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Related papers: Leptonic Dark Matter with Scalar Dilepton Mediator

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We examine the phenomenology of a simplified model of fermionic dark matter coupled to a light scalar mediator carrying lepton number 2. We find that the mediator can be very light and still consistent with laboratory and cosmological…

High Energy Physics - Phenomenology · Physics 2020-06-29 Arvind Rajaraman , Jordan Smolinsky

A simple scenario of long-lived dark matter is presented. Assuming lepton number $(L)$ conservation with Dirac neutrinos, the neutral component of an $SU(2)_L$ scalar triplet with $L=2$ is a suitable candidate, which decays to two…

High Energy Physics - Phenomenology · Physics 2021-02-24 Ernest Ma

The cold dark matter (CDM) candidate with weakly interacting massive particles can successfully explain the observed dark matter relic density in cosmic scale and the large-scale structure of the Universe. However, a number of observations…

High Energy Physics - Phenomenology · Physics 2021-04-07 Chung Kao , Yue-Lin Sming Tsai , Gwo-Guang Wong

A Dirac fermion carrying an integral weak isospin and the vanishing hypercharge is considered as its neutral component can be a promising dark matter candidate (called the minimal dark matter) whose mass is of order 100 GeV. While the…

High Energy Physics - Phenomenology · Physics 2011-07-18 Eung Jin Chun

In the singlet-triplet majoron model of neutrino mass, lepton number is spontaneously broken. If it is also softly broken, then a naturally light pseudoscalar particle $\eta_I$ exists. It may then act as a light mediator for a real singlet…

High Energy Physics - Phenomenology · Physics 2017-09-13 Ernest Ma , Markos Maniatis

The notion of U(1) lepton number (which may only be softly broken) is applied to models of dark matter which interacts with leptons. Previous scotogenic models of Majorana or Dirac neutrino mass are shown to be derivable in this framework…

High Energy Physics - Phenomenology · Physics 2020-09-02 Ernest Ma

The light mediator scenario of self-interacting dark matter is strongly constrained in many ways. After summarizing the various constraints, we discuss minimal options and models which allow to nevertheless satisfy all these constraints.…

High Energy Physics - Phenomenology · Physics 2020-05-07 Thomas Hambye , Laurent Vanderheyden

We explore a gauged $U(1)_{B-L}$ extension of standard model with inclusion of three right-handed neutrinos of exotic $B-L$ charges to cancel the gauge anomaly. Non-trivial transformation of new particles under $B-L$ symmetry forbids the…

High Energy Physics - Phenomenology · Physics 2022-07-13 Subhasmita Mishra , Nimmala Narendra , Prafulla Kumar Panda , Nirakar Sahoo

Lepton number is promoted to an $U(1)_L$ gauge symmetry in a simple extension of the standard model. The spontaneous breaking of $U(1)_L$ by three units allows a conserved $Z_3^L$ lepton symmetry to remain, guaranteeing that neutrinos are…

High Energy Physics - Phenomenology · Physics 2021-06-02 Ernest Ma

In the context of $SO(10) \to SU(5) \times U(1)_\chi$, it is shown how seesaw Dirac neutrinos may be obtained. In this framework, $U(1)$ lepton number is conserved, with which self-interaction dark matter with a light scalar dilepton…

High Energy Physics - Phenomenology · Physics 2019-01-08 Ernest Ma

The standard model of quarks and leptons is extended to include the gauge symmetry $U(1)_\chi$ which comes from $SO(10) \to SU(5) \times U(1)_\chi$. The radiative generation of Dirac neutrino masses through dark matter is discussed in two…

High Energy Physics - Phenomenology · Physics 2019-05-08 Ernest Ma

We study the influence of leptophilic dark matter interactions on decays of muons and ground state mesons in existing experiments. We consider a secluded dark sector exclusively interacting with leptons via either a (leptophilic) scalar or…

High Energy Physics - Phenomenology · Physics 2023-01-18 Gerrit Bickendorf , Manuel Drees

We investigate a simple model where Lepton number is promoted to a local $U(1)_L$ gauge symmetry which is then spontaneously broken, leading to a viable thermal DM candidate and vector-like leptons as a byproduct. The dark matter arises as…

High Energy Physics - Phenomenology · Physics 2015-06-15 Pedro Schwaller , Tim M. P. Tait , Roberto Vega-Morales

A light fermionic weakly interacting massive particle (WIMP) dark matter is investigated by studying its minimal renormalizable model, where it requires a scalar mediator to have an interaction between the WIMP and standard model particles.…

High Energy Physics - Phenomenology · Physics 2019-09-04 Shigeki Matsumoto , Yue-Lin Sming Tsai , Po-Yan Tseng

A new understanding of the stability of self-interacting dark matter is pointed out, based on the simplest spontaneously broken Abelian $U(1)$ gauge model with one complex scalar and one Dirac fermion. The key is the imposition of dark…

High Energy Physics - Phenomenology · Physics 2017-08-23 Ernest Ma

In the context of a simplified leptophilic Dark Matter (DM) scenario where the mediator is a new charged fermion carrying leptonic quantum number and the DM candidate is either scalar or vector, the complementarity of different bounds is…

High Energy Physics - Phenomenology · Physics 2018-04-11 D. Barducci , A. Deandrea , S. Moretti , L. Panizzi , H. Prager

We consider a fermionic dark matter candidate interacting via a scalar mediator coupled with the Standard Model through a Higgs portal. We consider general setting including both scalar and pseudoscalar interactions between the scalar and…

High Energy Physics - Phenomenology · Physics 2017-04-12 Kimmo Kainulainen , Kimmo Tuominen , Ville Vaskonen

In this paper, we put forward a connection between the self-interacting dark matter and the Dirac nature of neutrinos. Our exploration involves a $Z_4 \otimes Z_4'$ discrete symmetry, wherein the Dirac neutrino mass is produced through a…

High Energy Physics - Phenomenology · Physics 2024-03-05 Satyabrata Mahapatra , Sujit Kumar Sahoo , Narendra Sahu , Vicky Singh Thounaojam

We consider the singlet Majoron model with softly broken lepton number. This model contains three right-handed neutrinos and a singlet scalar besides the standard model fields. The real part of the singlet scalar develops a vacuum…

High Energy Physics - Phenomenology · Physics 2014-11-20 Pei-Hong Gu , Ernest Ma , Utpal Sarkar

Choosing how gauge $U(1)_\chi$ breaks in the context of $SO(10) \to SU(5) \times U(1)_\chi$, $Z_4$ lepton number may be obtained which maintains neutrinos as Dirac fermions. Choosing $\Delta(27)$ as the family symmetry of leptons,…

High Energy Physics - Phenomenology · Physics 2019-10-02 Ernest Ma
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