probing the epoch of reionization with the t omographic i onized-carbon

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Title Here obing the Epoch of Reionizati with the T omographic I onized-carbon M apping E xperiment (TIME) Jamie Bock Caltech / JPL CCAT Workshop, Boulder CO 21 September 2012

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Probing the Epoch of Reionization with the T omographic I onized-carbon M apping E xperiment (TIME) Jamie Bock Caltech / JPL CCAT Workshop, Boulder CO 21 September 2012. Large Scale Structure HerMES Lockman Survey Field. 3.6°. Use Maps to Measure Clustering. - PowerPoint PPT Presentation

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Page 1: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereProbing the Epoch of Reionizationwith the

Tomographic Ionized-carbonMapping Experiment (TIME)

Jamie BockCaltech / JPL

CCAT Workshop, Boulder CO21 September 2012

Page 2: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

3.6°

Large Scale StructureHerMES Lockman Survey Field

Page 3: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereUse Maps to Measure Clustering

Page 4: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereAn Example of Intensity Mapping

Page 5: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereRelationship Between Dark Matter and Galaxies

Halo Clustering Model

Cooray &Sheth 2002

Page 6: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

3.6°

Large Scale StructureHerMES Lockman Survey Field

Page 7: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

1-halo clustering

2-halo clustering

Spatial Power Spectrum of SPIRE Maps

Viero et al. arXiv 1208.5049

Page 8: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

Measuring to the Galactic Ensemble• Luminosity function• Total photon production• Large-scale structure

Science Applications• Galaxy evolution• Link between dark matter and galaxy formation• Epoch of Reionization?• Baryon Acoustic Oscillations?

Observationally Expedient• Does not require a large telescope!

Advantages of Intensity Mapping

Page 9: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HerekSZ and Galaxies: SPIRE & mm-wave

500 um

350 um

250 um

SPT Herschel/SPIREPrecise Measures of kSZ and tSZ

Correlate FIR galaxieswith CMB lensingprojected potential:

CMB lensing x CIB

Page 10: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereNear-IR Fluctuations from the EOR?

2p/q [arcsec]

Kashlinsky et al. 20053.6 um 4.5 um

2.4 um 3.2 um 4.1 um

10 arcmin

12 x 6 arcmin

Matsumoto et al. 2010

Akari

Page 11: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereAdvantages of Line Intensity Mapping

Measuring to the Galactic Ensemble• Luminosity function• Total photon production• Large-scale structure

Science Applications• Galaxy evolution• Link between dark matter and galaxy formation• Epoch of Reionization!• Baryon Acoustic Oscillations!

Observationally Expedient• Does not require a large telescope!• Does require a high-AW spectrometer

Page 12: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

Simulated Sky in C+

C+ Theory Predictions

• C+ serves as a tracer of star formation• The clustering signal traces total luminosity -> unlike a flux-limited galaxy survey• Use C+ to spatially trace SF during the reionization epoch

Gong, Cooray et al. 2012, ApJ 745, 49G

Page 13: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereCO vs C+

CO for EOR studies: Visbal & Loeb 2010, Carilli 2011, Lidz et al. 2011, Gong et al. 2011

Page 14: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereCO Foreground Contamination?

Gong et al. 2012, ApJ 745, 49G

Page 15: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereTIME: Tomographic Ionized-C Mapping Experiment

Experiment Units TIME-Full TIME-PilotAperture Diameter m 1 3 10 10Survey Area sq. degrees 16 0.01Total Integration Time hours 4000 120Free Spectral Range GHz 185 - 310 245 - 420Frequency Resolution GHz 0.4 0.65Bolometers # 20,000 265Spectral Channels # 312 265Spatial Pixels # 64 1Beam FWHM arcmin 4.4 1.5 0.4 0.3Beams in Survey Area # 2600 23,000 260,000 200Noise Equiv. Intensity MJy√s / sr 2.5 6 – 50

Int. Time per Beam hours 100 10 1 0.6z = 4.5 PN

CII (Jy2/sr2) Mpc3/h3 - 430 x 109

z = 6 PNCII (Jy2/sr2) Mpc3/h3 5.4 x 109 100 x 109

z = 7 PNCII (Jy2/sr2) Mpc3/h3 4.8 x 109 -

z = 8 PNCII (Jy2/sr2) Mpc3/h3 4.4 x 109 -

Page 16: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereTIME C+ Sensitivity Predictions

LCII fromVisbal & Loeb

Visbal & LoebD2

CO* (104)2

±1s error inMZ – M relation

10 mPo

isson

Clustering

Lidz et al. 2011D2

CO*40002

agrees withGong C+ modelat z = 7

Gong et al. 2012, ApJ 745, 49G

Page 17: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

2.5 arcmin

C+ and 21 cm Cross-Correlation

• Star formation rate vs. z• Ionization state vs. z• Bubble size

Gong et al. 2012, ApJ 745, 49G

Using 21 cm & C+ Together

Page 18: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereTIME-Pilot Sensitivity

z = 6 4.5 3.7

Goals:• Measure C+ fluctuation amplitude• Constrain high-J CO fluctuations by cross-band correlations• Determine atmospheric noise after spectral template subtraction

Page 19: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereFilter-Bank Spectrometer

Credit: Jonas ZmuidzinasSee talk by Matt Bradford later today!

• Radiation propagates down main feed line• Resonators respond in narrow bands• Couple to power detector (MKID or TES)

Page 20: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

7 m

m

SuperSpec: 80-Channel Test Device

Erik Shirokoff, chip design

Page 21: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereConclusions

EOR Science accessible with a 3-m classdedicated telescope

A moderate pilot experiment can probeC+ signal amplitude at lower z

Develop new filter-band spectrometertechnologies for CCAT

Page 22: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereLow-NEP TES BolometersWork with SQUID TD Mux

Page 23: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

Viero et al. arXiv 1208.5049

Power Spectra in 3 Bands

Page 24: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title Here

Erik Shirokoff, SuperSpec chip design

Inverted microstrip stack

Page 25: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereHigh Redshift Galaxies in HerMES500 um peaked sources

250 um 350 um 500 um *

*Confusion reduced S(500) – fS(250)

Red Source Abundance Dowell 2011, in prep.Red Source Case Study Riechers 2011, in prep.

New: Galaxies with Red Colors

Are they cold or at high redshift (z=4-7)?

Obtain mm-wave redshifts (CO, C+)!!

APEX

CSO

PdBI CARMA

ZSPEC: Bolometric spectrometer

Page 26: Probing the Epoch of  Reionization with the T omographic I onized-carbon

Title HereUse Clustering to Probe Reionization

See Cooray et al. 2004, Kashlinsky 2004

Fit to

Spitzer

Minimum

reionizatio

n

Spatial Power Spectrum Electromagnetic Spectrum

Why CIBER is Robust to Systematic Errors• Zodiacal Smoothness? Observe at different times of year• Flat Field? Use difference images, lab flat• 1/f noise? Assess using sky differences• Galaxies? Large ℓ separation from EOR• Foregrounds? EOR has very different colors• Anything else? Cross-correlate with Spitzer