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NSR database version of April 29, 2024.

Search: Author = A.O.Gattone

Found 16 matches.

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1998CR03      Phys.Lett. 427B, 235 (1998)

R.J.Creswick, F.T.Avignone III, H.A.Farach, J.I.Collar, A.O.Gattone, S.Nussinov, K.Zioutas

Theory for the Direct Detection of Solar Axions by Coherent Primakoff Conversion in Germanium Detectors

doi: 10.1016/S0370-2693(98)00183-X
Citations: PlumX Metrics


1996DE25      Z.Phys. A355, 145 (1996)

A.Delfino, M.Chiapparini, M.Malheiro, L.V.Belvedere, A.O.Gattone

Derivative-Coupling Models and the Nuclear-Matter Equation of State

doi: 10.1007/s002180050091
Citations: PlumX Metrics


1996IZ03      Nucl.Phys. A609, 437 (1996)

E.D.Izquierdo, G.Barenboim, A.O.Gattone

Relativistic Two-Body Processes in Axial-Charge Transitions

NUCLEAR STRUCTURE 209Pb, 207Tl, 133Sn; calculated axial-charge transitions matrix elements. Relativistic two-body processes, meson-exchange, nonrelativistic, Dirac-Hartree, relativistic Hartree approximations.

doi: 10.1016/S0375-9474(96)00276-X
Citations: PlumX Metrics


1994IZ01      Phys.Rev. C49, 2005 (1994)

E.D.Izquierdo, A.O.Gattone

Ramdom-Phase-Approximation-Type Vertex Corrections to the Axial-Vector Current

NUCLEAR REACTIONS 16O(μ-, ν), E at rest; calculated muon capture rate vs model parameter C(PV). RPA type vertex corrections to axial vector current.

doi: 10.1103/PhysRevC.49.2005
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1993BA54      Phys.Rev. C48, 2537 (1993)

G.Barenboim, A.O.Gattone, E.D.Izquierdo

Meson-Exchange-Currents Contribution to Axial Charge Transitions

NUCLEAR STRUCTURE 207Tl, 209Pb; calculated meson exchange current contribution to transitions connecting to states in 207Pb, 209Bi. Mean field, relativistic Hartree approximations.

doi: 10.1103/PhysRevC.48.2537
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1993DI03      Phys.Rev. C47, 2916 (1993)

D.E.DiGregorio, S.Gil, H.Huck, E.R.Batista, A.M.J.Ferrero, A.O.Gattone

No Evidence of the 17-keV Neutrino in the Decay of 71Ge

RADIOACTIVITY 71Ge(EC); measured internal bremsstrahlung spectrum; deduced no evidence for 17 keV neutrino.

doi: 10.1103/PhysRevC.47.2916
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1992GA13      Phys.Rev. C46, 788 (1992)

A.O.Gattone, E.D.Izquierdo, M.Chiapparini

Relativity and the Enhancement of the Weak Axial-Charge Matrix Elements in the Lead Region

RADIOACTIVITY 209Pb(β-); 207Tl(β-); calculated first-forbidden β-decay matrix element; deduced matrix element enhancement. Relativistic mean field, Hartree approximations.

doi: 10.1103/PhysRevC.46.788
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1991CH19      Nucl.Phys. A529, 589 (1991)

M.Chiapparini, A.O.Gattone, B.K.Jennings

Dirac Phenomenology and the Lambda-Nucleus Potential

NUCLEAR STRUCTURE A=9-16; calculated lambda hypernuclei binding energies, spin-orbit splitting. Dirac phenomenology in potential.

doi: 10.1016/0375-9474(91)90586-U
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1991GA13      Phys.Rev. C44, 548 (1991)

A.O.Gattone, M.Chiapparini, E.D.Izquierdo

Lambda-Hypernuclei Magnetic Moments in a Relativistic Model

doi: 10.1103/PhysRevC.44.548
Citations: PlumX Metrics


1990CH02      Phys.Rev. C41, 753 (1990)

M.Chiapparini, A.O.Gattone

Medium Effects in Electric Form Factors and Transition Strengths

NUCLEAR STRUCTURE 40Ca; calculated B(λ). Relativistic model.

doi: 10.1103/PhysRevC.41.753
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1989CH24      Phys.Lett. 224B, 243 (1989)

M.Chiapparini, A.O.Gattone

Medium Induced Magnetization Current and Nuclear Magnetic Moments

NUCLEAR STRUCTURE 15N, 15,17O, 17F; calculated μ; deduced medium induced magnetization contribution.

doi: 10.1016/0370-2693(89)91223-9
Citations: PlumX Metrics


1989GA04      Phys.Lett. 219B, 22 (1989)

A.O.Gattone, J.P.Vary

Relativistic Effects in the Elastic Magnetic Form Factor of 17O

NUCLEAR REACTIONS 17O(e, e), E not given; calculated magnetic form factor.

doi: 10.1016/0370-2693(89)90829-0
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1985GA06      Phys.Rev. C31, 1430 (1985)

A.O.Gattone, B.Goulard, W-Y.P.Hwang

Recoil Effects in the Relativistically Corrected Impulse Approximation

NUCLEAR STRUCTURE 15N; calculated μ, charge radius. Relativistic impulse approximation, recoil effects.

doi: 10.1103/PhysRevC.31.1430
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1984GA15      Nucl.Phys. A424, 1 (1984)

A.O.Gattone, A.M.J.Ferrero, O.Dragun

The Contribution of One- and Two-Step Processes to Inclusive (p, d) Reactions

NUCLEAR REACTIONS, ICPND 54Fe, 209Bi(p, d), E=38.8, 62 MeV; 120Sn(p, d), E=28.8, 62 MeV; calculated σ(Ed), σ(θ). 54Fe, 209Bi(p, d), E=39, 62 MeV; calculated σ. 54Fe(p, pd), E=62 MeV; calculated σ vs transfer L. 209Bi, 54Fe(p, p'), E=62 MeV; calculated σ(Ep'); deduced one-step process dominance. Multi-step direct reaction model.

doi: 10.1016/0375-9474(84)90126-X
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1983DU13      Phys.Rev.Lett. 51, 2366 (1983)

G.G.Dussel, A.O.Gattone, E.E.Maqueda

Prediction of Enhanced Large-Angle Scattering in Heavy-Ion Elastic Reactions

NUCLEAR STRUCTURE A=20-77, Z=9-35; analyzed heavy-ion elastic scattering σ(θ) leading to compound nuclei; deduced nuclear surface transparency.

doi: 10.1103/PhysRevLett.51.2366
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1982DR07      Phys.Lett. 119B, 25 (1982)

O.Dragun, A.M.J.Ferrero, A.O.Gattone

The (p, d) Reaction: A good test to elucidate the strength of large energy loss one-step processes

NUCLEAR REACTIONS 54Fe(p, d), E=29, 39, 62 MeV; 209Bi(p, d), E=39, 62 MeV; calculated σ(θ), angle integrated σ; deduced large energy loss one-step process strength. DWBA analysis.

doi: 10.1016/0370-2693(82)90235-0
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