Search results for "MSS"

showing 10 items of 2513 documents

The effect of magnetic field strength on the time evolution of high energy bremsstrahlung radiation created by an electron cyclotron resonance ion so…

2009

Abstract An electron cyclotron resonance (ECR) ion source is one of the most used ion source types for high charge state heavy ion production. In ECR plasma the electrons are heated by radio frequency microwaves in order to provide ionization of neutral gases. As a consequence, ECR heating also generates very high electron energies (up to MeV region) which can produce a vast amount of bremsstrahlung radiation causing problems with radiation shielding and heating superconducting cryostat of an ECR ion source. To gain information about the time evolution of the electron energies in ECR plasma radial bremsstrahlung measurements were performed. JYFL 14 GHz ECR ion source was operated in pulsed …

PhysicsNuclear and High Energy PhysicsArgonBremsstrahlungchemistry.chemical_elementPlasmaElectronElectron cyclotron resonanceIon sourcechemistryPhysics::Plasma PhysicsIonizationPhysics::Accelerator PhysicsAtomic physicsInstrumentationIon cyclotron resonanceNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Neutrino Bremsstrahlung from electrons in neutron star crusts

2001

The process of v (v) over bar Bremsstrahlung via electron scattering off nuclei in the crust of a cooling neutron star is studied within the Random Phase Approximation. We show that the electromagnetic plasma screens the vector weak coupling of electrons with the neutrino field. This screening effect takes place in both the crystalline and liquid phase of the neutron star crust, when the momentum carried out by the neutrino pair is smaller than the inverse Debye screening distance of the electrons. This condition holds in the crust volume at temperatures and densities where the electron Bremsstrahlung dominates the neutrino production. As a result, the vector weak current contribution to th…

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaDegenerate energy levelsBremsstrahlungElectronAstrophysicsRadiationPartícules (Física nuclear)Nuclear physicsNeutron starEmissivityFísica nuclearNeutrinoBar (unit)
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Incoherent bremsstrahlung in nuclei

1994

We have studied the processes A(e, e′γ)X in nuclei, or incoherent bremsstrahlung, and determined expressions for the cross section in terms of the same nuclear response functions RL, RT, which appear in inclusive electron scattering (e, e′) in nuclei. Calculations of the cross sections are carried out using a Fermi gas model, complemented by the local-density approximation, to evaluate the response functions. We have carried out a study which shows that the reaction can be used to determine reliably the response functions from experimental data. On the other hand we have compared the incoherent bremsstrahlung with the coherent one in order to see the limits to the tagging technique, which p…

PhysicsNuclear and High Energy PhysicsCross section (physics)PhotonScatteringIncoherent scatterBremsstrahlungElectronAtomic physicsFermi gasElectron scatteringComputational physicsNuclear Physics A
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Electro-produced slow positrons

1989

During the last 6 years it has been demonstrated that electro-produced intense beams of slow positrons are possible. High energy electrons from an accelerator generate bremsstrahlung in a thick conversion target of high element number Z. The photons produce electronpositron pairs and a small fraction of the positrons may be moderated to thermal energies. A review is given of the existing slow positron beam lines using this technique. At accelerator energies of 100 MeV total conversion efficiencies of several slow positrons per 106 primary electrons have been obtained, resulting in average intensities of several 109 slow positrons per second or more than 105 slow positrons in pulses having a…

PhysicsNuclear and High Energy PhysicsHigh energyPhotonBremsstrahlungElectronCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIntensity (physics)Nuclear physicsPositronThermalPhysics::Accelerator PhysicsPhysical and Theoretical ChemistryAtomic physicsOrder of magnitudeHyperfine Interactions
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The selection and performance of diamond radiators used in coherent bremsstrahlung experiments

2005

The bremsstrahlung emitted as a result of scattering electrons in thin diamond crystals provides a useful source of high energy photons for use in photonuclear experiments, since the coherent bremsstrahlung produced is linearly polarized. Techniques for selecting the most favorable diamonds have been investigated. These are optical polaroid analysis, X-ray topography and rocking curve measurements. The diamonds are characterized with a view to determining their performance as radiators, and bremsstrahlung spectra from a diamond radiator used at the Mainz MAMI-B facility are presented. The changes caused by high energy electrons to the crystal properties of the diamond and to the resulting c…

