Too perfect? Where are the fluctuations? Gil Holder Herschel - - PowerPoint PPT Presentation

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Too perfect? Where are the fluctuations? Gil Holder Herschel - - PowerPoint PPT Presentation

Too perfect? Where are the fluctuations? Gil Holder Herschel (Spire) 100 sq deg with full overlap with SPT deep field (23h30,-55d) 250,350,500 um Clustering of Galaxies: Projected sky maps of large scale structure have ~1-10%


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Too perfect? Where are the fluctuations?

Gil Holder

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SLIDE 2

Herschel (Spire)

  • 100 sq deg with

full overlap with SPT deep field (23h30,-55d)

  • 250,350,500 um
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SLIDE 3

Clustering of Galaxies:

Projected sky maps of large scale structure have ~1-10% fluctuations

  • Radio and IR/submm

sources presumably trace the large scale matter fluctuations

  • Back of the envelope:

– Power spectrum contribution: mean T2 x projected clustering amplitude – Arcminute scales: few Mpc has clustering ~1 in 3D, divide by number of independent cells along line of sight => 1e-3

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CMB Angular Power Spectrum

Well-fit by just 5+1 parameters: Dark energy, Dark matter, Baryon density, Initial amplitude, Power-law index+optical depth

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Angular Power Spectra at mm-wavelengths

  • large angles

dominated by CMB

  • small scales

dominated by emission from galaxies

– combination of shot noise in galaxy number & intrinsic clustering from large scale structure

10 90

  • 1
  • 10

100 1000 500 1500 2500 10 5 Angular Scale 6000 10000 2 1

Planck SPT - S13 SPT 150 GHz SPT 220 GHz SPT 95 GHz

George et al 2015

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SLIDE 6

Galaxy clustering at mm/submm wavelengths

  • cleanly measured

at many frequencies

  • consistent with

~10% rms fluctuations on scales of a few arcminutes

Addison, Dunkley & Bond 2013

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SLIDE 7

HerMES power spectra

Combined 5 fields

  • ver 70 deg2

Viero & Wang et al. (2012b) arXiv: 1208.5049

l = 216 l = 21,600 Poisson 2-halo

2-halo

1-halo

1-halo

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SLIDE 8

Planck CIB Measurements

Planck collaboration 2012

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Planck CIB Measurements

Planck collaboration 2012

Lenz, Hensley & Dore 1706.00011

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Clustering of Galaxies:

Projected sky maps of large scale structure have ~1-10% fluctuations

  • Radio and IR/submm

sources presumably trace the large scale matter fluctuations

  • Back of the envelope:

– Power spectrum contribution: mean T2 x projected clustering amplitude – Arcminute scales: few Mpc has clustering ~1 in 3D, divide by number of independent cells along line of sight => 1e-3

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SLIDE 11

Angular Power Spectra at mm-wavelengths

  • large angles

dominated by CMB

  • small scales

dominated by emission from galaxies

– combination of shot noise in galaxy number & intrinsic clustering from large scale structure

10 90

  • 1
  • 10

100 1000 500 1500 2500 10 5 Angular Scale 6000 10000 2 1

Planck SPT - S13 SPT 150 GHz SPT 220 GHz SPT 95 GHz

George et al 2015

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SLIDE 12

CMB 20 years ago….

  • possibly a

peak, upper limits on small scales

  • typical upper

limits measured in 10s of uK

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Bennett, Turner & White 1997

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Upper limits ~2000

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Holzapfel et al 2000 μK2

Qflat2=5/12 l(l+1)Cl/2π

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Upper limits ~2000

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Holzapfel et al 2000 μK2

Qflat2=5/12 l(l+1)Cl/2π

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SLIDE 15

Excess radio emission at low frequencies?

Fixsen et al 2011

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Low-frequency CMB/Radio Background Upper Limits

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T-Tcmb T-Tcmb-Tcounts

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SLIDE 17
  • minimal assumption:

unbiased tracer of linear (2-halo) fluctuations

  • old searches for

CMB anisotropy found no evidence for any fluctuations at radio wavelengths

If there is an excess, it is remarkably unclustered

1•104 2•104 3•104 multipole l 0.01 0.10 [l(l+1)Cl/2]1/2 (T/T) VLA 4.9 GHz VLA 8.4 GHz ATCA 8.7 GHz Planck 857 GHz C(↵) = Z d⇧ 1 ⇧2 d f d⇧ 2P( ↵ ⇧, ⇧) ) is the matter power spectrum at

GH 2014

Fomalont et al 1988 Partridge et al 1997 Subrahmanyan et al 2000

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  • if not foreground

contamination, must be either

– extremely diffuse (no small scale structure on scales probed by VLA or ATCA) – at very high redshift (where intrinsic clustering amplitudes are lower)

If there is an excess, it is remarkably unclustered

GH 2014

1•104 2•104 3•104 0.01 0.10 VLA 4.9 GHz VLA 8.4 GHz ATCA 8.7 GHz

z=[0,1] z=[0,2] z=[5,10]

1 Mpc/h 2 Mpc/h

Planck 857 GHz

⇧ [⇧(⇧ + 1)C⇥/2]1/2(∆T/T )

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Conclusions

  • galaxies are clustered

– presumably because they are tracing dark matter, which is clustered

  • a background that is a superposition of a bunch of galaxies

will show clustering

– e.g., the cosmic infrared background shows clustering at the level

  • f ~10% on scales of a few arcminutes
  • the radio background on arc minute scales is smooth at the

percent level

– it probably isn’t made up of a simple superposition of galaxies

  • unless: small-scale features are smoothed out or at high redshift so that

the dark matter is relatively unclustered or coming from rare enough sources that the (small-area) radio CMB limits don’t apply

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