A&A 520, A4 (2010)DOI: 10.1051/0004-6361/200912853c○ ESO 2010<strong>Pre</strong>-launch status of the <strong>Planck</strong> missionAstronomy&AstrophysicsSpecial feature<strong>Planck</strong> pre-launch status: Design and description of the LowFrequency InstrumentM. Bersanelli 1,2 ,N.Mandolesi 3 ,R.C.Butler 3 ,A.Mennella 1,2 ,F.Villa 3 ,B.Aja 4 ,E.Artal 4 ,E.Artina 5 ,C. Baccigalupi 6,15 ,M.Balasini 5 ,G.Baldan 5 ,A.Banday 7,32 ,P.Bastia 5 ,P.Battaglia 5 ,T.Bernardino 8 ,E.Blackhurst 9 ,L. Boschini 5 ,C.Burigana 3 ,G.Cafagna 5 ,B.Cappellini 1,2 ,F.Cavaliere 1 ,F.Colombo 5 ,G.Crone 10 ,F.Cuttaia 3 ,O. D ′ Arcangelo 11 ,L.Danese 6 ,R.D.Davies 9 ,R.J.Davis 9 ,L.DeAngelis 12 ,G.C.DeGasperis 13 ,L.DeLaFuente 4 ,A. De Rosa 3 ,G.DeZotti 14 ,M.C.Falvella 12 ,F.Ferrari 5 ,R.Ferretti 5 ,L.Figini 11 ,S.Fogliani 15 ,C.Franceschet 1 ,E. Franceschi 3 ,T.Gaier 16 ,S.Garavaglia 11 ,F.Gomez 17 ,K.Gorski 16 ,A.Gregorio 18 ,P.Guzzi 5 ,J.M.Herreros 17 ,S. R. Hildebrandt 17 ,R.Hoyland 17 ,N.Hughes 19 ,M.Janssen 16 ,P.Jukkala 19 ,D.Kettle 9 ,V.H.Kilpiä 19 ,M.Laaninen 20 ,P. M. Lapolla 5 ,C.R.Lawrence 16 ,D.Lawson 9 ,J.P.Leahy 9 ,R.Leonardi 21 ,P.Leutenegger 5 ,S.Levin 16 ,P.B.Lilje 22 ,S. R. Lowe 9 ,P.M.Lubin 21 ,D.Maino 1 ,M.Malaspina 3 ,M.Maris 15 ,J.Marti-Canales 10 ,E.Martinez-Gonzalez 8 ,A. Mediavilla 4 ,P.Meinhold 21 ,M.Miccolis 5 ,G.Morgante 3 ,P.Natoli 13 ,R.Nesti 23 ,L.Pagan 5 ,C.Paine 16 ,B. Partridge 24 ,J.P.Pascual 4 ,F.Pasian 15 ,D.Pearson 16 ,M.Pecora 5 ,F.Perrotta 15,6 ,P.Platania 11 ,M.Pospieszalski 25 ,T. Poutanen 26,27,28 ,M.Prina 16 ,R.Rebolo 17 ,N.Roddis 9 ,J.A.Rubiño-Martin 17 ,M.J.Salmon 8 ,M.Sandri 3 ,M. Seiffert 16 ,R.Silvestri 5 ,A.Simonetto 11 ,P.Sjoman 19 ,G.F.Smoot 29 ,C.Sozzi 11 ,L.Stringhetti 3 ,E.Taddei 5 ,J. Tauber 30 ,L.Terenzi 3 ,M.Tomasi 1 ,J.Tuovinen 31 ,L.Valenziano 3 ,J.Varis 31 ,N.Vittorio 13 ,L.A.Wade 16 ,A. Wilkinson 9 ,F.Winder 9 ,A.Zacchei 15 ,andA.Zonca 1,2(Affiliations can be found after the references)Received 8 July 2009 / Accepted 15 December 2009ABSTRACTIn this paper we present the Low Frequency Instrument (LFI), designed and developed as part of the <strong>Planck</strong> space mission, the ESA programmededicated to precision imaging of the cosmic microwave background (CMB). <strong>Planck</strong>-LFI will observe the full sky in intensity and polarisationin three frequency bands centred at 30, 44 and 70 GHz, while higher frequencies (100−850 GHz) will be covered by the HFI instrument. TheLFI is an array of microwave radiometers based on state-of-the-art indium phosphide cryogenic HEMT amplifiers implemented in a differentialsystem using blackbody loads as reference signals. The front end is cooled to 20 K for optimal sensitivity and the reference loads are cooled to4Ktominimiselow-frequencynoise.WeprovideanoverviewoftheLFI,discuss the leading scientific requirements, and describe the designsolutions adopted for the various hardware subsystems. The main drivers of theradiometric,optical,andthermaldesignarediscussed,includingthe stringent requirements on sensitivity, stability, and rejection of systematic effects. Further details on the key instrument units and the results ofground calibration are provided in a set of companion papers.Key words. cosmic microwave background – cosmology: observations – space vehicles: instruments1. IntroductionObservations of the cosmic microwave background (CMB) haveplayed a central role in the enormous progress of cosmologyin the past few decades. Technological developments in bothcoherent radio receivers and bolometric detectors have supportedan uninterrupted chain of successful experiments, fromthe initial discovery (Penzias & Wilson 1965) uptothepresentgeneration of precision measurements. Following COBE 1 andWMAP 2 ,the<strong>Planck</strong> 3 satellite, launched on 14 May 2009, is thenext-generation space mission dedicated to CMB observations.1 http://lambda.gsfc.nasa.gov/product/cobe/2 http://map.gsfc.nasa.gov/3 <strong>Planck</strong> (http://www.esa.int/<strong>Planck</strong>) is a project of theEuropean Space Agency – ESA – with instruments provided by two scientificConsortia funded by ESA member states (in particular the leadcountries: France and Italy) with contributions from NASA (USA), andThe <strong>Planck</strong> instruments are designed to extract all the cosmologicalinformation encoded in the CMB temperature anisotropieswith an accuracy set by cosmic variance and astrophysical confusionlimits, and to push polarisation measurements well beyondpreviously reached results. <strong>Planck</strong> will image the sky innine frequency bands across the CMB blackbody peak, leadingto a full-sky map of the CMB temperature fluctuations withsignal-to-noise >10 and angular resolution
A&A 520, A4 (2010)In addition, all <strong>Planck</strong> bands between 30 and 350 GHz are sensitiveto linear polarisation.The imaging power of <strong>Planck</strong> is sized to extract the temperaturepower spectrum with high precision over the entire angularrange dominated by primordial fluctuations. This will lead toaccurate estimates of cosmological parameters that describe thegeometry, dynamics, and matter-energy content of the universe.The <strong>Planck</strong> polarisation measurements are expected to delivercomplementary information on cosmological parameters and toprovide a unique probe of the thermal history of the universein the early phase of structure formation. <strong>Planck</strong> will also testthe inflationary paradigm with unprecedented sensitivity throughstudies of non-Gaussianity and of B-mode polarisation as a signatureof primordial gravitational waves (<strong>Planck</strong> Collaboration2005).The wide frequency range of <strong>Planck</strong> is required primarilyto ensure accurate discrimination of foreground emissions fromthe cosmological signal. However, the nine <strong>Planck</strong> maps willalso represent a rich data set for galactic and extragalactic astrophysics.Up to now, no single technology can reach the requiredperformances in the entire <strong>Planck</strong> frequency range. Forthis reason two complementary instruments are integrated at the<strong>Planck</strong> focal plane exploiting state-of-the-art radiometric andbolometric detectors in their best windows of operation. TheLow Frequency Instrument (LFI), described in this paper, coversthe 27−77 GHz range with a radiometer array cooled to 20 K.The High Frequency Instrument (HFI) will observe in six bandsin the 90−900 GHz range with a bolometer array cooled to 0.1 K(Lamarre et al. 2010). The two instruments share the focal planeof a single telescope, a shielded off-axis dual reflector Gregoriansystem with 1.5 × 1.9 m primary aperture (Tauber et al. 2010b).The design of the <strong>Planck</strong> satellite and mission plan is largelydriven by the extreme thermal requirements imposed by the instruments.The cold payload enclosure (
