The Accelerating Universe
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L. Perivolaropoulos
http://leandros.physics.uoi.gr
Department of Physics
University of Ioannina
Geometrical
(Standard Candles, Standard Rulers)
Cosmological Tests of
the Cosmological Constant Λ
Dynamical
(Growth of Fluctuations by Gravity)
The Cosmological Constant (w=-1) remains
consistent with all current data as a driving force of the acceleration.
Q: What could be the origin of Λ?
Α: Vacuum Fluctuations with Cutoff (ωc=10-3eV, lc=0.1mm)
Q: What Experiment could probe the cutoff structure of the vacuum in the lab?
A: Casimir Effect (detected attraction of metal plates)
Cutoff Prediction:
Extra Dimension:
Change of sign of Casimir Force ( d lr lc )
Change of sign at higher separations
lr lc
Predicted Hubble Expansion History (flat universe):
H ( z)
2
CDM
a2
3
2 H02 0m 1 z
a
0 m 1
Luminosity Distance (standard candles - SnIa):
Obs
SnIa
L
l
4 d L2
dz
d L ( z )th c 1 z
0 H z ; m
z
dL z
SnIa : z (0,1.7]
Angular Diameter Distance (standard rulers – CMB sound horizon):
dA z
rs
dA z
rs
c z
dz
d A ( z )th
1
z
0 H z ; m
BAO : z 0.35
CMB Spectrum : z 1089
CDM w0 , w1 1,0
Generalize H(z):
w z w0 w1
z
1 z
5log10 d L, A ( zi )obs 5log d L, A ( zi ; w0 , w1 )th
min
2 m , w0 , w1
2
2
Minimize:
N
i 1
ESSENCE+SNLS+HST data
i
WMAP3+SDSS(2007) data
Standard Candles
(SnIa)
0 m 0.24
2σ tension between
standard candles and
standard rulers
Lazkoz, Nesseris, LP
arxiv: 0712.1232
Standard Rulers
(CMB+BAO)
Measure growth function of cosmological perturbations:
Predicted Evolution of δ :
(General Relativity)
Parametrization:
f m a
Wang, Steinhardt, Astrophys.J.508:483-490,1998
CDM : de const
6
11
f m a
Parametrization:
CDM : de const
6
11
Parametrization:
CDM : de const
6
11
Fit to LSS data:
0 m 0.3
ΛCDM
ΛCDM provides an excellent fit
to the linear perturbations
growth data
best fit
S. Nesseris, LP, arxiv: 0710.1092,
Phys.Rev.D77:023504,2008
Equivalence Principle
EM field zero point vacuum energy:
V
Gravity couples to the
zero point energy of the
vacuum
pmax
?
V const
Q: Can we probe the zero point energy of the vacuum in the lab?
A: No! Non-gravitational experiments are only sensitive to changes
of the zero point energy.
But: This is not so in the presence of a physical finite cutoff !
Majajan, Sarkar, Padmanbhan,
Phys.Lett.B641:6-10,2006
Casimir Force Experiments can pick up the presence of a physical cutoff !!
Vacuum Energy gets modified in the presence
of the plates (boundary conditions)
d
2
FCas
ECas
2
hc
240d 4
2
hc
720d 3
Attractive Force
d
Agreement between
theory and experiment
at 1%
Harris, Chen, Mohideen,
2000
d (nm)
EM vacuum energy with cutoff
UV regulator
L d
d2
L
d
Modification of vacuum energy
due to the plates:
β=1
repulsive
L
attractive
d
β=0 (R=0)
LP, arxiv: 0802.1531, accepted in
Phys.Rev.D (to appear)
β=0 (R=0)
β=1
Thus, the cutoff predicts a Casimir
force which becomes repulsive for
d<0.6mm (not consistent with
experiments)
L
Casimir Force decreases
in the presence of an extra dimension
d
Poppenhaeger et. al.
hep-th/0309066 Phys.Lett.B582:1-5,2004
A change of sign of the Casimir force at low surface separations could
be an indication of a fundamental cutoff in the vacuum energy modes.
Such a cutoff could be an indication of both new physics and the origin of
the Cosmological Constant.
β=0 (R=0)
β=1
Standard Rulers are systematically less in favor of ΛCDM
than Standard Candles.
L
d
Geometrical
(Standard Candles, Standard Rulers)
Cosmological Tests of
the Cosmological Constant Λ
Dynamical
(Growth of Fluctuations by Gravity)
The Cosmological Constant (w=-1) remains
consistent with all current data as a driving force of the acceleration.
Q: What could be the origin of Λ?
Α: Vacuum Fluctuations with Cutoff (ωc=10-3eV, lc=0.1mm)
Q: What Experiment could probe the cutoff structure of the vacuum in the lab?
A: Casimir Effect (detected attraction of metal plates)
Cutoff Prediction:
Extra Dimension:
d l l ) : Not Detected
Change of sign of Casimir Force (d<l
c
r
Change of sign at higher separations
c
lr lc
Unless New Physics is imposed, current Casimir force experiments are not consistent
with the presence of the cutoff required to produce the observed value of Λ.