Search results for "nuclear-structure"

showing 7 items of 7 documents

Gamow-Teller response in the configuration space of a density-functional-theory–rooted no-core configuration-interaction model

2018

Background: The atomic nucleus is a unique laboratory in which to study fundamental aspects of the electroweak interaction. This includes a question concerning in medium renormalization of the axial-vector current, which still lacks satisfactory explanation. Study of spin-isospin or Gamow-Teller (GT) response may provide valuable information on both the quenching of the axial-vector coupling constant as well as on nuclear structure and nuclear astrophysics.Purpose: We have performed a seminal calculation of the GT response by using the no-core configuration-interaction approach rooted in multireference density functional theory (DFT-NCCI). The model treats properly isospin and rotational sy…

HE-8Nuclear TheoryNUCLEAR-STRUCTURE114 Physical sciences01 natural sciencesENERGY-LEVELSQuantum mechanics0103 physical sciencesBETA-DECAY010306 general physicsPhysicsta114nuclear density functional theory010308 nuclear & particles physicsGROUND-STATE PROPERTIESNuclear structureNuclear shell modelConfiguration interactionelectroweak interactions in nuclear physicsIsospinAtomic nucleusSHELL-MODELSlater determinantSum rule in quantum mechanicsConfiguration spacebeta decayPhysical Review C
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The electronion scattering experiment ELISe at the International Facility for Antiproton and Ion Research (FAIR) - A conceptual design study

2011

The electronion scattering experiment ELISe is part of the installations envisaged at the new experimental storage ring at the International Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany. It offers an unique opportunity to use electrons as probe in investigations of the structure of exotic nuclei. The conceptual design and the scientific challenges of ELISe are presented. © 2011 Elsevier B.V. All rights reserved.

Nuclear and High Energy PhysicselectronscatteringFORM-FACTORS[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Electron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]DATA-ACQUISITION SYSTEMNUCLEAR-STRUCTURE01 natural sciencesBINDING-ENERGIESCHARGE-DENSITY DISTRIBUTIONSIonCROSS-SECTIONSNuclear physicsNuclei far off stabilityConceptual designeA collider0103 physical sciencesCENTRAL DEPRESSIONElectron scattering010306 general physicsInstrumentationPhysics010308 nuclear & particles physicsScattering29.27.-a 25.30.Bf25.30.Dh21.10.Ft29.20.Dh29.30.-hRELATIVISTIC HEAVY-IONSEXOTIC NUCLEIFacility for Antiproton and Ion ResearchGIANT-RESONANCESStorage ring
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Mass measurements on stable nuclides in the rare-earth region with the Penning-trap mass spectrometer RIGA-TRAP

2011

The masses of 15 stable nuclides in the rare-earth region have been measured with the Penning-trap mass spectrometer TRIGA-TRAP. This is the first series of absolute mass measurements linking these nuclides to the atomic-mass standard $^{12}\mathrm{C}$. Previously, nuclear reaction studies almost exclusively determined the literature values of these masses in the Atomic-Mass Evaluation. The TRIGA-TRAP results show deviations on the order of 3--4 standard deviations from the latest published values of the Atomic-Mass Evaluation 2003 for some cases. However, the binding-energy differences that are important for nuclear structure studies have been confirmed and improved. The new masses are dis…

Nuclear reactionNuclear and High Energy PhysicsBinding energyRESONANCE NEUTRON-CAPTURE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryNUCLEAR-STRUCTURE01 natural sciencesBeta-decay stable isobarsNuclear physics0103 physical sciencesNuclidePhysics::Atomic PhysicsSU(4) SYMMETRY010306 general physicsNuclear ExperimentSEPARATION ENERGIESPhysicsIsotopeCARBON CLUSTERS010308 nuclear & particles physicsCarbon-12ISOSPIN SYMMETRYRAMSEY METHODGAMMAPenning trapISOTOPESATOMIC MASS
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Magnetic and quadrupole moments of neutron deficient 58-62Cu isotopes

