Search results for "Collective model"

showing 10 items of 18 documents

Isovector and isoscalar spin-multipole giant resonances in the parent and daughter nuclei of double-β-decay triplets

2022

The strength distributions, including giant resonances, of isovector and isoscalar spin-multipole transitions in the commonly studied double-β-decay triplets are computed in the framework of the quasiparticle random-phase approximation (QRPA) using the Bonn-A two-body interaction in no-core single-particle valence spaces. The studied nuclei include the double-β parent and daughter pairs (76Ge, 76Se), (82Se, 82Kr), (96Zr, 96Mo), (100Mo, 100Ru), (116Cd, 116Sn), (128Te, 128Xe), (130Te, 130Xe), and (136Xe, 136Ba). The studied transitions proceed from the ground states to the Jπ=0−,1−,2− (spin-dipole transitions) and Jπ=1+,2+,3+ (spin-quadrupole transitions) excited states in these nuclei. Compa…

59 ≤ A ≤ 8990 ≤ A ≤ 149nuclear physicsbeetasäteilyneutriinotdouble beta decaynuclear structure & decayscollective modelshiukkasfysiikkaydinfysiikkakvasihiukkaset
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Thouless-Valatin Rotational Moment of Inertia from the Linear Response Theory

2017

Spontaneous breaking of continuous symmetries of a nuclear many-body system results in appearance of zero-energy restoration modes. Such modes introduce a non-physical contributions to the physical excitations called spurious Nambu-Goldstone modes. Since they represent a special case of collective motion, they are sources of important information about the Thouless-Valatin inertia. The main purpose of this work is to study the Thouless-Valatin rotational moment of inertia as extracted from the Nambu-Goldstone restoration mode that results from the zero-frequency response to the total angular momentum operator. We examine the role and effects of the pairing correlations on the rotational cha…

Angular momentumNuclear Theorymedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesRotary inertiaInertia114 Physical sciences01 natural sciencesbinding energy and massesMoment of inertia factorNuclear Theory (nucl-th)symbols.namesake0103 physical sciences010306 general physicsRotational partition functionEuler's equationsEQUATIONSmedia_commonPhysicsta114nuclear density functional theory010308 nuclear & particles physicstiheysfunktionaaliteoriacollective modelsMoment of inertianuclear structure and decayssuprajuoksevuusRotational energyClassical mechanicssuperfluiditysymbolsydinfysiikka
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Spectroscopy of low-spin states in $^{157}\mathrm{Dy}$: Search for evidence of enhanced octupole correlations

2019

Low-spin states of 157Dy have been studied using the JUROGAM II array, following the 155Gd ({\alpha}, 2n) reaction at a beam energy of 25 MeV. The level scheme of 157Dy has been expanded with four new bands. Rotational structures built on the [523]5/2- and [402]3/2+ neutron orbitals constitute new additions to the level scheme as do many of the inter- and intra-band transitions. This manuscript also reports the observation of cross I- to (I-1)- and I- to (I-1)+ E1 dipole transitions inter-linking structures built on the [523]5/2- (band 5) and [402]3/2+ (band 7) neutron orbitals. These interlacing band structures are interpreted as the bands of parity doublets with simplex quantum number s =…

Nuclear Theory (nucl-th)Nuclear Theorynuclear spin and parityshell modelFOS: Physical sciencescollective levelscollective modelsNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikkaNuclear Structurenuclear structure and decaysNuclear Experiment
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Neutrinoless ββ nuclear matrix elements using isovector spin-dipole Jπ = 2− data

2018

Ground-state-to-ground-state neutrinoless double-beta (0νββ) decays in nuclei of current experimental interest are revisited. In order to improve the reliability of the nuclear matrix element (NME) calculations for the light Majorana-neutrino mode, the NMEs are calculated by exploiting the newly available data on isovector spin-dipole (IVSD) Jπ=2− giant resonances. In order to correctly describe the IVSD up to and beyond the giant-resonance region, the present computations are performed in extended no-core single-particle model spaces using the spherical version of the proton-neutron quasiparticle random-phase approximation (pnQRPA) with two-nucleon interactions based on the Bonn one-boson-…

Nuclear Theorycollective modelscharge-exchange reactionsNuclear Experimentydinfysiikkaneutrinoless double beta decay
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Isovector spin-multipole strength distributions in double-β-decay triplets

2017

In this work the energetics and strength distributions of isovector spin-dipole and spin-quadrupole transitions from the ground states of the pairs (76Ge, 76Se), (82Se, 82Kr), (96Zr, 96Mo), (100Mo, 100Ru), (116Cd, 116Sn), (128Te, 128Xe), (130Te, 130Xe), and (136Xe, 136Ba), of double-β-decay initial and final nuclei, to the Jπ=0−,1−,2−,1+,2+, and 3+ excited states of the intermediate odd-odd nuclei 76As, 82Br, 96Nb, 100Tc, 116In, 128,130I, and 136Cs are investigated. The calculations are performed using a proton-neutron quasiparticle random-phase approximation (pnQRPA) theory framework with the Bonn-A two-body interaction in no-core single-particle valence spaces. peerReviewed

Nuclear Theorydouble beta decaycharge-exchange reactionscollective models
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Structure of transactinide nuclei with relativistic energy density functionals

