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Transcript of 1 General Relativistic Alternatives for Dark Matter and Dark Energy Grant J. Mathews Center for...
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General Relativistic Alternatives for Dark Matter and Dark Energy
Grant J. Mathews Center for Astrophysics (CANDU)Department of PhysicsUniversity of Notre Dame
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Premise of this talk:Dark energy and dark matter contribute comparable amounts of mass energy
This begs the question:
Could they be different aspects of the same physical phenomenon?
Appearing Dark Matter
Viscous/Decaying Dark Matter
Relativistic Corrections to Friedmann Cosmology
3
Bulk Dimension
m0
Z
• The flow of matter back into the 3-brane will appear as spontaneous matter creation
• Fixed point solution => a constant energy density as the universe expands
Dark Energy may be caused by the inflow of dark matter from the bulk to our 3-space in 5 dimensional gravity
m0
m0
Umezu, Ichiki, Kajino, Mathews, Yahiro PRD, 73 063527 (2006)
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Transfer from/to the Bulk leads to Modified Cosmic Expansion
• E = “Dark Radiation” or Electric part of the bulk Weyl tensor
€
ρ=ρM + ρ R + ρDM
€
H 2 =8πGN
3ρ −
ka2 +
Λ4
3+
κ 54
36ρ 2 + E
€
€
dEdt
+ 4HE =κ 5
4τ9
T05 =
κ 54τ9
Γρ DM
€
˙ ρ ρ
+ 3(1 + w) = −2T 05
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Growing Dark Matter CosmologyUmezu, et al. (2006)T0
5 = (ρDM + p) U5 ; U5 = -l H
Supernovae areFit with =0
Supernovae
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Growing Dark Matter CosmologyUmezu, et al. (2006)T0
5 = (ρDM + p) U5 ; U5 = -l H
Explains the diminished power for the lowest multipoles in the CMBfluctuations
CMB Power Spectrum
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Growing Dark Matter CosmologyUmezu, et al. (2006)T0
5 = (ρDM + p) U5 ; U5 = -l H
Matter Power Spectrum
Less power on the scales near the horizon
Bulk Viscosity and Decaying Dark MatterG. J. Mathews, N. Q. Lan, C. Kolda - Univ. Notre Dame
J. R. Wilson, LLNLG. M. Fuller, UC San Diego
PRD in press/ astro-ph/0609687
1. Decaying dark matter leads to dissipative bulk viscosity in the cosmic fluid
2. This viscosity may account for some or all of the apparent cosmic acceleration
Need a Physical Model for Bulk Viscosity
If a gas is out of pressure equilibrium as it expands or contracts a bulk viscosity is generated
Particle decay :Pressureless DM relativistic particles P = ρ/3
Out of temperature and pressure equilibrium=> Dissipation & Bulk Viscosity
During decay: matter and relativistic particles are out of pressure and
temperature equilibrium = 3 ρ
heq[(1/3) - (∂P/ ρ]
eq = 0 P()/P(0)dt = /(1 + 3 H)
Need (∂P/ ρ) ~ P/ ρ 1/3
P = (ρl + ρ)/3
ρ = ρDM + ρb + ρh + ρ + ρl
Weinberg (1971)
Candidates for Decaying Dark Matter
Late Cascading decays: Sterile neutrinos S e
1 2 3 4 5 6 regular neutrinos
Late decays due to time varying mass or a late phase transition:
sneutrino ge
Gauge mediated supersymmetry breaking
R + R
~~
~
~ ~ ~ ~ ~ ~
16
Dark Energy Could be Correction for Non-Friedmannian Clumpy Cosmology
Kolb et al. PRD, 71, 023524 2006, astro-ph/0506534
In a clumpy universe the motion there are acceleration terms
€
H 2 =8πG
3ρeff
€
ρeff = ρD
−QD
16πG−
RD
16πG
€
QD =23
Θ2
D− Θ D
2− 2σ 2
( )
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Schools of Thought:
This cannot produce Acceleration: (e.g.. Siegel & Fry 2005; Ishibashi & Wald 2006)
Needs to be tested without recourse to perturbative schemes or special symmetry
This can produce acceleration: Kolb 2005; 2006
This fits the luminosity-distance relation in special symmetric (e.g. Lemaitre-Tolman-Bondi ) models :Barausse et al. 2005; Celerier 2000; Menim et al. 2005a;b; Alnes, Amarzguioui, and Gron 2005; Enqvist & Mattsson 2006; Garfinkle 2006; Moffit 2006; Szydowski & Godowski 2006)
Large Scale StructureZhao, Mathews, Haywood (2006)
Nρ
Universe characterized by local regions with deepening potentials and large voids with diminishing gravity
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Conclusions
The challenge of accounting for dark matter and dark energy makes for an exciting time in relativity physics and cosmology
Could Galaxy Rotation Curves be accounted for by relativistic
corrections instead of dark matter?Cooperstock & Tieu astro-ph/0507619, 0512048
Menzies & Mathews gr-qc/0604092
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Problem with this picture• Implies DM is moved to outside galaxies,
but is still there: Mgal =
Menzies & Mathews (2006)
How to fix this?
Late decays:
Cascading decays: Sterile neutrinos1 2 3 4 5 6 regular neutrinos
Late decays due to time varying mass or a late phase transition