Exact third-order density perturbation and one-loop power spectrum in general dark energy models

Under the standard perturbation theory (SPT), we obtain the fully consistent third-order density fluctuation and kernels for the general dark energy models without using the Einstein–de Sitter (EdS) universe assumption for the first time. We also show that even though the temporal and spatial compon...

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Main Authors: Seokcheon Lee, Changbom Park, Sang Gyu Biern
Format: Article
Language:English
Published: Elsevier 2014-09-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269314005565
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spelling doaj-5ce3717b4c3648b08e7561d9e3a0b2992020-11-24T22:31:08ZengElsevierPhysics Letters B0370-26931873-24452014-09-01736C40341010.1016/j.physletb.2014.07.054Exact third-order density perturbation and one-loop power spectrum in general dark energy modelsSeokcheon Lee0Changbom Park1Sang Gyu Biern2School of Physics, Korea Institute for Advanced Study, Heogiro 85, Seoul 130-722, Republic of KoreaSchool of Physics, Korea Institute for Advanced Study, Heogiro 85, Seoul 130-722, Republic of KoreaDepartment of Physics and Astronomy, Seoul National University, Seoul 151-747, Republic of KoreaUnder the standard perturbation theory (SPT), we obtain the fully consistent third-order density fluctuation and kernels for the general dark energy models without using the Einstein–de Sitter (EdS) universe assumption for the first time. We also show that even though the temporal and spatial components of the SPT solutions cannot be separable, one can find the exact solutions to any order in general dark energy models. With these exact solutions, we obtain the less than % error correction of one-loop matter power spectrum compared to that obtained from the EdS assumption for k=0.1 hMpc−1 mode at z=0(1,1.5). Thus, the EdS assumption works very well at this scale. However, if one considers the correction for P13, the error is about 6 (9, 11)% for the same mode at z=0(1,1.5). One absorbs P13 into the linear power spectrum in the renormalized perturbation theory (RPT) and thus one should use the exact solution instead of the approximation one. The error on the resummed propagator N of RPT is about 14 (8, 6)% at z=0(1,1.5) for k=0.4 hMpc−1. For k=1 hMpc−1, the error correction of the total matter power spectrum is about 3.6 (4.6, 4.5)% at z=0(1,1.5). Upcoming observation is required to archive the sub-percent accuracy to provide the strong constraint on the dark energy and this consistent solution is prerequisite for the model comparison.http://www.sciencedirect.com/science/article/pii/S0370269314005565
collection DOAJ
language English
format Article
sources DOAJ
author Seokcheon Lee
Changbom Park
Sang Gyu Biern
spellingShingle Seokcheon Lee
Changbom Park
Sang Gyu Biern
Exact third-order density perturbation and one-loop power spectrum in general dark energy models
Physics Letters B
author_facet Seokcheon Lee
Changbom Park
Sang Gyu Biern
author_sort Seokcheon Lee
title Exact third-order density perturbation and one-loop power spectrum in general dark energy models
title_short Exact third-order density perturbation and one-loop power spectrum in general dark energy models
title_full Exact third-order density perturbation and one-loop power spectrum in general dark energy models
title_fullStr Exact third-order density perturbation and one-loop power spectrum in general dark energy models
title_full_unstemmed Exact third-order density perturbation and one-loop power spectrum in general dark energy models
title_sort exact third-order density perturbation and one-loop power spectrum in general dark energy models
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2014-09-01
description Under the standard perturbation theory (SPT), we obtain the fully consistent third-order density fluctuation and kernels for the general dark energy models without using the Einstein–de Sitter (EdS) universe assumption for the first time. We also show that even though the temporal and spatial components of the SPT solutions cannot be separable, one can find the exact solutions to any order in general dark energy models. With these exact solutions, we obtain the less than % error correction of one-loop matter power spectrum compared to that obtained from the EdS assumption for k=0.1 hMpc−1 mode at z=0(1,1.5). Thus, the EdS assumption works very well at this scale. However, if one considers the correction for P13, the error is about 6 (9, 11)% for the same mode at z=0(1,1.5). One absorbs P13 into the linear power spectrum in the renormalized perturbation theory (RPT) and thus one should use the exact solution instead of the approximation one. The error on the resummed propagator N of RPT is about 14 (8, 6)% at z=0(1,1.5) for k=0.4 hMpc−1. For k=1 hMpc−1, the error correction of the total matter power spectrum is about 3.6 (4.6, 4.5)% at z=0(1,1.5). Upcoming observation is required to archive the sub-percent accuracy to provide the strong constraint on the dark energy and this consistent solution is prerequisite for the model comparison.
url http://www.sciencedirect.com/science/article/pii/S0370269314005565
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AT changbompark exactthirdorderdensityperturbationandonelooppowerspectrumingeneraldarkenergymodels
AT sanggyubiern exactthirdorderdensityperturbationandonelooppowerspectrumingeneraldarkenergymodels
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