, G Giardino, N Giglietto, P Giommi, F Giordano, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, M Juvela, E Keihänen, R Keskitalo, O King, T S Kisner, R Kneissl, L Knox, T P Krichbaum, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, N Lavonen, C R Lawrence, S Leach, R Leonardi, J LeĂłn-Tavares, M Linden-Vørnle, E Lindfors, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, M Massardi, S Matarrese, F Matthai, W Max-Moerbeck, M N Mazziotta, P Mazzotta, A Melchiorri, L Mendes, A Mennella, P F Michelson, M Mingaliev, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, C Monte, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, I Nestoras, C B Netterfield, E Nieppola, K Nilsson, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, B Partridge, F Pasian, G Patanchon, V Pavlidou, T J Pearson, O Perdereau, L Perotto, M Perri, F Perrotta, F Piacentini, M Piat, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, P Procopio, S Prunet, J -L Puget, J P Rachen, S Rainò, W T Reach, A Readhead, R Rebolo, R Reeves, M Reinecke, R Reinthal, C Renault, S Ricciardi, J Richards, T Riller, D Riquelme, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, J Saarinen, M Sandri, P Savolainen, D Scott, M D Seiffert, A Sievers, A Sillanpää, G F Smoot, Y Sotnikova, J -L Starck, M Stevenson, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, L Takalo, J Tammi, J A Tauber, L Terenzi, D J Thompson, L Toffolatti, M Tomasi, M Tornikoski, J -P Torre, G Tosti, A Tramacere, M Tristram, J Tuovinen, M TĂĽrler, M Turunen, G Umana, H Ungerechts, L Valenziano, E Valtaoja, J Varis, F Verrecchia, P Vielva, F Villa, N Vittorio, B D Wandelt, J Wu, D Yvon, A Zacchei, J A Zensus, X Zhou, A Zonca (2011)  Planck early results. XV. Spectral energy distributions and radio continuum spectra of northern extragalactic radio sources   Astronomy & Astrophysics 536: A15 December  
Abstract: Spectral energy distributions (SEDs) and radio continuum spectra are presented for a northern sample of 104 extragalactic radio sources, based on the Planck Early Release Compact Source Catalog (ERCSC) and simultaneous multifrequency data. The nine Planck frequencies, from 30 to 857 GHz, are complemented by a set of simultaneous observations ranging from radio to gamma-rays. This is the first extensive frequency coverage in the radio and millimetre domains for an essentially complete sample of extragalactic radio sources, and it shows how the individual shocks, each in their own phase of development, moving in the relativistic jet, shape the radio spectra. The SEDs presented in this paper were fitted with second and third degree polynomials to estimate the frequencies of the synchrotron and inverse Compton (IC) peaks, and the spectral indices of low and high frequency radio data, including the Planck ERCSC data, were calculated. SED modelling methods are discussed, with an emphasis on proper, physical modelling of the synchrotron bump using multiple components. Planck ERCSC data also suggest that the original accelerated electron energy spectrum could be much harder than commonly thought, with power-law index s around 1.5 instead of the canonical 2.5. The implications of this for the acceleration mechanisms effective in blazar shocks are discussed.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, C Bot, F R Bouchet, F Boulanger, M Bucher, C Burigana, P Cabella, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, K Dobashi, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, O Forni, M Frailis, E Franceschi, Y Fukui, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, G Helou, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, W C Jones, M Juvela, A Kawamura, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, R Leonardi, C Leroy, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, S Madden, B Maffei, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, F Nati, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, T Onishi, S Osborne, F Pajot, R Paladini, D Paradis, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, G Savini, D Scott, M D Seiffert, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, G Umana, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, N Ysard, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. XVII. Origin of the submillimetre excess dust emission in the Magellanic Clouds   Astronomy & Astrophysics 536: A17 December  
Abstract: The integrated Spectral Energy Distributions of the Large and Small Magellanic Cloud appear significantly flatter than expected from dust models based on their FIR and radio emission. The origin of this millimetre excess is still unexplained, and is here investigated using the Planck data. The background CMB contribution is subtracted using an ILC method performed locally around the galaxies. The foreground emission from the Milky Way is subtracted. After subtraction, the emission of both galaxies correlates closely with the gas emission of the LMC and SMC. The millimetre excess in the LMC can be explained by CMB fluctuations, but a significant excess is still present in the SMC SED. The Planck and IRIS data at 100 micron are combined to produce thermal dust temperature and optical depth maps of the two galaxies. The LMC temperature map shows the presence of a warm inner arm already found with the Spitzer data, but also shows the existence of a previously unidentified cold outer arm. Several cold regions are found along this arm, some of which are associated with known molecular clouds. The average emissivity spectral index is found to be consistent with beta=1.5 and beta=1.2 below 500 microns for the LMC and SMC respectively, significantly flatter than the values observed in the Milky Way. Furthermore, there is evidence in the SMC for a further flattening of the SED in the sub-mm. The spatial distribution of the millimetre dust excess in the SMC follows the gas and thermal dust distribution. Different models are explored in order to fit the dust emission in the SMC. It is concluded that the millimetre excess is unlikely to be caused by very cold dust emission and that it could be due to a combination of spinning dust. emission and thermal dust emission by more amorphous dust grains than those present in our Galaxy.
Notes:
Planck Collaboration, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, M L Brown, M Bucher, C Burigana, P Cabella, C M Cantalupo, J -F Cardoso, P Carvalho, A Catalano, L CayĂłn, A Challinor, A Chamballu, L -Y Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, J M Diego, K Dolag, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, I Flores-Cacho, O Forni, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, R González-Riestra, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, P Heinämäki, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, G Hurier, A H Jaffe, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, M Le Jeune, S Leach, R Leonardi, A Liddle, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, F Pasian, G Patanchon, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, R Piffaretti, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, E Saar, M Sandri, D Santos, B M Schaefer, D Scott, M D Seiffert, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sunyaev, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, B D Wandelt, S D M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. IX. XMM-Newton follow-up for validation of Planck cluster candidates   Astronomy & Astrophysics 536: A9 December  
Abstract: We present the XMM-Newton follow-up for validation of Planck cluster candidates. Twenty-five candidates have been observed to date using snapshot (~10 ksec) exposures: ten as part of a pilot programme to sample a low range of signal-to-noise ratios (4\ltS/N\lt6), and a further fifteen in a programme to observe a sample of S/N\gt5 candidates. The sensitivity and spatial resolution of XMM-Newton allows unambiguous discrimination between clusters and false candidates. A total of 21 candidates are confirmed as extended X-ray sources. Seventeen are single clusters, the majority of which are found to have highly irregular and disturbed morphologies. The remaining four sources are multiple systems, including the unexpected discovery of a supercluster at z=0.45. For most of the sources we are able to derive a redshift estimate from the X-ray Fe K line (albeit of variable quality). The new clusters span the redshift range 0.09 \lt~ z \lt~ 0.54 with a median redshift of z ~ 0.37. A first estimate is made of their X-ray properties including the characteristic size, which is used to improve the SZ Compton parameter estimate. The validation programme has helped to optimise the Planck candidate selection process. It has also provided a preview of the X-ray properties of these newly-discovered clusters, allowing comparison to their SZ properties, and to the X-ray and SZ properties of known clusters observed in the Planck survey. Our results suggest that Planck may have started to reveal a non-negligible population of massive dynamically perturbed objects that is under-represented in X-ray surveys. However, despite their particular properties, these new clusters appear to follow the Ysz-Yx relation established for X-ray selected objects.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, J G Bartlett, E Battaner, R Battye, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, M L Brown, M Bucher, C Burigana, P Cabella, C M Cantalupo, J -F Cardoso, P Carvalho, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, L -Y Chiang, C Chiang, G Chon, P R Christensen, E Churazov, D L Clements, S Colafrancesco, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, A Da Silva, H Dahle, L Danese, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, J M Diego, K Dolag, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, P Eisenhardt, T A EnĂźlin, F Feroz, F Finelli, I Flores-Cacho, O Forni, P Fosalba, M Frailis, E Franceschi, S Fromenteau, S Galeotta, K Ganga, R T GĂ©nova-Santos, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, R González-Riestra, K M GĂłrski, K J B Grainge, S Gratton, A Gregorio, A Gruppuso, D Harrison, P Heinämäki, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, G Hurier, N Hurley-Walker, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, M Le Jeune, S Leach, R Leonardi, C Li, A Liddle, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, S Mei, P R Meinhold, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, F Nati, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, M Olamaie, S Osborne, F Pajot, F Pasian, G Patanchon, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, R Piffaretti, S Plaszczynski, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, E Saar, M Sandri, D Santos, R D E Saunders, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, G F Smoot, A Stanford, J -L Starck, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, R Sunyaev, D Sutton, J -F Sygnet, N Taburet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, J Weller, S D M White, M White, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. VIII. The all-sky early Sunyaev-Zeldovich cluster sample   Astronomy & Astrophysics 536: A8 December  
Abstract: We present the first all-sky sample of galaxy clusters detected blindly by the Planck satellite through the Sunyaev-Zeldovich (SZ) effect from its six highest frequencies. This Early SZ (ESZ) sample of 189 candidates comprises high signal-to-noise clusters, from 6 to 29. Its high reliability (purity above 95%) is further insured by an extensive validation process based on Planck-internal quality assessments and external cross-identification and follow-up observations. Planck provides the first measured SZ signal for about 80% of the 169 ESZ known clusters. Planck further releases 30 new cluster candidates among which 20 are within the ESZ signal-to-noise selection criterion. Eleven of these 20 ESZ candidates are confirmed using XMM-Newton snapshot observations as new clusters, most of them with disturbed morphologies and low luminosities. The ESZ clusters are mostly at moderate redshifts (86% with z below 0.3) and span over a decade in mass, up to the rarest and most massive clusters with masses above 10\^15 Msol.
Notes:
F Del Torto, M Bersanelli, F Cavaliere, A De Rosa, O D’Arcangelo, C Franceschet, M Gervasi, A Mennella, E Pagana, A Simonetto, A Tartari, F Villa, M Zannoni (2011)  W-band prototype of platelet feed-horn array for CMB polarisation measurements   Journal of Instrumentation 6: P06009 June  
Abstract: We present the design and performance of a 2x2 prototype array of corrugated feed- horns in W-band. The module is fabricated using a so-called “platelet” technique by milling Alu- minum plates. This technique is suitable for low-cost and scalable high performance applications. Room temperature Return Loss measurements show a low (< â’30 dB) reflection over a 30% band- width with a maximum matching of -42 dB at 100 GHz for all four antennas. Beam pattern mea- surements indicate good repeatability and a low (-25 dB) sidelobe and crosspolarisation levels. This work is particularly relevant for future Cosmic Microwave Background polarisation measurements, which require large microwave cryogenic detector arrays coupled to high performance corrugated feed horns.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, E Angelakis, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, A Bonaldi, L Bonavera, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, P Cabella, B Cappellini, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, X Chen, L -Y Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, F Finelli, O Forni, M Frailis, E Franceschi, L Fuhrmann, S Galeotta, K Ganga, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, D Harrison, S Henrot-VersillĂ©, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, W Hovest, R J Hoyland, K M Huffenberger, M Huynh, A H Jaffe, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, T P Krichbaum, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, N Lavonen, C R Lawrence, S Leach, J P Leahy, R Leonardi, J LeĂłn-Tavares, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, E MartĂ­nez-González, S Masi, M Massardi, S Matarrese, F Matthai, P Mazzotta, P R Meinhold, A Melchiorri, L Mendes, A Mennella, M Mingaliev, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, I Nestoras, C B Netterfield, E Nieppola, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, S Osborne, F Pajot, R Paladini, B Partridge, F Pasian, G Patanchon, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, P Procopio, S Prunet, J -L Puget, J P Rachen, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, D Riquelme, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, A Sajina, M Sandri, P Savolainen, D Scott, M D Seiffert, A Sievers, G F Smoot, Y Sotnikova, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, J -F Sygnet, J Tammi, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, M Tornikoski, J -P Torre, M Tristram, J Tuovinen, M TĂĽrler, M Turunen, G Umana, H Ungerechts, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, A Wilkinson, D Yvon, A Zacchei, J A Zensus, A Zonca (2011)  Planck early results. XIV. ERCSC validation and extreme radio sources   Astronomy & Astrophysics 536: A14 December  
Abstract: Planck’s all sky surveys at 30-857 GHz provide an unprecedented opportunity to follow the radio spectra of a large sample of extragalactic sources to frequencies 2-20 times higher than allowed by past, large area, ground-based surveys. We combine the results of the Planck Early Release Compact Source Catalog (ERCSC) with quasi-simultaneous ground-based observations, as well as archival data, at frequencies below or overlapping Planck frequency bands, to validate the astrometry and photometry of the ERCSC radio sources and study the spectral features shown in this new frequency window opened by Planck. The ERCSC source positions and flux density scales are found to be consistent with the ground-based observations. We present and discuss the spectral energy distributions (SEDs) of a sample of ”extreme” radio sources to illustrate the richness of the ERCSC for the study of extragalactic radio sources. Variability is found to play a role in the unusual spectral features of some of these sources.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, M Baker, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, K Bennett, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borrill, F R Bouchet, T Bradshaw, M Bremer, M Bucher, C Burigana, R C Butler, P Cabella, C M Cantalupo, B Cappellini, J -F Cardoso, R Carr, M Casale, A Catalano, L CayĂłn, A Challinor, A Chamballu, J Charra, R -R Chary, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, G Crone, M Crook, F Cuttaia, L Danese, O D’Arcangelo, R D Davies, R J Davis, P de Bernardis, J de Bruin, G de Gasperis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, J Dick, C Dickinson, K Dolag, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, S Foley, O Forni, P Fosalba, M Frailis, E Franceschi, M Freschi, T C Gaier, S Galeotta, J Gallegos, B Gandolfo, K Ganga, M Giard, G Giardino, G Gienger, Y Giraud-HĂ©raud, J González, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, G Guyot, J Haissinski, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, A Hornstrup, W Hovest, R J Hoyland, K M Huffenberger, A H Jaffe, T Jagemann, W C Jones, J J Juillet, M Juvela, P Kangaslahti, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, M Krassenburg, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A E Lange, A Lasenby, R J Laureijs, C R Lawrence, S Leach, J P Leahy, R Leonardi, C Leroy, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, S Lowe, P M Lubin, J F MacĂ­as-PĂ©rez, T Maciaszek, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, M Massardi, S Matarrese, F Matthai, P Mazzotta, A McDonald, P McGehee, P R Meinhold, A Melchiorri, J -B Melin, L Mendes, A Mennella, C Mevi, R Miniscalco, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, N Morisset, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, I Ortiz, S Osborne, P Osuna, C A Oxborrow, F Pajot, R Paladini, B Partridge, F Pasian, T Passvogel, G Patanchon, D Pearson, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, L Popa, T Poutanen, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, R Rebolo, M Reinecke, J -M Reix, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, E Salerno, M Sandri, D Santos, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, A Simonetto, G F Smoot, C Sozzi, J -L Starck, J Sternberg, F Stivoli, V Stolyarov, R Stompor, L Stringhetti, R Sudiwala, R Sunyaev, J -F Sygnet, D Tapiador, J A Tauber, D Tavagnacco, D Taylor, L Terenzi, D Texier, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, M TĂĽrler, M Tuttlebee, G Umana, L Valenziano, J Valiviita, J Varis, L Vibert, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, C Watson, S D M White, M White, A Wilkinson, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. I. The Planck mission   Astronomy & Astrophysics 536: A1 December  
Abstract: The European Space Agency’s Planck satellite was launched on 14 May 2009, and has been surveying the sky stably and continuously since 13 August 2009. Its performance is well in line with expectations, and it will continue to gather scientific data until the end of its cryogenic lifetime. We give an overview of the history of Planck in its first year of operations, and describe some of the key performance aspects of the satellite. This paper is part of a package submitted in conjunction with Planck’s Early Release Compact Source Catalogue, the first data product based on Planck to be released publicly. The package describes the scientific performance of the Planck payload, and presents results on a variety of astrophysical topics related to the sources included in the Catalogue, as well as selected topics on diffuse emission.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, M Baker, A Balbi, A J Banday, R B Barreiro, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, P Bhandari, R Bhatia, J J Bock, A Bonaldi, J R Bond, J Borders, J Borrill, F R Bouchet, B Bowman, T Bradshaw, E BrĂ©elle, M Bucher, C Burigana, R C Butler, P Cabella, P Camus, C M Cantalupo, B Cappellini, J -F Cardoso, A Catalano, L CayĂłn, A Challinor, A Chamballu, J P Chambelland, J Charra, M Charra, L -Y Chiang, C Chiang, P R Christensen, D L Clements, B Collaudin, S Colombi, F Couchot, A Coulais, B P Crill, M Crook, F Cuttaia, C Damasio, L Danese, R D Davies, R J Davis, P de Bernardis, G de Gasperis, A de Rosa, J Delabrouille, J -M Delouis, F -X DĂ©sert, K Dolag, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, C Filliard, F Finelli, S Foley, O Forni, P Fosalba, J -J Fourmond, M Frailis, E Franceschi, S Galeotta, K Ganga, E Gavila, M Giard, G Giardino, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, G Guyot, D Harrison, G Helou, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, A Hornstrup, W Hovest, R J Hoyland, K M Huffenberger, U Israelsson, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, J -M Lamarre, P Lami, A Lasenby, R J Laureijs, A Lavabre, C R Lawrence, S Leach, R Lee, R Leonardi, C Leroy, P B Lilje, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, T Maciaszek, C J MacTavish, B Maffei, D Maino, N Mandolesi, R Mann, M Maris, E MartĂ­nez-González, S Masi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, F Melot, L Mendes, A Mennella, M -A Miville-DeschĂŞnes, A Moneti, L Montier, J Mora, G Morgante, N Morisset, D Mortlock, D Munshi, A Murphy, P Naselsky, A Nash, P Natoli, C B Netterfield, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, F Pasian, G Patanchon, D Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G PrĂ©zeau, M Prina, S Prunet, J -L Puget, J P Rachen, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, J A Rubiño-MartĂ­n, B Rusholme, M Sandri, D Santos, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, P Stassi, F Stivoli, V Stolyarov, R Stompor, R Sudiwala, J -F Sygnet, J A Tauber, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, L Valenziano, L Vibert, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, C Watson, S D M White, A Wilkinson, P Wilson, D Yvon, A Zacchei, B Zhang, A Zonca (2011)  Planck early results. II. The thermal performance of Planck   Astronomy & Astrophysics 536: A2 December  
Abstract: The performance of the Planck instruments in space is enabled by their low operating temperatures, 20K for LFI and 0.1K for HFI, achieved through a combination of passive radiative cooling and three active mechanical coolers. Active coolers were chosen to minimize straylight on the detectors and to maximize lifetime. The scientific requirement for very broad frequency led to two detector technologies with widely different temperature and cooling needs. This made use of a helium cryostat, as used by previous cryogenic space missions (IRAS, COBE, ISO, SPITZER, AKARI), infeasible. Radiative cooling is provided by three V-groove radiators and a large telescope baffle. The active coolers are a hydrogen sorption cooler (\lt20K), a 4He Joule-Thomson cooler (4.7K), and a 3He-4He dilution cooler (1.4K and 0.1K). The flight system was at ambient temperature at launch and cooled in space to operating conditions. The bolometer plate of the High Frequency Instrument reached 93mK on 3 July 2009, 50 days after launch. The solar panel always faces the Sun, shadowing the rest of Planck, and operates at a mean temperature of 384K. At the other end of the spacecraft, the telescope baffle operates at 42.3K and the telescope primary mirror operates at 35.9K. The temperatures of key parts of the instruments are stabilized by both active and passive methods. Temperature fluctuations are driven by changes in the distance from the Sun, sorption cooler cycling and fluctuations in gas-liquid flow, and fluctuations in cosmic ray flux on the dilution and bolometer plates. These fluctuations do not compromise the science data.
