Search results for "yield"

showing 10 items of 1338 documents

Development of a PbWO 4 detector for single-shot positron annihilation lifetime spectroscopy at the GBAR experiment

2020

International audience; We have developed a PbWO 4 (PWO) detector with a large dynamic range to measure the intensity of a positron beam and the absolute density of the ortho-positronium (o-Ps) cloud it creates. A simulation study shows that a setup based on such detectors may be used to determine the angular distribution of the emission and reflection of o-Ps to reduce part of the uncertainties of the measurement. These will allow to improve the precision in the measurement of the cross section for the (anti) hydrogen formation by (anti) proton-positronium charge exchange and to optimize the yield of antihydrogen ion which is an essential parameter in the GBAR experiment.

PhysicsPhysics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]DetectorMeasure (physics)General Physics and Astronomy7. Clean energyIonNuclear physicsCross section (physics)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]PACS: 78.70.Bj 41.75.Fr 36.10.DrYield (chemistry)Reflection (physics)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]AntihydrogenSpectroscopyComputingMilieux_MISCELLANEOUS
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Spectroscopy of Cd98 by two-nucleon removal from In100

2021

Low-lying states of Cd-98 have been populated by the two-nucleon removal reaction (In-100, Cd-98+gamma) and studied using in-beam gamma-ray spectroscopy at the Radioactive Isotope Beam Factory at RIKEN. Two new gamma transitions were identified and assigned as decays from a previously unknown state. This state is suggested to be based on a pi 1g(/9/2)(-1)2p(1/2)(-2) configuration with J(pi) = 5(-). The present observation extends the systematics of the excitation energies of the first 5(-) state in N = 50 isotones toward Sn-100. The determined energy of the 5(- )state in Cd-98 continues a smooth trend along the N = 50 isotones. The systematics are compared with shell-model calculations in d…

PhysicsProton010308 nuclear & particles physicsSpace (mathematics)01 natural sciences7. Clean energyAtomic orbitalYield (chemistry)0103 physical sciencesLevel structureAtomic physics010306 general physicsSpectroscopyNucleonExcitationPhysical Review C
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Distillation of entanglement between distant systems by repeated measurements on an entanglement mediator

2004

A recently proposed purification method, in which the Zeno-like measurements of a subsystem can bring about a distillation of another subsystem in interaction with the former, is utilized to yield entangled states between distant systems. It is shown that the measurements of a two-level system locally interacting with other two spatially separated not coupled subsystems, can distill entangled states from the latter irrespectively of the initial states of the two subsystems.

PhysicsQuantum PhysicsFOS: Physical sciencesQuantum entanglementInformation theoryMultipartite entanglementAtomic and Molecular Physics and Opticslaw.inventionlawYield (chemistry)Quantum mechanicsStatistical physicsPurification methodsQuantum Physics (quant-ph)Distillationeffects decay survival probabilityPhysical Review A
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Multiplicity dependence of inclusive J/ψ production at midrapidity in pp collisions at s=13 TeV

2020

Measurements of the inclusive J/ψ yield as a function of charged-particle pseudorapidity density dNch/dη in pp collisions at √s = 13 TeV with ALICE at the LHC are reported. The J/ψ meson yield is measured at midrapidity (|y| < 0.9) in the dielectron channel, for events selected based on the charged-particle multiplicity at midrapidity (|η| < 1) and at forward rapidity (−3.7 < η < −1.7 and 2.8 < η < 5.1); both observables are normalized to their corresponding averages in minimum bias events. The increase of the normalized J/ψ yield with normalized dNch/dη is significantly stronger than linear and dependent on the transverse momentum. The data are compared to theoretical predictions, which de…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsLarge Hadron ColliderMeson010308 nuclear & particles physicsMultiplicity (mathematics)Quarkonium01 natural sciencesNuclear physicsPseudorapidityYield (chemistry)0103 physical sciencesRapidity010306 general physicsPhysics Letters B
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Isotopic Differences in the Charge Distribution of Even Molybdenum Isotopes from Elastic Electron Scattering

1975

Elastic-electron-scattering cross sections for $^{92,94,96,98,100}\mathrm{Mo}$ in an effective momentum transfer range of 0.6-2.1 ${\mathrm{fm}}^{\ensuremath{-}1}$ are analyzed in a practically model-independent way, using a Fourier-Bessel expansion for the charge distribution. The ratios of cross sections of neighboring isotopes yield differences of charge distributions, which exhibit pronounced shell effects.

PhysicsRange (particle radiation)IsotopechemistryMolybdenumScatteringYield (chemistry)Momentum transferGeneral Physics and Astronomychemistry.chemical_elementCharge densityCharge (physics)Atomic physicsPhysical Review Letters
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Modelling of Boltzmann transport equation for freeze-out

2005

The freeze-out (FO) in high-energy heavy-ion collisions is assumed to be continuous across finite layer in space–time. Particles leaving local thermal equilibrium start to freeze out gradually till they leave the layer, where all the particles are frozen out. To describe such a kinetic process we start from Boltzmann transport equation (BTE). However, we will show that the basic assumptions of BTE, such as molecular chaos or spatial homogeneity do not hold for the above-mentioned FO process. The aim of the presented work is to analyse the situation, discuss the modification of BTE and point out the physical causes, which yield to these modifications of BTE for describing FO.

