NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = A.S.Rinat Found 51 matches. 2010RI04 Phys.Rev. C 82, 015207 (2010) Neutron observables from inclusive lepton scattering on nuclei
doi: 10.1103/PhysRevC.82.015207
2007RI02 Nucl.Phys. A784, 25 (2007) A.S.Rinat, M.F.Taragin, M.Viviani Inclusive scattering data on light nuclei as a tool for the extraction of GnM NUCLEAR REACTIONS 2H, 4He(e, e'X), E=0.9-21 GeV; analyzed σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1016/j.nuclphysa.2006.10.086
2007RI05 Eur.Phys.J. A 31, 415 (2007) A.S.Rinat, M.F.Taragin, M.Viviani Extraction of GnM from inclusive electron scattering on D, 4He NUCLEAR REACTIONS 2H, 4He(e, e'X), E=high; analyzed σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1140/epja/i2006-10293-3
2006RI06 Phys.Rev. C 73, 045201 (2006) Relation between nuclear and nucleon structure functions and their moments NUCLEAR STRUCTURE 2H, C, Fe; analyzed structure functions, moments.
doi: 10.1103/PhysRevC.73.045201
2005RI09 Phys.Rev. C 72, 015211 (2005) A.S.Rinat, M.F.Taragin, M.Viviani Simple qualitative description of EMC ratios μA for 0.2 ≤ x ≤ 1.5 and some sample calculations NUCLEAR STRUCTURE 4He, C, Fe, Au; calculated structure function ratios. Comparison with data.
doi: 10.1103/PhysRevC.72.015211
2005RI21 Phys.Rev. C 72, 065209 (2005) Distribution functions for partons in nuclei NUCLEAR STRUCTURE 4He, C, Fe, Au; calculated parton distribution functions and structure functions.
doi: 10.1103/PhysRevC.72.065209
2004RI13 Phys.Rev. C 70, 014003 (2004) A.S.Rinat, M.F.Taragin, M.Viviani Neutron magnetic form factor GnM(Q2) from quasielastic inclusive scattering data on D and 4He NUCLEAR REACTIONS 2H(e, e'X), E=4 GeV; 4He(e, e'X), E=2-3.6 GeV; analyzed quasielastic σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1103/PhysRevC.70.014003
2003RI01 Phys.Lett. 551B, 284 (2003) Extraction of the neutron structure function Fn2 from inclusive scattering data on composite nuclei NUCLEAR REACTIONS 2H, C, Fe(e, e'X), E=high; analyzed data; deduced parameters, method for extracting neutron structure function.
doi: 10.1016/S0370-2693(02)03052-6
2003VI01 Phys.Rev. C 67, 034003 (2003) M.Viviani, A.Kievsky, A.S.Rinat Gersch-Rodriquez-Smith computation of deep inelastic electron scattering on 4He NUCLEAR REACTIONS 4He(e, e'X), E=3.6 GeV; calculated σ(E, θ). Comparison with data.
doi: 10.1103/PhysRevC.67.034003
2002GU04 Phys.Rev. C65, 024310 (2002) Relativistic Approaches to Structure Functions of Nuclei NUCLEAR REACTIONS 4He(e, e'X), E=3.595 GeV; calculated σ(E, θ). Relativistic structure function, Gersch-Rodriguez-Smith theory.
doi: 10.1103/PhysRevC.65.024310
2002RI04 Phys.Rev. C65, 042201 (2002) Description of Inclusive Scattering of 4.045 GeV Electrons from 2H NUCLEAR REACTIONS 2H(e, e'), E=4.045 GeV; calculated σ(E, θ). Comparison with data.
doi: 10.1103/PhysRevC.65.042201
2000RI16 Phys.Rev. C62, 034602 (2000) R Ratios and Moments of Nuclear Structure Functions
doi: 10.1103/PhysRevC.62.034602
1999RI08 Phys.Rev. C59, 3371 (1999) Equivalence of the Impulse Approximation and the Gersch-Rodriguez-Smith Series for Structure Functions
doi: 10.1103/PhysRevC.59.3371
1999RI13 Phys.Lett. 459B, 431 (1999) Extraction of Nucleon Momentum Distributions from Inclusive Electron Scattering on Nuclei NUCLEAR STRUCTURE He, Fe; analyzed electron scattering data; deduced nucleon momentum distributions.
