0000000000328436

AUTHOR

F. Radeck

showing 5 related works from this author

Isomers and high-spin structures in the N=81 isotones Xe135 and Ba137

2017

The high-spin structures of the N = 81 isotones 135Xe and 137Ba are investigated after multinucleontransfer (MNT) and fusion-evaporation reactions. Both nuclei are populated in (i) 136Xe+238U and (ii) 136Xe+208Pb MNT reactions employing the high-resolution Advanced Gamma Tracking Array (AGATA) coupled to the magnetic spectrometer PRISMA, (iii), in the 136Xe+198Pt MNT reaction employing the -ray array GAMMASPHERE in combination with the gas detector array Chico, and (iv) via a 11B+130Te fusion-evaporation reaction. The high-spin level schemes of 135Xe and 137Ba are considerably extended to higher energies. The 2058-keV (19=2 ) state in 135Xe is identified as an isomer, completing the systema…

PhysicsSpectrometer010308 nuclear & particles physics0103 physical sciencesQuadrupoleSHELL modelGammasphereAGATAAtomic physics010306 general physicsSpin (physics)01 natural sciencesPhysical Review C
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Testing refined shell-model interactions in thesdshell: Coulomb excitation ofNa26

2015

Background: Shell-model calculations crucially depend on the residual interaction used to approximate the nucleon-nucleon interaction. Recent improvements to the empirical universal $sd$ interaction (USD) describing nuclei within the $sd$ shell yielded two new interactions---USDA and USDB---causing changes in the theoretical description of these nuclei.Purpose: Transition matrix elements between excited states provide an excellent probe to examine the underlying shell structure. These observables provide a stringent test for the newly derived interactions. The nucleus $^{26}\mathrm{Na}$ with 7 valence neutrons and 3 valence protons outside the doubly-magic ${}^{16}\mathrm{O}$ core is used a…

PhysicsNuclear and High Energy PhysicsMatrix (mathematics)Valence (chemistry)Excited stateShell (structure)Coulomb barrierNeutronObservableCoulomb excitationAtomic physicsPhysical Review C
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High-spin structure of Xe134

2016

A. Vogt et al. ; 12 págs.; 9 figs.; 1 tab.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsFissionNuclear structureAnalytical chemistryMolecularSpin structure[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Kinetic energy01 natural sciences7. Clean energyAtomicNuclear & Particles PhysicsSubatomär fysikParticle and Plasma Physics0103 physical sciencesSubatomic PhysicsHeavy ionGammasphereAGATANuclear010306 general physicsSpin (physics)Nuclear Experiment
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Coulomb excitation of Na-29,Na-30: Mapping the borders of the island of inversion

2014

Seidlitz, M., et all ; 10 pags. ; 9 figs. ; 1 tab. ; PACS number(s): 21.60.Cs, 23.20.Js, 25.70.De, 29.38.Gj

PhysicsNuclear and High Energy Physicsregionta114Spectrometer010308 nuclear & particles physicsIsland of inversionshell-modelNuclear TheoryGamma rayCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesnuclear-data sheetsExcited state0103 physical sciencesPhysics::Accelerator PhysicsAtomic physics010306 general physicsNucleonWave functionNuclear ExperimentBeam (structure)
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Testing refined shell-model interactions in the sd shell: Coulomb excitation of 26Na

2015

Background: Shell-model calculations crucially depend on the residual interaction used to approximate the nucleon-nucleon interaction. Recent improvements to the empirical universal sd interaction (USD) describing nuclei within the sd shell yielded two new interactions—USDA and USDB—causing changes in the theoretical description of these nuclei. Purpose: Transitionmatrix elements between excited states provide an excellent probe to examine the underlying shell structure. These observables provide a stringent test for the newly derived interactions. The nucleus 26Na with 7 valence neutrons and 3 valence protons outside the doubly-magic 16O core is used as a test case. Method: A radioactive b…

shell-model calculationsnucleirefined shell-model interactions
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