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A Zacchei, D Maino, C Baccigalupi, M Bersanelli, A Bonaldi, L Bonavera, C Burigana, R C Butler, F Cuttaia, G de Zotti, J Dick, M Frailis, S Galeotta, J González-Nuevo, K M GĂłrski, A Gregorio, E Keihänen, R Keskitalo, J Knoche, H Kurki-Suonio, C R Lawrence, S Leach, J P Leahy, M LĂłpez-Caniego, N Mandolesi, M Maris, F Matthai, P R Meinhold, A Mennella, G Morgante, N Morisset, P Natoli, F Pasian, F Perrotta, G Polenta, T Poutanen, M Reinecke, S Ricciardi, R Rohlfs, M Sandri, A -S Suur-Uski, J A Tauber, D Tavagnacco, L Terenzi, M Tomasi, J Valiviita, F Villa, A Zonca, A J Banday, R B Barreiro, J G Bartlett, N Bartolo, L Bedini, K Bennett, P Binko, J Borrill, F R Bouchet, M Bremer, P Cabella, B Cappellini, X Chen, L Colombo, M Cruz, A Curto, L Danese, R D Davies, R J Davis, G de Gasperis, A de Rosa, G de Troia, C Dickinson, J M Diego, S Donzelli, U Dörl, G Efstathiou, T A EnĂźlin, H K Eriksen, M C Falvella, F Finelli, E Franceschi, T C Gaier, F Gasparo, R T GĂ©nova-Santos, G Giardino, F GĂłmez, A Gruppuso, F K Hansen, R Hell, D Herranz, W Hovest, M Huynh, J Jewell, M Juvela, T S Kisner, L Knox, A Lähteenmäki, J -M Lamarre, R Leonardi, J LeĂłn-Tavares, P B Lilje, P M Lubin, G Maggio, D Marinucci, E MartĂ­nez-González, M Massardi, S Matarrese, M T Meharga, A Melchiorri, M Migliaccio, S Mitra, A Moss, H U Nørgaard-Nielsen, L Pagano, R Paladini, D Paoletti, B Partridge, D Pearson, V Pettorino, D Pietrobon, G PrĂ©zeau, P Procopio, J -L Puget, C Quercellini, J P Rachen, R Rebolo, G Robbers, G Rocha, J A Rubiño-MartĂ­n, E Salerno, M Savelainen, D Scott, M D Seiffert, J I Silk, G F Smoot, J Sternberg, F Stivoli, R Stompor, G Tofani, L Toffolatti, J Tuovinen, M TĂĽrler, G Umana, P Vielva, N Vittorio, C Vuerli, L A Wade, R Watson, S D M White, A Wilkinson (2011)  Planck early results. V. The Low Frequency Instrument data processing   Astronomy & Astrophysics 536: A5 December  
Abstract: We describe the data processing pipeline employed by the Low Frequency Instrument (LFI) Data Processing Centre (DPC) to create and characterize the frequency maps used by the ERCSC (Early Release Compact Source Catalogue) first product of Planck to become public. In particular, we discuss the various steps involved in reducing the data, starting from telemetry (TM)packets through to the production of cleaned calibrated timelines and calibrated frequency maps. Data are continuously calibrated using the modulation induced on the mean temperature of the Cosmic Microwave Background Radiation by the proper motion of the spacecraft. The sky signals other than the dipole are removed by an iterative procedure based on simultaneous fitting of calibration parameters and sky maps. Noise properties are estimated from time-ordered data where the sky signal is removed using a Generalized Least Square map-making algorithm. The measured 1/f noise knee-frequencies range from $$sim 100 mHz at 30 GHz to a few tens of mHz at 70 GHz. A destriping code (Madam) is employed to combine radiometric data and pointing information into sky maps, minimizing the variance of correlated noise. Noise covariance matrices required to compute statistical uncertainties on LFI and Planck products are also produced. Main beams are estimated down to the $$approx -10 dB level using Jupiter transits which are also used for the geometrical calibration of the focal plane.
Notes:
Planck Collaboration, P A R Ade, N Aghanim, M Arnaud, M Ashdown, J Aumont, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, J G Bartlett, E Battaner, K Benabed, A BenoĂ®t, J -P Bernard, M Bersanelli, R Bhatia, A Bonaldi, L Bonavera, J R Bond, J Borrill, F R Bouchet, M Bucher, C Burigana, R C Butler, P Cabella, C M Cantalupo, B Cappellini, J -F Cardoso, P Carvalho, A Catalano, L CayĂłn, A Challinor, A Chamballu, R -R Chary, X Chen, L -Y Chiang, C Chiang, P R Christensen, D L Clements, S Colombi, F Couchot, A Coulais, B P Crill, F Cuttaia, L Danese, R J Davis, P de Bernardis, A de Rosa, G de Zotti, J Delabrouille, J -M Delouis, F -X DĂ©sert, C Dickinson, J M Diego, K Dolag, H Dole, S Donzelli, O DorĂ©, U Dörl, M Douspis, X Dupac, G Efstathiou, T A EnĂźlin, H K Eriksen, F Finelli, O Forni, P Fosalba, M Frailis, E Franceschi, S Galeotta, K Ganga, M Giard, Y Giraud-HĂ©raud, J González-Nuevo, K M GĂłrski, S Gratton, A Gregorio, A Gruppuso, J Haissinski, F K Hansen, D Harrison, G Helou, S Henrot-VersillĂ©, C Hernández-Monteagudo, D Herranz, S R Hildebrandt, E Hivon, M Hobson, W A Holmes, A Hornstrup, W Hovest, R J Hoyland, K M Huffenberger, M Huynh, A H Jaffe, W C Jones, M Juvela, E Keihänen, R Keskitalo, T S Kisner, R Kneissl, L Knox, H Kurki-Suonio, G Lagache, A Lähteenmäki, J -M Lamarre, A Lasenby, R J Laureijs, C R Lawrence, S Leach, J P Leahy, R Leonardi, J LeĂłn-Tavares, C Leroy, P B Lilje, M Linden-Vørnle, M LĂłpez-Caniego, P M Lubin, J F MacĂ­as-PĂ©rez, C J MacTavish, B Maffei, G Maggio, D Maino, N Mandolesi, R Mann, M Maris, F Marleau, D J Marshall, E MartĂ­nez-González, S Masi, M Massardi, S Matarrese, F Matthai, P Mazzotta, P McGehee, P R Meinhold, A Melchiorri, J -B Melin, L Mendes, A Mennella, S Mitra, M -A Miville-DeschĂŞnes, A Moneti, L Montier, G Morgante, D Mortlock, D Munshi, A Murphy, P Naselsky, P Natoli, C B Netterfield, H U Nørgaard-Nielsen, F Noviello, D Novikov, I Novikov, I J O’Dwyer, S Osborne, F Pajot, R Paladini, B Partridge, F Pasian, G Patanchon, T J Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, R Piffaretti, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, T Poutanen, G W Pratt, G PrĂ©zeau, S Prunet, J -L Puget, J P Rachen, W T Reach, R Rebolo, M Reinecke, C Renault, S Ricciardi, T Riller, I Ristorcelli, G Rocha, C Rosset, M Rowan-Robinson, J A Rubiño-MartĂ­n, B Rusholme, A Sajina, M Sandri, D Santos, G Savini, B M Schaefer, D Scott, M D Seiffert, P Shellard, G F Smoot, J -L Starck, F Stivoli, V Stolyarov, R Sudiwala, R Sunyaev, J -F Sygnet, J A Tauber, D Tavagnacco, L Terenzi, L Toffolatti, M Tomasi, J -P Torre, M Tristram, J Tuovinen, M TĂĽrler, G Umana, L Valenziano, J Valiviita, J Varis, P Vielva, F Villa, N Vittorio, L A Wade, B D Wandelt, S D M White, A Wilkinson, D Yvon, A Zacchei, A Zonca (2011)  Planck early results. VII. The Early Release Compact Source Catalogue   Astronomy & Astrophysics 536: A7 December  
Abstract: A brief description of the methodology of construction, contents and usage of the Planck Early Release Compact Source Catalogue (ERCSC), including the Early Cold Cores (ECC) and the Early Sunyaev-Zeldovich (ESZ) cluster catalogue is provided. The catalogue is based on data that consists of mapping the entire sky once and 60% of the sky a second time by Planck. A Monte-Carlo algorithm based on the injection and extraction of artificial sources into the Planck maps was implemented to select reliable sources among all extracted candidates such that the cumulative reliability of the catalogue is \gt=90%. As a result of the Monte-Carlo assessment of the reliability of sources from different techniques, the PowellSnakes source extraction technique was used at the 5 frequencies between 30 and 143 GHz while the SExtractor technique was used between 217 and 857 GHz. The 10 sigma photometric flux density limit of the catalogue at |b|\gt30 deg is 0.49, 1.0, 0.67, 0.5, 0.33, 0.28, 0.25, 0.47 and 0.82 Jy at each of the nine frequencies between 30 and 857 GHz. Sources which are up to a factor of 2 fainter than this limit, and which are present in ”clean” regions of the Galaxy where the sky background due to emission from the interstellar medium is low, are included in the ERCSC if they meet the high reliability criterion. The Planck ERCSC provides a robust list of stars with dust shells, stellar cores, radio galaxies, blazars, infrared luminous galaxies, Galactic interstellar medium features, 915 cold molecular cloud core candidates, 189 SZ cluster candidates as well as unclassified sources from the first high sensitivity radio/submillimetre observations of the entire sky. The source list, with more than 15000 unique sources, is ripe for follow-up characterisation.
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A Mennella, R C Butler, A Curto, F Cuttaia, R J Davis, J Dick, M Frailis, S Galeotta, A Gregorio, H Kurki-Suonio, C R Lawrence, S Leach, J P Leahy, S Lowe, D Maino, N Mandolesi, M Maris, E MartĂ­nez-González, P R Meinhold, G Morgante, D Pearson, F Perrotta, G Polenta, T Poutanen, M Sandri, M D Seiffert, A -S Suur-Uski, D Tavagnacco, L Terenzi, M Tomasi, J Valiviita, F Villa, R Watson, A Wilkinson, A Zacchei, A Zonca, B Aja, E Artal, C Baccigalupi, A J Banday, R B Barreiro, J G Bartlett, N Bartolo, P Battaglia, K Bennett, A Bonaldi, L Bonavera, J Borrill, F R Bouchet, C Burigana, P Cabella, B Cappellini, X Chen, L Colombo, M Cruz, L Danese, O D’Arcangelo, R D Davies, G de Gasperis, A de Rosa, G de Zotti, C Dickinson, J M Diego, S Donzelli, G Efstathiou, T A EnĂźlin, H K Eriksen, M C Falvella, F Finelli, S Foley, C Franceschet, E Franceschi, T C Gaier, R T GĂ©nova-Santos, D George, F GĂłmez, J González-Nuevo, K M GĂłrski, A Gruppuso, F K Hansen, D Herranz, J M Herreros, R J Hoyland, N Hughes, J Jewell, P Jukkala, M Juvela, P Kangaslahti, E Keihänen, R Keskitalo, V -H Kilpia, T S Kisner, J Knoche, L Knox, M Laaninen, A Lähteenmäki, J -M Lamarre, R Leonardi, J LeĂłn-Tavares, P Leutenegger, P B Lilje, M LĂłpez-Caniego, P M Lubin, M Malaspina, D Marinucci, M Massardi, S Matarrese, F Matthai, A Melchiorri, L Mendes, M Miccolis, M Migliaccio, S Mitra, A Moss, P Natoli, R Nesti, H U Nørgaard-Nielsen, L Pagano, R Paladini, D Paoletti, B Partridge, F Pasian, V Pettorino, D Pietrobon, M Pospieszalski, G PrĂ©zeau, M Prina, P Procopio, J -L Puget, C Quercellini, J P Rachen, R Rebolo, M Reinecke, S Ricciardi, G Robbers, G Rocha, N Roddis, J A Rubi no-MartĂ­n, M Savelainen, D Scott, R Silvestri, A Simonetto, P Sjoman, G F Smoot, C Sozzi, L Stringhetti, J A Tauber, G Tofani, L Toffolatti, J Tuovinen, M TĂĽrler, G Umana, L Valenziano, J Varis, P Vielva, N Vittorio, L A Wade, C Watson, S D M White, F Winder (2011)  Planck early results. III. First assessment of the Low Frequency Instrument in-flight performance   Astronomy & Astrophysics 536: A3 December  
Abstract: The scientific performance of the Planck Low Frequency Instrument (LFI) after one year of in-orbit operation is presented. We describe the main optical parameters and discuss photometric calibration, white noise sensitivity, and noise properties. A preliminary evaluation of the impact of the main systematic effects is presented. For each of the performance parameters, we outline the methods used to obtain them from the flight data and provide a comparison with pre-launch ground assessments, which are essentially confirmed in flight.
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2010
F Villa, L Terenzi, M Sandri, P Meinhold, T Poutanen, P Battaglia, C Franceschet, N Hughes, M Laaninen, P Lapolla, M Bersanelli, R C Butler, F Cuttaia, O D’Arcangelo, M Frailis, E Franceschi, S Galeotta, A Gregorio, R Leonardi, S R Lowe, N Mandolesi, M Maris, L Mendes, A Mennella, G Morgante, L Stringhetti, M Tomasi, L Valenziano, A Zacchei, A Zonca, B Aja, E Artal, M Balasini, T Bernardino, E Blackhurst, L Boschini, B Cappellini, F Cavaliere, A Colin, F Colombo, R J Davis, L De La Fuente, J Edgeley, T Gaier, A Galtress, R Hoyland, P Jukkala, D Kettle, V Kilpia, C R Lawrence, D Lawson, J P Leahy, P Leutenegger, S Levin, D Maino, M Malaspina, A Mediavilla, M Miccolis, L Pagan, J P Pascual, F Pasian, M Pecora, M Pospieszalski, N Roddis, M J Salmon, M Seiffert, R Silvestri, A Simonetto, P Sjoman, C Sozzi, J Tuovinen, J Varis, A Wilkinson, F Winder (2010)  Planck pre-launch status : calibration of the Low Frequency Instrument flight model radiometers   Astronomy & Astrophysics 520: A6  
Abstract: The Low Frequency Instrument (LFI) on-board the ESA Planck satellite carries eleven radiometer subsystems, called Radiometer Chain Assemblies (RCAs), each composed of a pair of pseudo-correlation receivers. We describe the on-ground calibration campaign performed to qualify the flight model RCAs and to measure their pre-launch performances. Each RCA was calibrated in a dedicated flight-like cryogenic environment with the radiometer front-end cooled to 20K and the back-end at 300K, and with an external input load cooled to 4K. A matched load simulating a blackbody at different temperatures was placed in front of the sky horn to derive basic radiometer properties such as noise temperature, gain, and noise performance, e.g. 1/f noise. The spectral response of each detector was measured as was their susceptibility to thermal variation. All eleven LFI RCAs were calibrated. Instrumental parameters measured in these tests, such as noise temperature, bandwidth, radiometer isolation, and linearity, provide essential inputs to the Planck-LFI data analysis.