doi: 10.1016/S0370-2693(99)00669-3
1999RI16 Phys.Rev. C60, 044601 (1999) Theoretical Aspects of Inclusive Scattering of 4.05 GeV Electrons from Nuclei NUCLEAR REACTIONS Fe(e, e'X), E=4.05 GeV; analyzed σ(E, θ); deduced structure function, reaction mechanism features.
doi: 10.1103/PhysRevC.60.044601
1997RI09 Nucl.Phys. A620, 417 (1997); Erratum Nucl.Phys. A624, 773 (1997) Predictions for the 4 GeV TJNAF Inclusive Electron Scattering Experiment and for FSI Effects in EMC Ratios NUCLEAR REACTIONS Fe, 197Au(e, e'X), E=4 GeV; calculated total inclusive σ. Nuclear structure functions as generalized convolutions of the nucleon structure function. NUCLEAR STRUCTURE Fe, C; calculated structure function. Nuclear structure functions as generalized convolutions of the nucleon structure function.
doi: 10.1016/S0375-9474(97)00167-X
1997RI13 Nucl.Phys. A623, 519 (1997) Some Remarks on Off-Shell Scattering in the Eikonal Approximation and Applications to Semi-Inclusive Reactions NUCLEAR REACTIONS C, O, 27Al, Ca, Fe, 197Au(e, e'X), E=high; calculated semi-inclusive reaction nuclear transparencies; deduced NN correlations role.
doi: 10.1016/S0375-9474(97)00387-4
1996RI03 Nucl.Phys. A597, 636 (1996) Effect of NN Correlations on Predictions of Nuclear Transparencies for Protons, Knocked Out in High Q2 (e, e'p) Reactions NUCLEAR REACTIONS C(e, e'p), E=high; calculated knocked-out proton transparency vs Q2; deduced NN-correlations role.
doi: 10.1016/0375-9474(95)00454-8
1996RI06 Nucl.Phys. A598, 349 (1996) Description of Inclusive Scattering of Few-GeV Electrons from Finite A Nuclei and Nuclear Matter NUCLEAR REACTIONS Fe, 27Al, 197Au(e, e'X), E=3.6 GeV; calculated inclusive reaction σ. Total structure function treated as a convolution of W(N) components.
doi: 10.1016/0375-9474(95)00510-2
1995RI06 Phys.Rev. C52, R28 (1995) Nuclear Transparencies for Nucleons, Knocked-Out under Various Semi-Inclusive Conditions
doi: 10.1103/PhysRevC.52.R28
1994PA07 Nucl.Phys. A572, 1 (1994) Exact Response of the Non-Relativistic Harmonic Oscillator
doi: 10.1016/0375-9474(94)90416-2
1994PA13 Phys.Lett. 325B, 289 (1994) On the Nature of the Large-q Expansion of the Response for a Non-Relativistic Confined System
doi: 10.1016/0370-2693(94)90012-4
1994RI02 Nucl.Phys. A568, 873 (1994) Generalized Transparency in Semi-Inclusive Processes NUCLEAR REACTIONS 58Ni(e, e'p), E not given; calculated transparency vs outgoing momentum.
doi: 10.1016/0375-9474(94)90364-6
1994RI05 Nucl.Phys. A571, 733 (1994) Inclusive Scattering of Electrons from Nuclear Matter in the GeV Range
doi: 10.1016/0375-9474(94)90718-8
1988JE02 Nucl.Phys. A485, 421 (1988) On the Description of the Tensor Analysing Power T20 in Elastic πd Scattering NUCLEAR REACTIONS 2H(π, π), E=140, 256 MeV; calculated σ(θ), tensor analyzing power vs θ; deduced second order diagram roles.
doi: 10.1016/0375-9474(88)90545-3
1987GU21 Phys.Lett. 197B, 6 (1987) On the Final-State Interaction in Inclusive A(e, e')X Reactions NUCLEAR REACTIONS 3,4He, 12C, 58Ni(e, e'X), E not given; calculated scaling function; deduced final state interaction role.
doi: 10.1016/0370-2693(87)90330-3
1985RI02 J.Phys.(London) G11, 309 (1985) Are Quark Signals Expected in Medium-Energy πd Observables ( Question ) NUCLEAR REACTIONS 2H(π, π), E=140, 180, 256, 294 MeV; calculated vector, tensor polarization vs θ; deduced quark signal characteristics role. Cloudy bag model.
doi: 10.1088/0305-4616/11/3/009
1985RI14 J.Phys.(Paris), Colloq.C-2, 475 (1985) Cloudy Bag Description of πd → πd, pp NUCLEAR REACTIONS 2H(π, π), E=140 MeV; analyzed vector polarization. Cloudy bag model.
