Nuclear Science References (NSR)

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2000BL13 Phys.Rev. C62, 025206 (2000)

J.C.R.Bloch, M.A.Ivanov, T.Mizutani, C.D.Roberts, S.M.Schmidt

K → ππ and a Light Scalar Meson

doi: 10.1103/PhysRevC.62.025206
Citations: PlumX Metrics

1998IV03 Few-Body Systems 24, 201 (1998)

M.A.Ivanov, T.Mizutani, Yu.M.Valit

Heavy-to-Light Form Factors in the Quark Model with Infrared Heavy-Quark Propagators

doi: 10.1007/s006010050086
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
Citations: PlumX Metrics

1996IV04 Few-Body Systems 20, 49 (1996)

M.A.Ivanov, T.Mizutani

Heavy-Quark Limit in a Relativistic Quark-Confinement Model

doi: 10.1007/s006010050031
Citations: PlumX Metrics

1994NO13 Prog.Theor.Phys.(Kyoto) 91, 893 (1994)

H.Noda, T.Tashiro, T.Mizutani

Study of the Neutron and Deuteron Polarized Structure Functions in a Constituent Quark Model

NUCLEAR STRUCTURE ²H, ¹n; analyzed polarized structure function. Constituent quark model.

doi: 10.1143/ptp/91.5.893
Citations: PlumX Metrics

1994NO14 Prog.Theor.Phys.(Kyoto) 92, 909 (1994)

H.Noda, T.Tashiro, T.Mizutani

Strange Sea Polarization in the Proton and a Constituent Quark Model

NUCLEAR STRUCTURE ¹H; calculated valence quark, q(q-bar)-sea polarizations. Polarized proton, constituent quark model.

doi: 10.1143/ptp/92.4.909
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1990SA15 Phys.Rev. C41, 2286 (1990)

F.Sammarruca, T.Mizutani

Single Pion Production in Nucleon-Nucleon Collisions

NUCLEAR REACTIONS ¹H(p, pπ⁺), E=800 MeV; calculated σ(θp, θ(π)) vs proton momentum.

doi: 10.1103/PhysRevC.41.2286
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1986MI07 Czech.J.Phys. B36, 314 (1986)

T.Mizutani

A Quark-Based NN Annihilation Potential and the Low Energy NN Scattering

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E=490-860 MeV/c; calculated σ(θ). ¹H(p-bar, n-bar), E=490, 690 MeV/c; calculated σ(θ). Quark based nucleon-antinucleon annihilation potential.

doi: 10.1007/BF01597167
Citations: PlumX Metrics

1986TE04 Phys.Lett. 182B, 6 (1986)

R.Tegen, F.Myhrer, T.Mizutani

Low Energy p-p(bar) Scattering and the Quark Confinement Radius

NUCLEAR REACTIONS H(p-bar, p-bar), (p-bar, n-bar), E=490 MeV/c; calculated σ(θ). New annihilation potential.

doi: 10.1016/0370-2693(86)91068-3
Citations: PlumX Metrics

1982MI02 Czech.J.Phys. B32, 147 (1982)

T.Mizutani

A Study in the Coupled πNN-NN System and the Question of Dinucleon Resonances

NUCLEAR REACTIONS ²H(π⁺, π⁺), E=82-292; calculated σ(θ). ²H(π, π), E=256 MeV; calculated analyzing power vs θ. Polarized target. ¹H(polarized p, d), E=570 MeV; calculated vector analyzing power. Unitary relativistic equations.

doi: 10.1007/BF01608041
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1977MI14 Ann.Phys.(New York) 109, 1 (1977)

T.Mizutani, D.S.Koltun

Coupled Channel Theory of Pion-Deuteron Reaction Applied to Threshold Scattering

NUCLEAR REACTIONS ²H(π^-, π^-); calculated scattering parameters.

doi: 10.1016/0003-4916(77)90164-6
Citations: PlumX Metrics

Back to query form