NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.M.Eisenberg Found 56 matches. 1997EI03 Acta Phys.Pol. B28, 2919 (1997) Skyrmions in Nuclei
1997PA33 Phys.Rev. C56, 3134 (1997) P.K.Panda, A.Mishra, J.M.Eisenberg, W.Greiner Hot Nuclear Matter in the Quark Meson Coupling Model
doi: 10.1103/PhysRevC.56.3134
1996EI03 Int.J.Mod.Phys. E5, 423 (1996) The Nucleon-Nucleon Force from Skyrmions
doi: 10.1142/S0218301396000219
1996KA17 Nucl.Phys. A600, 436 (1996) G.Kalbermann, J.M.Eisenberg, B.Svetitsky Hot Nuclear Matter with Dilatons
doi: 10.1016/0375-9474(96)00015-2
1995KA13 Phys.Lett. 349B, 416 (1995) An Attractive Nucleon-Nucleon Spin-Orbit Force from Skyrmions with Dilatons
doi: 10.1016/0370-2693(95)00286-T
1995KA16 Nucl.Phys. A587, 609 (1995) Spin Content from Skyrmions with Parameters Fit to Baryon Properties NUCLEAR STRUCTURE 1n, 1H; calculated μ; deduced proton spin content related parameter. Skyrmions with parameters fit to baryon properties.
doi: 10.1016/0375-9474(95)00028-Y
1994DE37 Phys.Lett. 334B, 290 (1994) Skyrmions at Finite Temperature
doi: 10.1016/0370-2693(94)90690-4
1994KA31 Phys.Lett. 329B, 164 (1994) G.Kalbermann, L.L.Frankfurt, J.M.Eisenberg Changes in the Radius of a Nucleon in Interaction with Another Nucleon
doi: 10.1016/0370-2693(94)90754-4
1994KA34 Phys.Lett. 339B, 211 (1994) G.Kalbermann, J.M.Eisenberg, A.Schafer Proton Spin Content from Skyrmions NUCLEAR STRUCTURE 1H; calculated spin content. Particular term in skyrmion lagrangian in SU(3).
doi: 10.1016/0370-2693(94)90633-5
1991KA17 Phys.Rev. C44, 899 (1991) G.Kalbermann, G.Pari, J.M.Eisenberg Consequences of an Alternate Skyrmion Stabilizing Term for the NN Force NUCLEAR STRUCTURE 1n, 1H; calculated μ, charge, radii.
doi: 10.1103/PhysRevC.44.899
1990KA34 Phys.Lett. 247B, 206 (1990) Properties of the Baryon Octet in the SU(3) Skyrme Model NUCLEAR STRUCTURE 1n, 1H; calculated μ, charge radii. SU(3) Skyrme model.
doi: 10.1016/0370-2693(90)90882-7
1987KA10 Phys.Lett. 188B, 311 (1987) An Improved Approximation for the Skyrmion Description of the NN System NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms radius. Skyrme model.
doi: 10.1016/0370-2693(87)91386-4
1984CO02 Phys.Rev. C29, 914 (1984) Response to Spin-Isospin Longitudinal Probes and Pionlike Excitations in Finite Nuclei NUCLEAR STRUCTURE 12C, 16O; calculated longitudinal operator renormalized matrix element, pion self energy for certain levels, response function; deduced spin-isopin strength distribution effects. Infinite nuclear matter techniques, diagrammatic approach.
doi: 10.1103/PhysRevC.29.914
1984KA32 Nucl.Phys. A426, 599 (1984) The ABC Effect and Chiral-Bag-Model Form Factors NUCLEAR REACTIONS 1H(n, 2π0), E at 1.88 GeV/c; calculated σ(θ(π)) vs deuteron momentum. Chiral bag model form factors.
doi: 10.1016/0375-9474(84)90166-0
1984KR22 Nucl.Phys. A430, 525 (1984) J.Kronenfeld, A.Gal, J.M.Eisenberg Antiproton-Nucleus Scattering with Self-Consistent Model for Medium Corrections NUCLEAR REACTIONS 40Ca, 12C(p-bar, p-bar), E=46.8 MeV; calculated σ(θ); deduced antiproton-nucleus interaction parameters. Self-consistent model, medium corrections.
doi: 10.1016/0375-9474(84)90092-7
1983CO04 Nucl.Phys. A395, 389 (1983) The (π, 2π) Reaction and Spin-Isospin Strength Distribution in Nuclei NUCLEAR REACTIONS 16O(π+, 2π+), (π+, π+π-), E ≈ 170-410 MeV; calculated production σ(total). DWIA, local density approximation.
