httpleandrosphysicsuoigr Department of Physics University of Ioannina Open page Collaborators I Antoniou Ioannina J Bueno Sanchez Madrid J Grande Barcelona S ID: 199688
Download Presentation The PPT/PDF document "L. Perivolaropoulos" is the property of its rightful owner. Permission is granted to download and print the materials on this web site for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.
Slide1
L. Perivolaropouloshttp://leandros.physics.uoi.grDepartment of PhysicsUniversity of Ioannina
Open page
Collaborators: I. Antoniou (Ioannina)J. Bueno-Sanchez (Madrid)J. Grande (Barcelona) S. Nesseris (Madrid)A. Mariano (Lecce)
Accelerating Expansion of the Universe from Topological
SolitonsSlide2
Main Points
The expansion of the Universe has entered an
accelerating phase during recent cosmological times. Repulsive gravity on large scales is needed to explain this accelerating expansion. This may be provided by the ΛCDM model.There are some puzzling conflicts between ΛCDM predictions and some cosmological observations(Galaxy Velocity Flows, Cosmic Microwave Background Temperature Asymmetry, Fine Structure Constant Dipole, Dark energy Dipole)Most of these puzzles are related to the existence of preferred anisotropy axes which appear to be surprisingly close to each other! The simplest mechanism that can give rise to a cosmological preferred axis is based on an off-center observerin a spherical energy inhomogeneity (dark matter or dark energy)
Topological Quintessence
is a simple physical mechanism that can give rise
to a Hubble scale dark energy
inhomogeneity
.Slide3
3FRW Metric
Universe Description
Homogeneous-Isotropic System+ PerturbationsGeneral RelativityTwo Parameters: Geometry ( Curvature k=-1,0,+1), Scale (Scale Factor a(t))
Closed
Flat
Open
Universe Expands
Flat: Favored by Observations and TheorySlide4
4
Dynamics: The Dark Energy Puzzle
General RelativityDirectlyObservableDirectlyObservableDark Energy(Inferred)Q: Is GR the correct theory on the Largest Scales?What is the Correct Theory?
What are the properties of the dark energy?
What microphysical theory can reproduce these properties?
No
Yes
Flat
Friedmann EquationSlide5
The scale factor
α(
t) and the redshift zHubble’s Law (z<<1):Photons from distant galaxies have a larger redshiftSlide6
Hubble’s Law
(1929): The Universe is ExpandingSlide7
The observed evolution of α(t)
a(t)
tAcceleratingUniverset0present
0
t
0
Decelerating
Universe
Decelerating expansion due to attractive gravity of matter
Accelerating expansion due to
???
Empty Universe
Discovery
1998 (
SCP,
HzSST
)
Nobel: 2011 (
Perlmutter
, Schmidt,
Riess
)Slide8
Why is the Universe Accelerating?Slide9
Einstein (1915) General Relativity: Gμν
= κ T
μν Cosmological Constant + Matter :Gmn - L gmn = k TmnCosmological ConstantCosmological Constant: The simplest model
Cosmic Repulsion
(
p
Λ
=-
ρ
Λ
c
2
)
Acceleration of scale factorSlide10
10
Equation of State:
Quintessence: Homogeneous Scalar FieldHomogeneous Scalar Field Dynamics:Repulsive gravity and accelerating expansion from the negative pressure of a homogenous scalar fieldPotential resolution of Coincidence Problem (why cosmological constant is so small to lead to acceleration only recently?)Slide11
11
Direct Probes of the Cosmic Metric:Geometric Observational Probes
Luminosity Distance (standard candles: SnIa,GRB):Angular Diameter Distance (standard rulers: CMB sound horizon, clusters):
SnIa
Obs
GRB
flat
Direct Probes of H(z):Slide12
Geometric Constraints
Parametrize H(z):
Minimize:Slide13
Consistency of
ΛCDM with Data
Good Agreement with Geometric Probes!SNLSESSENCE
GOLD06
UNION
CONSTITUTION
WMAP5+SDSS5
WMAP7+SDSS7
UNION2
J. C.
Bueno
Sanchez, S.
Nesseris
, LP,
JCAP 0911:029,2009,
0908.2636 Slide14
Puzzling Data
Puzzles for
ΛCDM are related to the existence of a preferred axisA. Kashlinsky et. al. Astrophys.J.686:L49-L52,2009 arXiv:0809.3734Quadrupole component of CMB mapOctopole component of CMB mapDipole component of CMB map
M.
