0000000000174300

AUTHOR

Morten Hjorth-jensen

showing 9 related works from this author

Shell-Model Effective Operators for Muon Capture in ^{20}Ne

1999

It has been proposed that the discrepancy between the partially-conserved axial-current prediction and the nuclear shell-model calculations of the ratio $C_P/C_A$ in the muon-capture reactions can be solved in the case of ^{28}Si by introducing effective transition operators. Recently there has been experimental interest in measuring the needed angular correlations also in ^{20}Ne. Inspired by this, we have performed a shell-model analysis employing effective transition operators in the shell-model formalism for the transition $^{20}Ne(0^+_{g.s.})+\mu^- \to ^{20}F(1^+; 1.057 MeV) + \nu_\mu$. Comparison of the calculated capture rates with existing data supports the use of effective transiti…

Nuclear Theory (nucl-th)PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryFormalism (philosophy)SHELL modelFOS: Physical sciencesAnisotropyMuon capture
researchProduct

Magnetic dipole moments near 132Sn: new measurement on 135I by NMR/ON

1998

Abstract On-line low temperature nuclear orientation (OLNO) experiments have been performed on the isotope 135 I using the technique of nuclear magnetic resonance on oriented nuclei (NMR/ON). The magnetic moment of the 7 2 + ground state has been measured to be μ( 7 2 + 135 I ) = 2.940(2) μ N , thereby extending the known data on these states in odd- A I isotopes up to the neutron shell closure at N = 82. Shell-model calculations have been performed for the magnetic moments of 7 2 + states in the N = 82 isotones using free-nucleon and effective g -factors. The effective g -factors are obtained from a perturbation calculation that includes corrections for core polarisation and meson-exchange…

PhysicsNuclear and High Energy PhysicsMagnetizationMagnetic energyMagnetic momentNeutron magnetic momentProton magnetic momentNuclear TheoryNuclear magnetic momentAtomic physicsNuclear ExperimentMagnetic dipoleElectron magnetic dipole momentNuclear Physics A
researchProduct

Extended shell model calculation for even N = 82 isotones with a realistic effective interaction

1996

The shell model within the $2s1d0g_{7/2}0h_{11/2}$ shell is applied to calculate nuclear structure properties of the even Z=52 - 62, N=82 isotones. The results are compared with experimental data and with the results of a quasiparticle random-phase approximation (QRPA) calculation. The interaction used in these calculations is a realistic two-body G-matrix interaction derived from modern meson-exchange potential models for the nucleon-nucleon interaction. For the shell model all the two-body matrix elements are renormalized by the $\hat{Q}$-box method whereas for the QRPA the effective interaction is defined by the G-matrix.

Nuclear Theory (nucl-th)PhysicsNuclear and High Energy PhysicsMatrix (mathematics)Nuclear TheorySHELL modelNuclear TheoryShell (structure)Nuclear structureQuasiparticleFOS: Physical sciencesNuclear ExperimentMolecular physics
researchProduct

Nuclear structure theory for the astrophysical rp-process and r-process

2003

Abstract The astrophysical processes of rapid-proton capture and rapid-neutron capture require the knowledge of many nuclear properties which are not known from experiment. I will describe two examples of how theoretical models are used to provide this input. The first of these uses the Hartree-Fock method for displacement energies to obtain the masses of proton-rich nuclei needed for the rp-process. The second uses a model for configuration mixing near 132 Sn to provide Q values and beta-decay lifetimes for the r-process.

Nuclear physicsPhysicsNuclear and High Energy PhysicsAstrophysical ProcessesMixing (mathematics)Nuclear TheoryNuclear structureTheoretical modelsr-processrp-processNuclear ExperimentDisplacement (vector)Nuclear Physics A
researchProduct

Renormalization of the weak hadronic current in the nuclear medium

2000

The renormalization of the weak charge-changing hadronic current as a function of the reaction energy release is studied at the nucleonic level. We have calculated the average quenching factors for each type of current (vector, axial vector and induced pseudoscalar). The obtained quenching in the axial vector part is, at zero momentum transfer, 19% for the sd shell and 23% in the fp shell. We have extended the calculations also to heavier systems such as $^{56}$Ni and $^{100}$Sn, where we obtain stronger quenchings, 44% and 59%, respectively. Gamow--Teller type transitions are discussed, along with the higher order matrix elements. The quenching factors are constant up to roughly 60 MeV mom…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryMomentum transferHadronFOS: Physical sciencesInverseType (model theory)7. Clean energy01 natural sciencesNuclear Theory (nucl-th)RenormalizationPseudoscalar0103 physical sciencesNuclear Experiment010306 general physicsNucleonPseudovectorPhysical Review C
researchProduct

