reionisation and the cross-correlation between the cmb and the 21-cm line fluctuations hiroyuki...
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![Page 1: Reionisation and the cross-correlation between the CMB and the 21-cm line fluctuations Hiroyuki Tashiro IAS, ORSAY 43rd Rencontres de Moriond La Thuile,](https://reader036.vdocument.in/reader036/viewer/2022080222/56649f515503460f94c73ddf/html5/thumbnails/1.jpg)
Reionisation and the cross-correlation between the CMB and the 21-cm line fluctuations
Hiroyuki Tashiro
IAS, ORSAY
43rd Rencontres de Moriond La Thuile, Italy
N. Aghanim (IAS, Orsay)M. Langer (IAS, Orsay)M. Douspis (IAS, Orsay)S. Zaroubi (Uuiv. of Groningen)
Based on arXiv:0802.3893
In the collaboration with
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Reionisation : When does reionisation start?How does reionisation proceed?
Introduction
We know only two observational constraints
Gunn-Peterson effect : absorption of the from the high redshift quasars
CMB anisotropies : Thomson scattering of CMB photons by electrons during reionisation
Redshifted 21 cm line fluctuations one of most promising probing methods for reionisation
Optical depth (WMAP 5 year data)
Neutral hydrogen fraction
To obtain new constraints
(Fan et al, 2006)
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The 21 cm cross correlations with CMB polarisation from the reionisation epoch
21 cm transitions of HIAbsorb 21 cm line from CMB
Emit 21 cm line to CMB
Produce fluctuations of CMB brightness temperature
Line emission : redshifted by the cosmological expansion
Multi frequency observations allow us to obtain redshift slices of Universe
{
In this talk,
Observation projects : LOFAR, MWA, SKA
CMB Doppler effect Alvarez et al. (2006)
Kinematic Sunyaev-Zeldvich effect
The cross-correlation with CMB temperatures
Salvaterra et al. (2005)
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21 cm lines fluctuations
Linear expression of the fluctuations (during the reionisation epoch)
In order to obtain the cross correlations, we need expression for spherical harmonics coefficients,
The 21 cm line fluctuations depends on and
Expanded on the spherical harmonics
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E-mode polarisation
Thomson scattering + quadrupole in CMB temperature anisotropies
produce the CMB polarisation
Primordial density fluctuations E-mode polarisation
E-mode polarisation depends on initial gravitational potential
Expression for the spherical harmonics
Source term :
Quadrupole
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The angular power spectrum of the cross-correlation
: specified by the cosmological model (
: specified by the reionisation model
From of E-mode polarisation and 21 cm lines,we can obtain the cross-correlation
)
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Toy model of reionisation
• Ionised fraction is related to the ratio of ionising photons per hydrogen
•ionising photons comes from collapsed objects ( T_vir > 10^4 )
To obtain , we make two assumptions
Cross power spectrum
Alvarez et al. (2006)
: Transfer function of matter : average bias
Evolution of average ionised fraction
: reionisation epoch
: reionisation duration
>
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Angular power spectrum of the cross-correlation
If reionisation has the long duration,quadrupole components during reionisation are superposed.
damping of the oscillations on small scales
•Spectrum shape reflects the quadrupole of CMB
1-st peak position
The angular separation scale of the quadrupole component
• The duration of reionisation induces
The longer it lasts, the more oscillations are damped.
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Angular power spectrum of the cross-correlation
The dependence on the reionisation epoch
The evolution of first peak
Multi frequency observations
E-mode polarisation : electron density
21 cm fluctuation : HI density
The shapes of power spectrum does not strongly depend on the reionisation epoch
is the redshift, when
If
,the amplitude reaches to maximum
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Angular power spectrum of the cross-correlation
Double reionisation model
The number of peaks in the first peak evolution is
the number of crossings of the 0.5 level of the ionised fraction
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Summary
The cross-correlation between 21 cm lines and E-mode polarisation
• Shape of the power spectrum : the quadrupole component of CMB temperature anisotropies
The first peak position gives the scale of the quadrupole
21 cm lines : neutral hydrogenE-mode polarisation : the optical depth
• Damping on small scales : signature of the duration of reionisation
The detection or no detection of the signal gives constraints on the duration
• first peak evolution : the signal reaches its maximum when x_e=0.5
We can follow the redshift evolution of ionisation fraction
For details, see arXiv:0802.3893
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21 cm lines fluctuations
HI 21 cm transitionsAbsorb 21 cm lines from CMB
Emit 21 cm lines to CMB
Produce the fluctuations of CMB brightness temperature !
The cosmological redshift : 21 line is redshiftd
Liner expression of the fluctuations (during the reionisation epoch)
Observing the 21/(1+z) lines, we obtain the redshift slice of Universe !
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First peak evolution of the power spectrum