Tegmark
et
. al
.,
PRD 68, 123523 (2003),
Copi
et. al.
Adv.Astron.2010:847541,2010
.
Dark Velocity Flow
Λ
CDM prediction
WMAP Cosmic Microwave Background mapSlide15
Puzzles for
ΛCDM
Large Scale Velocity Flows - Predicted: On scale larger than 50 h-1Mpc Dipole Flows of 110km/sec or less. - Observed: Dipole Flows of more than 400km/sec on scales 50 h-1Mpc or larger. - Probability of Consistency: 1%Anisotropy of Cosmic Accelerating Expansion - Predicted: Isotropic Rate of Accelerating Expansion - Observed: SnIa data show hints for an anisotropic acceleration fit by a Dipole - Probability of Consistency: 5%From LP, 0811.4684,I. Antoniou, LP, JCAP 1012:012, 2010, arxiv:1007.4347R. Watkins et. al. , Mon.Not.Roy.Astron.Soc.392:743-756,2009, 0809.4041. A. Kashlinsky et. al. Astrophys.J.686:L49-L52,2009 arXiv:0809.3734A. Mariano, LP, ,
Phys.Rev
. D86 (2012) 083517
,
Alignment of Low CMB Spectrum
Multipoles
-
Predicted:
Multipole
components of CMB map should be uncorrelated.
-
Observed:
l=2 and l=3 CMB map components are unlikely planar and close to each other.
-
Probability of Consistency:
1%
Cosmic Spatial Dependence of the Fine Structure Constant
-
Predicted:
The value of the Fine Structure Constant is Space-Time Independent.
-
Observed
:
There is a cosmic spatial dependence well fit by a Dipole with δα/α~10-5
- Probability of Consistency: 0.0
1%
Webb et. al.. , Phys. Rev. Lett. 107, 191101 (2011)
M. Tegmark et. al.,
PRD 68, 123523 (2003), Copi et. al. Adv.Astron.2010:847541,2010. Slide16
Cosmic Anisotropy Axes
Dark Flow Direction
(3σ)Watkins et. al. arxiv: 0809.4041, Kashlinsky et. al. arxiv: 0809.3734WMAP7 CMB Map – Maximum Temperature Asymmetry (1.5 σ) (A. Mariano, LP, arXiv:1211.5915 Phys. Rev. D. 87, 043511 (2013))α Dipole (4σ)Webb et. al. , Phys. Rev. Lett. 107, 191101 (2011)Q1: How anomalous is this coincidence?
Q2: Is there a physical model that can predict this coincidence
Dark Energy Dipole (2
σ)
A. Mariano, LP, ,
Phys.Rev
. D86 (2012) 083517
.
Slide17
Basic Issues
A1: The probability that the combined quasar absorber and
SnIa data are obtained in the context of a homogeneous and isotropic cosmology is less than one part in 106.A2: There is a simple physical model based on a Hubble scale topological defect non-minimally coupled to electromagnetism that has the potential to explain the observed aligned dipoles.Q1: What is the probability to produce the observed combination of just the two dipoles in a homogeneous-isotropic cosmological model?Q2: What physical model has the potential to predict the existence of the above combined dipoles?Slide18
Models Predicting a Preferred Axis
Anisotropic dark energy equation of state (
eg vector fields) (T. Koivisto and D. Mota (2006), R. Battye and A. Moss (2009))Fundamentaly Modified Cosmic Topology or Geometry (rotating universe, horizon scale compact dimension, non-commutative geometry etc) (J. P. Luminet (2008), P. Bielewicz and A. Riazuelo (2008), E. Akofor, A. P. Balachandran, S. G. Jo, A. Joseph,B. A. Qureshi (2008), T. S. Koivisto, D. F. Mota, M. Quartin and T. G. Zlosnik (2010)) Statistically Anisotropic Primordial Perturbations (eg vector field inflation) (A. R. Pullen and M. Kamionkowski (2007), L. Ackerman, S. M. Carroll and M. B. Wise (2007), K. Dimopoulos, M. Karciauskas, D. H. Lyth and Y. Ro-driguez (2009)) Horizon Scale Primordial Magnetic Field. (T. Kahniashvili, G. Lavrelashvili and B. Ratra (2008), L. Campanelli (2009), J. Kim and P. Naselsky (2009)) Horizon Scale Dark Matter or Dark Energy Perturbations (eg few Gpc void) (J. Garcia-Bellido and T. Haugboelle (2008), P.