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M Tomasi, B Cappellini, A Gregorio, F Colombo, M Lapolla, L Terenzi, G Morgante, M Bersanelli, R C Butler, S Galeotta, N Mandolesi, M Maris, A Mennella, L Valenziano, A Zacchei (2010)  Dynamic validation of the Planck-LFI thermal model   Journal of Instrumentation 5: T01002 jan  
Abstract: The Low Frequency Instrument (LFI) is an array of cryogenically cooled radiometers on board the Planck satellite, designed to measure the temperature and polarization anisotropies of the cosmic microwave backgrond (CMB) at 30, 44 and 70 GHz. The thermal requirements of the LFI, and in particular the stringent limits to acceptable thermal fluctuations in the 20 K focal plane, are a critical element to achieve the instrument scientific performance. Thermal tests were carried out as part of the on-ground calibration campaign at various stages of instrument integration. In this paper we describe the results and analysis of the tests on the LFI flight model (FM) performed at Thales Laboratories in Milan (Italy) during 2006, with the purpose of experimentally sampling the thermal transfer functions and consequently validating the numerical thermal model describing the dynamic response of the LFI focal plane. This model has been used extensively to assess the ability of LFI to achieve its scientific goals: its validation is therefore extremely important in the context of the Planck mission. Our analysis shows that the measured thermal properties of the instrument show a thermal damping level better than predicted, therefore further reducing the expected systematic effect induced in the LFI maps. We then propose an explanation of the increased damping in terms of non-ideal thermal contacts.
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J P, Leahy, M Bersanelli, O D'Arcangelo, K Ganga, S M Leach, A Moss, E Keihänen, R Keskitalo, H Kurki-Suonio, T Poutanen, M Sandri, D Scott, J Tauber, L Valenziano, F Villa, A Wilkinson, A Zonca, C Baccigalupi, J Borrill, R C Butler, F Cuttaia, R J Davis, M Frailis, E Francheschi, S Galeotta, A Gregorio, R Leonardi, N Mandolesi, M Maris, P Meinhold, L Mendes, A Mennella, G Morgante, G Prezeau, G Rocha, L Stringhetti, L Terenzi, M Tomasi (2010)  Planck pre-launch status : expected LFI polarisation capability   Astronomy & Astrophysics 520: A8  
Abstract: We present a system-level description of the Low Frequency Instrument (LFI) considered as a differencing polarimeter, and evaluate its expected performance. The LFI is one of the two instruments on board the ESA Planck mission to study the cosmic microwave background. It consists of a set of 22 radiometers sensitive to linear polarisation, arranged in orthogonally-oriented pairs connected to 11 feed horns operating at 30, 44 and 70 GHz. In our analysis, the generic Jones and Mueller-matrix formulations for polarimetry are adapted to the special case of the LFI. Laboratory measurements of flight components are combined with optical simulations of the telescope to investigate the values and uncertainties in the system parameters affecting polarisation response. Methods of correcting residual systematic errors are also briefly discussed. The LFI has beam-integrated polarisation efficiency >99% for all detectors, with uncertainties below 0.1%. Indirect assessment of polarisation position angles suggests that uncertainties are generally less than 0. 5, and this will be checked in flight using observations of the Crab nebula. Leakage of total intensity into the polarisation signal is generally well below the thermal noise level except for bright Galactic emission, where the dominant effect is likely to be spectral-dependent terms due to bandpass mismatch between the two detectors behind each feed, contributing typically 1–3% leakage of foreground total intensity. Comparable leakage from compact features occurs due to beam mismatch, but this averages to < 5 × 10â’4 for large-scale emission. An inevitable feature of the LFI design is that the two components of the linear polarisation are recovered from elliptical beams which differ substantially in orientation. This distorts the recovered polarisation and its angular power spectrum, and several methods are being developed to correct the effect, both in the power spectrum and in the sky maps. The LFI will return a high-quality measurement of the CMB polarisation, limited mainly by thermal noise. To meet our aspiration of measuring polarisation at the 1% level, further analysis of flight and ground data is required. We are still researching the most effective techniques for correcting subtle artefacts in polarisation; in particular the correction of bandpass mismatch effects is a formidable challenge, as it requires multi-band analysis to estimate the spectral indices that control the leakage.
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A Zonca, B Roucaries, B Williams, I Rubin, O D’Arcangelo, P Meinhold, P Lubin, C Franceschet, S Yahn, A Mennella, M Bersanelli (2010)  Modeling the frequency response of microwave radiometers with QUCS   Journal of Instrumentation 5: 12. T12001  
Abstract: Characterization of the frequency response of coherent radiometric receivers is a key element in estimating the flux of astrophysical emissions, since the measured signal depends on the convolution of the source spectral emission with the instrument band shape. Laboratory Radio Frequency (RF) measurements of the instrument bandpass often require complex test setups and are subject to a number of systematic effects driven by thermal issues and impedance matching, particularly if cryogenic operation is involved. In this paper we present an approach to modeling radiometers bandpasses by integrating simulations and RF measurements of individual components. This method is based on QUCS (Quasi Universal Circuit Simulator), an open-source circuit simulator, which gives the flexibility of choosing among the available devices, implementing new analytical software models or using measured S-parameters. Therefore an independent estimate of the instrument bandpass is achieved using standard individual component measurements and validated analytical simulations. In order to automate the process of preparing input data, running simulations and exporting results we developed the Python package python-qucs and released it under GNU Public License. We discuss, as working cases, bandpass response modeling of the COFE and Planck Low Frequency Instrument (LFI) radiometers and compare results obtained with QUCS and with a commercial circuit simulator software. The main purpose of bandpass modeling in COFE is to optimize component matching, while in LFI they represent the best estimation of frequency response, since end-to-end measurements were strongly affected by systematic effects.
Notes:
M Bersanelli, N Mandolesi, R C Butler, A Mennella, F Villa, B Aja, E Artal, E Artina, C Baccigalupi, M Balasini, G Baldan, A Banday, P Bastia, P Battaglia, T Bernardino, E Blackhurst, L Boschini, C Burigana, G Cafagna, B Cappellini, F Cavaliere, F Colombo, G Crone, F Cuttaia, O D’Arcangelo, L Danese, R D Davies, R J Davis, L De Angelis, G C De Gasperis, L De La Fuente, A De Rosa, G De Zotti, M C Falvella, F Ferrari, R Ferretti, L Figini, S Fogliani, C Franceschet, E Franceschi, T Gaier, S Garavaglia, F Gomez, K Gorski, A Gregorio, P Guzzi, J M Herreros, S R Hildebrandt, R Hoyland, N Hughes, M Janssen, P Jukkala, D Kettle, V H Kilpia, M Laaninen, P M Lapolla, C R Lawrence, J P Leahy, R Leonardi, P Leutenegger, S Levin, P B Lilje, S R Lowe, D L P M Lubin, D Maino, M Malaspina, M Maris, J Marti-Canales, E Martinez-Gonzalez, A Mediavilla, P Meinhold, M Miccolis, G Morgante, P Natoli, R Nesti, L Pagan, C Paine, B Partridge, J P Pascual, F Pasian, D Pearson, M Pecora, F Perrotta, P Platania, M Pospieszalski, T Poutanen, M Prina, R Rebolo, N Roddis, J A Rubino-Martin, n J Salmon, M Sandri, M Seiffert, R Silvestri, A Simonetto, P Sjoman, G F Smoot, C Sozzi, L Stringhetti, E Taddei, J Tauber, L Terenzi, M Tomasi, J Tuovinen, L Valenziano, J Varis, N Vittorio, L A Wade, A Wilkinson, F Winder, A Zacchei, A Zonca (2010)  Planck pre-launch status : Design and description of the Low Frequency Instrument   Astronomy & Astrophysics 520: A4  
Abstract: In this paper we present the Low Frequency Instrument (LFI), designed and developed as part of the Planck space mission, the ESA programme dedicated to precision imaging of the cosmic microwave background (CMB). Planck-LFI will observe the full sky in intensity and polarisation in three frequency bands centred at 30, 44 and 70 GHz, while higher frequencies (100-850 GHz) will be covered by the HFI instrument. The LFI is an array of microwave radiometers based on state-of-the-art indium phosphide cryogenic HEMT amplifiers implemented in a differential system using blackbody loads as reference signals. The front end is cooled to 20K for optimal sensitivity and the reference loads are cooled to 4K to minimise low-frequency noise. We provide an overview of the LFI, discuss the leading scientific requirements, and describe the design solutions adopted for the various hardware subsystems. The main drivers of the radiometric, optical, and thermal design are discussed, including the stringent requirements on sensitivity, stability, and rejection of systematic effects. Further details on the key instrument units and the results of ground calibration are provided in a set of companion papers.
Notes: 2010
A Mennella, M Bersanelli, R C Butler, F Cuttaia, O D’Arcangelo, R J Davis, M Frailis, S Galeotta, A Gregorio, C R Lawrence, R Leonardi, S R Lowe, N Mandolesi, M Maris, P Meinhold, L Mendes, G Morgante, M Sandri, L Stringhetti, L Terenzi, M Tomasi, L Valenziano, F Villa, A Zacchei, A Zonca, M Balasini, C Franceschet, P Battaglia, P M Lapolla, P Leutenegger, M Miccolis, L Pagan, R Silvestri, B Aja, E Artal, G Baldan, P Bastia, T Bernardino, L Boschini, G Cafagna, B Cappellini, F Cavaliere, F Colombo, L de La Fuente, J Edgeley, M C Falvella, F Ferrari, S Fogliani, E Franceschi, T Gaier, F Gomez, J M Herreros, S Hildebrandt, R Hoyland, N Hughes, P Jukkala, D Kettle, M Laaninen, D Lawson, P Leahy, S Levin, P B Lilje, D Maino, M Malaspina, P Manzato, J Marti-Canales, E Martinez-Gonzalez, A Mediavilla, F Pasian, J P Pascual, M Pecora, L Peres-Cuevas, P Platania, M Pospieszalsky, T Poutanen, R Rebolo, N Roddis, M Salmon, M Seiffert, A Simonetto, C Sozzi, J Tauber, J Tuovinen, J Varis, A Wilkinson, F Winder (2010)  Planck pre-launch status : Low Frequency Instrument calibration and expected scientific performance   Astronomy & Astrophysics 520: A5  
Abstract: We present the calibration and scientific performance parameters of the Planck Low Frequency Instrument (LFI) measured during the ground cryogenic test campaign. These parameters characterise the instrument response and constitute our optimal pre-launch knowledge of the LFI scientific performance. The LFI shows excellent 1/f stability and rejection of instrumental systematic effects; its measured noise performance shows that LFI is the most sensitive instrument of its kind. The calibration parameters will be updated during flight operations until the end of the mission.
Notes:
J A Tauber, N Mandolesi, J L Puget, T Banos, M Bersanelli, F R Bouchet, R C Butler, J Charra, G Crone, J Dodsworth, G Efstathiou, R Gispert, G Guyot, A Gregorio, J J Juillet, J M Lamarre, R J Laureijs, C R Lawrence, H U Nargaard-Nielsen, T Passvogel, J M Reix, D Texier, L Vibert, A Zacchei, P A R Ade, N Aghanim, B Aja, E Alippi, L Aloy, P Armand, M Arnaud, A Arondel, A Arreola-Villanueva, E Artal, E Artina, A Arts, M Ashdown, J Aumont, M Azzaro, A Bacchetta, C Baccigalupi, M Baker, M Balasini, A Balbi, A J Banday, G Barbier, R B Barreiro, M Bartelmann, P Battaglia, E Battaner, K Benabed, J L Beney, R Beneyton, K Bennett, A Benoit, J P Bernard, P Bhandari, R Bhatia, M Biggi, R Biggins, G Billig, Y Blanc, H Blavot, J J Bock, A Bonaldi, R Bond, J Bonis, J Borders, J Borrill, L Boschini, F Boulanger, J Bouvier, M Bouzit, R Bowman, E Breelle, T Bradshaw, M Braghin, M Bremer, D Brienza, C Burigana, M Burkhalter, P Cabella, T Cafferty, M Cairola, S Caminade, D Broszkiewicz, P Camus, C M Cantalupo, B Cappellini, J F Cardoso, R Carr, A Catalano, L Cayon, M Cesa, M Chaigneau, A Challinor, A Chamballu, J P Chambelland, M Charra, L Y Chiang, G Chlewicki, P R Christensen, S Church, E Ciancietta, M Cibrario, R Cizeron, D Clements, B Collaudin, J M Colley, S Colombi, A Colombo, F Colombo, O Corre, F Couchot, B Cougrand, A Coulais, P Couzin, B Crane, B Crill, M Crook, D Crumb, F Cuttaia, U Dorl, P daSilva, R Daddato, C Damasio, L Danese, G d'Aquino, O D'Arcangelo, K Dassas, R D Davies, W Davies, R J Davis, P De Bernardis, D de Chambure, G de Gasperis, M L De la Fuente, P De Paco, A De Rosa, G De Troia, G De Zotti, M Dehamme, J Delabrouille, J M Delouis, F X Desert, G di Girolamo, C Dickinson, E Doelling, K Dolag, I Domken, M Douspis, D Doyle, S Du, D Dubruel, C Dufour, C Dumesnil, X Dupac, P Duret, C Eder, A Elfving, T A Ensslin, P Eng, K English, H K Eriksen, P Estaria, M C Falvella, F Ferrari, F Finelli, A Fishman, S Fogliani, S Foley, A Fonseca, G Forma, O Forni, P Fosalba, J J Fourmond, M Frailis, C Franceschet, E Franceschi, S Franois, M Frerking, M F Gomez-Renasco, K M Gorski, T C Gaier, S Galeotta, K Ganga, A Garnica, M Gaspard, E Gavila, M Giard, G Giardino, G Gienger, J Garcia Lazaro, Y Giraud-Heraud, J M Glorian, M Griffin, A Gruppuso, L Guglielmi, D Guichon, B Guillaume, P Guillouet, J Haissinski, F K Hansen, J Hardy, D Harrison, A Hazell, M Hechler, V Heckenauer, D Heinzer, R Hell, S Henrot-VersillĂ©, C Hernandez-Monteagudo, D Herranz, J M Herreros, V Hervier, A Heske, A Heurtel, S R Hildebrandt, R Hills, E Hivon, M Hobson, D Hollert, W Holmes, A Hornstrup, W Hovest, R J Hoyland, G Huey, K M Huffenberger, N Hughes, U Israelsson, B Jackson, A Jaffe, T R Jaffe, T Jagemann, N C Jessen, J Jewell, W Jones, M Juvela, J Kaplan, P Karlman, F Keck, E Keihanen, M King, T S Kisner, P Kletzkine, J Knoche, L Knox, T Koch, M Krassenburg, H Kurki-Suonio, A Lahteenmaki, R Kneissl, G Lagache, E Lagorio, P Lami, J Lande, A Lange, F Langlet, R Lapini, M Lapolla, A Lasenby, M LeJeune, J P Leahy, M Lefebvre, F Legrand, G LeMeur, R Leonardi, B Leriche, C Leroy, P Leutenegger, S M Levin, P B Lilje, C Lindensmith, M Linden-Vornle, A Loc, Y Longval, P M Lubin, T Luchik, I Luthold, J F Macias-Perez, T Maciaszek, C MacTavish, S Madden, B Maffei, C Magneville, D Maino, A Mambretti, B Mansoux, D Marchioro, M Maris, F Marliani, J C Marrucho, J Martì-Canales, E Martìnez-GonzĂ lez, A Martìn-Polegre, P Martin, C Marty, W Marty, S Masi, M Massardi, S Matarrese, F Matthai, P Mazzotta, A McDonald, P McGrath, A Mediavilla, P R Meinhold, J B MĂ©lin, F Melot, L Mendes, A Mennella, C Mervier, L Meslier, M Miccolis, M A Miville-Deschenes, A Moneti, D Montet, L Montier, J Mora, G Morgante, G Morigi, G Morinaud, N Morisset, D Mortlock, S Mottet, J Mulder, D Munshi, A Murphy, P Murphy, P Musi, J Narbonne, P Naselsky, A Nash, F Nati, P Natoli, B Netterfield, J Newell, M Nexon, C Nicolas, P H Nielsen, N Ninane, F Noviello, D Novikov, I Novikov, I J O'Dwyer, P Oldeman, P Olivier, L Ouchet, C A Oxborrow, L Pèrez-Cuevas, L Pagan, C Paine, F Pajot, R Paladini, F Pancher, J Panh, G Parks, P Parnaudeau, B Partridge, B Parvin, J P Pascual, F Pasian, D P Pearson, T Pearson, M Pecora, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, O Piersanti, E Plaige, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, L Popa, G Poulleau, T Poutanen, G Prezeau, L Pradell, M Prina, S Prunet, J P Rachen, D Rambaud, F Rame, I Rasmussen, J Rautakoski, W T Reach, R Rebolo, M Reinecke, J Reiter, C Renault, S Ricciardi, P Rideau, T Riller, I Ristorcelli, J B Riti, G Rocha, Y Roche, R Roger Pons, R Rohlfs, D Romero, S Roose, C Rosset, S Rouberol, M Rowan-Robinson, J A Rubino-MartiĂŚÂn, P Rusconi, B Rusholme, M Salama, E Salerno, M Sandri, D Santos, J L Sanz, L Sauter, F Sauvage, G Savini, A Schnorhk, W Schwarz, D Scott, M D Seiffert, M Sias, J I Silk, R Silvestri, R Sippel, G F Smoot, J L Starck, P Stassi, C Shih, F Stivoli, V Stolyarov, R Stompor, L Stringhetti, D Strommen, T Stute, R Sudiwala, J Sternberg (2010)  Planck pre-launch status : The Planck mission   Astronomy & Astrophysics 520: A2  
Abstract:
Notes:
