Search results for "yield"

showing 10 items of 1338 documents

Separation of fission products by the ion guide fed isotope separator, IGISOL

1987

Abstract The performance of the ion guide method in the on-line mass separation of fission products has been investigated. Activity was produced by bombarding nat. U targets with a beam of 20 MeV protons. All the mass chains from A = 95 through A = 120 have been scanned using conventional methods of nuclear spectroscopy. No chemical selectivity in the separation was observed; isotopes of highly nonvolatile elements from yttrium to palladium were produced with efficiencies equal to those for the more volatile ones. The boundary of known neutron-rich nuclides was reached throughout the mass region from A = 106 to A = 118. During the course of this preliminary study the new isotope 116 Rh was …

Nuclear and High Energy PhysicsFission productsIsotopeRadiochemistryOxideAnalytical chemistrychemistry.chemical_elementFission product yieldYttriumIonchemistry.chemical_compoundchemistryNuclideInstrumentationPalladiumNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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On-line yields obtained with the ISOLDE RILIS

2003

The ISOLDE resonance ionization laser ion source (RILIS) allows to ionize efficiently and selectively many metallic elements. In recent yield surveys and on-line experiments with the ISOLDE RILIS we observed 23–34 Mg, 26–34 Al, 98–132 Cd, 149 Tb, 155–177 Yb, 179–200 Tl, 183–215 Pb and 188–218 Bi. The obtained yields are presented together with measured release parameters which allow to extrapolate the release efficiency towards more exotic (short-lived) nuclides of the same elements. 2002 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsIsotopeChemistryRadiochemistryLaserAccelerators and Storage RingsIon sourcelaw.inventionNuclear physicslawIonizationIsotopes of cadmiumYield (chemistry)NuclideInstrumentationIsotopes of magnesiumParticle Physics - Experiment
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Investigation of precipitate in an austenitic ODS steel containing a carbon-rich process control agent

2018

This work has been carried out within the framework of the German Helmholtz Association and has received funding from the topic “Materials Research for the Future Energy Supply”. The work of M. Parish and Rainer Ziegler is gratefully acknowledged. Thanks are also due to the team of the chemical laboratory at the KIT for performing the chemical analysis. The help of the beamline staff at ELETTRA (project 20140052 ) synchrotron radiation facility is acknowledged. We acknowledge support by Deutsche Forschungsgemeinschaft and Open Access Publishing Fund of Karlsruhe Institute of Technology.

Nuclear and High Energy PhysicsMaterials scienceYield (engineering)Materials Science (miscellaneous)Oxidechemistry.chemical_elementProcess control agent02 engineering and technology01 natural sciences010305 fluids & plasmasCarbidechemistry.chemical_compound0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Process controlAusteniteMetallurgytechnology industry and agricultureX-ray absorption spectroscopy021001 nanoscience & nanotechnologylcsh:TK9001-9401Oxide dispersion strengthened steelNuclear Energy and Engineeringchemistry8. Economic growthlcsh:Nuclear engineering. Atomic powerAustenitic steelMechanical alloying0210 nano-technologyDispersion (chemistry)CarbonTransmission electron microscopyTitaniumNuclear Materials and Energy
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Neutron yield from carbon, light- and heavy-water thick targets irradiated by 40MeV deuterons

2009

Abstract Angular and energy distributions of neutrons produced by the interaction of deuterons of 40 MeV in carbon, light- and heavy-water targets, in which they are stopped, have been measured by the activation method. A discrepancy with a time-of-flight measurement for d + C has been found. The results are compared with a Monte-Carlo calculation and are discussed in the frame of building a deuteron-to-neutron converter for the SPIRAL2 radioactive ion-beam facility.

Nuclear and High Energy PhysicsNuclear TheoryActivationchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicschemistry.chemical_compoundNeutron yield0103 physical sciencesThick target neutronyieldMonte-Carlo codeNeutronIrradiationNuclear Experiment010306 general physicsInstrumentationHeavy waterPhysics010308 nuclear & particles physicschemistryDeuteriumMonte carlo codePhysics::Accelerator PhysicsActivation methodCarbonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Design of large scale sensors in 180 nm CMOS process modified for radiation tolerance

2019

International audience; The last couple of years have seen the development of Depleted Monolithic Active Pixel Sensors (DMAPS) fabricated with a process modification to increase the radiation tolerance. Two large scale prototypes, Monopix with a column drain synchronous readout, and MALTA with a novel asynchronous architecture, have been fully tested and characterized both in the laboratory and in test beams. This showed that certain aspects have to be improved such as charge collection after irradiation and the output data rate. Some improvements resulting from extensive TCAD simulations were verified on a small test chip, Mini-MALTA. A detailed cluster analysis, using data from laboratory…

Nuclear and High Energy PhysicsOn-chip clusteringPhysics::Instrumentation and Detectors01 natural sciencesCMOS sensors ; Tracking detectors ; Monolithic sensors ; MAPS ; On-chip clustering030218 nuclear medicine & medical imaging03 medical and health sciencesTracking detectors0302 clinical medicinesemiconductor detector: pixelRadiation toleranceCMOS sensors0103 physical sciencesMAPSElectronic engineeringIrradiation[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]numerical calculationsInstrumentationradiation: damagePhysicsPixelirradiation010308 nuclear & particles physicstracking detector: upgradecharge: yieldBandwidth (signal processing)ATLASDigital architectureChipUpgradeAsynchronous communicationMonolithic sensors
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A Precise Measurement of the Tau Lepton Lifetime

1996

The tau lepton lifetime has been measured using three different methods with the DELPHI detector. Two measurements of one-prong decays are combined, accounting for correlations, giving a result of \tau_\tau = 291.8 \pm 3.3 \mbox{ (stat.)} \pm 2.0 \mbox{(sys.) fs} while the decay length distribution of three-prong decays gives the result \tau_{\tau} = 286.7 \pm 4.9 \mbox{ (stat.)} \pm 3.3 \mbox{ (sys.) fs}. Combining the results presented here with previous DELPHI measurements, we get \tau_{\tau} = 291.4 \pm 3.0 fs and find that the ratio of the coupling constant for tau decay relative to that for muon decay is 0.990 \pm 0.009, compatible with lepton universality.

