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Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17
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Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Dec 28, 2015

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Page 1: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Cosmological post-Newtonian Approximation compared with

Perturbation Theory

J. HwangKNU/KIAS2012.02.17

Page 2: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Question

Compared with Einstein’s gravity, is Newton's gravity reliable in near horizon scale simulation?

Linear deviation from homogeneous-isotropic background

Action at a distance

Page 3: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Newton’s theory: Non-relativistic (no c)

Action at a distance, violate causality c=∞ limit of Einstein’s gravity: 0th post-

Newtonian limit No horizon Static nature

No strong pressure No strong gravity No gravitational waves Incomplete and inconsistent

Einstein’s gravity: Relativistic Strong gravity, dynamic Simplest

Page 4: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Perturbation method: Perturbation expansion All perturbation variables are small Weakly nonlinear Strong gravity; fully relativistic Valid in all scales

Post-Newtonian method: Abandon geometric spirit of GR: recover the

good old absolute space and absolute time Provide GR correction terms in the Newtonian

equations of motion Expansion in strength of gravity

Fully nonlinear No strong gravity situation; weakly relativistic Valid far inside horizon

Page 5: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

FullyRelativistic

FullyNonlinear

WeaklyRelativistic

WeaklyNonlinear

?

Studies of Large-scale Structure

NewtonianGravity axis

Linear Perturbation

Background World Model axis

Page 6: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

FullyRelativistic

FullyNonlinear

WeaklyRelativistic

Post-Newtonian (PN)Approximation

Pert

urb

ati

on

Th

eory

(P

T)

“Terra Incognita”Numerical Relativity

PT vs. PN

WeaklyNonlinear

NewtonianGravity axis

Background World Model axis

Page 7: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

FullyRelativistic

FullyNonlinear

WeaklyRelativistic

“Terra Incognita”Numerical Relativity

Cosmological 1st order Post-Newtonian (1PN)

Cosmological Nonlinear Perturbation (2nd and 3rd order)

Linear Perturbation vs. 1PN

WeaklyNonlinear

NewtonianGravity axis

Linear Perturbation

Background World Model axis

Page 8: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Newtonian Theory

Page 9: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Mass conservation:

Momentum conservation:

Poisson’s equation:

Newtonian perturbation equations:

Newtonian (0PN) metric:

Page 10: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

By combining:

To linear order:

Page 11: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Perturbation Theory

Page 12: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Metric convention: (Bardeen 1988)

Spatial gauge:

Bardeen, J.M. in “Particle Physics and Cosmology” edited by Fang, L., & Zee, A. (Gordon and Breach, London, 1988) p1

Page 13: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

To linear order:

Perturbed Lapse, Acceleration Curvature perturbation

Perturbed expansion Shear

Page 14: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Gauge-invariant combinations:

: A gauge-invariant density perturbation based on the comoving gauge

Page 15: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Relativistic/Newtonian correspondences:

Comoving gauge Zero-shear gauge

Uniform-expansion-gauge Uniform-curvature gauge

Perturbed density, Perturbed velocity

Perturbed gravitational potential Perturbed curvature

JH, Noh, Gong (2012)

Page 16: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Relativistic/Newtonian correspondence includes Λ, but assumes:

1. Flat Friedmann background2. Zero-pressure3. Irrotational4. Single component fluid5. No gravitational waves6. Second order in perturbations

Relaxing any of these assumptions could lead to pure general relativistic effects!

Page 17: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Linear order: Lifshitz (1946)/Bonnor(1957)

Second order: Peebles (1980)/Noh-JH (2004)

Third order: JH-Noh (2005)

Physical Review D 69 10411 (2004); 72 044012 (2005)Pure General Relativistic corrections

(comoving-synchronous gauge)

Curvature perturbation in the comoving gauge

~10-5

(K=0, comoving gauge)

Page 18: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Jeong, Gong, Noh, JH, ApJ 722, 1(2011)

The unreasonable effectiveness of Newtonian gravity in cosmology!

Vishniac MN 1983

Jeong et al 2011

Pure Einstein

Page 19: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Post-Newtonian Approximation

Page 20: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Minkowski background

Robertson-Walker background

Newtonian gravitational potential

JH, Noh, Puetzfeld, JCAP 03 010 (2008)

Page 21: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Zero-pressure 1PN equations:

Nonlinear

E-conservation:

Mom-conservation:

Raychaudhury-eq:G0

0-Gii

Mom-constraint:G0

i

Page 22: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

1PN compared with Newtonian:

0PN:

1PN: 1PN

v=u

Page 23: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

PN vs. PT

Page 24: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Comparison (flat background):

1PN:

Linear PT:

Page 25: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Comparison: PT PN

PN: gauge-invariantPT: depends on the gauge condition

Page 26: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Comoving gauge:

Page 27: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Zero-shear gauge:

Page 28: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Uniform-expansion gauge:

Page 29: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Noh, JH, Bertschinger (2012)

Page 30: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

For growing solution: (Takada & Futamase, MN 1999)

Spurious mode

Physical density fluctuations

Page 31: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Newtonian interpretation:

Newtonian:

Einstein:

Correspondence with mixed gauges:

To second-order

Page 32: Cosmological post-Newtonian Approximation compared with Perturbation Theory J. Hwang KNU/KIAS 2012.02.17.

Question

Compared with Einstein’s gravity, is Newton's gravity reliable in near horizon scale simulation?