Dunsby
, N.
Goheer
, B.
Osano
and J. P.
Uzan
(2010), T.
Biswas
, A.
Notari
and W.
Valkenburg
(2010))Slide19
Coincidence Problem: Why Now? Time Dependent Dark EnergyAlternatively:
Why Here? Inhomogeneous Dark Energy
Inhomogeneous Dark Energy: Why Consider?Standard Model (ΛCDM):1. Homogeneous - Isotropic Dark and Baryonic Matter.2. Homogeneous-Isotropic-Constant Dark Energy (Cosmological Constant)3. General RelativityConsider Because:1. New generic generalization of ΛCDM (breaks homogeneity of dark energy). Includes ΛCDM as special case.Natural emergence of preferred axis (off – center observers)Well defined physical mechanism (topological quintessence with Hubble scale global monopoles).J. Grande, L.P., Phys. Rev. D 84, 023514 (2011).J. B. Sanchez, LP, Phys.Rev. D84 (2011) 123516 Slide20
Topological Quintessence
Global Monopole with Hubble scale Core
General Metric with Spherical Symmetry:Energy – Momentum Tensor:Slide21
Global Monopole Configuration
Global Monopole: Field Direction in Space and Energy Density
Off-center ObserverVariation of expansion rate due to dark energy density variationVariation of α?Slide22
Extended Topological Quintessence
Global Monopole Configuration:
Non-minimally coupled scalar fieldFine Structure Constant:Fine Structure Constant Spatial Variation: Slide23
Global Monopole Configuration
Global Monopole: Field Direction in Space and Energy Density
Off-center ObserverVariation of α due to field variationVariation of expansion rate due to dark energy density variationSlide24
Model Parameters
Monopole Core Scale:
Potential Energy Density at the Core:Approximate Cosmic Evolution at the Core:Approximate Cosmic Evolution away from the Core:Physical Requirements:
Cosmological Scale Core
Core Density similar as present matter density
J. B. Sanchez, LP, ,
Phys.Rev
. D84 (2011) 123516Slide25
Full Dynamical Equations
Initial-Boundary Conditions
Energy-Momentum ConservationStatic Monopole Profile (Φ=f(r) )Homogeneous, Flat Matter Dominated (A=B=1)Slide26
Main Questions
Does the Monopole Energy Density Eventually Dominate over matter in the Monopole Core?
Does the possible domination lead to accelerating expansion in the monopole core?Can this cosmological expansion in the core fit the cosmological data?Slide27
Energy Densities
Monopole energy density slowly shrinks and dominates at late times in the core.
Matter develops underdensity at the core.Slide28
Scale Factors
η=0.1
Mpl η=0.6 Mpl η=0.1 Mpl η=0.6 Mpl Accelerating Expansion at the core.r=0r=0.5
r=5Slide29
Summary
Early hints for
deviation from the cosmological principle and statistical isotropy are being accumulated. This appears to be one of the most likely directions which may lead to new fundamental physics in the coming years.The simplest mechanism that can give rise to a cosmological preferred axis is based on an off-center observerin a spherical energy inhomogeneity (dark matter of dark energy)Such a mechanism can also give rise to large scale velocity flows and Fine Structure Constant Dipole. Other interesting effects may occur (quasar polarization alignment etc).Topological Quintessence constitutes a physical mechanism to produce Hubble scale dark energy inhomogeneities. Slide30
Simplest Model:
Lematre-Tolman-Bondi
Faster expansion rate at low redshifts (local space equivalent to recent times)Local spherical underdensity of matter (Void), no dark energy
Central Observer
Apparent AccelerationSlide31
Shifted Observer: Preferred Direction
Faster expansion rate at low
redshifts (local space equivalent to recent times)Local spherical underdensity of matter (Void)
Observer
Preferred DirectionSlide32
Luminosity Distance
Metric:
Cosmological Equation:Geodesics:Luminosity Distance:
FRW limit:
MSlide33
Constraints: Union2 Data – Central Observer
Advantages:
1. No need for dark energy.2. Natural Preferred Axis.3. Coincidence ProblemJ. Grande, L.P., Phys. Rev. D 84, 023514 (2011).Problems:1. No simple mechanism to create such large voids.2. Off-Center Observer produces too large CMB Dipole.3. Worse Fit than LCDM.4. Ruled out by kSZ – CMB (Zhang and Stebbins, Phys.Rev.Lett. 107 (2011) 041301 )