2018
DOI: 10.1140/epjc/s10052-018-6199-9
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Viable super inflation scenario from F(T) modified teleparallel gravity

Abstract: Viability of the super inflation scenario is discussed in F(T ) modified teleparallel gravity. We calculate the power spectrum of the primordial curvature and tensor perturbations, and we derive two important parameters corresponding to these perturbations, i.e., spectral index parameter n s and scalar-to-tensor ratio r . We observe that the super inflation scenario provides a nearly scale invariant power spectrum of scalar and tensor perturbations in the observational bounds of n s and r , according to choosi… Show more

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Cited by 17 publications
(4 citation statements)
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“…Of course inflation is known to start quite earlier than the horizon crossing time instance, but we choose t i to be the horizon crossing time instance, because the condition k = aH is vital for the calculation of the power spectrum, both scalar and tensor. Also we need to note that the initial condition of the constant-roll k-inflation theory may be a Bunch-Davies vacuum state [82] or a quasi-de Sitter like expansion which leads to a Bunch-Davies vacuum state [83]. Expressed in terms of the scalar field, the e-foldings number is equal to,…”
Section: Constant-roll K-inflation Gravity: Equations Of Motion and I...mentioning
confidence: 99%
“…Of course inflation is known to start quite earlier than the horizon crossing time instance, but we choose t i to be the horizon crossing time instance, because the condition k = aH is vital for the calculation of the power spectrum, both scalar and tensor. Also we need to note that the initial condition of the constant-roll k-inflation theory may be a Bunch-Davies vacuum state [82] or a quasi-de Sitter like expansion which leads to a Bunch-Davies vacuum state [83]. Expressed in terms of the scalar field, the e-foldings number is equal to,…”
Section: Constant-roll K-inflation Gravity: Equations Of Motion and I...mentioning
confidence: 99%
“…From a thermodynamics perspective, it was obtained the Friedmann equations in the studies [7,63]. In the background of the line element which describes a homogeneous and isotropic spacetime geometry, i.e., Friedmann-Robertson-Walker metric,…”
Section: Modified Friedmann Equationsmentioning
confidence: 99%
“…It is worth emphasizing that the slow-roll indices, and consequently, the inflation parameters (7) should be calculated at the horizon crossing point(k = a H) as the fluctuations in the inflation field [71,72] (scalar field φ) become crucial at this point. Here, k shows the comoving wave vectors [63,73]. We assume that the inflation begins where the fluctuations of the field occur during the horizon crossing.…”
Section: Modified Friedmann Equationsmentioning
confidence: 99%
“…The nature of the inflaton field motivated the elaboration of a plethora of competing cosmological models [10][11][12][13][14][15][16][17][18][19] due to the fact that the form of the inflation field is not determined and the standard phenomenological model Λ cold dark matter (ΛCDM) with the fluid parameter w = −1 rapidly decays at the end of the inflationary period [20]. Thus, the inflaton field cannot be directly regarded as a cosmological constant Λ for the late acceleration of the universe.…”
Section: Introductionmentioning
confidence: 99%