Search results for " Dark Matter"

showing 10 items of 159 documents

Reconciling dark matter, solar and atmospheric neutrinos

1993

We present models that can reconcile the solar and atmospheric neutrino data with the existence of a hot dark matter component in the universe. This dark matter is a quasi-Dirac neutrino whose mass $m_{DM}$ arises at the one-loop level. The solar neutrino deficit is explained via nonadiabatic conversions of electron neutrino to a sterile neutrino and the atmospheric neutrino data via maximal muon neutrino to tau neutrino oscillations generated by higher order loop diagrams. For $m_{DM} \sim 30$ eV the radiative neutrino decay can lead to photons that can ionize interstellar hydrogen. In one of the models one can have observable $\nu_e$ to $\nu_\tau$ oscillation rates, with no appreciable mu…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSolar neutrinoHot dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Tau neutrinoHigh Energy Physics::ExperimentMuon neutrinoNeutrinoElectron neutrinoComputer Science::DatabasesNuclear Physics B
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Reconciling dark matter and solar neutrinos

1993

Abstract We present a simple model for neutrino dark matter in which neutrino masses arise radiatively and the solar neutrino data are explained via the MSW effect. The dark matter scale arises at the one-loop level with the MSW scale arises only in two loops. The model is compatible with all observational facts and allows observable ν e ν τ or ν μ ν τ oscillation rates in the laboratory if the limits from primordial big bang nucleosynthesis (BBN) are taken conservatively. In addition, it can be probed by searching for muon number violating processes such as μ → e + γ , and μ →3 e . These rates can well lie within the sensitivities of present experiments. Finally, if we ignore BBN limits we…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrinoPhysics::Instrumentation and DetectorsSolar neutrinoDark matterHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemNuclear physicsWarm dark matterMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationParticle Physics - Phenomenology
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Collider signatures of sneutrino cold dark matter

1999

Decays of sneutrinos are considered in the case that in the presence of lepton-number violation in the sneutrino sector the lighter tau-sneutrino is the Lightest Supersymmetric Particle and the Cold Dark Matter in the Universe. In such circumstances the signals from sparticle decays differ considerably from the ``standard'' case where the lightest neutralino is the Lightest Supersymmetric Particle and it is found that in a wide range of parameters compatible with the sneutrino Cold Dark Matter hypothesis signatures characteristic for such a scenario should be easily observable at for example a Next Linear Collider.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsCold dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesSuperpartnerFísicaObservableLightest Supersymmetric Particlelaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawNeutralinoHigh Energy Physics::ExperimentCollider
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Electron beam studies of light collection in a scintillating counter with embedded fibers

2021

The light collection of several fiber configurations embedded in a box-shaped plastic scintillating counter was studied by scanning with minimum ionizing electrons. The light was read out by silicon photomultipliers at both ends. The light yield produced by the 855-MeV beam of the Mainz Microtron showed a strong dependence on the transverse distance from the beam position to the fibers. The observations were modeled by attributing the collection of indirect light inside of the counter and of direct light reaching a fiber to the total light yield. The light collection with fibers was compared to that of a scintillating counter without fibers. These studies were carried out within the develop…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsbusiness.industryFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)ElectronOpticsSilicon photomultiplierCathode rayPhysics::Accelerator PhysicsFiberNuclear Experiment (nucl-ex)businessNuclear ExperimentInstrumentationLight dark matterMicrotronBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Joint constraints on galaxy bias and σ8 through the N-pdf of the galaxy number density

2015

We present a full description of the N-probability density function of the galaxy number density fluctuations. This N-pdf is given in terms, on the one hand, of the cold dark matter correlations and, on the other hand, of the galaxy bias parameter. The method relies on the assumption commonly adopted that the dark matter density fluctuations follow a local non-linear transformation of the initial energy density perturbations. The N-pdf of the galaxy number density fluctuations allows for an optimal estimation of the bias parameter (e.g., via maximum-likelihood estimation, or Bayesian inference if there exists any a priori information on the bias parameter), and of those parameters defining …

PhysicsNumber densityCold dark matter010308 nuclear & particles physicsModel selectionDark matterEstimatorAstronomy and AstrophysicsProbability density functionAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesGalaxy0103 physical sciencesStatistical physics010303 astronomy & astrophysicsGalaxy clusterAstrophysics - Cosmology and Nongalactic Astrophysics
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X-Ray Lines from Dark Matter Annihilation at the keV Scale.

