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NSR database version of May 1, 2024.

Search: Author = L.Losano

Found 15 matches.

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2002DI01      J.Phys.(London) G28, 121 (2002)

A.Dimarco, C.Barbero, H.Dias, F.Garcia, J.Horvath, L.Losano

Influence of Low-Lying Discrete Nuclear States on Isotopic Abundances in Presupernova Cores

NUCLEAR STRUCTURE Z=20-30; calculated astrophysical isotopic abundances, sensitivity to low-lying nuclear structure.

doi: 10.1088/0954-3899/28/1/309
Citations: PlumX Metrics

2000DI24      Int.J.Mod.Phys. E9, 319 (2000)

A.Dimarco, H.Dias, F.Garcia Velasco, L.Losano

Influence of the Low-Lying Discrete Nuclear States on the Partition Function for Stellar Electron Capture and Beta Decay Rates

NUCLEAR STRUCTURE ^56,57Fe, ^59,60Co; calculated level densities, partition functions. Application to stellar decay rates discussed.

doi: 10.1016/S0218-3013(00)00026-X
Citations: PlumX Metrics

1997CE03      Nucl.Phys. A619, 129 (1997)

C.A.P.Ceneviva, L.Losano, N.Teruya, H.Dias

Microscopic Projected-Quasiparticle Description of Odd-Mass Pb Isotopes

NUCLEAR STRUCTURE ^{193,195,197,199,201,203,205}Pb; calculated levels, magnetic dipole moments, electric quadrupole moments. ^201,203,205Pb calculated spectroscopic factors. Number-projected one- and three-quasiparticle BCS approximation, surface delta interaction.

doi: 10.1016/S0375-9474(97)00059-6
Citations: PlumX Metrics

1997TE05      Phys.Rev. C55, 1998 (1997)

N.Teruya, C.A.P.Ceneviva, H.Dias, L.Losano

Escape Width of the Giant Monopole Resonance in ⁹⁰Zr

NUCLEAR STRUCTURE ⁹⁰Zr; calculated giant monopole resonance nucleon decay widths. Collective, statistical doorway states, hybrid model of decay.

doi: 10.1103/PhysRevC.55.1998
Citations: PlumX Metrics

1996CH03      Nucl.Phys. A597, 253 (1996)

L.C.Chamon, D.Pereira, E.S.Rossi, Jr., C.P.Silva, H.Dias, L.Losano, C.A.P.Ceneviva

Isotopic Dependence of the Ion-Ion Potential in the Systems ¹⁶O + ^58,60,62,64Ni

NUCLEAR REACTIONS ^58,60,62,64Ni(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), E=34-37 MeV; measured σ(θ); deduced optical potential. ^58,60,62,64Ni levels deduced B(E2), deformation lengths. Shell-model, double-folding calculations, coupled-channel analysis.

doi: 10.1016/0375-9474(95)00467-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0937.

1996LO01      Int.J.Mod.Phys. E5, 153 (1996)

L.Losano, H.Dias

Quasiparticle and Phonon Excitations in Odd-Mass N = 83 Isotones

NUCLEAR STRUCTURE ¹³⁵Te, ¹³⁷Xe, ¹³⁹Ba, ¹⁴¹Ce, ¹⁴³Nd, ¹⁴⁵Sm, ¹⁴⁷Gd, ¹⁴⁹Dy, ¹⁵¹Er; calculated levels J, π, spectroscopic factors. Quasiparticle-phonon coupling model.

doi: 10.1142/S0218301396000074
Citations: PlumX Metrics

1996LO16      Phys.Lett. 384B, 20 (1996)

L.Losano, H.Dias, T.T.S.Kuo

Projected Quasi-Particle Calculations of ¹¹⁹Sn, ¹²¹Sn, and ¹²³Sn using Realistic Interactions

NUCLEAR STRUCTURE ^123,121,119Sn; calculated levels. Projected quasiparticle calculations, realistic interactions.

