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Multi-Component DM System and Their Observation Prospects. arXiv:1207.3318. by Jisuke Kubo, Kanazawa University(KU). in collaboration with Mayumi Aoki (KU&MPI,Heidelberg) Michael Duerr (MPI,Heidelberg) Hiroshi Takano(KU). Our Universe. Do you believe there exists only one kind of DM?.
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Multi-Component DM System and Their Observation Prospects arXiv:1207.3318 by Jisuke Kubo, Kanazawa University(KU) in collaboration with Mayumi Aoki (KU&MPI,Heidelberg) Michael Duerr (MPI,Heidelberg) Hiroshi Takano(KU)
Our Universe Do you believe there exists only one kind of DM? 3 Neutrinos as hot DM ~1.3%
How does a multi-component DM emerge? [1] Boehm, Fayet+Silk,03, two R parities in N=2 SUSY to explain gamma rays of two different scales from our galaxy. [2] Hur, Lee+Nasri,07, SUSY x U(1) to soften the mu problem where U(1) -> Z2. [3] Cao, Ma, Wukuda+Yuan,07, R x Z2 to relax the MSSM parameter space. etc etc
Radiative Seesaw coupled with mSUGRRA Aoki, Okawa, Takano+Kubo,11 cold DM candidates (R x Z2) Neutralino Inert Higgsino Inert Higgs RHD sneutrino RHD neutrino LHD sneutrino We assume: DM=
CMSSM Higgsino like gaugino mass Bino like soft scalar mass mSUGRA+Radiative seesaw =>R x Z2 Bino like LHC Aoki,Okawa,Takano+Kubo,2011
PLAN 1 Non-standard annihilations and relic abundance 2 Radiative See Saw and DMs 3 Indirect search of DM at Neutrino Telescopes 4 Conclusion
1 Non-standard annihilations and relic abundance standard conversion semi-annihilation
Coupled Boltzmann eqs. see also:D‘Eramo+Thaler, 11,Belanger,Kannike, Pukov+Raidal,12 XX standard conversion X semi-annihilation
A fictive model of 3-comp. DM system standard conversion semi- annihilation
standard: Temperature evolution only standard standard+ conversion
standard: Temperature evolution only standard standard+ semi-annihilation
Small size area zoomed. Conversion Semi-annihilation
2 Radiative See Saw and DMs Radiative Neutrino Mass Generation (Zee,‘80;86; Wolfenstein,80; Babu,88, etc) Radiative See Saw (Kraus, Nasri + Trodden,02; Ma,06; Aoki, Kanemura+ Seto,08; etc) Unbroken Z2: NR, Inert Higgs, DM
Z2-odd One-loop See-Saw with an unbroken Z2 Ma, 06 Inert SU(2) doublet Higgs NR and eta are DM candidates.
NR DM studied by Kraus, Nasri and Trodden,02; Kubo, Ma, Suematsu, ’06, etc CDM eta DM studied by Barbieri, Hall and Rychkov, '06; Lopez, Oliver and Tytgat,’06; Dolle and Su,’09 etc Promotion of Z2 to Z2 x Z2 by Aoki, Duerr, Kubo and Tankano, 12 Promotion to a three component DM system
, Radiative see-saw (Ma)+ Majorana + Scalar with Conversion CDM candidates Semi-annihilation We assume :DM=
Model with only was studied by Relic abundance Lopez, Oliver and Tytgat,’06 Only low mass and higher mass regimes are allowed.
total WMAP
Dependence of total WMAP
Including all the constraints: Without and : Dolle and Su,’09 DD DS PB For LEP VEV
With and : For
3 Indirect search of DMs at Neutrino Telescopes DM can be captured and annihilated in the Sun producing neutrinos that escape from the Sun DM diffuse DM DM
Change of the DM number: 2 Fixed point at C=CA N =>equilibrium => maxi. rate 2X annihilation rate Capture rate Annihilation rate rate Only diffuse in the MSSM. N time normalized to
Three component DM Semi-annihilation monochromatic Time Evolution of the numbers of DM in the Sun
Time evolution diffuse fixed point monochromatic Annihilation rates Input: etc
/sec Limits from Neutrino telescopes: IceCube(AMANDA) ANTARES SUPER-K /sec 0.05 events per year at Ice Cube
4 Conclusion Non-standard annihilations of DM can be very important, not only in calculating the relic abundance of DM, but also in indirect observation of DM. Especially, an observation of monochromatic neutrinos from the Sun may indicate multi-component DM in the Universe.