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilation01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)tau lepton lifetimeNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsZ-DECAYSDELPHICoupling constantPhysicsMuon010308 nuclear & particles physicsDELPHI; tau lepton lifetime; one-prong; three-prongLARGE ELECTRON POSITRON COLLIDERthree-prongYield (chemistry)PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIone-prongDecay lengthPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearVertex detectorParticle Physics - ExperimentLepton
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Exact relativistic beta decay endpoint spectrum

2007

5 pages, 3 figures.-- PACS nrs.: 14.60.Pq; 13.30.-a; 23.40.-s; 23.40.Bw.-- ISI Article Identifier: 000250620900070.-- ArXiv pre-print available at: http://arxiv.org/abs/0706.0897

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsFOS: Physical sciences[PACS] Neutrino mass and mixingelectron and muon captureHigh Energy Physics - Phenomenology (hep-ph)FactorizationDouble beta decayNuclear Experiment (nucl-ex)Neutrino oscillationNuclear ExperimentPhysics[PACS] β decay[PACS] Decays of baryonsSpectrum (functional analysis)[PACS] β decay; double β decay; electron and muon captureFísicaBeta decay[PACS] Weak-interaction and lepton (including neutrino) aspects of β decayHigh Energy Physics - Phenomenologydouble β decayYield (chemistry)High Energy Physics::ExperimentNeutrinoKATRIN
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Measurement of the semileptonic branching fraction of the B_{s} meson

2012

We report a measurement of the inclusive semileptonic branching fraction of the B_s meson using data collected with the BaBar detector in the center-of-mass (CM) energy region above the Upsilon(4S) resonance. We use the inclusive yield of phi mesons and the phi yield in association with a high-momentum lepton to perform a simultaneous measurement of the semileptonic branching fraction and the production rate of B_s mesons relative to all B mesons as a function of CM energy. The inclusive semileptonic branching fraction of the B_s meson is determined to be B(B_s to l nu X)=9.5 (+2.5/-2.0)(stat)(+1.1/-1.9)(syst)%, where l indicates the average of e and mu.

Nuclear and High Energy PhysicsParticle physicssemileptonic branching fractionMesonHigh Energy Physics::Latticesemileptonic branching fraction B_s mesonFOS: Physical sciences01 natural sciencesResonance (particle physics)semileptonic Bs-meson decaysHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Mesons (Nuclear physics)B mesonSDG 7 - Affordable and Clean EnergyMesons (Física nuclear)010306 general physicsNuclear Experiment14.40.Nd 13.20.HePhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy010308 nuclear & particles physicsBranching fractionLeptons (Física nuclear)High Energy Physics::PhenomenologyBABAR detectorbranching fraction measurementHEPPACS: 14.40.Nd 13.20.HeBaBar detector at SLAC; semileptonic Bs-meson decays; branching fraction measurementLeptons (Nuclear physics)Yield (chemistry)BaBarB_s mesonHigh Energy Physics::ExperimentBaBar detector at SLACsemileptonic Bs-meson decayLeptonProduction rate
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Characterization and performance of the DTAS detector

2018

11 pags., 16 figs., 3 tabs.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaMonte Carlo methodspektrometritβ decayFOS: Physical sciencesNon-proportional scintillation light yield: Monte Carlo simulationsMonte Carlo simulations [Non-proportional scintillation light yield]y-ray spectrometerB decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMonte Carlo simulationsOpticsDistortion0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsAbsorption (electromagnetic radiation)Nuclear ExperimentInstrumentation[formula omitted] decayNuclear ExperimentPhysicsta114Spectrometer010308 nuclear & particles physicsbusiness.industryNaI(Tl) detectorPulse generatorTotal absorption [formula omitted]-ray spectrometerDetectornon-proportional scintillation light yieldInstrumentation and Detectors (physics.ins-det)Total absorption γ -ray spectrometerNon-proportional scintillation light yieldFísica nuclearTotal absorptionydinfysiikkabusinessDelayed neutronExotic nucleiNuclear instruments & methods inphysics research section A: Accelerators spectrometers detectors and associated equipment 910: 79-89 (2018)
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Status report of the SARA IGISOL used in the study of the 238U(α 40 MeV, ƒ) reaction

1992

Abstract A new ion guide isotope separator on-line (IGISOL), operating with the SARA facility, has been constructed. Using the 238U(α 40 MeV, ƒ) reaction to produce very neutron-rich radioisotopes, all mass chains from A = 96 to 122 have been scanned by conventional methods of nuclear spectroscopy. Provided the stopping volume is separated from the primary beam, it has been proved that the yield is nearly proportional to the He pressure. In addition to the usual advantages (quasi-independence from physical and chemical properties of elements), this makes IGISOL a powerful technique for high energy recoil products. During the experiments the boundary of known neutron-rich nuclei was reached …

Nuclear and High Energy PhysicsRange (particle radiation)Isotope010308 nuclear & particles physicsChemistryAnalytical chemistrySeparator (oil production)7. Clean energy01 natural sciencesIonNuclear physicsRecoilVolume (thermodynamics)Yield (chemistry)0103 physical sciencesNuclear Experiment010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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