2013

A microscopic theoretical framework based on relativistic energy density functionals (REDFs) is applied to studies of shape evolution, excitation spectra, and decay properties of transactinide nuclei. Axially symmetric and triaxial relativistic Hartree-Bogoliubov (RHB) calculations, based on the functional DD-PC1 and with a separable pairing interaction, are performed for the even-even isotopic chains between Fm and Fl. The occurrence of a deformed shell gap at neutron number $N=162$ and its role on the stability of nuclei in the region around $Z=108$ is investigated. A quadrupole collective Hamiltonian, with parameters determined by self-consistent constrained triaxial RHB calculations, is…

Nuclear and High Energy PhysicsNuclear TheoryTransactinide element01 natural sciencesenergy density functionalsSeparable spacesymbols.namesake0103 physical sciences010306 general physicsPhysicsta114010308 nuclear & particles physicsObservablecollective modelstransactinide nuclei ; energy density functionals ; collective modelsNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.transactinide nucleiTheoretical nuclear physicsPairingNeutron numberQuadrupolesymbolsAtomic physicsHamiltonian (quantum mechanics)Axial symmetry
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Lifetime measurements of excited states in $^{163}$W and the implications for the anomalous B(E2) ratios in transitional nuclei

2019

Grahn, Tuomas/0000-0002-6255-2279; Herzan, Andrej/0000-0002-6736-7638; Cullen, Dave/0000-0002-0041-1606; Barber, Liam/0000-0002-7409-9352; Keatings, James Michael/0000-0003-4271-8021; SAYGI, BAHADIR/0000-0001-5406-506X; Greenlees, Paul/0000-0002-5986-5274; Spagnoletti, Pietro/0000-0002-7674-989X; Parr, Edward/0000-0001-6204-4461; Bondili, S Nara Singh/0000-0002-4096-2429

Nuclear and High Energy PhysicsspektroskopiaNuclear TheoryMean lifetimes[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencessymbols.namesake0103 physical sciencesCollective modelmedicineNeutronGamma spectroscopy010306 general physicsNuclear ExperimentPhysicsmean lifetimes010308 nuclear & particles physicsRecoil-distance Doppler-shift methodlcsh:QC1-999Nuclear deformationGamma-ray SpectroscopyCore (optical fiber)Rotational modelmedicine.anatomical_structureB(E2) reduced transition probabilitiesgamma-ray spectroscopyExcited statesymbolsAtomic physicsydinfysiikkaNucleusDoppler effectlcsh:Physics
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Excitation and decay of two-phonon giant dipole resonances

1999

Abstract In heavy ion collisions at near relativistic energies, electromagnetic excitation of the double giant dipole resonance occurs with large cross sections. We summarize the presently available experimental data and discuss related theoretical efforts. Emphasis is paid to the question of anharmonicities and to the damping of the two-phonon states.

Nuclear physicsPhysicsNuclear reactionNuclear and High Energy PhysicsDipolePhononGiant resonanceCollective modelResonanceHeavy ionAtomic physicsExcitationNuclear Physics A
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X(5) critical-point symmetries in 138Gd

2011

International audience; The lifetimes of low-lying transitions in 138Gd have been measured using the recoil-distance Doppler-shift technique. The resultant reduced transition probabilities have been compared to X(5) critical-point calculations to assess the potential 'phase-transitional' behaviour of 138Gd. The X(5) symmetry describes the first order 'phase transition' between sphericity, U(5) and an axially deformed nuclear shape, SU(3). Although a high degree of correspondence is observed between the experimental and theoretical excitation energies, the large uncertainties of the experimental B(E2) values cannot preclude contributions from either vibrational or rotational modes of excitat…

PhysicsHistory010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]First order01 natural sciencesCritical point (mathematics)Computer Science ApplicationsEducationBohr modelSphericityKokeellinen ydinfysiikka21.10.Tg Lifetimes widths 27.60.+j 90(less-than-or-equal-to)A(less-than-or-equal-to)149 21.65.-f Nuclear matter 23.20.-g Electromagnetic transitions 21.10.Re Collective levels 21.60.Ev Collective modelssymbols.namesakeQuantum mechanics0103 physical sciencesHomogeneous spacesymbolsExperimental nuclear physics010306 general physicsHamiltonian (quantum mechanics)Axial symmetryExcitation
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Isovector spin-multipole strength distributions in double- β -decay triplets

2017

In this work the energetics and strength distributions of isovector spin-dipole and spin-quadrupole transitions from the ground states of the pairs ($^{76}\mathrm{Ge}, ^{76}\mathrm{Se}$), ($^{82}\mathrm{Se}, ^{82}\mathrm{Kr}$), ($^{96}\mathrm{Zr}, ^{96}\mathrm{Mo}$), ($^{100}\mathrm{Mo}, ^{100}\mathrm{Ru}$), ($^{116}\mathrm{Cd}, ^{116}\mathrm{Sn}$), ($^{128}\mathrm{Te}, ^{128}\mathrm{Xe}$), ($^{130}\mathrm{Te}, ^{130}\mathrm{Xe}$), and ($^{136}\mathrm{Xe}, ^{136}\mathrm{Ba}$), of double-$\ensuremath{\beta}$-decay initial and final nuclei, to the ${J}^{\ensuremath{\pi}}={0}^{\ensuremath{-}},{1}^{\ensuremath{-}},{2}^{\ensuremath{-}},{1}^{+},{2}^{+}$, and ${3}^{+}$ excited states of the interm…

PhysicsValence (chemistry)ta114Isovector010308 nuclear & particles physicsdouble beta decaycollective models01 natural sciencesExcited state0103 physical sciencesQuasiparticlecharge-exchange reactionsAtomic physics010306 general physicsMultipole expansionSpin (physics)Physical Review C
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