anisotropic perturbations due to dark energy jodrell bank observatory university of manchester...
TRANSCRIPT
ANISOTROPIC PERTURBATIONS
DUE TO DARK ENERGY
JODRELL BANK OBSERVATORYUNIVERSITY OF MANCHESTER
RICHARD BATTYE & ADAM MOSS astro-ph/0602377
DOMAIN WALL DOMINATED UNIVERSE
ADAM MOSS TALK : SHOWED THERE EXIST LOCALLY STABLE CONFIGURATIONS
BUT THEY DON'T APPEAR TO BE ATTRACTORS IN THE SIMPLEMODELS WE CONSIDERED – WORK CONTINUES
w = -2/3
DIMENSIONS :
PLAN OF TALK● MOTIVATION
● COSMOLOGICAL PERTURBATIONS
● ELASTIC DARK ENERGY
● ANISOTROPIC PERTURBATIONS
● CORRELATED MODES ON LARGE SCALES
THE STANDARD LORESCALAR-VECTOR-TENSOR SPLIT
BASIC IDEAISOTROPIC AND ANISOTROPIC ELASTICITYSPEED SOUND FOR CUBIC SYMMETRY
ANISOTROPY FROM ADIABATIC INITIAL CONDITIONSANALYTIC & NUMERICAL CALCULATIONS
(THE MODEL FORMERLY KNOWNAS SOLID DARK MATTER/ENERGY)
ALIGNMENT IN CMB MAPS
D'Oliveria-Costa et al
Eriksen et al
Land & Magueijo
Alignment of thel=2 and l=3 multipoles
North-South ratio ofPpower spectrum & 3-pt correlation fn
“Axis of Evil” -correlated multipoles
BIANCHI TYPE VIIh UNIVERSE (T. Jaffe et al)
WMAP
BIANCHI MODEL
WMAP-BIANCHI
now compatible with Gaussianity and isotropy
BASIC IDEA
ADD STANDARD ADIABATICMODEL AND BEST FITTING
BIANCHI TEMPLATE
SCALAR-VECTOR-TENSOR SPLIT
ENERGY-MOMENTUM TENSOR
VELOCITY :
ANISOTROPICSTRESS :
SCALARVECTOR
SCALAR
VECTORTENSOR
LAGRANGIAN, EM TENSOR
ACTION :
EM-TENSOR :
RELATIVISTIC ELASTICITY TENSOR :
HENCE PARAMETERIZES FLUID PERTS
STANDARDDEFINITIONS
THEORY DEVELOPED BY CARTER AND OTHERS IN 1970s TO MODEL NEUTRON STARS
STANDARD ASSUMPTION
STANDARD ELASTICITY TENSOR
WHERE
STANDARD : 21 COMPONENTS
LAGRANGIAN & EULERIANPERTURBATIONS
EULERIAN LAGRANGIAN
1 BULK MODULUS 20 SHEAR MODULI
3+1 SPLIT}
ISOTROPY
ISOTROPIC TENSORS
P = PRESSURE
= BULK MODULUS
= SHEAR MODULUS
SOUND SPEEDS
LONGITUDINAL(SCALAR)
TRANSVERSE(VECTOR)
DOMAIN WALLS
w = -2/3
STABILITY
NB w=0, IS CDM
(BUCHER & SPERGEL 1998,BATTYE, BUCHER & SPERGEL 1999)
ADIABATIC
POINT SYMMETRIES
NON-ZERO MODULI
TRICLINIC 18MONOCLINIC 12ORTHORHOMIBIC 9TETRAGONAL 6RHOMBOHEDRAL 6HEXAGONAL 5CUBIC 3ISOTROPIC 2
eg FROM LANDAU & LIFSCHITZ
EG CUBIC CASE
PRESSURE ISOTROPIC :
POSSIBLE SYMMETRIES ARE CLASSIFIED BY
THE BRAVAIS LATTICES
ELASTICITY TENSOR :
WHERE 1 = xx, 2 = yy, 3 = zz4 = xy, 5 =yz, 6 = zx
BULK MODULUS +2 SHEAR MODULI
ANISOTROPY FROM ADIABATIC PERTS- ie. FROM INFLATION
● INITIAL CONDITIONS
● POWER SERIES SOLUTION
● "WOULD-BE SCALAR MODE"
THOSE USED FOR INFLATION
CUBICSYMMETRY
CMB ANISOTROPIES : IN PROGRESS
ISOTROPIC(COMPUTE USING CAMB)
ANISOTROPIC
EXAMPLE OF SASH : l =4
SYMMETRY ADAPTEDSPHERICAL HARMONICS (SASH) eg VON DE LAGE & BETHE 1947
ROTATION
CONCLUSIONS● PERTURBATIONS IN DARK ENERGY ARE IMPORTANT
● ADIABATIC ELASTIC DARK ENERGY MODELS CAN BE STABLE
● THERE APPEAR TO BE ALIGNMENTS IN THE CMB
● QUALITATIVELY, THEY MAYBE DUE TO ANISOTROPIC DARK ENERGY
● WE HAVE INVESTIGATED THE CASE OF CUBIC SYMMETRY
● NEXT (AND VERY IMPORTANT STEP) IS TO COMPUTE
● THEN WE CAN INVESTIGATE THE FIT TO THE DATA
● NB ONE IS NOT RESTRICTED TO CUBIC SYMMETRY