Study of medium-spin states of neutron-rich 87, 89, 91Rb isotopes

2019

International audience; Excited states of the rubidium isotopes$_{37}^{87, 89, 91}$Rb have been studied at the INFN Legnaro National Laboratory. Measurements of the $\gamma$ -ray decay of fragments produced in binary grazing reactions resulting from the interaction of a beam of 530 MeV$^{96}$Zr ions with a$^{124}$Sn target have been complemented by studies of the $\gamma$ -ray decay of fission fragments produced in the interaction of a beam of 230 MeV$^{36}$S ions with a thick$^{176}$Yb target. The structure of the yrast states of$_{37}^{87, 89, 91}$Rb has been discussed within the context of spherical shell-model and cranked Nilsson-Strutinsky calculations.

PhysicsNuclear and High Energy PhysicsSpin states[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsFissionYrastNuclear TheoryContext (language use)01 natural sciencesIsotopes of rubidiumNuclear physicsExcited state0103 physical sciencesnuclear structure ; Rb isotopesPhysics::Accelerator PhysicsNuclear fusionNeutronNuclear Experiment010306 general physicsydinfysiikka
researchProduct

White paper: from bound states to the continuum

2020

This white paper reports on the discussions of the 2018 Facility for Rare Isotope Beams Theory Alliance (FRIB-TA) topical program ‘From bound states to the continuum: Connecting bound state calculations with scattering and reaction theory’. One of the biggest and most important frontiers in nuclear theory today is to construct better and stronger bridges between bound state calculations and calculations in the continuum, especially scattering and reaction theory, as well as teasing out the influence of the continuum on states near threshold. This is particularly challenging as many-body structure calculations typically use a bound state basis, while reaction calculations more commonly utili…

Nuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Structure (category theory)nucleus: structure functionFew-body systems[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesMany-body problemTheoretical physicsFew-body systems0103 physical sciencesBound stateReactionsNuclear structure010306 general physicsPhysicsBasis (linear algebra)010308 nuclear & particles physicsContinuum (topology)ScatteringscatteringNuclear structurePhysique atomique et nucléairebound statefew-body problemmany-body problem
researchProduct

N=82Shell Quenching of the Classicalr-Process “Waiting-Point” NucleusCd130

2003

First $\ensuremath{\beta}$- and $\ensuremath{\gamma}$-spectroscopic decay studies of the $N=82$ $r$-process ``waiting-point'' nuclide $^{130}\mathrm{C}\mathrm{d}$ have been performed at CERN/ISOLDE using the highest achievable isotopic selectivity. Several nuclear-physics surprises have been discovered. The first one is the unanticipatedly high energy of 2.12 MeV for the [$\ensuremath{\pi}{g}_{9/2}\ensuremath{\bigotimes}\ensuremath{\nu}{g}_{7/2}]$ ${1}^{+}$ level in $^{130}\mathrm{I}\mathrm{n}$, which is fed by the main Gamow-Teller transition. The second surprise is the rather high ${Q}_{\ensuremath{\beta}}$ value of 8.34 MeV, which is in agreement only with recent mass models that include…

PhysicsQuenchingHigh energyParticle physicsmedicine.anatomical_structuremedicineShell (structure)General Physics and Astronomyr-processAtomic physicsNuclear ExperimentNucleusPhysical Review Letters
researchProduct

β-decay studies of135–137Snusing selective resonance laser ionization techniques

2002

The decays of the very neutron rich Sn isotopes Sn135-137 were studied at CERN/ISOLDE using isotopic and isobaric selectivity achieved by the use of a resonance ionization laser ion source and mass spectroscopy, respectively. Neutron decay rates, gamma-ray singles, and gamma-gamma coincidence data were collected as a function of time. The half-life (T-1/2) and delayed neutron emission probability (P-n) values of 135 Sn were measured to be 530(20) ms and 21(3)%, respectively. For Sn-136, a T-1/2 of 250(30) ms was determined along with a P-n value of 30(5)%. For Sn-137, a T-1/2 of 190(60) ms and a P-n value of 58(15)% were deduced. Identification of low-energy transitions in Sb-135 was made p…

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaIonizationDouble beta decayExcited stateNeutronAtomic physicsMass spectrometryGround stateBeta decayDelayed neutronPhysical Review C
researchProduct