january 25, 2006 ncw, nice 1 1 caustics in dark matter halos sergei shandarin, university of kansas...

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January 25, 2006 NCW, Nice 1 Caustics in Dark Matter Halos Sergei Shandarin, University of Kansas (collaboration with Roya Mohayaee, IAP) Nonlinear Cosmology Program: Nice-Marseille-Paris

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January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 11

Caustics in Dark Matter Halos

Caustics in Dark Matter HalosSergei Shandarin, University of Kansas

(collaboration with Roya Mohayaee, IAP)

Nonlinear Cosmology Program: Nice-Marseille-Paris

Sergei Shandarin, University of Kansas

(collaboration with Roya Mohayaee, IAP)

Nonlinear Cosmology Program: Nice-Marseille-Paris

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 22

OutlineOutline

LCDM and LWDM models Introduction to caustics: 1D and 2D cases 3D universe Summary 1 What kills caustics? Summary 2

LCDM and LWDM models Introduction to caustics: 1D and 2D cases 3D universe Summary 1 What kills caustics? Summary 2

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 33

A big question: what is the dark matter?

A big question: what is the dark matter?

DIRECT DETECTIONINDIRECT DETECTION

Annihilation of self-annihilatedaxions and neutralinos producesgamma-raysHESS, GLAST experimentsAharonian et al 2005, Science

Weak lensinge.g. Gavazzi, Mohayee, Fort 2005

e.g. Sikivie, Ipser 1992Sikivie, Tkachev, Wang 1997: role of internal and external caustics

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 44

Unresolved problems in LCDM Reduction of satellite halos

Kauffmann et al 1993; Klypin et al 1999; Moore et al 1999; Willman et al 2004

Reduction of galaxies in voids Peebles 2001; Bode et al 2001

Low concentration of DM in galaxies Dalcanton & Hogan 2001; van den Bosch & Swaters 2001; Zentner & Bullock 2002; Abazajian et al 2005

Angular momentum problem and formation of disk galaxies

Dolgov & Sommer-Larson 2001; Governato et al 2004;

Kormendy & Fisher 2005

Possible solution: Warm Dark Matter

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 55

Lamda Warm Dark Matter

(LWDM)

Lamda Warm Dark Matter

(LWDM)

Abazajian 20051.7 keV < m < 8.2 keV

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 66

Why caustics?Why caustics?

Saichev 1976

For 100 GeV SUSY neutralino (LCDM)

For a few keV sterile neutrino or gravitino (LWDM)

Galaxy formation is not hierarchical or only marginally hierarchical! ( only a few mergers results in the halo of galactic size)

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 77

Caustics in geometric optics

Caustics in geometric optics

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 88

Generic singularities in 1DGeneric singularities in 1D

Points at a generic instant of time

Points at particular instants of time

Arnol’d, Shandarin, Zel’dovich 1982

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 99

Collisionless DM and collisional baryons

Collisionless DM and collisional baryons

Shandarin, Zel’dovich 1989

Dark matter

Baryons

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1010

Zel’dovich ApproximationZel’dovich Approximation

in comoving coordinates

potential perturbations

Density

are eigen values of

is a symmetric tensor

Density becomes

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1111

Generic singularities in 2DGeneric singularities in 2D

Lines (1D) at a generic instant of time

Points (0D) at a generic instant of time

Points (0D) at particular instants of time

Points (0D) at particular instants of time

Arnol’d, Shandarin, Zel’dovich 1982

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1212

Zel’dovichApproximation (2D)

N-body simulations (2D)

versus

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1313

2D N-body simulations (discreteness effect)

2D N-body simulations (discreteness effect)

Melott, Shandarin 1989

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1414

Caustics in high

resolution

2D Simulatio

ns

Caustics in high

resolution

2D Simulatio

ns

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1515

2D vs 3D2D vs 3D

2D simulations 3D simulations

Melott, Shandarin 1989 Shirokov, Bertschinger 2005

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1616

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

Shirokov, Bertschinger 2005

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1717

Complexity of caustics(2D simulations)

