Jochen Weller Benasque August, 2006 Constraining Inverse Curvature Gravity with Supernovae O. Mena,...
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Transcript of Jochen Weller Benasque August, 2006 Constraining Inverse Curvature Gravity with Supernovae O. Mena,...
![Page 1: Jochen Weller Benasque August, 2006 Constraining Inverse Curvature Gravity with Supernovae O. Mena, J. Santiago and JW PRL, 96, 041103, 2006.](https://reader038.fdocuments.us/reader038/viewer/2022103101/56649e725503460f94b72051/html5/thumbnails/1.jpg)
Jochen Weller
BenasqueAugust, 2006
Constraining Inverse Constraining Inverse Curvature Gravity with Curvature Gravity with
SupernovaeSupernovae
O. Mena, J. Santiago and JW
PRL, 96, 041103, 2006
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Jochen Weller
Benasque,August 2006
New Gravitational New Gravitational ActionAction
Simple approach: F(R) = R+mRn
Einstein Gravity has not been tested on large scales (Hubble radius)
But in general:
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Jochen Weller
Benasque,August 2006
Well known for n>1 early de Sittere.g. Starobinsky (1980)
Interest here: Late time modification n<0 n<0 (inverse curvature)
modification becomes important at low curvatureand can lead to accelerated expansion[Capozziello, Carloni, Troisy (’03), Carroll, Duvvuri, Trodden, Turner (’03), Carroll, De Felice, Duvvuri, Easson, Trodden, Turner (’04)]
purely gravitational alternative to dark energy
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Jochen Weller
Benasque,August 2006
H
dH/dt1/R model1/R model
accelerated attractor: [CDDETT] vacuum solutions:
de Sitter (unstable) Future Singularity power law acceleration a(t) ~ t2
For = 10-33 eV corrections only important today Observational consequences similar to dark energy
with w = -2/3
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Jochen Weller
Benasque,August 2006
General f(R) actionsGeneral f(R) actions
e.g. 2(n+1)/Rn , with n>1 have late-timeacceleration
Can satisfy observational constraints form Supernovae
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Jochen Weller
Benasque,August 2006
General Brans-Dicke theories:
f(R) models in Einstein frame ( = 0):
Simplest model (1/Rn) ruled out by observations of distant Quasars and the deflection of their light by the sun with VLBI: >35000 [Chiva (‘03), Soussa, Woodard (‘03),...]
Non-Cosmological Non-Cosmological Constraints on f(R) Constraints on f(R)
TheoriesTheories
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Jochen Weller
Benasque,August 2006
The New ModelThe New Model
Unstable de Sitter solution Corrections negligible in the past (large curvature),but dominant for R 2; acceleration today for H0 (Again why now problem and small parameter)
Late time accelerated attractor [CDDTT’04]
[CDDTT’04]
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Jochen Weller
Benasque,August 2006
H
Example 1/RExample 1/RRR Model Model
Unstable de Sitter Point (H=const)
Two late time attractors:acceleration with p=3.22
deceleration with p=0.77
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Jochen Weller
Benasque,August 2006
Afraid of Ghosts ?Afraid of Ghosts ?
In the presence of ghosts: negative energy states, hence background unstable towards the generation of small scale inhomogeneities
If one chooses: c = -4b in action, there are NO GHOSTS: I. Navarro and K. van Acoleyen 2005
In general F(R,Q-4P) with Q=RR and P=R R
has no ghosts, however...
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Jochen Weller
Benasque,August 2006
We are still afraid of tachyons
Q=4P is necessary, but not sufficient condition for positive energy eigenstates (vanishing of 4th order terms is guarantied so)
Also have to check 2nd order derivatives for finite propagation speeds (De Felice et al. astro-ph/0604154)
some parameter combination are still allowed !
For higher inverse powers 1/(aR2+bP+cQ)n there is hope !
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Jochen Weller
Benasque,August 2006
Solar Systems TestsSolar Systems Tests
Linear expansion around Schwarzschild metric
Navarro et al. 2005
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Jochen Weller
Benasque,August 2006
Non-Cosmological TestsNon-Cosmological Tests
with critical radius
for solar system: 10pc !for galaxies: 102kpcfor clusters: 1Mpc !
