Multicomponent dark matter particles in a two-loop neutrino model

We construct a loop induced seesaw model in a TeV scale theory with gauged U(1)B−L symmetry. Light neutrino masses are generated at two-loop level and right-handed neutrinos also obtain their masses by one-loop effect. Multi-component Dark Matters (DMs) are included in our model due to the remnant discrete symmetry after the B − L symmetry breaking and the Z2 parity which is originally imposed to the model. We investigate the multi-component DM properties, in which we have two fermionic DMs with different mass scales, O(10) GeV and O (100-1000) GeV. The former mass corresponds to the lightest right-handed neutrino mass induced by the loop effect, although the latter one to the SM gauge singlet fermion. We show each of the DM annihilation processes and compare to the observation of relic abundance, together with the constraints of Lepton Flavor Violation (LFV) and active neutrino masses. Moreover we show that our model has some parameter region allowed by the direct detection result reported by XENON100, and it is possible to search the region by the future XENON experiment.

[1]  P. Minkowski μ→eγ at a rate of one out of 109 muon decays? , 1977 .

[2]  G. Senjanovic,et al.  Neutrino Mass and Spontaneous Parity Nonconservation , 1980 .

[3]  José W. F. Valle,et al.  Neutrino masses in SU(2) ⊗ U(1) theories , 1980 .

[4]  J. Valle,et al.  Neutrino mass and baryon-number nonconservation in superstring models. , 1986, Physical review. D, Particles and fields.

[5]  J. Valle,et al.  Fast decaying neutrinos and observable flavour violation in a new class of Majoron models , 1989 .

[6]  A. Broeils,et al.  Extended rotation curves of spiral galaxies: dark haloes and modified dynamics , 1991 .

[7]  Takeuchi,et al.  Estimation of oblique electroweak corrections. , 1992, Physical review. D, Particles and fields.

[8]  P. Nāth,et al.  Gaugino mass nonuniversality and dark matter in supergravity, strings, and D-brane models , 2000, hep-ph/0003186.

[9]  Astronomy,et al.  A Model for neutrino masses and dark matter , 2002, hep-ph/0210389.

[10]  A. ADoefaa,et al.  ? ? ? ? f ? ? ? ? ? , 2003 .

[11]  Search for neutrino oscillations on a long base-line at the CHOOZ nuclear power station , 2003, hep-ex/0301017.

[12]  Ernest Ma Verifiable radiative seesaw mechanism of neutrino mass and dark matter , 2006 .

[13]  S. Khalil Low-scale B?L extension of the standard model , 2006, hep-ph/0611205.

[14]  R. Ellis,et al.  Dark matter maps reveal cosmic scaffolding , 2007, Nature.

[15]  U. Sarkar,et al.  Radiative seesaw in left-right symmetric model , 2008, 0807.0270.

[16]  S. Hashimoto,et al.  Nucleon sigma term and strange quark content from lattice QCD with exact chiral symmetry , 2008, 0806.4744.

[17]  U. Sarkar,et al.  Radiative Neutrino Mass, Dark Matter and Leptogenesis , 2007, 0712.2933.

[18]  Edward J. Wollack,et al.  FIVE-YEAR WILKINSON MICROWAVE ANISOTROPY PROBE * OBSERVATIONS: COSMOLOGICAL INTERPRETATION , 2008, 0803.0547.

[19]  J. Edsjo,et al.  Inert Doublet Model and LEP II Limits , 2008, 0810.3924.

[20]  S. Kanemura,et al.  Neutrino mass, dark matter, and Baryon asymmetry via TeV-scale physics without fine-tuning. , 2008, Physical review letters.

[21]  Spencer Chang,et al.  Magnetic Inelastic Dark Matter , 2010, 1007.4200.

[22]  An R-parity conserving radiative neutrino mass model without right-handed neutrinos , 2010 .

[23]  P. Belli,et al.  New results from DAMA/LIBRA , 2010, 1002.1028.

[24]  M. Lindner,et al.  Dark Matter and neutrino masses from global U (1) B - L symmetry breaking , 2011, 1105.4626.

[25]  Takashi Toma,et al.  Dark matter in the supersymmetric radiative seesaw model with an anomalous U(1) symmetry , 2010, 1011.2839.

[26]  Tejpreet Singh Golan,et al.  Indication of electron neutrino appearance from an accelerator-produced off-axis muon neutrino beam. , 2011, Physical review letters.

[27]  S. Kanemura,et al.  Masses of dark matter and neutrino from TeV scale spontaneous $U(1)_{B-L}$ breaking , 2011, 1101.5713.

[28]  J. C. Mitchell,et al.  Improved search for Muon-neutrino to electron-neutrino oscillations in MINOS. , 2011, Physical review letters.

[29]  Edward J. Wollack,et al.  FIVE-YEAR WILKINSON MICROWAVE ANISOTROPY PROBE OBSERVATIONS: COSMOLOGICAL INTERPRETATION , 2008, 0803.0547.

