POINCARE - cmbpol.uchicago.edu

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Goddard Space Flight Center POINCARE P olarimeter for O bserving In flationary C osmology at the R eionization E poch David T. Chuss NASA Goddard Space Flight Center CMBPol Systematics Workshop Annapolis, MD July 29, 2008

Transcript of POINCARE - cmbpol.uchicago.edu

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Goddard Space Flight Center

POINCAREPolarimeter for Observing Inflationary Cosmology at

the Reionization Epoch

David T. ChussNASA Goddard Space Flight Center

CMBPol Systematics WorkshopAnnapolis, MDJuly 29, 2008

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Goddard Space Flight Center

TeamJohns Hopkins

Chuck BennettBen GoldJoseph EimerLingzhen Zeng

NASA GSFCGary HinshawEd WollackHarvey MoseleyDavid ChussGeorge VoellmerJames Hinderks

U. British ColumbiaMark Halpern

NIST BoulderKent IrwinKi Won YoonWilliam DuncanSherry ChoGene HiltonMike Niemack

Northwestern U.Giles Novak

U. ColoradoNils Halverson

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Experimental DetailsAngular resolution 120’

Frequency Coverage 40-150 GHz

Sky Coverage ~Full Sky

Multipole Coverage ~2-90

Polarization ModulationVariable-delay Polarization

Modulator (VPM)

Types of Detectors Feedhorn-coupled TES

Location Ground

Expected limit on r ~0.01

Status Future

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Instrument Architecture

VPM is the first element

Fastest modulation is in Polarization (~3 Hz modulator cycle)

Q and U are measured in separate optical paths

Multiple observatories deployed to cover full sky

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Detectors

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40 GHz GSFC Detectors

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OMT Design

CPW

TESHeater

Gold meander

150 GHz CMB polarimeter fabricated

at NIST

Components designed by NIST, CU-Boulder, University of Chicago and Princeton University

Filter Design

6 mm

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Variable-delay Polarization Modulators (VPMs)

Stokes V

Stokes U

Stokes Q

Qdetector = Q cos φ + V sin φ

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Systematic Advantages of VPMs

Allows for spectropolarimetry

Used in reflection- no dielectrics to introduce differential loss

Employs small linear motions rather than large circular ones - a potential reliability advantage for space mission

More flexibility in size than HWP

Allows symmetry for “hiding” systematics in unmeasured Stokes parameter.

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Submillimeter VPMs

Voellmer et al. (2006), Krejny et al. (2008)

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•Wire diameter = 67 µm•Wire spacing = 200 µm•Grid diameter = 50 cm•Flatness < 50 µm•Wire resonant frequency > 128 Hz•2 miles of wire•2 Tons of force on the frame

50 cm

Voellmer et al. (2008)

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Data Stream

0 5000 10000 150000

Grid!Mirror Separation (microns)

H

V

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Goddard Space Flight Center

3 mm Laboratory Tests

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Goddard Space Flight Center

Systematics/CalibrationSystematic Mitigation

E → B Ensure cross-calibration is good between Q and U measurements, measuring Q, U independently

∆T → B Front-end modulation- beam shape not changed by modulator

T → B1. Beams underfill VPM so variability in edge illumination is

minimized. 2. This effect is monotonic with separation- signal is oscillatory. 3. Common mode signal is manifest in

unmeasured linear Stokes parameter.

∆TOptics → B Modulator located in front of optics. Modulate faster than temperatures can drift

∆TCold Stage → B Monitor bias, external calibrator, Calibrate using astrophysical standards.

Foregrounds → B Multiple frequencies & operation near the suspected foreground minimum

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Systematic Concerns

Concern Mitigation

Beam Walkoff location of VPM at (primary) pupil

Variable Beam Truncation sufficient edge taper; symmetry of system

Variable Grid Emission High polarization isolation; symmetry of system.

Wire Vibrations High resonant frequency (tight wires)

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Status

Pathfinder for POINCARE (single optical path) is being proposed to NSF this fall

40 GHz Detector components in fabrication at NASA/GSFC

150 GHz Detector components in fabrication at NIST/Boulder

VPM grid fabricated; VPM expected early 2009Cryostat for Pathfinder under developmentViper telescope to be shipped to JHU early Fall.