NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = J.Cohen Found 35 matches. 2002CO13 Phys.Rev. A65, 052714 (2002) Capture of Negative Muons and Antiprotons by Noble-Gas Atoms ATOMIC PHYSICS He, Ne, Ar, Kr, Xe(μ-, X), (p-bar, X), E=low; calculated capture σ. Fermion molecular dynamics method.
doi: 10.1103/PhysRevA.65.052714
1999CO07 Phys.Rev. A59, 1160 (1999) Isotope Effects on Antiproton and Muon Capture by Hydrogen and Deuterium Atoms and Molecules ATOMIC PHYSICS, Mesic-atoms 2H(p-bar, X), E at rest; 1,2H(μ-, X), E at rest; calculated total, capture σ; deduced isotope effects. Molecular systems also studied. Fermion molecular dynamics.
doi: 10.1103/PhysRevA.59.1160
1999CO12 Phys.Rev. A59, 4300 (1999) Negative Pion Capture in HD Gas and in H2 + D2 Gas Mixtures: Resolution of the isotope puzzle ATOMIC PHYSICS, Mesic-atoms; 1,2H(π-, X), E=low; calculated capture σ for molecular hydrogen; deduced molecular structure, isotopic effects.
doi: 10.1103/PhysRevA.59.4300
1998CO25 J.Phys.(London) B31, L833 (1998) Fermion Molecular Dynamics in the Capture of Muons by Hydrogen Atoms ATOMIC PHYSICS, Mesic-atoms 1H(μ-, X), E at rest; calculated capture σ. Fermion molecular dynamics method.
doi: 10.1088/0953-4075/31/19/011
1993CO10 Phys.Rev. C48, 1346 (1993) Nuclear and Hypernuclear Particle-Hole States in the Relativistic σ-(Omega) Mean Field Theory: Nuclear matter formalism NUCLEAR STRUCTURE A=16-208; calculated hypernuclear magnetic moments. Relativistic σ-omega mean field theory, nuclear matter formalism.
doi: 10.1103/PhysRevC.48.1346
1992CO28 Nucl.Phys. A547, 133c (1992) Weak Non-Mesonic Decays of (Lambda)-Hypernuclei NUCLEAR STRUCTURE A=4-20; compiled, reviewed weak, nonmesonic decay of lambda hypernuclei decay.
doi: 10.1016/0375-9474(92)90719-Z
1989CO16 Phys.Rev. C40, 1468 (1989) 0+, T = 0(p, p')0-, T = 1 Pionlike Excitations and Nuclear Response in the Spin-Isospin Channel NUCLEAR REACTIONS 40Ca(p, p'), E not given; calculated spin-isospin channel response function; deduced spin-isospin renormalization effects in σ. Pionlike excitations. NUCLEAR STRUCTURE 40Ca, 16O; calculated spin-isospin operator matrix elements. Pionlike excitations.
doi: 10.1103/PhysRevC.40.1468
1989CO23 Nature(London) 338, 705 (1989) The Cold Fusion Family
doi: 10.1038/338705a0
1989CO24 Nature(London) 342, 487 (1989) Is Cold Fusion Hot ( Question )
doi: 10.1038/342487b0
1989CO25 Nucl.Instrum.Methods Phys.Res. B42, 419 (1989) Muon Catalyzed Fusion
doi: 10.1016/0168-583X(89)90095-5
1989CO26 Phys.Rev. A39, 915 (1989) Effect of Anisotropy on the Sticking in Muon-Catalyzed Fusion Determined by the X-Ray Method
doi: 10.1103/PhysRevA.39.915
1987CO09 Phys.Lett. 188B, 393 (1987) J.Cohen, M.W.Price, G.E.Walker Kaon Electroproduction and Low-Lying Hypernuclear Excitations using a Relativistic Transition Operator and Nuclear Structure Model NUCLEAR REACTIONS 16O(e, e'K+), E=2 GeV/c; calculated σ(EK, θK, E(e'), θ(e')). Relativistic model.
doi: 10.1016/0370-2693(87)91636-4
1987CO20 J.Phys.(London) G13, 1099 (1987) RPA Finite-Nucleus Response to Spin-Isospin Probes: Investigation of the role of theoretical inputs on the strength distribution effects NUCLEAR STRUCTURE 12C; calculated response function matrix partial waves, longitudinal, transverse reduced matrix elements. RPA.
doi: 10.1088/0305-4616/13/9/012
1987CO37 J.Phys.(London) G13, 1497 (1987) Investigation of the Role of Spin-Isospin Strength Distribution Effects in Stretched Excitations of Medium Nuclei NUCLEAR STRUCTURE 40Ca; calculated stretched excitation response functions; deduced spin-isospin strength distribution.
doi: 10.1088/0305-4616/13/12/008
1987WI07 Phys.Rev.Lett. 58, 2023 (1987) J.F.Wilkerson, T.J.Bowles, M.P.Maley, R.G.H.Robertson, J.S.Cohen, R.L.Martin, D.A.Knapp, J.A.Helffrich Limit on (ν-bar(e)) Mass from Free-Molecular-Tritium Beta Decay RADIOACTIVITY 3H(β-); measured molecular beta spectrum; deduced electron-antineutrino mass limit. Si detector, beta spectrometer.