N Mandolesi, M Bersanelli, R C Butler, E Artal, C Baccigalupi, A Balbi, A J Banday, R B Barreiro, M Bartelmann, K Bennett, P Bhandari, A Bonaldi, J Borrill, M Bremer, C Burigana, R C Bowman, P Cabella, C Cantalupo, B Cappellini, T Courvoisier, G Crone, F Cuttaia, L Danese, O D’Arcangelo, R D Davies, R J Davis, L De Angelis, G de Gasperis, A De Rosa, G De Troia, G de Zotti, J Dick, C Dickinson, J M Diego, S Donzelli, U Dörl, X Dupac, T A EnĂźlin, H K Eriksen, M C Falvella, F Finelli, M Frailis, E Franceschi, T Gaier, S Galeotta, F Gasparo, G Giardino, F Gomez, J Gonzalez-Nuevo, K M GĂłrski, A Gregorio, A Gruppuso, F Hansen, R Hell, D Herranz, J M Herreros, S Hildebrandt, W Hovest, R Hoyland, K Huffenberger, M Janssen, T Jaffe, E Keihänen, R Keskitalo, T Kisner, H Kurki-Suonio, A Lähteenmäki, C R Lawrence, S M Leach, J P Leahy, R Leonardi, S Levin, P B Lilje, M LĂłpez-Caniego, S R Lowe, P M Lubin, D Maino, M Malaspina, M Maris, J Marti-Canales, E Martinez-Gonzalez, M Massardi, S Matarrese, F Matthai, P Meinhold, A Melchiorri, L Mendes, A Mennella, G Morgante, G Morigi, N Morisset, A Moss, A Nash, P Natoli, R Nesti, C Paine, B Partridge, F Pasian, T Passvogel, D Pearson, L PĂ©rez-Cuevas, F Perrotta, G Polenta, L A Popa, T Poutanen, G Prezeau, M Prina, J P Rachen, R Rebolo, M Reinecke, S Ricciardi, T Riller, G Rocha, N Roddis, R Rohlfs, J A Rubiño-Martin, E Salerno, M Sandri, D Scott, M Seiffert, J Silk, A Simonetto, G F Smoot, C Sozzi, J Sternberg, F Stivoli, L Stringhetti, J Tauber, L Terenzi, M Tomasi, J Tuovinen, M TĂĽrler, L Valenziano, J Varis, P Vielva, F Villa, N Vittorio, L Wade, M White, S White, A Wilkinson, A Zacchei, A Zonca (2010)  Planck pre-launch status : the Planck-LFI programme   Astronomy & Astrophysics 520: A3  
Abstract: This paper provides an overview of the Low Frequency Instrument (LFI) programme within the ESA Planck mission. The LFI instrument has been developed to produce high precision maps of the microwave sky at frequencies in the range 27–77 GHz, below the peak of the cosmic microwave background (CMB) radiation spectrum. The scientific goals are described, ranging from fundamental cosmology to Galactic and extragalactic astrophysics. The instrument design and development are outlined, together with the model philosophy and testing strategy. The instrument is presented in the context of the Planck mission. The LFI approach to ground and inflight calibration is described. We also describe the LFI ground segment. We present the results of a number of tests demonstrating the capability of the LFI data processing centre (DPC) to properly reduce and analyse LFI flight data, from telemetry information to calibrated and cleaned time ordered data, sky maps at each frequency (in temperature and polarization), component emission maps (CMB and diffuse foregrounds), catalogs for various classes of sources (the Early Release Compact Source Catalogue and the Final Compact Source Catalogue). The organization of the LFI consortium is briefly presented as well as the role of the core team in data analysis and scientific exploitation. All tests carried out on the LFI flight model demonstrate the excellent performance of the instrument and its various subunits. The data analysis pipeline has been tested and its main steps verified. In the first three months after launch, the commissioning, calibration, performance, and verification phases will be completed, after which Planck will begin its operational life, in which LFI will have an integral part.
Notes:
2009
M Tomasi, A Mennella, S Galeotta, S R Lowe, L Mendes, R Leonardi, F Villa, B Cappellini, A Gregorio, P Meinhold, M Sandri, F Cuttaia, L Terenzi, M Maris, L Valenziano, M J Salmon, M Bersanelli, P Binko, R C Butler, O D’Arcangelo, S Fogliani, M Frailis, E Franceschi, F Gasparo, G Maggio, D Maino, M Malaspina, N Mandolesi, P Manzato, M Meharga, G Morgante, N Morisset, F Pasian, F Perrotta, R Rohlfs, M TĂĽrler, A Zacchei, A Zonca (2009)  Off-line radiometric analysis of Planck-LFI data   Journal of Instrumentation 4: T12020 dec  
Abstract: The Planck Low Frequency Instrument (LFI) is an array of 22 pseudo-correlation radiometers on-board the Planck satellite to measure temperature and polarization anisotropies in the Cosmic Microwave Background (CMB) in three frequency bands (30, 44 and 70 GHz). To calibrate and verify the performances of the LFI, a software suite named LIFE has been developed. Its aims are to provide a common platform to use for analyzing the results of the tests performed on the single components of the instrument (RCAs, Radiometric Chain Assemblies) and on the integrated Radiometric Array Assembly (RAA). Moreover, its analysis tools are designed to be used during the flight as well to produce periodic reports on the status of the instrument. The LIFE suite has been developed using a multi-layered, cross-platform approach. It implements a number of analysis modules written in RSI IDL, each accessing the data through a portable and heavily optimized library of functions written in C and C++. One of the most important features of LIFE is its ability to run the same data analysis codes both using ground test data and real flight data as input. The LIFE software suite has been successfully used during the RCA/RAA tests and the Planck Integrated System Tests. Moreover, the software has also passed the verification for its in-flight use during the System Operations Verification Tests, held in October 2008.
Notes:
A Zacchei, M Frailis, M Maris, N Morisset, R Rohlfs, M Meharga, P Binko, M TĂĽrler, S Galeotta, F Gasparo, E Franceschi, R C Butler, F Cuttaia, O D’Arcangelo, S Fogliani, A Gregorio, R Leonardi, S R Lowe, D Maino, G Maggio, M Malaspina, N Mandolesi, P Manzato, P Meinhold, L Mendes, A Mennella, G Morgante, F Pasian, F Perrotta, M Sandri, L Stringhetti, L Terenzi, M Tomasi, A Zonca (2009)  Level 1 on-ground telemetry handling in Planck-LFI   Journal of Instrumentation 4: T12019 dec  
Abstract: The Planck Low Frequency Instrument (LFI) will observe the Cosmic Microwave Background (CMB) by covering the frequency range 30-70 GHz in three bands. The primary instrument data source are the temperature samples acquired by the 22 radiometers mounted on the Planck focal plane. Such samples represent the scientific data of LFI. In addition, the LFI instrument generates the so called housekeeping data by sampling regularly the on-board sensors and registers. The housekeeping data provides information on the overall health status of the instrument and on the scientific data quality. The scientific and housekeeping data are collected on-board into telemetry packets compliant with the ESA Packet Telemetry standards. They represent the primary input to the first processing level of the LFI Data Processing Centre. In this work we show the software systems which build the LFI Level 1. A real-time assessment system, based on the ESA SCOS 2000 generic mission control system, has the main purpose of monitoring the housekeeping parameters of LFI and detect possible anomalies. A telemetry handler system processes the housekeeping and scientific telemetry of LFI, generating timelines for each acquisition chain and each housekeeping parameter. Such timelines represent the main input to the subsequent processing levels of the LFI DPC. A telemetry quick-look system allows the real-time visualization of the LFI scientific and housekeeping data, by also calculating quick statistical functions and fast Fourier transforms. The LFI Level 1 has been designed to support all the mission phases, from the instrument ground tests and calibration to the flight operations, and developed according to the ESA engineering standards.
Notes:
O D’Arcangelo, L Figini, A Simonetto, F Villa, M Pecora, P Battaglia, M Bersanelli, R C Butler, F Cuttaia, S Garavaglia, P Guzzi, N Mandolesi, A Mennella, G Morgante, L Pagan, L Valenziano (2009)  The Planck-LFI flight model composite waveguides   Journal of Instrumentation 4: T12007 dec  
Abstract: The Low Frequency Instrument on board the PLANCK satellite is designed to give the most accurate map ever of the CMB anisotropy of the whole sky over a broad frequency band spanning 27 to 77 GHz. It is made of an array of 22 pseudo-correlation radiometers, composed of 11 actively cooled (20 K) Front End Modules (FEMs), and 11 Back End Modules (BEMs) at 300K, each FEM and BEM set comprising two radiometers. The connection between the two parts is made with rectangular Wave Guides (WGs). Considerations of very different nature (thermal, electromagnetic and mechanical), imposed stringent requirements on the WGs characteristics and drove their design. From the thermal point of view, the WG should guarantee good insulation between the FEM and the BEM sections to avoid overloading the cryocooler. On the other hand it is essential that the signals do not undergo excessive attenuation through the WG. Finally, given the different positions of the FEM modules behind the focal surface and the mechanical constraints given by the surrounding structures, different mechanical designs were necessary. A composite configuration of Stainless Steel and Copper was selected to satisfy all the requirements described. Given the complex shape and the considerable length (about 1.5-2 m) of the LFI WGs, manufacturing and testing the WGs was a challenge. This work deals with the development of the LFI WGs, including the choice of the final configuration and of the fabrication process. It also describes the testing procedure adopted to fully characterize these components from the electromagnetic point of view and the space qualification process they underwent. The Scattering parameters of the WGs were obtained in a one port configuration, minimizing instrumental errors. The space qualification process required manufacturing ad-hoc facilities to support the WGs during vibration tests and to allow electromagnetic tests without removing them. Results obtained during the test campaign are reported and compared with the stringent requirements. The performance of the LFI WGs is in line with requirements, and the WGs were successfully space qualified.
Notes:
E Artal, B Aja, M L de la Fuente, J P Pascual, A Mediavilla, E Martinez-Gonzalez, L Pradell, P de Paco, M Bara, E Blanco, E GarcĂ­a, R Davis, D Kettle, N Roddis, A Wilkinson, M Bersanelli, A Mennella, M Tomasi, R C Butler, F Cuttaia, N Mandolesi, L Stringhetti (2009)  LFI 30 and 44 GHz receivers Back-End Modules   Journal of Instrumentation 4: T12003 dec  
Abstract: The 30 and 44 GHz Back End Modules (BEM) for the Planck Low Frequency Instrument are broadband receivers (20% relative bandwidth) working at room temperature. The signals coming from the Front End Module are amplified, band pass filtered and finally converted to DC by a detector diode. Each receiver has two identical branches following the differential scheme of the Planck radiometers. The BEM design is based on MMIC Low Noise Amplifiers using GaAs P-HEMT devices, microstrip filters and Schottky diode detectors. Their manufacturing development has included elegant breadboard prototypes and finally qualification and flight model units. Electrical, mechanical and environmental tests were carried out for the characterization and verification of the manufactured BEMs. A description of the 30 and 44 GHz Back End Modules of Planck-LFI radiometers is given, with details of the tests done to determine their electrical and environmental performances. The electrical performances of the 30 and 44 GHz Back End Modules: frequency response, effective bandwidth, equivalent noise temperature, 1/f noise and linearity are presented.
Notes:
R J Davis, A Wilkinson, R D Davies, W F Winder, N Roddis, E J Blackhurst, D Lawson, S R Lowe, C Baines, M Butlin, A Galtress, D Shepherd, B Aja, E Artal, M Bersanelli, R C Butler, C Castelli, F Cuttaia, O D’Arcangelo, T Gaier, R Hoyland, D Kettle, R Leonardi, N Mandolesi, A Mennella, P Meinhold, M Pospieszalski, L Stringhetti, M Tomasi, L Valenziano, A Zonca (2009)  Design, development and verification of the 30 and 44 GHz front-end modules for the Planck Low Frequency Instrument   Journal of Instrumentation 4: T12002 dec  
Abstract: We give a description of the design, construction and testing of the 30 and 44 GHz Front End Modules (FEMs) for the Low Frequency Instrument (LFI) of the Planck mission to be launched in 2009. The scientific requirements of the mission determine the performance parameters to be met by the FEMs, including their linear polarization characteristics. The FEM design is that of a differential pseudo-correlation radiometer in which the signal from the sky is compared with a 4-K blackbody load. The Low Noise Amplifier (LNA) at the heart of the FEM is based on indium phosphide High Electron Mobility Transistors (HEMTs). The radiometer incorporates a novel phase-switch design which gives excellent amplitude and phase match across the band. The noise temperature requirements are met within the measurement errors at the two frequencies. For the most sensitive LNAs, the noise temperature at the band centre is 3 and 5 times the quantum limit at 30 and 44 GHz respectively. For some of the FEMs, the noise temperature is still falling as the ambient temperature is reduced to 20 K. Stability tests of the FEMs, including a measurement of the 1/f knee frequency, also meet mission requirements. The 30 and 44 GHz FEMs have met or bettered the mission requirements in all critical aspects. The most sensitive LNAs have reached new limits of noise temperature for HEMTs at their band centres. The FEMs have well-defined linear polarization characteristcs.
Notes:
A Cimatti, M Robberto, C Baugh, S V W Beckwith, R Content, E Daddi, G De Lucia, B Garilli, L Guzzo, G Kauffmann, M Lehnert, D Maccagni, A MartĂ­nez-Sansigre, F Pasian, I N Reid, P Rosati, R Salvaterra, M Stiavelli, Y Wang, M Z Osorio, M Balcells, M Bersanelli, F Bertoldi, J Blaizot, D Bottini, R Bower, A Bulgarelli, A Burgasser, C Burigana, R C Butler, S Casertano, B Ciardi, M Cirasuolo, M Clampin, S Cole, A Comastri, S Cristiani, J G Cuby, F Cuttaia, A de Rosa, A D Sanchez, M di Capua, J Dunlop, X Fan, A Ferrara, F Finelli, A Franceschini, M Franx, P Franzetti, C Frenk, J P Gardner, F Gianotti, R Grange, C Gruppioni, A Gruppuso, F Hammer, L Hillenbrand, A Jacobsen, M Jarvis, R Kennicutt, R Kimble, M Kriek, J Kurk, J P Kneib, O Le Fevre, D Macchetto, J MacKenty, P Madau, M Magliocchetti, D Maino, N Mandolesi, N Masetti, R McLure, A Mennella, M Meyer, M Mignoli, B Mobasher, E Molinari, G Morgante, S Morris, L Nicastro, E Oliva, P Padovani, E Palazzi, F Paresce, A Perez Garrido, E Pian, L Popa, M Postman, L Pozzetti, J Rayner, R Rebolo, A Renzini, H Röttgering, E Schinnerer, M Scodeggio, M Saisse, T Shanks, A Shapley, R Sharples, H Shea, J Silk, I Smail, P SpanĂł, J Steinacker, L Stringhetti, A Szalay, L Tresse, M Trifoglio, M Urry, L Valenziano, F Villa, I Villo Perez, F Walter, M Ward, R White, S White, E Wright, R Wyse, G Zamorani, A Zacchei, W W Zeilinger, F Zerbi (2009)  SPACE : the spectroscopic all-sky cosmic explorer   Experimental Astronomy 23: 39-66 mar  
Abstract: We describe the scientific motivations, the mission concept and the instrumentation of SPACE, a class-M mission proposed for concept study at the first call of the ESA Cosmic-Vision 2015-2025 planning cycle. SPACE aims to produce the largest three-dimensional evolutionary map of the Universe over the past 10 billion years by taking near-IR spectra and measuring redshifts for more than half a billion galaxies at 0 < z < 2 down to AB~23 over 3 Ï€ sr of the sky. In addition, SPACE will also target a smaller sky field, performing a deep spectroscopic survey of millions of galaxies to AB~26 and at 2 < z < 10 +. These goals are unreachable with ground-based observations due to the â‰500 times higher sky background (see e.g. Aldering, LBNL report number LBNL-51157, <CitationRef CitationID="CR2">2001</CitationRef>). To achieve the main science objectives, SPACE will use a 1.5 m diameter Ritchey-Chretien telescope equipped with a set of arrays of Digital Micro-mirror Devices covering a total field of view of 0.4 deg2, and will perform large-multiplexing multi-object spectroscopy (e.g. â‰6000 targets per pointing) at a spectral resolution of R~400 as well as diffraction-limited imaging with continuous coverage from 0.8 to 1.8 μm. Owing to the depth, redshift range, volume coverage and quality of its spectra, SPACE will reveal with unique sensitivity most of the fundamental cosmological signatures, including the power spectrum of density fluctuations and its turnover. SPACE will also place high accuracy constraints on the dark energy equation of state parameter and its evolution by measuring the baryonic acoustic oscillations imprinted when matter and radiation decoupled, the distance-luminosity relation of cosmological supernovae, the evolution of the cosmic expansion rate, the growth rate of cosmic large-scale structure, and high- z galaxy clusters. The datasets from the SPACE mission will represent a long lasting legacy for the whole astronomical community whose data will be mined for many years to come.
