Search results for "HIDDEN"

showing 10 items of 210 documents

The width of the omega meson in the nuclear medium

2013

We evaluate the width of the omega meson in nuclear matter. We consider the free decay mode of the omega into three pions, which is dominated by rho IEuro decay, and replace the rho and pi propagators by their medium-modified ones. We also take into account the quasielastic and inelastic processes induced by a vector-baryon interaction dominated by vector meson exchange, as well as the contributions coming from the mechanism with medium-modified K , propagators. We obtain a substantial increase of the omega width in the medium, reaching a value of 121 +/- 10 MeV at normal nuclear matter density for an omega at rest, which comes mainly from omega N -> pi pi N, omega NN -> pi NN processes ass…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryNuclear TheoryNuclear physicsFOS: Physical sciences7. Clean energy01 natural sciencesOmegaMomentumNuclear Theory (nucl-th)PionChiral perturbation theory0103 physical sciencesMesons (Nuclear physics)Vector mesonMesons (Física nuclear)Nuclear structure010306 general physicsNuclear ExperimentPhysicsEstructura nuclear010308 nuclear & particles physicsPropagatorHeavy-Ion CollisionsFísicaNuclear matterFísica nuclearHigh Energy Physics::ExperimentHidden Local SymmetryBar (unit)
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Charmed hadrons in nuclear medium

2010

5th International Conference on Quarks and Nuclear Physics (QNP09).Inst High Energy Phys Chinese Acad Sci, Beijing, PEOPLES R CHINA, SEP 21-25, 2009

Nuclear and High Energy PhysicsParticle physicsMesondynamically-generated baryonic resonancesNuclear TheoryHadronScalar (mathematics)Nuclear TheoryFOS: Physical sciencesspectral functionCharmed and hidden charmed scalar resonances01 natural sciences7. Clean energyNuclear Theory (nucl-th)symbols.namesakePauli exclusion principleHigh Energy Physics - Phenomenology (hep-ph)charmed and hidden charmed scalar resonances0103 physical sciencesNuclear Experiment (nucl-ex)Open-charm mesons010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentPhysics010308 nuclear & particles physicsBlocking (radio)Dynamically-generated baryonic resonancesHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsSpectral functionBaryonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentDense matterRESONANCESMATTERopen-charm mesons
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Search for K+ decays to a muon and invisible particles

2021

The NA62 experiment at CERN reports searches for $K^+\to\mu^+N$ and $K^+\to\mu^+\nu X$ decays, where $N$ and $X$ are massive invisible particles, using the 2016-2018 data set. The $N$ particle is assumed to be a heavy neutral lepton, and the results are expressed as upper limits of ${\cal O}(10^{-8})$ of the neutrino mixing parameter $|U_{\mu4}|^2$ for $N$ masses in the range 200-384 MeV/$c^2$ and lifetime exceeding 50 ns. The $X$ particle is considered a scalar or vector hidden sector mediator decaying to an invisible final state, and upper limits of the decay branching fraction for $X$ masses in the range 10-370 MeV/$c^2$ are reported for the first time, ranging from ${\cal O}(10^{-5})$ t…

Nuclear and High Energy PhysicsScalar (mathematics)FOS: Physical sciences01 natural sciences7. Clean energyNA62High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesheavy neutral leptonsDark sector NA62physics beyond Standard Model010306 general physicsPhysicsRange (particle radiation)Muonkaon decays010308 nuclear & particles physicsBranching fractionDark sectorSettore FIS/04Kaonslcsh:QC1-999Hidden sectorParticleHigh Energy Physics::ExperimentNeutrinoParticle Physics - Experimentlcsh:PhysicsLepton
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The search for dark matter gauge bosons with the Mainz Microtron

2011

Abstract A pilot experiment in the search for light gauge bosons at the spectrometer setup of the A1 collaboration at MAMI is presented. Light gauge bosons arise naturally in a wide range of theoretical approaches beyond the standard model and are in accordance with several pieces of experimental evidence not yet understood in the standard model. A first test measurement at MAMI showed that existing limits on the coupling of such a light gauge boson can be improved by nearly an order of magnitude by fixed target experiments at existing electron accelerators.

Nuclear physicsHidden sectorPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsSpectrometerPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDark matterTechnicolorMicrotronStandard ModelProgress in Particle and Nuclear Physics
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isotracer: An R package for the analysis of tracer addition experiments

2021

AbstractTracer addition experiments, particularly using isotopic tracers, are becoming increasingly important in a variety of studies aiming at characterizing the flows of molecules or nutrients at different levels of biological organization, from the cellular and tissue levels, to the organismal and ecosystem levels.We present an approach based on Hidden Markov Models (HMM) to estimate nutrient flow parameters across a network, and its implementation in the R package isotracer.The isotracer package is capable of handling a variety of tracer study designs, including continuous tracer drips, pulse experiments, and pulse-chase experiments. It can also take into account tracer decay when radio…

Nutrient flowRadionuclideR packageTRACERModel selectionEnvironmental scienceMontane ecologyBiological systemHidden Markov model
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Case in favor of the N*(1700)(3/2(-))

