PHYS08200605006 D.K. Hazra - Homi Bhabha National Institute
PHYS08200605006 D.K. Hazra - Homi Bhabha National Institute
PHYS08200605006 D.K. Hazra - Homi Bhabha National Institute
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Chapter 6<br />
Effects of primordial features on the<br />
formation of halos<br />
As we had described in the introductory chapter, apart from the CMB, the LSS data too<br />
are expected to provide constraints on the pattern as well as the characteristics of the<br />
primordial perturbations. Any significant change in the primordial scalar power spectrum<br />
will correspondingly modify the matter power spectrum [cf. Eq. (1.30)] evaluated<br />
today. Hence, the features in the inflationary scalar perturbation spectrum that we had<br />
discussed extensively in Chapters 2 and 3, in addition to their imprints on the CMB, will<br />
affect the matter power spectrum which, in turn, will leave its signatures on the formation<br />
rates of the dark matter halos. In fact, the effects of steps or oscillations in the inflaton<br />
potential on the predicted number of halos was investigated recently [126]. The analysis<br />
was carried out with the inflationary perturbation spectrum evaluated using the slow<br />
roll approximation. But, the slow roll parameters can turn large in the presence of steps<br />
or oscillatory terms in the inflationary potentials and, as a result, the power spectrum<br />
evaluated in the slow roll approximation can differ considerably from the actual power<br />
spectrum. Moreover, with the ever increasing quality of the LSS observations, in particular,<br />
the halo power spectrum constructed using the Luminous Red Galaxies (LRG) from<br />
the seventh data release (DR7) of SDSS [3, 4], it may be a worthwhile exercise to actually<br />
compare the models with the available data to arrive at additional constraints on the<br />
primordial features that we had considered in the preceding chapters.<br />
With the above points in mind, in this chapter, we shall utilize the code that we<br />
have developed to compute the inflationary perturbation spectrum (cf. Section 4.3.3) and,<br />
thereby, evaluate the corresponding matter power spectrum and the number of halos<br />
formed. We shall compute the number densities and the formation rates of halos in the<br />
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