Search results for "velocity"

showing 10 items of 881 documents

High-precision momentum measurements of projectile fragments in Sn+Sn collisions at 1·A GeV

2012

Production cross-sections and longitudinal velocity distributions of the projectilelike residues produced in peripheral and mid-peripheral reactions 112Sn + 112Sn and 124Sn + 124Sn both at an incident beam energy of 1 A GeV were measured with the high-resolution magnetic spectrometer, the Fragment Separator of GSI. For both reactions the characteristics of the velocity distributions and nuclide production cross-sections were determined for residues with nuclear charge Z 10. A comparison of the results of the two reactions is presented and the results are studied in the frame of dynamical transport calculations coupled with a statistical multifragmentation code. In mid-peripheral collisions …

Nuclear Theoryscatteringmulti-fragmentationmomentum dependenceyieldmagnetic spectrometerheavy ionabrasion-ablationfragmentationmean field approximationtransport theory1 GeV/nucleonfysiikkaNuclear Experimentydinfysiikkanuclidevelocity spectrumDarmstadt SISequation of stateexperimental results
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Round Robin computer simulation of ejection probability in sputtering

1989

Abstract We have studied the ejection of a copper atom through a planar copper surface as a function of recoil velocity and depth of origin. Results were obtained from six molecular dynamics codes, four binary collision lattice simulation codes, and eight Monte Carlo codes. Most results were found with a Born-Mayer interaction potential between the atoms with Gibson 2 parameters and a planar surface barrier, but variations on this standard were allowed for, as well as differences in the adopted cutoff radius for the interaction potential, electronic stopping, and target temperature. Large differences were found between the predictions of the various codes, but the cause of these differences…

Nuclear and High Energy PhysicsChemistryBinary number02 engineering and technology021001 nanoscience & nanotechnologyCollision01 natural sciencesComputational physicsMolecular dynamicsPlanarSputteringLattice (order)0103 physical sciencesRecoil velocityCutoffStatistical physics010306 general physics0210 nano-technologyInstrumentation
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DNP in MRI: an in-bore approach at 1.5 T.

2011

Abstract We have used liquid state (“Overhauser”) Dynamic Nuclear Polarization (DNP) to significantly enhance the signal to noise ratio (SNR) of Magnetic Resonance Imaging (MRI). For the first time this was achieved by hyperpolarizing directly in the MRI-scanner field of 1.5 T in continuous flow mode and immediately delivering the hyperpolarized substance to the imaging site to ensure maximum contrast between hyperpolarized sample and sample at thermal polarization. We achieve a maximum absolute signal enhancement factor of 98; while the hyperpolarized sample is transported at a flow rate of up to 30 ml/h yielding an average flow speed up to 470 mm/s over a distance of approximately 80 mm. …

Nuclear and High Energy PhysicsContrast enhancementMagnetic Resonance Spectroscopymedicine.diagnostic_testContinuous flowChemistryPhantoms ImagingBiophysicsMagnetic resonance imagingSignal-To-Noise RatioCondensed Matter PhysicsPolarization (waves)BiochemistryMagnetic Resonance ImagingVolumetric flow rateSignal enhancementCyclic N-OxidesLiquid stateNuclear magnetic resonanceFlow velocitymedicineImage Processing Computer-AssistedSpin LabelsMicrowavesCopperJournal of magnetic resonance (San Diego, Calif. : 1997)
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A Time Projection Chamber with GEM-Based Readout

2016

For the International Large Detector concept at the planned International Linear Collider, the use of time projection chambers (TPC) with micro-pattern gas detector readout as the main tracking detector is investigated. In this paper, results from a prototype TPC, placed in a 1 T solenoidal field and read out with three independent GEM-based readout modules, are reported. The TPC was exposed to a 6 GeV electron beam at the DESY II synchrotron. The efficiency for reconstructing hits, the measurement of the drift velocity, the space point resolution and the control of field inhomogeneities are presented.

Nuclear and High Energy PhysicsDrift velocityPhysics - Instrumentation and DetectorsInternational Linear ColliderMicropattern gaseous detectors (MPGD)Physics::Instrumentation and DetectorsFOS: Physical sciencesTracking (particle physics)01 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Gas electron multipliers (GEM)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]International Large Detector (ILD)electron: irradiationtracking detector[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationspatial resolution[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Physicsmagnetic field: spatial distributionInternational Linear Collider (ILC)Time projection chamber010308 nuclear & particles physicsILD detectorDetectordrift velocityDESYInstrumentation and Detectors (physics.ins-det)Synchrotrontime projection chamberefficiencygas electron multiplierGas electron multiplierPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentTime projection chambers (TPC)
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Sizeable beta-strength in $^{31}$Ar (β3p) decay

2014

5 pags. ; 7 figs. ; Open Access funded by SCOAP3 - Sponsoring Consortium for Open Access Publishing in Particle Physics

Nuclear and High Energy PhysicsFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesNuclear physicsESPECTROSCOPÍA0103 physical sciencesNuclear Physics - ExperimentBeta (velocity)Nuclear Experiment (nucl-ex)010306 general physicsFÍSICA NUCLEARNuclear ExperimentPhysicsta114Isotope010308 nuclear & particles physicsIsotopes of chlorineIsotopes of argonSPECTROSCOPICBeta decaylcsh:QC1-999DESINTEGRATION3. Good healthFísica nuclearHigh Energy Physics::ExperimentAtomic physicsEMISSIONlcsh:PhysicsFÍSICAEnergy (signal processing)ExcitationRadioactive decay
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New method for calculating electromagnetic effects in semileptonic beta-decays of mesons

