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NSR database version of April 27, 2024.

Search: Author = P.Grange

Found 15 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

1986BH01      Phys.Rev. C33, 954 (1986)

K.H.Bhatt, P.Grange, B.Hiller

Nuclear Friction and Lifetime of Induced Fission

NUCLEAR STRUCTURE A=248; calculated fission rate, transition time, T1/2 vs scission point position.

doi: 10.1103/PhysRevC.33.954
Citations: PlumX Metrics

1986GA12      Phys.Lett. 176B, 312 (1986)

A.Gavron, A.Gayer, J.Boissevain, H.C.Britt, J.R.Nix, A.J.Sierk, P.Grange, S.Hassani, H.A.Weidenmuller, J.R.Beene, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, G.A.Petitt, C.Butler

Neutron Emission Prior to Fission

NUCLEAR REACTIONS 142Nd(16O, F), E=207 MeV; measured fission(fragment)n-coin, σ(En, θn); deduced post, prior fission neutron multiplicity relationship. 158Er deduced fission barrier, other parameters, reduced nuclear dissipation coefficient limit.

doi: 10.1016/0370-2693(86)90170-X
Citations: PlumX Metrics

1986GR09      Phys.Rev. C34, 209 (1986)

P.Grange, S.Hassani, H.A.Weidenmuller, A.Gavron, J.R.Nix, A.J.Sierk

Effect of Nuclear Dissipation on Neutron Emission Prior to Fission

NUCLEAR REACTIONS 142Nd(16O, F), E=207 MeV; calculated neutron emission multiplicity prior to fission. 158Er deduced saddle to scission time vs reduced dissipation coefficient, Γf vs t. Bohr-Wheeler statistical model.

doi: 10.1103/PhysRevC.34.209
Citations: PlumX Metrics

1986HA35      Z.Phys. A325, 95 (1986)

S.Hassani, P.Grange

Nuclear Dissipation, Fission Probability and Neutron Multiplicity prior to Fission

NUCLEAR REACTIONS 142Nd(16O, F), (16O, n), E=207 MeV; calculated fission probabilities, average neutron multiplicity vs reduced dissipation coefficient. 158Er deduced transients role on pre-fission decay neutron multiplicity. Statistical model, inclusion of transients, inclusion of both transients and mean saddle.

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

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

1984GR31      Nucl.Phys. A428, 37c (1984)

P.Grange

Effects of Transients on Particle Emission prior to Fission in a Transport Description of the Fission Process

NUCLEAR STRUCTURE 168Yb; calculated fission rate vs time, temperature, neutron multiplicity vs excitation energy. 248Cf; calculated neutron multiplicity following fission vs excitation energy. Transport process model.

doi: 10.1016/0375-9474(84)90241-0
Citations: PlumX Metrics

1984HA17      Phys.Lett. 137B, 281 (1984)

S.Hassani, P.Grange

Neutron Multiplicities in Fission Viewed as a Diffusion Process

NUCLEAR STRUCTURE 248Cf; calculated fission rate, neutron multiplicity vs excitation. 168Yb; calculated fission neutron multiplicity; deduced nuclear friction parameter dependence. Diffusion model.

doi: 10.1016/0370-2693(84)91716-7
Citations: PlumX Metrics

1980GR13      Phys.Lett. B96, 26 (1980)

P.Grange, H.A.Weidenmuller

Fission Probability and the Nuclear Friction Constant

RADIOACTIVITY, Fission 226Ra, 236Np, 232Pa; calculated ΓF/Γn vs excitation energy; deduced induced fission probability vs friction coefficient. Diffusion model.

doi: 10.1016/0370-2693(80)90204-X
Citations: PlumX Metrics

1978BE03      Z.Phys. A284, 61 (1978)

M.Berlanger, C.Ngo, P.Grange, J.Richert, H.Hofmann

Statistical Fluctuations and the Double Differential Cross Section for Energy and Angle in Deep Inelastic Reactions

NUCLEAR REACTIONS 232Th(40Ar, 40Ar), E=388 MeV; calculated σ(θ).

doi: 10.1007/BF01433876
Citations: PlumX Metrics

1978BE18      Phys.Rev. C17, 1495 (1978)

M.Berlanger, P.Grange, H.Hofmann, C.Ngo, J.Richert

Influence of Coulomb and Nuclear Forces on the Pattern of the Double Differential Cross Section d2σ/dθdE for Deep Inelastic Reactions

NUCLEAR REACTIONS 120Sn(84Kr, X), E=514 MeV; 208Pb(208Pb, X), E=1560 MeV; 208Pb(136Xe, X), E=1000 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.17.1495
Citations: PlumX Metrics

1978BE23      Z.Phys. A286, 207 (1978)

M.Berlanger, P.Grange, H.Hofmann, C.Ngo, J.Richert

Triple Differential Cross Section for Angle, Atomic Number and Energy (Or Angular Momentum Transfer) Calculated for the 280 MeV 40Ar + 58Ni (Or 365 MeV 63Cu + 197Au) System in a Simple Model

NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; 197Au(63Cu, X), E=365 MeV; calculated σ(E, Z, θ).

doi: 10.1007/BF01408977
Citations: PlumX Metrics

1974GR03      Nucl.Phys. A219, 266 (1974)

P.Grange, M.A.Preston

A Treatment of Renormalization, Potential Energy of Intermediate States and Re-Arrangement Effects in Brueckner Calculations of Closed Shell Nuclei

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energy.

doi: 10.1016/0375-9474(74)90066-9
Citations: PlumX Metrics

1972GR48      Phys.Lett. 42B, 35 (1972)

P.Grange, M.A.Preston

Higher Partial Wave Contribution to Nuclear Matter Binding Energy: Phase Shift Approximation Versus One Pion-Plus sigma-Exchange Potential

doi: 10.1016/0370-2693(72)90708-3
Citations: PlumX Metrics

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