- Page 1 and 2:
A&A 520, E1 (2010)DOI: 10.1051/0004
- Page 3 and 4:
ABSTRACTThe European Space Agency
- Page 5 and 6:
A&A 520, A1 (2010)Fig. 2. An artist
- Page 7 and 8:
A&A 520, A1 (2010)Fig. 4. Planck fo
- Page 9 and 10:
A&A 520, A1 (2010)Fig. 6. The Planc
- Page 11 and 12:
A&A 520, A1 (2010)Table 4. Summary
- Page 13 and 14:
A&A 520, A1 (2010)three frequency c
- Page 15 and 16:
A&A 520, A1 (2010)Fig. 12. The left
- Page 17 and 18:
A&A 520, A1 (2010)Fig. 14. Left pan
- Page 19 and 20: A&A 520, A1 (2010)flux limit of the
- Page 21 and 22: A&A 520, A1 (2010)- University of C
- Page 23 and 24: A&A 520, A1 (2010)57 Instituto de A
- Page 25 and 26: A&A 520, A2 (2010)Fig. 1. (Left) Th
- Page 27 and 28: A&A 520, A2 (2010)Fig. 3. (Top)Twos
- Page 29 and 30: A&A 520, A2 (2010)Table 2. Predicte
- Page 31 and 32: Table 3. Predicted in-flight main b
- Page 33 and 34: A&A 520, A2 (2010)materials. Theref
- Page 35 and 36: A&A 520, A2 (2010)Fig. 11. Comparis
- Page 37 and 38: A&A 520, A2 (2010)Table 5. Inputs u
- Page 39 and 40: A&A 520, A2 (2010)Fig. 16. Three cu
- Page 41 and 42: A&A 520, A2 (2010)Table 7. Optical
- Page 43 and 44: A&A 520, A2 (2010)Fig. A.1. Dimensi
- Page 45 and 46: A&A 520, A2 (2010)5 Università deg
- Page 47 and 48: A&A 520, A3 (2010)Horizon 2000 medi
- Page 49 and 50: A&A 520, A3 (2010)Fig. 1. CMB tempe
- Page 51 and 52: A&A 520, A3 (2010)Ω ch 2τn s0.130
- Page 53 and 54: A&A 520, A3 (2010)Fig. 6. Integral
- Page 55 and 56: A&A 520, A3 (2010)Table 2. LFI opti
- Page 57 and 58: 3.3.1. SpecificationsThe main requi
- Page 59 and 60: A&A 520, A3 (2010)Fig. 11. Schemati
- Page 61 and 62: A&A 520, A3 (2010)features of the r
- Page 63 and 64: A&A 520, A3 (2010)Fig. 13. Level 2
- Page 65 and 66: A&A 520, A3 (2010)Fig. 15. Level 3
- Page 67 and 68: A&A 520, A3 (2010)GUI = graphical u
- Page 69: A&A 520, A3 (2010)23 Centre of Math
- Page 73 and 74: A&A 520, A4 (2010)Table 2. Sensitiv
- Page 75 and 76: A&A 520, A4 (2010)Fig. 2. Schematic
- Page 77 and 78: A&A 520, A4 (2010)Fig. 6. LFI recei
- Page 79 and 80: A&A 520, A4 (2010)Fig. 9. Schematic
- Page 81 and 82: A&A 520, A4 (2010)Table 4. Specific
- Page 83 and 84: A&A 520, A4 (2010)Fig. 15. DAE bias
- Page 85 and 86: A&A 520, A4 (2010)Fig. 19. Picture
- Page 87 and 88: A&A 520, A4 (2010)Table 10. Main ch
- Page 89 and 90: Table 13. Principal requirements an
- Page 91 and 92: A&A 520, A5 (2010)DOI: 10.1051/0004
- Page 93 and 94: A. Mennella et al.: LFI calibration
- Page 95 and 96: A. Mennella et al.: LFI calibration
- Page 97 and 98: A. Mennella et al.: LFI calibration
- Page 99 and 100: A. Mennella et al.: LFI calibration
- Page 101 and 102: A. Mennella et al.: LFI calibration
- Page 103 and 104: A. Mennella et al.: LFI calibration
- Page 105 and 106: D.1. Step 1-extrapolate uncalibrate
- Page 107 and 108: A&A 520, A6 (2010)DOI: 10.1051/0004
- Page 109 and 110: F. Villa et al.: Calibration of LFI