Complexity of caustics(2D simulations)

Melott, Shandarin 1989

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 1818

OutlineOutline

LCDM and LWDM models Introduction to caustics: 1D and 2D cases 3D universe Summary 1 What kills caustics? Summary 2

LCDM and LWDM models Introduction to caustics: 1D and 2D cases 3D universe Summary 1 What kills caustics? Summary 2

z=153

z=7.2

z=86z=115

z=0z=1

LCDM simulation (Diemand et al 2005)

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2020

* Hierarchical clustering

* Smallest halos

* Hierarchical clustering

* Smallest halos

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2121

LWDM simulations

m_x = 1.2 h^(5/4)) keV

Gotz & Sommer-Larson 2003

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2222

Generic singularities in 3DGeneric singularities in 3D

Lines (1D) at a generic instant of time

Surfaces (2D) at a generic instant of time

Points (0D) at a generic instant of time

Points (0D) at a generic instant of time

Points (0D) at particular instants of time

Points (0D) at particular instants of time

Arnol’d, Shandarin, Zel’dovich 1982

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2323

Caustics in hot systems

Caustics in hot systems

Colombi, Touma 2005

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2424

Summary 1Summary 1

Formation of caustics in dark matter halos (structures) is a more universal phenomenon than many cosmologists thought

before. Caustics have a complex geometry. The generic caustics can be

Surfaceses (2D) Lines (1D) Points (0D) at generic time Points (0D) at particular times

Exiting prospect: testing particle physics using caustics in DM halos.

Formation of caustics in dark matter halos (structures) is a more universal phenomenon than many cosmologists thought

before. Caustics have a complex geometry. The generic caustics can be

Surfaceses (2D) Lines (1D) Points (0D) at generic time Points (0D) at particular times

Exiting prospect: testing particle physics using caustics in DM halos.

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2525

Three things that destroy caustics.

Three things that destroy caustics.

• Discreteness (numerical, not physical)

• Phase-space becomes too fine-grained eventually reaching the physical discreatness (physical)

• Thermal velocity dispersion (physical)

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2626

2D N-body simulations (discreteness effect)

2D N-body simulations (discreteness effect)

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2727

Phase space becomes too fine-

grained

Phase space becomes too fine-

grained

Colombi, Touma 2005

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2828

Self-similar spherically symmetric solution

Self-similar spherically symmetric solution

Fillmore & Goldreich 1984; Bertschinger 1985

Equation of motion

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 2929

Nondimensional EquationNondimensional Equation

Initial condition

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3030

Function

Function

Bertschinger 1985

At constant q:trajectory of particle

At constant \tau:positions of particles

Two interpretations

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3131

Density near caustics

Density near caustics

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3232

Density (cold medium)Density (cold medium)

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3333

Density near caustics

Density near caustics

Tully 2005

NGC 5846

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3434

Effect of thermal velocity dispersion

Effect of thermal velocity dispersion

Initial condition in coldmedium

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3535

Effect of thermal velocity dispersion

Effect of thermal velocity dispersion

Distance of the caustic in stream Distance of the caustic in stream v from the caustic in stream v=0v from the caustic in stream v=0

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3636

Universal density profiles in the vicinity of caustics

Universal density profiles in the vicinity of caustics

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3737

Gravitational cooling

Mohayaee, Shandarin 2005

January 25, 2006January 25, 2006 NCW, NiceNCW, Nice 3838

Summary 2Summary 2

Spherical (self-similar) model can be used as a guideline More realistic models are badly needed Other singularities may be more interesting for

annihilation detection provided that they can be resolved Evolution in phase space needs to be studied in more

detail

Spherical (self-similar) model can be used as a guideline More realistic models are badly needed Other singularities may be more interesting for

annihilation detection provided that they can be resolved Evolution in phase space needs to be studied in more

detail