Search results for "Dark matter"

showing 10 items of 627 documents

Sneutrino Dark Matter in Low-scale Seesaw Scenarios

2012

We consider supersymmetric models in which sneutrinos are viable dark matter candidates. These are either simple extensions of the Minimal Supersymmetric Standard Model with additional singlet superfields, such as the inverse or linear seesaw, or a model with an additional U(1) group. All of these models can accomodate the observed small neutrino masses and large mixings. We investigate the properties of sneutrinos as dark matter candidates in these scenarios. We check for phenomenological bounds, such as correct relic abundance, consistency with direct detection cross section limits and laboratory constraints, among others lepton flavour violating (LFV) charged lepton decays. While inverse…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physics010308 nuclear & particles physicsDark matterHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesInverse01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry13. Climate action0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsLeptonMinimal Supersymmetric Standard Model
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Diagnostic Potential of Cosmic-Neutrino Absorption Spectroscopy

2004

Annihilation of extremely energetic cosmic neutrinos on the relic-neutrino background can give rise to absorption lines at energies corresponding to formation of the electroweak gauge boson $Z^{0}$. The positions of the absorption dips are set by the masses of the relic neutrinos. Suitably intense sources of extremely energetic ($10^{21}$ -- $10^{25}$-eV) cosmic neutrinos might therefore enable the determination of the absolute neutrino masses and the flavor composition of the mass eigenstates. Several factors--other than neutrino mass and composition--distort the absorption lines, however. We analyze the influence of the time-evolution of the relic-neutrino density and the consequences of …

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsCosmologiaPhysics::Instrumentation and Detectorsmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaDark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysicsPartícules (Física nuclear)UniverseCosmic neutrino backgroundHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedInvariant massHigh Energy Physics::ExperimentAbsorption (logic)Neutrinomedia_common
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Interior spacetimes of stars in Palatinif(R)gravity

2006

We study the interior spacetimes of stars in the Palatini formalism of f(R) gravity and derive a generalized Tolman-Oppenheimer-Volkoff and mass equation for a static, spherically symmetric star. We show that matching the interior solution with the exterior Schwarzschild-De Sitter solution in general gives a relation between the gravitational mass and the density profile of a star, which is different from the one in General Relativity. These modifications become neglible in models for which $\delta F(R) \equiv \partial f/\partial R - 1$ is a decreasing function of R however. As a result, both Solar System constraints and stellar dynamics are perfectly consistent with $f(R) = R - \mu^4/R$.

PhysicsNuclear and High Energy PhysicsGeneral relativityAstrophysics (astro-ph)Dark matterFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)AstrophysicsGeneral Relativity and Quantum CosmologyCosmologyMass formulaGravitationGeneral Relativity and Quantum CosmologyStarsClassical mechanicsStellar dynamicsf(R) gravityMathematical physicsPhysical Review D
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Gravitational waves from galaxy encounters

2007

We discuss the emission of gravitational radiation produced in encounters of dark matter galactic halos. To this aim we perform a number of numerical simulations of typical galaxy mergers, computing the associated gravitational radiation waveforms as well as the energy released in the processes. Our simulations yield dimensionless gravitational wave amplitudes of the order of $10^{-13}$ and gravitational wave frequencies of the order of $10^{-16}$ Hz, when the galaxies are located at a distance of 10 Mpc. These values are of the same order as those arising in the gravitational radiation originated by strong variations of the gravitational field in the early Universe, and therefore, such gra…

PhysicsNuclear and High Energy PhysicsGravitational-wave observatoryGravitational waveInstituto de Ciencias del PatrimonioAstrophysics (astro-ph)Dark matterFOS: Physical sciencesAstronomyAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsGalaxy mergerAstrophysicsGravitational energyInstitute of Heritage SciencesGeneral Relativity and Quantum CosmologyGravitational fieldgalaxy encountersgravitational wavesIncipitGravitational collapseAstrophysics::Galaxy AstrophysicsGravitational redshift
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Theoretical direct WIMP detection rates for transitions to the first excited state inKr83

2015

The direct detection of dark matter constituents, in particular the weakly interacting massive particles (WIMPs), is central to particle physics and cosmology. In this paper we study transitions to the excited states, possible in some nuclei, which have sufficiently low lying excited states. Examples considered previously were the first excited states of $^{127}\mathrm{I}$ and $^{129}\mathrm{Xe}$. We examine here $^{83}\mathrm{Kr}$, which offers some kinematical advantages and is a possible target. We estimate appreciable rates for the inelastic scattering mediated by the spin cross sections, with an inelastic event rate of $4.4\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}\text{ …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionDark matterGamma rayInelastic scattering01 natural sciencesWIMPWeakly interacting massive particlesExcited state0103 physical sciences010306 general physicsSpin (physics)Physical Review D
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Generation patterns, modified $\gamma-Z$ mixing, and hidden sector with dark matter candidates as framed standard model results

