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NSR database version of April 29, 2024.

Search: Author = G.Bassani

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1975SE08      Phys.Rev. C11, 2087 (1975)

K.K.Seth, K.A.Buzard, J.Picard, G.Bassani

Comment on the ⁸⁷Sr(d, p) Reaction

NUCLEAR REACTIONS ⁸⁷Sr(d, p), E=12 MeV; analyzed data. ⁸⁸Sr levels deduced revised two-body matrix elements.

doi: 10.1103/PhysRevC.11.2087
Citations: PlumX Metrics

1974SE10      Phys.Rev. C10, 1928 (1974)

K.K.Seth, K.A.Buzard, J.Picard, G.Bassani

⁸⁷Sr(d, p)⁸⁸Sr Reaction

NUCLEAR REACTIONS ⁸⁷Sr(d, p), E=12 MeV; measured σ(Ep, θ). ⁸⁸Sr deduced levels, J, π.

doi: 10.1103/PhysRevC.10.1928
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1577.

1972BA52      Nucl.Phys. A189, 353 (1972)

G.Bassani, N.Saunier, B.M.Traore, J.Raynal, A.Foti, G.Pappalardo

Optical-Model Analysis of ⁶Li Elastic Scattering

NUCLEAR REACTIONS ¹¹B, ¹²C, ¹³C(⁶Li, ⁶Li), E=28 MeV; measured σ(θ); deduced optical potentials. Self-supporting enriched ¹¹B, ¹³C targets. Natural ¹²C target.

doi: 10.1016/0375-9474(72)90300-4
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1971BA31      Phys.Lett. 34B, 612 (1971)

G.Bassani, G.Pappalardo, N.Saunier, B.M.Traore

The ¹⁶O First Rotational Band from the ¹²C(⁶Li, d)¹⁶O Reaction

NUCLEAR REACTIONS ¹²C(⁶Li, d), E=20-32 MeV; measured σ(Ed, θ). ¹⁶O deduced levels, J, π, level-width, rotational band structure.

doi: 10.1016/0370-2693(71)90152-3
Citations: PlumX Metrics

1969BA21      Nucl.Phys. A131, 653 (1969)

G.Bassani, J.Picard

Spectroscopic Studies in the A = 90 Mass Region (II). Neutron Hole States in N = 49 Nuclei

NUCLEAR REACTIONS ⁸⁸Sr, ⁸⁹Y, ⁹⁰Zr, ⁹²Mo(³He, α), E=18 MeV; measured σ(Eα, θ). ⁸⁷Sr, ⁸⁸Y, ⁸⁹Zr, ⁹¹Mo deduced levels, J, π, L, S. Enriched targets.

doi: 10.1016/0375-9474(69)90601-0
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1969BA50      Phys.Letters 30B, 621 (1969)

G.Bassani, T.H.Kruse, N.Saunier, G.Souchere

The ¹³C(⁶Li, t)¹⁶O Reaction at 20 MeV

NUCLEAR REACTIONS ¹³C(⁶Li, t), E = 20 MeV; measured σ(Et, θ). ¹⁶O deduced levels.

doi: 10.1016/0370-2693(69)90075-6
Citations: PlumX Metrics

1969PI05      Nucl.Phys. A131, 636 (1969)

J.Picard, G.Bassani

Spectroscopic Studies in the A = 90 Mass Region (I). The (³He, d) reaction on ⁸⁸Sr, ⁹⁰Zr and ⁹²Mo Nuclei

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo(³He, d), E=18 MeV; measured σ(Ed, θ). ⁸⁹Y, ⁹¹Nb, ⁹³Tc deduced levels, J, π, L, S. Enriched targets.

doi: 10.1016/0375-9474(69)90600-9
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1968BA55      Proc.Intern.Conf.Nucl.Struct., Tokyo (1967), J.Sanada, Ed., Suppl.J.Phys.Soc.Japan 24, 649 (1968)

G.Bassani, J.Picard, N.Saunier, G.Souchere

Neutron Hole States in N = 49 Nuclei

NUCLEAR REACTIONS ⁸⁸Sr, ⁸⁹Y, ⁹⁰Zr, ⁹²Mo(³He, α), E=18 MeV; measured σ(θ). ⁸⁷Sr, ⁸⁸Y, ⁸⁹Zr, ⁹¹Mo deduced levels, L(n), S.

1968BA56      J.Phys.(Paris), Suppl.No.1, Colloq.C1-162 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

La Reaction (tau, d) sur les Noyaux ⁸⁸Sr, ⁹⁰Zr et ⁹²Mo

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo(³He, d), E=18 MeV; measured σ(θ). ⁸⁹Y, ⁹¹Nb, ⁹³Tc deduced levels, L(p), S.