2020

We construct several classes of hadronic matrix elements and relate them to the low-energy constants in Chiral Perturbation Theory that describe the electromagnetic effects in the semileptonic beta decay of the pion and the kaon. We propose to calculate them using lattice QCD, and argue that such a calculation will make an immediate impact to a number of interesting topics at the precision frontier, including the outstanding anomalies in $|V_{us}|$ and the top-row Cabibbo-Kobayashi-Maskawa matrix unitarity.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryelectromagnetic [effect]MesonNuclear TheoryHigh Energy Physics::LatticeHadronFOS: Physical scienceschiral [perturbation theory]anomalyLattice QCD01 natural sciences530High Energy Physics - ExperimentNuclear Theory (nucl-th)Matrix (mathematics)High Energy Physics - Experiment (hep-ex)Kaon PhysicsPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBeta (velocity)lcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530Precision QEDNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologysemileptonic decay [meson]lattice field theorysemileptonic decay [pi]Lattice QCDHigh Energy Physics - PhenomenologyChiral Lagrangianslcsh:QC770-798High Energy Physics::Experimentunitarity [CKM matrix]
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Do T asymmetries for neutrino oscillations in uniform matter have a CP-even component?

2019

Observables of neutrino oscillations in matter have, in general, contributions from the effective matter potential. It contaminates the CP violation asymmetry adding a fake effect that has been recently disentangled from the genuine one by their different behavior under T and CPT. Is the genuine T-odd CPT-invariant component of the CP asymmetry coincident with the T asymmetry? Contrary to CP, matter effects in uniform matter cannot induce by themselves a non-vanishing T asymmetry; however, the question of the title remained open. We demonstrate that, in the presence of genuine CP violation, there is a new non-vanishing CP-even, and so CPT-odd, component in the T asymmetry in matter, which i…

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFOS: Physical sciencesDiscrete Symmetries01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityBeta (velocity)010306 general physicsNeutrino oscillationMixing (physics)media_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyObservableHigh Energy Physics - PhenomenologyCP violationlcsh:QC770-798CP violationHigh Energy Physics::ExperimentNeutrinoEnergy (signal processing)Journal of High Energy Physics
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Observation and applications of single-electron charge signals in the XENON100 experiment

2014

The XENON100 dark matter experiment uses liquid xenon in a time projection chamber (TPC) to measure xenon nuclear recoils resulting from the scattering of dark matter Weakly Interacting Massive Particles (WIMPs). In this paper, we report the observation of single-electron charge signals which are not related to WIMP interactions. These signals, which show the excellent sensitivity of the detector to small charge signals, are explained as being due to the photoionization of impurities in the liquid xenon and of the metal components inside the TPC. They are used as a unique calibration source to characterize the detector. We explain how we can infer crucial parameters for the XENON100 experim…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsDrift velocity[PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]Physics::Instrumentation and DetectorsDark matterchemistry.chemical_elementFOS: Physical sciencesdouble phase TPC01 natural sciencesdark matterHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)XenonWIMPdouble phase TPC; photoionization; single electron; xenon0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsphotoionizationInstrumentation and Methods for Astrophysics (astro-ph.IM)PhysicsTime projection chamber010308 nuclear & particles physicsScatteringDetectorAstrophysics::Instrumentation and Methods for AstrophysicsInstrumentation and Detectors (physics.ins-det)single electron3. Good health[SDU.ASTR.IM]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]xenonchemistryWeakly interacting massive particlesAtomic physicsAstrophysics - Instrumentation and Methods for AstrophysicsJ. Phys.
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High-gradient testing of an $S$-band, normal-conducting low phase velocity accelerating structure

2020

A novel high-gradient accelerating structure with low phase velocity, $v/c=0.38$, has been designed, manufactured and high-power tested. The structure was designed and built using the methodology and technology developed for CLIC $100\text{ }\text{ }\mathrm{MV}/\mathrm{m}$ high-gradient accelerating structures, which have speed of light phase velocity, but adapts them to a structure for nonrelativistic particles. The parameters of the structure were optimized for the compact proton therapy linac project, and specifically to 76 MeV energy protons, but the type of structure opens more generally the possibility of compact low phase velocity linacs. The structure operates in S-band, is backward…

Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Field (physics)[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]cavityType (model theory)01 natural sciencesp: accelerationLinear particle accelerator0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsReview ArticlesPhysics010308 nuclear & particles physicsvelocity: lowPulse durationSurfaces and Interfaceslinear acceleratorgradient: highAccelerators and Storage Ringsvelocity: phasePulse (physics)particle: nonrelativisticDistribution (mathematics)lcsh:QC770-798Atomic physicsPhase velocityEnergy (signal processing)performance
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First application of the Laser Ion Source and Trap (LIST) for on-line experiments at ISOLDE

2012

The Laser Ion Source and Trap (LIST) provides a new mode of operation for the resonance ionization laser ion source (RILIS) at ISOLDE/CERN, reducing the amount of surface-ionized isobaric contaminants by up to four orders of magnitude. After the first successful on-line test at ISOLDE in 2011 the LIST was further improved in terms of efficiency, selectivity, and reliability through several off-line tests at Mainz University and at ISOLDE. In September 2012, the first on-line physics experiments to use the LIST took place at ISOLDE. The measurements of the improved LIST indicate more than a twofold increase in efficiency compared to the LIST of the 2011 run. The suppression of surface-ionize…

Nuclear and High Energy Physics[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Ion trapchemistry.chemical_element01 natural sciencesIn-source laser spectroscopylaw.inventionFranciumTrap (computing)LISTlawIonization0103 physical sciences010306 general physicsInstrumentationLaser ion sourceLarge Hadron Collider[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]010308 nuclear & particles physicsChemistryOn-line mass separatorOrders of magnitude (angular velocity)LaserIon sourceIon trapAtomic physics
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