dark matter direct and indirect detection martti raidal nicpb, tallinn, estonia 07.01.2015nordita...

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Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015 NORDITA Winer School 2015 1

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Page 1: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

1

Dark Matter direct and indirect detection

Martti Raidal

NICPB, Tallinn, Estonia

07.01.2015 NORDITA Winer School 2015

Page 2: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

07.01.2015 NORDITA Winer School 2015 2

We are experiencing very interesting period in fundamental physics

there are paradigm shifts in several fields

Page 3: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Instead of introduction:

A lesson from the LHC

07.01.2015 NORDITA Winer School 2015 3

Page 4: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

LHC discovered the Higgs boson

17.12.2014 Frascati, 2014 4

Page 5: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

All LHC + Tevatron data - 10σ signal

17.12.2014 Frascati, 2014 5

P. Giardino, K. Kannike, I. Masina, M. Raidal, A. Strumia,arXiv:1303.3570

Page 6: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Tests of Higgs couplings

17.12.2014 Frascati, 2014 6

Page 7: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

New physics enters only in loops

17.12.2014 Frascati, 2014 7

Page 8: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

At the same time ….

• LHC:– No SUSY discovered yet – No signals of compositness, no new resonances – No extra dimensions– No unexpected results

• Precision physics and flavour physics:– No new sources of flavour and CP violation– No higher dim. operators below 10-100 TeV

17.12.2014 Frascati, 2014 8

Page 9: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

This is exactly opposite to the expectations by naturalness:

• All scalar masses must be at cutoff scale …

• … unless there exists a stabilizing mechanism at EW scale

• … or Nature is fine tuned

17.12.2014 Frascati, 2014 9

Page 10: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

17.12.2014 Frascati, 2014 10

The hierarchy problem is properly named: it is not the "quadratic divergence problem”

It concerns the physical hierarchy of physical particles

Naturalness is a real, physical principle for NP

Page 11: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

The lesson

Physics is experimental science!

• No SUSY seems to be around the corner

• Higgs indicates no GUTs

• Community is polarized in rethinking naturalness

07.01.2015 NORDITA Winer School 2015 11

Page 12: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Dark Matter comes to rescue!

07.01.2015 NORDITA Winer School 2015 12

Page 13: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Outline of my lectures

• Dark Matter – the evidence

• Dark Matter candidates

• Ways to detect Dark Matter – direct, indirect, colliders, dark matter self-interactions

07.01.2015 NORDITA Winer School 2015 13

Page 14: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

History of DM Jan Oort (1932) Fritz Zwicky (1933)

07.01.2015 NORDITA Winer School 2015 14

Movement of starsin the Galaxy

Movement of galaxiesin clusters

Page 15: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Evidences for DM

• Small scale (galactic sizes/distances)

• Medium scale (galaxy clusters)

• Large scale (observable Universe)

• DM is dark because it is seen only through its gravitational interaction. No interaction with SM seen so far!

07.01.2015 NORDITA Winer School 2015 15

Page 16: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Small scale - rotation curves of galaxies

07.01.2015 NORDITA Winer School 2015 16

Page 17: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Medium scale – galaxy clusters• Velocity dispersion of galaxies in clusters• Gravitational lensing

07.01.2015 NORDITA Winer School 2015 17

Page 18: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Medium scale – bullet clusters

• Kills MOND, constrains DM self-interactions07.01.2015 NORDITA Winer School 2015 18

Page 19: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Large scale

• Cosmic Microwave Background (CMB) anisotropies

• Large Scale Structure (LSS)

• Baryon Acoustic Oscillations (BAO)

07.01.2015 NORDITA Winer School 2015 19

Page 20: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

The history of Universe

07.01.2015 NORDITA Winer School 2015 20

Page 21: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Anisotropies in the Cosmic Microwave Background

