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NSR database version of May 24, 2024.

Search: Author = C.Fayard

Found 25 matches.

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2013MI04      Phys.Rev. C 87, 035201 (2013)

T.Mizutani, C.Fayard, B.Saghai, K.Tsushima

Faddeev-chiral unitary approach to the K-d scattering length

doi: 10.1103/PhysRevC.87.035201
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2003BB09      Phys.Rev. C 68, 064001 (2003)

A.Bahaoui, C.Fayard, T.Mizutani, B.Saghai

Low energy (K-bar)N interactions and Faddeev calculation of the K-d scattering length in isospin and particle bases

NUCLEAR REACTIONS 1H(K-, K-), (K-, X), E at 0-250 MeV/c; analyzed data; deduced scattering length, related parameters. 2H(K-, X), E not given; calculated scattering length. Effective nonlinear chiral meson-baryon Lagrangian.

doi: 10.1103/PhysRevC.68.064001
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2002BB01      Phys.Rev. C 66, 057001 (2002)

A.Bahaoui, C.Fayard, T.Mizutani, B.Saghai

Three-body approach to the K-d scattering length in particle basis

NUCLEAR REACTIONS 2H(K-, X), E not given; calculated scattering length. Relativistic three-body approach.

doi: 10.1103/PhysRevC.66.057001
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1998LE26      Nucl.Phys. A639, 247c (1998)

T.-S.H.Lee, V.Stoks, B.Saghai, C.Fayard

Study of Hyperon-Nucleon Interactions with d(e, e'K) Reactions

NUCLEAR REACTIONS 2H(e, e'K+), E not given; calculated hyperon production σ(Q2, θ). Hyperon-nucleon interactions compared.

doi: 10.1016/S0375-9474(98)00280-2
Citations: PlumX Metrics


1998MI16      Phys.Rev. C58, 75 (1998)

T.Mizutani, C.Fayard, G.-H.Lamot, B.Saghai

Off-Shell Effects in the Electromagnetic Production of Strangeness

NUCLEAR REACTIONS 1H(polarized γ, X), E=1-2.5 GeV; calculated strangeness production associated σ(θ), σ, asymmetry; 1H(e, e'X), E not given; calculated strangeness production associated σ(θ); deduced sensitivity to off-shell effects. Effective hadronic Lagrangian approaches.

doi: 10.1103/PhysRevC.58.75
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1996DA13      Phys.Rev. C53, 2613 (1996)

J.C.David, C.Fayard, G.H.Lamot, B.Saghai

Electromagnetic Production of Associated Strangeness

NUCLEAR REACTIONS 1H(γ, X), E=1-2.1 GeV; calculated σ(θ), σ(E) for strangeness production. 1H(polarized γ, X), E=1.45 GeV; calculated Λ-polarization asymmetry. Feynman diagrammatic techniques, isobaric approach.

doi: 10.1103/PhysRevC.53.2613
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1992FA06      Phys.Rev. C46, 118 (1992)

C.Fayard, G.H.Lamot, T.Mizutani, B.Saghai

πNN System with Two-Term Potentials in the P33 and P11 πN Channels

NUCLEAR REACTIONS 2H(π, π), E=142-256 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Two-term π-nucleon interaction potentials.

doi: 10.1103/PhysRevC.46.118
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1990BA12      Nucl.Phys. A508, 335c (1990)

A.Bahaoui, C.Fayard, G.H.Lamot, T.Mizutani

The YN and K(bar)N Interactions and Low-Energy K-d Elastic Scattering

NUCLEAR REACTIONS 2H(K-, K-), E at 15-135 MeV/c; calculated σ(E). Two-body data analysis for parametrization.

doi: 10.1016/0375-9474(90)90494-7
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1989MI22      Phys.Rev. C40, 2763 (1989)

T.Mizutani, C.Fayard, G.H.Lamot, B.Saghai

T20 Problem and Spin Observables in Pion-Deuteron Scattering

NUCLEAR REACTIONS 2H(π, π), E=142, 256, 294 MeV; calculated σ(θ), polarization, spin observables vs θ. Coupled pion-nucleon-exchange equations.

doi: 10.1103/PhysRevC.40.2763
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1987LA01      Phys.Rev. C35, 239 (1987)

G.H.Lamot, J.L.Perrot, C.Fayard, T.Mizutani

Unified Description of πd-πd, πd-NN, and NN-NN Reactions at Intermediate Energies

NUCLEAR REACTIONS 2H(π-, n), (π-, π-), E=142, 180, 256 MeV; 1n(n, n), E=560-1000 MeV; calculated σ(θ). 2H(π+, p), E=142, 180, 256 MeV; calculated σ(θ), vector, tensor polarizations, polarized target; deduced nucleon-nucleon phase shifts, inelasticity parameters. Off-shell modifications, heavy meson exchange.

doi: 10.1103/PhysRevC.35.239
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1985FR04      Nucl.Phys. A435, 738 (1985)

J.Frohlich, B.Saghai, C.Fayard, G.H.Lamot

Effects of a Refined Coulomb Treatment on π± - Deuteron Elastic Scattering Observables

NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E=47-360 MeV; calculated σ(θ), vector analyzing power, tensor polarization vs θ, charge asymmetry parameters; deduced different Coulomb contributions role.

