Search results for "SHELL"

showing 10 items of 748 documents

Forbidden nonuniqueβdecays and effective values of weak coupling constants

2016

Forbidden nonunique $\ensuremath{\beta}$ decays feature shape functions that are complicated combinations of different nuclear matrix elements and phase-space factors. Furthermore, they depend in a very nontrivial way on the values of the weak coupling constants, ${g}_{\mathrm{V}}$ for the vector part and ${g}_{\mathrm{A}}$ for the axial-vector part. In this work we include also the usually omitted second-order terms in the shape functions to see their effect on the computed decay half-lives and electron spectra ($\ensuremath{\beta}$ spectra). As examples we study the fourth-forbidden nonunique ground-state-to-ground-state ${\ensuremath{\beta}}^{\ensuremath{-}}$ decay branches of $^{113}\ma…

PhysicsCoupling constantta114cadmium010308 nuclear & particles physicsElectron spectrabeta deacySpectrum (functional analysis)Nuclear shell modelindiumweak coupling01 natural sciencesSpectral line0103 physical sciencesBeta (velocity)beta spectrum010306 general physicsMathematical physicsPhysical Review C
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Octupole states in Tl207 studied through β decay

2020

The β decay of 207Hg into the single-proton-hole nucleus 207Tl has been studied through γ-ray spectroscopy at the ISOLDE Decay Station (IDS) with the aim of identifying states resulting from coupling of the πs−11/2, πd−13/2, and πh−111/2 shell model orbitals to the collective octupole vibration. Twenty-two states were observed lying between 2.6 and 4.0 MeV, eleven of which were observed for the first time, and 78 new transitions were placed. Two octupole states (s1/2-coupled) are identified and three more states (d3/2-coupled) are tentatively assigned using spin-parity inferences, while further h11/2-coupled states may also have been observed for the first time. Comparisons are made with st…

PhysicsCoupling010308 nuclear & particles physicsSHELL modelState (functional analysis)01 natural sciencesAtomic orbital0103 physical sciencesAtomic physics010306 general physics10. No inequalityNucleonSpectroscopyMixing (physics)Physical Review C
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Closed-shell coupled-cluster theory with spin-orbit coupling

2008

A two-component closed-shell coupled-cluster (CC) approach using relativistic effective core potentials with spin-orbit coupling included in the post-Hartree-Fock treatment is proposed and implemented at the CC singles and doubles (CCSD) level as well as at the CCSD level augmented by a perturbative treatment of triple excitations [CCSD(T)]. The latter invokes as an additional approximation the neglect of the occupied-occupied and virtual-virtual blocks of the spin-orbit coupling matrix in order to avoid the iterative N(7) steps in the treatment of triple excitations. The computational effort of the implemented two-component CC methods is about 10-15 times that of its corresponding nonrelat…

PhysicsCouplingCoupled clusterField (physics)Quantum electrodynamicsGeneral Physics and AstronomyMolecular orbitalPerturbation theory (quantum mechanics)Spin–orbit interactionPhysical and Theoretical ChemistryTriplet stateOpen shellThe Journal of Chemical Physics
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Analytic energy gradients in closed-shell coupled-cluster theory with spin-orbit coupling

2008

Gradients in closed-shell coupled-cluster (CC) theory with spin-orbit coupling included in the post Hartree-Fock treatment have been implemented at the CC singles and doubles (CCSD) level and at the CCSD level augmented by a perturbative treatment of triple excitations [CCSD(T)]. The additional computational effort required in analytic energy-gradient calculations is roughly the same as that for ground-state energy calculations in the case of CCSD, and it is about twice in the case of CCSD(T) calculations. The structures, harmonic frequencies, and dipole moments of some heavy-element compounds have been calculated using the present analytic energy-gradient techniques including spin-orbit co…

PhysicsCouplingStructure (category theory)General Physics and AstronomySpin–orbit interactionDipoleCoupled clusterQuantum electrodynamicsPhysics::Atomic and Molecular ClustersHarmonicPhysics::Chemical PhysicsPhysical and Theoretical ChemistryAtomic physicsOpen shellHyperfine structureThe Journal of Chemical Physics
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Isomer Spectroscopy in90216Th126and the Magicity of92218U126

2001

Excited states in (216)Th were investigated via prompt and delayed gamma decays and the recoil-decay tagging method. The decay schemes of the I(pi) = (8+), t(1/2) = 128(8) micros, the I(pi) = (11-), t(1/2) = 615(55) ns, and the I(pi) = (14+), t(1/2) > or = 130 ns isomers were established. The configuration pi h(9/2)f(7/2) is assigned to the I(pi) = (8+) isomer, which implies that the h(9/2) and f(7/2) states are nearly degenerate. This is ascribed to increased binding of the f(7/2) orbital by its coupling to a low-lying I(pi) = (3-) state at E(x) = 1687 keV. The role of octupole and pairing correlations for a Z = 92 shell closure prediction is discussed on the basis of shell model calculati…