07.01.2015 NORDITA Winer School 2015 21

The ESA Planck satellite

Fluctuations 10-5

Page 22: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

CMB tells the content of the Universe

07.01.2015 NORDITA Winer School 2015 22

• The first peak – overall mass-energy content Ω• The second peak – baryonic matter Ωb

• The third peak – cold Dark Matter ΩDM

• The Universe can be described with ΛCDM

Page 23: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Energy budget of the Universe

07.01.2015 NORDITA Winer School 2015 23

Also SN observations confirm the accelerated expansion of the Universe

Page 24: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

CMB polarization

• Induced by Thomson scattering at the end of recombination – very small effect

• Consistency check for inflation

• Planck Mission polarization data must come out these days!

• The rumor is …..

07.01.2015 NORDITA Winer School 2015 24

Page 25: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Two types of polarization – E-modes and B-modes!

• BICEP2 claims to measure primordial B-modes– Fluctuations of gravity– Gravitational lensing (excluded)

• Can also be induced by dust• Assuming the first, the measured tensor-to-

scalar ratio r=0.2 implies the scale of inflation to be 1016GeV

• This is our only realistic exp. test of quantum nature of gravity

17.12.2014 Frascati, 2014 25

Page 26: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Tension with Planck data

17.12.2014 Frascati, 2014 26

Page 27: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Implications for inflation and gravity?

• V=(1016)4 GeV4 is sub-Planckian – particle physics is under control

• But Lyth bound implies trans-Planckian field excursions

• What about operators likeϕ6, ϕ48, ϕ234567 which all must be there according to standard paradigm?• Inflation data shows no trans-Planckian operators!

17.12.2014 Frascati, 2014 27

Page 28: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Planck published first dust data

17.12.2014 Frascati, 2014 28

The BICEP2 signal strength can be explained with• r=0.2 and no dust• R=0 and dust only

Page 29: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

One needs to study correlations between the BICEP2 and dust maps

17.12.2014 Frascati, 2014 29

• Done by theorists• Small but significant correlation found

• r=0.1±0.04

This analyses must be repeated by experiments

Page 30: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Large scale - BAO

Matter distributionhas a preferred scale

07.01.2015 NORDITA Winer School 2015 30

Acoustic peak dependson DM and baryon content

Page 31: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Large Scale Structure

• Primordial fluctuations are seeds of structure

• Structure formation happens dimension by dimension

• Structure has fractal properties – it repeats itself in different scales

07.01.2015 NORDITA Winer School 2015 31

Page 32: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

DM in galaxies - where is it?• DM halos are believed to

be spherical (cannot loose energy)

• N-body simulations suggest rich sub-halo content (satellite and dwarf galaxies observed)

• Detection of DM depends on mass distribution and minimal mass of subhalos

• Detection of DM depends on DM halo properties around Sun

07.01.2015 NORDITA Winer School 2015 32

Page 33: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

DM density profiles in galaxies

07.01.2015 NORDITA Winer School 2015 33

Page 34: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Non-relativistic DM velocity distribution

07.01.2015 NORDITA Winer School 2015 34

Page 35: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Problems/challenges/future work

• Core vs. cusp problem - N-body simulations prefer cuspy profiles (NFW, Einasto)

• “Missing” satellites compared to N-body sim.• “Too big to fail” – satellites less massive than sim.

• DM self-interactions?

• Planes of satellites in the Galaxy• Bulge-less disc galaxies • Voids too empty?

07.01.2015 NORDITA Winer School 2015 35

Page 36: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Example – core vs cusp problem• Density profile in dwarfs seems to have a core• Problem of physics or obs./sim.?• Baryonic matter dominatesin the Galactic centre• DM self-interactions, warm DM?

• Solutions:• GAIA satellite will measure movement of stars in our

Galaxy and in dwarf satellite galaxies!• N-body simulations become realistic (baryons, DM self)

07.01.2015 NORDITA Winer School 2015 36

Page 37: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

What is the Dark Matter?

