TY - JOUR
T1 - Phenomenology with fluctuating quantum geometries in loop quantum cosmology
AU - Agullo, Ivan
AU - Ashtekar, Abhay
AU - Gupt, Brajesh
N1 - Publisher Copyright:
© 2017 IOP Publishing Ltd.
PY - 2017/3/7
Y1 - 2017/3/7
N2 - The goal of this paper is to probe phenomenological implications of large fluctuations of quantum geometry in the Planck era, using cosmology of the early universe. For the background (Friedmann, Lemaître, Robertson, Walker) quantum geometry, we allow 'widely spread' states in which the relative dispersions are as large as in the Planck regime. By introducing suitable methods to overcome the ensuing conceptual and computational issues, we calculate the power spectrum and the spectral index n s(k) of primordial curvature perturbations. These results generalize the previous work in loop quantum cosmology which focused on those states which were known to remain sharply peaked throughout the Planck regime. Surprisingly, even though the fluctuations we now consider are large, their presence does not add new features to the final and n s(k): within observational error bars, their effect is degenerate with a different freedom in the theory, namely the number of pre-inflationary e-folds between the bounce and the onset of inflation. Therefore, with regard to observational consequences, one can simulate the freedom in the choice of states with large fluctuations in the Planck era using the simpler, sharply peaked states, simply by allowing for different values of NB∗.
AB - The goal of this paper is to probe phenomenological implications of large fluctuations of quantum geometry in the Planck era, using cosmology of the early universe. For the background (Friedmann, Lemaître, Robertson, Walker) quantum geometry, we allow 'widely spread' states in which the relative dispersions are as large as in the Planck regime. By introducing suitable methods to overcome the ensuing conceptual and computational issues, we calculate the power spectrum and the spectral index n s(k) of primordial curvature perturbations. These results generalize the previous work in loop quantum cosmology which focused on those states which were known to remain sharply peaked throughout the Planck regime. Surprisingly, even though the fluctuations we now consider are large, their presence does not add new features to the final and n s(k): within observational error bars, their effect is degenerate with a different freedom in the theory, namely the number of pre-inflationary e-folds between the bounce and the onset of inflation. Therefore, with regard to observational consequences, one can simulate the freedom in the choice of states with large fluctuations in the Planck era using the simpler, sharply peaked states, simply by allowing for different values of NB∗.
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U2 - 10.1088/1361-6382/aa60ec
DO - 10.1088/1361-6382/aa60ec
M3 - Article
AN - SCOPUS:85015805234
SN - 0264-9381
VL - 34
JO - Classical and Quantum Gravity
JF - Classical and Quantum Gravity
IS - 7
M1 - 074003
ER -