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Search: Author = A.S.Rinat

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2010RI04      Phys.Rev. C 82, 015207 (2010)

A.S.Rinat, M.F.Taragin

Neutron observables from inclusive lepton scattering on nuclei

doi: 10.1103/PhysRevC.82.015207
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2006RI06      Phys.Rev. C 73, 045201 (2006)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2005RI21      Phys.Rev. C 72, 065209 (2005)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003RI01      Phys.Lett. 551B, 284 (2003)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2002GU04      Phys.Rev. C65, 024310 (2002)

S.A.Gurvitz, A.S.Rinat

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
Citations: PlumX Metrics

2002RI04      Phys.Rev. C65, 042201 (2002)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

2000RI16      Phys.Rev. C62, 034602 (2000)

A.S.Rinat, M.F.Taragin

R Ratios and Moments of Nuclear Structure Functions

doi: 10.1103/PhysRevC.62.034602
Citations: PlumX Metrics

1999RI08      Phys.Rev. C59, 3371 (1999)

A.S.Rinat, B.K.Jennings

Equivalence of the Impulse Approximation and the Gersch-Rodriguez-Smith Series for Structure Functions

doi: 10.1103/PhysRevC.59.3371
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1999RI13      Phys.Lett. 459B, 431 (1999)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

1999RI16      Phys.Rev. C60, 044601 (1999)

A.S.Rinat, M.F.Taragin

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
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1997RI09      Nucl.Phys. A620, 417 (1997); Erratum Nucl.Phys. A624, 773 (1997)

A.S.Rinat, M.F.Taragin

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
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1997RI13      Nucl.Phys. A623, 519 (1997)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

1996RI03      Nucl.Phys. A597, 636 (1996)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

1996RI06      Nucl.Phys. A598, 349 (1996)

A.S.Rinat, M.F.Taragin

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
Citations: PlumX Metrics

1995RI06      Phys.Rev. C52, R28 (1995)

A.S.Rinat, M.F.Taragin

Nuclear Transparencies for Nucleons, Knocked-Out under Various Semi-Inclusive Conditions

doi: 10.1103/PhysRevC.52.R28
Citations: PlumX Metrics

1994PA07      Nucl.Phys. A572, 1 (1994)

E.Pace, G.Salme, A.S.Rinat

Exact Response of the Non-Relativistic Harmonic Oscillator

doi: 10.1016/0375-9474(94)90416-2
Citations: PlumX Metrics

1994PA13      Phys.Lett. 325B, 289 (1994)

E.Pace, G.Salme, A.S.Rinat

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
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1994RI02      Nucl.Phys. A568, 873 (1994)

A.S.Rinat, B.K.Jennings

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
Citations: PlumX Metrics

1994RI05      Nucl.Phys. A571, 733 (1994)

A.S.Rinat, M.F.Taragin

Inclusive Scattering of Electrons from Nuclear Matter in the GeV Range

doi: 10.1016/0375-9474(94)90718-8
Citations: PlumX Metrics

1988JE02      Nucl.Phys. A485, 421 (1988)

B.K.Jennings, A.S.Rinat

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
Citations: PlumX Metrics

1987GU21      Phys.Lett. 197B, 6 (1987)

S.A.Gurvitz, A.S.Rinat

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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.S.Rinat, Y.Starkand

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1980AR15      Nucl.Phys. A350, 205 (1980)

J.Arvieux, A.S.Rinat

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1979HA36      Phys.Lett. 85B, 193 (1979)

E.Hammel, H.Baier, A.S.Rinat

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
Citations: PlumX Metrics

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
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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
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1978HO21      Phys.Rev. C18, 2683 (1978)

M.M.Hoenig, A.S.Rinat

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
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1977AL01      Nucl.Phys. A278, 525 (1977)

Y.Alexander, A.S.Rinat

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
Citations: PlumX Metrics

1977JU01      Nucl.Phys. A280, 467 (1977)

D.I.Julius, A.S.Rinat

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
Citations: PlumX Metrics

1977RI06      Nucl.Phys. A282, 365 (1977)

A.S.Rinat, A.W.Thomas

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976JU01      Nucl.Phys. A268, 477 (1976)

D.I.Julius, A.S.Rinat

Unitarity Effects in High-Energy Nuclear Abrasion

NUCLEAR REACTIONS 12C, 60Ni, 208Pb(p, X); calculated σ.

doi: 10.1016/0375-9474(76)90544-3
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1974GU09      Phys.Lett. 51B, 109 (1974)

S.A.Gurvitz, A.S.Rinat

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
Citations: PlumX Metrics

1974HO29      Phys.Rev. C10, 2102 (1974)

M.M.Hoenig, A.S.Rinat

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
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1974ST14      Phys.Rev. C10, 1253 (1974)

M.Stingl, A.S.Rinat

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
Citations: PlumX Metrics

1973AL14      Phys.Lett. 45B, 190 (1973)

Y.Alexander, A.S.Rinat

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1972RI10      Nucl.Phys. A190, 328 (1972)

A.S.Rinat, L.P.Kok, M.Stingl

Vertex Parameters and Coupling Constants for the Virtual Decay of Light Nuclei

doi: 10.1016/0375-9474(72)90145-5
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1971AV05      Phys.Lett. 36B, 161 (1971)

Y.Avishai, A.S.Rinat

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
Citations: PlumX Metrics

1971AV07      Phys.Lett. 37B, 487 (1971)

Y.Avishai, A.S.Rinat

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
Citations: PlumX Metrics

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