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The nature of dark matter (DM) and how it might interact with the particles of the Standard Model (SM) is an ever-growing mystery. It is possible that the existence of new `dark sector' forces, yet undiscovered, are the key to solving this…

High Energy Physics - Phenomenology · Physics 2020-11-20 Thomas D. Rueter , Thomas G. Rizzo

A new light gauge boson $U$ may have both vector and axial couplings. In a large class of theories however, the new $U(1)$ current $J^\mu_F$ naturally combines with the weak neutral current $J^\mu_{Z_{\rm sm}}$, both parity-violating, into…

High Energy Physics - Phenomenology · Physics 2017-03-08 Pierre Fayet

In this work we consider the extension of the standard model by dark fields with an Abelian $U(1)_{d}$ spontaneously broken gauge symmetry in a hidden dark matter scenario. Considering all the dimension four gauge invariant terms we show…

High Energy Physics - Phenomenology · Physics 2021-10-19 M. Napsuciale , S. Rodríguez , H. Hernández-Arellano

We examine the possibility that dark matter may be the manifestation of dark forces of a hidden sector, i.e. "Dark Force = Dark Matter." As an illustrative and minimal example we consider the hidden SU(2)_h x U(1)_h gauge group. The hidden…

High Energy Physics - Phenomenology · Physics 2014-04-02 Hooman Davoudiasl , Ian M. Lewis

We present a fermionic dark matter model mediated by the hidden gauge boson. We assume the QED-like hidden sector which consists of a Dirac fermion and U(1)$_X$ gauge symmetry, and introduce an additional scalar electroweak doublet field…

High Energy Physics - Phenomenology · Physics 2020-12-16 Dong-Won Jung , Soo-hyeon Nam , Chaehyun Yu , Yeong Gyun Kim , Kang Young Lee

The primary aim of the thesis is to explore the possibility of spontaneous symmetry breaking by strong Yukawa dynamics. Technically, the symmetry is assumed to be broken by formation of symmetry-breaking parts of both the scalar and the…

High Energy Physics - Phenomenology · Physics 2012-08-10 Petr Benes

A new dynamical symmetry breaking model of electroweak interactions is proposed based on interacting fermions. Two fermions of different SU_{L}(2) representations form a symmetry breaking condensate and generate the lepton and quark masses.…

High Energy Physics - Phenomenology · Physics 2009-01-07 G. Cynolter , E. Lendvai , G. Pocsik

Kinetic mixing of the dark photon, the gauge boson of a hidden $U(1)_D$, with the Standard Model (SM) gauge fields to induce an interaction between ordinary matter and dark matter (DM) at 1-loop requires the existence of portal matter (PM)…

High Energy Physics - Phenomenology · Physics 2024-02-20 Thomas G. Rizzo

We discuss dynamical breaking of non-abelian gauge groups in three dimensional (lattice) gauge systems via the formation of fermion condensates. A physically relevant example, motivated by condensed-matter physics, is that of a fermionic…

High Energy Physics - Lattice · Physics 2016-09-01 K. Farakos , N. E. Mavromatos

A spontaneously broken hidden U(1)$_h$ gauge symmetry can explain both the dark matter stability and the observed relic abundance. In this framework, the light gauge boson can mediate the strong dark matter self-interaction, which addresses…

High Energy Physics - Phenomenology · Physics 2019-03-27 Ayuki Kamada , Masaki Yamada , Tsutomu T. Yanagida

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

The interaction between the dark $U(1)_d$ sector with the visible Standard Model (SM) sector takes place through the kinetic mixing between the dark photon $U(1)_d$ field $Z_d^\mu$ and the SM $U(1)_Y$ gauge field $B_\mu$. After the…

High Energy Physics - Phenomenology · Physics 2023-02-14 Ashok Goyal , Mukesh Kumar , Satendra Kumar , Rafiqul Rahaman

We discuss the electroweak gauge symmetry breaking triggered by a new strong attractive interaction to condensate fermion-antifermion, and topcolor is a prototype. To deal with the fermion pairing, a general method based on the…

High Energy Physics - Phenomenology · Physics 2011-01-13 V. H. Nguyen , X. Y. Pham

A dynamical symmetry breaking model of electroweak interactions is investigated based on strongly interacting fermions. Vector-like fermions of different representations of the weak SU(2) form a symmetry breaking condensate and generate the…

High Energy Physics - Phenomenology · Physics 2015-03-18 G. Cynolter , E. Lendvai

We study a $U(1)\otimes U(1)$ system coupled to scalar fields. Initially the model is studied in a novel continuum formulation and study of the appropriate diagonalizations is performed. Three models are examined, in two of which the scalar…

High Energy Physics - Lattice · Physics 2025-10-28 K. Farakos , V. Iconomou , G. Koutsoumbas

In this work we study the interactions of the $Z$ and $Z^{\prime}$ generated by kinetic mixing in a class of theories for physics beyond the standard model motivated by the dark matter problem, containing a spontaneously broken extra…

High Energy Physics - Phenomenology · Physics 2021-10-19 M. Napsuciale , S. Rodriguez , H. Hernandez-Arellano

The most general Lagrangian for a model with two U(1) gauge symmetries contains a renormalizable operator which mixes their gauge kinetic terms. Such kinetic mixing can be generated at arbitrarily high scales but will not be suppressed by…

High Energy Physics - Phenomenology · Physics 2009-07-09 Keith R. Dienes , Christopher Kolda , John March-Russell

Fermion mass generation in the strongly coupled U(1) lattice gauge theory with fermion and scalar fields of equal charge is investigated by means of numerical simulation with dynamical fermions. Chiral symmetry of this model is broken by…

High Energy Physics - Lattice · Physics 2009-10-30 W. Franzki , J. Jersak

We provide a simple UV theory for a Dirac dark matter with a massless Abelian gauge boson. We introduce a single fermion transforming as the $\bf{16}$ representation in the SO(10)$'$ gauge group, which is assumed to be spontaneously broken…

High Energy Physics - Phenomenology · Physics 2020-07-22 Ayuki Kamada , Masaki Yamada , Tsutomu T. Yanagida

We consider a simple model of a dark sector with a chiral $U(1)$ gauge symmetry. The anomaly-free condition requires at least five chiral fermions. Some of the fermions acquire masses through a vacuum expectation value of a Higgs field, and…

High Energy Physics - Phenomenology · Physics 2026-03-03 Xiao He , Takaaki Nomura , Norimi Yokozaki