Search results for "nuclear physics"

showing 10 items of 5307 documents

Spectroscopy of Low-lying States in $^{140}$Sm

2014

International audience; Electromagnetic transition strengths and spectroscopic quadrupole moments for Sm-140 were measured by means of multi-step Coulomb excitation with radioactive beam at the ISOLDE facility at CERN. A complementary experiment was performed at the Heavy Ion Laboratory in Warsaw to assign spins for non-yrast states using the angular correlation technique. Based on the new experimental data previous spin assignments need to be revised.

Physicsta114General Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ddc:nuclear spectrumNuclear physicsPhysics::Accelerator PhysicsAtomic physicsSpectrum analysissamariumSpectroscopyNuclear ExperimentLying
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Charged-current neutrino-nucleus scattering off Xe isotopes

2019

Xenon detectors are used in the search for dark matter and neutrinoless double-beta decay ($0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta})$. As the next-generation detectors reach masses in the ton scale, neutrinos from astrophysical sources are soon predicted to become background in such detectors. Theoretical predictions of neutrino scattering cross sections and information of nuclear structure effects therein are crucial in accounting for the background. We perform calculations for differential and total cross sections of charged-current neutrino scattering off the most abundant xenon isotopes. The nuclear-structure calculations are made in the proton-neutron quasiparticle random…

Physicsta114Physics::Instrumentation and DetectorsScatteringSolar neutrinoDark matterneutriinotNuclear structurechemistry.chemical_elementnucleus-neutrino interactionsNuclear physicsSupernovaXenonchemistrysolar neutrinosIsotopes of xenonHigh Energy Physics::ExperimentNeutrinoPhysical Review C
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Occupation probabilities of single particle levels using the microscopic interacting boson model: Application to some nuclei of interest in neutrinol…

2016

We have developed a new method to calculate the occupancies of single particle levels in atomic nuclei. This method has been developed in the context of the microscopic interacting boson model, in which neutron and proton degrees of freedom are treated explicitly. The energies of the single particle levels constitute a very important input for the calculation of the occupancies in this method. In principle these energies can be considered as input parameters that can be fitted to reproduce the experimental occupancies. Instead of fitting, in this study we have extracted the single particle energies from experimental data on nuclei with a particle more or one particle less than a shell closu…

Physicsta114Proton010308 nuclear & particles physicsNuclear TheoryDegrees of freedom (physics and chemistry)double beta decayContext (language use)01 natural sciences7. Clean energyNuclear physicssingle particle levelsParticle decayatomic nucleimicroscopic interacting boson model0103 physical sciencesAtomic nucleusParticleNeutronInteracting boson modelAtomic physics010303 astronomy & astrophysicsPhysical Review C
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Mean-Field Calculation Based on Proton-Neutron Mixed Energy Density Functionals

2015

We have performed calculations based on the Skyrme energy density functional (EDF) that includes arbitrary mixing between protons and neutrons. In this framework, single-particle states are generalized as mixtures of proton and neutron components. The model assumes that the Skyrme EDF is invariant under the rotation in isospin space and the Coulomb force is the only source of the isospin symmetry breaking. To control the isospin of the system, we employ the isocranking method, which is analogous to the standard cranking approach used for describing high-spin states. Here, we present results of the isocranking calculations performed for the isobaric analog states in A = 40 and A = 54 nuclei.

Physicsta114Proton010308 nuclear & particles physicsNuclear TheoryInvariant (physics)01 natural sciencesenergy density functionalsCoulomb's lawNuclear physicssymbols.namesakeMean field theoryproton-neutron mixingisobaric analog statesQuantum electrodynamicsIsospin0103 physical sciencessymbolsIsobaric processNeutronSymmetry breakingNuclear Experiment010306 general physicsProceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)
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Reduced transition probabilities along the yrast line in W-166

2017

WOS: 000406755100001

Physicsta114Spectrometer010308 nuclear & particles physicsYrast01 natural sciences7. Clean energynuclear physicsExcited state0103 physical sciencesNuclideAtomic physics010306 general physicsAxial symmetry
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Prompt gamma ray-spectroscopy of N = 50 fission fragments

2013

Excited states in the nuclei 83 As and 84,86 Se have been studied via prompt -ray spectroscopy. The nuclei were produced by the proton-induced fission of a 238 U target, at the accelerator of the University of Jyvaskyla. The JUROGAM-II array was used to detect prompt -rays and a triple- coincidence analysis performed. A comparison of the N = 50 nuclei with shell-model calculations reproduces the low-lying states in 83 As and 84 Se well. The inclusion of particle-hole excitations is necessary to correctly describe the states above ∼ 3.5 MeV.

