Multicomponent dark matter particles in a two-loop neutrino model
暂无分享,去创建一个
[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.