Search results for "Nuclear and high energy physics"

showing 10 items of 8241 documents

Testing for new physics with low-energy anti-neutrino sources: LAMA as a case study

1998

Some electroweak models with extended neutral currents, such as those based on the $E_6$ group, lead to an increase of the $\bar{\nu}-e$ scattering cross section at energies below 100 keV. We propose to search for the heavy Z' boson contribution in an experiment with a high-activity artificial neutrino source and with a large-mass detector. We present the case for the LAMA experiment with a large NaI(Tl) detector located at the Gran Sasso underground laboratory. The neutrino flux is known to within a one percent accuracy, in contrast to the reactor case and one can reach lower neutrino energies. Both features make our proposed experiment more sensitive to extended gauge models, such as the …

GAUGE BOSONSNuclear and High Energy PhysicsParticle physicsVIOLATIONPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelFOS: Physical sciencesFluxMASSSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Phenomenology (hep-ph)GAUGE BOSONS; MASS; CONSTRAINTS; SCATTERING; VIOLATION; SEARCHSEARCHSCATTERINGSensitivity (control systems)BosonPhysicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyElectroweak interactionDetectorCONSTRAINTSFísicaGauge (firearms)High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoNuclear Physics B
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Hadronic calibration of the ATLAS liquid argon end-cap calorimeter in the pseudorapidity region in beam tests

2004

Abstract A full azimuthal φ -wedge of the ATLAS liquid argon end-cap calorimeter has been exposed to beams of electrons, muons and pions in the energy range 6 GeV ⩽ E ⩽ 200 GeV at the CERN SPS. The angular region studied corresponds to the ATLAS impact position around the pseudorapidity interval 1.6 | η | 1.8 . The beam test setup is described. A detailed study of the performance is given as well as the related intercalibration constants obtained. Following the ATLAS hadronic calibration proposal, a first study of the hadron calibration using a weighting ansatz is presented. The results are compared to predictions from Monte Carlo simulations, based on GEANT 3 and GEANT 4 models.

GEANT-3PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsMonte Carlo methodHadron01 natural sciences7. Clean energyCalorimeterNuclear physicsmedicine.anatomical_structureAtlas (anatomy)Pseudorapidity0103 physical sciencesmedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Coupled theoretical and experimental studies for the radiation hardening of silica-based optical fibers

2014

International audience; We applied theoretical and experimental spectroscopy tools to ad hoc silica-based "canonical" samples to characterize the influence of several dopants and of some drawing process parameters on their radiation sensitivities. We present in this paper, the recent advances and results occurring from our coupled approach. On the experimental side, we studied the doping influence on the response of optical fibers and showed that changing the drawing parameters has a negligible influence on the fiber response in the case of specialty fibers. We focus mainly on the ${rm SiE}^prime$ defect that is observed through Electron Paramagnetic Resonance (EPR) measurements in all cano…

GW approximationNuclear and High Energy PhysicsOptical fiberMaterials scienceoptical fibersSiliconchemistry.chemical_element02 engineering and technology01 natural sciencesMolecular physics030218 nuclear medicine & medical imaginglaw.invention03 medical and health sciences[SPI]Engineering Sciences [physics]0302 clinical medicinelaw0103 physical sciencespoint defectsElectrical and Electronic Engineering010306 general physicsElectron paramagnetic resonanceSpectroscopydefectsdensity functional theoryCondensed matter physics010308 nuclear & particles physicsSettore FIS/01 - Fisica Sperimentale021001 nanoscience & nanotechnologyNuclear Energy and EngineeringchemistryUnpaired electronsilicaradiation effectsDensity functional theorytheoretical spectroscopyAb initio calculationsLocal-density approximation0210 nano-technology
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Geometric inequivalence of metric and Palatini formulations of General Relativity

2020

Projective invariance is a symmetry of the Palatini version of General Relativity which is not present in the metric formulation. The fact that the Riemann tensor changes nontrivially under projective transformations implies that, unlike in the usual metric approach, in the Palatini formulation this tensor is subject to a gauge freedom, which allows some ambiguities even in its scalar contractions. In this sense, we show that for the Schwarzschild solution there exists a projective gauge in which the (affine) Kretschmann scalar, K≡R R , can be set to vanish everywhere. This puts forward that the divergence of curvature scalars may, in some cases, be avoided by a gauge transformation of the …

General RelativityNuclear and High Energy PhysicsRiemann curvature tensorFísica-Modelos matemáticosGeneral relativityScalar (mathematics)FOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmology//purl.org/becyt/ford/1 [https]symbols.namesakeGeneral Relativity and Quantum Cosmology0103 physical sciencesSchwarzschild metricFísica matemáticaGauge theoryTensorGeometric inequivalence010306 general physicsMathematical PhysicsMathematical physicsPhysics010308 nuclear & particles physicsKretschmann scalar//purl.org/becyt/ford/1.3 [https]Mathematical Physics (math-ph)lcsh:QC1-999Symmetry (physics)symbolslcsh:PhysicsPhysics Letters
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Three pseudoscalar meson production ine+e−annihilation

2013

Conversations with German Rodrigo on the topic of this paper are warmly acknowledged. We would like to thank Henryk Czyz for fruitful discussions on context of MC PHOKHARA 7.0. We also wish to thank Michael R. Pennington for a careful reading of our manuscript and for his suggestions. Lingyun Dai thanks the China Scholarship Council for their support. This research has been supported in part by the funds of the Polish National Science Centre under decisions DEC-2012/04/M/ST2/00240 and DEC-2011/03/B/ST2/00107 (O. S.) and by the Spanish Government and ERDF funds from the EU Commission [Grants No. FPA2007-60323, No. FPA2011-23778, No. CSD2007-00042 (Consolider Project CPAN)]. This paper has be…