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J Varis, N J Hughes, M Laaninen, V H Kilpiä, P Jukkala, J Tuovinen, S Ovaska, P Sjöman, P Kangaslahti, T Gaier, R Hoyland, P Meinhold, A Mennella, M Bersanelli, R C Butler, F Cuttaia, E Franceschi, R Leonardi, P Leutenegger, M Malaspina, N Mandolesi, M Miccolis, T Poutanen, H Kurki-Suonio, M Sandri, L Stringhetti, L Terenzi, M Tomasi, L Valenziano (2009)  Design, development, and verification of the Planck Low Frequency Instrument 70 GHz Front-End and Back-End Modules   Journal of Instrumentation 4: T12001 dec  
Abstract: 70 GHz radiometer front-end and back-end modules for the Low Frequency Instrument of the European Space Agency's Planck Mission were built and tested. The operating principles and the design details of the mechanical structures are described along with the key InP MMIC low noise amplifiers and phase switches of the units. The units were tested in specially designed cryogenic vacuum chambers capable of producing the operating conditions required for Planck radiometers, specifically, a physical temperature of 20 K for the front-end modules, 300 K for the back-end modules and 4 K for the reference signal sources. Test results of the low noise amplifiers and phase switches, the front and back-end modules, and the combined results of both modules are discussed. At 70 GHz frequency, the system noise temperature of the front and back end is 28 K; the effective bandwidth 16 GHz, and the 1/f spectrum knee frequency is 38 mHz.The test results indicate state-of-the-art performance at 70 GHz frequency and fulfil the Planck performance requirements.
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L Terenzi, M Lapolla, M Laaninen, P Battaglia, F Cavaliere, A De Rosa, N Hughes, P Jukkala, V H Kilpiä, G Morgante, M Tomasi, J Varis, M Bersanelli, R C Butler, F Ferrari, C Franceschet, P Leutenegger, N Mandolesi, A Mennella, R Silvestri, L Stringhetti, J Tuovinen, L Valenziano, F Villa (2009)  Cryogenic environment and performance for testing the Planck radiometers   Journal of Instrumentation 4: T12015 dec  
Abstract: The Planck LFI Radiometer Chain Assemblies (RCAs) have been calibrated in two dedicated cryogenic facilities. In this paper the facilities and the related instrumentation are described. The main satellite thermal interfaces for the single chains have to be reproduced and stability requirements have to be satisfied. Setup design, problems occurred and improving solutions implemented are discussed. Performance of the cryogenic setup are reported.
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M Maris, M Tomasi, S Galeotta, M Miccolis, S Hildebrandt, M Frailis, R Rohlfs, N Morisset, A Zacchei, M Bersanelli, P Binko, C Burigana, R C Butler, F Cuttaia, H Chulani, O D’Arcangelo, S Fogliani, E Franceschi, F Gasparo, F Gomez, A Gregorio, J M Herreros, R Leonardi, P Leutenegger, G Maggio, D Maino, M Malaspina, N Mandolesi, P Manzato, M Meharga, P Meinhold, A Mennella, F Pasian, F Perrotta, R Rebolo, M TĂĽrler, A Zonca (2009)  Optimization of Planck-LFI on-board data handling   Journal of Instrumentation 4: T12018 dec  
Abstract: To asses stability against 1/f noise, the Low Frequency Instrument (LFI) on-board the Planck mission will acquire data at a rate much higher than the data rate allowed by the science telemetry bandwith of 35.5 Kbps. The data are processed by an on-board pipeline, followed on-ground by a decoding and reconstruction step, to reduce the volume of data to a level compatible with the bandwidth while minimizing the loss of information. This paper illustrates the on-board processing of the scientific data used by Planck/LFI to fit the allowed data-rate, an intrinsecally lossy process which distorts the signal in a manner which depends on a set of five free parameters (Naver, r1, r2, q, Script O) for each of the 44 LFI detectors. The paper quantifies the level of distortion introduced by the on-board processing as a function of these parameters. It describes the method of tuning the on-board processing chain to cope with the limited bandwidth while keeping to a minimum the signal distortion. Tuning is sensitive to the statistics of the signal and has to be constantly adapted during flight. The tuning procedure is based on a optimization algorithm applied to unprocessed and uncompressed raw data provided either by simulations, pre-launch tests or data taken in flight from LFI operating in a special diagnostic acquisition mode. All the needed optimization steps are performed by an automated tool, OCA2, which simulates the on-board processing, explores the space of possible combinations of parameters, and produces a set of statistical indicators, among them: the compression rate Cr and the processing noise epsilonQ. For Planck/LFI it is required that Cr = 2.4 while, as for other systematics, epsilonQ would have to be less than 10% of rms of the instrumental white noise. An analytical model is developed that is able to extract most of the relevant information on the processing errors and the compression rate as a function of the signal statistics and the processing parameters to be tuned. This model will be of interest for the instrument data analysis to asses the level of signal distortion introduced in the data by the on-board processing. The method was applied during ground tests when the instrument was operating in conditions representative of flight. Optimized parameters were obtained and inserted in the on-board processor and the performance has been verified against the requirements with the result that the required data rate of 35.5 Kbps has been achieved while keeping the processing error at a level of 3.8% of the instrumental white noise and well below the target 10% level.
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A Zonca, C Franceschet, P Battaglia, F Villa, A Mennella, O D’Arcangelo, R Silvestri, M Bersanelli, E Artal, R C Butler, F Cuttaia, R J Davis, S Galeotta, N Hughes, P Jukkala, V H Kilpiä, M Laaninen, N Mandolesi, M Maris, L Mendes, M Sandri, L Terenzi, J Tuovinen, J Varis, A Wilkinson (2009)  Planck-LFI radiometers’ spectral response   Journal of Instrumentation 4: T12010 dec  
Abstract: The Low Frequency Instrument (LFI) is an array of pseudo-correlation radiometers on board the Planck satellite, the ESA mission dedicated to precision measurements of the Cosmic Microwave Background. The LFI covers three bands centred at 30, 44 and 70 GHz, with a goal bandwidth of 20% of the central frequency. The characterization of the broadband frequency response of each radiometer is necessary to understand and correct for systematic effects, particularly those related to foreground residuals and polarization measurements. In this paper we present the measured band shape of all the LFI channels and discuss the methods adopted for their estimation. The spectral characterization of each radiometer was obtained by combining the measured spectral response of individual units through a dedicated RF model of the LFI receiver scheme. As a consistency check, we also attempted end-to-end spectral measurements of the integrated radiometer chain in a cryogenic chamber. However, due to systematic effects in the measurement setup, only qualitative results were obtained from these tests. The measured LFI bandpasses exhibit a moderate level of ripple, compatible with the instrument scientific requirements.
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P Meinhold, R Leonardi, B Aja, E Artal, P Battaglia, M Bersanelli, E Blackhurst, C R Butler, L P Cuevas, F Cuttaia, O D’Arcangelo, R Davis, M L de la Fuente, M Frailis, C Franceschet, E Franceschi, T Gaier, S Galeotta, A Gregorio, R Hoyland, N Hughes, P Jukkala, D Kettle, M Laaninen, P Leutenegger, S R Lowe, M Malaspina, R Mandolesi, M Maris, E MartĂ­nez-González, L Mendes, A Mennella, M Miccolis, G Morgante, N Roddis, M Sandri, M Seiffert, M SalmĂłn, L Stringhetti, T Poutanen, L Terenzi, M Tomasi, J Tuovinen, J Varis, L Valenziano, F Villa, A Wilkinson, F Winder, A Zacchei, A Zonca (2009)  Noise properties of the Planck-LFI receivers   Journal of Instrumentation 4: T12009 dec  
Abstract: The Planck Low Frequency Instrument (LFI) radiometers have been tested extensively during several dedicated campaigns. The present paper reports the principal noise properties of the LFI radiometers. A brief description of the LFI radiometers is given along with details of the test campaigns relevant to determination of noise properties. Current estimates of flight sensitivities, 1/f parameters, and noise effective bandwidths are presented. The LFI receivers exhibit exceptional 1/f noise, and their white noise performance is sufficient for the science goals of Planck.
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P Battaglia, C Franceschet, A Zonca, M Bersanelli, R C Butler, O D’Arcangelo, R J Davis, S Galeotta, P Guzzi, R Hoyland, N Hughes, P Jukkala, D Kettle, M Laaninen, R Leonardi, D Maino, N Mandolesi, P Meinhold, A Mennella, P Platania, L Terenzi, J Tuovinen, J Varis, F Villa, A Wilkinson (2009)  Advanced modelling of the Planck-LFI radiometers   Journal of Instrumentation 4: T12014 dec  
Abstract: The Low Frequency Instrument (LFI) is a radiometer array covering the 30-70 GHz spectral range on-board the ESA Planck satellite, launched on May 14th, 2009 to observe the cosmic microwave background (CMB) with unprecedented precision. In this paper we describe the development and validation of a software model of the LFI pseudo-correlation receivers which enables to reproduce and predict all the main system parameters of interest as measured at each of the 44 LFI detectors. These include system total gain, noise temperature, band-pass response, non-linear response. The LFI Advanced RF Model (LARFM) has been constructed by using commercial software tools and data of each radiometer component as measured at single unit level. The LARFM has been successfully used to reproduce the LFI behavior observed during the LFI ground-test campaign. The model is an essential element in the database of LFI data processing center and will be available for any detailed study of radiometer behaviour during the survey.
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A Mennella, F Villa, L Terenzi, F Cuttaia, P Battaglia, M Bersanelli, R C Butler, O D’Arcangelo, E Artal, R Davis, M Frailis, C Franceschet, S Galeotta, A Gregorio, N Hughes, P Jukkala, D Kettle, V H Kilpiä, M Laaninen, P M Lapolla, R Leonardi, P Leutenegger, S Lowe, N Mandolesi, M Maris, P Meinhold, L Mendes, M Miccolis, G Morgante, N Roddis, M Sandri, R Silvestri, L Stringhetti, M Tomasi, J Tuovinen, L Valenziano, A Zacchei, J Varis, A Wilkinson, A Zonca (2009)  The linearity response of the Planck-LFI flight model receivers   Journal of Instrumentation 4: T12011 dec  
Abstract: In this paper we discuss the linearity response of the Planck-LFI receivers, with particular reference to signal compression measured on the 30 and 44 GHz channels. In the article we discuss the various sources of compression and present a model that accurately describes data measured during tests performed with individual radiomeric chains. After discussing test results we present the best parameter set representing the receiver response and discuss the impact of non linearity on in-flight calibration, which is shown to be negligible.
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L Valenziano, F Cuttaia, A De Rosa, L Terenzi, A Brighenti, G P Cazzola, A Garbesi, S Mariotti, G Orsi, L Pagan, F Cavaliere, M Biggi, R Lapini, E Panagin, P Battaglia, R C Butler, M Bersanelli, O D’Arcangelo, S Levin, N Mandolesi, A Mennella, G Morgante, G Morigi, M Sandri, A Simonetto, M Tomasi, F Villa, M Frailis, S Galeotta, A Gregorio, R Leonardi, S R Lowe, M Maris, P Meinhold, L Mendes, L Stringhetti, A Zonca, A Zacchei (2009)  Planck-LFI : design and performance of the 4 Kelvin Reference Load Unit   Journal of Instrumentation 4: T12006 dec  
Abstract: The LFI radiometers use a pseudo-correlation design where the signal from the sky is continuously compared with a stable reference signal, provided by a cryogenic reference load system. The reference unit is composed by small pyramidal horns, one for each radiometer, 22 in total, facing small absorbing targets, made of a commercial resin ECCOSORB CRTM, cooled to ~ 4.5 K. Horns and targets are separated by a small gap to allow thermal decoupling. Target and horn design is optimized for each of the LFI bands, centered at 70, 44 and 30 GHz. Pyramidal horns are either machined inside the radiometer 20K module or connected via external electro-formed bended waveguides. The requirement of high stability of the reference signal imposed a careful design for the radiometric and thermal properties of the loads. Materials used for the manufacturing have been characterized for thermal, RF and mechanical properties. We describe in this paper the design and the performance of the reference system.
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F Cuttaia, A Mennella, L Stringhetti, M Maris, L Terenzi, M Tomasi, F Villa, M Bersanelli, R C Butler, B Cappellini, L P Cuevas, O D’Arcangelo, R Davis, M Frailis, C Franceschet, E Franceschi, A Gregorio, R Hoyland, R Leonardi, S Lowe, N Mandolesi, P Meinhold, L Mendes, N Roddis, M Sandri, L Valenziano, A Wilkinson, A Zacchei, A Zonca, P Battaglia, S De Nardo, S Grassi, M Lapolla, P Leutenegger, M Miccolis, R Silvestri (2009)  Planck-LFI radiometers tuning   Journal of Instrumentation 4: T12013 dec  
Abstract: This paper describes the Planck Low Frequency Instrument tuning activities performed through the ground test campaigns, from Unit to Satellite Levels. Tuning is key to achieve the best possible instrument performance and tuning parameters strongly depend on thermal and electrical conditions. For this reason tuning has been repeated several times during ground tests and it has been repeated in flight before starting nominal operations. The paper discusses the tuning philosophy, the activities and the obtained results, highlighting developments and changes occurred during test campaigns. The paper concludes with an overview of tuning performed during the satellite cryogenic test campaign (Summer 2008) and of the plans for the just started in-flight calibration.
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L Terenzi, M J Salmon, A Colin, A Mennella, G Morgante, M Tomasi, P Battaglia, M Lapolla, M Bersanelli, R C Butler, F Cuttaia, O D’Arcangelo, R Davis, C Franceschet, S Galeotta, A Gregorio, N Hughes, P Jukkala, D Kettle, M Laaninen, P Leutenegger, R Leonardi, N Mandolesi, M Maris, P Meinhold, M Miccolis, N Roddis, L Sambo, M Sandri, R Silvestri, J Tuovinen, L Valenziano, J Varis, F Villa, A Wilkinson, A Zonca (2009)  Thermal susceptibility of the Planck-LFI receivers   Journal of Instrumentation 4: T12012 dec  
Abstract: This paper describes the impact of the Planck Low Frequency Instrument front end physical temperature fluctuations on the output signal. The origin of thermal instabilities in the instrument are discussed, and an analytical model of their propagation and impact on the receivers signal is described. The experimental test setup dedicated to evaluate these effects during the instrument ground calibration is reported together with data analysis methods. Finally, main results obtained are discussed and compared to the requirements.
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2007
L Valenziano, M Sandri, G Morgante, C Burigana, M Bersanelli, R C Butler, F Cuttaia, F Finelli, E Franceschi, M Galaverni, A Gruppuso, M Malaspina, N Mandolesi, A Mennella, F Paci, L Popa, P Procopio, L Stringhetti, L Terenzi, M Tomasi, F Villa, J Zuccarelli (2007)  The low frequency instrument on-board the Planck satellite : Characteristics and performance   New Astronomy Review 51: 287-297 mar  
Abstract: Planck is the third generation space mission, after COBE/DMR and WMAP, devoted to image the CMBR anisotropies. The low frequency instrument (LFI) will simultaneously observe the sky in three frequency bands centered at 30, 44 and 70 GHz. It is composed by 11 pseudo-correlation receivers, actively cooled to 20 K, able to detect both orthogonal polarisation of the incoming signal. The LFI will be located, along with the high frequency instrument (HFI), in the focal region of a 1.5 m aperture telescope. The LFI will produce full-sky maps of the anisotropies of the CMBR with a FWHM angular resolution of 33′, 27′ and 14′ for the 30, 44 and 70 GHz LFI bands, respectively.
