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Velocity distribution of dark matter Malcolm Fairbairn

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Page 1: Malcolm Fairbairn - hep.ph.ic.ac.uk

Velocity distribution of dark matter

Malcolm Fairbairn

Page 2: Malcolm Fairbairn - hep.ph.ic.ac.uk

1.Dark matter density uncertainties

2.Dark matter anisotropy uncertainties

3. Is it smooth?

4. Is it Maxwellian?

Outline

Page 3: Malcolm Fairbairn - hep.ph.ic.ac.uk

Catena and Ullio arXiv:0907.0018

Density of Dark Matter

at Solar Radius

Relatively under control?

Page 4: Malcolm Fairbairn - hep.ph.ic.ac.uk

...but is it really understood?

Weber and de Boer arXiv:0910.4272

Page 5: Malcolm Fairbairn - hep.ph.ic.ac.uk

Default halo model for dark matter

direct detection

1. Isothermal halo

2.Gaussian velocity distribution

3. Isotropic velocity distribution

PROBABLY NONE OF THESE ARE TRUE !

Page 6: Malcolm Fairbairn - hep.ph.ic.ac.uk

So what?

Page 7: Malcolm Fairbairn - hep.ph.ic.ac.uk

Direct detection of dark matter

Page 8: Malcolm Fairbairn - hep.ph.ic.ac.uk

Solar Orbit signal

Page 9: Malcolm Fairbairn - hep.ph.ic.ac.uk

Earth goes round Sun, Sun goes round Galaxy

Page 10: Malcolm Fairbairn - hep.ph.ic.ac.uk

Annual modulation signal

Page 11: Malcolm Fairbairn - hep.ph.ic.ac.uk

DAMA/LIBRA results

Page 12: Malcolm Fairbairn - hep.ph.ic.ac.uk
Page 13: Malcolm Fairbairn - hep.ph.ic.ac.uk

Typical values obtained from simulations

are 1 < g < 1.5 ,b = 3

Diemand et al.

(2005)

Simulations show halos not isothermal

Page 14: Malcolm Fairbairn - hep.ph.ic.ac.uk

Tangential

Velocity

Dispersion

Radial

Velocity

Dispersion

Page 15: Malcolm Fairbairn - hep.ph.ic.ac.uk

Gustafsson, MF and Sommer-Larsen arXiv:0608634

Dark matter particle orbits far from circular

Page 16: Malcolm Fairbairn - hep.ph.ic.ac.uk

radial

tangential

0812.1048, Sommer-Larsen astro-ph/0602595, astro-ph/0204366

Dark Matter halos anisotropic

Page 17: Malcolm Fairbairn - hep.ph.ic.ac.uk

g

Hansen 0812.1048

Anisotropy vs density gradient

Page 18: Malcolm Fairbairn - hep.ph.ic.ac.uk

Jeans equation

hydrostatic equilibrium

Can use plus assumptions to derive b(r).

Authors have tested method using simulated clusters.

Velocity Anisotropy in Galaxy Clusters

Host et al. arXiv:0808.2049

Page 19: Malcolm Fairbairn - hep.ph.ic.ac.uk

Velocity Anisotropy in Galaxy Clusters

Host et al. arXiv:0808.2049

Page 20: Malcolm Fairbairn - hep.ph.ic.ac.uk

Ludlow et al.arXiv:1001.2310

Pseudo Phase-space Density

Page 21: Malcolm Fairbairn - hep.ph.ic.ac.uk

Trying to model this

Page 22: Malcolm Fairbairn - hep.ph.ic.ac.uk

Try to reconstruct Einasto profile using Jean’s equation

and our model for Pseudo Phase Space Density

We integrate this

And (try to) fit to get Einasto profile!!

See also Dehnen and McLaughlin for related approach.