doi: 10.1103/PhysRevLett.58.2023
1985CO03 Phys.Lett. 150B, 45 (1985) Nuclear Renormalization Effects in Exclusive (π, πN) Reactions NUCLEAR REACTIONS 12C(π+, π+p), E=high; calculated σ(E(π), θ(π), θp). Simple pion-nucleon scattering amplitude renormalization.
doi: 10.1016/0370-2693(85)90134-0
1985CO05 J.Phys.(London) G11, 635 (1985) Finite-Nucleus Treatment of the Response to σ(μ)τ(λ) Probes and Pion-Like Excitations. II: The Role of Rho-Meson Exchange NUCLEAR STRUCTURE 12C; calculated spin-isospin probe matrix element renormalization for 1+, T=1 level; deduced ρ-meson role.
doi: 10.1088/0305-4616/11/5/010
1985CO14 Phys.Rev. C32, 543 (1985) Hypernuclear Physics with Electron Beams: Exclusive and inclusive excitations NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(e, e'K+), E not given; calculated exclusive, inclusive σ(E(K+), θ(K+)) vs electron momentum.
doi: 10.1103/PhysRevC.32.543
1985CO16 Phys.Rev. C32, 961 (1985) Noncoplanar Geometry for Detecting Nuclear Renormalization Effects in Exclusive (π, πN) Reactions NUCLEAR REACTIONS 12C(π+, π+p), E=300, 350, 375 MeV; calculated σ(θp, θπ) vs pion momentum; deduced isobar resonance renormalization in nuclear interior. Noncoplanar geometry.
doi: 10.1103/PhysRevC.32.961
1985CO25 Phys.Lett. 164B, 207 (1985) Stretched Isovector Excitations and Spin-Isospin Strength Distribution Effects in Finite Nuclei NUCLEAR STRUCTURE 40Ca; calculated stretched transition longitudinal, transverse spin-isospin operator matrix element renormalization ratio.
doi: 10.1016/0370-2693(85)90310-7
1985CO26 Phys.Lett. 164B, 253 (1985) 0+ → 0- Pion-Like Excitations in Light and Medium Nuclei NUCLEAR STRUCTURE 40Ca; calculated pion-like excitation characteristics, longitudinal spin-isospin operator matrix element renormalization ratio.
doi: 10.1016/0370-2693(85)90320-X
1985CO30 Phys.Lett. 165B, 229 (1985) Magnetic Moments of Baryons in a Constituent Quark Model with Relativistic and Pionic Corrections NUCLEAR STRUCTURE 1n, 1H; calculated μ. Constituent quark model.
doi: 10.1016/0370-2693(85)91219-5
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
1984CO16 Phys.Rev. C30, 1238 (1984) Response to Spin-Isospin Transverse Probes and Pionlike Excitations in Finite Nuclei NUCLEAR STRUCTURE 12C; calculated transverse probe renormalized matrix elements, longitudinal, transverse response functions.
doi: 10.1103/PhysRevC.30.1238
1984CO21 Phys.Rev. C30, 1573 (1984) Investigation of the Role of the Rho-Meson Exchange in Spin-Isospin Strength Distribution Effects in a Finite Nucleus NUCLEAR STRUCTURE 12C; calculated spin-isospin strength distribution; deduced rho-meson exchange role. Finite nucleus formalism.
doi: 10.1103/PhysRevC.30.1573
1984CO23 J.Phys.(London) G10, 1347 (1984) Finite-Nucleus Treatment of the Response to σ(μ)τ(λ) Probes and Pion-Like Excitations NUCLEAR STRUCTURE 12C; calculated spin, isospin probe response function, matrix element ratio. Finite nucleus treatment, partial wave expansion, good total angular momentum.
doi: 10.1088/0305-4616/10/10/007
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
1983CO08 J.Phys.(London) G9, 621 (1983) The A Dependence and Threshold Behaviour of the Inclusive (π, 2π) Reaction for T = 0 Nuclei NUCLEAR REACTIONS 16O(π+, 2π+), (π+, π-π+), E at 300 MeV/c; calculated inclusive σ(θ(π)) vs E(π); deduced Coulomb effects, mass dependence. Other calculation input.
doi: 10.1088/0305-4616/9/6/007
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
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
1965CO13 J.Phys.(Paris) 26, 427 (1965) Reaction (p, 2p) sur Quelques Isotopes du Titane NUCLEAR STRUCTURE 44Sc, 48Sc, 47Sc, 46Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:01965002607042700
1963VA39 Phys.Lett. 7, 163 (1963) L.Valentin, G.Albouy, J.P.Cohen, M.Gusakow Reactions induites par des protons de 155 MeV sur des noyaux legers NUCLEAR REACTIONS 12C(p, np), (p, 3n3p), E=155 MeV; measured reaction products, Eγ, Iγ. 7Be, 10,11C, 13N, 14,15O, 17,18F, 19Ne; deduced σ. Orsay synchrocyclotron.
doi: 10.1016/0031-9163(63)90651-6
1962AL16 Phys.Letters 2, 306 (1962) G.Albouy, J.P.Cohen, M.Gusakow, N.Poffe, H.Sergolle, L.Valentin Spallation de L'Oxygene par des Protons de 20 A 150 MeV NUCLEAR STRUCTURE 16O, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(62)90119-1
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