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Dark Matter Alejandro Ibarra Technische Universität München Summer School on Particle Physics ICTP, Trieste June 2013
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Page 1: Dark Matter - ICTP

Dark MatterAlejandro Ibarra

Technische Universität München

Summer School on Particle PhysicsICTP, TriesteJune 2013

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Outline

Lecture 1: Evidence for dark matter.

Lecture 2: Dark matter production.

Lecture 3: Indirect dark matter detection.

Lecture 4: Direct dark matter detection. Collider searches.

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Main results from the previous lecture

SM

SM

DM

DM

annihilation

production

scat

teri

ng

WIMP dark matter

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Main results from the previous lecture

SM

SM

DM

DM

annihilation

production

scat

teri

ng

WIMP dark matter

~ weak interaction

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Main results from the previous lecture

WIMP dark matter

SM

SM

DM

DM

annihilation

scat

teri

ng

Relic abundance of DM particles

Correct relic density if

production

~ weak interaction

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Main results from the previous lecture

SM

SM

DM

DM

annihilation

scat

teri

ng

Relic abundance of DM particles

Correct relic density if

(provided )

WIMP dark matter

production

~ weak interaction

DM

DM

Z0SM

SM

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Fifteen years ago...Cosmic antiprotons Collider experiments

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TodayCosmic antiprotons Collider experiments

Beam energy: 4000 GeVIntegrated luminosity: 23.26 fb-1

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End of this decadeCosmic antiprotons Collider experiments

Beam energy: 6500 GeVIntegrated luminosity: 500 fb-1

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Dark matter distribution

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The universe at T~1 GeV

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200 million years after the Big Bang

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Distance Sun to Earth ~ 8.5 kpc

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Density distribution of dark matter particles:

Assume spherical symmetry (in a first approximation).

Radial distribution:

NFW

Isothermal

Moore

Einasto

Normalized such that the local DM density is r(r=8.5 kpc) = 0.38 GeV/cm3

NFW, Isothermal, Moore

Einasto

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General idea:1) Dark matter particles annihilate or decay producing a flux of stable particles: photons, electrons, protons, positrons, antiprotons or (anti-)neutrinos.

DM

DM

DM

Indirect dark matter searches

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Indirect dark matter searchesGeneral idea:1) Dark matter particles annihilate or decay producing a flux of stable particles: photons, electrons, protons, positrons, antiprotons or (anti-)neutrinos.

2) These particles propagate through the galaxy and through theSolar System. Some of them will reach the Earth.

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General idea:1) Dark matter particles annihilate or decay producing a flux of stable particles: photons, electrons, protons, positrons, antiprotons or (anti-)neutrinos.

3) The products of the dark matter annihilations or decays are detectedtogether with other particles produced in astrophysical processes (for example, cosmic ray collisions with nuclei of the interstellar medium).The existence of dark matter can then be inferred if there is a significant excess in the fluxes compared to the expected astrophysical backgrounds.

Indirect dark matter searches

2) These particles propagate through the galaxy and through theSolar System. Some of them will reach the Earth.

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General idea:1) Dark matter particles annihilate or decay producing a flux of stable particles: photons, electrons, protons, positrons, antiprotons or (anti-)neutrinos.

3) The products of the dark matter annihilations or decays are detectedtogether with other particles produced in astrophysical processes (for example, cosmic ray collisions with nuclei of the interstellar medium).The existence of dark matter can then be inferred if there is a significant excess in the fluxes compared to the expected astrophysical backgrounds.

Indirect dark matter searches

2) These particles propagate through the galaxy and through theSolar System. Some of them will reach the Earth.

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Indirect dark matter searchesAntimatter

Gamma-rays

Neutrinos

Production

Propagation

Detection

of

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AntimatterAntimatter

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The production is described by the source function: number of particles produced at a given position per unit volume, unit time and unit energy.

ProductionProduction

DM

DM

DM

Annihilationrate r2

Decayrate r

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PropagationPropagation

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PropagationPropagation

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Propagation

h=100 pc

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Propagation

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PropagationR = 20 kpc

L=1-15 kpc

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Propagation

xy

zR = 20 kpc

L=1-15 kpc

f : number density of antiparticles per unit kinetic energy

interstellar antimatter flux:

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Propagation

xy

zR = 20 kpc

L=1-15 kpc

Source term

dark matter annihilation

dark matter decay

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Propagation

xy

zR = 20 kpc

L=1-15 kpc

Source term

dark matter annihilation

dark matter decay

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Propagation

xy

zR = 20 kpc

L=1-15 kpc

Source term

dark matter annihilation

dark matter decay

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Negligible for positrons. For antiprotons,

Propagation

xy

z

Annihilation term

Tan, Ng

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Propagation

xy

z

Convection term ● Due to the Milky Way galactic wind. ● It drifts particles away from the Galactic disk. ● Difficult to model. Assume:

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● Due to inverse Compton scattering on the interstellar radiation field (starlight, thermal radiation of dust, CMB)and synchrotron radiation.● Negligible for antiprotons and antideuterons● Can be modelled

Propagation

xy

z

Energy loss term

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● Energy loss due to Inverse Compton scattering: e+g e+g

Porter et al.

ge= Ee/me Lorentz factor.