1983RI03 Nucl.Phys. A397, 381 (1983) A Comparative Study of the NNπ System (I). The πd → πd, πd → NN channels NUCLEAR REACTIONS 2H(π, π), E=50-290 MeV; calculated σ(elastic), σ(θ), σ vs E, vector polarization. 1H(p, π+), (polarized p, π+), E=382-878 MeV; calculated σ(θ), asymmetry vs θ, E; 2H(π, p), E=200-300 MeV; calculated vector polarization it11(θ), polarized target; deduced deuteron from factor, nucleon-nucleon-pion vertex dependences.
doi: 10.1016/0375-9474(83)90609-7
1983RI08 Phys.Lett. 126B, 151 (1983) Do πd Vector Polarization Data Show Quark Substructure of Baryons ( Question ) NUCLEAR REACTIONS 2H(π, π), E=142, 256, 294 MeV; analyzed vector polarization data, σ(θ), σ; deduced possible baryon quark substructure. Cloudy bag model.
doi: 10.1016/0370-2693(83)90580-4
1981RI05 Nucl.Phys. A364, 486 (1981) A.S.Rinat, Y.Starkand, E.Hammel Calculation of πd → NN, NN → πd Observables NUCLEAR REACTIONS 2H(π, π), E=47.5-262 MeV; 1H(p, π), E=381-810 MeV; calculated σ(θ), analyzing power vs θ. Field theoretical model, two-body channel coupling, integral equations.
doi: 10.1016/0375-9474(81)90584-4
1980AR15 Nucl.Phys. A350, 205 (1980) A Phase-Shift Analysis of Elastic Pion-Deuteron Scattering NUCLEAR REACTIONS 2H(π+, π+), E=82-292 MeV; calculated σ(θ), σ(E, total), tensor analyzing power vs E, θ, phase shifts. S-matrix formalism.
doi: 10.1016/0375-9474(80)90456-X
1980GU04 Ann.Phys.(New York) 124, 313 (1980) S.A.Gurvitz, L.P.Kok, A.S.Rinat Non-Eikonal Effects in High-Energy Scattering IV. Inelastic Scattering NUCLEAR REACTIONS 12C(p, p'), E=1.04 GeV; calculated σ(θ). Non-eikonal corrections, Glauber theory.
doi: 10.1016/0003-4916(80)90212-2
1979HA36 Phys.Lett. 85B, 193 (1979) Relativistic Corrections on Three Nucleon Observables NUCLEAR STRUCTURE 3He; compared ground state properties obtained from covariant, standard, nonrelativistic Faddeev theory; deduced changes in position of minimum, maximum of charge factor.
doi: 10.1016/0370-2693(79)90576-8
1979RI02 Phys.Lett. 80B, 166 (1979) A.S.Rinat, Y.Starkand, E.Hammel, A.W.Thomas The Effect of Genuine Pion Absorption and Emission on πd Scattering NUCLEAR REACTIONS 2H(π, π), E=142-256 MeV; calculated σ(θ), iT11, T20, T21, T22. Intermediate pion absorption, reemission through π, ρ rescattering.
doi: 10.1016/0370-2693(79)90189-8
1979RI15 Nucl.Phys. A329, 285 (1979) A.S.Rinat, E.Hammel, Y.Starkand, A.W.Thomas A Relativistic Description of πd Scattering (II). Effects of Small πN Waves, NN Rescattering, R-Exchange and π Absorption and Emission NUCLEAR REACTIONS 2H(π-, π-), E=142, 180, 256 MeV; calculated σ(θ), P(θ), total σ. Relativistic description, rho-exchange, nucleon-nucleon scattering, pion absorption, emission effects.