2011

Abstract This paper reports on the ground state nuclear moments measured in 58–62Cu using collinear laser spectroscopy at the ISOLDE facility. The quadrupole moments for 58–60Cu have been measured for the first time as Q ( Cu 58 ) = − 15 ( 3 ) efm 2 , Q ( Cu 59 ) = − 19.3 ( 19 ) efm 2 , Q ( Cu 60 ) = + 11.6 ( 12 ) efm 2 and with higher precision for 61,62Cu as Q ( Cu 61 ) = − 21.1 ( 10 ) efm 2 , Q ( Cu 62 ) = − 2.2 ( 4 ) efm 2 . The magnetic moments of 58,59Cu are measured with a higher precision as μ ( Cu 58 ) = + 0.570 ( 2 ) μ N and μ ( Cu 59 ) = + 1.8910 ( 9 ) μ N . The experimental nuclear moments are compared to large-scale shell-model calculations with the GXPF1 and GXPF1A effective i…

PhysicsNuclear and High Energy Physicsnuclear-structureIsotopeMagnetic momentNuclear moments010308 nuclear & particles physicsshell-modelNuclear structureN=287. Clean energy01 natural sciencesShell modelCu58Cu59Cu60Cu61Cu620103 physical sciencesQuadrupoleNuclear spinNeutronHyperfine structureAtomic physicsLaser spectroscopy010306 general physicsGround stateSpectroscopyHyperfine structure
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Isotope Shifts of Radium Monofluoride Molecules

2021

Isotope shifts of $^{223-226,228}$Ra$^{19}$F were measured for different vibrational levels in the electronic transition $A^{2}{}{\Pi}_{1/2}\leftarrow X^{2}{}{\Sigma}^{+}$. The observed isotope shifts demonstrate the particularly high sensitivity of radium monofluoride to nuclear size effects, offering a stringent test of models describing the electronic density within the radium nucleus. Ab initio quantum chemical calculations are in excellent agreement with experimental observations. These results highlight some of the unique opportunities that short-lived molecules could offer in nuclear structure and in fundamental symmetry studies.

[PHYS.NUCL] Physics [physics]/Nuclear Theory [nucl-th]FIELD SHIFTNuclear TheoryAtomic Physics (physics.atom-ph)Ab initioGeneral Physics and AstronomyNUCLEAR-STRUCTUREnucl-ex01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmasENERGYchemistry.chemical_compoundatomifysiikkaMOMENTSPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentPhysicsIsotopePhysicsNuclear structureradiumNuclear Physics - TheoryPhysical SciencesAtomic physicsydinfysiikkanucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Monofluoride[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.PHYS.PHYS-GEN-PH] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Physics MultidisciplinaryOther Fields of PhysicsFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]physics.atom-phMolecular electronic transitionELECTRONIC-STRUCTURE CALCULATIONSNuclear Theory (nucl-th)ATOMS0103 physical sciencesMoleculeSPECTRANuclear Physics - ExperimentSensitivity (control systems)010306 general physicsisotoopitScience & Technology[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]chemistryMECHANICSMASS DEPENDENCELASERElectronic density
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α decay of the πh11/2 isomer in Ir164

2014

The α -decay branch of the πh 11 / 2 isomer in 164 Ir has been identified using the GREAT spectrometer. The 164 Ir nuclei were produced using the 92 Mo( 78 Kr ,p 5 n ) 164 Ir reaction and separated in flight using the recoil ion transport unit (RITU) gas-filled separator. The measured α -decay energy of 6880 ± 10 keV allowed the excitation of the πh 11 / 2 state in 160 Re to be deduced as 166 ± 14 keV. The half-life of 164 Ir was measured with improved precision to be 70 ± 10 μ sandan α -decay branching ratio of 4 ± 2% was determined. Improved half-life and branching ratio measurements were also obtained for 165 Ir, but no evidence was found for the ground-state decays of either 164 Ir or 1…

neutron-deficent isotopesenergianuclear-structuremodeltotal data readout. proton drip-lineemissionrituosmiumvolframi
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Charged-current neutrino and antineutrino scattering off 116Cd described by Skyrme forces

2014

We perform calculations of the cross sections for charged-current neutrino and antineutrino scattering off 116Cd using ten different Skyrme interactions, at energies typical of supernova neutrinos. We use the quasiparticle random-phase approximation in its charged-changing mode (pnQRPA) to construct the required nuclear wave functions for the participant initial and final states. We compare the results of these calculations with the results of calculations based on the Bonn one-boson-exchange potential. The response of 116Cd to supernova neutrinos is calculated by folding the obtained cross sections with suitably parametrized Fermi-Dirac distributions of the electron-neutrino and electron-a…

nuclear-structureAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimentdoble-beta decay
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