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Infrared divergence of pure Einstein gravity contributions to cosmological density power spectrum
J. Hwang, H. Noh, D. Jeong
1Phys. Rev. Lett. 103, 121301, arXiv:0902.4285
Linear order: Lifshitz (1946)/Bonnor(1957)
Second order: Peebles (1980)/Noh-Hwang(2004)
Third order: Hwang-Noh (2005)
Physical Review D, 72, 044012 (2005). Pure General Relativistic corrections
(comoving-synchronous gauge)
2
Curvature perturbation in the comoving gauge
~10-5
(K=0, comoving gauge)
General relativistic contributions to second-order power spectrum:
132211
312
22
12
321
)Re(2||||||
PPP
P
Pure General Relativistic contribution!
EinsteinNewton
EinsteinNewton
PPP ,13,1313
,3,33
Relativistic/Newtonian4
Density power spectrum to second-order:
Physical Review D, 77,123533 (2008)
Pure General Relativistic corrections P13,Einstein
Newtonian
P22 +
P13,Newton
K=0 =Λ:
5
Dashed line: negative
P13,Einstein
P22
P11
P13,Newton
PTotal
P22 + P
13,Newton
9Phys. Rev. Lett. 103, 121301, arXiv:0902.4285
P13,Einstein
Large-scale limit (k→0, r→∞):
P13,Newton
Leading orderNewton
Next-to-leading orderNewton
10
In the large scale we discover an infrared divergence in the next-to-leading-order power spectrum due to pure Einstein gravity contribution appearing in the third-order perturbation.
Despite cancellations of the leading-order and next-to-leading order terms in P
13,Newton, no such cancellations occur in
P13,Einstein
.
11
P13,Einstein
Small-scale limit (k→∞, r→0):
P13,Newton
Leading order, Einstein
Next-to-leading order, Einstein
Leading order, Newton
13
P22
In the small-scale the Einstein's gravity contribution is still negligibly small.
Due to cancellation of the leading-order and next-to-leading order terms in P
13,Einstein, despite a cancellation between P
22 in
P13,Newton
.
14