Evidence for an inflationary phase transition from the LSS and CMB anisotropy data

(2000)

Authors:

J Barriga, E Gaztanaga, MG Santos, S Sarkar

On the APM power spectrum and the CMB anisotropy: Evidence for a phase transition during inflation?

ArXiv astro-ph/0011398 (2000)

Authors:

Jose Barriga, Enrique Gaztanaga, Mario Santos, Subir Sarkar

Abstract:

Adams et al. (1997b) have noted that according to our current understanding of the unification of fundamental interactions, there should have been phase transitions associated with spontaneous symmetry breaking {\em during} the inflationary era. This may have resulted in the breaking of scale-invariance of the primordial density perturbation for brief periods. A possible such feature was identified in the power spectrum of galaxy clustering in the APM survey at the scale $k \sim 0.1 h$ Mpc^{-1} and it was shown that the secondary acoustic peaks in the power spectrum of the CMB anisotropy should consequently be suppressed. We demonstrate that this prediction is confirmed by the recent Boomerang and Maxima observations, which favour a step-like spectral feature in the range $k \sim (0.06-0.6)h$ Mpc^{-1}, independently of the similar previous indication from the APM data. Such a spectral break enables an excellent fit to both APM and CMB data with a baryon density consistent with the BBN value. It also allows the possibility of a matter-dominated universe with zero cosmological constant, which we show can now account for even the evolution of the abundance of rich clusters.

On the APM power spectrum and the CMB anisotropy: Evidence for a phase transition during inflation?

(2000)

Authors:

Jose Barriga, Enrique Gaztanaga, Mario Santos, Subir Sarkar

Thermalisation after inflation

ArXiv hep-ph/0009078 (2000)

Authors:

Sacha Davidson, Subir Sarkar

Abstract:

During (re)heating of the universe after inflation, the relativistic decay products of the inflaton field $\phi$ must lose energy and additional particles must be produced to attain a thermalised state at a temperature $T_{\reh}$. We estimate the rate of energy loss via elastic and inelastic scattering interactions. Elastic scattering is an inefficient energy loss mechanism so inelastic processes, although higher order in the coupling $\alpha$, can be faster because more energy is transfered. The timescale to produce a particle number density of ${\cal O}(T_{\reh}^3)$ is the inelastic energy loss timescale, $\sim(\alpha^3 n_\phi/T_{\reh}^2)^{-1}$.

Thermalisation after inflation

(2000)

Authors:

Sacha Davidson, Subir Sarkar