doi: 10.1016/0375-9474(83)90050-7
1983CO15 Phys.Rev. C28, 1309 (1983) (e, e'π) Reaction on Light Nuclei and Spin-Isospin Strength Distribution Effects NUCLEAR REACTIONS 16O(e, e'π-), (e, e'X), E at 400, 800 MeV/c; calculated exclusive, inclusive pion production σ; deduced kinematical condition, energy transfer role in enhancement. Local density approximation, spin-isospin modes.
doi: 10.1103/PhysRevC.28.1309
1983CO18 Nuovo Cim. 76A, 483 (1983) The (e, e'π) Reaction on Light Nuclei and Spin-Isospin Strength Distribution Effects NUCLEAR REACTIONS 12C, 16O(e, e'π), E at 400, 800 MeV/c; calculated inclusive pion production σ; deduced quasifree peak enhancement, spin-isospin strength distribution dependence.
doi: 10.1007/BF02833744
1983CO19 Nuovo Cim. 76A, 488 (1983) The (π, 2π) Reaction and Spin-Isospin Strength Distribution in Nuclei NUCLEAR REACTIONS 16O(π+, 2π+), (π+, π-π+), E not given; calculated σ(inclusive), σ(θ(π1), θ(π2), E(π1)). DWIA, spin-isospin mode enhancement via local density approximation.
doi: 10.1007/BF02833745
1983EI01 J.Phys.(London) G9, 707 (1983) A Schematic Model for Spin-Isospin Strength Distribution in Finite Nuclei NUCLEAR STRUCTURE 4He; calculated spin-isospin transition strength distribution, transition matrix element enhancements. Pion-like excitation, direct, exchange terms, shell model.
doi: 10.1088/0305-4616/9/7/007
1983KR10 Nucl.Phys. A402, 569 (1983) J.Kronenfeld, A.Gal, J.M.Eisenberg An Eikonal Treatment Including Two-Step Mechanisms for the (p, n) Reaction on Light Nuclei NUCLEAR REACTIONS 7Li(p, n), E=160 MeV; 13C(p, n), E=160, 200, 150 MeV; calculated σ(θ) vs momentum transfer; deduced two-step process role. DWIA, eikonal treatment.
doi: 10.1016/0375-9474(83)90220-8
1982KA16 Nucl.Phys. A382, 413 (1982) Final-State Effects in the (π-, 2N) Reaction NUCLEAR REACTIONS 16O(π-, 2n), (π-, pn), E ≈ 200 MeV; calculated two-nucleon emission rates. Final state effects, direct absorption mode.
doi: 10.1016/0375-9474(82)90354-2
1981CO14 J.Phys.(London) G7, 881 (1981) Pion Exchange-Current Contribution to Pion Inelastic Scattering NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E at 200, 300, 400 MeV/c; calculated σ(θ). 12C level deduced exchange current effects on excitation. S-matrix, Feynman diagrams.
doi: 10.1088/0305-4616/7/7/011
1981EI01 Nucl.Phys. A355, 312 (1981) Threshold Electroproduction of Charged Pions and Pion Condensation Precursor Phenomena NUCLEAR REACTIONS 12C(e, eπ+), E at 500 MeV/c; calculated σ(θ(e), θ(π), E(π)); deduced pion condensation precusor effects. Plane wave pion field, catastrophic interaction term, Fermi gas model, nucleon-hole, isobar-hole excitation.
doi: 10.1016/0375-9474(81)90529-7
1981LE06 Nucl.Phys. A355, 277 (1981) A Theoretical Study of Pion-Induced Knockout Reactions in Nuclei NUCLEAR REACTIONS 16O(π+, π+p), E=100, 130, 165 MeV; calculated σ(θ(π), E(π), θp); deduced sensitivity to pion optical model, off-shell, spin-dependent effects. DWIA analysis.
doi: 10.1016/0375-9474(81)90528-5
1980EI01 J.Phys.(London) G6, 1265 (1980) A Simple Relationship between Pion-Nucleus Charge-Exchange and Inelastic Cross Sections NUCLEAR REACTIONS 13C(π+, π0), (π+, π+'), E=75-200 MeV; calculated σ(θ); deduced connection between charge exchange, inelastic scattering processes near (3, 3) resonance. Optical potential, eikonal approximation.
