Neutrinos and Dark Matter Alejandro Ibarra Technische Universitt - - PowerPoint PPT Presentation

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Neutrinos and Dark Matter Alejandro Ibarra Technische Universitt - - PowerPoint PPT Presentation

Neutrinos and Dark Matter Alejandro Ibarra Technische Universitt Mnchen Neutrino 2014 Boston 6 June 2014 Neutrinos and Dark Matter Outline: Neutrinos as dark matter Neutrinos from dark matter Neutrinos as dark matter Neutrinos as dark


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Neutrinos and Dark Matter

Alejandro Ibarra Technische Universität München

Neutrino 2014 Boston 6 June 2014

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Neutrinos and Dark Matter

Neutrinos as dark matter Neutrinos from dark matter

Outline:

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Non-relativistic Relativistic

White'86

Hot Dark Matter Cold Dark Matter

Neutrinos as dark matter Neutrinos as dark matter

The dark matter plays a central role in the formation of the first structures in our Universe

(neutrino dark matter)

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Non-relativistic Relativistic

White'86

Hot Dark Matter Cold Dark Matter

Neutrinos as dark matter Neutrinos as dark matter

(neutrino dark matter)

The dark matter plays a central role in the formation of the first structures in our Universe

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Neutrinos as dark matter Neutrinos as dark matter

The existence of dark rk matter constitutes an evidence for physics beyond the Standard Model

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Simplest scenario accounting for the dark matter of the Universe  One new particle, ns  Two new parameters: mDM, qas.  No new symmetries

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Simplest scenario accounting for the dark matter of the Universe  One new particle, ns  Two new parameters: mDM, qas.  No new symmetries

Five things to know about sterile neutrino dark matter

1 Sterile neutrinos can be produced in the early Universe via mixing na - ns.

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Simplest scenario accounting for the dark matter of the Universe  One new particle, ns  Two new parameters: mDM, qas.  No new symmetries

Five things to know about sterile neutrino dark matter

1 Sterile neutrinos can be produced in the early Universe via mixing na - ns. 2 Sterile neutrinos should not be overproduced  upper limit on the mixing angle as a function of the DM mass

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Simplest scenario accounting for the dark matter of the Universe  One new particle, ns  Two new parameters: mDM, qas.  No new symmetries

Five things to know about sterile neutrino dark matter

2 Sterile neutrinos should not be overproduced  upper limit on the mixing angle as a function of the DM mass 3 The existence of a lepton asymmetry can resonantly enhance the dark matter production, via the MSW mechanism. 1 Sterile neutrinos can be produced in the early Universe via mixing na - ns.

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

4 Sterile neutrinos are fermions and obey the exclusion principle. It is not possible to have an arbitrarily large ns number density. The observed DM density in dwarf galaxies implies a lower limit

  • n the DM mass.
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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

4 Sterile neutrinos are fermions and obey the exclusion principle. It is not possible to have an arbitrarily large ns number density. The observed DM density in dwarf galaxies implies a lower limit

  • n the DM mass.

5 Sterile neutrinos are not absolutely stable

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Abazajian et al. arXiv:1204.5379

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

2

Abazajian et al. arXiv:1204.5379

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

3 2

Abazajian et al. arXiv:1204.5379

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

3 4 2

Abazajian et al. arXiv:1204.5379

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

5 3 4 2

Abazajian et al. arXiv:1204.5379

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Recent hints for an unidentified X-ray line signal

Boyarsky al, 1402.4119 Bulbul et al, 1402.2301

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

3.53±0.025

Recent hints for an unidentified X-ray line signal

Boyarsky al, 1402.4119 Bulbul et al, 1402.2301

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Recent hints for an unidentified X-ray line signal

Boyarsky al, 1402.4119 Bulbul et al, 1402.2301

3.53±0.025

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Recent hints for an unidentified X-ray line signal

Boyarsky al, 1402.4119 Bulbul et al, 1402.2301

3.53±0.025

 Not observed in the deep “blank sky” dataset. Probably not instrumental.  Observed in different datasets at different redshifts.  Atomic origin not demonstrated: candidate atomic lines expected to be much fainter.