2018

In 2014, several groups reported hints for a yet unidentified line in astrophysical x-ray signals from galaxies and galaxy clusters at an energy of 3.5 keV. While it is not unlikely that this line is simply a reflection of imperfectly modeled atomic transitions, it has renewed the community’s interest in models of keV-scale dark matter, whose decay would lead to such a line. The alternative possibility of dark matter annihilation into monochromatic photons is far less explored, a lapse that we strive to amend in this Letter. More precisely, we introduce a novel model of fermionic dark matter χ with O(keV) mass, annihilating to a scalar state ϕ which in turn decays to photons, for instance v…

PhysicsParticle physics010308 nuclear & particles physicsHot dark matterDark matterScalar field dark matterGeneral Physics and Astronomy01 natural sciencesBaryonic dark matterWeakly interacting massive particles0103 physical sciencesWarm dark matter010303 astronomy & astrophysicsLight dark matterDark fluidPhysical review letters
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Dark Matter Decay between Phase Transitions at the Weak Scale

2017

We propose a new alternative to the weakly interacting massive particle paradigm for dark matter. Rather than being determined by thermal freeze-out, the dark matter abundance in this scenario is set by dark matter decay, which is allowed for a limited amount of time just before the electroweak phase transition. More specifically, we consider fermionic singlet dark matter particles coupled weakly to a scalar mediator S_{3} and to auxiliary dark sector fields, charged under the standard model gauge groups. Dark matter freezes out while still relativistic, so its abundance is initially very large. As the Universe cools down, the scalar mediator develops a vacuum expectation value (VEV), which…

PhysicsParticle physics010308 nuclear & particles physicsHot dark matterHigh Energy Physics::PhenomenologyDark matterScalar field dark matterGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesBaryonic dark matter0103 physical sciencesMixed dark matterWarm dark matter010306 general physicsLight dark matterDark fluidPhysical Review Letters
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Shell-model study on event rates of lightest supersymmetric particles scattering offKr83andTe125

2016

We investigate the elastic and inelastic scattering of lightest supersymmetric particle (LSP) dark matter off two possible target nuclei, $^{83}\mathrm{Kr}$ and $^{125}\mathrm{Te}$. For the nuclear-structure calculations, we employ the nuclear shell model using recently generated realistic interactions. We have condensed the nuclear-physics contribution to a set of nuclear-structure factors that are independent of the adopted supersymmetric (SUSY) model. Total event rates are then easily calculated by combining the nuclear-structure factors with SUSY parameters of choice. In particular, $^{125}\mathrm{Te}$ shows promise as a detector material with both the elastic and inelastic channels yie…

PhysicsParticle physics010308 nuclear & particles physicsScatteringPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyNuclear TheoryNuclear shell modelSupersymmetryInelastic scattering7. Clean energy01 natural sciencesLightest Supersymmetric ParticleNuclear physicsWeakly interacting massive particles0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsLight dark matterPhysical Review D
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Review of dark photon searches

2016

Dark Photons are hypothetical extra-U(1) gauge bosons, which are motivated by a number of astrophysical anomalies as well as the presently seen deviation between the Standard Model prediction and the direct measurement of the anomalous magnetic moment of the muon, (g − 2)μ . The Dark Photon does not serve as the Dark Matter particle itself, but acts as a messenger particle of a hypothetical Dark Sector with residual interaction to the Standard Model. We review recent Dark Photon searches, which were carried out in a global effort at various hadron and particle physics facilities. We also comment on the perspectives for future invisble searches, which directly probe the existence of Light Da…

PhysicsParticle physicsAnomalous magnetic dipole moment010308 nuclear & particles physicsAxion Dark Matter ExperimentHot dark matterPhysicsQC1-999Dark matterScalar field dark matterAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesDark photonNuclear physicsWeakly interacting massive particles0103 physical sciences010306 general physicsLight dark matterEPJ Web of Conferences
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Dark Matter and the Seesaw Scale

2018

We discuss the possibility to find an upper bound on the seesaw scale using the cosmological bound on the cold dark matter relic density. We investigate a simple relation between the origin of neutrino masses and the properties of a dark matter candidate in a simple theory where the new symmetry breaking scale defines the seesaw scale. Imposing the cosmological bounds, we find an upper bound of order multi-TeV on the lepton number violation scale. We investigate the predictions for direct and indirect detection dark matter experiments, and the possible signatures at the Large Hadron Collider.

PhysicsParticle physicsCold dark matter010308 nuclear & particles physicsDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesLepton numberUpper and lower boundsPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryWeakly interacting massive particles0103 physical sciencesGran col·lisionador d'hadrons (França i Suïssa)High Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physics
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