- Page 111 and 112: F. Villa et al.: Calibration of LFI
- Page 113 and 114: F. Villa et al.: Calibration of LFI
- Page 115 and 116: F. Villa et al.: Calibration of LFI
- Page 117 and 118: F. Villa et al.: Calibration of LFI
- Page 119 and 120: F. Villa et al.: Calibration of LFI
- Page 121 and 122:
A&A 520, A7 (2010)DOI: 10.1051/0004
- Page 123 and 124:
M. Sandri et al.: Planck pre-launch
- Page 126 and 127:
A&A 520, A7 (2010)Fig. 8. Footprint
- Page 128 and 129:
-30-40-30-6-3-20A&A 520, A7 (2010)0
- Page 130 and 131:
A&A 520, A7 (2010)Table 4. Galactic
- Page 132 and 133:
A&A 520, A7 (2010)Fig. A.1. Polariz
- Page 134 and 135:
A&A 520, A8 (2010)inflation, giving
- Page 136 and 137:
A&A 520, A8 (2010)estimated from th
- Page 138 and 139:
A&A 520, A8 (2010)ways the most str
- Page 140 and 141:
unmodelled long-timescale thermally
- Page 142 and 143:
A&A 520, A8 (2010)Fig. 5. Polarisat
- Page 144 and 145:
A&A 520, A8 (2010)Table 3. Band-ave
- Page 146 and 147:
A&A 520, A8 (2010)where S stands fo
- Page 148 and 149:
A&A 520, A8 (2010)Fig. 11. Simulate
- Page 150 and 151:
stored in the LFI instrument model,
- Page 152 and 153:
A&A 520, A8 (2010)Table 5. Statisti
- Page 154 and 155:
A&A 520, A8 (2010)comparable in siz
- Page 156 and 157:
A&A 520, A8 (2010)Table B.1. Main b
- Page 158 and 159:
A&A 520, A8 (2010)Bond, J. R., Jaff
- Page 160 and 161:
A&A 520, A9 (2010)- (v) an optical
- Page 162 and 163:
A&A 520, A9 (2010)Fig. 2. The Russi
- Page 164 and 165:
A&A 520, A9 (2010)Table 3. Estimate
- Page 166 and 167:
A&A 520, A9 (2010)Fig. 7. Picture o
- Page 168 and 169:
A&A 520, A9 (2010)Fig. 9. Cosmic ra
- Page 170 and 171:
A&A 520, A9 (2010)Fig. 13. Principl
- Page 172 and 173:
A&A 520, A9 (2010)Fig. 16. Noise sp
- Page 174 and 175:
A&A 520, A9 (2010)Table 6. Basic ch
- Page 176 and 177:
A&A 520, A9 (2010)with warm preampl
- Page 178 and 179:
A&A 520, A9 (2010)20 Laboratoire de
- Page 180 and 181:
A&A 520, A10 (2010)Table 1. HFI des
- Page 182 and 183:
A&A 520, A10 (2010)based on the the
- Page 184 and 185:
A&A 520, A10 (2010)Fig. 6. The Satu
- Page 186 and 187:
A&A 520, A10 (2010)5. Calibration a
- Page 188 and 189:
A&A 520, A10 (2010)Fig. 16. Couplin
- Page 190 and 191:
A&A 520, A10 (2010)217-5a channel:
- Page 192 and 193:
A&A 520, A10 (2010)10 -310 -495-The
- Page 194 and 195:
A&A 520, A11 (2010)DOI: 10.1051/000
- Page 196 and 197:
P. A. R. Ade et al.: Planck pre-lau
- Page 198 and 199:
P. A. R. Ade et al.: Planck pre-lau
- Page 200 and 201:
P. A. R. Ade et al.: Planck pre-lau
- Page 202 and 203:
A&A 520, A12 (2010)Table 1. Summary
- Page 204 and 205:
arrangement was also constrained by
- Page 206 and 207:
A&A 520, A12 (2010)frequency cut-of
- Page 208 and 209:
A&A 520, A12 (2010)Fig. 9. Gaussian
- Page 210 and 211:
A&A 520, A12 (2010)the horn-to-horn
- Page 212 and 213:
A&A 520, A12 (2010)Fig. 15. Composi
- Page 214 and 215:
A&A 520, A12 (2010)Fig. 19. Broad-b
- Page 216 and 217:
A&A 520, A13 (2010)DOI: 10.1051/000
- Page 218 and 219:
C. Rosset et al.: Planck-HFI: polar
- Page 220 and 221:
C. Rosset et al.: Planck-HFI: polar
- Page 222 and 223:
of frequencies and shown to have po
- Page 224 and 225:
C. Rosset et al.: Planck-HFI: polar
- Page 226 and 227:
C. Rosset et al.: Planck-HFI: polar