2018

A descriptive summary is given of the results to-date from the framed standard model (FSM) which: Assigns geometric meaning to the Higgs field and to fermion generations, hence offering an explanation for the observed mass and mixing patterns of quarks and leptons, reproducing near-quantitatively 17 of SM parameters with only 7. Predicts a new vector boson [Formula: see text] which mixes with [Formula: see text] and [Formula: see text], leading to deviations from the SM mixing scheme. For [Formula: see text] TeV, these deviations are within present experimental errors but should soon be detectable at LHC when experimental accuracy is further improved. Suggests the existence of a hidden sec…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterAstronomy and Astrophysics01 natural sciencesAtomic and Molecular Physics and OpticsStandard ModelHidden sectorHigh Energy Physics - Phenomenology0103 physical sciences010306 general physicsMixing (physics)
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WIMP dark matter as radiative neutrino mass messenger

2013

The minimal seesaw extension of the Standard SU(3)(c)circle times SU(2)(L)circle times U(1)(Y) Model requires two electroweak singlet fermions in order to accommodate the neutrino oscillation parameters at tree level. Here we consider a next to minimal extension where light neutrino masses are generated radiatively by two electroweak fermions: one singlet and one triplet under SU(2)(L). These should be odd under a parity symmetry and their mixing gives rise to a stable weakly interactive massive particle (WIMP) dark matter candidate. For mass in the GeV-TeV range, it reproduces the correct relic density, and provides an observable signal in nuclear recoil direct detection experiments. The f…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterElectroweak interactionHigh Energy Physics::PhenomenologyMassive particleFOS: Physical sciencesFermionCosmology of Theories beyond the SM7. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryWIMP0103 physical sciencesBeyond Standard ModelHigh Energy Physics::ExperimentNeutrino PhysicsNeutrino010306 general physicsNeutrino oscillation
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A theory for scotogenic dark matter stabilised by residual gauge symmetry

2020

Dark matter stability can result from a residual matter-parity symmetry, following naturally from the spontaneous breaking of the gauge symmetry. Here we explore this idea in the context of the $\mathrm{SU(3)_c \otimes SU(3)_L \otimes U(1)_X \otimes U(1)_{N}}$ electroweak extension of the standard model. The key feature of our new scotogenic dark matter theory is the use of a triplet scalar boson with anti-symmetric Yukawa couplings. This naturally implies that one of the light neutrinos is massless and, as a result, there is a lower bound for the $\rm 0\nu\beta\beta$ decay rate.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesScalar boson01 natural sciencesSymmetry (physics)lcsh:QC1-999Massless particleStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicslcsh:PhysicsGauge symmetry
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Theoretical predictions for the direct detection of neutralino dark matter in the NMSSM

2004

We analyse the direct detection of neutralino dark matter in the framework of the Next-to-Minimal Supersymmetric Standard Model. After performing a detailed analysis of the parameter space, taking into account all the available constraints from LEPII, we compute the neutralino-nucleon cross section, and compare the results with the sensitivity of detectors. We find that sizable values for the detection cross section, within the reach of dark matter detectors, are attainable in this framework. For example, neutralino-proton cross sections compatible with the sensitivity of present experiments can be obtained due to the exchange of very light Higgses with $m_{h_1^0}\lsim 70$ GeV. Such Higgses…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterHigh Energy Physics::PhenomenologyAstrophysics (astro-ph)FOS: Physical sciencesSupersymmetryParameter spaceAstrophysics01 natural sciencesNext-to-Minimal Supersymmetric Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutralinoBibliographyHigh Energy Physics::ExperimentSensitivity (control systems)010306 general physicsMinimal Supersymmetric Standard Model
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Accidental stability of dark matter

2013

We propose that dark matter is stable as a consequence of an accidental Z(2) that results from a flavour symmetry group which is the double-cover group of the symmetry group of one of the regular geometric solids. Although model-dependent, the phenomenology resembles that of a generic >inert Higgs> dark matter scheme.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterHigh Energy Physics::Phenomenologyneutrino masses and mixingFOS: Physical sciencesFísicaSymmetry group01 natural sciencesdark matterHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Accidental0103 physical sciencesHiggs boson010306 general physicsPhenomenology (particle physics)flavour symmetry
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