Search results for "hell"

showing 10 items of 1035 documents

Central depression in nuclear density and its consequences for the shell structure of superheavy nuclei

2006

The influence of the central depression in the density distribution of spherical superheavy nuclei on the shell structure is studied within the relativistic mean field theory. Large depression leads to the shell gaps at the proton Z=120 and neutron N=172 numbers, while flatter density distribution favors N=184 for neutrons and leads to the appearance of a Z=126 shell gap and to the decrease of the size of the Z=120 shell gap. The correlations between the magic shell gaps and the magnitude of central depression are discussed for relativistic and non-relativistic mean field theories.

PhysicsNuclear and High Energy PhysicsNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryShell (structure)FOS: Physical sciencesCharge densityNuclear Theory (nucl-th)Nuclear physicsDensity distributionPhysics::Atomic and Molecular ClustersNeutronAtomic physicsNuclear ExperimentNuclear theoryNuclear density
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Gamow-Teller decay ofZn80: Shell structure and astrophysical implications

1988

Gamow-Teller \ensuremath{\beta} decay of $^{80}\mathrm{Zn}$ to levels in $^{80}\mathrm{Ga}$ has been calculated from a random-phase-approximation shell model with Nilsson model wave functions. The predicted features are compared to existing experimental results. Gross \ensuremath{\beta}-decay properties as well as quasiparticle structure indicate shape coexistence for $^{80}\mathrm{Ga}$. This result implies a rather rapid weakening of the shell strength far from \ensuremath{\beta} stability above $_{28}^{78}\mathrm{Ni}_{50}$. The nuclear properties of $^{80}\mathrm{Zn}$ as an astrophysical ``waiting-point'' nucleus suggest that the r-process scenario which is responsible for the solar r abu…

PhysicsNuclear and High Energy PhysicsNuclear TheorySHELL modelShell (structure)QuasiparticleBeta (velocity)Atomic physicsWave functionPhysical Review C
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First measurement ofK-shell-electron to internal-pair conversion probability ratios forE0 transitions inf p shell region

1986

Magnetic plus Si(Li) spectrometers designed for high-resolution conversion-electron and internal-pair measurements, are employed to obtainK-shell-electron to internal-pair conversion probability ratios forE0 transitions in54Fe,60Ni,64Zn and70Ge. The results are found to be in good agreement with theoretical predictions.

PhysicsNuclear and High Energy PhysicsNuclear magnetic resonanceSpectrometerShell (structure)Nuclear fusionElectronAtomic physicsZeitschrift f�r Physik A Atomic Nuclei
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Gamow-Teller transitions in theA=40isoquintet of relevance for neutrino captures inAr40

2014

Background: The Gamow-Teller response of $^{40}\mathrm{Ar}$ is important for the use of liquid argon as a medium for neutrino detection. An ambiguity about the Gamow-Teller strength for the excitation of ${1}^{+}$ states at 2290 and 2730 keV in $^{40}\mathrm{K}$ results in a significant uncertainty for neutrino capture rates. This ambiguity is caused by the large discrepancy observed between strengths extracted from $^{40}\mathrm{Ar}$($p$, $n$) charge-exchange data and the transition strengths for the analog transitions studied in the $\ensuremath{\beta}$ decay of $^{40}\mathrm{Ti}$.Purpose: This study was aimed at resolving the ambiguity between the results from the $^{40}\mathrm{Ar}$($p$,…

PhysicsNuclear and High Energy PhysicsParticle physicsAmplitudeSHELL modelLiquid argonNeutrinoBorn approximationEnergy (signal processing)ExcitationNeutrino scatteringPhysical Review C
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On-shell two-loop three-gluon vertex

1998

The two-loop three-gluon vertex is calculated in an arbitrary covariant gauge, in the limit when two of the gluons are on the mass shell. The corresponding two-loop results for the ghost-gluon vertex are also obtained. It is shown that the results are consistent with the Ward-Slavnov-Taylor identities.