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Recent hints for an unidentified X-ray line signal

Boyarsky al, 1402.4119 Bulbul et al, 1402.2301

3.53±0.025

 Not observed in the deep “blank sky” dataset. Probably not instrumental.  Observed in different datasets at different redshifts.  Atomic origin not demonstrated: candidate atomic lines expected to be much fainter.  Originated by sterile neutrino decay?

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Sterile neutrinos as dark matter Sterile neutrinos as dark matter

Bulbul et al, 1402.2301 Boyarsky al, 1402.4119

The future Astro-H mission will hopefully clarify the nature of this line. Requires nL/s ~ 10-5 (compared to nB/s ~ 10-10 )

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Many pieces of evidence for particle dark matter. However, very little is known about the properties of the dark matter particle: Mass: 10-15 GeV  1015 GeV Interaction cross section with nucleons: 10-40 pb  10-5 pb Lifetime: 109 years  infinity Spin: 0 or 1/2 or 1 or 3/2 (or possibly higher if composite)

(axions) (WIMPzillas) (gravitinos) (neutralinos)

Annihilation cross section into SM particles: 10-40 pb  10-5 pb

(gravitinos) (neutralinos)

Neutrinos from dark matter Neutrinos from dark matter

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Many pieces of evidence for particle dark matter. However, very little is known about the properties of the dark matter particle: Mass: 10-15 GeV  1015 GeV Interaction cross section with nucleons: 10-40 pb  10-5 pb Lifetime: 109 years  infinity Spin: 0 or 1/2 or 1 or 3/2 (or possibly higher if composite)

(axions) (WIMPzillas) (gravitinos) (neutralinos)

Annihilation cross section into SM particles: 10-40 pb  10-5 pb

(gravitinos) (neutralinos)

Neutrinos from dark matter Neutrinos from dark matter

Cons nstrained by neutrino telescop

  • pes
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Limits on the annihilation cross-section Limits on the annihilation cross-section

Neutrinos from dark matter annihilations in the Milky Way halo

DM DM

g e-,e+ p, p n, n

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Limits on the annihilation cross-section Limits on the annihilation cross-section

Source term (particle physics) Line-of-sight integral (astrophysics)

Neutrinos from dark matter annihilations in the Milky Way halo

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50 100 150  deg 1 10 100 1000  ds 2,s

NFW Isothermal Moore Einasto

Limits on the annihilation cross-section Limits on the annihilation cross-section

Source term (particle physics) Line-of-sight integral (astrophysics)

Neutrinos from dark matter annihilations in the Milky Way halo

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Limits on the annihilation cross-section Limits on the annihilation cross-section

Source term (particle physics) Line-of-sight integral (astrophysics)

IceCube SuperK Neutrinos from dark matter annihilations in the Milky Way halo

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Mijakowski '13

Limits on the annihilation cross-section Limits on the annihilation cross-section

Neutrinos from dark matter annihilations in the Milky Way halo

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Limits on the annihilation cross-section Limits on the annihilation cross-section

IceCube collaboration. ICRC 2013

Neutrinos from dark matter annihilations in the Milky Way halo

(For the preliminary limits from ANTARES, see talk by J.J. Hernández-Rey)

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Aartsen et al., arXiv:1307.3473

Limits on the annihilation cross-section Limits on the annihilation cross-section

Neutrinos from dark matter annihilations in dwarf galaxies & galaxy clusters.

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Limits on the scattering cross-section Limits on the scattering cross-section

capture rate  DM,p

  • If the dark matter particles have a “sizable” interaction cross section

with ordinary matter, they can be captured inside the Sun (and inside the Earth).

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Limits on the scattering cross-section Limits on the scattering cross-section

  • DM particles captured inside the Sun can annihilate.
  • If the dark matter particles have a “sizable” interaction cross section

with ordinary matter, they can be captured inside the Sun (and inside the Earth).

