Search results for "Ground state"

showing 10 items of 928 documents

First observation of excited states inHg17595

2009

Excited states of the neutron-deficient nucleus Hg-175, populated using fusion-evaporation reactions, are reported for the first time. The spin and parity of the ground state has been determined to ...

PhysicsNuclear and High Energy Physicsmedicine.anatomical_structureExcited stateNuclear TheorymedicineParity (physics)Alpha decayAtomic physicsNuclear ExperimentGround stateNucleusPhysical Review C
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Systematic study of the single-state dominance in 2νββ decay transitions

1999

Abstract The single-state-dominance hypothesis (SSDH) states that the decay rates of the two-neutrino double-beta decay are governed by a virtual two-step transition connecting the initial and final ground states through the first 1 + state, 1 l + , of the intermediate odd-odd nucleus, for those odd-odd nuclei where the 1 l + state is the ground state. To investigate the validity of the SSDH we have performed a systematical theoretical analysis of all known double-beta-decay transitions where the SSDH conditions are fulfilled. the calculations are based on the quasiparticle random-phase approximation (QRPA) and the results have been obtained by using realistic single-particle bases and real…

PhysicsNuclear and High Energy Physicsmedicine.anatomical_structuremedicineQuasiparticleState (functional analysis)Atomic physicsGround stateNucleusNuclear Physics A
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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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Spectroscopy at the two-proton drip line: Excited states in 158W

2017

Abstract Excited states have been identified in the heaviest known even-Z N = 84 isotone 158W, which lies in a region of one-proton emitters and the two-proton drip line. The observation of γ-ray transitions feeding the ground state establishes the excitation energy of the yrast 6+ state confirming the spin-gap nature of the α-decaying 8+ isomer. The 8+ isomer is also expected to be unbound to two-proton emission but no evidence for this decay mode was observed. An upper limit for the two-proton decay branch has been deduced as b 2 p ≤ 0.17% at the 90% confidence level. The possibility of observing two-proton emission from multiparticle isomers in nearby nuclides is considered.

PhysicsNuclear and High Energy Physicsproton radioactivityProtonta114010308 nuclear & particles physicsYrastNuclear Theory01 natural scienceslcsh:QC1-999Excited state0103 physical sciencesNuclideAtomic physics010306 general physicsSpectroscopyGround stateNuclear Experimentmultiparticle excited stateslcsh:PhysicsExcitationLine (formation)Physics Letters B
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Nuclear ground-state properties in a relativistic Meson-Field theory

1986

We investigate the ability of a relativistic Mean-Field theory to reproduce nuclear ground state properties by an exhaustive fit to experimental data. We find that the bulk properties of nuclei from16O to208Pb can be adjusted very well. There remain problems with level density and fluctuations in the charge density similar as in fits using the conventional Skyrme Hartree-Fock model.

PhysicsNuclear and High Energy Physicssymbols.namesakeMesonDirac equationQuantum electrodynamicsNuclear TheorysymbolsForm factor (quantum field theory)Charge densityNuclear fusionField theory (psychology)Ground stateZeitschrift f�r Physik A Atomic Nuclei
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Proton emission from an oblate nucleus 151Lu

2013

Abstract Excited states in the proton-unbound nucleus 151Lu have been established using γ-ray coincidence techniques. The lifetime of the first excited state above the proton-emitting ground state has been measured using the recoil-distance Doppler-shift method combined with recoil-decay tagging. The experimental level scheme and extracted lifetime have been compared with state-of-the-art theoretical calculations based upon a non-adiabatic deformed Woods–Saxon potential. This comparison suggests that the proton-emitting ground state in 151Lu is mildly oblate with a deformation β = − 0.11 − 0.05 + 0.02 and represents the best evidence to date for proton emission from an oblate nucleus.

PhysicsNuclear and High Energy Physicsta114010308 nuclear & particles physicsNuclear TheoryHadronElementary particle01 natural sciences7. Clean energyBaryonmedicine.anatomical_structureExcited state0103 physical sciencesmedicineddc:530Atomic physicsProton emissionNuclear Experiment010306 general physicsGround stateNucleonNucleusPhysics Letters B
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Investigation of the Δn = 0 selection rule in Gamow-Teller transitions: The β-decay of 207Hg

2019

5 pags., 3 figs., 1 tab. -- Open Access funded by Creative Commons Atribution Licence 4.0

PhysicsNuclear and High Energy Physicsta114010308 nuclear & particles physicsState (functional analysis)01 natural scienceslcsh:QC1-999Nuclear physicsmedicine.anatomical_structureNucleosynthesis0103 physical sciencesmedicineNuclear Physics - ExperimentLimit (mathematics)Gamow-Teller transitionsydinfysiikka010306 general physicsGround stateWave functionNuclear ExperimentNucleuslcsh:PhysicsPhysics Letters B
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Global analysis of 12CH335Cl and 12CH337Cl: simultaneous fit of the lower five polyads (0–2600cm−1)

2005

Abstract The global analysis of the infrared spectrum of chloromethane involving the ground state and the 13 vibrational states lying up to 2600 cm −1 is reported. This work incorporates and extends to the fifth polyad, the preliminary study of the lower four polyads published by [J. Mol. Spectrosc. 221 (2003) 199]. More than 20 000 transitions (including numerous hot bands) for each isotopomer 12 CH 3 35 Cl and 12 CH 3 37 Cl have been assigned and fitted with a standard deviation of about 3 × 10 −4  cm −1 close to the experimental precision. A common set of 288 (resp. 303) effective parameters was determined for each isotopomer. Our global model allowed us to reproduce simultaneously and a…

PhysicsNuclear magnetic resonanceInfraredPhysical and Theoretical ChemistryAtomic physicsGround statePolyadGlobal modelSpectroscopyAtomic and Molecular Physics and OpticsStandard deviationIsotopomersJournal of Molecular Spectroscopy
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High-resolution studies of beta-delayed proton emitters at IGISOL facility

1998

Beta-decays of23Al and41Ti have been studied by applying ion guide techniques, gamma detection and a gas-Si telescope for charged-particle detection. The experimental beta-decay strength of41Ti was found to be quenched by a factor ofq2 = 0.64 compared to our shell model calculations below 8 MeV excitation energy in41Sc. This result is in line with the generally accepted value ofq = 0.77. The isobaric analogue state of the41Ti ground state was measured to contain 10(8)% isospin impurity. This relatively high value could be well reproduced by the shell model calculation in thesdfp space. Gamma-decay of theT = 3/2 isobaric analogue state in23Mg was observed together with its decay by proton em…

PhysicsNuclear physicsDecay schemeProtonIsospinNuclear TheoryIsobaric processProton emissionAtomic physicsNuclear ExperimentGround stateExcitationIon
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Moments and Radii of 78–100Sr

1988

The chain of Sr isotopes ranges from the neutron-shell closure at N = 50 into both the N = 38 and N = 60 deformation regions which represent the main topic of this workshop. For a detailed understanding of the nature of these nuclei, laser spectroscopy can provide the ground state spins and moments, as well as the the changes in the mean square charge radii as a function of the neutron number N. Recent experiments at Karlsruhe [1] and at Daresbury [2] essentially cover the neutron-deficient and stable Sr isotopes between N = 40 and N = 50. In order to complement these results, and to extend the measurements into the region of neutron-rich isotopes, we have performed an experiment at the ISO…

PhysicsNuclear physicsMean squareLarge Hadron ColliderSpinsIsotopeCharge radiusNeutron numberNuclear TheoryNuclear ExperimentGround stateSpectroscopy
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