NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Rinat Found 53 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
1988SM04 Phys.Rev. C38, 240 (1988) G.R.Smith, D.R.Gill, D.Ottewell, G.D.Wait, P.Walden, R.R.Johnson, R.Olszewski, R.Rui, M.E.Sevior, R.P.Trelle, J.Brack, J.J.Kraushaar, R.A.Ristinen, H.Chase, E.L.Mathie, V.Pafilis, R.B.Schubank, N.R.Stevenson, A.Rinat, Y.Alexander Energy Dependence of the Charge Asymmetry A(T(π), θ) in πd Elastic Scattering NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E=143-256 MeV; measured charge asymmetry vs E, θ; deduced Δ-isobar parameters.
doi: 10.1103/PhysRevC.38.240
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
1978DI07 Phys.Lett. 76B, 135 (1978) A.E.L.Dieperink, F.Iachello, A.Rinat, C.Creswell Electron Scattering in the Interacting Boson Model NUCLEAR STRUCTURE 150Nd, 150,152,154Sm; calculated B(E2). Interacting boson model.
doi: 10.1016/0370-2693(78)90259-9
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
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