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We propose a new motivation for the stability of dark matter (DM). We suggest that the same non-abelian discrete flavor symmetry which accounts for the observed pattern of neutrino oscillations, spontaneously breaks to a Z2 subgroup which…

High Energy Physics - Phenomenology · Physics 2010-12-24 M. Hirsch , S. Morisi , E. Peinado , J. W. F. Valle

Multiple cosmological observations hint at neutrino self-interactions beyond the Standard Model, yet such interactions face severe constraints from terrestrial experiments. We resolve this tension by introducing a model where active…

High Energy Physics - Phenomenology · Physics 2026-04-03 Anirban Das , P. S. Bhupal Dev , Christina Gao , Subhajit Ghosh , Taegyun Kim

We examine simple extension of the standard model with a pair of fermions, one singlet and a doublet, in a common thread linking the dark matter problem with the smallness of neutrino masses associated with several exciting features. In the…

High Energy Physics - Phenomenology · Physics 2020-07-28 Partha Konar , Ananya Mukherjee , Abhijit Kumar Saha , Sudipta Show

Dirac leptogenesis, in which neutrinos are purely Dirac and develop small but nonzero effective masses without the aid of the see-saw mechanism, provides an interesting alternative to the standard leptogenesis picture. Here we review the…

High Energy Physics - Phenomenology · Physics 2007-12-27 Brooks Thomas

Dark matter self-interactions have important implications for the distributions of dark matter in the Universe, from dwarf galaxies to galaxy clusters. We present benchmark models that illustrate characteristic features of dark matter that…

High Energy Physics - Phenomenology · Physics 2013-10-25 Manoj Kaplinghat , Sean Tulin , Hai-Bo Yu

We propose a simple radiative neutrino mass scenario with a Dirac dark matter candidate, which is minimally realized by a Z3 symmetry. We introduce two Dirac neutrinos and two inert doublets. We demonstrate that the model has a large…

High Energy Physics - Phenomenology · Physics 2020-11-03 Hiroshi Okada , Yutaro Shoji

Dark matter (DM) is usually assumed to be stabilized by a symmetry, which is mostly considered to be $Z_2$. For example, in supersymmetry it is $R$ parity, i.e. $(-1)^{3B+L+2j}$. However, it may be $Z_n$ or $U(1)_D$, and derivable from…

High Energy Physics - Phenomenology · Physics 2020-04-28 Ernest Ma

Sterile neutrinos only interact with the Standard Model through the neutrino sector, and thus represent a simple dark matter (DM) candidate with many potential astrophysical and cosmological signatures. Recently, sterile neutrinos produced…

Cosmology and Nongalactic Astrophysics · Physics 2023-11-16 Rui An , Vera Gluscevic , Ethan O. Nadler , Yue Zhang

Neutral vectorlike fermion as inspired by unified theories might become quasi-Dirac states at TeV due to a violation in lepton-like symmetry. It is shown that such quasi-Dirac fermions can properly achieve radiative neutrino mass generation…

High Energy Physics - Phenomenology · Physics 2026-03-16 Nguyen Thi Nguyet Nga , Nguyen Huy Thao , Phung Van Dong

In 2006, a simple extension of the Standard Model was proposed in which neutrinos obtain radiative Majorana masses at one-loop level from their couplings with dark matter, hence the term "scotogenic," from the Greek "scotos" meaning…

High Energy Physics - Phenomenology · Physics 2013-05-30 Yasaman Farzan , Ernest Ma

We study a model of neutrino and dark matter within the framework of a minimal extended seesaw. This framework is based on $A_4$ flavor symmetry along with the discrete $Z_4$ symmetry to stabilize the dark matter and construct desired mass…

High Energy Physics - Phenomenology · Physics 2020-04-22 Pritam Das , Mrinal Kumar Das , Najimuddin Khan

We propose the first scotogenic neutrino mass model with gauged lepton number $U(1)_L$, which is spontaneously broken by three units $\Delta L=3$ down to a residual discrete gauge symmetry $\mathbb{Z}_6$. The latter guarantees that…

High Energy Physics - Phenomenology · Physics 2026-03-27 A. E. Cárcamo Hernández , Andrés Enríquez , Sergey Kovalenko , Eduardo Peinado , Carlos A. Vaquera-Araujo

Self-interacting dark matter resolves the issue of cuspy profiles that appear in non-interacting cold dark matter simluations; it may additionally resolve the so-called "too big to fail" problem in structure formation. Asymmetric dark…

High Energy Physics - Phenomenology · Physics 2013-07-05 Lauren Pearce , Alexander Kusenko

Unexplored interactions of neutrinos could be the key to understanding the nature of the dark matter (DM). In particular, active neutrinos with new self-interactions can produce keV-mass sterile neutrinos that account for the whole of the…

High Energy Physics - Phenomenology · Physics 2022-09-21 Carlos Chichiri , Graciela B. Gelmini , Philip Lu , Volodymyr Takhistov

keV scale sterile neutrinos are excellent warm dark matter candidates. In the early Universe, these can be produced from oscillations and scatterings of active neutrinos. However, in the absence of any new physics, this mechanism is in…

High Energy Physics - Phenomenology · Physics 2022-03-02 Manibrata Sen

Neutrinos and dark matter (DM) are two of the least understood components of the Universe, yet both play crucial roles in cosmic evolution. Clues about their fundamental properties may emerge from discrepancies in cosmological measurements…

Cosmology and Nongalactic Astrophysics · Physics 2026-01-12 Lei Zu , William Giarè , Chi Zhang , Eleonora Di Valentino , Yue-Lin Sming Tsai , Sebastian Trojanowski

We present models of resonant self-interacting dark matter in a dark sector with QCD, based on analogies to the meson spectra in Standard Model QCD. For dark mesons made of two light quarks, we present a simple model that realizes resonant…

High Energy Physics - Phenomenology · Physics 2022-10-11 Yu-Dai Tsai , Robert McGehee , Hitoshi Murayama

We propose the first viable radiative seesaw model, in which the neutrino masses are induced radiatively via the two-loop Feynman diagram involving Strongly Interacting Massive Particles (SIMP). The stability of SIMP dark matter (DM) is…

High Energy Physics - Phenomenology · Physics 2017-07-28 Shu-Yu Ho , Takashi Toma , Koji Tsumura

The $SU(3)_c^{}\times SU(2)_L^{} \times U(1)_Y^{}$ standard model is extended by a $U(1)_{B-L}^{}$ gauge symmetry with four right-handed neutrinos. Because of their Yukawa couplings to a Higgs singlet for spontaneously breaking the…

High Energy Physics - Phenomenology · Physics 2025-08-21 Pei-Hong Gu

We analyze a model with unbroken B-L gauge symmetry where neutrino masses are generated at one loop, after spontaneous breaking of a global U(1) symmetry. These symmetries ensure dark matter stability and the Diracness of neutrinos. Within…

High Energy Physics - Phenomenology · Physics 2021-05-14 Carlos Alvarado , Cesar Bonilla , Julio Leite , José W. F. Valle