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NSR database version of April 29, 2024.

Search: Author = E.J.Moniz

Found 19 matches.

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1995BR37      Ann.Phys.(New York) 243, 420 (1995)

A.M.S.Breitschaft, V.C.Barbosa, L.F.Canto, M.S.Hussein, E.J.Moniz, J.Christley, I.J.Thompson

Coupled-Channel Effects on Heavy-Ion Sub-Barrier Fusion within the Doorway Expansion Method

NUCLEAR REACTIONS, ICPND ²⁸Si(¹⁶O, X), E ≈ 20-36 MeV; calculated fusion σ(E); deduced coupled-channels role. Doorway expansion method.

doi: 10.1006/aphy.1995.1103
Citations: PlumX Metrics

1995FR13      Phys.Rev. C51, 3435 (1995)

L.L.Frankfurt, E.J.Moniz, M.M.Sargsyan, M.I.Strikman

Correlation Effects in Nuclear Transparency

NUCLEAR STRUCTURE ¹²C; calculated color transparency vs Q²; deduced correlations role. Glauber model.

doi: 10.1103/PhysRevC.51.3435
Citations: PlumX Metrics

1995JA17      Z.Phys. A353, 175 (1995)

R.J.Janner, E.J.Moniz

A Simple Model of Resonance-Dominated Quasi-Elastic Scattering

doi: 10.1007/BF01295895
Citations: PlumX Metrics

1994BR39      Ann.Phys.(New York) 234, 162 (1994)

A.M.S.Breitschaft, L.F.Canto, H.Schechter, M.S.Hussein, E.J.Moniz

Doorway State Expansion Approach to Coupled Channels Problems and Application to Heavy Ions

NUCLEAR REACTIONS ²⁸Si(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), E(cm)=55 MeV; calculated S-matrix. Doorway expansion method, extension to coupled-channels, comparison with DWBA.

doi: 10.1006/aphy.1994.1077
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1992MO21      Nucl.Phys. A546, 287c (1992)

E.J.Moniz

Electronuclear Physics with Spin

NUCLEAR STRUCTURE ²H; compiled, reviewed tensor polarization, charge monopole form factor data, model interpretation.

doi: 10.1016/0375-9474(92)90516-M
Citations: PlumX Metrics

1992WA39      Int.J.Mod.Phys. E1, 833 (1992)

Y.-C.Wang, F.E.Serr, E.J.Moniz, N.Teruya, H.Dias, M.S.Hussein

Calculation of Giant Resonance Widths from Damped Single Particle Motion

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ²⁰⁸Pb; calculated isoscalar quadrupole response, transition strength, giant resonance spreading, escape widths.

doi: 10.1142/S0218301392000369
Citations: PlumX Metrics

1987HE03      Phys.Rev. C35, 718 (1987)

L.Heller, S.Kumano, J.C.Martinez, E.J.Moniz

Pion-Nucleon Bremsstrahlung and Δ Electromagnetic Moments

NUCLEAR REACTIONS ¹H(π⁺, π⁺'γ), (π^-, π^-'γ), E=298 MeV; analyzed bremsstrahlung σ(Eγ, θπ, θγ), polarization asymmetries; deduced isobar dipole, quadrupole moments role, energy dependence. Gauge invariant model.

doi: 10.1103/PhysRevC.35.718
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1986KA05      Phys.Rev. C33, 974 (1986)

B.Karaoglu, E.J.Moniz

Pion Optical Potential with Δ Dynamics

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺), E=50-240 MeV; calculated σ(θ), σ(E). ²⁰⁸Pb(π⁺, π⁺), (π^-, π^-), E=80, 162 MeV; calculated σ(θ). ¹⁶O(γ, π⁰), E not given; calculated coherent pion production σ(θ); deduced pion-nucleus potential, Δ-nucleus interaction.

doi: 10.1103/PhysRevC.33.974
Citations: PlumX Metrics

1984KA36      Phys.Lett. 148B, 253 (1984)

T.Karapiperis, E.J.Moniz

Medium Corrections to Inelastic π⁺/π^- Cross Section Ratios

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺'), (π^-, π^-'), E=164 MeV; analyzed isospin mixing coefficients from σ(π⁺)/σ(π^-); deduced pion amplitude isobar dominance.

doi: 10.1016/0370-2693(84)90082-0
Citations: PlumX Metrics

1984KO33      Ann.Phys.(New York) 154, 99 (1984)

