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Dark matter Particle Physics and Cosmology LianTao Wang University of Chicago UCAS.

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Page 1: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Dark matter Particle Physics and

Cosmology

LianTao WangUniversity of Chicago

UCAS.

Page 2: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Introduction

Page 3: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Dark matter in the universe

We know dark matter is out there.But we don’t know what it is.

Page 4: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Observational evidence of dark matter

Page 5: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

More matter than light

Zwicky 1933

Page 6: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

More matter than lightDark matter in the satellites of the Milky Way

Bullock/Geha

Strigari et al, Nature, Volume 454, pp. 1096-1097 (2008)

Page 7: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Rotational curve

M33

Vera Rubin1970

Page 8: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Bullet cluster

Page 9: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Bullet cluster

gas

Page 10: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Bullet cluster

dark matter

Page 11: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

A consistent pictureConsistency of different cosmological measures of the matter density

The different measures of matter density from growth of clusters, fraction of gas in clusters, CMB, Supernova distances and Baryon acoustic oscillation all agree on a value for the matter density that is close to 25% of the critical density of the universe, which is about 6 times the density in baryons.

AA49CH11-Allen ARI 2 August 2011 10:40

Clustergrowth

Clustergrowth

SNIa WMAP5

WMAP5

a b

0.10– 2.5

– 2.0

– 1.5

– 1.0

w

– 0.5

0

0.2 0.3 0.4 0.60.5

Ωm

– 2.0

– 1.5

– 1.0w

– 0.5

0

1.11.00.90.80.70.6

σ8

All

All

Cluster growth + WMAP5

fgas

BAO

Figure 11Joint 68.3% and 95.4% confidence regions for the dark energy equation of state and mean matter density (a) or perturbation amplitude(b) from the abundance and growth of ROSAT All-Sky Survey (RASS) clusters at z < 0.5 (Mantz et al. 2010b) and fgas measurements atz < 1.1 (Allen et al. 2008), compared with those from Wilkinson Microwave Anisotropy Probe (WMAP) (Dunkley et al. 2009), SNIa(Kowalski et al. 2008) and baryon acoustic oscillations (BAO) (Percival et al. 2010) for spatially flat, constant w models. Combinedresults from RASS clusters and WMAP are shown in gray in panel b; gold contours in both panels show the combination of all data sets.The BAO-only constraint differs from that in Figure 10 due to the use of different priors. Adapted from Mantz et al. (2010b; the BAOconstraints in panel a have been updated to reflect more recent data).

2009a, Andersson et al. 2010), or gravitational lensing signal (e.g., Hoekstra 2007, Johnston et al.2007, Rykoff et al. 2008, Leauthaud et al. 2010, Okabe et al. 2010) have been employed.

These variations in mass estimation and analysis methods, in addition to changes to instrumentcalibration over the years, make a comprehensive and fair census of scaling relation results prob-lematic. Here, we focus on the cosmological importance of scaling relation measurements, citingexamples from recent work where the issues mentioned above are at least partially mitigated.

For X-ray and SZ observables, under the assumption of strict self-similarity (no additionalheating or cooling), Kaiser (1986) derived specific slopes and redshift dependences for the power-law form of Equation 16:

Lbol

E(z)∝ [E(z)M ]4/3,

kTmw ∝ [E(z)M ]2/3,

E(z)Y ∝ [E(z)M ]5/3,

(24)

where the factors of E(z) = H (z)/H 0 are appropriate for measurements made at a fixed critical-overdensity radius. The subscripts bol and mw reflect the fact that these predictions apply tothe bolometric luminosity and mass-weighted temperature. Optical richness is more complex topredict, but empirical studies that map galaxies to subhalos in simulations support a power-lawrichness-mass relation for groups and clusters (Conroy & Wechsler 2009).

Figures 12 and 13 show a few examples of recent scaling relation measurements. Leauthaudet al. (2010) present a M − LX relation for X-ray-selected clusters in the Comological EvolutionSurvey (COSMOS) field by measuring stacked weak lensing masses (Figure 12a). Under the

www.annualreviews.org • Cosmology from Galaxy Clusters 441

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Allen et al, Annual Review of Astronomy and Astrophysics, vol. 49, pp. 409-470 (2011)

Mantz et al, Monthly Notices of the Royal Astronomical Society, Volume 406, Issue 3, pp. 1759-1772 (2010)

Page 12: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Basic facts about dark matter.

Page 13: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Basic facts about dark matter.

- Heavy, slow moving. Or “cold”. mDM > 10 keV.

Page 14: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Basic facts about dark matter.

- Heavy, slow moving. Or “cold”. mDM > 10 keV.

- Stable. Life time >> age of universe (1017 sec).

Page 15: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Basic facts about dark matter.

- Heavy, slow moving. Or “cold”. mDM > 10 keV.

- Stable. Life time >> age of universe (1017 sec).

- Very dark, charge < 10-3 e.

Page 16: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Basic facts about dark matter.

- Heavy, slow moving. Or “cold”. mDM > 10 keV.

- Stable. Life time >> age of universe (1017 sec).

- Very dark, charge < 10-3 e.

- Mass. Seed structure: 1/m = de Brogile wave length < size of sub-halo. m > 10-33 GeV

Not too big to block light. m < 10 47 GeV.

80 order of magnitude allowed range.

Page 17: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Beyond the Standard Model

Stable SM particles can not be dark matter

Photon: masslessNeutrino: < 1 eVElectron: charged

Page 18: Dark matter Particle Physics and Cosmologytheory.uchicago.edu/.../dark-matter-472/cdm_intro.pdf · 2016-06-22 · CMB, Supernova distances and Baryon acoustic oscillation all agree

Beyond the Standard Model

Stable SM particles can not be dark matter

Photon: masslessNeutrino: < 1 eVElectron: charged

Dark matter = new unknown particle !