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L Terenzi, F Villa, A Mennella, M Bersanelli, R C Butler, F Cuttaia, O D’Arcangelo, E Franceschi, S Galeotta, D Maino, M Malaspina, N Mandolesi, G Morgante, M Sandri, L Stringhetti, M Tomasi, L Valenziano, C Burigana, F Finelli, M Galaverni, A Gruppuso, F Paci, L Popa, P Procopio, J Zuccarelli (2007)  The Planck LFI RCA flight model test campaign   New Astronomy Review 51: 305-309 mar  
Abstract: The Planck satellite is the third generation of space missions devoted to cosmic microwave background (CMB) measurements. It will perform two sky surveys and measure the CMB anisotropies and polarization between 30 and 850 GHz. The low frequency instrument is an array of 22 pseudo-correlation radiometers at 30, 44, and 70 GHz. Before integrating the complete array assembly, a first set of tests is performed for each radiometer chain assembly (RCA), consisting of two radiometers. In this paper, the test campaign experimental setup and methods are discussed.
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2005
N Figueiredo, M Bersanelli, J Childers, O D’Arcangelo, D Halevi, M Janssen, K Kedward, N Lemaster, P Lubin, N Mandolesi, J Marvil, P Meinhold, J MejĂ­a, A Mennella, P Natoli, H O’Neil, A Pina, M Pryor, M Sandri, A Simonetto, C Sozzi, C Tello, F Villa, T Villela, B Williams, C A Wuensche (2005)  The Optical Design of the Background Emission Anisotropy Scanning Telescope (BEAST)   \apjs 158: 118-123 may  
Abstract: We present the optical design of the Background Emission Anisotropy Scanning Telescope (BEAST), an off-axis Gregorian telescope designed to measure the angular distribution of the cosmic microwave background radiation (CMBR) at 30 and 41.5 GHz on angular scales ranging from 20' to 10°. The aperture of the telescope is 1.9 m, and our design meets the strict requirements imposed by the scientific goals of the mission: the beam size is 20' at 41.5 GHz and 26' at 30 GHz, while the illumination at the edge of the mirrors is lower than -30 dB for the central horn. The primary mirror is an off-axis section of a paraboloid, and the secondary an off-axis section of an ellipsoid. A spinning flat mirror located between the sky and the primary provides a two-dimensional chop by rotating the beams around an ellipse on the sky. BEAST uses a receiver array of cryogenic low noise InP High Electron Mobility Transistor (HEMT) amplifiers. The baseline array has seven horns matched to one amplifier each and one horn matched to two amplifiers (two polarizations) for a total of nine amplifiers. Two horns operate around 30 GHz, and six operate around 41.5 GHz. Subsequent campaigns will include 90 GHz and higher frequency channels.
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2004
M Maris, A Mennella, L Terenzi, D Maino, G Morgante, M Prina, F Pasian, M Bersanelli (2004)  Reconstruction and Removal of Thermal Effects in Planck/LFI Scientific Data Streams Using Telemetry Information   Memorie della Societa Astronomica Italiana Supplement 5:  
Abstract: The ESA CMB Planck mission will require an accurate control and removal of instrumental systematics below a level of few mu K. Telemetry information monitoring the instrument status may improve the effectiveness of procedures for the removal of systematic effects in the time domain. A good example is given by thermal instabilities of the 20 K stage of the PLANCK cooling chain. A successful, yet simple approach, based on the use of telemetry information has been developed and is presented here.
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F Cuttaia, L Valenziano, M Bersanelli, R C Butler, O D’Arcangelo, D Kettle, S Levin, N Mandolesi, A Mennella, G Morgante, G Morigi, N Roddis, A Simonetto, L Terenzi, M Tomasi, F Villa (2004)  Analysis of the radiometer-reference load system on board the Planck/LFI instrument   Nuclear Instruments and Methods in Physics Research A 520: 396-401 mar  
Abstract: The Low Frequency Instrument aboard the Planck satellite will employ pseudo-correlation radiometers, operating over three broad bands centered at 30, 44, 70GHz. This choice is oriented to maximize the instrumental stability reducing non-white noise effects produced inside the radiometers. The radiometer scheme allows the simultaneous comparison of two input signals, one coming from the telescope and the other coming from a reference blackbody (the ``reference load'' RL) at a stable temperature near 4K. In order to minimize non-white noise, typically exhibiting a 1/f spectrum, the Reference Load temperature must be as close as possible to the sky temperature (about 2.7K). The accuracy of the measurement is tightly related to the ability of keeping under control and minimizing all systematic effects potentially perturbing the RL signal, particularly those not easily removable in software during data analysis. A model of the radiometer and RL system interface, based on the finite elements method, has been developed, together with a detailed thermal modeling, to characterize the physical system and to optimize its performance. The function of the radiometric chain, the modeling and the changes made in the baseline configuration to improve the system performances are described. The impact of systematic effects on the optimized configuration are also quantitatively investigated.
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L Terenzi, A Mennella, M Bersanelli, N Mandolesi, G Morgante, M Prina, M Tomasi, L Valenziano (2004)  Thermal stability in precision cosmology experiments : the Planck LFI case   Nuclear Instruments and Methods in Physics Research A 520: 393-395 mar  
Abstract: After the great success of NASA's satellite missions COBE and WMAP, the Planck mission represents the third generation of mm-wave instruments designed for space observations of CMB anisotropies. Two instruments, the Low-Frequency Instrument (LFI) and the High-Frequency Instrument (HFI) will produce CMB maps with unprecedented angular resolution, sensitivity and frequency coverage. This ambitious task will be achieved by using low noise HEMT detectors cryogenically cooled at ~20K for the LFI and bolometric detectors cooled at 0.1K for the HFI; in particular, the LFI is based on pseudo-correlation receivers in which the sky signal is continuously compared to a cryogenic reference load in thermal contact with the HFI 4K stage. Such high sensitivity in Planck detectors calls for a strict control of systematic effects, which must be kept at μK level in the final maps; this in turn imposes tight requirements on the thermal and electrical stability of the different stages in the instrument. In this paper we discuss a study of the impact of thermal fluctuations at the level of the 20K cooler cold-end on the Planck-LFI measurements and present some viable solutions that have been adopted to keep the residual systematic error within the required values for Planck-LFI.
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M Maris, D Maino, C Burigana, A Mennella, M Bersanelli, F Pasian (2004)  The effect of signal digitisation in CMB experiments   A&A 414: 777-794 feb  
Abstract: Signal digitisation may produce significant effects in balloon - borne or space CMB experiments, when the limited bandwidth for downlink of data requires loss-less data compression. In fact, the data compressibility depends on the quantization step q applied on board by the instrument acquisition chain. In this paper we present a study of the impact of the quantization error in CMB experiments using, as a working case, simulated data from the PLANCK/LFI 30 and 100 GHz channels. At TOD level, the effect of the quantization can be approximated as a source of nearly normally distributed noise, with RMS ≠q/\sqrt{12 Ns}, with deviations from normality becoming relevant for a relatively small number of repeated measures Ns ⪉ 20. At map level, the data quantization alters the noise distribution and the expectation of some higher order moments. We find a constant ratio, ≠1/({\sqrt{12}Ï/q}), between the RMS of the quantization noise and RMS of the instrumental noise, Ï over the map (≠0.14 for Ï/q ≠2), while, for Ï/q Ëś 2, the bias on the expectation for higher order moments is comparable to their sampling variances. Finally, we find that the quantization introduces a power excess, Câ„“ex, that, although related to the instrument and mission parameters, is weakly dependent on the multipole â„“ at middle and large â„“ and can be quite accurately subtracted. For Ï/q ≠2, the residual uncertainty, Δ Câ„“ex, implied by this subtraction is only â‰1-2% of the RMS uncertainty, Δ Câ„“noise, on Câ„“sky reconstruction due to the noise power, Câ„“noise. Only for â„“ ⪉ 30 the quantization removal is less accurate; in fact, the 1/f noise features, although efficiently removed, increase Câ„“noise, Δ Câ„“noise, Câ„“ex and then Δ Câ„“ex; anyway, at low multipoles Câ„“sky ≫ Δ Câ„“noise > Δ Câ„“ex. This work is based on PLANCK LFI activities.
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A Zacchei, M Maris, S Fogliani, M Salomon, D Maino, E Franceschi, M Malaspina, A Mennella, P Leutenegger, M Miccolis, F Pasian, M Bersanelli (2004)  Planck/LFI Ground Tests : data management and analysis   Memorie della Societa Astronomica Italiana Supplement 5:  
Abstract: Ground Tests are a fundamental milestone within the development of the Low Frequency Instrument (LFI) which will fly onboard the ESA satellite PLANCK. They allow the collection of information which can not be supplied by monitoring onboard activity of the satellite during operations. Here methods and principles driving the management and elaboration of data collected during the Ground Tests campaign for the PLANCK/LFI are synthetically presented. Ground Tests take place in LABEN (Milano) and will last for about one year.
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M Sandri, M Bersanelli, C Burigana, R C Butler, F Cuttaia, F Finelli, E Franceschi, A Gruppuso, M Malaspina, N Mandolesi, A Mennella, G Morgante, G Morigi, L Popa, L Terenzi, L Valenziano, F Villa, L F I Consortium (2004)  PLANCK Low Frequency Instrument : towards a final imaging of the CMB anisotropies   Memorie della Societa Astronomica Italiana Supplement 5:  
Abstract: PLANCK is the third generation of mm-wave instruments designed for space observations of the cosmic microwave background (CMB) anisotropies within the new Cosmic Vision 2020 ESA Science Program. PLANCK will map the whole sky with unprecedented sensitivity, angular resolution, and frequency coverage, and it likely leads us to the final comprehension of the CMB anisotropies. The Low Frequency Instrument (LFI), operating in the 30 / 70 GHz range, is one of the two instruments onboard PLANCK satellite, sharing the focal region of a 1.5 meter off-axis dual reflector telescope together with the High Frequency Instrument (HFI) operating at 100 / 857 GHz. We present LFI and discuss the major instrumental systematic effects that could degrade the measurements and the solutions adopted in the design phase in order to adequately reduce and control them.
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2003
P Platania, C Burigana, D Maino, E Caserini, M Bersanelli, B Cappellini, A Mennella (2003)  Full sky study of diffuse Galactic emission at decimeter wavelenghts   A&A 410: 847-863 nov  
Abstract: A detailed knowledge of the Galactic radio continuum is of high interest for studies of the dynamics and structure of the Galaxy as well as for the problem of foreground removal in Cosmic Microwave Background measurements. In this work we present a full-sky study of the diffuse Galactic emission at frequencies of few GHz, where synchrotron radiation is by far the dominant component. We perform a detailed combined analysis of the extended surveys at 408, 1420 and 2326 MHz (by Haslam et al. 1982; Reich 1982; Reich & Reich 1986; Jonas et al. 1998, respectively). Using the technique applied by Schlegel et al. (1998) to the IRAS data, we produce destriped versions of the three maps. This allows us to construct a nearly-full-sky map of the spectral index and of the normalization factor with sub-degree angular resolution. The resulting distribution of the spectral indices has an average of bar beta = 2.695 and dispersion sigma beta = 0.120. This is representative for the Galactic diffuse synchrotron emission, with only minor effects from free-free emission and point sources. The maps produced in this work are available via ftp at cdsarc.u-strasbg.fr The maps produced in this work are only available in electronic form via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsweb.u-strasbg/cgi-bin/qcat?J/A+A/410/847 Colour figures are only available in the electronic edition of this paper via http://www.edpsciences.org
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O D’Arcangelo, S Garavaglia, A Simonetto, C Sozzi, M Bersanelli, A Mennella, F Villa (2003)  Measurements of Beam Pattern Perturbation in Corrugated Feed Horn Arrays for CMB Observations   Experimental Astronomy 16: 165-187 dec  
Abstract: An experimental study on the perturbation of the angular response of a W-band corrugated horn produced by nearby feeds, reproducing a typical situation of multi-feed arrays commonly used in high sensitivity Cosmic Microwave Background instruments, is reported in this paper. The effects for different positions of the scattering horn in the two principal polarisation planes were measured. We analyze the effects on both the side-lobe level and on the main beam. In particular, these results allowed us to validate design criterion for the multi-frequency focal array of the ESA PLANCK mission.
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A Mennella, M Bersanelli, M Seiffert, D Kettle, N Roddis, A Wilkinson, P Meinhold (2003)  Offset balancing in pseudo-correlation radiometers for CMB measurements   A&A 410: 1089-1100 nov  
Abstract: Radiometric CMB measurements need to be highly stable and this stability is best obtained with differential receivers. The residual 1/f noise in the differential output is strongly dependent on the radiometer input offset which can be cancelled using various balancing strategies. In this paper we discuss a software method implemented in the PLANCK-LFI pseudo-correlation receivers which uses a tunable gain modulation factor, r, in the sky-load difference. Numerical simulations and experimental data show how proper tuning of the parameter r ensures a very stable differential output with knee frequencies of the order of few mHz. Various approaches to calculate r using the radiometer total power data are discussed with some examples relevant to PLANCK-LFI. Although the paper focuses on pseudo-correlation receivers and the examples are relative to PLANCK-LFI, the proposed method and its analysis is general and can be applied to a large class of differential radiometric receivers.
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P Platania, C Burigana, D Maino, E Caserini, M Bersanelli, B Cappellini, A Mennella (2003)  Galactic emission at decimeter wavelengths (Platania+, 2003)   VizieR Online Data Catalog 341: oct  
Abstract: The diffuse galactic emission maps at decimeter wavelengths (408 MHz, Haslam et al., 1982A&AS...47....1H), (1420 MHz, Reich, 1982A&AS...48..219R, Reich & Reich 1986A&AS...63..205R), (2326 MHz, Jonas et al., 1998MNRAS.297..977J) have been destriped using the method proposed by Schlegel et al., 1998ApJ...500..525S. Statistical and systematic errors have been evaluated for each map. Each map is presented in two different pixelizations: ECP (Cartesian Projection) and HEALPix. In the case of HEALPix pixelization (in which the pixel area is constant), we omitted the (constant) error maps; the statistical and systematic errors for each map are summarized in the "Table 2" section below. Synchrotron spectral index and normalization factor have been evaluated using the three destriped surveys. Some of the results in this work have been derived using the HEALPix (Gorski et al., 1999, Proceedings of the MPA/ESO Conference on Evolution of Large-Scale Structure: from Recombination to Garching, ed. A.J. Banday, R.K. Sheth, & L. Da Costa, 37).
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B Cappellini, D Maino, G Albetti, P Platania, R Paladini, A Mennella, M Bersanelli (2003)  Optimized in-flight absolute calibration for extended CMB surveys   A&A 409: 375-385 oct  
Abstract: Accurate measurements of the Cosmic Microwave Background (CMB) anisotropy call for high precision and reliability of the in-flight calibration. For extended surveys the CMB dipole provides an excellent calibration source at frequencies lower than ~ 200 GHz; however poorly known foreground emissions, such as diffuse galactic components, complicate the signal and introduce a systematic error in the calibration. We show that introducing a weight function that takes into account the uncertainty in the a priori knowledge of the sky, allows us to substantially improve the calibration accuracy with respect to methods involving galactic latitude cuts. This new method is tested for PLANCK-LFI radiometers at 30 and 100 GHz. On short time scales (less than 1 day) the absolute calibration of each channel can be recovered with an overall 1-2% accuracy. We also consider the effect of CMB anisotropy itself on the calibration, and find that knowledge of the CMB pattern on large scales is needed to keep the short-time scale calibration accuracy within 1%.
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M Maris, D Maino, C Burigana, A Mennella, M Bersanelli, F Pasian (2003)  The scientific impact of signal quantization on Planck/LFI observations   Memorie della Societa Astronomica Italiana 74:  
Abstract: The real data processing of the signal observed by the Planck Low Frequency Instrument (LFI) introduces systematic effects in the time ordered data (TOD), maps and, finally, in the reconstruction of the sky angular power spectrum C_lsky. With analytical and numerical methods we studied the signal quantization of LFI TOD in order to evaluate the possibility to model and remove its effect on the C_lsky recovery. We find that it introduces a power excess, C_lex, only weakly dependent on the multipole l at middle and large l. It can be quite accurately subtracted, leaving an uncertainty, Delta C_lex, of only 1-2% of the RMS uncertainty, Delta C_lnoise, on C_lsky reconstruction due to the noise power, C_lnoise.
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2002
A Mennella, M Bersanelli, C Burigana, D Maino, N Mandolesi, G Morgante, G Stanghellini (2002)  PLANCK : Systematic effects induced by periodic fluctuations of arbitrary shape   A&A 384: 736-742 mar  
Abstract: A fundamental requirement in the new generation of high resolution Cosmic Microwave Background imaging experiments is a strict control of systematic errors that must be kept at $\mu$K level in the final maps. Some of these errors are of celestial origin, while others will be generated by periodic fluctuations of the satellite environment. These environment instabilities will cause fluctuations in the measured signal output thus generating correlated effects in the reconstructed maps. In this paper we present an analytical study of the impact of periodic signal fluctuations on the measured sky maps produced by the PLANCK survey. In particular we show how it is possible to estimate analytically the damping factor of the peak-to-peak amplitude of the fluctuation at the instrument output after the projection in the final maps.
