Talk detail

MG14 - Talk detail

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 Participant

Banerjee, Shreya

Institution

TATA INSTITUTE OF FUNDAMENTAL RESEARCH  - DR. HOMI BHABHA ROAD, NAVY NAGAR, COLABA - MUMBAI - MAHARASHTRA - India

Session

EU1

Accepted

Yes

Order

3

Time

14:30 15'

Talk

Oral abstract

Title

Classicalization Of Inflationary Perturbations By Collapse Models
Coauthors Das, Suratna; Sahu, Satyabrata; Banerjee, Shreya; Singh,Tejinder P.

Abstract

The success of the inflationary paradigm rests on its ability to explain the observed classicality of primordial quantum fluctuations despite their quantum origin. Squeezing of primordial cosmological inhomogeneities along with the mechanism of decoherence accounts for many aspects of this quantum to classical transition, although it remains a matter of debate as to whether this is sufficient to explain the issue of realization of a single outcome from a quantum ensemble given that the universe is a closed system. Apart from decoherence there have been attempts to resolve this issue through Continuous Spontaneous Localization (CSL), which is a stochastic nonlinear modification of the non-relativistic Schrodinger equation . In this talk, I shall revisit one such recently proposed working model of classicalization by spontaneous collapse to look for possible modifications to scalar and tensor power spectra and their implications. I shall show that it can potentially change the consistency relation of single-field models and a precise measurement of tensor spectral tilt and its running could serve as a test of such dynamics in the early universe. [Journal-ref: Phys. Rev. D 88, 085020 (2013); Phys. Rev. D 90, 043503 (2014)]

Pdf file

pdf file 

Session

DE1

Accepted

Yes

Order

5

Time

15:50 15'

Talk

Oral abstract

Title

Cosmic Acceleration In A Model Of Fourth Order Gravity
Coauthors Banerjee, Shreya; Jayswal, Nilesh; Singh, Tejinder. P

Abstract

We investigate a fourth order model of gravity, having a free length parameter, and no cosmological constant or dark energy. We consider cosmological evolution of a flat Friedmann universe in this model for the case that the length parameter is of the order of present Hubble radius. By making a suitable choice for the present value of the Hubble parameter, and value of third derivative of the scale factor (the jerk) we find that the model can explain cosmic acceleration to the same degree of accuracy as the standard concordance model. If the free length parameter is assumed to be time-dependent, and of the order of the Hubble parameter of the corresponding epoch, the model can still explain cosmic acceleration, and provides a possible resolution of the cosmic coincidence problem. We work out the effective equation of state, and its time evolution, in our model. We also compare redshift drift in our model, with that in the standard model. The equation of state and the redshift drift serve to discriminate our model from the standard model. [arXiv:1504.01867 (2015), submitted to Physical Review D].

Pdf file

pdf file 

Session

EU2

Accepted

Yes

Order

3

Time

15:45 15'

Talk

Oral abstract

Title

Cosmological Constant, Quantum Measurement, And The Problem Of Time
Coauthors Banerjee, Shreya; Bera, Sayantani; Singh, Tejinder. P

Abstract

Three of the big puzzles of theoretical physics are the following: (i) There is apparently no time evolution in the dynamics of quantum general relativity, because the allowed quantum states must obey the Hamiltonian constraint. (ii) During a quantum measurement, the state of the quantum system randomly collapses from being in a linear superposition of the eigenstates of the measured observable, to just one of the eigenstates, in apparent violation of the predictions of the deter- ministic, linear Schro ̈dinger equation. (iii) The observed value of the cosmological constant is exceedingly small, compared to its natural value, creating a serious fine-tuning problem. In this essay we propose a novel idea to show how the three problems help solve each other. [This essay received an honourable mention in the Gravity Research Foundation 2015 Essay Contest. arXiv:1505.03805 (2015), submitted to Int. J. Mod. Phys. D]

Pdf file

pdf file 

Session

AT1

Accepted

Yes

Order

12

Time

17:50 10'

Talk

Oral abstract

Title

Hysteresis in the Sky
Coauthors Choudhury Sayantan; Banerjee Shreya

Abstract

Hysteresis is a phenomenon occurring naturally in several magnetic and electric materials in condensed matter physics. When applied to cosmology, aka cosmological hysteresis, has interesting and vivid implications in the scenario of a cyclic bouncy universe. Most importantly, this physical prescription can be treated as an alternative proposal to inflationary paradigm. Cosmological hysteresis is caused by the asymmetry in the equation of state parameter during expansion and contraction phase of the universe, due to the presence of a single scalar field. This process is purely thermodynamical in nature, results in a non-vanishing hysteresis loop integral (∮pdV) in cosmology. When applied to variants of modified gravity models -1) Dvali-Gabadadze-Porrati (DGP) brane world gravity, 2) Cosmological constant dominated Einstein gravity, 3) Loop Quantum Gravity (LQG), 4) Einstien-Gauss-Bonnet brane world gravity and 5) Randall Sundrum single brane world gravity (RSII), under certain circumstances, this phenomenon leads to the increase in amplitude of the consecutive cycles and to a universe with older and larger successive cycles, provided we have physical mechanisms to make the universe bounce and turnaround. This inculcates an arrow of time in a dissipationless cosmology. Remarkably, this phenomenon appears to be widespread in several cosmological potentials in variants of modified gravity background, which we explicitly study for- i) Hilltop, ii) Natural and iii) Colemann-Weinberg potentials, in this paper. Semi-analytical analysis of these models, for different potentials with minimum/minima, show that the conditions which creates a universe with an ever increasing expansion, depend on the signature of the hysteresis loop integral (∮pdV) as well as on the variants of model parameters. [arXiv:1506.02260, (2015)]

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