10-14 October 2016
Milan Hotel
Europe/Moscow timezone

The high-frequency gravitational waves in exact inflationary models with Gauss-Bonnet term

11 Oct 2016, 17:00
15m
Rossini (Milan Hotel)

Rossini

Milan Hotel

Shipilovskaya Street, 28A, Moscow, Russia, 115563
Plenary/section talk Nuclear physics and particle physics Nuclear physics and particle physics - parallel III

Speakers

Prof. ANDREY Morozov (Bauman Moscow State Technical University) Mr. Igor Fomin (Bauman Moscow State Technical University)

Description

The theory of the cosmological inflation successfully describes the accelerated expansion of the universe evolution at early stages. Also, inflation in the early universe has become the standard model for the generation of cosmological perturbations in the universe, the seeds for large-scale structure and temperature anisotropies of the cosmic microwave background. Quantum fluctuations of the inflaton field give rise to an almost scale-invariant power spectrum of cosmological perturbations. String theory is often regarded as the leading candidate for unifying gravity with the other fundamental forces and for a quantum theory of gravity. It is known that the effective supergravity action from superstrings induces correction terms of higher order in the curvature, which may play a significant role in the early universe. The simplest such correction is the Gauss-Bonnet term in the low-energy effective action of the string theory. Such term provides the possibility of avoiding the initial singularity of the Universe. We consider an action with the Gauss-Bonnet term that is coupled to a scalar field \begin{equation} S_{GB}=\int d^{4}x\sqrt{-g}\left[\frac{1}{2}R-\frac{1}{2}(\partial^{\mu}\phi\partial_{\mu}\phi)-V(\phi)-\frac{1}{2}\xi(\phi)R^{2}_{GB}\right], \end{equation} where $\phi$ is an inflaton field with a potential $V(\phi)$, $R$ is the Ricci scalar curvature of the spacetime, $R^{2}_{\rm GB} = R_{\mu\nu\rho\sigma} R^{\mu\nu\rho\sigma} - 4 R_{\mu\nu} R^{\mu\nu} + R^2$ is the Gauss-Bonnet term, and $8\pi G=c=1$. The Gauss-Bonnet coupling $\xi(\phi)$ is required to be a function of a scalar field in order to give nontrivial effects on the background dynamics. The method of exact solutions of the background dynamical equations in a spatially flat Friedmann-Robertson-Walker universe is based on the connection between Hubble parameters for inflation with Gauss-Bonnet term and standard inflation is considereded in this work. On the basis of this connection we calculate the exact values of the parameters of cosmological perturbations at the crossing of the Hubble radius for the inflationary models with Gauss-Bonnet correction. The detection of relic gravitational waves can provide the main information about early universe and can be used to test the theoretical models. In this context, it is important to develop a new methods for the detection of gravitational waves. One of the promising method in the high-frequency part of the spectrum is based on the low-frequency optical resonance phenomenon in the Fabry-Perot interferometers. The description of this method and comparison with another methods are also presented.

Primary authors

Prof. ANDREY Morozov (Bauman Moscow State Technical University) Mr. Igor Fomin (Bauman Moscow State Technical University)

Presentation Materials

Your browser is out of date!

Update your browser to view this website correctly. Update my browser now

×