Ge=4 ge e/me

q=Eg/G(Ee-Eg)

sT=0.67 barn Compton scattering cross section in the Thomson limit.

Number density of photons in ISRF

● Energy loss due to synchrotron radiation:

Approximately

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● Energy loss due to Inverse Compton scattering: e+g e+g

Porter et al.

ge= Ee/me Lorentz factor.

Ge=4 ge e/me

q=Eg/G(Ee-Eg)

sT=0.67 barn Compton scattering cross section in the Thomson limit.

Number density of photons in ISRF

● Energy loss due to synchrotron radiation:

Approximately

Not very well known,though...

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xy

z

Diffusion term● Due to the tangled magnetic field of the Galaxy.● Difficult to model. Assume

b = velocity = rigidity

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Maurin, Donato, Taillet, Salati '01

K0, , Vc

(as well as L) must be determined with measurementsof other cosmic ray species (mainly B/C ratio).

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Propagation inside the Solar System

solar modulation parameter

F=500 MV 1.3 GV

In the “force field approximation”,the flux at the top of the atmosphere (TOA)is related to the interstellar flux (IS) by

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Gast, Schael '09

Cosmic ray proton spectrum as measured by BESS, AMS-01 and PAMELA

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PAMELA collaborationarXiv:1007.0821

Experimental results: antiprotons

Fairly good agreement between the measurements and the theoretical predictions from collisions of cosmic rays on the interstellar medium p p → p X

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Expectations from theory

A concrete example in the minimal supersymmetric standard model.TeV 10-26 cm3s-1

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Expectations from theory

A concrete example in the minimal supersymmetric standard model.TeV 10-26 cm3s-1

sv = 3 10-26 cm3s-1

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Expectations from theory

A concrete example in the minimal supersymmetric standard model.TeV 10-26 cm3s-1

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Expectations from theory

A concrete example in the minimal supersymmetric standard model.TeV 10-26 cm3s-1

Annihilation rate “boosted”!

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Experimental results: positrons

Expected from “secondary production”,namely collisions of cosmic rays on theinterstellar medium (p p → e+ X).

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Experimental results: positrons

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Experimental results: positrons

PAMELA coll.arXiv:0810.4995

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Experimental results: positrons

AMS-02 coll.Phys.Rev.Lett. 110 (2013) 14, 141102

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More puzzles: the electron+positron flux

Abdo et al.ArXiv:0905.0025

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Present situation:

Evidence for a primary component of positrons (possibly accompanied by electrons)

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Cholis et al.arXiv:0811.3641

An electron/positron excess could arise from dark matter annihilations ...

Dark matter interpretation

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… or dark matter decays

“Democratic” decay n

Ibarra, Tran, Weniger

mDM=2500 GeV

mDM=600 GeV

AI, Tran, WenigerarXiv:0906.1571

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sv = 3 10-26 cm3s-1

Is this the first non-gravitational evidence of dark matter?

“Extraordinary claims require extraordinary evidence” Carl Sagan

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Beware of backgrounds!

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Pulsars Pulsars areare sources sources of high energy of high energy electrons electrons && positrons positrons

Atoyan, Aharonian, Völk;Chi, Cheng, Young;Grimani

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Pulsar explanation I: Geminga + Monogem

Monogem (B0656+14)Geminga

T=370 000 yearsD=157 pc

T=110 000 yearsD=290 pc

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Nice agreement. However, it is not a prediction!● dN

e/dE

e E

e

-1.7 exp(-Ee/1100 GeV)

● Energy output in e+e- pairs: 40% of the spin-down rate

Pulsar explanation I: Geminga + Monogem Grasso et al.

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● dNe/dE

e E

e

-a exp(-Ee/E

0), 1.5 < a < 1.9, 800 GeV < E

0 < 1400 GeV

● Energy output in e+e- pairs: between 10-30% of the spin-down rate

Pulsar explanation II: Multiple pulsars Grasso et al.

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The origin of the positron excess is still unclear:

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The origin of the positron excess is still unclear:

Dark matter? Probably not.

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The origin of the positron excess is still unclear:

Dark matter? Probably not.

Pulsars? Perhaps yes.

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The origin of the positron excess is still unclear:

Dark matter? Probably not.

Pulsars? Perhaps yes.

Something else? Perhaps yes.


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