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L.  Perivolaropoulos L.  Perivolaropoulos

L. Perivolaropoulos - PowerPoint Presentation

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L. Perivolaropoulos - PPT Presentation

httpleandrosphysicsuoigr Department of Physics University of Ioannina Open page Accelerating Universe Geometric Observational Constraints and Growth of Perturbations Main Points Recent Geometric Probe Data SnIa CMB BAO ID: 250033

coupling cdm minimal perturbations cdm coupling perturbations minimal energy dark scales scalar halo profiles data consistency scale cluster hubble

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Slide1

L. Perivolaropouloshttp://leandros.physics.uoi.grDepartment of PhysicsUniversity of Ioannina

Open page

Accelerating Universe:

Geometric Observational Constraints

and

Growth of PerturbationsSlide2

Main Points

Recent Geometric Probe Data (SnIa, CMB, BAO)

Expansion Rate of the Universe is very similar

to the rate predicted by

Λ

CDM

There are some puzzling conflicts between ΛCDM predictions and LSS cosmological observations

Q: Is there a concrete physical model where dark energy can have significant clustering properties on small scales?

Yes. This naturally occurs in Scalar-Tensor cosmologies due to the direct coupling of the scalar field perturbations to matter induced curvature perturbations

Large Scale Velocity Flows (3

σ)

Galaxy and Cluster Halo Profiles (2σ-3σ)

There is a potential resolution

of these conflicts if Dark Energy had

clustering properties. Slide3

3

Geometric Probes: Recent SnIa Datasets

Q2: What is the consistency of each dataset with

Λ

CDM?

Q3: What is the consistency of each dataset with Standard Rulers?

J. C. Bueno Sanchez, S. Nesseris, LP, JCAP 0911:029,2009,

0908.2636 Q1: What is the Figure of Merit of each dataset? Slide4

Figures of Merit

The Figure of Merit:

Inverse area of the 2

σ

CPL parameter contour. A measure of the effectiveness of the dataset in constraining the given parameters.

SNLS

ESSENCE

GOLD06

UNION

CONSTITUTION

WMAP5+SDSS5

WMAP5+SDSS7Slide5

5

Figures of Merit

The Figure of Merit:

Inverse area of the 2

σ CPL parameter contour. A measure of the effectiveness of the dataset in constraining the given parameters.

SDSS5

SDSS7

Percival et. al.

Percival et. al.Slide6

6

Consistency with Λ

CDM

ESSENCE+SNLS+HST data

SNLS 1yr data

Trajectories of Best Fit Parameter Point

The trajectories of SNLS and Constitution

are clearly

closer to ΛCDM for most values of Ω0mGold06 is the furthest from Λ

CDM for most values of Ω0mQ: What about the σ-distance (dσ

) from ΛCDM?

Ω0m=0.24Slide7

7

The σ-

distance to

Λ

CDM

ESSENCE+SNLS+HST data

Trajectories of Best Fit Parameter Point

Consistency with

ΛCDM Ranking:Slide8

8

The σ-distance to Standard Rulers

Consistency with Standard Rulers Ranking:

ESSENCE+SNLS+HST

Trajectories of Best Fit Parameter PointSlide9

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%

Cluster and Galaxy Halo Profiles: - Predicted: Shallow, low-concentration mass profiles - Observed: Highly concentrated, dense halos -

Probability of Consistency: 3-5%

From LP, 0811.4684R. Watkins et. al. , 0809.4041

Broadhurst et. al. ,ApJ 685, L5, 2008, 0805.2617, S. Basilakos, J.C. Bueno Sanchez, LP., 0908.1333, PRD, 80, 043530, 2009. Slide10

10

Cluster Halo Profiles

NFW profile:

Λ

CDM prediction:

The predicted concentration parameter c

vir

is significantly smaller than the observed.

From S. Basilakos, J.C. Bueno-Sanchez and LP,

PRD, 80, 043530, 2009, 0908.1333.

