Search results for "interaction [electron p]"

showing 10 items of 282 documents

Calculated Line Broadening Coefficients in the nu2 Band of CH3D Perturbed by Helium

2003

International audience; Line broadening coefficients have been calculated, at room temperature, for lines in the P and R branches of the nu2 band of monodeuterated methane. A properly symmetrized semiclassical model with parabolic relative trajectories has been used. Two interaction potential models have been considered. The first is a Lennard-Jones type atom-atom potential, while the second one was derived from ab initio calculations. The calculated line widths were compared to the available experimental data and a satisfactory agreement was found, although the model contains no other adjustable parameters than the four atomic Lennard-Jones ones. Nonetheless, failures of calculations have …

PhysicsLine broadening coefficients010304 chemical physicsCondensed matter physics[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Semiclassical physicschemistry.chemical_elementQuantum numberSemiclassical calculations01 natural sciences7. Clean energyAtomic and Molecular Physics and OpticsCH3DInteraction potentialchemistry[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Ab initio quantum chemistry methods0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysical and Theoretical ChemistryAtomic physics010303 astronomy & astrophysicsSpectroscopyHeliumLine (formation)
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ScalarΛNandΛΛinteraction in a chiral unitary approach

2006

We study the central part of the {lambda}N and {lambda}{lambda} potential by considering the correlated and uncorrelated two-meson exchange in addition to the {omega} exchange contribution. The correlated two-meson exchange is evaluated within a chiral unitary approach. We find that a short-range repulsion is generated by the correlated two-meson potential, which also produces an attraction in the intermediate-distance region. The uncorrelated two-meson exchange produces a sizable attraction in all cases that is counterbalanced by the {omega} exchange contribution.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyScalar (mathematics)LambdaLambda baryonUnitary stateOmegaUncorrelatedQuantum mechanicsHigh Energy Physics::ExperimentChirality (chemistry)Interaction rangePhysical Review C
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Ultra-long-lived particles searches with MATHUSLA

2018

Abstract There are many theoretical motivations for long-lived particle (LLP) signals at the LHC in a comprehensive survey of Standard Model (SM) extensions. LLPs are a common prediction of a wide range of theories that address unsolved fundamental mysteries such as naturalness, dark matter, baryogenesis and neutrino masses, and represent a natural and generic possibility for physics beyond the SM (BSM). MATHUSLA (MAssive Timing Hodoscope for Ultra Stable neutraL pArticles) is a proposal for a minimally instrumented, large-volume surface detector to detect such LLPs. The MATHUSLA surface detector will consist of an air-filled decay volume surrounded by charged particles detectors (top, bott…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderInteraction pointPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDark matterDetectorSettore FIS/01 - Fisica SperimentaleLong-lived particle01 natural sciences7. Clean energyCharged particleBaryogenesisLong-lived particlesTracking detectorsHodoscope0103 physical sciencesRPCNeutrino010306 general physicsInstrumentation
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New ALICE detectors for Run 3 and 4 at the CERN LHC

2020

Abstract Run 3 at the CERN LHC is scheduled to start in March 2021. In preparation for this new data taking period the ALICE experiment is making major modifications to its subsystems and is introducing three new detectors: the new Inner Tracking System, the Muon Forward Tracker, and the Fast Interaction Trigger. The new detectors will enhance tracking, especially at low transverse momenta, improve vertexing, provide the required triggering, fast timing, luminosity, and forward multiplicity functionality. For instance, it will be possible to measure beauty from displaced J/ ψ vertices down to transverse momenta p T ∼ 0 and improve precision for the ψ (2S) measurements. The upgraded ALICE wi…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonLuminosity (scattering theory)Large Hadron Colliderbusiness.industryPhysics::Instrumentation and DetectorsDetectortutkimuslaitteetMultiplicity (mathematics)Tracking systemhiukkasfysiikkaTracking (particle physics)ALICE upgradeinner tracking systemmuon forward trackerALICE (propellant)businessInstrumentationHL-LHCfast interaction trigger
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On the variational approach to Jastrow correlations in nuclei

1973

The variational equation determining the Jastrow correlation function is investigated with particular emphasis on the healing problem for both nuclear matter and finite nuclei. The consequences of several healing conditions are discussed. Furthermore, influences from the choice of the single particle basis and from long range correlations are studied and are found to be small in the short range region.