doi: 10.1088/0305-4616/6/10/013
1978WA02 Nucl.Phys. A294, 321 (1978) J.Warszawski, A.Gal, J.M.Eisenberg Isovector Correlations and Pion Single Charge Exchange Reactions in Light Nuclei NUCLEAR REACTIONS 13C, 7Li(π+, π0); calculated σ.
doi: 10.1016/0375-9474(78)90221-X
1978WA12 Nucl.Phys. A312, 253 (1978) J.Warszawski, J.M.Eisenberg, A.Gal The Quadrupole Term of the Lorentz-Lorenz Effect in Pionic Atoms ATOMIC PHYSICS, Mesic-Atoms 27Al, 60Co; calculated contribution of quadrupole terms to observed shifts of pionic atomic energy levels due to Lorentz-Lorenz effect.
doi: 10.1016/0375-9474(78)90589-4
1977LE20 Nucl.Phys. A292, 459 (1977) The Exchange of p-Mesons in π-d and π-4He Elastic Scattering NUCLEAR REACTIONS 2H, 4He(π-, π-), E ≈ 150, 260 MeV; calculated σ(θ) for exchange of p-mesons.
doi: 10.1016/0375-9474(77)90630-3
1976GA21 Phys.Rev. C14, 1273 (1976) Comment on 13C(π+, π0)13N(g.s.) In the (3, 3) Resonance Region NUCLEAR REACTIONS 13C(π+, π0); analyzed necessity of including two-step processes in multiple scattering treatment of reaction.
doi: 10.1103/PhysRevC.14.1273
1975EI01 Phys.Lett. 53B, 405 (1975) J.M.Eisenberg, V.B.Mandelzweig Pion Absorption Effects in the Reaction 3H(π+, π0)3He NUCLEAR REACTIONS 3H(π+, π0); calculated σ.
doi: 10.1016/0370-2693(75)90203-8
1975GA08 Nucl.Phys. A244, 487 (1975) Off-Shell πN Effects in Pion-Nucleus Inelastic Scattering NUCLEAR REACTIONS 12C(π, π'), E=69.5, 87.5, 100, 200, 260 MeV; measured σ(θ).
doi: 10.1016/0375-9474(75)90553-9
1975HE06 Nucl.Phys. A241, 493 (1975) Inelastic Pion-Nucleus Scattering in Distorted-Wave Impulse Approximation NUCLEAR REACTIONS 12C(π, π'), E=70, 150, 200, 250 MeV; 4He, 16O, 90Zr, 208Pb(π, π'), E=200 MeV; 16O, 40Ca(π, π'), E=180 MeV; calculated σ(Eπ', θ).
doi: 10.1016/0375-9474(75)90400-5
1975TO01 Nucl.Phys. A237, 441 (1975) A Heuristic Model of Pion-Nucleus Charge-Exchange Scattering NUCLEAR REACTIONS 91Zr(π+, π0), E=40-300 MeV; calculated σ.
doi: 10.1016/0375-9474(75)90410-8
1974GA08 Nucl.Phys. A220, 13 (1974) Double-Nucleon Emission Following Pion Absorption with a Three-Body Description of the Final State NUCLEAR REACTIONS 12C(π-, 2n); calculated σ(θ).
doi: 10.1016/0375-9474(74)90750-7
1973EI01 Phys.Lett. 43B, 20 (1973) J.M.Eisenberg, R.Guy, J.V.Noble, H.J.Weber Pion Production by 600 MeV Protons on Light Nuclei NUCLEAR REACTIONS 4He, 12C, 14N, 16O(p, π+), E=600 MeV; calculated σ.
doi: 10.1016/0370-2693(73)90532-7
1973EI05 Phys.Lett. 45B, 93 (1973) J.M.Eisenberg, R.Guy, J.V.Noble, H.J.Weber Pion Production by 600 MeV Protons on Light Nuclei NUCLEAR REACTIONS 12C, 14N, 16O(p, π+), E=600 MeV; measured nothing, calculated σ.
doi: 10.1016/0370-2693(73)90072-5
1973EI06 Phys.Lett. 45B, 110 (1973) Exclusion Principle Effects in Pion-Nucleus Scattering in the Region of the 3, 3 Resonance NUCLEAR REACTIONS 12C(π-, π-'); measured nothing, calculated σ(E(π-), θ).