doi: 10.1016/0375-9474(85)90186-1
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1980FA11      Phys.Rev.Lett. 45, 524 (1980)

C.Fayard, G.H.Lamot, T.Mizutani

Effect of Pion Absorption on πd Elastic Scattering from Threshold to the Resonance Region

NUCLEAR REACTIONS 2H(π+, π+), E=threshold-260 MeV; calculated phase shifts; 2H(π+, π+), E=142, 180, 256 MeV; calculated σ(θ). Integral equation, intermediate pion absorption, relativistic treatment.

doi: 10.1103/PhysRevLett.45.524
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1980GI03      Phys.Rev. C21, 1959 (1980)

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

Relativistic Description of πd Elastic Scattering in the (3, 3) Resonance Region

NUCLEAR REACTIONS 2H(π, π), E=140-260 MeV; calculated total σ, σ(θ), vector, tensor polarization. Relativistic nucleon-nucleon tensor force, polarized target.

doi: 10.1103/PhysRevC.21.1959
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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
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1978GI03      Phys.Rev.Lett. 40, 438 (1978)

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

Three-Body Calculation of πd Elastic Scattering at 142 MeV

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

doi: 10.1103/PhysRevLett.40.438
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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
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1977CH07      Phys.Rev. C15, 864 (1977)

B.Charnomordic, C.Fayard, G.H.Lamot

Three-Body Calculation of 6Li and d-α Elastic Scattering

NUCLEAR STRUCTURE 6Li; calculated levels.

NUCLEAR REACTIONS 4He(d, d), E=0-25 MeV; calculated σ(E, θ).

doi: 10.1103/PhysRevC.15.864
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1975ZA03      Lett.Nuovo Cim. 12, 221 (1975)

H.Zankel, C.Fayard, G.H.Lamot

Coulomb Energy of 3He

NUCLEAR STRUCTURE 3H, 3He; calculated Coulomb energies.

doi: 10.1007/BF02784801
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1974LA16      Lett.Nuovo Cim. 9, 653 (1974)

G.H.Lamot, C.Fayard, E.Elbaz

Theoretical Phase Shift Analysis in the (n, d) Elastic Scattering

NUCLEAR REACTIONS 1H(d, d), E=10.85; calculated pd(θ). 1H(d, pn), E=10.85; calculated pn(θ). 2H(n, n); analyzed phase shift.

doi: 10.1007/BF02763217
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1973EL04      Phys.Rev. C7, 1445 (1973)

E.Elbaz, C.Fayard, G-H.Lamot, J.Meyer, R.S.Nahabetian, J.Pigeon, P.Boschan

Survey of Some Nuclear Properties Given by a Nonlocal Separable Nucleon-Nucleon Interaction

NUCLEAR STRUCTURE 3H, 4He, 12C, 16O, 28Si, 32S, 40Ca calculated binding energy; 20Ne, 24Mg, 28Si, 32S, 36Ar calculated Hartree-Fock energies, energy gap, mean J2. 20Ne, 24Mg, 28Si calculated measured B(E2).

doi: 10.1103/PhysRevC.7.1445
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1972LA31      Lett.Nuovo Cim. 5, 647 (1972)

G.H.Lamot, E.El Baz, C.Fayard, J.Pigeon

Two-Term Nonlocal Separable Potentials in the Three-Nucleon Problem

NUCLEAR STRUCTURE 2,3H; calculated binding energies, n-d scattering σ.

doi: 10.1007/BF02812301
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1971BA42      Nuovo Cim. 1A, 285 (1971)

J.Barguil, J.Pigeon, C.Fayard, G.-H.Lamot, E.El Baz

Nucleon Elastic Scattering by 4He with Nonlocal Separable Potentials

NUCLEAR REACTIONS 4He(n, n), (p, p), E < 23 MeV; calculated phase shifts. One-term nonlocal separable potential.

doi: 10.1007/BF02722670
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1971PI04      Phys.Rev. C4, 704 (1971)

J.Pigeon, J.Barguil, C.Fayard, G-H.Lamot, E.El Baz

Description of Elastic Scattering Processes with the Use of Nonlocal Separable Potentials

NUCLEAR REACTIONS 4He(p, p), 4He(α, α), E < 100 MeV; calculated σ(E;θ). Nonlocal separable potential.

doi: 10.1103/PhysRevC.4.704
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1968LE11      Nucl.Phys. A116, 196(1968)

B.Leroux, K.El-Hammami, J.Dalmas, R.Chastel, G.Lamot, C.Fayard, J.Hajj Boutros

Etude des Reactions (n, α) sur les Noyaux 16O et 14N a 14.9 MeV

NUCLEAR REACTIONS 16O, 14N(n, α); E=14.9 MeV measured σ(Eα, θ). Natural targets.

doi: 10.1016/0375-9474(68)90491-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21461.


1967VI03      J.Phys.(Paris) 28, 617 (1967)

J.-L.Vidal, R.Bouche, C.Fayard, L.Feuvrais, M.Gaillard, P.Gaillard, M.Gouanere, M.Gusakow, G.H.Lamot, J.R.Pizzi

Reaction 14N(d, α)12C a 28, 5 MeV

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphys:01967002808-9061700
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