2013

Using an interaction extracted from the local hidden-gauge Lagrangians, which brings together vector and pseudoscalar mesons, and the coupled channels rho N (s wave), pi N (d wave), pi Delta (s wave), and pi Delta (d wave), we look in the region ofv root s = 1400-1850 MeV and find two resonances dynamically generated by the interaction of these channels, which are naturally associated to N*(1520)(3/2(-)) and N*(1700)(3/2(-)). N*(1700)(3/2(-)) appears neatly as a pole in the complex plane. The free parameters of the theory are chosen to fit the pi N (d-wave) data. Both the real and imaginary parts of the pi N amplitude vanish in our approach in the vicinity of this resonance, which is simila…

Partial-wave análisisPi-nIsobar-modelGauge bosonElectroproductionResonancesAmplitudesTransitionHidden local symmetryDynamics
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Observational constraints on decoupled hidden sectors

2016

We consider an extension of the Standard Model with a singlet sector consisting of a real (pseudo)scalar and a Dirac fermion coupled with the Standard Model only via the scalar portal. We assume that the portal coupling is weak enough for the singlet sector not to thermalize with the Standard Model allowing the production of singlet particles via the freeze-in mechanism. If the singlet sector interacts with itself sufficiently strongly, it may thermalize within itself, resulting in dark matter abundance determined by the freeze-out mechanism operating within the singlet sector. We investigate this scenario in detail. In particular, we show that requiring the absence of inflationary isocurva…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterScalar (mathematics)FOS: Physical sciencesParameter space114 Physical sciences01 natural sciencesStandard Modeldecouplingsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)ABELL 38270103 physical sciencesSinglet state010306 general physicsdark matter abundanceInflation (cosmology)PhysicsINTERACTING DARK-MATTERta114010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyextensions of the Standard ModelHidden sectorHigh Energy Physics - Phenomenologysinglet sectorCOSMOLOGICAL SIMULATIONSDirac fermionGALAXY CLUSTER 1E-0657-56symbols3.5 KEV LINEINTERACTION CROSS-SECTIONAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Reheating the Standard Model from a hidden sector

2016

We consider a scenario where the inflaton decays to a hidden sector thermally decoupled from the visible Standard Model sector. A tiny portal coupling between the hidden and the visible sectors later heats the visible sector so that the Standard Model degrees of freedom come to dominate the energy density of the Universe before Big Bang Nucleosynthesis. We find that this scenario is viable, although obtaining the correct dark matter abundance and retaining successful Big Bang Nucleosynthesis is not obvious. We also show that the isocurvature perturbations constituted by a primordial Higgs condensate are not problematic for the viability of the scenario.

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Ultimate fate of the universereheatingmedia_common.quotation_subjectDark matterUNIVERSEFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics114 Physical sciences01 natural sciencesdark matterdecouplingpimeä aineHigh Energy Physics - Phenomenology (hep-ph)INFLATIONBig Bang nucleosynthesis0103 physical sciencesDARK-MATTERELECTROWEAK VACUUM010306 general physicsmedia_commonPhysicsQuintom scenariota114STABILITY010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDecoupling (cosmology)InflatonHIGGSUniverseHidden sectorextensions of the Standard ModelHigh Energy Physics - Phenomenologyhidden sectorsSCALARAstrophysics - Cosmology and Nongalactic Astrophysics
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Icecube/DeepCore tests for novel explanations of the MiniBooNE anomaly

2019

While the low-energy excess observed at MiniBooNE remains unchallenged, it has become increasingly difficult to reconcile it with the results from other sterile neutrino searches and cosmology. Recently, it has been shown that non-minimal models with new particles in a hidden sector could provide a better fit to the data. As their main ingredients they require a GeV-scale $Z'$, kinetically mixed with the photon, and an unstable heavy neutrino with a mass in the 150 MeV range that mixes with the light neutrinos. In this letter we point out that atmospheric neutrino experiments (and, in particular, IceCube/DeepCore) could probe a significant fraction of the parameter space of such models by l…

Particle physicsSterile neutrinoPhotonPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsParameter space01 natural sciencesCosmologyHigh Energy Physics - ExperimentMiniBooNEHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHidden sectorHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentAnomaly (physics)NeutrinoThe European Physical Journal C
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Los prejuicios no percibidos y el caso Sócrates: un ejemplo paradigmático

2021

En un trabajo anterior defendimos que no se había prestado suficiente atención al procedimiento utilizado en el juicio contra Sócrates, sin que examináramos las causas de esa desatención. Ahora, tras analizarlas, llegamos a la conclusión de que ese procedimiento se habría malentendido completamente al haberse implementado un prejuicio no percibido. Habríamos extrapolado a ese procedimiento los presupuestos individualistas de los procedimientos vigentes hoy en día y, en consecuencia, habríamos estado sordos a lo que nos dice la tradición. Un ejemplo de sordera que podría ser muy útil para detectar otros casos semejantes de implementación de prejuicios no percibidos. In a previous work, we de…

Philosophyhidden prejudicestrial proceduressorderaprocedimiento judicialdeafness:CIENCIAS JURÍDICAS Y DERECHO [UNESCO]SócratesGadamerUNESCO::CIENCIAS JURÍDICAS Y DERECHOprejuicios no percibidosLawSocrates
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