Lorenzo Moncelsi. SPIDER Probing The Dawn Of Time From Above The Clouds

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Transcription:

SPIDER Probing The Dawn Of Time From Above The Clouds

Planck 2013 B-modes BICEP2 2014 Thomson scattering within local quadrupole anisotropies generates linear polarization Scalar modes T, E Tensor modes T, E, B Ratio r = Δ T / Δ S Gravitational waves at LSS create B-mode polarization Probes Lyth bound in Inflation and indirectly proves that gravity is quantized Ekpyrotic models r = 0 Tensor modes gravitational waves W. Hu B>0 B<0

The quest for (primordial) B-modes Planck x BICEP 2015 Planck XX 2015

SPIDER: science goals Measure cosmological B-modes on degree angular scales in the presence of foregrounds 1) Verify angular spectrum (many uncorrelated bins out to large scales) 2) Verify statistical isotropy (large sky to check sub-regions) 3) Verify frequency spectrum (multiple frequencies needed to separate foregrounds)

Platform summary

Platform summary New Technology needs SQ careful, can bite easy but can SQ B. Netterfield

Why ballooning? A. Rahlin Fraisse+ 2013

SPIDER Overview Instrument: balloon-borne microwave polarimeter Goals: Primordial B-modes, foreground characterization The good: Frequency coverage Sky coverage Pol angle coverage The bad: Mass/power constraints One shot at quality data Recovery The ugly: Government shutdowns Frequencies 94 / 150 GHz (+ 280) Beam FWHM Visible sky 10% 42 / 31 arcmin Flight 1 Dec. 2013 2014, McMurdo Station Observation time Pol modulation 10-20 days Stepped HWP # detectors 2400, 85% yield NET/det Map depth 100 140 uk-rts 12 / 10 uk-arcmin BICEP2: 5 uk-arcmin (+Keck = 3.4)

ObsCos 17 April 2014

SPIDER: the instrument Lightweight, carbon fiber gondola frame and sun shields Largest cryogenic vessel on a balloon payload Reaction wheel + pivot for fast Az scanning Redundant pointing sensors for in-flight and post-flight reconstruction - star cameras - dgps - gyroscopes - pinhole sun sensors - magnetometer Designed for nearly autonomous observations

Cryogenic System Lightweight (850 kg) 1300-L LHe4-only cryostat (4K) Two vapor cooled shields (30K, 120K) Capillary-fed 20-L superfluid LHe4 tank (1.5K) Closed-cycle He3 adsorption fridge per telescope (300mK) Two weeks from close up to cold detectors Baselined for 20 day hold time Gudmundsson+ 2010 & 2015

The Telescope Runyan+ 2010 Filippini+ 2010

Half-Wave Plates Sapphire with quartz (90 GHz) and Cirlex (150 GHz) bonded AR coatings 95GHz 150GHz Custom worm-gear mechanism turns at 4K Stepped twice daily to modulate polarization 150GHz 150GHz Custom absolute and relative encoders to reconstruct HWP angle to better than 0.1 Bryan+ 2010 95GHz 95GHz

Rome La Sapienza 14/7/15 FPU and TES architecture Filippini+ 2010

Scan strategy Rahlin+ 2014 Planck XXX 2014 geometric f sky = 10% hits-weighted f sky = 6.5% actual 2015

Expected Sensitivity Rahlin+ 2014 20-day flight

Expected Sensitivity Dec 2014: 3x (90 GHz, 150 GHz) r<0.03 (99%CL) without FG for a 20-day flight Dec 2017: 2x (90 GHz, 150 GHz, 280 GHz) r<0.02 (99%CL) without FG, r<0.03 (99%CL) with FG Planck x BICEP 2015 Fraisse+ 2013

SPIDER: flight summary - launched on 1/1/15 - all systems operational! (except dgps) - 16 days of science data - f sky = geometric 10%, hits-weighted 6.5% - 1.5 TB of data (analysis ongoing)

SPIDER: in-flight performance Preliminary map of RCW38 (bright embedded star cluster 5500 LY away) - one of four 60-minute observations for in-flight pointing check - one 150 GHz telescope shown, simple filtering - compared to Planck map filtered to match Chandra/Spitzer/2MASS

SPIDER: in-flight performance - NETs in line with expectations - cosmic rays are not an issue - no obvious magnetic pick-up preliminary calibration from RCW38 - pointing reconstruction <1 - <10% total flagging expected point & stare Total in-flight optical loading instrument frequency (GHz) in-band power (pw) SPIDER 95 0.25 SPIDER 150 0.35 BOOMERanG 150 0.75 BICEP2 150 4.7 corresponding to a warm telescope emissivity of ~0.3% ε P opt /ktδν with T=250K

SPIDER: recovery Credits: British Antarctic Survey

SPIDER2 Planck x BICEP 2015 - foreground-optimized channel: 280 GHz - very hard to observe from the ground - r < 0.03 (3σ) with foregrounds - planning for Dec 2017, pending recovery new cryostat under construction! Fraisse+ 2013

QUESTIONS? SCAR AAA: site testing at mm wavelengths in Northern Hemisphere