Data from:

Navarro, Frenk, White, Ap.J., 463, 563, 1996Slide11

11

Cluster Halo Profiles

NFW profile:

clustered dark energy

Clustered Dark Energy can produce more concentrated halo profiles

From S.

Basilakos

, J.C.

Bueno

-Sanchez and LP,

PRD, 80, 043530, 2009, 0908.1333.

Data from:

Navarro, Frenk, White, Ap.J., 463, 563, 1996Slide12

Producing Dark energy Perturbations

Q: Is there a model with a similar expansion rate as

Λ

CDM but with significant clustering of dark energy?

A: Yes. This naturally occurs in Scalar-Tensor cosmologies

due to the direct coupling of the scalar field perturbations

to matter induced curvature perturbationsSlide13

Scalar-Tensor Theories

Rescale

Φ

Units:

General Relativity:

Generalized Einstein-Field Equations:Slide14

Background Cosmological Evolution

Flat FRW metric:

Generalized Friedman equations:Slide15

Advantages and Constraints

Advantages:

Natural generalizations of GR (superstring

dilaton

, Kaluza-Klein theories) General theories (f(R) and

Brans-Dicke theories consist a special case of ST) Potential for Resolution of Coincidence Problem Natural Super-acceleration (w

eff <-1) Amplified Dark Energy Perturbations

Constraints:Solar System

CosmologySlide16

Background Evolution

J. C.

Bueno

Sanchez., LP in preparation Slide17

Minimally Coupled Quintessence

Thawing Minimally Coupled Quintessence

Slide18

Non-minimal Coupling

Oscillations (due to coupling to

ρ

m

) and non-trivial evolutionSlide19

Effective Equation of State

Effective Equation of State:

Scalar-Tensor (

λ

f

=5)

Minimal

Coupling

f=0)

w

eff

zSlide20

Perturbations: Analytical Approximations

Perturbed FRW metric (Newtonian gauge):

Generalized Einstein-Field Equations:Slide21

Analytical Approximations: Sub-Hubble ST scales

No suppression on small scales!Slide22

Analytical Approximations: Sub-Hubble GR scales

Suppressed fluctuations on small scales!

Sub-Hubble GR scales

(as in minimally coupled quintessence)Slide23

Numerical Solutions

Scalar Field Perturbations

Minimal Coupling (F=1)

Scale = 30 h

-1

Mpc

Non-Minimal Coupling (F=1-

λf2

Φ2)Slide24

Numerical Solutions

Matter Density Perturbations

Minimal Coupling (F=1)

Non-Minimal Coupling (F=1-

λ

f

2

Φ2)Slide25

Numerical Solutions

Scalar Field Density Perturbations

Minimal Coupling (F=1)

Non-Minimal Coupling (F=1-

λ

f

2

Φ2)Slide26

Numerical Solutions

Scale Dependence of Dark

Energy/Dark Matter

Perturbations

Minimal Coupling (F=1)

Non-Minimal Coupling (F=1-

λ

f Φ2

)

Dramatic Difference on sub-Hubble scales!Slide27

Numerical Solutions

Scale Dependence of Dark Energy Perturbations

Minimal Coupling (F=1)

Non-Minimal Coupling (F=1-

λ

f

Φ2)

Dramatic Difference on sub-Hubble scales!Slide28

SUMMARY

Recent Geometric Probe Data (SnIa, CMB, BAO

)

are increasingly consistent with

Λ

CDM and with each other. The Constitution SnIa dataset is of the highest quality and is also the most consistent with ΛCDM and with Standard

Rulers.Observed Cluster Halo Profiles

are significantly more concentrated than predicted by ΛCDM. This may be interpreted as a trace of an additional clustering energy component in the halo.

Scalar Tensor cosmologies are generic extensions of GR. They naturally allow for crossing of the w=-1 line and amplified dark energy perturbations on sub-Hubble scale by a factor of more than 104

compared to quintessence. This may help in the resolution of the cluster profile puzzle.

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