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DC Field | Value | Language |
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dc.contributor.author | Sarkar, Tapomoy Guha | - |
dc.date.accessioned | 2024-04-16T08:57:28Z | - |
dc.date.available | 2024-04-16T08:57:28Z | - |
dc.date.issued | 2009-08 | - |
dc.identifier.uri | https://iopscience.iop.org/article/10.1088/1475-7516/2009/08/019/meta | - |
dc.identifier.uri | http://dspace.bits-pilani.ac.in:8080/jspui/xmlui/handle/123456789/14564 | - |
dc.description.abstract | The late-time growth of large scale structures is imprinted in the CMBR anisotropy through the Integrated Sachs Wolfe (ISW) effect. This is perceived to be a very important observational probe of dark energy. Future observations of redshifted 21-cm radiation from the cosmological neutral hydrogen (HI) distribution hold the potential of probing the large scale structure over a large redshift range. We have investigated the possibility of detecting the ISW through cross-correlations between the CMBR anisotropies and redshifted 21-cm observations. Assuming that the HI traces the dark matter, we find that the ISW-HI cross-correlation angular power spectrum at an angular multipole ℓ is proportional to the dark matter power spectrum evaluated at the comoving wave number ℓ/r, where r is the comoving distance to the redshift from which the HI signal originated. The amplitude of the cross-correlation signal depends on parameters related to the HI distribution and the growth of cosmological perturbations. However, the cross-correlation is extremely weak as compared to the CMBR anisotropies and the predicted HI signal. Even in an ideal situation, the cross-correlation signal is smaller than the cosmic variance and a statistically significant detection is not very likely. | en_US |
dc.language.iso | en | en_US |
dc.publisher | IOP | en_US |
dc.subject | Physics | en_US |
dc.subject | CMBR ISW | en_US |
dc.subject | CMBR anisotropy | en_US |
dc.title | The CMBR ISW and HI 21 cm cross-correlation angular power spectrum | en_US |
dc.type | Article | en_US |
Appears in Collections: | Department of Physics |
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