Physicsta114[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsFissionAstrophysics::High Energy Astrophysical PhenomenaPhysicsQC1-999Nuclear Theory01 natural sciences7. Clean energyCoincidenceNuclear physicsExcited state0103 physical sciencesGamma spectroscopyAtomic physics010306 general physicsSpectroscopyNuclear ExperimentComputingMilieux_MISCELLANEOUSEPJ Web of Conferences
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Thermalization in the initial stage of heavy ion collisions

2017

The high density non-abelian matter produced in heavy ion collisions is extremely anisotropic. Prethermal dynamics for the anisotropic and weakly coupled matter is discussed. Thermalization is realized with the effective kinetic theory in the leading order accuracy of the weakly coupled expansion. With the initial condition from color glass condensate, hydrodynamization time for the LHC energies is realized to be about 1 fm/c, while the thermalization happens much later than the hydrodynamization. peerReviewed

PhysicsthermalizationLarge Hadron Colliderta114010308 nuclear & particles physicsPhysicsQC1-999heavy ion collisionsHigh density01 natural sciences7. Clean energyColor-glass condensateNuclear physicsThermalisationChemical physics0103 physical sciencesKinetic theory of gasescolor glass condensatehydrodynamizationInitial value problemHeavy ion010306 general physicsAnisotropyQuark Confinement and the Hadron Spectrum
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Beam Energy Scan of Specific Heat Through Temperature Fluctuations in Heavy Ion Collisions

2016

Temperature fluctuations may have two distinct origins, first, quantum fluctuations that are initial state fluctuations, and second, thermodynamical fluctuations. We discuss a method of extracting the thermodynamic temperature from the mean transverse momentum of pions, by using controllable parameters such as centrality of the system, and range of the transverse momenta. Event-by-event fluctuations in global temperature over a large phase space provide the specific heat of the system. We present Beam Energy Scan of specific heat from data, AMPT and HRG model prediction. Experimental results from NA49, STAR, PHENIX, PHOBOS and ALICE are combined to obtain the specific heat as a function of …

Physicsthermodynamical fluctuationHistory010308 nuclear & particles physicsbeam energy scanheavy ion collisionsThermal fluctuationsThermodynamic temperature01 natural sciencesComputer Science ApplicationsEducationNuclear physicsTransverse planePionLattice (order)Phase space0103 physical sciences010306 general physicsNuclear ExperimentQuantum fluctuationEvent generator
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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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High-spin states in the neutron-rich A∼100 region

2009

Two experimental setups have been used to study excited states of neutron‐rich nuclei in the A∼100 region. Extended level schemes and lifetime measurements were obtained using deep‐inelastic and fusion‐fission reactions with the CLARA‐PRISMA spectrometer and the Ge‐array GASP respectively. Experimental information from GASP has been used to complement the CLARA‐PRISMA experiment. Time spectra have been used to measure the lifetimes of isomeric states. Preliminary results are presented for 89Rb.

Physicsγ-ray transitionsSpin statesSpectrometerAstrophysics::High Energy Astrophysical PhenomenaLifetimesPRISMA-CLARA spectrometerGASP arrayDeep inelastic scatteringSpectral lineNuclear physicsPhysics and Astronomy (all)Excited stateNuclear fusionNeutronGamma spectroscopyAtomic physicsγ-ray transitions; GASP array; Lifetimes; PRISMA-CLARA spectrometer; Physics and Astronomy (all)Nuclear ExperimentAIP Conference Proceedings
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