Planck – Mission and Technology
Transcription
Planck – Mission and Technology
Planck – Mission and Technology Petri Jukkala, Nicholas Hughes, Mikko Laaninen, Ville-Hermanni Kilpiä YLINEN Electronics Ltd Jussi Tuovinen, Jussi Varis, Anna Karvonen MilliLab, VTT Information Technology © YLINEN Electronics Ltd 2004 Contents Planck Mission - Cosmic Microwave Background (CMB) radiation - History of CMB measurements Planck Payload - High Frequency Instrument (HFI) - Low frequency Instrument (LFI) 70 GHz receiver - specifications - receiver technology - measurement system - performance Conclusions © YLINEN Electronics Ltd 2004 The Big Bang • • • • Expansion or Collapse - depends on gravity • Ω is the ratio of actual to critical density • Ω=1 equilibrium; Ω>1 collapse • free space shows ~0.2 atoms/m3; • planets, stars, etc ~0.1 atoms/3 • Ω=1 requires 5 atoms/m3 Remaining density named “dark matter” • can possibly be detected by gravitational lensing • but is not known if enough for Ω=1 Current “Inflation” model • shows a fireball after 3min to 300,000years • gravity battling against thermal pressure (like a star) • star converts hydrogen to helium • during last stages helium to heavier elements • not time in fireball - evidenced by min. He of 23% • and fireball expanding and cooling At 300,000years • gravity WINS and atoms form • energy (photons) can propagate - end of dark age • the cosmic background we can detect © YLINEN Electronics Ltd 2004 Cosmic Structures IF transition to Gravity dominance smooth – a smooth and even atomic structure created – constant density, – no grouping of atoms – no dust clouds, – no primordial stars, – no galaxies However, if density (sonic) oscillations in Fireball – at decoupling these would lead to density variations during expansion, gravity would, – increase higher densities – decrease lower densities – thus dust clouds form & coalesce forming the first stars this implies a variable transition to atom forming – the radiation should also show this variation – radiation would be over a large frequency range thus anisotropies in CMB show fireball structure © YLINEN Electronics Ltd 2004 Cosmic Microwave Background CMB • CMB Anisotropies - ripples • were noted by COBE • have different sizes (wavelengths & amplitudes) • Acoustic Horizon • determines longest ripple (fundamental?) • above this smaller ripples (harmonics?) • So mapping of these ripples, will provide • a better model for the fireball • a more reliable value of Ω • possibly the expansion/collapse answer • or something else • So we need more sensitive measurements © YLINEN Electronics Ltd 2004 Earlier Missions • COBE (COsmic Background Explorer) provided • the first evidence of CMB anistropy • launched 1989 • BOOMERANG, (Balloon Observations Of Millimetric Extragalactic Radiation And Geomagnetics) • made more sensitive measurements from a balloon • over 3% sky area. • showed strong evidence for CMB anisotropy • 1997 • WMAP, (Wilkinson Microwave Anisotropy Probe), • launched 2001 • provides an overall survey • but with lower sensitivity and resolution than Planck © YLINEN Electronics Ltd 2004 Mission comparision Planck vs. WMAP Sensitivity 10x Frequency coverage 10x Angular resolution 2x © YLINEN Electronics Ltd 2004 The Planck Mission • Planck and Herschel • launched together on Ariane 5 • separate before reaching L2 • Planck will achieve orbit as shown • LeGrange predicted neutral gravity points • at L2 sun+earth gravity balanced by solar centripedal force • Check-out and calibration • map complete sky • rotating at 1rpm • 1+ year mission • data transmission direct to ground • potential 100+ manyears data analysis © YLINEN Electronics Ltd 2004 Planck Payload is comprised of – support “service” module – Hydrogen sorption cooler system – passively cooled 1,5 m aperture off-set reflector antenna – the HIGH Frequency Instrument (HFI) – the LOW Frequency Instrument (LFI) the HFI has – bolometer receivers – at 100, 143, 217, 353, 545, 857GHz – cooled to 0.1 K the LFI has – radiometric receivers – at 30, 44, 70 GHz – cooled to 20K with a 4K reference © YLINEN Electronics Ltd 2004 Planck Payload module © YLINEN Electronics Ltd 2004 LFI Payload Focal Plane Unit light blue 2 x 30 GHz blue 3 x 44 GHz red 6 x 70 GHz Waveguides Back End Unit © YLINEN Electronics Ltd 2004 LFI Payload © YLINEN Electronics Ltd 2004 70 GHz receiver • “continuous comparison” provides continuous measurement, • maximises available viewing opportunity • and maximises sensitivity To other polarisation radiometer ½FEM 1st.Hybird (WG Magic-T) CMB Target ½BEM LNA.1 LNA.2 Phase Shifter φ OMT 2nd.Hybird (WG Magic-T) LNA.3 BPF Diode Voltage Detector Amplifier φ 4K Ref. • single antenna horn + OMT, provides