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Limits on the scattering cross-section Limits on the scattering cross-section

n, n n, n n, n e+, g, p

  • If the dark matter particles have a “sizable” interaction cross section

with ordinary matter, they can be captured inside the Sun (and inside the Earth).

  • The annihilation produces a neutrino flux which might be detected in neutrino
  • bservatories. All other annihilation products (gammas, positrons, antiprotons...)

are absorbed before escaping the Sun.

  • DM particles captured inside the Sun can annihilate.

Neutrino flux related To the scattering cross-section

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IceCube Collaboration arXiv:1212.4097

Limits on the scattering cross-section Limits on the scattering cross-section

Limits on the spin-dependent and spin-independent scattering cross section

  • f dark matter particles with protons.

Super-Kamiokande limits from arXiv:1108.3384

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Limits on the scattering cross-section Limits on the scattering cross-section

Boliev et al. arXiv:1301.1138

Competitive limits from ANTARES and Baksan

ANTARES limits from arXiv:1212.2416

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Limits on the scattering cross-section Limits on the scattering cross-section

Limits on annihilations channels into light fermions. The annihilation DM DM → q q , with q a light quark, does not produce high energy neutrinos. The light quark produces pions which are quickly stopped in the solar interior before decaying. This annihilation channel produces only MeV neutrinos.

Bernal, Martín-Albo, Palomares-Ruiz, arXiv:1208.0834 See also Rott, Siegal-Gaskins, Beacom, arXiv:1208.0827

The MeV neutrinos could be detected at Super-Kamiokande

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Limits on the scattering cross-section Limits on the scattering cross-section

The higher order annihilations DM DM → q q Z or DM DM → Z Z do produce high energy neutrinos via the decay of the Z boson

AI, Totzauer, Wild, arXiv:1402.4375

Dirac dark matter Majorana/scalar dark matter

Limits on annihilations channels into light fermions.

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Limits on the dark matter lifetime Limits on the dark matter lifetime

DM

g e-,e+ p, p n, n

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Neutrinos from dark matter decay in the galactic halo

Source term (particle physics) Line-of-sight integral (astrophysics)

50 100 150  deg 1 10 100 1000  ds ,s

NFW Isothermal Moore Einasto

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Covi, Grefe, AI, Tran arXiv:0912.3521

Neutrinos from dark matter decay in the galactic halo

IceCube collaboration ArXiv:1101.3349

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Opening up the dark matter mass window...

mass

meV meV eV MeV GeV TeV PeV EeV ZeV WIMPs keV

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Opening up the dark matter mass window...

mass

meV meV eV MeV GeV TeV PeV EeV ZeV WIMPs keV

AMANDA IceCube -22 IceCube -40 Auger Anita

arXiv:0705.1315 arXiv:1202.4564 arXiv:1103.4250 arXiv:1202.1493 arXiv:1011.5004

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Esmaili, AI, Peres arXiv:1205.5281

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Decaying dark matter as the origin of the IceCube PeV neutrinos?

Esmaili, Serpico, arXiv:1308.1105 Feldstein et al, arXiv:1303.7320 IceCube Collaboration, arXiv:1304.5356

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Limits on the dark matter lifetime Limits on the dark matter lifetime

Esmaili, Serpico, arXiv:1308.1105 Feldstein et al, arXiv:1303.7320

Decaying dark matter as the origin of the IceCube PeV neutrinos?

IceCube Collaboration, arXiv:1405.5303

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Conclusions Conclusions

 The three known active neutrinos contribute to the energy-density of the Universe (approx. 0.3%), but cannot account for all the dark matter.  A simple extension of the SM accounting for the DM consists in introducing

  • ne sterile neutrino with mass ~ 1 – 50 keV. Strong limits on the model from

X-ray observations (and possible signals?).  The annihilation and decay of dark matter particles generically produce

  • neutrinos.  Limits on DM properties from neutrino telescopes.

 The limits are complementary to those from other experiments, although usually weaker. Except:

  • Annihilation cross section of WIMPs with mass few TeV – 100 TeV.
  • Spin-dependent scattering cross section WIMP-proton.
  • Lifetime of DM particles with mass few TeV – 1016 GeV.