varying supercluster shape in different cosmology

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Varying supercluster shape in different cosmology Junsup Shim 1 , Jounghun Lee 1 , Baojiu Li 2 , Marco Baldi 3 3rd Korea-Japan Workshop on Dark Energy 1 Seoul National Univ., Korea 2 Durham Univ., UK 3 Bologna Univ., INAF, INFN, Italy

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Page 1: Varying supercluster shape in different cosmology

Varying supercluster shape in different cosmology

Junsup Shim1, Jounghun Lee1, Baojiu Li2, Marco Baldi3

3rd Korea-Japan Workshop on Dark Energy

1 Seoul National Univ., Korea 2 Durham Univ., UK 3 Bologna Univ., INAF, INFN, Italy

Page 2: Varying supercluster shape in different cosmology

Expanding Universe

Our Universe is known to be expanding faster and faster.

(NASA & ESA)

Our Universe

(Hubble29)

Page 3: Varying supercluster shape in different cosmology

Accelerated expansion

Physical origin of this acceleration is a hot issue in cosmology.

(Riess+  98)(Perlmutter+  99)

Page 4: Varying supercluster shape in different cosmology

‘Ʌ’CDM cosmology

Accelerated expansion is attributed to ‘Ʌ’. (Riess+98, Perlmutter+99)

Our Universe is mainly (~95%) dominated by dark components.

Dark%energy%68%%

Dark%ma.er%27%%

Ordinary%ma.er%5%%

Cosmic%energy%budget%

Page 5: Varying supercluster shape in different cosmology

Features of Cosmos

Ade+15    (Planck  collaborations)

Large scale structure CMB power spectrumSpringel+06

“Concordance cosmology”

Page 6: Varying supercluster shape in different cosmology

Fine tuning of Ʌ

ɅCDM suffers from fine tuning problem

(𝝆vaccum/𝝆Ʌ ~ 10120) of cosmological

constant Ʌ.

Alternative theories to explain the accelerating expansion, at the same time, to avoid/alleviate the fine tuning have been suggested.

Page 7: Varying supercluster shape in different cosmology

Possible origin of accelerated expansion

Cosmological constant Ʌ (Concordance cosmology)

Dynamic dark energy

Modification of gravity

Page 8: Varying supercluster shape in different cosmology

Conventional probesConventional LSS statistics mainly focused on the strength of clustering. (Sutter+08, Lombriser+12, Bel+15, Munshi+16)

To survive as viable from the stringent tests (Bean+08, Reyes+10, Wojtak+11, Wei+13), their behavior should mimic concordance cosmology.

Page 9: Varying supercluster shape in different cosmology

Complimentary probe

In this work, we concentrate on the pattern of clustering in particular at the largest scale through the superclusters.

Page 10: Varying supercluster shape in different cosmology

The Largest scale clustering

Strength of clusteringGravitational law ? Nature of dark energy ?

Pattern of clustering

Cosmic web= func(Gravity, Repulsion)

Superclusters are located at the densest part of the cosmic web.

Page 11: Varying supercluster shape in different cosmology

Supercluster

2nd order clusters, Cluster of clusters (Abell 58)

The largest structure known in the cosmos. Wray+06

Page 12: Varying supercluster shape in different cosmology

Filamentary supercluster

Superclusters have elongated filamentary structures. (Dekel+84, Wray+06, Einasto+11)

ESA & Planck Collaboration / Rosat/ Digitised Sky Survey

Mshapley ~ 1016h-1M⦿

Page 13: Varying supercluster shape in different cosmology

Superclusters in different Universe?We compare straightness of superclusters in

- Coupled dark energy (cDE) : a branch of dynamic DE

- f(R) gravity : a branch of modified gravity

by analyzing halo catalogs from cosmological simulations of respective cosmologies.

Page 14: Varying supercluster shape in different cosmology

Supercluster Size & specific size

The degree of how much straight the supercluster is.

size S

S̃ ⌘ S

Ncluster

cluster

(Shim & Lee 13)

Page 15: Varying supercluster shape in different cosmology

Supercluster straightness

The larger the value of S, the straighter the supercluster is.

S̃ = 0.92h�1Mpc

S̃ = 1.95h�1Mpc

S̃ = 3.07h�1Mpc

stra

ight

er

xy plane yz plane xz plane~

(Shim & Lee 13)

Page 16: Varying supercluster shape in different cosmology

Coupled dark energy

- Coupled dark energy (cDE) : Interaction exists between scalar field dark energy 𝝓 and CDM.

Model U(𝝓) 𝞪 𝛃(𝝓)𝚲CDM Const … …

EXP002 e-𝞪𝝓 0.08 0.1EXP003 e-𝞪𝝓 0.08 0.15

EXP003e3 e-𝞪𝝓 0.08 0.4e3𝝓

SUGRA003 𝝓-𝞪e𝝓2/2 2.15 -0.15

=> additional fifth force

�(�) ⌘ �dlnmCDM

d�

Coupling function

Page 17: Varying supercluster shape in different cosmology

f(R) gravity

- f(R) gravity : Modified gravity model which generalizes Ricci scalar R in Einstein-Hilbert action to f(R).

f(R) = �m2 c1(�R/m2)n

c2(�R/m2)n + 1 (Hu & Sawicki 07)

fR ⌘ df

dRfR0 = 0, f(R) = ⇤

General Relativity

where=> addition

al

fifth force

Page 18: Varying supercluster shape in different cosmology

Simulation setup

cDE f(R) gravity

Data CoDECS (Baldi12) ECOSMOG (Li+12)

# particles 10243 10243

Box size 1h-1Gpc 1h-1Gpc

(𝞨m, 𝞨Ʌ, 𝞨b) (0.27, 0.73, 0.045) (0.24, 0.76, 0.045)

(h, 𝝈8, ns) (0.703, 0.809, 0.966) (0.73, 0.8, 0.96)

Page 19: Varying supercluster shape in different cosmology

Construction of supercluster

We apply Friends-of-Friends group finder to halos of mass M≧1013h-1M⦿ and regard clusters within the linking length as member of supercluster.

Then we also apply minimal spanning tree method to identify filamentary structure.

Page 20: Varying supercluster shape in different cosmology

Superclusters in cDE

(Shim & Lee 13)

Page 21: Varying supercluster shape in different cosmology

Superclusters were straighter in the past.

Straightness deviation from ɅCDM is growing in higher redshift.

Superclusters in cDE

(Shim & Lee 13)

Page 22: Varying supercluster shape in different cosmology

Superclusters in f(R)

F5 : fR0 = �10�5

F6 : fR0 = �10�6

(Shim+14)

Page 23: Varying supercluster shape in different cosmology

Superclusters in f(R)

Superclusters were straighter in the past.

Straightness deviation from ɅCDM is diminishing in higher redshift.

(Shim+14)

Page 24: Varying supercluster shape in different cosmology

cDE vs f(R)

(Shim+14) (Shim&Lee13)

Page 25: Varying supercluster shape in different cosmology

SummaryWe investigate how the clustering pattern at the largest scale changes in cDE/f(R) gravity through superclusters shape.

It is found that superclusters in cDE/f(R) gravity are significantly less straight than those in ɅCDM.

Straightness evolutions of cDE/f(R) gravity compared to that of ɅCDM are in the opposite direction.

Page 26: Varying supercluster shape in different cosmology

Superclusters in f(R)+𝝼

Page 27: Varying supercluster shape in different cosmology

Superclusters in f(R)+𝝼