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F Villa, M Sandri, N Mandolesi, R Nesti, M Bersanelli, A Simonetto, C Sozzi, O D’Arcangelo, V Muzzini, A Mennella, P Guzzi, P Radaelli, R Fusi, E Alippi (2002)  High Performance Corrugated Feed Horns for Space Applications at Millimetre Wavelengths   Experimental Astronomy 14: 1-15 aug  
Abstract: We report on the design fabrication and testing of a set of high performance corrugated feed horns at 30, 70, and 100 GHz, built as advanced prototypes for the Low Frequency Instrument (LFI) of the ESA Planck mission. The electromagnetic designs include linear (100 GHz) and dual shaped (30 and 70 GHz) profiles. Fabrication has been achieved by direct machining at 30 GHz and by electro-formation at higher frequencies. The measured performances on side lobe and return loss meet the stringent Planck requirements over the large (20%) instrument bandwidth. Moreover, the advantage in terms of main lobe shape and side lobe levels of the dual profiled designs has been demonstrated.
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M Seiffert, A Mennella, C Burigana, N Mandolesi, M Bersanelli, P Meinhold, P Lubin (2002)  1/f noise and other systematic effects in the Planck-LFI radiometers   A&A 391: 1185-1197 sep  
Abstract: We use an analytic approach to study the susceptibility of the PLANCK Low Frequency Instrument radiometers to various systematic effects. We examine the effects of fluctuations in amplifier gain, in amplifier noise temperature and in the reference load temperature. We also study the effect of imperfect gain modulation, non-ideal matching of radiometer parameters, imperfect isolation in the two legs of the radiometer and back-end 1/f noise. We find that with proper gain modulation 1/f gain fluctuations are suppressed, leaving fluctuations in amplifier noise temperature as the main source of 1/f noise. We estimate that with a gain modulation factor within +/- 1% of its ideal value the overall 1/f knee frequency will be relatively small (<0.1 Hz).
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M Bersanelli, D Maino, A Mennella (2002)  Anisotropies of the cosmic microwave background   Nuovo Cimento Rivista Serie 25: 9. 090000-82 sep  
Abstract: We review the present status of Cosmic Microwave Background (CMB) anisotropy observations and discuss the main related astrophysical issues, instrumental effects and data analysis techniques. We summarise the balloon-borne and ground-based experiments that, after COBE-DMR, yielded detection or significant upper limits to CMB fluctuations. A comparison of subsets of combined data indicates that the acoustic features observed today in the angular power spectrum are not dominated by undetected systematics. Pushing the accuracy of CMB anisotropy measurements to their ultimate limits represents one of the best opportunities for cosmology to develop into a precision science in the next decade. We discuss the forthcoming sub-orbital and space programs, as well as future prospects of CMB observations.
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2001
1999
1998
1995
1993
D Farina, R Pozzoli, A Mennella, D Ronzio (1993)  Stochastic energy diffusion of electrons in a plasma by an electron cyclotron wave   Physics of Fluids B 5: 104-111 jan  
Abstract: The investigation of the energy diffusion process of the electrons in a magnetized plasma due to an electron cyclotron wave in perpendicular propagation with respect to the magnetic field is performed. Starting from the description of the relativistic electron motion by means of an actionâ€angle Hamiltonian H(I,θ,t), the Fokker–Planck–Kolmogorov (FPK) approach to the diffusion is considered for a globally stochastic regime of the system. In this regime, the phase correlation process is analyzed, and the characteristic decay time is estimated analytically. The action diffusion coefficient D(I) is derived and compared with a local quasilinear expression. With explicit reference to the lowâ€density regime, where D increases with I, and is very close to the quasilinear coefficient, the solution of the diffusion equation is compared with the results obtained by direct numerical integration of the motion equations for a statistically significant ensemble of particles. A good agreement with the local quasilinear FPK diffusion is observed. In addition, when the amplitude of the perturbation is varied, oscillations of the average action values around the quasilinear results are found on the long time scale.
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A Mennella, F Prodi (1993)  Optical characterization of size separated aerosol particles of different composition and morphology with a polar nephelometer   Pure Applied Optics 2: 471-488 sep  
Abstract: A new technique for the determination of the complex refractive index of aerosol particles has been developed. The particles are deposited on a membrane filter by means of an aerosol inertial spectrometer, in order to have fixed and size-separated particles. The filter is then made transparent by exposure to acetone vapours and the sample inspected with a laser beam. Scattering data are then analysed and the complex refractive index is obtained. Data and results are presented for a number of materials.
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1990

Conference papers

2006
M Tomasi, P Battaglia, M Bersanelli, F Cuttaia, C Franceschet, M Lapolla, R Leonardi, P Leutenegger, D Maino, P Meinhold, A Mennella, M Miccolis, T Poutanen, M Salmon, M Sandri, L Stringhetti, L Terenzi (2006)  Data analysis of the Planck/LFI ground-test campaign   In: Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series  
Abstract: The ESA Planck mission is the third generation (after COBE and WMAP) space experiment dedicated to the measurement of the Cosmic Microwave Background (CMB) anisotropies. Planck will map the whole CMB sky using two instruments in the focal plane of a 1.5 m off-axis aplanatic telescope. The High Frequency Instrument (HFI) is an array of 52 bolometers in the frequency range 100-857 GHz, while the Low Frequency Instrument (LFI) is an array of 11 pseudo-correlation radiometric receivers which continuously compare the sky signal with the reference signal of a blackbody at ~ 4.5 K. The LFI has been tested and calibrated at different levels of integration, i.e. on the single units (feed-horns, OMTs, amplifiers, waveguides, etc.), on each integrated Radiometric Chain Assembly (RCA) and finally on the complete instrument, the Radiometric Array Assembly (RAA). In this paper we focus on some of the data analysis algorithms and methods that have been implemented to estimate the instrument performance and calibration parameters. The paper concludes with the discussion of a custom-designed software package (LIFE) that allows to access the complex data structure produced by the instrument and to estimate the instrument performance and calibration parameters via a fully graphical interface.
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N Morisset, R Rohlfs, M TĂĽrler, A Mennella, M Maris, S Fogliani, X Dupac, A Zacchei, D Maino (2006)  Planck LFI Data Processing During Instrument Calibration Tests   In: Astronomical Data Analysis Software and Systems XV Edited by:C Arviset, D Ponz, & S Enrique C. Gabriel.  
Abstract: The qualification model of the Low Frequency Instrument (LFI) of the Planck satellite was tested and calibrated during several weeks at Laben, Milan, Italy. The level 1 pipeline system (the Demonstration Model) was used to receive the data from the instrument, decode the telemetry packets, decompress the data and store the data in FITS files. Graphical tools have been developed to visualize the scientific and housekeeping data and display them in real time. The same tools are also used to display the archived data. Hereafter, we present the level 1 data processing software components, the display tools and the upgrades needed for the creation of the Operations Model, that will be used during the Planck
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M Tomasi, G Baldan, M Lapolla, A Mennella, G Morgante, L Pagan, L Terenzi (2006)  Thermal models of the Planck/LFI QM/FM instruments   In: Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series  
Abstract: The ESA Planck mission is the third generation (after COBE and WMAP) space experiment dedicated to the measurement of the Cosmic Microwave Background (CMB) anisotropies. Two instruments will be integrated onboard: the High Frequency Instrument (HFI), an array of bolometers, and the Low Frequency Instrument (LFI), an array of pseudo-correlation HEMT radiometers. In this paper we will discuss the development of analytical and numerical models to estimate the thermal behavior of LFI, both in steady-state and transient conditions. We then describe their application to the qualification model (QM) tests. QM test data were also used to calibrate the numerical models. Finally, we show some examples about how these models can be used in predicting the instrument performances and the impact of thermal systematic effects on the scientific results.
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A Mennella, B Aja, E Artal, M Balasini, G Baldan, P Battaglia, T Bernardino, M Bersanelli, E Blackhurst, L Boschini, C Burigana, R C Butler, B Cappellini, F Colombo, F Cuttaia, O D’Arcangelo, S Donzelli, R Davis, L De La Fuente, F Ferrari, L Figini, S Fogliani, C Franceschet, E Franceschi, T Gaier, S Galeotta, S Garavaglia, A Gregorio, M Guerrini, R Hoyland, N Hughes, P Jukkala, D Kettle, M Laaninen, P M Lapolla, D Lawson, R Leonardi, P Leutenegger, G Mari, P Meinhold, M Miccolis, D Maino, M Malaspina, N Mandolesi, M Maris, E Martinez-Gonzalez, G Morgante, L Pagan, F Pasian, P Platania, M Pecora, S Pezzati, L Popa, T Poutanen, M Pospieszalski, N Roddis, M Salmon, M Sandri, R Silvestri, A Simonetto, C Sozzi, L Stringhetti, L Terenzi, M Tomasi, J Tuovinen, L Valenziano, J Varis, F Villa, A Wilkinson, F Winder, A Zacchei (2006)  Calibration and testing of the Planck-LFI QM instrument   In: Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series  
Abstract: In this paper we present the test results of the qualification model (QM) of the LFI instrument, which is being developed as part of the ESA Planck satellite. In particular we discuss the calibration plan which has defined the main requirements of the radiometric tests and of the experimental setups. Then we describe how these requirements have been implemented in the custom-developed cryo-facilities and present the main results. We conclude with a discussion of the lessons learned for the testing of the LFI Flight Model (FM).
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2005
M Bersanelli, B Aja, E Artal, M Balasini, G Baldan, P Battaglia, T Bernardino, P Bhandari, E Blackhurst, L Boschini, R Bowman, C Burigana, R C Butler, B Cappellini, F Cavaliere, F Colombo, F Cuttaia, R Davis, X Dupac, J Edgeley, O D’Arcangelo, L de La Fuente, A de Rosa, F Ferrari, L Figini, S Fogliani, C Franceschet, E Franceschi, P Jukkala, T Gaier, A Galtress, S Garavaglia, F Gomez-Renasco, P Guzzi, J M Herreros, R Hoyland, N Huges, D Kettle, V H Kilpel, M Laaninen, M Lapolla, C R Lawrence, D Lawson, R Leonardi, P Leutenegger, S Levin, P B Lilje, P M Lubin, D Maino, M Malaspina, N Mandolesi, G Mari, M Maris, E Martinez-Gonzalez, A Mediavilla, P Meinhold, A Mennella, M Miccolis, G Morgante, A Nash, R Nesti, L Pagan, C Paine, J P Pascual, F Pasian, M Pecora, S Pezzati, M Pospieszalski, P Platania, M Prina, R Rebolo, N Roddis, N Sabatini, M Sandri, M J Salmon, M Seiffert, R Silvestri, A Simonetto, G F Smoot, C Sozzi, L Stringhetti, L Terenzi, M Tomasi, J Tuovinen, L Valenziano, J Varis, F Villa, L Wade, A Wilkinson, F Winder, A Zacchei (2005)  Planck-LFI : Instrument Design and Ground Calibration Strategy   In: Journal of the European Microwave Association Vol. 1, Issue 3 : p. 189-195 189-195  
Abstract: We present the optical design of the Background Emission Anisotropy Scanning Telescope (BEAST), an off-axis Gregorian telescope designed to measure the angular distribution of the cosmic microwave background radiation (CMBR) at 30 and 41.5 GHz on angular scales ranging from 20' to 10°. The aperture of the telescope is 1.9 m, and our design meets the strict requirements imposed by the scientific goals of the mission: the beam size is 20' at 41.5 GHz and 26' at 30 GHz, while the illumination at the edge of the mirrors is lower than -30 dB for the central horn. The primary mirror is an off-axis section of a paraboloid, and the secondary an off-axis section of an ellipsoid. A spinning flat mirror located between the sky and the primary provides a two-dimensional chop by rotating the beams around an ellipse on the sky. BEAST uses a receiver array of cryogenic low noise InP High Electron Mobility Transistor (HEMT) amplifiers. The baseline array has seven horns matched to one amplifier each and one horn matched to two amplifiers (two polarizations) for a total of nine amplifiers. Two horns operate around 30 GHz, and six operate around 41.5 GHz. Subsequent campaigns will include 90 GHz and higher frequency channels.
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M Sandri, F Villa, C Burigana, A Mennella, R Nesti, N Mandolesi, M Bersanelli (2005)  Straylight analysis and minimization strategy in PLANCK low frequency instrument   In: Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Edited by:L Mazuray & R Wartmann. 575-586  
Abstract: PLANCK is the space mission of the European Space Agency devoted to measure of the anisotropies of the cosmic microwave background (CMB), the relic radiation left by the big bang. The satellite will be launched in 2007 and it will carry state-of-the-art of microwave radiometers and bolometers arranged in two instruments, respectively the Low Frequency Instrument and the High Frequency Instrument, both coupled with a 1.5 m telescope and working in nine frequency channels between 30 and 857 GHz. From the second Lagrangian point of the Sun-Earth system, the instruments will produce a survey that will cover the whole sky with unprecedented combination of sensitivity, angular resolution, and frequency coverage, and they will likely lead us to extract all the cosmological information encoded in the CMB temperature anisotropies. The development strategy of PLANCK and the two instruments has been to set up a mission that inherently minimizes the systematic effects. The optics, composed by an optimised telescope-feed array assembly, introduce unwanted systematic effects in the measurements like the so called external straylight due to the sidelobe pick-up. A trade-off between angular resolution and external straylight has been carried out for LFI in order to reach the best optical performances preventing the Galactic contamination. The main product of the study has been the definition of the internal geometry of the flight model of the LFI feed horns and the characterization of the overall optical response of the instrument. Thermal emission from all components of the spacecraft produces the so called internal straylight, that has been evaluated and controlled in the design phase. In this paper we present the study carried out on the minimization of straylight contamination in PLANCK LFI.
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2004
A Mennella, M Bersanelli, B Cappellini, D Maino, P Platania, S Garavaglia, R C Butler, N Mandolesi, F Pasian, O D’Arcangelo, A Simonetto, C Sozzi (2004)  The Low Frequency Instrument in the ESA PLANCK mission   In: Plasmas in the Laboratory and in the Universe : New Insights and New Challenges Edited by:D Farina, & R Pozzoli G. Bertin. 401-404  
Abstract: Measurements of the cosmic microwave background (CMB) allow high precision observation of the cosmic plasma at redshift z ~1100. After the success of the NASA satellite COBE, that in 1992 provided the first detection of the CMB anisotropy, results from many ground-based and balloon-borne experiments have showed a remarkable consistency between different results and provided quantitative estimates of fundamental cosmological properties. During the current year the team of the NASA WMAP satellite has released the first improved full-sky maps of the CMB since COBE, leading to a deeper insight in the origin and evolution of the Universe. The ESA satellite PLANCK, scheduled for launch in 2007, is designed to provide the ultimate measurement of the CMB temperature anisotropy over the full sky, with an accuracy that will be limited only by astrophysical foregrounds, and robust detection of polarisation anisotropy. PLANCK will observe the sky with two instruments over a wide spectral band (the Low Frequency Instrument, based on coherent radiometers, from 30 to 70 GHz and the High Frequency Instrument, based on bolometric detectors, from 100 to 857 GHz). The mission performances will improve dramatically the scientific return compared to WMAP. Furthermore the LFI radiometers (as well as some of the HFI bolometers) are intrinsically sensitive to polarisation so that by combining the data from different receivers it will be possible to measure accurately the E mode and to detect the B mode of the polarisation power spectrum. PLANCK sensitivity will offer also the possibility to detect the non-Gaussianities imprinted in the CMB.
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P Platania, R Paladini, B Cappellini, D Maino, C Burigana, M Bersanelli, A Mennella (2004)  Probing Galactic Plasma with Radio Measurements   In: Plasmas in the Laboratory and in the Universe : New Insights and New Challenges Edited by:D Farina, & R Pozzoli G. Bertin. 405-408  
Abstract: The detailed study of radio continuum emission allows a direct evaluation of the conditions of the Galactic plasma as well as of some important parameters describing the dynamics and structure of the Galaxy. An additional, independent motivation for accurate knowledge of the diffuse Galactic background is that such emission represents one of the main sources of unwanted signal in experiments dedicated to measure the Cosmic Microwave Background (CMB). The mechanism responsible for radio continuum from the Galactic plasma are synchrotron and thermal Bremsstrahlung emissions. In this work we present the results of our analysis on diffuse synchrotron emission: we revised the current status of data and removed systematic effects in present surveys with the aim to construct detailed maps of the spectral index and normalization factor over the whole observed sky with sub-degree angular resolution. The resulting distribution of the spectral index is representative for the Galactic diffuse synchrotron emission, with only minor effects from free-free and point sources. Moreover we present the most up-to-date compilation of HII regions comprising 1422 objects for which we study the level of completness as well as their spatial distribution. We further investigate their properties constructing a 3-D distribution of the sampled HII regions as a function of their distance from the Sun. This catalog could be extremely useful for present and future microwave CMB experiments.
