Analysis of Large Scale Structure using Percolation, Genus and Shape Statistics (original) (raw)

1999, Proceedings of the International Astronomical Union

We study a class of FRW space-times with a non-minimally coupled scalar field. We find exact solutions of the Klein-Gordon equation and show that negative values of the coupling parameter xi, lead to more long range power in the two point function and in the vacuum expectation value of the energy-momentum tensor tmn. This fundamentally affects Inflationary particle production of massless non-minimal scalars since the dominant contribution to comes from Hubble-scale modes. As a result the energy density of created scalar particles exceeds that of conventional matter at late times, leading to Omegam < 1 and a `coasting' expansion rate a propto t. Thus Inflation can generically predict Omegam < 1 while retaining a flat geometry if the vacuum contains contributions from massless non-minimal scalar fields. This might provide a resolution to the `Omega problem' for low density cosmological models.

Does Inflationary Particle Production Suggest Omegam < 1?

Phys Rev Lett, 1998

We study a class of Friedmann-Robertson-Walker spacetimes with a nonminimally coupled light massive scalar field. Values of the coupling parameter ξ<0 enhance long range power in the vacuum expectation value of the energy-momentum tensor <Tμν> and fundamentally alter the nature of inflationary particle production: the energy density of created particles behaves like an effective cosmological constant, leading generically to Ωm<1 in clustered matter and providing a possible resolution of the `` Ω problem'' for low density cosmological models.

A new phase of scalar field in a non-minimal model for inflation

arXiv: Cosmology and Nongalactic Astrophysics, 2013

W consider the dynamics of a scalar field non-minimally coupled to gravity in the context of cosmology. It is demonstrated that there exists a new phase for the scalar field, in addition to the inflationary and dust-like (reheating period) phases. Analytic expressions for the scalar field and the Hubble parameter, which describe the new phase are given. The Hubble parameter indicates an accelerating expanding Universe. We explicitly show that the scalar field oscillates with time- dependent frequency. Moreover, an interaction between the scalar field in the new phase and other fields is discussed. It turns out that the parametric resonance is absent, which is another crucial difference between the dynamic of the scalar field in the new phase and dust-like phase.

Nonequilibrium evolution of scalar fields in FRW cosmologies

Physical Review D, 1994

We derive the effective equations for the out of equilibrium time evolution of the order parameter and the fluctuations of a scalar field theory in spatially flat FRW cosmologies.The calculation is performed both to one-loop and in a non-perturbative, self-consistent Hartree approximation.The method consists of evolving an initial functional thermal density matrix in time and is suitable for studying phase transitions out of equilibrium. The renormalization aspects are studied in detail and we find that the counterterms depend on the initial state. We investigate the high temperature expansion and show that it breaks down at long times. We also obtain the time evolution of the initial Boltzmann distribution functions, and argue that to one-loop order or in the Hartree approximation, the time evolved state is a ``squeezed'' state. We illustrate the departure from thermal equilibrium by numerically studying the case of a free massive scalar field in de Sitter and radiation dominated cosmologies. It is found that a suitably defined non-equilibrium entropy per mode increases linearly with comoving time in a de Sitter cosmology, whereas it is {\it not} a monotonically increasing function in the radiation dominated case.

FRW-Type Cosmologies and Structure Formation

1999

We derive the growth of density perturbations in Newtonian cos-mological models. A special case where the source of the particle creation is Ψ = 3nβH is examined. Constraints on the value of β from the observed anisotropy of the cosmic microwave background radiation are also obtained.

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