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The extension of the Standard model (SM) with three heavy right handed neutrinos, a complex scalar and the gauged $U(1)_{\rm B-L}$ symmetry (the minimal $B-L$ model) is considered the most compelling minimal one: the presence and the…

High Energy Physics - Phenomenology · Physics 2021-01-19 Gongjun Choi , Tsutomu T. Yanagida , Norimi Yokozaki

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

We investigate the phenomenology of singlet scalar dark matter in a simple $B-L$ gauge extension of the Standard Model where the dark matter particle is charged under the $U(1)_{B-L}$ symmetry. The non-trivial gauge anomalies are cancelled…

High Energy Physics - Phenomenology · Physics 2021-01-12 Shivaramakrishna Singirala , Rukmani Mohanta , Sudhanwa Patra

A possibility of explaining the anomalies in the semileptonic $B$-meson decay $B \to K^{*} \mu \bar\mu$ has been explored in the framework of the gauged $U(1)_{\mu-\tau}$ symmetry. Apart from the muon anomalous magnetic moment and neutrino…

High Energy Physics - Phenomenology · Physics 2019-04-03 Parada T. P. Hutauruk , Takaaki Nomura , Hiroshi Okada , Yuta Orikasa

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 scalar dark matter model featuring a hidden gauge symmetry, denoted as U(1)_X, with two complex scalars, Phi and S. In this framework, Phi spontaneously breaks the U(1)_X gauge symmetry, while S serves as a viable dark matter…

High Energy Physics - Phenomenology · Physics 2025-05-20 Yu-Hang Su , Chengfeng Cai , Yu-Pan Zeng , Hong-Hao Zhang

If dark matter is light, it may be due to a seesaw mechanism just as neutrinos are. It is postulated that both originate from the same type of heavy fermion anchors, either singlets or triplets. In the latter case, a shift of the $W$ mass…

High Energy Physics - Phenomenology · Physics 2023-11-16 Ernest Ma

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

We establish a hybrid seesaw mechanism to explain small neutrino masses and predict cold dark matter candidate in the context of the B-L gauge symmetry extension of the Standard Model. In this model a new scalar doublet and two new fermion…

High Energy Physics - Phenomenology · Physics 2015-03-13 Tong Li , Wei Chao

Superheavy dark matter can satisfy the observed dark matter abundance if the stability condition is fulfilled. Here, we propose a new Abelian gauge symmetry ${\rm U(1)}_H$ for the stability of superheavy dark matter as the electromagnetic…

High Energy Physics - Phenomenology · Physics 2015-06-23 Jong-Chul Park , Seong Chan Park

The $U(1)_{B-L}$ gauge symmetry is a promising extension of the standard model of particle physics, which is supposed to be broken at some high energy scale. Associated with the $U(1)_{B-L}$ gauge symmetry breaking, right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2018-09-28 Nobuchika Okada , Osamu Seto

Seesaw mechanism provides a natural explanation of light neutrino masses through suppression of heavy seesaw scale. In inverse seesaw models the seesaw scale can be much lower than that in the usual seesaw models. If terms inducing seesaw…

High Energy Physics - Phenomenology · Physics 2015-06-05 Gang Guo , Xiao-Gang He , Guan-Nan Li

An interesting possibility for dark matter is a scalar particle of mass of order 10 MeV-1 GeV, interacting with a U(1) gauge boson (dark photon) which mixes with the photon. We present a simple and natural model realizing this possibility.…

High Energy Physics - Phenomenology · Physics 2016-08-17 Keisuke Harigaya , Yasunori Nomura

We propose a radiative lepton seesaw model with the ${\mathbb Z}_3$ Tambara-Yamagami fusion rule and gauged $B-L$ symmetry. The heavier right-handed neutral fermions ($N_R$) simultaneously contribute to the masses of charged-leptons and…

High Energy Physics - Phenomenology · Physics 2025-06-23 Takaaki Nomura , Hiroshi Okada

We extend the Type I seesaw and suggest a $new$ seesaw mechanism to generate neutrino masses within the left-right symmetric theories where parity is spontaneously broken. We construct a next to minimal left-right symmetric model where…

High Energy Physics - Phenomenology · Physics 2014-11-21 Joydeep Chakrabortty

We propose a new seesaw mechanism for neutrino masses within a class of supersymmetric SO(10) models with broken D-parity. It is shown that in such scenarios the B-L scale can be as low as TeV without generating inconsistencies with gauge…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Malinsky , J. C. Romao , J. W. F. Valle

We propose a simple testable model with mass generation mechanisms for dark matter and neutrino based on the gauged $U(1)_{B-L}$ symmetry and an exact $Z_2$ parity. The $U(1)_{B-L}$ symmetry is spontaneously broken at the TeV scale, by…

High Energy Physics - Phenomenology · Physics 2011-08-08 Shinya Kanemura , Osamu Seto , Takashi Shimomura

We discuss the possibility of cogenesis generating the ratio of baryon asymmetry to dark matter in a Stueckelberg U(1) extension of the standard model and of the minimal supersymmetric standard model. For the U(1) we choose…

High Energy Physics - Phenomenology · Physics 2012-07-03 Wan-Zhe Feng , Pran Nath , Gregory Peim

We study the $B-L$ gauge extension of the Standard Model which contains a singlet scalar and three right-handed neutrinos. The vacuum expectation value of the singlet scalar breaks the $U(1)_{B-L}$ symmetry. Here the third generation…

High Energy Physics - Phenomenology · Physics 2014-03-27 Tanushree Basak , Tanmoy Mondal

It is shown that in extensions of the standard model of quarks and leptons where additive lepton number $L$ is broken by two units, so that $Z_2$ lepton parity, i.e. $(-1)^L$ which is either even or odd, remains exactly conserved, there is…

High Energy Physics - Phenomenology · Physics 2015-07-08 Ernest Ma