Band termination in the N=Z Odd-Odd Nucleus 46V

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dc.creatorLenzi, S. M.
dc.creatorNapoli, D. R.
dc.creatorUr, C. A.
dc.creatorBazzacco, D.
dc.creatorBrandolini, F.
dc.creatorCameron, J. A.
dc.creatorCaurier, E.
dc.creatorde Angelis, G.
dc.creatorDe Poli, M.
dc.creatorFarnea, E.
dc.creatorGadea, A.
dc.creatorHankonen, S.
dc.creatorLunardi, S.
dc.creatorMartinez-Pinedo, G.
dc.creatorPodolyak, Zs.
dc.creatorPoves, A.
dc.creatorAlvarez, C. Rossi
dc.creatorSanchez-Solano, J.
dc.creatorSomacal, H.
dc.date1999-07-01
dc.date.accessioned2026-07-07T12:04:08Z
dc.date.available2026-07-07T12:04:08Z
dc.descriptionHigh spin states in the odd-odd N=Z nucleus 46V have been identified. At low spin, the T=1 isobaric analogue states of 46Ti are established up to I = 6+. Other high spin states, including the band terminating state, are tentatively assigned to the same T=1 band. The T=0 band built on the low-lying 3+ isomer is observed up to the 1f7/2-shell termination at I=15. Both signatures of a negative parity T=0 band are observed up to the terminating states at I = 16- and I = 17-, respectively. The structure of this band is interpreted as a particle-hole excitation from the 1d3/2 shell. Spherical shell model calculations are found to be in excellent agreement with the experimental results.
dc.description5 pages, 4 figures
dc.identifierhttps://arxiv.org/abs/nucl-ex/9907001
dc.identifierhttp://arxiv.org/abs/nucl-ex/9907001
dc.identifierPhys.Rev.C60:021303,1999
dc.identifierdoi:10.1103/PhysRevC.60.021303
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/208030
dc.subjectNuclear Experiment
dc.titleBand termination in the N=Z Odd-Odd Nucleus 46V
dc.typetext

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