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Related papers: Protophobic Light Vector Boson as a Mediator to th…

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The connection between a hidden nonthermal sector and a thermal plasma can be established by a light thermal fermion mediator. When the fermion mediator is much lighter than the hidden species, kinematically forbidden decay of the mediator…

High Energy Physics - Phenomenology · Physics 2023-05-10 Shao-Ping Li

We discuss novel ways in which neutrino oscillation experiments can probe dark matter. In particular, we focus on interactions between neutrinos and ultra-light ("fuzzy") dark matter particles with masses of order $10^{-22}$ eV. It has been…

High Energy Physics - Phenomenology · Physics 2018-02-05 Vedran Brdar , Joachim Kopp , Jia Liu , Pascal Prass , Xiao-Ping Wang

We show that supersymmetric "Dark Force" models with gravity mediation are viable. To this end, we analyse a simple string-inspired supersymmetric hidden sector model that interacts with the visible sector via kinetic mixing of a light…

High Energy Physics - Phenomenology · Physics 2013-01-22 S. Andreas , M. D. Goodsell , A. Ringwald

Vector bosons heavier than $10^{-22}$ eV can be viable dark matter candidates with distinctive experimental signatures. Ultralight dark matter generally requires a non-thermal origin to achieve the observed density, while still behaving…

High Energy Physics - Phenomenology · Physics 2019-03-06 Jeff A. Dror , Keisuke Harigaya , Vijay Narayan

We point out that production of new bosons by charged meson decays can greatly enhance the sensitivity of beam-focused accelerator-based experiments to new physics signals. This enhancement arises since the charged mesons are focused and…

High Energy Physics - Phenomenology · Physics 2022-09-21 Bhaskar Dutta , Doojin Kim , Adrian Thompson , Remington T. Thornton , Richard G. Van de Water

If the standard model of particle interactions is extended to include a neutral SU(2)_N gauge factor, with SU(3)_C x SU(2)_L x U(1)_Y x SU(2)_N embedded in E_6 or [SU(3)]^3, a conserved generalized R parity may appear. As a result, we have…

High Energy Physics - Phenomenology · Physics 2011-04-06 J. Lorenzo Diaz-Cruz , Ernest Ma

We show that the $\mathrm{SU}(3)_C \times \mathrm{SU}(3)_L \times \mathrm{U}(1)_N$ model with right-handed neutrinos naturally accommodates a viable sub-MeV dark matter (DM) candidate realized as pseudo-Goldstone boson that acquires tiny…

High Energy Physics - Phenomenology · Physics 2026-04-15 Vinicius Oliveira , D. Cogollo , A. Doff , C. A. de S. Pires

We investigate a so-called 331 extension of the Standard Model gauge sector which accommodates neutrino masses and where the lightest of the new neutral fermions in the theory is a viable particle dark matter candidate. In this model,…

High Energy Physics - Phenomenology · Physics 2015-06-16 Stefano Profumo , Farinaldo S. Queiroz

The nature of dark matter remains a central question in particle physics, cosmology, and astrophysics. The prevailing hypothesis postulates that dark matter consists of particles that interact only weakly with Standard Model particles.…

High Energy Physics - Phenomenology · Physics 2023-12-01 Leon M. G. de la Vega , R. Ferro-Hernandez , A. García-Viltres , Eduardo Peinado , E. Vázquez-Jáuregui

Simplified models of light new physics provide a convenient benchmark for experimental searches for new physics signatures, including dark matter (DM). However, additional detection modes can arise in less simplified and more realistic…

High Energy Physics - Phenomenology · Physics 2024-08-20 Krzysztof Jodłowski , Leszek Roszkowski , Sebastian Trojanowski

Recently, a peak in the light fermion pair spectrum at invariant q^2 approximately equal to 16.7 Me^2. has been observed in the bombardment of Li-7 by protons. This peak has been interpreted in terms of a protophobic interaction of fermions…

High Energy Physics - Phenomenology · Physics 2018-04-10 Ulrich D. Jentschura , Istvan Nandori

Direct detection experiments for dark matter are increasingly ruling out large parameter spaces. However, light dark matter models with particle masses $<$ GeV are still largely unconstrained. Here we examine a proposal to use atom…

High Energy Physics - Phenomenology · Physics 2024-09-09 Yufeng Du , Clara Murgui , Kris Pardo , Yikun Wang , Kathryn M. Zurek

We study the sensitivity of the Fermilab Short-Baseline Neutrino (SBN) experiments, MicroBooNE, ICARUS, and SBND, to MeV- to GeV-scale inelastic dark matter interacting through a dark photon mediator. These models provide interesting…

High Energy Physics - Phenomenology · Physics 2021-11-03 Brian Batell , Joshua Berger , Luc Darmé , Claudia Frugiuele

We explore the sensitivity of collider experiments to a broad class of GeV-scale dark vector models of new physics via production in proton and neutron bremsstrahlung and initial state radiation. This is achieved using a new physically…

High Energy Physics - Phenomenology · Physics 2025-09-16 Felix Kling , Peter Reimitz , Adam Ritz

Superconducting targets have recently been proposed for the direct detection of dark matter as light as a keV, via elastic scattering off conduction electrons in Cooper pairs. Detecting such light dark matter requires sensitivity to…

High Energy Physics - Phenomenology · Physics 2016-07-27 Yonit Hochberg , Tongyan Lin , Kathryn M. Zurek

Dark matter particles interacting via the exchange of very light spin-0 mediators can have large self-interaction rates and obtain their relic abundance from thermal freeze-out. At the same time, these models face strong bounds from direct…

High Energy Physics - Phenomenology · Physics 2017-12-25 Felix Kahlhoefer , Kai Schmidt-Hoberg , Sebastian Wild

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