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NSR database version of May 9, 2024.

Search: Author = Y.Avishai

Found 16 matches.

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1989AV01      Nucl.Phys. A491, 677 (1989)

Y.Avishai, P.Grange

Parity Violation Asymmetry in Nucleon-Nucleon Scattering

NUCLEAR REACTIONS 1n(polarized n, n), E=45, 230 MeV; calculated σ(θ), σ helicity dependence.

doi: 10.1016/0375-9474(89)90524-1
Citations: PlumX Metrics

1987AV02      Nucl.Phys. A468, 578 (1987)

Y.Avishai, M.Fabre de la Ripelle

Electric Dipole Moment of 3He

NUCLEAR STRUCTURE 3He; calculated electric dipole moment; deduced charge conjugation, parity voilation effect contributions.

doi: 10.1016/0375-9474(87)90183-7
Citations: PlumX Metrics

1986MO17      Nucl.Phys. A457, 518 (1986)

S.Morioka, P.Grange, Y.Avishai

Parity Violating Observables in n + p → d + γ with a Realistic Weak Model and the Paris NN Potential

NUCLEAR STRUCTURE 2H; calculated 3P1 wave function component. Desplanques-Donoghue-Holstein weak interaction model, strong nucleon-nucleon interaction.

NUCLEAR REACTIONS 1H(polarized n, γ), E=thermal; calculated γ CP, assymmetry; deduced parity violation effects. Desplanques-Donoghue-Holstein weak interaction model, strong nucleon-nucleon interaction.

doi: 10.1016/0375-9474(86)90465-3
Citations: PlumX Metrics

1984AV01      Phys.Lett. 142B, 1 (1984)

Y.Avishai

Parity Nonconserving Spin Rotation in Weak Neutron-Proton Scattering

NUCLEAR REACTIONS 1H(polarized n, n), E=threshold; calculated total elastic amplitude; deduced neutron spin rotation angle, parity nonconservation effect. Weak nucleon-nucleon force separable form.

doi: 10.1016/0370-2693(84)91123-7
Citations: PlumX Metrics

1984AV03      J.Phys.(Paris), Colloq.C3, 75 (1984)

Y.Avishai

Nucleon Nucleus Weak Scattering within a Single Particle Model

NUCLEAR REACTIONS 40Ca(polarized n, n), E=2-8 MeV; calculated σ(θ), asymmetry vs θ. Single particle model, weak nucleon-nucleon interaction.

1984AV09      J.Phys.(London) G10, L263 (1984)

Y.Avishai, P.Grange

Parity Violation in Threshold Neutron-Proton Scattering

NUCLEAR REACTIONS 1H(polarized n, n), (polarized n, γ), E ≈ threshold; calculated neutron spin rotation angle, σ asymmetry; deduced small parity violation effect.

doi: 10.1088/0305-4616/10/12/001
Citations: PlumX Metrics

1982AV02      Phys.Lett. 112B, 311 (1982)

Y.Avishai

Parity Non-Conserving n-α Elastic Scattering: Estimates of observables

NUCLEAR REACTIONS 4He(polarized n, n), E=5 MeV; calculated σ(total), asymmetry vs θ, spin rotation. 4He(polarized p, p), E=10 MeV; calculated asymmetry vs θ. Nonrelativistic Hamiltonian, parity nonconservation effects.

doi: 10.1016/0370-2693(82)91057-7
Citations: PlumX Metrics

1979GI02      Phys.Rev. C19, 465 (1979)

N.Giraud, Y.Avishai, C.Fayard, G.H.Lamot

Three-Body Calculation of πd Elastic Scattering Observables at Energies up to the (3, 3) Resonance

NUCLEAR REACTIONS 2H(π+, π+), E=25-180 MeV; calculated σ(θ), σ(E), vector, tensor polarizations. Fadeev approach.

doi: 10.1103/PhysRevC.19.465
Citations: PlumX Metrics

1978AV03      Z.Phys. A286, 285 (1978)

Y.Avishai

Fusion Cross Section at Sub-Coulomb Energies

NUCLEAR REACTIONS 12C, 14N, 16O(16O, X), 14N(14N, X), 12C(14N, X), (13C, X), (12C, X), (11B, X), (10B, X), E=sub-Coulomb MeV; calculated fusion parameters.

doi: 10.1007/BF01408258
Citations: PlumX Metrics

1978AV07      J.Phys.(Paris), Lett. 39, L-417 (1978)

Y.Avishai

On the Production of Super-Heavy Elements by Fusion Reactions at Barrier Energies

NUCLEAR REACTIONS 248Cm(48Ca, 2n), E=10 MeV above Coulomb barrier. 294Lv; deduced optimal energies, angular momenta for production of superheavy element.

doi: 10.1051/jphyslet:019780039022041700
Citations: PlumX Metrics

1978GI12      Phys.Lett. 77B, 141 (1978)

N.Giraud, Y.Avishai, C.Fayard, G.H.Lamot

Polarization Observables in π-d Scattering

NUCLEAR REACTIONS 2H(polarized π-, π-), E=142 MeV; calculated σ(θ), A(θ).

doi: 10.1016/0370-2693(78)90607-X
Citations: PlumX Metrics

1977AV03      Z.Phys. A282, 347 (1977)

Y.Avishai

Probabilistic Model for Deep Inelastic Reactions

NUCLEAR REACTIONS 209Bi(84Kr, X), E=525 MeV; calculated σ.

doi: 10.1007/BF01414903
Citations: PlumX Metrics

1976AV04      Z.Phys. A278, 173 (1976)

Y.Avishai

A New Look at Nuclear Glory

NUCLEAR REACTIONS 40Ca(α, α), E=50-150 MeV; calculated σ(θ). Optical potential.

doi: 10.1007/BF01437772
Citations: PlumX Metrics

1972AV02      Phys.Rev. C6, 677 (1972)

Y.Avishai

First 0+ Excited State of 16O in the α-Particle Model of Light Nuclei

NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated binding energies. α-particle model, Narodetskii pole approximation.

doi: 10.1103/PhysRevC.6.677
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1971AV05      Phys.Lett. 36B, 161 (1971)

Y.Avishai, A.S.Rinat

Coulomb Effects and the Question of Charge-Symmetry Breaking in Low-Energy pd Scattering

NUCLEAR REACTIONS 2H(p, X), 2H(n, X), E not given; calculated scattering lengths. Perturbation theory.

NUCLEAR STRUCTURE 3H, 3He; calculated binding energies. Perturbation theory.

doi: 10.1016/0370-2693(71)90058-X
Citations: PlumX Metrics

1971AV07      Phys.Lett. 37B, 487 (1971)

Y.Avishai, A.S.Rinat

Exact Calculations of Nucleon-Deuteron Scattering with Internuclear Forces Including a Tensor Component

NUCLEAR REACTIONS 2H(n, n), E=14.4 MeV; 2H(p, p), E=31 MeV; calculated σ(θ), P(θ).

doi: 10.1016/0370-2693(71)90352-2
Citations: PlumX Metrics

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