PhysicsThermal equilibriumNuclear and High Energy PhysicsWork (thermodynamics)Yield (engineering)Molecular chaosStatistical physicsSpatial homogeneityPhysics::Classical PhysicsKinetic energyBoltzmann equationJournal of Physics G: Nuclear and Particle Physics
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The use of the integral-bias summing coincidence spectrometer in directional correlation measurements

1968

Abstract The performance of the integral-bias summing coincidence spectrometer (the sum-peak spetrometer) in measurements of directional correlations of gamma rays has been tested. As compared with the conventional method, the sum-peak spectrometer is easier to use and seems to yield results which agree with those obtained with the ordinary method. Because of the complex shapes of response functions of gamma rays above about 3 MeV, the new method is best suited to the study of cascading transitions below this energy, where the two methods appear to complement each other. The analysis of the sum-peak spectra in the present work is based on a simple graphical method which seems to yield satis…

PhysicsWork (thermodynamics)Spectrometer010308 nuclear & particles physicsGamma rayGeneral Medicine01 natural sciencesCoincidenceSpectral lineNuclear physicsYield (chemistry)0103 physical sciences010306 general physicsEnergy (signal processing)Complement (set theory)Nuclear Instruments and Methods
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Calculation of the wetting parameter from a cluster model in the framework of nanothermodynamics

2003

The critical wetting parameter ${\ensuremath{\omega}}_{c}$ determines the strength of interfacial fluctuations in critical wetting transitions. In this Brief Report, we calculate ${\ensuremath{\omega}}_{c}$ from considerations on critical liquid clusters inside a vapor phase. The starting point is a cluster model developed by Hill and Chamberlin in the framework of nanothermodynamics [Proc. Natl. Acad. Sci. USA 95, 12779 (1998)]. Our calculations yield results for ${\ensuremath{\omega}}_{c}$ between 0.52 and 1.00, depending on the degrees of freedom considered. The findings are in agreement with previous experimental results and give an idea of the universal dynamical behavior of the cluste…

PhysicsYield (engineering)Condensed matter physicsVapor phaseDegrees of freedom (physics and chemistry)Cluster (physics)WettingOmegaVortexMathematical physics
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Development of High Resolution Resonance Ionization Mass Spectrometry for Neutron Dosimetry Technique with93Nb(n,n')93mNb Reaction

2016

We have proposed an advanced technique to measure the 93mNb yield precisely by Resonance Ionization Mass Spectrometry, instead of conventional characteristic X-ray spectroscopy. 93mNb-selective resonance ionization is achievable by distinguishing the hyperfine splitting of the atomic energy levels between 93Nb and 93mNb at high resolution. In advance of 93mNb detection, we could successfully demonstrate high resolution resonant ionization spectroscopy of stable 93Nb using an all solid-state, narrowband and tunable Ti:Sapphire laser system operated at 1 kHz repetition rate. peerReviewed

Physicsmassaspektrometriata114resonance Ionization010308 nuclear & particles physicsPhysicsQC1-999Analytical chemistryMass spectrometryLaser01 natural scienceslaw.inventionNuclear physicslawIonizationYield (chemistry)0103 physical sciencesResonance ionizationPhysics::Atomic and Molecular ClustersSapphirePhysics::Atomic Physics010306 general physicsSpectroscopyHyperfine structuremass spectrometryEPJ Web of Conferences
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A facility for fast-neutron irradiations at Jyväskylä and its use for nuclide cross-section measurements in fission

2013

Abstract An efficient and reliable transport system for fast-neutron irradiations has been built at the Physics Department, Jyvaskyla, Finland. It is constructed from commercial bicycle components and is driven by a computer-controlled stepping motor. It can be operated in single or cyclic mode. The neutron irradiated targets are moved within 1.2 s (full stop to full stop) to a well-shielded position 3 m away where they can be removed or directly investigated by γ spectroscopy. The system has been built with the aim to experimentally verify the calculated production rates of neutron-rich nuclei in the SPIRAL2 uranium target. However, the facility can be used for various kinds of fast-neutro…

Physicsthick target neutron yieldNuclear and High Energy Physicsta114010308 nuclear & particles physicsNeutron emissionXenon-135Fission product yield[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyFast fissionNeutron temperature29.25.Dz 29.30.Hs 25.85.Ec.Nuclear physicsPrompt neutron0103 physical sciencesNeutron cross sectionfissionNeutronactivationneutron-induced 13 fission010306 general physicsInstrumentation
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