J.H.Koch, E.J.Moniz, N.Ohtsuka

Nuclear Photoabsorption and Compton Scattering at Intermediate Energy

NUCLEAR REACTIONS ¹²C(γ, X), E=200-400 MeV; calculated photoabsorption σ(E). ¹²C(γ, γ), E(cm)=325 MeV; ⁴He(γ, γ), E(cm)=200, 325 MeV; calculated elastic Compton scattering σ(θ). Isobar-hole approach.

doi: 10.1016/0003-4916(84)90141-6
Citations: PlumX Metrics

1983KO02      Phys.Rev. C27, 751 (1983)

J.H.Koch, E.J.Moniz

Coherent π⁰ Photoproduction at Intermediate Energy

NUCLEAR REACTIONS ⁴He, ¹²C(γ, π⁰), E=200-400 MeV; calculated production σ(E), σ(θ). Isobar-hole formalism.

doi: 10.1103/PhysRevC.27.751
Citations: PlumX Metrics

1979DU06      Phys.Rev. C20, 725 (1979)

J.F.Dubach, E.J.Moniz, G.D.Nixon

Dynamical Polarization in Pionic Atoms

ATOMIC PHYSICS, Mesic-Atoms ⁴⁸Ti, ¹⁰⁴Ru, ¹¹⁰Pd, ¹¹²Cd, ¹⁵⁰Sm; pionic atoms; measured X-rays.

NUCLEAR REACTIONS ⁴⁸Ti, ¹⁰⁴Ru, ¹¹⁰Pd, ¹¹²Cd, ¹⁵⁰Sm(π^-, X), E ≈ 0; measured dynamic nuclear polarization; deduced interference between nuclear, atomic transition.

doi: 10.1103/PhysRevC.20.725
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1979HI04      Ann.Phys.(New York) 120, 205 (1979)

M.Hirata, J.H.Koch, F.Lenz, E.J.Moniz

Isobar-Hole Doorway States and π-¹⁶O Scattering

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺), (π^-, π^-), E=50-340 MeV; calculated σ(θ). Isobar-hole doorway state model.

doi: 10.1016/0003-4916(79)90287-2
Citations: PlumX Metrics

1979KO17      Phys.Rev. C20, 235 (1979)

J.H.Koch, E.J.Moniz

Coherent π⁰ Photoproduction in the Isobar-Hole Formalism

NUCLEAR REACTIONS ¹⁶O(γ, π⁰), E not given; calculated coherent production σ. Isobar-hole formalism for pion-nucleus interactions.

doi: 10.1103/PhysRevC.20.235
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1977HI10      Phys.Lett. 70B, 281 (1977)

M.Hirata, J.H.Koch, F.Lenz, E.J.Moniz

Extended Schematic Model for Pion-Nucleus Scattering

NUCLEAR REACTIONS ¹⁶O(π^-, π^-); calculated scattering parameters.

doi: 10.1016/0370-2693(77)90658-X
Citations: PlumX Metrics

1976WO01      Phys.Rev. C13, 286 (1976)

R.M.Woloshyn, E.J.Moniz, R.Aaron

Relativistic Three-Body Calculation of πd Scattering

NUCLEAR REACTIONS ²H(π, π), E=80-240 MeV; calculated σ(θ). Relativistic 3-body calculation.

doi: 10.1103/PhysRevC.13.286
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1974CH28      Phys.Rev. C10, 344 (1974)

M.Chemtob, E.J.Moniz, M.Rho

Deuteron Electromagnetic Structure at Large Momentum Transfer

NUCLEAR STRUCTURE ²H; calculated form factors.

doi: 10.1103/PhysRevC.10.344
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1971MO06      Phys.Rev.Lett. 26, 445 (1971)

E.J.Moniz, I.Sick, R.R.Whitney, J.R.Ficenec, R.D.Kephart, W.P.Trower

Nuclear Fermi Momenta from Quasielastic Electron Scattering

NUCLEAR REACTIONS ⁶Li, ¹²C, ²⁴Mg, ⁴⁰Ca, ⁵⁸Ni, ⁸⁹Y, ¹¹⁸Sn, ¹⁸¹Ta, ²⁰⁸Pb(e, e'X), E=500 MeV; measured σ(Ee'). ⁶Li, ¹²C, ²⁴Mg, ⁴⁰Ca, ⁵⁸Ni, ⁸⁹Y, ¹¹⁸Sn, ¹⁸¹Ta, ²⁰⁸Pb deduced nuclear Fermi momentum.

doi: 10.1103/PhysRevLett.26.445
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1971MO36      Ann.Phys.(New York) 67, 58 (1971)

E.J.Moniz, G.D.Nixon

High Energy Coherent Processes with Nuclear Targets

doi: 10.1016/0003-4916(71)90004-2
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