PhysicsNuclear and High Energy PhysicsRange (mathematics)Correlation function (statistical mechanics)Basis (linear algebra)Variational equationQuantum electrodynamicsNuclear TheoryNuclear fusionStatistical physicsNuclear matterInteraction rangeZeitschrift für Physik A Hadrons and nuclei
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Neutron emission from electromagnetic dissociation of Pb nuclei at $\sqrt {s_{NN}} = 2.76$ TeV measured with the ALICE ZDC

2014

The ALICE Zero Degree Calorimeter system (ZDC) is composed of two identical sets of calorimeters, placed at opposite sides with respect to the interaction point, 114 meters away from it, complemented by two small forward electromagnetic calorimeters (ZEM). Each set of detectors consists of a neutron (ZN) and a proton (ZP) ZDC. They are placed at zero degrees with respect to the LHC axis and allow to detect particles emitted close to beam direction, in particular neutrons and protons emerging from hadronic heavy-ion collisions (spectator nucleons) and those emitted from electromagnetic processes. For neutrons emitted by these two processes, the ZN calorimeters have nearly 100% acceptance. Du…

PhysicsParticle physicsLarge Hadron ColliderInteraction pointProtonNeutron emissionPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaPhysicsQC1-999HadronNuclear Theory7. Clean energyCalorimeterNuclear physicsPhysics and Astronomy (all)NeutronHigh Energy Physics::ExperimentNuclear Physics - ExperimentNucleonNuclear Experiment
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Search for Long-Lived Particles ine+e−Collisions

2015

We present a search for a neutral, long-lived particle L that is produced in e^+e^− collisions and decays at a significant distance from the e^+e^− interaction point into various flavor combinations of two oppositely charged tracks. The analysis uses an e^+e^− data sample with a luminosity of 489.1  fb^(−1) collected by the BABAR detector at the Υ(4S), Υ(3S), and Υ(2S) resonances and just below the Υ(4S). Fitting the two-track mass distribution in search of a signal peak, we do not observe a significant signal, and set 90% confidence level upper limits on the product of the L production cross section, branching fraction, and reconstruction efficiency for six possible two-body L decay modes …

PhysicsParticle physicsLuminosity (scattering theory)Mass distributionInteraction pointBranching fractionElectron–positron annihilationHadronGeneral Physics and AstronomyFunction (mathematics)7. Clean energyNuclear physicsMass spectrumHigh Energy Physics::ExperimentPhysical Review Letters
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Measurement of the single π0 production rate in neutral current neutrino interactions on water

2018

The single π0 production rate in neutral current neutrino interactions on water in a neutrino beam with a peak neutrino energy of 0.6 GeV has been measured using the POD, one of the subdetectors of the T2K near detector. The production rate was measured for data taking periods when the POD contained water (2.64×1020 protons-on-target) and also periods without water (3.49×1020 protons-on-target). A measurement of the neutral current single π0 production rate on water is made using appropriate subtraction of the production rate with water in from the rate with water out of the target region. The subtraction analysis yields 106±41±69 signal events where the uncertainties are statistical (stat.…

PhysicsParticle physicsNeutral currentPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorFluxInteraction energy01 natural sciences7. Clean energyNuclear physicsCross section (physics)0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentNeutrinoNuclear Experiment010306 general physicsNucleonPhysical Review D
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Harmonic oscillator model for the atom-surface Casimir-Polder interaction energy

2012

In this paper we consider a quantum harmonic oscillator interacting with the electromagnetic radiation field in the presence of a boundary condition preserving the continuous spectrum of the field, such as an infinite perfectly conducting plate. Using an appropriate Bogoliubov-type transformation we can diagonalize exactly the Hamiltonian of our system in the continuum limit and obtain non-perturbative expressions for its ground-state energy. From the expressions found, the atom-wall Casimir-Polder interaction energy can be obtained, and well-know lowest-order results are recovered as a limiting case. Use and advantage of this method for dealing with other systems where perturbation theory …

PhysicsQuantum PhysicsAtom-field interactionsAnharmonicityContinuous spectrumFOS: Physical sciencesInteraction energyAtomic and Molecular Physics and OpticsCasimir effectsymbols.namesakeCasimir-Polder energyQuantum harmonic oscillatorQuantum mechanicssymbolsBoundary value problemQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Harmonic oscillatorPhysical Review A
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A microscopic approach to Casimir and Casimir-Polder forces between metallic bodies

2014

We consider the Casimir-Polder interaction energy between a metallic nanoparticle and a metallic plate, as well as the Casimir interaction energy between two macroscopic metal plates, in terms of the many-body dispersion interactions between their constituents. Expressions for two- and three-body dispersion interactions between the microscopic parts of a real metal are first obtained, both in the retarded and non-retarded limits. These expressions are then used to evaluate, a compare each other, the overall two- and three-body contributions to the macroscopic Casimir-Polder and Casimir force, by summing up the contributions from the microscopic constituents of the bodies (metal nanoparticle…

PhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsFOS: Physical sciencesGeneral Physics and AstronomyNanoparticlemany-body interactionsCasimir-Polder interactionInteraction energyCasimir effectMetalCasimir effectClassical mechanicsvisual_artMesoscale and Nanoscale Physics (cond-mat.mes-hall)Dispersion (optics)Convergence (routing)visual_art.visual_art_mediumRapidityQuantum Physics (quant-ph)Metal nanoparticles
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