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M Bersanelli, D Maino, A Mennella (2004)  Current Status and Perspectives of Cosmic Microwave Background Observations   In: Plasmas in the Laboratory and in the Universe : New Insights and New Challenges Edited by:D Farina, & R Pozzoli G. Bertin. 385-390  
Abstract: Measurements of the cosmic microwave background (CMB) radiation provide a unique opportunity for a direct study of the primordial cosmic plasma at redshift z ~10^3. The angular power spectra of temperature and polarisation fluctuations are powerful observational objectives as they encode information on fundamental cosmological parameters and on the physics of the early universe. A large number of increasingly ambitious balloon-borne and ground-based experiments have been carried out following the first detection of CMB anisotropies by COBE-DMR, probing the angular power spectrum up to high multipoles. The recent data from WMAP provide a new major step forward in measurements percision. The ESA mission ``Planck Surveyor'', to be launched in 2007, is the third-generation satellite devoted to CMB imaging. Planck is expected to extract the full cosmological information from temperature anisotropies and to open up new fronteers in the CMB field.
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F Cuttaia, P Battaglia, L Terenzi, C Franceschet, M Bersanelli, C Burigana, C R Butler, O D’Arcangelo, P Guzzi, D Maino, N Mandolesi, A Mennella, G Morgante, A Simonetto, L Valenziano, F Villa (2004)  Analysis of the pseudocorrelation radiometers for the low frequency instrument onboard the PLANCK satellite   In: Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Edited by:P A R Ade, J E Aguirre, J J Bock, M Dragovan, L Duband, L Earle, J Glenn, H Matsuhara, B J Naylor, H T Nguyen, M Yun, & J Zmuidzinas C. M. Bradford. 756-767  
Abstract: The Low Frequency Instrument aboard the PLANCK satellite will employ pseudo-correlation radiometers, operating over three broad bands centred at 30, 44 ,and 70 GHz. The radiometer scheme is based on the simultaneous comparison of two input signals, one coming from the sky and the other coming from a reference blackbody at a stable cryogenic temperature (near 4K) as close as possible to the sky temperature (about 2.7K). This choice is made in order to minimize non-white instrumental noise, typically exhibiting a 1/f spectrum. Effects due to the residual offset are minimised with a gain modulation factor applied in software. Fluctuations of the reference signal, due to fluctuation in the cooling chain or to straylight radiation, can also produce a parasitic signal which would mimic a true sky fluctuation. The PLANCK scientific goal of a high precision imaging of the CMB anisotropy requires an accurate characterisation of each part constituting the chain by using tools of modellisation and experimental tests. In this work we describe the concept of the radiometric chain, its functioning and the main sources of systematic errors, showing how, only with a hard modelling effort, it is possible to characterise, reduce and then remove in the data processing those systematic effects that may in principle compromise the quality of the whole instrument response.
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A Simonetto, C Sozzi, O D’Arcangelo, V Muzzini, S Garavaglia, F Villa, M Sandri, L Valenziano, F Cuttaia, M Bersanelli, A Mennella, P Guzzi (2004)  Millimeterwave Techniques For Fusion Plasmas And For Experimental Cosmology   In: Plasmas in the Laboratory and in the Universe : New Insights and New Challenges Edited by:D Farina, & R Pozzoli G. Bertin. 455-460  
Abstract: The millimetric region of the electromagnetic spectrum is of great interest both to plasma physics and to experimental cosmology. Building on the common technological interest, the tests on passive components of the Low Frequency Instrument of the PLANCK mission are made in IFP's microwave laboratory. The experimental techniques and sample results are shown.
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P Platania, C Burigana, D Maino, E Caserini, M Bersanelli, B Cappellini, A Mennella (2004)  A re-analysis of the wide coverage radio surveys of Galactic diffuse emission   In: Milky Way Surveys : The Structure and Evolution of our Galaxy Edited by:R Shah, & T Brainerd D. Clemens.  
Abstract: The three wide coverage radio surveys at 408, 1420 and 2326 MHz have been analysed in order to remove artifacts from each map by means of the tecnique applied by Schlegel, Finkbeiner, & Davis (1998) to IRAS data. A detailed analysis of systematic errors has been performed including an attempt to minimize inter-calibration effects using the combination of the three maps. Nearly-full-sky maps of spectral index and normalization factor with sub-degree resolution have been derived with a pixel by pixel fitting. The resulting distributions are representative of the Galactic diffuse synchrotron emission.
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M Maris, S Fogliani, N Lama, F Pasian, A Zacchei, M Bersanelli, D Maino, P Leutenegger, M Miccolis, E Franceschi, M Malaspina, A Mennella, M Salmon (2004)  Data Handling for Planck/LFI Ground Tests   In: Astronomical Data Analysis Software and Systems (ADASS) XIII Edited by:M G Allen, & D Egret F. Ochsenbein.  
Abstract: Ground Tests are a fundamental milestone within the development of the Low Frequency Instrument (LFI) which will fly onboard the ESA satellite Planck. They allow the collection of information which can not be supplied by monitoring onboard activity of the satellite during operations. Here methods and principles driving the management and elaboration of data collected during the Ground Tests campaign for the Planck / LFI are synthetically presented.
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2003
F Villa, M Sandri, M Bersanelli, R C Butler, N Mandolesi, A Mennella, J Marti-Canales, J Tauber (2003)  PLANCK/LFI : an Advanced Multi-beam High Performance mm-wave Optics for Space Applications   In: 25th Antenna Workshop on Satellite Antenna Technology, 18-20 Sept. 2002, ESA-ESTEC, NL  
Abstract: The Low Frequency Instrument (LFI) is one of the two instruments onboard the ESA PLANCK satellite foreseen to be launched in 2007. The LFI will image the Cosmic Microwave Background (CMB) anisotropies and the polarization in four different bands, with an unprecedented combination of sky coverage, calibration accuracy, control of systematic errors, and sensitivity. LFI is coupled to the PLANCK Telescope by an array of 23 high performance dual profiled corrugated feed horns. The dual reflector off axis-design of the 1.5 meter projected aperture telescope is the most advanced optical design ever conceived for accommodating large multi-beam and multi-frequency focal plane units. The location and the design of the feed horns, for both instruments, have been optimised in order to maintain good beam symmetry, even far from the optical axis, and an excellent straylight rejection. In this paper we describe the LFI instrument with emphasis on its optical performance and coupling with the PLANCK telescope.
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A Mennella, M Bersanelli, R C Butler, D Maino, N Mandolesi, G Morgante, L Valenziano, F Villa, T Gaier, M Seiffert, S Levin, C Lawrence, P Meinhold, P Lubin, J Tuovinen, J Varis, T Karttaavi, N Hughes, P Jukkala, P Sjman, P Kangaslahti, N Roddis, D Kettle, F Winder, E Blackhurst, R Davis, A Wilkinson, C Castelli, B Aja, E Artal, L de la Fuente, A Mediavilla, J P Pascual, J Gallegos, E Martinez-Gonzalez, P de Paco, L Pradell (2003)  Advanced pseudo-correlation radiometers for the Planck-LFI instrument   In: 3rd ESA Workshop on millimetre wave technology and applications (ESPOO, 21-23 May 2003)  
Abstract: The LFI (Low Frequency Instrument) on board the ESA Planck satellite is constituted by an array of radiometric detectors actively cooled at 20 K in the 30-70 GHz frequency range in the focal plane of the Planck telescope. In this paper we present an overview of the LFI instrument, with a particular focus on the radiometer design. The adopted pseudo-correlation scheme uses a software balancing technique (with a tunable parameter called gain modulation factor) which is effective in reducing the radiometer susceptibility to amplifier instabilities also in presence of small non-idealities in the radiometric chain components, provided that the gain modulation factor is estimated with an accuracy of the order of 0.2%. These results have been recently confirmed by experimental laboratory measurements conducted on the LFI prototype radiometers at 30, 70 and 100 GHz.
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2002
L Terenzi, M Bersanelli, C Burigana, R C Butler, G de Zotti, N Mandolesi, D Mennella, G Morgante, M Sandri, L Valenziano, F Villa (2002)  Sources variability with Planck LFI   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 245-247  
Abstract: Planck LFI (Low Frequency Instrument) will produce a complete survey of the sky at millimeter wavelengths. Data stream analysis will provide the possibility to reveal unexpected millimeter sources and to study their flux evolution in time at different frequencies. We describe here the main implications and discuss data analysis methods. Planck sensitivities typical for this kind of detection are taken into account. We present also preliminary results of our simulation activity.
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F Villa, N Mandolesi, M Bersanelli, R C Butler, C Burigana, A Mennella, G Morgante, M Sandri, L Valenziano (2002)  The low frequency instrument of the Planck mission   In: Astrophysical Polarized Backgrounds Edited by:S Cortiglioni, R Sault, & C Sbarra S. Cecchini. 144-149  
Abstract: The Low Frequency Instrument (LFI) is one of the two instruments onboard the ESA Planck satellite. LFI will image the Cosmic Microwave Background anisotropies and the polarization status in four different bands, from 30 GHz to 100 GHz, with an array of 54 radiometers. The characteristics of the instrument are reported, underlining the ability of LFI to perform polarization measurements. .
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F Villa, M Bersanelli, C Burigana, R C Butler, N Mandolesi, A Mennella, G Morgante, M Sandri, L Terenzi, L Valenziano (2002)  The Planck Telescope   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 224-228  
Abstract: In this paper we present an overview of the Telescope designed for ESA's mission dedicated to map the Cosmic Microwave Background Anisotropies and Polarization. Two instrument, LFI and HFI, operate in an overall frequency range between 25 and 900 GHz and share the focal region of the 1.5 meter optimized aplanatic telescope. The optimization techniques adopted for the optical design and the telescope characteristic are reported and discussed.
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N Mandolesi, M Bersanelli, R C Butler, C Burigana, D Maino, A Mennella, G Morgante, L Valenziano, F Villa (2002)  Planck low frequency instrument   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 193-201  
Abstract: The Low Frequency Instrument (LFI) is one of the two instrument onboard the ESA Planck Mission. LFI will image the Cosmic Microwave Background anisotropies in four different bands, from 30 GHz to 100 GHz, with an array of 54 radiometers. The instrument characteristics and expected performances are presented, with particular attention to the control of systematic effects. .
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A Mennella, M Bersanelli, C Burigana, D Maino, R Ferretti, G Morgante, M Prina, N Mandolesi, C Butler, L Valenziano, F Villa (2002)  Analysis of thermally-induced effects in Planck Low Frequency Instrument   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 229-233  
Abstract: The Planck mission will provide full-sky maps of the Cosmic Microwave Background with unprecedented angular resolution (~10') and sensitivity (ΔT/T~10^-6). This requires cryogenically cooled, high sensitivity detectors as well as an extremely accurate control of systematic errors, which must be kept at μK level. In this work we focus on systematic effects arising from thermal instabilities in the Low Frequency Instrument, operating in the 30-100 GHz range. Our results show that it is of crucial importance to assure ``in hardware'' a high degree of stability. In addition, we provide an estimate of the level at which it is possible to reduce the contamination level in the observed maps by proper analysis of the Time Ordered Data. .
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M Sandri, M Bersanelli, C Burigana, R C Butler, M Malaspina, N Mandolesi, A Mennella, G Morgante, L Terenzi, L Valenziano, F Villa (2002)  Planck Low Frequency Instrument : Beam patterns   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 242-244  
Abstract: The Low Frequency Instrument on board the Planck satellite is coupled to the Planck 1.5 meter off-axis dual reflector telescope by an array of 27 corrugated feed horns operating at 30, 44, 70, and 100 GHz. We briefly present here a detailed study of the optical interface devoted to optimize the angular resolution (10 arcmin at 100 GHz as a goal) and at the same time to minimize all the systematics coming from the sidelobes of the radiation pattern. Through optical simulations, we provide shapes, locations on the sky, angular resolutions, and polarization properties of each beam. (On behalf of LFI Collaboration).
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L Valenziano, M Bersanelli, R C Butler, F Cuttaia, N Mandolesi, A Mennella, G Morigi, G Morgante, M Sandri, L Terenzi, F Villa (2002)  The 4K Reference Load for the Planck Low Frequency Instrument   In: Experimental Cosmology at Millimetre Wavelengths Edited by:M de Petris & M Gervasi. 219-223  
Abstract: The Low Frequency Instrument (LFI) on-board the Planck satellite, is composed by an array of 54 receivers. They follow a pseudo-correlation scheme, continuously observing the sky and a stable reference load, at a temperature T~4 K. The so-called 4 K Reference Load is made of 54 small absorbing targets, mechanically and thermally connected to the High Frequency Instrument (HFI) cryostat. The 4K Reference Load requirements pose severe limits to its mass, dimensions, power dissipation and performance. .
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1999
A Mennella, L Chiappa, T P Lockhart, G Burrafato (1999)  Candidate and Chemical Selection Rules for Water Shutoff Polymer Treatments   In: 1999 SPE European Formation Damage Conference, The Hague (NL), 31 May – 1 June 1999 (paper SPE 54736)  
Abstract: Water shutoff treatments with polymers that selectively reduce the water permeability can be effective to reduce water production from hydrocarbon wells that cannot be treated with conventional approaches. In this paper we present an analysis that starts from the principal operative questions and defines the main physical-chemical issues to be understood in order to develop a reliable technology. These issues are discussed by showing results from a number of experimental and simulation studies conducted in our laboratories with the goal to link the understanding of basic mechanisms to the development of operational rules. This work shows the elaboration of understanding-based rules for candidate and chemical selection to be an effective strategy for the application of this technology in the field.
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1998
A Mennella, L Chiappa, S L Bryant, G Burrafato (1998)  Pore-scale mechanism for selective permeability reduction by polymer injection   In: SPE/DOE Symposium on Improved Oil Recovery, Tulsa (OK), 19-22 April 1998 (paper SPE 39634)  
Abstract: In this paper we discuss a pore-scale picture of the mechanism underlying the selective permeability reduction caused by the adsorption of a polymer layer in a water wet porous medium. Our analysis is based on the use of physically representative model of the porous medium, which allows us to estimate directly the expected permeability reduction. Comparison of model predictions with coreflood experimental data has revealed that the selectivity in permeability reduction cannot be explained if the polymer layer is modeled as a rigid, impenetrable layer. This result is consistent with the suggestion that swelling-shrinking phenomena of the adsorbed polymer later is responsible for the selectivity in the permeability modification induced by these treatments.
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L Chiappa, A Mennella, G Burrafato (1998)  Polymer/rock interactions in polymer treatments for water-cut control   In: SPE/DOE Symposium on Improved Oil Recovery, Tulsa (OK), 19-22 April 1998 (paper SPE 39619)  
Abstract: In this paper we study the adsorption of polymers bearing differently charged groups onto solid surfaces of siliceous nature. By means of static adsorption tests we show that the adsorption is dominated by the electrostatic interactions between the polymer molecules and the solid surface. We also show that both lithology and brine composition can strongly influence the adsorption behavior; such effects must be therefore carefully assessed before applying these treatments in the field.
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1997
A Mennella, S L Bryant, T P Lockhart (1997)  Propagation of Tracers through Cores Containing an immobile Fluid Phase   In: SPE International Symposium on Oilfield Chemistry, Houston (TX - USA), Feb. 17-21 1997 (paper SPE 37248)  
Abstract: The analysis of a tracer experiment requires care when one of the fluid phases within the porous medium is immobile but miscible with the tracer carrier fluid. High levels of dispersion (Pe < 10) are commonly encountered in this situation. Applying the classical analytical expression for the tracer concentration in an infinite core is straightforward and convenient but introduces significant mass balance errors at low Peclet numbers. Theoretical effluent concentration histories from a finite core in the absence of interphase mass transfer span a well-defined and relatively limited area on a plot of concentration versus time. Comparison of experimental effluent histories with this family of curves provides a rapid test of whether mass transfer into the immobile phase is important. At high mass transfer rates the effluent history becomes insensitive to the volume fractions of the fluid phases. Thus it can be difficult to determine a unique set of fitting parameters. To avoid this difficulty, experiments should be conducted at high flow rates (low residence times) or with slowly diffusing tracers.
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1994
M Bartosek, A Mennella, T P Lockhart, E Causin, E Rossi, C Passucci (1994)  Polymer Gels for Conformance Treatments : Propagation of Cr(III) Crosslinking Complexes in Porous Media   In: SPE/DOE Symposium on Improved Oil Recovery, Tulsa (OK), 17-20 April 1994 (paper SPE 27828)  
Abstract: The influence of pH, temperature, and gelation delaying ligands on the stability of Cr(III) complexes in bulk solution and on Cr(III) propagation in porous media has been investigated for acetate, glycolate, and malonate complexes of Cr(III). For a given complex, Cr(III) instability to hydrolysis and Cr(III) retention increase with increasing pH and temperature. The chemical nature of the gelation delaying ligands bound to Cr(III) and their concentration in the solution have a profound influence on the resistance of the Cr(III) complex to hydrolysis and on Cr(III) retention. Thus, whereas the Cr(III) acetate crosslinker, by itself, propagates poorly at elevated temperature, addition of sodium glycolate to the solution markedly reduces retention. We show that Cr(III) retention in sandstone cores can be virtually eliminated at 90 C by appropriate formulation of the gel-formiag solution. Other experiments establish that Cr(III) precipitation at elevated temperature is reversible in the presence of polymer and that significant accumulation of the Cr(III) precipitate can have a negative impact on injectivity.
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1990
1989
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