doi: 10.1016/0370-2693(96)00645-4
Citations: PlumX Metrics

1995CE07      Int.J.Mod.Phys. E4, 419 (1995)

C.A.P.Ceneviva, L.Losano, H.Dias

Number-Projected Quasiparticle Phonon Coupling Applied to Odd-Mass Te Isotopes

NUCLEAR STRUCTURE ^{115,117,119,121,123,125,127,129,131}Te; calculated levels, spectroscopic factors, μ, quadrupole moment. Number-projected quasiparticle-phonon coupling model.

doi: 10.1142/S0218301395000146
Citations: PlumX Metrics

1994DI06      Phys.Rev. C50, 1377 (1994)

H.Dias, L.Losano

Semimicroscopic Description of the Odd-A Te Isotopes

NUCLEAR STRUCTURE ^{115,117,119,121,123,125,127,129,131}Te; calculated levels, single nucleon transfer spectroscopic factors. Quasiparticle phonon model.

doi: 10.1103/PhysRevC.50.1377
Citations: PlumX Metrics

1993LO06      Phys.Rev. C48, 148 (1993)

L.Losano, M.D.O.Roos, H.Dias

Cluster-Phonon Model Applied to the ⁹¹Zr Nucleus

NUCLEAR STRUCTURE ^90,91Zr, ⁹⁰Y; calculated levels, B(λ). Cluster-phonon model.

doi: 10.1103/PhysRevC.48.148
Citations: PlumX Metrics

1992DI05      Phys.Rev. C46, 2289 (1992)

H.Dias, L.Losano

Projected Quasiparticle Calculations on the Heavy Odd-Mass N = 82 Isotones

NUCLEAR STRUCTURE ¹⁴⁷Tb, ¹⁵¹Tm, ¹⁴⁹Ho, ¹⁵³Lu; calculated levels, μ, quadrupole moments. Number projected Tamm-Dancoff approximation, quasi-particle formalism.

doi: 10.1103/PhysRevC.46.2289
Citations: PlumX Metrics

1991LO07      Phys.Rev. C44, 2536 (1991)

L.Losano, H.Dias

Projected Quasiparticle Calculations for the N = 82 Odd-Proton Isotones

NUCLEAR STRUCTURE ¹³⁷Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁴³Pm, ¹⁴⁵Eu; calculated levels, B(λ), effective μ, quadrupole moments. Projected quasiparticles, Tamm-Dancoff approximation.

doi: 10.1103/PhysRevC.44.2536
Citations: PlumX Metrics

1990AN34      Rev.Brasil.Fis. 20, 68 (1990)

R.M.Anazawa, M.N.Rao, W.A.Seale, R.V.Ribas, H.Dias, L.Losano

Lifetime in ⁹¹Zr

NUCLEAR REACTIONS ⁸⁸Sr(α, nγ), E=9.75-10.8 MeV; measured Eγ, Iγ, DSA. ⁹¹Zr levels deduced T_1/2. Shell model comparison.

1988LO12      Phys.Rev. C38, 2902 (1988)

L.Losano, H.Dias, F.Krmpotic, B.H.Wildenthal

Comparisons between Shell-Model Calculations, Seniority Truncation, and Quasiparticle Approximations: Application to the odd Ni isotopes and odd N = 82 isotones

NUCLEAR STRUCTURE ^59,61,63,65Ni, ¹³⁵I, ¹³⁷Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁴³Pm; calculated levels, μ, quadrupole moments, B(λ). Shell model.

doi: 10.1103/PhysRevC.38.2902
Citations: PlumX Metrics

1986DI06      Z.Phys. A324, 53 (1986)

H.Dias, F.Krmpotic, L.Losano, R.C.Mastroleo

Semi Microscopic Description of ⁸⁴Kr

NUCLEAR STRUCTURE ⁸⁴Kr; calculated levels, J, π, δ(E2/M1). Cluster-phonon model, pairing interaction.