Search results for "Massive particle"

showing 10 items of 47 documents

Reconstructing WIMP properties with neutrino detectors

2008

If the dark matter of the Universe is constituted by weakly interacting massive particles (WIMP), they would accumulate in the core of astrophysical objects as the Sun and annihilate into particles of the Standard Model. High-energy neutrinos would be produced in the annihilations, both directly and via the subsequent decay of leptons, quarks and bosons. While Cherenkov neutrino detectors/telescopes can only count the number of neutrinos above some threshold energy, we study how, by exploiting their energy resolution, large magnetized iron calorimeter and, possibly, liquid argon and totally active scintillator detectors, planned for future long baseline neutrino experiments, have the capabi…

PhysicsAstrofísicaParticle physicsNuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Dark matterHigh Energy Physics::PhenomenologyAstrophysics::Instrumentation and Methods for AstrophysicsFOS: Physical scienceshep-phSolar neutrino problemAstrophysicsNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino detectorWIMPastro-phWeakly interacting massive particlesHigh Energy Physics::ExperimentNeutrinoLight dark matterPhysics Letters B
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Ionization of atoms by slow heavy particles, including dark matter

2016

Atoms and molecules can become ionized during the scattering of a slow, heavy particle off a bound electron. Such an interaction involving leptophilic weakly interacting massive particles (WIMPs) is a promising possible explanation for the anomalous 9 sigma annual modulation in the DAMA dark matter direct detection experiment [R. Bernabei et al., Eur. Phys. J. C 73, 2648 (2013)]. We demonstrate the applicability of the Born approximation for such an interaction by showing its equivalence to the semiclassical adiabatic treatment of atomic ionization by slow-moving WIMPs. Conventional wisdom has it that the ionization probability for such a process should be exponentially small. We show, howe…

PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Atomic Physics (physics.atom-ph)010308 nuclear & particles physicsScatteringDark matterAtoms in moleculesFOS: Physical sciencesGeneral Physics and AstronomyElectron01 natural sciencesAstrophysics - Astrophysics of GalaxiesPhysics - Atomic PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysics of Galaxies (astro-ph.GA)IonizationWeakly interacting massive particles0103 physical sciencesBorn approximationAtomic physics010306 general physicsRelativistic quantum chemistryAstrophysics - Cosmology and Nongalactic Astrophysics
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Search for dark matter in the Sun with the ANTARES neutrino telescope in the CMSSM and mUED frameworks

2012

ANTARES is the first neutrino telescope in the sea. It consists of a three-dimensional array of 885 photomultipliers to collect the Cherenkov light induced by relativistic muons produced in CC interactions of high energy neutrinos. One of the main scientific goals of the experiment is the search for dark matter. We present here the analysis of data taken during 2007 and 2008 to look for a WIMP signal in the Sun. WIMPs are one of the most popular scenarios to explain the dark matter content of the Universe. They would accumulate in massive objects like the Sun or the Galactic Center and their self-annihilation would produce (directly or indirectly) high energy neutrinos detectable by neutrin…

PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaDark matterAstrophysics::Instrumentation and Methods for AstrophysicsAstronomyFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsSolar neutrino problemHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Neutrino detectorWeakly interacting massive particlesHigh Energy Physics::ExperimentFísica nuclearNeutrinoNeutrino astronomyAstrophysics - High Energy Astrophysical PhenomenaInstrumentationLight dark matter
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Fuzzy Dark Matter and Non-Standard Neutrino Interactions

2018

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 shown previously that such dark matter candidates are phenomenologically successful and might help ameliorate the tension between predicted and observed small scale structures in the Universe. We argue that coherent forward scattering of neutrinos on fuzzy dark matter particles can significantly alter neutrino oscillation probabilities. These effects could be observable in current and future experiments. We set new limits on fuzzy dark matter interacting…

PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Particle physicsSterile neutrino010308 nuclear & particles physicsSolar neutrinoDark matterScalar field dark matterFOS: Physical sciencesSolar neutrino problem7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Weakly interacting massive particles0103 physical sciencesNeutrinoAstrophysics - High Energy Astrophysical Phenomena010306 general physicsDark fluid
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Inelastic WIMP-nucleus scattering to the first excited state in125Te

2016

The direct detection of dark matter constituents, in particular the weakly interacting massive particles (WIMPs), is considered 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 $^{127}$I and $^{129}$Xe and $^{83}$Kr. Here we examine $^{125}$Te, which offers some advantages and is currently being considered as a target.In all these cases the extra signature of the gamma rays following the de-excitation of these states has definite advantages over the purely nuclear recoil and, in principle, such a signat…

PhysicsNuclear and High Energy PhysicsCold dark matter010308 nuclear & particles physicsScatteringDark matterFOS: Physical sciencesContext (language use)Inelastic scattering01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)WIMPExcited stateWeakly interacting massive particles0103 physical sciences010306 general physicsJournal of Physics G: Nuclear and Particle Physics
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Connection between certain massive and massless diagrams

1996

A useful connection between two-loop massive vacuum integrals and one-loop off-shell triangle diagrams with massless internal particles is established for arbitrary values of the space-time dimension {ital n}. {copyright} {ital 1996 The American Physical Society.}

PhysicsNuclear and High Energy PhysicsComputer Science::Information RetrievalSpace timeDimension (graph theory)Massive particlePropagatorMatter creationMassless particlesymbols.namesakeQuantum mechanicssymbolsFeynman diagramConnection (algebraic framework)Mathematical physicsPhysical Review D
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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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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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2019

Abstract We perform calculations of structure functions for elastic and inelastic spin-dependent scattering of weakly interacting massive particles (WIMPs) off 125Te, 129Xe, and 131Xe. The nuclear structure calculations are performed in the microscopic interacting boson-fermion model (IBFM-2). In our calculations we employ one-body and leading long-range two-body WIMP-nucleus currents derived from chiral effective field theory. We demonstrate that the relevant matrix elements can be reliably computed in the IBFM-2, which will allow investigation of heavy deformed nuclei previously inaccessible to theoretical calculations.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsScatteringNuclear structureFermion01 natural sciencesWIMPWeakly interacting massive particles0103 physical sciencesEffective field theory010306 general physicsBosonSpin-½Nuclear Physics A
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Cold positrons from decaying dark matter

2012

Many models of dark matter contain more than one new particle beyond those in the Standard Model. Often heavier particles decay into the lightest dark matter particle as the Universe evolves. Here we explore the possibilities that arise if one of the products in a (Heavy Particle) $\rightarrow$ (Dark Matter) decay is a positron, and the lifetime is shorter than the age of the Universe. The positrons cool down by scattering off the cosmic microwave background and eventually annihilate when they fall into Galactic potential wells. The resulting 511 keV flux not only places constraints on this class of models but might even be consistent with that observed by the INTEGRAL satellite.

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Astrophysics::High Energy Astrophysical PhenomenaHot dark matterDark matterScalar field dark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Weakly interacting massive particlesMixed dark matterWarm dark matterLight dark matterDark fluidAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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