2017
DOI: 10.1103/physrevd.95.083507
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Detailed investigation of the duration of inflation in loop quantum cosmology for a Bianchi I universe with different inflaton potentials and initial conditions

Abstract: There is a wide consensus on the correct dynamics of the background in loop quantum cosmology. In this article we make a systematic investigation of the duration of inflation by varying what we think to be the most important "unknowns" of the model: the way to set initial conditions, the amount of shear at the bounce and the shape of the inflaton potential.

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Cited by 44 publications
(48 citation statements)
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“…For exemple, even within the narrow community of loop quantum cosmology, there is a lively debate on the "most probable" number of inflationary e-folds predicted by the model after the bounce. The approach advocated in [24,25] does not agree at all with the one pushed in [26][27][28][29]. Another known huge discrepancy is between the probability for inflation estimated in [30] and the one calculated in [31].…”
Section: Fine-tuning and Inflation Potentialmentioning
confidence: 80%
“…For exemple, even within the narrow community of loop quantum cosmology, there is a lively debate on the "most probable" number of inflationary e-folds predicted by the model after the bounce. The approach advocated in [24,25] does not agree at all with the one pushed in [26][27][28][29]. Another known huge discrepancy is between the probability for inflation estimated in [30] and the one calculated in [31].…”
Section: Fine-tuning and Inflation Potentialmentioning
confidence: 80%
“…As we explained in Sec. V, this is a subtle issue during the bouncing phase because in general there is not a preferred initial state for a quantum field in arbitrarily curved spacetime [62,66,67] (see also [68,69] for a recent discussion). The general solution of the Bogoliubov coefficients α k and β k given by Eqs.…”
Section: Discussionmentioning
confidence: 99%
“…In the framework of LQC, various sets of initial conditions have been investigated [38,55,[62][63][64][65][66][67][68][69]. However, this is a subtle issue, because in general there is not a preferred initial state for a quantum field in arbitrarily curved space-times.…”
Section: A Initial Conditions Of Primordial Perturbationsmentioning
confidence: 99%
“…Theμ scheme made it possible to perform thermodynamical analyses where the Loopquantized FLRW model is considered a thermodynamical system, and the energy density and pressure are given a precise thermodynamical meaning [97,98]; the computations for the duration of the inflationary de Sitter phase give results consistent with the minimum amount of e-folds necessary to solve the paradoxes (although slightly higher, depending on some parameters, such as the shear at the Bounce in anisotropic models), predict a phase of deflation in the contracting branch and also allow the extension of the standard inflationary paradigm from the Planck scale up to the onset of slow roll inflation, yielding novel effects, such as non-Gaussianities [99][100][101][102][103][104]. Most importantly, the improved scheme allows for a computation of the primordial power spectrum through two main methods: in the first, the implementation of holonomy corrections as a deformed algebra yields a slightly blue-tilted scale invariant spectrum followed by oscillations and an exponential behavior in the ultraviolet [105,106]; in the other, a test field approximation is used such that the evolution of tensor modes on any background quantum geometry is completely equivalent to that of the same modes propagating on a smooth but quantum-corrected metric called "dressed metric", and it is able to recover the red-titled ultraviolet power spectrum of classical cosmology [99,107].…”
Section: Improved Loop Quantum Cosmologymentioning
confidence: 63%