PhysicsCrystallographyNuclear magnetic resonancePairingExcited stateDegenerate energy levelsSHELL modelPiGeneral Physics and AstronomySpectroscopyPhysical Review Letters
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Equivalent-Single-Layer discontinuous Galerkin methods for static analysis of multilayered shells

2021

Abstract An original formulation for the elastic analysis of multilayered shells is presented in this work. The key features of the formulation are: the representation of the shell mean surface via a generic system of curvilinear coordinates; the unified treatment of general shell theories via an Equivalent-Single-Layer approach based on the through-the-thickness expansion of the covariant components of the displacement field; and an Interior Penalty discontinuous Galerkin scheme for the solution of the set of governing equations. The combined use of these features enables a high-order solution of the multilayered shell problem. Several numerical tests are presented for isotropic, orthotrop…

PhysicsCurvilinear coordinatesApplied MathematicsMathematical analysisIsotropyShell (structure)02 engineering and technologyOrthotropic material01 natural sciences020303 mechanical engineering & transports0203 mechanical engineeringDiscontinuous Galerkin methodModeling and Simulation0103 physical sciencesDisplacement fieldCovariant transformationDiscontinuous galerkin methods Equivalent-Single-Layer theories High-order modelling Multilayered shellsBoundary value problemSettore ING-IND/04 - Costruzioni E Strutture Aerospaziali010301 acoustics
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β decay of Cd127 and excited states in In127

2019

A dedicated spectroscopic study of the β decay of 127Cd was conducted at the IGISOL facility at the University of Jyvaskyla. Following high-resolution mass separation in a Penning trap, β-γ-γ coincidences were used to considerably extend the decay scheme of 127In. The β-decaying 3/2+ and 11/2- states in 127Cd have been identified with the 127Cd ground state and the 283-keV isomer. Their respective half-lives have been measured to 0.45(+12-8)s and 0.36(4) s. The experimentally observed β feeding to excited states of 127In and the decay scheme of 127In are discussed in conjunction with large-scale shell-model calculations.

PhysicsDecay scheme010308 nuclear & particles physicsNuclear shell modelPenning trap01 natural sciencesBeta decayMass separationExcited state0103 physical sciencesGamma spectroscopyAtomic physics010306 general physicsGround statePhysical Review C
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Nuclear energy density optimization: Shell structure

2013

Nuclear density functional theory is the only microscopical theory that can be applied throughout the entire nuclear landscape. Its key ingredient is the energy density functional. In this work, we propose a new parameterization UNEDF2 of the Skyrme energy density functional. The functional optimization is carried out using the POUNDerS optimization algorithm within the framework of the Skyrme Hartree-Fock-Bogoliubov theory. Compared to the previous parameterization UNEDF1, restrictions on the tensor term of the energy density have been lifted, yielding a very general form of the energy density functional up to second order in derivatives of the one-body density matrix. In order to impose c…

PhysicsDensity matrixNuclear and High Energy PhysicsWork (thermodynamics)ta114Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsOrbital-free density functional theoryBinding energyNuclear TheoryFOS: Physical sciences01 natural sciencesComputational physicsNuclear physicsNuclear Theory (nucl-th)0103 physical sciencesTensor010306 general physicsParametrizationOpen shellNuclear density
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Experimental and theoretical study of thenf-level lifetimes of potassium

2008

The theoretical and experimental values of the 5f ,6 f ,7 f, and 8f radiative lifetimes of neutral potassium are reported. The reduced matrix elements for all allowed electric-dipole nf5/2-nd5/2, nf5/2-nd3/2, and nf7/2-nd5/2 transitions with n =5–8 in K arecalculated using the relativistic linearized coupled-cluster method with single and double excitations of Dirac-Fock wave functions included to all orders in many-body perturbation theory. The resulting electric-dipole matrix elements are used to evaluate the lifetimes of the 5f ,6 f ,7 f, and 8f states in neutral K and their uncertainties. The contributions from the nf5/2-ng7/2, nf7/2-ng7/2, and nf7/2-ng9/2 transitions to the lifetimes o…

PhysicsDipoleElectric dipole momentExcited stateQuadrupoleElectron shellHartree–Fock methodAtomic physicsPerturbation theoryWave functionAtomic and Molecular Physics and OpticsPhysical Review A
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Evidence for Three Microscopically Different Kinds of E1 Transitions in Lead-Region Nuclei

1986

One outstanding feature of the shell model in heavy nuclei is that within a main shell the single-particle transitions of electric dipole (E1) character are forbidden. This leads to the experimentally observed fact that the E1 transitions are usually hindered by a factor of about 10 with respect to the Weisskopf estimate. But since there is a dispersion of about two or three orders of magnitude among these hindrance factors, the isomeric E1 transitions have not been used to elucidate the mocroscopic properties of the involved states, as has been done for the E3 transitions of this nuclear region [1]. The E3 transitions often proceed via admixtures of the low-lying collective octupole state,…

PhysicsDipoleOrders of magnitude (time)SHELL modelShell (structure)Electric dipole transitionAtomic physicsDispersion (chemistry)
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