CMB and the Topology of the Universe

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30/8/2005 COSMO-05, Bonn 2005 1 CMB and the Topology of the Universe Dmitri Pogosyan, UAlberta With: Tarun Souradeep Dick Bond and: Carlo Contaldi Adam Hincks Simon White, Garching, last week: Open questions in Cosmology: Is our Universe is finite or infin Is its space curved ? ….

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CMB and the Topology of the Universe. Dmitri Pogosyan, UAlberta. With: Tarun Souradeep Dick Bond and: Carlo Contaldi Adam Hincks. Simon White, Garching, last week: Open questions in Cosmology: Is our Universe is finite or infinite? Is its space curved ? …. - PowerPoint PPT Presentation

Transcript of CMB and the Topology of the Universe

Page 1: CMB and the Topology of the Universe

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CMB and the Topology of the Universe

Dmitri Pogosyan, UAlberta

With:

Tarun Souradeep

Dick Bond

and:

Carlo Contaldi

Adam Hincks

Simon White, Garching, last week:

Open questions in Cosmology:

Is our Universe is finite or infinite? Is its space curved ? ….

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Preferred parameter region, tot=1.02 ± 0.02

Ωtot=1.01RLSS/Rcurv=0.3

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How Big is the Observable Universe ?

Relative to the local curvature & topological scales

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Dirichlet domain and dimensions of the compact space

RLS < R<

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Dirichlet domain and dimensions of the compact space

RLS > R>

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Absence of large scale powerAbsence of large scale power

NASA/WMAP science team

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Correlation function of isotropic CMB

Oscillations in the angular spectrumcome from this break

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Perturbations in Compact space

• Spectrum has the lowest eigenvalue.• Spectrum is discrete, hence statistics in general is

anisotropic, especially at large scales.• Statistical properties can be inhomogeneous.• However, perturbations are Gaussian, and CMB

temperature fluctuations are fully described by pixel-pixel correlation matrix CT(p,p’)

• We implemented general method of images to compute CT(p,p’) for arbitrary compact topology (Bond,Pogosyan, Souradeep, 1998,2002)

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Pixel-pixel correlation with compact topology (using method of images, BPS, Phys Rev D. 2000)

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Example of strong correlation on last scattering surface

These two points on LSS are identical

And so are these

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Correlated Circles (after Cornish, Spergel, Starkman et al, 1998,2004)

(Figure: Bond, Pogosyan & Souradeep 1998, 2002)

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Temperature along the correlated circles(pure LSS signal)

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Temperature along the correlated circles (ISW modification)

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Positive curvature multiconnected Positive curvature multiconnected universe ?universe ?

: Perhaps, a Poincare dodecahedron

“Soccer ball cosmos” ?

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Isotropic Cpp’D/RLSS=10

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Surface term to DT/TD/RLSS=0.3

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Complete, surface and integrated large-angle ΔT/T

D/RLSS=0.3

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Variation of the pixel varianceD/RLSS=0.3

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Constraining the models from maps

• Complete topological information is retained when comparison with data is done on map level

• Low res (Nside=16) maps contain most information, although special techniques as circle searching may benefit from finer pixalization. The

cost – additional small scale effects which mask topological correlations. • Main signal comes from effects, localized in space, e.q on LSS. But even integrated along the line of sight contributions retain signature of compact topology.

• Orientation of the space (and, possibly, position of observer) are additional parameters to consider. What is the prior for them ?

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Likelehood comparison of compact closed

versus flat Universe with

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NASA/WMAP science team

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''*

'' mmlllmllm Caa

Single index n: (l,m) -> n

Diagonal

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Inadequacy of isotropized Cl’s:

alm cross correlation

Very small space Just a bit smaller than LSS

2 3 4 5 6 7 8 9 10 2 3 4 5 6 7 8 9 10

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Compression to isotropic Cls is lossy Inhanced cosmic variance of Cl’s

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2212

2 )]ˆ,ˆ()(8

1[)12(

21nnCddd nn

Bipolar Power spectrum (BiPS) :Bipolar Power spectrum (BiPS) :A Generic Measure of Statistical AnisotropyA Generic Measure of Statistical Anisotropy

A A weighted averageweighted average of the correlation function of the correlation function over all rotationsover all rotations

1)(0

Except forExcept for 0 when when

Bipolar multipole index

(This slide is provided as a free advertisement for T. Souradeep talk, Wednesday)

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Conclusions• A fundamental question – whether our Universe is finite or infinite –is still

open.

• The region near Otot=1 is rich with possibilities, with negatively or positively curved or flat spaces giving rise to distinct topological choices.

• Modern CMB data shows that small Universes with V < VLS are failing to describe the temperature maps. Reason – complex correlation are not really observed (in line with circle finding results).

• This is despite the fact that it is not too difficult to fit the low l suppression of isotropized angular power spectrum.

• Integrated along the line of sight contribution to temperature anisotropy masks and modifies topology signature. It must be taken into account for any accurate quantitative restrictions on compact spaces.

• Full likelihood analysis assumes knowledge of the models. Model independent search for statistical anisotropy calls for specialized techniques – see talk on BiPS by Tarun Souradeep on Wednesday.