PhysicsNuclear and High Energy PhysicsHigh energybusiness.industryScatteringLinear polarizationAstrophysics::High Energy Astrophysical PhenomenaBremsstrahlungDiamondElectronengineering.materialSpectral lineOpticsRadiator (engine cooling)engineeringAtomic physicsNuclear ExperimentbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Experimental study of theγp→ηpreaction with the Crystal Ball detector at the Mainz Microtron (MAMI-C)

2010

The gamma p - = W >= 1.87 GeV). Bremsstrahlung photons produced by the 1.5-GeV electron beam of the Mainz Microtron MAMI-C and momentum analyzed by the Glasgow tagging spectrometer were used for the eta-meson production. Our accumulation of 3.8 x 10(6) gamma p -< eta p -< 3 pi(0) p -< 6 gamma p events allows a detailed study of the reaction dynamics. The gamma p -< eta p differential cross sections were determined for 120 energy bins and the full range of the production angles. Our data show a dip near W = 1680 MeV in the total cross section caused by a substantial dip in eta production at forward angles. The data are compared to predictions of previous SAID and MAID partial-wave analyses a…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaPartial wave analysisHadronBremsstrahlung01 natural sciencesNuclear physicsParticle decay0103 physical sciencesNuclear Experiment010306 general physicsNucleonMicrotronCrystal BallPhysical Review C
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Physical mechanism of the linear beam-size effect at colliders

1996

We present qualitative but precise description of the linear beam-size effect predicted for the processes in which unstable but long--living particles collide with each other. We derive physically pronounced equation for the events rate which proves that the linear beam-size effect corresponds to the scattering of one beam of particles on the decay products of the other. We compare this linear beam-size effect with the known logarithmic beam-size effect measured in the experiments on a single bremsstrahlung at VEPP-4 and HERA.

PhysicsNuclear and High Energy PhysicsMuonLogarithmScatteringBremsstrahlungFOS: Physical sciencesHERANuclear physicsMechanism (engineering)Beam sizeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentBeam (structure)
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Discarding a 125 GeV heavy Higgs in an MSSM model with explicit CP-violation

2016

AbstractCurrent experimental constraints prove being enough to rule out the possibility of the mh∼125 GeV Higgs found at LHC being a heavy Higgs in a general MSSM context, even with explicit CP violation in the Higgs potential. Differently than what has been done in prior studies, we perform this job analitically, with expressions related to a few observables. Te relevance of ττ production through Higgs and BR(B→Xsγ) processes is emphasized, since they are enough to erase the possibility of finding an MSSM neutral Higgs lighter than the scalar discovered at LHC.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar (mathematics)ObservableContext (language use)CP-violationtau-tau01 natural scienceslight Higgs0103 physical sciencesHiggs bosonCP violationHigh Energy Physics::Experiment010306 general physicsMSSMNuclear and Particle Physics Proceedings
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Low-mass dileptons at high momenta in ultra-relativistic heavy-ion collisions

1992

Abstract We calculate the emission rate of low-mass dileptons at high momenta from a quark-gluon plasma. We find a large enhancement compared with the naive Born rate. Numerical estimates for relativistic heavy ions collisions at RHIC and LHC suggest, however, that the thermal signal is dominated by the background coming from meson decays and from hadronic bremsstrahlung.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronBremsstrahlungElementary particleIonNuclear physicsQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear ExperimentLeptonNuclear Physics B
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Quasifree photoproduction of eta mesons off protons and neutrons

2014

Differential and total cross sections for the quasifree reactions $\ensuremath{\gamma}p\ensuremath{\rightarrow}\ensuremath{\eta}p$ and $\ensuremath{\gamma}n\ensuremath{\rightarrow}\ensuremath{\eta}n$ have been determined at the MAMI-C electron accelerator by using a liquid deuterium target. Photons were produced via bremsstrahlung from the 1.5 GeV incident electron beam and energy tagged with the Glasgow photon tagger. Decay photons of the neutral decay modes $\ensuremath{\eta}\ensuremath{\rightarrow}2\ensuremath{\gamma}$ and $\ensuremath{\eta}\ensuremath{\rightarrow}3{\ensuremath{\pi}}^{0}\ensuremath{\rightarrow}6\ensuremath{\gamma}$ and coincident recoil nucleons were detected in a combin…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryProtonMesonNuclear TheoryBremsstrahlung7. Clean energyHigh Energy Physics - ExperimentNuclear physicsRecoilNeutronNuclear ExperimentNucleonNuclear ExperimentEnergy (signal processing)Crystal BallPHYSICAL REVIEW C
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