[30]  G. Drake,et al.  Results from a search for light-mass dark matter with a p-type point contact germanium detector. , 2010, Physical review letters.

[31]  Dark Matters in Gauged B-3L_i Model , 2012, 1212.0492.

[32]  L. Y. Wang,et al.  Observation of electron-antineutrino disappearance at Daya Bay. , 2012, Physical review letters.

[33]  J. A. Oller,et al.  The chiral representation of the $\pi N$ scattering amplitude and the pion-nucleon sigma term , 2011, 1110.3797.

[34]  M. Aoki,et al.  Impact of inert higgsino dark matter , 2011, 1110.5403.

[35]  S. Kanemura,et al.  TeV-Scale Seesaw with Loop-Induced Dirac Mass Term and Dark Matter from $U(1)_{B-L}$ Gauge Symmetry Breaking , 2011, 1111.0599.

[36]  D. Hauff,et al.  Results from 730 kg days of the CRESST-II Dark Matter search , 2011, 1109.0702.

[37]  I. G. Park,et al.  Observation of reactor electron antineutrinos disappearance in the RENO experiment. , 2012, Physical review letters.

[38]  A. Rashed,et al.  SCOTOGENIC A4 NEUTRINO MODEL FOR NONZERO θ13 AND LARGE δCP , 2012, 1206.1570.

[39]  M. Hirsch,et al.  Systematic study of the d = 5 Weinberg operator at one-loop order , 2012, 1204.5862.

[40]  K. Kumerički,et al.  Critique of fermionic RνMDM and its scalar variants , 2012, 1204.6597.

[41]  E. Ma Radiative scaling neutrino mass and warm dark matter , 2012, 1206.1812.

[42]  Alam,et al.  Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in pp collisions at √s = 7 TeV , 2012 .

[43]  E Aprile,et al.  Dark matter results from 225 live days of XENON100 data. , 2012, Physical review letters.

[44]  H. Okada,et al.  Fermionic dark matter in radiative inverse seesaw model with U(1) B-L , 2012, 1207.0864.

[45]  M. Baak,et al.  The electroweak fit of the standard model after the discovery of a new boson at the LHC , 2012, The European Physical Journal C.

[46]  Y. Farzan,et al.  Dirac neutrino mass generation from dark matter , 2012, 1204.4890.

[47]  A. Merle,et al.  Running of radiative neutrino masses: the scotogenic model , 2012, 1205.0008.

[48]  P. S. Bhupal Dev,et al.  Minimal Radiative Neutrino Mass Mechanism for Inverse Seesaw Models , 2012, 1209.4051.

[49]  K. Kumerički,et al.  TeV-scale seesaw mechanism with quintuplet fermions , 2012, 1204.6599.

[50]  T. Schwetz,et al.  Direct Detection of Leptophilic Dark Matter in a Model with Radiative Neutrino Masses , 2012, 1201.0906.

[51]  H. Okada,et al.  Light dark matter candidate in B–L gauged radiative inverse seesaw , 2012, 1210.2305.

[52]  M. Krawczyk,et al.  Inert Dark Matter and Strong Electroweak Phase Transition , 2012, 1207.0084.

[53]  H. Okada,et al.  Non-zero $\theta_{13}$ linking to Dark Matter from Non-Abelian Discrete Flavor Model in Radiative Seesaw , 2012, 1201.4436.

[54]  Y. Farzan,et al.  Scotogenic Dirac Neutrino Mass , 2012 .

[55]  K. L. McDonald,et al.  The Simplest Models of Radiative Neutrino Mass: Excluding Simplified Zee Models and Beyond , 2013, 1303.6384.

[56]  K. Yagyu,et al.  Two-loop radiative seesaw model with inert triplet scalar field , 2013, 1303.3463.

[57]  A. K. Soma,et al.  Limits on spin-independent couplings of WIMP dark matter with a p-type point-contact germanium detector. , 2013, Physical review letters.

[58]  A. Ibarra,et al.  A radiative model with a naturally mild neutrino mass hierarchy , 2012, 1208.3162.

[59]  R. Nardo,et al.  New constraint on the existence of the μ+ → e+ γ decay. , 2013, Physical review letters.

[60]  Michael Gustafsson,et al.  Predictive model for radiatively induced neutrino masses and mixings with dark matter. , 2012, Physical review letters.

[61]  Peihong Gu Mirror symmetry: from active and sterile neutrino masses to baryonic and dark matter asymmetries , 2013, 1303.6545.

[62]  Hiroshi Takano,et al.  Two-loop radiative seesaw mechanism with multicomponent dark matter explaining the possible γ excess in the Higgs boson decay and at the Fermi LAT , 2013, 1302.3936.

[63]  C. A. Oxborrow,et al.  Planck 2013 results. XVI. Cosmological parameters , 2013, 1303.5076.