doi: 10.1016/0375-9474(79)90377-4
1978HO21 Phys.Rev. C18, 2683 (1978) Analysis of Recent π d Elastic Scattering Data NUCLEAR REACTIONS 2H(π, π), 234 MeV < E < 513 MeV; calculated σ(θ), σ(E). Modified Glauber amplitude.
doi: 10.1103/PhysRevC.18.2683
1977AL01 Nucl.Phys. A278, 525 (1977) Analysis of Elastic and Inelastic α-12C Data (Eα = 1.37 GeV) with a Multiple Diffraction Model NUCLEAR REACTIONS 12C(α, α'), E=1.37 GeV; calculated σ(θ). DWIA calculations.
doi: 10.1016/0375-9474(77)90096-3
1977JU01 Nucl.Phys. A280, 467 (1977) A Four-Channel Unitary Model for the Description of Heavy-Ion Collisions at Relativistic Energies NUCLEAR REACTIONS 9Be(16O, X), E=2.1 GeV/c; calculated abrasion σ.
doi: 10.1016/0375-9474(77)90615-7
1977RI06 Nucl.Phys. A282, 365 (1977) A Relativistic Description of πd Scattering in the (3, 3) Resonance Region NUCLEAR REACTIONS 2H(π, π), E=142, 182, 256 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90063-X
1977RI12 Nucl.Phys. A287, 399 (1977) Exact Solution of a Model for πd Induced Reactions and its Application to Pion-Nucleus Reactions NUCLEAR REACTIONS 2H(π, π); calculated reaction parameters.
doi: 10.1016/0375-9474(77)90054-9
1976JU01 Nucl.Phys. A268, 477 (1976) Unitarity Effects in High-Energy Nuclear Abrasion NUCLEAR REACTIONS 12C, 60Ni, 208Pb(p, X); calculated σ.
doi: 10.1016/0375-9474(76)90544-3
1975GU17 Phys.Lett. 59B, 22 (1975) S.A.Gurvits, Y.Alexander, A.S.Rinat Analysis of 1 GeV Proton Scattering on D and 4He in a Non-Eikonal Approach NUCLEAR REACTIONS 2H, 4He(p, p), E=1 GeV; calculated σ(θ).
doi: 10.1016/0370-2693(75)90145-8
1974GU09 Phys.Lett. 51B, 109 (1974) Pion Scattering on Medium-Weight Nuclei and Distortion Effects in Double Charge Exchange Reactions NUCLEAR REACTIONS 40Ca(π-, π-), E=205, 215 MeV; 51V(π+, π-), E=200 MeV; calculated σ(θ), σ(E(π-), θ).
doi: 10.1016/0370-2693(74)90190-7
1974HO29 Phys.Rev. C10, 2102 (1974) Pseudo-Resonance Behavior of Partial Waves in Elastic Pion Scattering NUCLEAR REACTIONS 2H(π, π), E=142, 180, 256, 320, 450, 600 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.10.2102
1974ST14 Phys.Rev. C10, 1253 (1974) Partial-Wave Dispersion Relations for the Nonrelativistic Five-Nucleon System NUCLEAR REACTIONS 4He(n, n), E=0-40 MeV; calculated phase shifts. 3He(d, n), (d, d), E=6, 14.2 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.10.1253
1973AL14 Phys.Lett. 45B, 190 (1973) A Comparative Analysis of Nuclear Excitations by High Energy Electrons, Protons, Pions and Alpha's NUCLEAR REACTIONS 12C, 58Ni, 208Pb(e, e'), (p, p'), (π, π'), (α, α'); analyzed σ data.
doi: 10.1016/0370-2693(73)90179-2
1972RI03 Phys.Lett. 38B, 281 (1972) Evidence for the Existence of Highly Excited Bands of Intermediate Resonances Describing Quasi-Molecular Rotations NUCLEAR REACTIONS 40Ca(α, α), (α, α'), E=18-41 MeV; analyzed σ(θ); deduced intermediate resonances with quasi-molecular rotations.
doi: 10.1016/0370-2693(72)90246-8
1972RI10 Nucl.Phys. A190, 328 (1972) Vertex Parameters and Coupling Constants for the Virtual Decay of Light Nuclei
doi: 10.1016/0375-9474(72)90145-5
1971AV05 Phys.Lett. 36B, 161 (1971) 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
1971AV07 Phys.Lett. 37B, 487 (1971) 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
Back to query form |