Search results for "Cold dark matter"

showing 10 items of 39 documents

Warm dark matter and the ionization history of the Universe

2017

In warm dark matter scenarios structure formation is suppressed on small scales with respect to the cold dark matter case, reducing the number of low-mass halos and the fraction of ionized gas at high redshifts and thus, delaying reionization. This has an impact on the ionization history of the Universe and measurements of the optical depth to reionization, of the evolution of the global fraction of ionized gas and of the thermal history of the intergalactic medium, can be used to set constraints on the mass of the dark matter particle. However, the suppression of the fraction of ionized medium in these scenarios can be partly compensated by varying other parameters, as the ionization effic…

PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Cold dark matter010308 nuclear & particles physicsHot dark matterScalar field dark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics7. Clean energy01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesMixed dark matterOptical depth (astrophysics)Warm dark matter010303 astronomy & astrophysicsReionizationLight dark matterAstrophysics::Galaxy AstrophysicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Future sensitivity of neutrino telescopes to dark matter annihilations from the cosmic diffuse neutrino signal

2014

Cosmological observations and cold dark matter N-body simulations indicate that our Universe is populated by numerous halos, where dark matter particles annihilate, potentially producing Standard Model particles. In this paper we calculate the contribution to the diffuse neutrino background from dark matter annihilations in halos at all redshifts and we estimate the future sensitivity to the annihilation cross section of neutrino telescopes such as IceCube or ANTARES. We consider various parametrizations to describe the internal halo properties and for the halo mass function in order to bracket the theoretical uncertainty in the limits from the modeling of the cosmological annihilation flux…

PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Cold dark matterAstrophysics::High Energy Astrophysical PhenomenaMilky Waymedia_common.quotation_subjectDark matterGalactic CenterHalo mass functionFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsUniverse13. Climate actionHaloNeutrinoAstrophysics::Galaxy AstrophysicsAstrophysics - Cosmology and Nongalactic Astrophysicsmedia_commonJournal of Cosmology and Astroparticle Physics
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Interpreting deviations between AR-VTG and GR

2019

The cosmic microwave background (CMB) anisotropies predicted by two cosmological models are compared, one of them is the standard model of general relativity with cold dark matter and cosmological constant, whereas the second model is based on a consistent vector-tensor theory of gravitation explaining solar system and cosmological observations. It is proved that the resulting differences — between the anisotropies of both models — are due to the so-called late integrated Sachs–Wolfe effect and, consequently, cross-correlations between maps of CMB temperatures and tracers of the dark matter distribution could be used in future to select one of the above models. The role of reionization is …

PhysicsGeneral Relativity and Quantum CosmologyCold dark matterSpace and Planetary ScienceGeneral relativityCosmic microwave backgroundAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAnisotropyMathematical PhysicsStandard ModelInternational Journal of Modern Physics D
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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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Non-Gaussian Signatures in the Lens Deformations of the CMB Sky. A New Ray-Tracing Procedure

2003

We work in the framework of an inflationary cold dark matter universe with cosmological constant, in which the cosmological inhomogeneities are considered as gravitational lenses for the CMB photons. This lensing deforms the angular distribution of the CMB maps in such a way that the induced deformations are not Gaussian. Our main goal is the estimation of the deviations with respect to Gaussianity appeared in the distribution of deformations. In the new approach used in this paper, matter is evolved with a particle-mesh N-body code and, then, an useful ray-tracing technique designed to calculate the correlations of the lens deformations induced by nonlinear structures is applied. Our appro…

PhysicsNuclear and High Energy PhysicsCold dark matterGaussianCosmic microwave backgroundAstrophysics (astro-ph)FOS: Physical sciencesCosmological constantAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicslaw.inventionComputational physicsRay tracing (physics)Lens (optics)Gravitationsymbols.namesakeClassical mechanicslawObservational cosmologysymbols
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Reconciling Cold Dark Matter with COBE/IRAS Plus Solar and Atmospheric Neutrino Data

1994

We present a model where an unstable MeV Majorana tau \neu can naturally reconcile the cold dark matter model (CDM) with cosmological observations of large and small scale density fluctuations and, simultaneously, with data on solar and atmospheric neutrinos. The solar \neu deficit is explained through long wavelength, so-called {\sl just-so} oscillations involving conversions of \ne into both \nm and a sterile species \ns, while atmospheric \neu data are explained through \nm to \ne conversions. Future long baseline \neu oscillation experiments, as well as some reactor experiments will test this hypothesis. The model is based on the spontaneous violation of a global lepton number symmetry …

PhysicsNuclear and High Energy PhysicsParticle physicsCold dark matterOscillationAstrophysics (astro-ph)High Energy Physics::PhenomenologyFísicaOrder (ring theory)FOS: Physical sciencesAstrophysicsLepton numberSymmetry (physics)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentNeutrino
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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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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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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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Ultralight dark photon as a model for early universe dark matter

2019

Dark photon is a massive vector field which interacts only with the physical photon through the kinetic mixing. This coupling is assumed to be weak so that the dark photon becomes almost unobservable in processes with elementary particles, but can serve as a dark matter particle. We argue that in very early Universe ($z>3000$) this vector field may have the equation of state of radiation ($w=1/3$) but later behaves as cold dark matter ($w=0$). This may slightly change the expansion rate of the Universe at early time and reduce the value of the sound horizon of baryon acoustic oscillations (standard ruler). As a result, in this model the value of the Hubble constant appears to be larger than…

PhysicsParticle physicsCold dark matterCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsEquation of state (cosmology)Dark matterOrder (ring theory)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsCoupling (probability)01 natural sciencesDark photonsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessymbolsBaryon acoustic oscillations010306 general physicsHubble's lawAstrophysics - Cosmology and Nongalactic Astrophysics
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