07.01.2015 NORDITA Winer School 2015 37

Page 38: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

What is the DM mass scale?

07.01.2015 NORDITA Winer School 2015 38

• The SM does not haveviable cold DM candidate!• The SM neutrinos with Σ mi=0.1 eV contribute 0.2% of DM• The SM neutrinos arewarm DM

Whatever is DM, it couples to gravity via Tμν

Page 39: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Supermassive objects - MACHOs

07.01.2015 NORDITA Winer School 2015 39

Dead stars, planets etc., must be non-baryonic or created before BBN

Microlensing: MACHO fraction <20% for M=M

Page 40: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Primordial Black Holes (PBH)

07.01.2015 NORDITA Winer School 2015 40

Not predicted by standard cosmology because of small primordial perturbations

Page 41: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

DM as elementary particles

07.01.2015 NORDITA Winer School 2015 41

Page 42: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

DM as a thermal relic

07.01.2015 NORDITA Winer School 2015 42

Page 43: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

The WIMP miracle

07.01.2015 NORDITA Winer School 2015 43

This mass scale has nothing to do with EWSB

Page 44: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Warning – many alternatives possible

• DM stabilized by Z3 not Z2

semi-annihilations

• Freeze-in of very weakly coupled particle

very heavy DM possible

07.01.2015 NORDITA Winer School 2015 44

Page 45: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Asymmetric DM

07.01.2015 NORDITA Winer School 2015 45

• DM may be like proton

• The asymmetries in the baryon and DM sectors may be related

Scenarios contain dark forces and selfinteractions

Page 46: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Paradigm shift in WIMP DM physics

• Instead of Z2-stabilized one thermal relic (SUSY)– Dark sector can be as complicated as visible sector– Multi-component DM– Dark sector can contain dark forces• Dark photons• Dark Yukawa sector• Strong interactions in the dark sector – Dark Techicolor

– Dark Matter can form dark discs (10% of DM in our Galaxy) and/or affect large scale structure

07.01.2015 NORDITA Winer School 2015 46

Page 47: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

DM mass scale

07.01.2015 NORDITA Winer School 2015 47

Page 48: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Ultralight scalars: axion-like particles (ALPs)

• If scalar is light, its phase space density is high

Such a DM should be described as a field• To be viable DM, particles must be created at rest

07.01.2015 NORDITA Winer School 2015 48

Initial misalignment mechanism

Page 49: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

The QCD axion Pseudo-Goldstone boson of axial symmetry

07.01.2015 NORDITA Winer School 2015 49

Invented to explain the absence of strong CP violation

Axions solve the strong CP problem

Page 50: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

QCD axion couplingsCouples to gluons and photons due to mixing with the pion

where

Other possible interactions

1 MHz ≈ 4×10-9 eV

nucleon dipole moment d = gda

Page 51: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Detection principle

07.01.2015 NORDITA Winer School 2015 51

Look for axion-photon conversion• From cosmological sources• Create your own - laser

CAST

ADMXRes. microwave cavity

Page 52: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

07.01.2015 NORDITA Winer School 2015 52

Page 53: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Experiments: light-through a wall

• Photons „tunnel“ through a barrier via conversion to axions in a strong magnetic field

Page 54: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151
Page 55: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Nucleon electric dipole moment• Given that

– DM is a classical field a– that couples to nucleons as

• then all (local) nucleons will have a time dependent EDM (current bound |dn| < 2.9×10−26 e·cm)

• In the case of the QCD axion

(Molecular EDMs are about 28 orders of magnitude larger.)

Page 56: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

Expected CASPER sensitivity

Page 57: Dark Matter direct and indirect detection Martti Raidal NICPB, Tallinn, Estonia 07.01.2015NORDITA Winer School 20151

The message

New experiments are being planned to test light dark sector properties (APLs, dark photons etc.)

07.01.2015 NORDITA Winer School 2015 57