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Related papers: Confronting the Galactic 511 keV emission with $B-…

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The f\'eeton is the gauge boson of the $U(1)_{B-L}$ gauge theory. If the gauge coupling constant is extremely small, it becomes a candidate for dark matter. We show that its decay to a pair of electron and positron explains the observed…

High Energy Physics - Phenomenology · Physics 2024-05-13 Yu Cheng , Weikang Lin , Jie Sheng , Tsutomu T. Yanagida

The $U(1)_{B\textrm{--}L}$ symmetry, the essential component in the seesaw mechanism and leptogenesis, is naturally equipped with a massive gauge boson. If this gauge boson is the dark matter, the scenario consistent with the seesaw…

High Energy Physics - Phenomenology · Physics 2022-10-14 Weikang Lin , Luca Visinelli , Donglian Xu , Tsutomu T. Yanagida

In the type-I seesaw mechanism for neutrino masses, there exists a $B-L$ symmetry, whose breaking leads to the lepton number violating mass of the heavy Majorana neutrinos. This would imply the existence of a new neutral scalar associated…

High Energy Physics - Phenomenology · Physics 2018-02-16 P. S. Bhupal Dev , Rabindra N. Mohapatra , Yongchao Zhang

We show that a minimal local $B-L$ symmetry extension of the standard model can provide a unified description of both neutrino mass and dark matter. In our model, $B-L$ breaking is responsible for neutrino masses via the seesaw mechanism,…

High Energy Physics - Phenomenology · Physics 2020-07-01 Rabindra N. Mohapatra , Nobuchika Okada

If annihilating MeV-scale dark matter particles are responsible for the observed 511 keV emission from the Galactic bulge, then new light gauge bosons which mediate the dark matter annihilations may have other observable consequences. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 Dan Hooper

We propose a dynamical scoto-seesaw mechanism using a gauged $B-L$ symmetry. Dark matter is reconciled with neutrino mass generation, in such a way that the atmospheric scale arises \textit{a la seesaw}, while the solar scale is…

High Energy Physics - Phenomenology · Physics 2024-07-03 Julio Leite , Soumya Sadhukhan , José W. F. Valle

We show that spontaneous breaking of global $B-L$ symmetry responsible for small neutrino masses via the seesaw mechanism provides a unified picture of hybrid inflation and dark matter if the scale of $B-L$ breaking is close to the GUT…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Kazanas , R. N. Mohapatra , S. Nasri , V. L. Teplitz

We explore a mechanism of radiative B-L symmetry breaking in analogous to the radiative electroweak symmetry breaking. The breaking scale of B-L symmetry is related to the neutrino masses through the see-saw mechanism. Once we incorporate…

High Energy Physics - Phenomenology · Physics 2009-02-02 Tatsuru Kikuchi , Takayuki Kubo

We study a dynamical realization of the low-scale Inverse Seesaw mechanism in which the approximate $B-L$ symmetry is gauged and spontaneously broken. Anomaly cancellation requires additional chiral fermions, one of which becomes a stable…

We discuss phenomenology of the radiative seesaw model in which spontaneous breaking of the U(1)$_{B-L}$ gauge symmetry at the TeV scale gives the common origin for masses of neutrinos and dark matter (Kanemura et al., 2012). In this model,…

High Energy Physics - Phenomenology · Physics 2013-05-30 Shinya Kanemura , Takehiro Nabeshima , Hiroaki Sugiyama

We show that the canonical seesaw mechanism implemented by the $U(1)_{B-L}$ gauge symmetry provides two-component dark matter naturally. The seesaw scale that breaks $B-L$ defines a residual gauge symmetry to be $Z_6=Z_2\otimes Z_3$, where…

High Energy Physics - Phenomenology · Physics 2021-05-20 Phung Van Dong , Cao H. Nam , Duong Van Loi

We investigate the dark matter and the cosmological baryon asymmetry in a simple theory where baryon (B) and lepton (L) number are local gauge symmetries that are spontaneously broken. In this model, the cold dark matter candidate is the…

High Energy Physics - Phenomenology · Physics 2015-03-17 Timothy R. Dulaney , Pavel Fileviez Perez , Mark B. Wise

We propose a unified setup for dark matter, inflation and baryon asymmetry generation through the neutrino mass seesaw mechanism. Our scenario emerges naturally from an extended gauge group containing $B-L$ as a non-commutative symmetry,…

High Energy Physics - Phenomenology · Physics 2019-04-03 P. V. Dong , D. T. Huong , Daniel A. Camargo , Farinaldo S. Queiroz , José W. F. Valle

We provide a scenario in which a hidden U(1) gauge boson constitutes dark matter of the Universe and decays into the standard-model particles through a kinetic mixing with an $U(1)_{B-L}$ gauge boson. Interestingly, our model can naturally…

High Energy Physics - Phenomenology · Physics 2009-07-02 Chuan-Ren Chen , Fuminobu Takahashi , T. T. Yanagida

We explore a mechanism of radiative B-L symmetry breaking in analogous to the radiative electroweak symmetry breaking. The breaking scale of B-L symmetry is related to the neutrino masses through the see-saw mechanism. Once we incorporate…

High Energy Physics - Phenomenology · Physics 2008-11-26 Tatsuru Kikuchi , Takayuki Kubo

Recent observations indicate that a high production rate of positrons (strong 511 keV line) and a significant amount of excess GeV gamma-ray exist in our Galactic bulge. The latter issue can be explained by $\sim 40$ GeV dark matter…

High Energy Astrophysical Phenomena · Physics 2016-02-29 Man Ho Chan

Under a hypothesis of classically conformal theories, we investigate the minimal B-L extended Standard Model, which naturally provides the seesaw mechanism for explaining tiny neutrino masses. In this setup, the radiative gauge symmetry…

High Energy Physics - Phenomenology · Physics 2014-11-18 Satoshi Iso , Nobuchika Okada , Yuta Orikasa

In this paper I present the detail estimations for the width of the 511 keV line produced by a mechanism when dark matter is represented by macroscopically large dense nuggets. I argue that the width of 511 keV emission in this mechanism is…

Astrophysics · Physics 2008-11-26 Ariel Zhitnitsky

We argue that the gauge symmetry which includes SU(3)_L as a higher weak-isospin symmetry is manifestly given by SU(3)_C\otimes SU(3)_L\otimes U(1)_X\otimes U(1)_N, where the last two factors determine the electric charge and B-L,…

High Energy Physics - Phenomenology · Physics 2015-09-22 P. V. Dong

We explore dark matter mechanisms that can simultaneously explain the galactic 511 keV gamma rays observed by INTEGRAL/SPI, the DAMA/LIBRA annual modulation, and the excess of low-recoil dark matter candidates observed by CoGeNT. It…

High Energy Physics - Phenomenology · Physics 2011-08-16 James M. Cline , Andrew R. Frey , Fang Chen
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