PhysicsNuclear and High Energy PhysicsParticle physicsLoop (graph theory)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyShell (structure)Vertex functionFOS: Physical sciencesGauge (firearms)GluonHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Vertex modelVertex (curve)Covariant transformationHigh Energy Physics::ExperimentParticle Physics - Phenomenology
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Tz = ±1 → 0 ISOSPIN SYMMETRY GAMOW-TELLER TRANSITIONS IN pf-SHELL NUCLEI

2010

Studying the Gamow-Teller (GT) transitions of stable as well as unstable pf-shell nuclei is one of the key issues in nuclear and astro-nuclear physics. Under the assumption that isospin T is a good quantum number, symmetry is expected for mirror nuclei and the GT transitions starting from the mirror nuclei. We study the GT transitions starting from Tz = ±1 mirror nuclei, respectively, by means of hadronic (3 He , t) charge-exchange reactions and complementary β decays.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHadronShell (structure)General Physics and AstronomyAstronomy and AstrophysicsKey issuesSymmetry (physics)Nuclear physicsGood quantum numberIsospinMirror nucleiNuclear ExperimentModern Physics Letters A
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Pionic decay of Lambda Hypernuclei in a Continuum Shell Model

2002

We evaluate pionic decay widths of Lambda hypernuclei using a shell model for, both the nuclear bound and the continuum nucleon wave functions in the final state, and distorted waves for the outgoing pion. An excellent agreement with the recent KEK measurement of $\pi^-$-decay widths of $^{12}_\Lambda$C and $^{28}_\Lambda$Si is found. Besides, results for $^{56}_\Lambda$Fe are consistent with the existing upper bound.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheorySHELL modelNuclear TheoryFísicaFOS: Physical sciencesState (functional analysis)LambdaUpper and lower boundsNuclear Theory (nucl-th)PionHigh Energy Physics::ExperimentContinuum (set theory)Atomic physicsNucleonWave functionNuclear Experiment
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In-beam spectroscopy at the proton-drip line. First observation of excited states in 106Sb and 107Sb

1994

Neutron deficient nuclei close to Sn-100 have been investigated in-beam using the NORDBALL detector array. A target of Fe-54 was bombarded with a beam of Ni-58 at 270 MeV. Evaporation residues were identified by detecting protons and alpha particles in a 4 pi charged particle multi-detector set-up and neutrons in a 1 pi neutron detector wall in coincidence with gamma rays. Excited states of the proton drip line nucleus Sb-106 and of Sb-107 were identified for the first time. The yrast level schemes constructed from gamma-gamma-particle coincidence and gamma-gamma angular correlation analysis are presented and discussed within the framework of the nuclear shell model.

PhysicsNuclear and High Energy PhysicsProtonAstrophysics::High Energy Astrophysical PhenomenaYrastNuclear TheoryGamma rayNuclear shell modelAlpha particleCharged particleNeutron detectionNeutronAtomic physicsNuclear ExperimentPhysics Letters B
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Identification of low-lying proton-based intruder states in189–193Pb

2002

Low-lying proton-based intruder states have been observed in the odd-mass isotopes Pb-189,Pb-191,Pb-193 in experiments at the RITU gas-filled recoil separator. The identification has been performed ...

PhysicsNuclear and High Energy PhysicsProtonIsotope010308 nuclear & particles physicsSHELL modelNuclear structure01 natural sciencesRecoil separatorNuclear physicsExcited state0103 physical sciencesAlpha decayAtomic physicsNuclear Experiment010306 general physicsRadioactive decayPhysical Review C
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Effects of orbital occupation on 0νββ nuclear matrix element

2009

We have used the recently measured neutron occupancies in the 76 Ge and 76 Se nuclei as a guideline to define the neutron quasiparticle states in the 1p0f0g shell. The adjacent odd-mass nuclei help define the corresponding proton quasiparticle states. We insert the obtained quasiparticles in a proton-neutron quasiparticle random-phase approximation (pnQRPA) calculation of the nuclear matrix element of the neutrinoless double beta (0 νββ ) decay of 76 Ge. It is found that the resulting value of the 0 νββ matrix element is not far from the recently reported shell-model result.

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryShell (structure)Nuclear matrixAtomic and Molecular Physics and OpticsNuclear physicsCondensed Matter::SuperconductivityBeta (plasma physics)QuasiparticleMatrix elementNeutronElement (category theory)Atomic physicsNuclear ExperimentNuclear Physics B - Proceedings Supplements
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