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Dark matter and neutrinos provide the two most compelling pieces of evidence for new physics beyond the Standard Model of Particle Physics but they are often treated as two different sectors. In this paper, we consider how neutrino…

High Energy Physics - Phenomenology · Physics 2018-05-28 Andres Olivares-Del Campo , Sergio Palomares-Ruiz , Silvia Pascoli

We make use of swampland conjectures to explore the phenomenology of neutrino-modulino mixing in regions of the parameter space that are within the sensitivity of experiments at the CERN's Forward Physics Facility (FPF). We adopt the…

High Energy Physics - Phenomenology · Physics 2024-02-13 Luis A. Anchordoqui , Ignatios Antoniadis , Karim Benakli , Jules Cunat , Dieter Lust

I summarize the results of a recent analysis where the cosmological effects of interactions of neutrinos with cold Dark Matter (DM) is investigated. This interaction produces diffusion-damped oscillations in the matter power spectrum,…

Astrophysics · Physics 2008-11-26 Gianpiero Mangano

We consider, in a model-independent framework, the potential for observing dark matter in neutrino detectors through the interaction $\bar{f} p \to e^+ n$, where $f$ is a dark fermion. Operators of dimension six or less are considered, and…

High Energy Physics - Phenomenology · Physics 2009-10-19 Jennifer Kile

Cosmological limits on neutrino masses are softened, by more than a factor 2, if Cold Dark Matter (CDM) and Dark Energy (DE) are coupled. In turn, a neutrino mass yielding $\Omega_\nu$ up to $\sim0.20$ allows coupling levels $\beta \simeq…

Astrophysics · Physics 2010-04-15 G. La Vacca , S. A. Bonometto , L. P. L. Colombo

We revisit the WMAP dark matter constraints on Yukawa Unification in the presence of massive neutrinos. The large neutrino mixing indicated by the data modifies the predictions for the bottom quark mass, and enables Yukawa also for large…

High Energy Physics - Phenomenology · Physics 2009-05-01 M. E. Gomez , S. Lola , P. Naranjo , J. Rodriguez-Quintero

If the neutrino is Majorana type and the electroweak phase transition is second or weak first order, neutrino-induced interactions together with sphaleron transitions have the potential to erase a previously generated baryon asymmetry of…

High Energy Physics - Phenomenology · Physics 2009-10-31 H. V. Klapdor-Kleingrothaus , St. Kolb , U. Sarkar

We consider a class of theories in which neutrino masses depend significantly on environment, as a result of interactions with the dark sector. Such theories of mass varying neutrinos (MaVaNs) were recently introduced to explain the origin…

High Energy Physics - Phenomenology · Physics 2009-11-10 David B. Kaplan , Ann E. Nelson , Neal Weiner

Short baseline neutrino oscillation experiments have shown hints of the existence of additional sterile neutrinos in the eV mass range. Such sterile neutrinos are incompatible with cosmology because they suppress structure formation unless…

Cosmology and Nongalactic Astrophysics · Physics 2015-03-30 Maria Archidiacono , Steen Hannestad , Rasmus Sloth Hansen , Thomas Tram

We propose an extension to the Standard Model accommodating two families of Dirac neutral fermions and Majorana fermions under additional ${U(1)_{e-\mu} \times Z_3\times Z_2}$ symmetries where ${U(1)_{e-\mu}}$ is a flavor dependent gauge…

High Energy Physics - Phenomenology · Physics 2020-10-28 Holger Motz , Hiroshi Okada , Yoichi Asaoka , Kazunori Kohri

Mixing between light and heavy neutrino states has been proposed as an explanation (or partial explanation) for the 3-sigma NuTeV anomaly and the 2-sigma departure of the $Z^0$ invisible width from its expected value. I assume herein that…

High Energy Physics - Phenomenology · Physics 2016-09-06 Sheldon Lee Glashow

We propose a new model where the Dirac mass term for neutrinos, the Majorana mass term for right-handed neutrinos, and the other new fermion masses arise via the spontaneous breakdown of the $U(1)_{B-L}$ gauge symmetry. The anomaly-free…

High Energy Physics - Phenomenology · Physics 2014-07-10 Shinya Kanemura , Toshinori Matsui , Hiroaki Sugiyama

We study the inverse seesaw mechanism for neutrino masses and phenomenological consequences in the context of conformal electro-weak symmetry breaking. The main difference to the usual case is that all explicit fermion mass terms including…

High Energy Physics - Phenomenology · Physics 2015-06-16 Pascal Humbert , Manfred Lindner , Juri Smirnov

We show that Majorana neutrinos convert into antineutrinos in a background of ultralight vector dark matter coupled to lepton number, such as the gauge boson of $\text{U}(1)_{B-L}$ or $\text{U}(1)_{L_i - L_j}$ with $i, j = e , \mu, \tau$.…

High Energy Physics - Phenomenology · Physics 2026-05-11 Asher Berlin , Rodolfo Capdevilla , Ting Cheng , Matheus Hostert , Pedro A. N. Machado

We propose a supersymmetric scenario in which the small Yukawa couplings for the Dirac neutrino mass term are generated by the spontaneous-breaking of Pecci-Quinn symmetry. In this scenario, a right amount of dark matter relic density can…

High Energy Physics - Phenomenology · Physics 2015-06-18 Wan-Il Park

A dynamical mechanism, based on a confining non-abelian dark symmetry, which generates Majorana masses for hypercharge-less fermions, is proposed. We apply it to the inverse seesaw scenario, which allows to generate light neutrino masses…

High Energy Physics - Phenomenology · Physics 2024-08-08 Maximilian Berbig , Juan Herrero-Garcia , Giacomo Landini

We revisit the WMAP dark matter constraints on Yukawa Unification in the presence of massive neutrinos. The large lepton mixing indicated by the data may modify the predictions for the bottom quark mass, enabling Yukawa unification also for…

High Energy Physics - Phenomenology · Physics 2010-04-15 M. E. Gomez , S. Lola , P. Naranjo , J. Rodriguez-Quintero

The presence of light (m_a ~ 10^-6 ev) scalar fields in the early universe can modify the cosmology of neutrinos considerably by allowing their masses to vary on cosmological times. In this paper, we consider the effect of Planck-suppressed…

High Energy Physics - Phenomenology · Physics 2009-11-11 Neal Weiner , Kathryn Zurek

Some properties of a neutrino may differ significantly depending on whether it is Dirac or Majorana type. The type is determined by the relative size of Dirac and Majorana masses, which may vary if they arise from an oscillating scalar dark…

High Energy Physics - Phenomenology · Physics 2023-11-13 YeolLin ChoeJo , Yechan Kim , Hye-Sung Lee

The possibility of direct detection of light fermionic dark matter in neutrino detectors is explored from a model-independent standpoint. We consider all operators of dimension six or lower which can contribute to the interaction $\bar{f} p…

High Energy Physics - Phenomenology · Physics 2010-01-07 Jennifer Kile , Amarjit Soni