GermanPhysicsNuclear and High Energy PhysicsScholarshipGovernmentParticle physicsEffective lagrangianlanguageLibrary scienceContext (language use)CommissionPseudoscalar mesonlanguage.human_languagePhysical Review D
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Defects in glasses

1995

Abstract The absence of long range order in the glass structure allows to define only point defects in these materials. They are: 1) intrinsic defects—atomic size local deviation from short range order; 2) impurity defects—isolated impurity atoms or ions in the glass network; 3) intrinsic impurity defects—complexes consisting of the impurity atoms chemically bonded to one of the intrinsic defect atoms. The latter defects are characteristic for the doped glasses. Presence of point defects in glasses introduces new spectroscopic properties of these solid materials. Defect generation, interaction and recombination reactions resulting from the external influence causes the glass spectroscopic p…

Glass structureNuclear and High Energy PhysicsRange (particle radiation)RadiationMaterials scienceAbsorption spectroscopyCondensed matter physicsbusiness.industryDopingCondensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksCrystallographic defectIonOpticsImpurityGeneral Materials SciencebusinessRecombinationRadiation Effects and Defects in Solids
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Observable flavor violation from spontaneous lepton number breaking

2022

We propose a simple model of spontaneous lepton number violation with potentially large flavor violating decays, including the possibility that majoron emitting decays, such as $\mu \to e \, J$, saturate the experimental bounds. In this model the majoron is a singlet-doublet admixture. It generates a type-I seesaw for neutrino masses and contains also a vector-like lepton. As a by-product, the model can explain the anomalous $(g-2)_{\mu}$ in parts of its parameter space, where one expects that the branching ratio of the Higgs to muons is changed with respect to Standard Model expectations. However, the explanation of the muon $g-2$ anomaly would lead to tension with recent astrophysical bou…

Global SymmetriesHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. RadioactivityComputer Science::Information RetrievalBeyond Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesNeutrino PhysicsHigh Energy Physics::ExperimentQC770-798Journal of High Energy Physics
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The Inverse Seesaw Family: Dirac And Majorana

2021

After developing a general criterion for deciding which neutrino mass models belong to the category of inverse seesaw models, we apply it to obtain the Dirac analogue of the canonical Majorana inverse seesaw model. We then generalize the inverse seesaw model and obtain a class of inverse seesaw mechanisms both for Majorana and Dirac neutrinos. We further show that many of the models have double or multiple suppressions coming from tiny symmetry breaking "$\mu$-terms". These models can be tested both in colliders and with the observation of lepton flavour violating processes.

Global SymmetriesPhysicsNuclear and High Energy PhysicsClass (set theory)010308 nuclear & particles physicsDirac (video compression format)High Energy Physics::PhenomenologyFOS: Physical sciencesInverse01 natural sciencesMAJORANATheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryBeyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physicsLepton
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Stimulated transitions in resonant atom Majorana mixing

2018

Massive neutrinos demand to ask whether they are Dirac or Majorana particles. Majorana neutrinos are an irrefutable proof of physics beyond the Standard Model. Neutrinoless double electron capture is not a process but a virtual $\Delta L = 2$ mixing between a parent $^AZ$ atom and a daughter $^A(Z-2)$ excited atom with two electron holes. As a mixing between two neutral atoms and the observable signal in terms of emitted two-hole X-rays, the strategy, experimental signature and background are different from neutrinoless double beta decay. The mixing is resonantly enhanced for almost degeneracy and, under these conditions, there is no irreducible background from the standard two-neutrino cha…

Global SymmetriesPhysicsNuclear and High Energy Physicseducation.field_of_study010308 nuclear & particles physicsElectron capturePopulationFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Double beta decayExcited stateBeyond Standard Model0103 physical sciencesAtomlcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrinoAtomic physics010306 general physicseducationGround stateJournal of High Energy Physics
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Limits on neutral Higgs boson production in the forward region in $pp$ collisions at $\sqrt{s} = 7$ TeV

2013

Limits on the cross-section times branching fraction for neutral Higgs bosons, produced in p p collisions at root s = 7 TeV, and decaying to two tau leptons with pseudorapidities between 2.0 and 4.5, are presented. The result is based on a dataset, corresponding to an integrated luminosity of 1.0 fb(-1), collected with the LHCb detector. Candidates are identified by reconstructing final states with two muons, a muon and an electron, a muon and a hadron, or an electron and a hadron. A model independent upper limit at the 95% confidence level is set on a neutral Higgs boson cross-section times branching fraction. It varies from 8.6 pb for a Higgs boson mass of 90 GeV to 0.7 pb for a Higgs bos…

GravitacióSEARCH; MSSM; LHCHadronStandard-model Higgs boson7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Teoria quànticaNuclear ExperimentQCBosonPhysicsHiggs physicsQuantum field theoryHiggs bosonProduction (computer science)Física nuclearLHCHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesParticle Physics - ExperimentGravitationParticle physicsTeoria quàntica de campsNuclear and High Energy PhysicsFOS: Physical sciencesStandard-model Higgs bosons; Supersymmetric Higgs bosons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesHadronsPartícules (Física nuclear)Standard ModelSEARCH0103 physical sciences010306 general physicsLarge Hadron Collider (France and Switzerland)Standard-model Higgs bosonsMuonHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionComputer Science::Information RetrievalHadron-Hadron Scattering; Higgs physicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsHiggs physicSupersymmetric Higgs bosonSupersymmetric Higgs bosonsQuantum theoryHadron-Hadron Scattering; Higgs physics; Nuclear and High Energy PhysicsHigh Energy Physics::ExperimentMSSMLepton
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