skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Estimation of inflation parameters for Perturbed Power Law model using recent CMB measurements

Journal Article · · Journal of Cosmology and Astroparticle Physics
; ;  [1];  [2]
  1. Inter University Centre for Astronomy and Astrophysics, Post Bag 4, Ganeshkhind, Pune-411007 (India)
  2. Dept. of Physics, Alphonsa College, Pala, 686574 India (India)

Cosmic Microwave Background (CMB) is an important probe for understanding the inflationary era of the Universe. We consider the Perturbed Power Law (PPL) model of inflation which is a soft deviation from Power Law (PL) inflationary model. This model captures the effect of higher order derivative of Hubble parameter during inflation, which in turn leads to a non-zero effective mass m{sub eff} for the inflaton field. The higher order derivatives of Hubble parameter at leading order sources constant difference in the spectral index for scalar and tensor perturbation going beyond PL model of inflation. PPL model have two observable independent parameters, namely spectral index for tensor perturbation ν{sub t} and change in spectral index for scalar perturbation ν{sub st} to explain the observed features in the scalar and tensor power spectrum of perturbation. From the recent measurements of CMB power spectra by WMAP, Planck and BICEP-2 for temperature and polarization, we estimate the feasibility of PPL model with standard ΛCDM model. Although BICEP-2 claimed a detection of r=0.2, estimates of dust contamination provided by Planck have left open the possibility that only upper bound on r will be expected in a joint analysis. As a result we consider different upper bounds on the value of r and show that PPL model can explain a lower value of tensor to scalar ratio (r<0.1 or r<0.01) for a scalar spectral index of n{sub s}=0.96 by having a non-zero value of effective mass of the inflaton field m{sup 2}{sub eff}/H{sup 2}. The analysis with WP + Planck likelihood shows a non-zero detection of m{sup 2}{sub eff}/H{sup 2} with 5.7 σ and 8.1 σ respectively for r<0.1 and r<0.01. Whereas, with BICEP-2 likelihood m{sup 2}{sub eff}/H{sup 2} = −0.0237 ± 0.0135 which is consistent with zero.

OSTI ID:
22382007
Journal Information:
Journal of Cosmology and Astroparticle Physics, Vol. 2015, Issue 01; Other Information: Country of input: International Atomic Energy Agency (IAEA); ISSN 1475-7516
Country of Publication:
United States
Language:
English

Similar Records

Revised cosmological parameters after BICEP 2 and BOSS
Journal Article · Sun Feb 01 00:00:00 EST 2015 · Journal of Cosmology and Astroparticle Physics · OSTI ID:22382007

Planck 2015 results: XIII. Cosmological parameters
Journal Article · Tue Sep 20 00:00:00 EDT 2016 · Astronomy and Astrophysics · OSTI ID:22382007

Planck 2015 results: XX. Constraints on inflation
Journal Article · Tue Sep 20 00:00:00 EDT 2016 · Astronomy and Astrophysics · OSTI ID:22382007