1968BA57      J.Phys.(Paris), Suppl.No.1, Colloq.C1-163 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

Etats de Trou de Neutron dans les Noyaux N = 50

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo(³He, α), E=18 MeV; measured σ(Eα, θ). ⁸⁷Sr, ⁸⁹Zr, ⁹¹Mo deduced levels, L(n), S.

1967BA68      Contrib.Intern.Conf.Nucl.Struct., Tokyo, p.125 (1967)

G.Bassani, J.Picard, N.Saunier, G.Souchere

Neutron Hole States in N=49 Nuclei

NUCLEAR REACTIONS ⁸⁸Sr, ⁸⁹Y, ⁹⁰Zr, ⁹²Mo(³He, α), E=18 MeV; measured σ(θ). ⁸⁷Sr, ⁸⁸Y, ⁸⁹Zr, ⁹¹Mo deduced levels, L(n), S.

1966BA12      Phys.Letters 21, 442 (1966)

G.Bassani, Y.Cassagnou, C.Levi, L.Papineau

Spectroscopic Informations on Samarium Isotopes from Analogue State Experiments

NUCLEAR STRUCTURE ¹⁵¹Eu, ¹⁴⁹Eu, ¹⁵³Eu; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90524-5
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1966BA25      Phys.Letters 22, 189 (1966)

G.Bassani, M.Conjeaud, J.Gastebois, S.Harar, J.M.Laget, J.Picard, Y.Cassagnou

(³He, d) Reactions on the Even Sn Isotopes

NUCLEAR STRUCTURE ¹²¹Sb, ¹²³Sb, ¹²⁵Sb, ¹¹⁷Sb, ¹¹³Sb, ¹¹⁹Sb, ¹¹⁵Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90569-5
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1965BA20      Phys.Rev. 139, B830 (1965)

G.Bassani, N.M.Hintz, C.D.Kavaloski, J.R.Maxwell, G.M.Reynolds

(p, t) Ground-State L = 0 Transitions in the Even Isotopes of Sn and Cd at 40 MeV, N = 62 to 74

NUCLEAR STRUCTURE ¹¹⁶Sn, ¹¹⁸Sn, ¹¹⁴Sn, ¹¹⁴Cd, ¹¹²Sn, ¹²²Sn, ¹²⁰Sn, ¹⁰⁸Cd, ¹¹²Cd, ¹¹⁰Sn, ¹¹⁰Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.139.B830
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1964BA34      Phys. Rev. 136, B1006 (1964)

G.Bassani, N.M.Hintz, C.D.Kavaloski

Nuclear Structure Information from the (p, t) Reaction, A = 46 to A = 70

NUCLEAR STRUCTURE ⁵¹Cr, ⁵³Cr, ⁵³Mn, ⁵⁶Fe, ⁵²Fe, ⁵⁴Fe, ⁴⁶Ti, ⁵⁰Cr, ⁴⁸Ti, ⁴⁹V, ⁴⁴Ti, ⁶⁶Zn, ⁶²Zn, ⁶³Cu, ⁶⁴Zn, ⁶¹Cu, ⁶²Ni, ⁵⁶Ni, ⁵⁷Co, ⁶⁰Ni, ⁵⁸Ni, ⁶⁸Zn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.136.B1006
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1963KA26      Phys.Rev. 132, 813 (1963)

C.D.Kavaloski, G.Bassani, N.M.Hintz

(p, d) Nuclear Structure Studies on Nuclei between A=12 and A=48

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ²³Mg, ²⁴Mg, ⁴⁷Ti, ³⁹Ca, ³¹S, ³³S; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.813
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1962BA35      Bull.Am.Phys.Soc. 7, No.8, 551, U1 (1962)

G.Bassani, C.D.Kavaloski, N.M.Hintz

(p, t) Reactions on Medium A Nuclei at 40 MeV

NUCLEAR STRUCTURE ⁵⁶Fe, ⁵⁵Mn, ⁵⁴Fe, ⁴⁸Ti, ⁶⁵Cu, ⁶³Cu, ⁵⁸Ni, ⁶⁰Ni; measured not abstracted; deduced nuclear properties.

1962KA19      Bull.Am.Phys.Soc. 7, No.9, 551, U2 (1962)

C.D.Kavaloski, G.Bassani, N.M.Hintz

(p, d) Nuclear-Structure Studies at 40 MeV in the Region 16 ≤ A ≤ 40

NUCLEAR STRUCTURE ²⁴Mg, ²³Mg, ³³S, ³¹S, ³⁹Ca; measured not abstracted; deduced nuclear properties.