Michael Doran Institute for Theoretical Physics Universität Heidelberg Time Evolution of Dark...
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Transcript of Michael Doran Institute for Theoretical Physics Universität Heidelberg Time Evolution of Dark...
Michael Doran
Institute for Theoretical Physics
Universität Heidelberg
Time Evolution of Dark Energy(if any …)
Dark energy (a.k.a. quintessence)
(Semi-) Known Dark Energy Properties
• D.E. does not cluster on scales within horizon, because canonical:
• D.E. not coupled or very weakly coupled to matter
• Cosmological constant fits all observations
• Descriptions in terms of modified Einstein action and scalar fields possible and related
Extracting information on
Effects of dark energy I -- Geometry
• Additional component changes expansion history and horizons.
• Geometrical tests include:– Acoustic scale of the CMB – Baryon acoustic oscillations at low redshifts – Luminosity distance at low redshift from SNe Ia– Luminosity distance up to from -ray bursts (?) – Angular diameter distance using shape of
Effects of dark energy II -- Couplings
• If D.E. coupled to baryons: – mediates additional fifth force (hence very restricted)– might be linked to running coupling constants
• If D.E. coupled to cold dark matter: acts like self-interaction for dark matter, i.e. enhances clustering. Caution exchange.
Effects of dark energy III -- Structure growth & CMB
Not coupled: Suppresses growth of linear matter perturbations because additional non-clustering component is present.
Consequences?
Consequences!
• Gravitational potential decays during matter domination if D.E. present ISW effect in CMB
• The longer a mode is inside the horizon, the more it gets suppressed if D.E. present. However, all modes inside horizon at matter-radiation equality are equally suppressed. Up to running spectral index – then equal suppression.
• Rough rule of thumb: 10% dark energy during structure formation 50% less
Linear Power Spectrum
CDM
Early Dark Energy
Counterintuitive: More structure at higher redshifts
• Conditions for collapse roughly the same as in -CDM
• Yet, even after collapse of some halo starts, linear theory fluctuations grow less compared to -CDM
• So linear overdensity corresponding to collapsed object is lower than in -CDM
• Same non-linear structure with lower
.. more non-linear structure at higher redshiftM
ass
Fu
nct
ion
rel
. toL
CD
M
1
10
1013 1014 1015
Halo Mass [h-1 Msun]
z=1
z=0
Early Dark Energy influences the CMB ...
R.R. Caldwell et. al. (2003)
Dark Energy influences structure growth...
• Linear fluctuations grow less with dark energy.• CMB normalized, early dark energy predicts
more non-linear structure at higher redshifts compared to standard cosmological constant. M. Bartelmann, M.D., C. Wetterich (2005)
Mas
s F
unct
ion
rel.
to L
CD
M
Halo mass
.. more non-linear structure at higher redshiftM
ass
Fu
nct
ion
rel
. toL
CD
M
1
10
1013 1014 1015
Halo Mass [h-1 Msun]
z=1
z=0