two orthogonally polarised outputs • each output applied to separate radiometer • each radiometer amplifies and detects Target and 4K reference noise • detected signal appears as a noise voltage proportional to input noise power © YLINEN Electronics Ltd 2004 Receiver structure Analogue Data output DAE Interface 4K Ref. Source Filter 0 4K Ref. Antenna Amplifier/Detector π FEM_ACA FEM_Body DC Amplifier FEM_ACA 0 π Waveguide Input from Antenna via OMT Interconnection Waveguide © YLINEN Electronics Ltd 2004 70 GHz receiver main requirements • Frequency 63 – 77 GHz • Noise temperature 29 K, when cooled to 20 K • Isolation (phase switching) 13 dB (goal 20 dB) • 1/f noise knee frequency 50 mHz • RF Gain ~50 dB • FEM power consumption 24 mW (2 polarisations incl. 4 ACAs) • BEM power consumption 604 mW (4 back end receivers) © YLINEN Electronics Ltd 2004 Receiver technology FEM and ACA body: nickel/gold plated aluminium BEM body: cromatized and black painted aluminium Amplifiers (PHEMT) and switches (PIN) based on InP MMICs MMICs processed in NGST (TRW) Antenna horns, OMTs and interconnecting waveguides supplied by Italy © YLINEN Electronics Ltd 2004 Test system • 1,6 x 1,0 x 0.4 meter thermal vacuum chamber used for testing • Weight 1000 kg • 4 K (reference) and 20 K (receivers) coolers • WR12 waveguide Vector Network Analyzer • Noise temperature measurement with noise diode and thermal vane attenuator • Power meter • Data acquisition system • Low noise power supplies • Temperature sensors • Testing in class 100 000 clean room © YLINEN Electronics Ltd 2004 General configuration within the cryogenic shroud © YLINEN Electronics Ltd 2004 Test system © YLINEN Electronics Ltd 2004 General cryo chamber setup Radiation Shield 3dB "Magic-T" couplers 4K Load φ Data outputs BEM Antenna OMT FEM φ Antenna Load 4K Load Cryo. Chamber boundary Input stimulus Waveguide Waveguide Test Points FEM Output BEM Input © YLINEN Electronics Ltd 2004 On-chip measurement results Measurements made by MilliLab, both Room Temperature and Cryogenic, cryo measurements shown. NGST CRYOx & MLAB1, designs 70LN5B & 5C, Vds=0.4 V, Ids=7.5 mA, T=20 K; June 24, 2004 180 40 160 35 140 NGST MLAB2, wafer 4246-015, design 02004A_6, MMIC ID R2 C2 M0, T=20 K; August 11, 2004 0 Gt_425_old_cryo4 -0,5 Gt_121_new_cryo4 Gt_410_new_cryo4 120 100 20 80 15 60 Gt_710_cryo7 Gt_820_cryo7 Te_425_old_cryo4 Te_121_new_cryo4 Te_410_new_cryo4 Te_235_mlab1 Te_330_cryo9 Te_710_cryo7 40 5 20 0 0 -1,5 Gt_410_cryo9 Te_410_cryo9 10 100 Gt_330_cryo9 Te_820_cryo7 m a g S 2 1 (d B ) 25 150 -1 Gt_235_mlab1 N o is e te m p e ra tu re (K ) In s e rtio n g a in (d B ) 30 200 50 -2 0 -2,5 -3 -50 -3,5 -100 -4 -150 -4,5 -5 50 52,5 55 57,5 60 62,5 65 67,5 70 72,5 75 77,5 -200 50 52,5 55 57,5 60 62,5 65 67,5 70 72,5 75 77,5 80 80 Frequency (GHz) Frequency (GHz) © YLINEN Electronics Ltd 2004 p h a s e S 2 1 (d e g ) 45 magS21 (dB) - 1 magS21 (dB) - 2 phS21 (deg) - 1 phS21 (deg) - 2 FM ACA measuremet results, cryo MEP01: FEM_ACA Gain Measurement 55 50,0 60 65 Frequency - GHz MEP02: FEM_ACA Noise Temperature Measurement - Forward biased phase shifter 70 75 80 85 100,0 FEM_ACA Noise Temp. K 45,0 80,0 40,0 Gain - dB 35,0 60,0 30,0 25,0 40,0 20,0 15,0 20,0 10,0 5,0 0,0 FEM_ACA Gain, Phase shifter state 0 FEM_ACA Gain, Phase shifter state 1 © YLINEN Electronics Ltd 2004 0,0 60 65 Frequency 70 - GHz 75 80 EM FEM and BEM measurement results FEM Noise Temp. - TVA measurement FEM noise Phase shifter state 00 - Input.4 - Output.8 100 90 NT 80 (K) 70 60 50 40 30 20 10 0 62 Phase shifter state 01- Input.4 - Output.7 FEM gain and switching isolation Phase shifter state 10 - Input.4 - Output.7 Phase shifter state 10 - Input.4 - Output.8 64 66 68 BEM response (DC/RF) 70 72 74 76 78 Frequency GHz 72 Frequency (GHz) 70 FEM Input.1 to Output.2 (for all phase states) 00 01 68 10 11 50 dB Gain 40 Att_20 66 Att=30 30 Att=40 Att=50 64 20 Att=70 Att=90 10 0 -10 55 60 65 70 75 Frequency GHz 80 85 Att=110 62 Sensitivity dB(mV/mW) Att=130 60 55 © YLINEN Electronics Ltd 2004 60 65 70 75 80 85 EM Receiver measurement results Response (DC/RF) 1/f noise Sensitivity vs Frequency A ttenuato r setting = 20 A ttenuato r setting = 30 A ttenuato r setting = 40 A ttenuato r setting = 50 A ttenuato r setting = 70 A ttenuato r setting = 90 A ttenuato r setting = 110 160 150 140 130 Sensitivity 120 (dBmV/mW) 110 100 90 55 60 65 70 75 80 85 Frequency (GHz) © YLINEN Electronics Ltd 2004 Conclusions • Planck mission has been presented • Planck satellite payload (HFI and LFI) was explained • State of the art 70 GHz continuous comparision receiver technology and performance was presented • Planck satellite will be launched in summer 2007 © YLINEN Electronics Ltd 2004