doi: 10.1016/0370-2693(73)90077-4
1973HE30 Phys.Lett. 47B, 311 (1973) Effects of Spin and Isospin Degrees of Freedom for Pion-Nucleus Scattering in the Glauber Theory NUCLEAR REACTIONS 12C(π-, π-), E=60, 120, 180, 260 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(73)90610-2
1973NA24 Phys.Rev. C8, 2488 (1973) N.R.Nath, H.J.Weber, J.M.Eisenberg Exclusion Principle Effects in Pion-Deuteron Scattering Near the 3, 3 Resonance NUCLEAR REACTIONS 2H(π, π'), E=150-250 MeV; calculated σ.
doi: 10.1103/PhysRevC.8.2488
1972EI02 Can.J.Phys. 50, 57 (1972) Higher-Order Corrections to the Optical Potential for Kaonic Atoms
doi: 10.1139/p72-010
1972EI06 Ann.Phys.(New York) 71, 542 (1972) On the Relationship between the Glauber Approximation and the Watson Multiple-Scattering Theory
doi: 10.1016/0003-4916(72)90131-5
1972EI08 Microscopic Theory of the Nucleus, Nuclear Theory, Vol.3, North-Holland Publ.Co., Amsterdam (1972)
1971CH32 Nucl.Phys. A171, 625 (1971) L.A.Charlton, J.M.Eisenberg, W.B.Jones Pion Charge-Exchange Scattering on Nuclei and Isobaric Analog Resonances NUCLEAR REACTIONS 91Zr(π+, π0) , E=30 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(71)90608-7
1971CH41 Ann.Phys.(N.Y.) 63, 286 (1971) Multiple-Scattering Theory for Pion-Nucleus Scattering Near the 3, 3 Resonance NUCLEAR REACTIONS 4He, 16O(π, π), E=153, 195 MeV; calculated σ(θ) near 3-3 resonance.
doi: 10.1016/0003-4916(71)90304-6
1971EI01 Phys.Lett. 34B, 107 (1971) Electroproduction of Slow Pions on Nuclei and Giant Resonance Vibrations NUCLEAR REACTIONS 4He, 16O(e, e'π), E not given; calculated σ for excitation of spin-isospin vibrations.
doi: 10.1016/0370-2693(71)90680-0
1971GU13 Can.J.Phys. 49, 1879 (1971) Nuclear Photo-Emission Following Radiative Pion Absorption NUCLEAR REACTIONS 12C, 16O(π-, γ), E approx o; calculated transition rate.
doi: 10.1139/p71-227
1971MA38 Can.J.Phys. 49, 1826 (1971) Charge-Exchange Scattering of Pions on 14N NUCLEAR REACTIONS 14N(π+, π), E approx 180 MeV; calculated σ(θ). Impulse approximation, Chew-Low π-N scattering amplitude.
doi: 10.1139/p71-218
1970GU09 Phys.Lett. 33B, 137 (1970) Radiative Pion Absorption in Medium and Heavy Nuclei ATOMIC PHYSICS, Mesic-Atoms 40Ca, 90Zr, 208Pb; calculated radiative π-absorption rates.
doi: 10.1016/0370-2693(70)90282-0
1970HA46 Phys.Lett. 33B, 133 (1970) Dynamic Nuclear Effects in Pionic and Kaonic Atoms ATOMIC PHYSICS, Mesic-Atoms 16O, 40Ca, 56Fe, 90Zr, 110Cd, 172Yb, 208Pb, 232Th, 238U, 244Cm; calculated π-, K-absorption widths.
doi: 10.1016/0370-2693(70)90281-9
1970JO18 Nucl.Phys. A154, 49 (1970) Positive Pion Reactions with 12C NUCLEAR REACTIONS 12C(π+, π+), E=30, 40 MeV; 12C(π+, p), E=50 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(70)91068-7
1968CO13 Nucl.Phys. A114, 184 (1968) Odd-Parity States in the A = 6 and 14 Systems
doi: 10.1016/0375-9474(68)90823-3
1966BO17 Phys.Letters 22, 630 (1966) Core Excitation of 20Ne NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90684-6
1966FA09 Nucl.Phys. 88, 241 (1966) Particle-Hole Description of 28Si and 32S NUCLEAR STRUCTURE 28Si, 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90585-2
1966SE05 Nucl.Phys. 82, 308 (1966) Even Parity States in 16O NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90005-8
1964WE08 Nucl.Phys. 53, 508 (1964) Inelastic Electron Scattering from Ca40 in the Giant Resonance Region NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90630-3
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