Page 23: Malcolm Fairbairn - hep.ph.ic.ac.uk

Does it explain observed g-b relationship?

well kind of....... Expect things to go wrong

in the middle anyway

Page 24: Malcolm Fairbairn - hep.ph.ic.ac.uk

Phase space density with baryons

Tissera et al. arXiv:0911.2316

Page 25: Malcolm Fairbairn - hep.ph.ic.ac.uk

It gets worse

The distribution is non-Gaussian

Page 26: Malcolm Fairbairn - hep.ph.ic.ac.uk

sself-interaction< 1 cm2/g(Markevitch 2004)

Page 27: Malcolm Fairbairn - hep.ph.ic.ac.uk
Page 28: Malcolm Fairbairn - hep.ph.ic.ac.uk

Non Extensive Statistics

At any given time, probability of a particular delay time, t, given by

Over course of a year, b varies quite a lot due to seasonal factors.Therefore, over the long term, one needs to include fluctuations in b

Page 29: Malcolm Fairbairn - hep.ph.ic.ac.uk

Non Extensive Statistics

if b is sum over Gaussian random variables ...

leads to a c2 distribution ...

which yields

Page 30: Malcolm Fairbairn - hep.ph.ic.ac.uk

Applied to train times

Page 31: Malcolm Fairbairn - hep.ph.ic.ac.uk

1.Long range forces (gravity)

2.Lack of thermalisation (Non-self interacting)

3.Multiple populations of dark matter

Reasons why Non Extensive Statistics may be

relevant for dark matter

Page 32: Malcolm Fairbairn - hep.ph.ic.ac.uk

Intuition from spherical infall?

Sikivie, Tkachev and Wang astro-ph/9609022

Page 33: Malcolm Fairbairn - hep.ph.ic.ac.uk

Tangential tails vs. Radial Tails

Earlier simulations also claim tangential distribution changes less

tangential low r

tangential high r

radial low r

radial high r

Moore et al astro-ph/0106271

Page 34: Malcolm Fairbairn - hep.ph.ic.ac.uk

a = -1.1 q=0.79

a =-2 q=0.91

a =-2.6 q=1.05

a = -1.1 q=0.75

a =-2 q=0.89

a =-2.6 q=1.045

Universal Velocity Distribution?

Hansen, Moore, Zemp

and Stadel astro-ph/0505420

Page 35: Malcolm Fairbairn - hep.ph.ic.ac.uk
Page 36: Malcolm Fairbairn - hep.ph.ic.ac.uk

Via Lactea non-Gaussianity and anisotropy

MF and Schwetz : arXiv 0808.0704 :

Page 37: Malcolm Fairbairn - hep.ph.ic.ac.uk

Velocity distributions

around 8.5 kpc.

Kuhlen et al.

arXiv: 0912.2358

Best fit

Maxwell-Boltzmann

Page 38: Malcolm Fairbairn - hep.ph.ic.ac.uk

Fantin, Merrifield

and Green

arXiv:0808.1050

Page 39: Malcolm Fairbairn - hep.ph.ic.ac.uk

Detailed resimulation of Aquarius Halo

Vogelsberger and White arXiv:1002.3162

Page 40: Malcolm Fairbairn - hep.ph.ic.ac.uk

Large Number of Fine Streams Contributing to Dispersion

- No sharp features

Vogelsberger and White arXiv:1002.3162

Page 41: Malcolm Fairbairn - hep.ph.ic.ac.uk

Ling et al.

arXiv:

0909.2028

Simulations with Baryons

Page 42: Malcolm Fairbairn - hep.ph.ic.ac.uk

Ling et al. arXiv:0909.2028

Simulations with baryons

Non-gaussianity Evidence for co-rotating dark disk?

Page 43: Malcolm Fairbairn - hep.ph.ic.ac.uk

Conclusions

1. Dark Matter velocity distribution non-Gaussian.

2. Dark Matter velocity anisotropic.

3. Dark Matter velocity badly understood.

4. Normally will not effect discovery of dark matter in direct experiment.

5. Critical for comparing different experiments with each other,

6. Critical for comparing direct detection with colliders.

7. Will affect interpretation of positive signal from any detector.

Page 44: Malcolm Fairbairn - hep.ph.ic.ac.uk