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Jochen Weller
Benasque,August 2006
Modified Friedman Modified Friedman EquationEquation
Stiff, 2nd order non-linear differential equation, solution is hard numerical problem - initial conditions in radiation dominated era are close to singular point.
Source term is matter and radiation: NO DARK ENERGY
Effectively dependent on 3 extra parameters:
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Jochen Weller
Benasque,August 2006
Dynamical AnalysisDynamical Analysis
is fixed by the dynamical behavior of the system Four special values of
For 1: both values of are acceptable For 1 2: =+1 hits singularity in past For 2 4 : =-1 hits singularity in past For 2 3 : stable attractor that is decelerated
for <32/21 and accelerated for larger . For 3 4 : no longer stable attractor and
singularity is reached in the future through an accelerated phase. For small this appears in the past.
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Jochen Weller
Benasque,August 2006
Solving the Friedman Solving the Friedman Equation for n=1Equation for n=1
Numerical codes can not solve this from initial conditions in radiation dominated era or matter domination
Approximate analytic solution in distant past
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Jochen Weller
Benasque,August 2006
Perturbative Solution for =1
for = 1
good approximation in the past
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Jochen Weller
Benasque,August 2006
Solution and Conditions
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Jochen Weller
Benasque,August 2006
Specific Conditions
For example with =-4 ata=0.2:
In general all 3 conditions break down at a > 0.1-0.2
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Jochen Weller
Benasque,August 2006
Dynamics of best fit model
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Jochen Weller
Benasque,August 2006
Approximation and Approximation and Numerical SolutionNumerical Solution
Very accurate for z ≥ few (7), better than 0.1% with HE
2=8G/the standard Einstein gravity solution at early times.
Use approximate solution as initial condition at z=few (7) for numerical solution (approximation very accurate and numerical codes can cope)
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Jochen Weller
Benasque,August 2006
Include intrinsic magnitude of Supernovae as free parameter:Degenerate with value of H0 or better absolute scale of H(z).Measure all dimensionful quantities in units of
Remaining parameters: and
1 leads to very bad fits of the SNe data; remaining regions
Fit to Supernovae DataFit to Supernovae Data
low
high
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Jochen Weller
Benasque,August 2006
Fit to Riess et al (2004) gold sample; a compilation of 157 high confidence Type Ia SNe data.
very good fits, similar to CDM (2 = 183.3)
Universe hitssingularity in thepast
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Jochen Weller
Benasque,August 2006
low high
Combining DatasetsCombining Datasets
In order to set scale use prior from Hubble Key Project: H0 = 728 km/sec/Mpc [Freedman et al. ‘01]
Prior on age of the Universe: t0 > 11.2 Gyrs[Krauss, Chaboyer ‘03]
marginalized 0.07 < marginalized 0.07 < mm < < 0.21 (95% c.l.); require dark matter0.21 (95% c.l.); require dark matter
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Jochen Weller
Benasque,August 2006
CMB for the BraveCMB for the Brave
Small scale CMB anisotropies are mainly affected bythe physical cold dark matter and baryon densities andthe angular diameter distance to last scattering
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Jochen Weller
Benasque,August 2006
Angular Diameter Angular Diameter Distance to Last Distance to Last
ScatteringScattering
For the brave:Angular diameter distance to lastlast scattering with WMAP data - might as well be bogus ! Need full perturbationanalysis
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Jochen Weller
Benasque,August 2006
Inverse curvature gravity models can lead to accelerated expansion of the Universe and explain SNe data without violation of solar system tests. No No need for dark energy !need for dark energy !
Use of other data sets like CMB, LSS, Baryon Oscillations and clusters require careful analysis of perturbation regime and post - Newtonian limit on cluster scales (in progress)
So far No alternative for dark matter !No alternative for dark matter ! But only studied one functional form (n=1) ! Some ideas by Navarro et al. with logarithmic functions ?
ConclusionsConclusions
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Jochen Weller
Benasque,August 2006
The Model vs Dark The Model vs Dark EnergyEnergy
Require also small parameter: Larger n for truly physical models
Ghost free version has only scalar degree of freedom: is there a simple scalar-tensor theory ?
Is there any motivation for this model ?
“If at first an idea is not absurd, there is no hope for it”
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Jochen Weller
Benasque,August 2006
And finally ...thanks to the organizers for providingsuch beautiful views ...
On Pico de Tempestades