NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = C.Dover Found 55 matches. 1997DO16 Nucl.Phys. A625, 1 (1997) C.B.Dover, P.Fishbane, T.Gutsche On Threshold Proton-Antiproton Annihilation to K+-K--Meson States NUCLEAR REACTIONS 1H(p-bar, K+K-X), E not given; calculated φ, ω production σ ratios.
doi: 10.1016/S0375-9474(97)00488-0
1996BA04 Phys.Rev. C53, 362 (1996) Quark Model φ Coalescence from Kaons in Heavy-Ion Reactions NUCLEAR REACTIONS 197Au(Si, X), E at 14.6 GeV/c/nucleon; calculated kaon-, φ-meson multiplicities. Quark model of kaon coalescence.
doi: 10.1103/PhysRevC.53.362
1996KA12 Phys.Rev. C54, 338 (1996) D.E.Kahana, S.H.Kahana, Y.Pang, A.J.Baltz, C.B.Dover, E.Schnedermann, T.J.Schlagel Modeling Cluster Production at the BNL Alternating Gradient Synchrotron NUCLEAR REACTIONS 197Au(Si, X), E at 14.6 GeV/c/nucleon; analyzed data, relativistic collisions; deduced parameter free absolute deuteron yields. Deuteron coalescence, modeling cluster production.
doi: 10.1103/PhysRevC.54.338
1995DO01 Phys.Rev. C51, 541 (1995) Signatures of (Lambda)-Σ Mixing in the Magnetic Moments of Hypernuclei NUCLEAR STRUCTURE A=3, 4; calculated hypernuclear μ; deduced (lambda-Σ)-mixing role. Other nuclei studied.
doi: 10.1103/PhysRevC.51.541
1995DO20 Nucl.Phys. A590, 333c (1995) Aspects of Strangeness NUCLEAR REACTIONS 27Al, Cu, 197Au(Si, X), E=14.6 GeV/nucleon; compiled, reviewed, analyzed this, other data. Quark-gluon plasma, hadron gas thermal models, event generators.
doi: 10.1016/0375-9474(95)00245-V
1995GA11 Nucl.Phys. A585, 1c (1995) Strange Hadronic Matter NUCLEAR STRUCTURE A ≤ 500; compiled, reviewed binding energy per nucleon for stable multi-strange states based on 56Ni, 180Th cores. Other aspects discussed.
doi: 10.1016/0375-9474(94)00536-V
1995SC14 Phys.Lett. 345B, 119 (1995) E.Schnedermann, A.J.Baltz, C.B.Dover On the Production of Pineuts in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), (Si, X), 27Al(Si, X), E=high; calculated (π-nn), (π-4n), (2π-2n) bound system production rates.
doi: 10.1016/0370-2693(94)01536-L
1994AR15 Z.Phys. A348, 201 (1994) Z.Arvay, J.Zimanyi, T.Csorgo, C.B.Dover, U.Heinz Production of Strange Clusters by Quark-Gluon-Plasma Fragmentation
1994BA33 Phys.Lett. 325B, 7 (1994) A.J.Baltz, C.B.Dover, S.H.Kahana, Y.Pang, T.J.Schlagel, E.Schnedermann Strange Cluster Formation in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(Si, X), E at 14.6 GeV/c; calculated p, d rapidity distributions. Si, Pb(Si, X), E at 14.6 GeV/c; calculated lambda rapidity distributions. 197Au(197Au, X), E=relativistic; calculated lambda production rate (lambda)(lambda) rapidity, transverse momentum distributions. Simplified coalescence model.
doi: 10.1016/0370-2693(94)90063-9
1994DO09 Nucl.Phys. A572, 85 (1994) C.B.Dover, A.Gal, D.J.Millener On the Production and Decay of Strangeness S = -2 Hypernuclei
doi: 10.1016/0375-9474(94)90423-5
1994GO18 Phys.Rev. C50, 1594 (1994) Scalar and Vector Meson Production in (K-, K+) Reactions on Nuclei NUCLEAR REACTIONS 12C, 27Al, 107Ag, 208Pb, 63Cu(K-, K+), E at 1.65 GeV/c; analyzed data; deduced scalar, vector meson production, decay role on K+ spectrum.
doi: 10.1103/PhysRevC.50.1594
1994MI37 Prog.Theor.Phys.(Kyoto), Suppl. 117, 307 (1994) D.J.Millener, C.B.Dover, A.Gal Widths of Ξ Hypernuclear States NUCLEAR STRUCTURE A=12; calculated Λ-, neutron decay widths in hypernuclei. Shell model approach.
doi: 10.1143/PTPS.117.307
1993DO12 Nucl.Phys. A560, 559 (1993) A Generalized Bethe-Weizsacker Mass Formula for Strange Hadronic Matter NUCLEAR STRUCTURE A=50-300; calculated multi-lambda hypernuclei binding energy, charge, strangeness fractions per baryon. Extension of Bethe-Weizsacker mass formula to strange hadronic matter.
doi: 10.1016/0375-9474(93)90115-E
1993KA07 Phys.Rev. C47, R1356 (1993) S.H.Kahana, Y.Pang, T.Schlagel, C.B.Dover Antiproton Production from Heavy Ion Collisions at 14.6 GeV/c NUCLEAR REACTIONS 27Al, 197Au(Si, X), E at 14.6 GeV/c; analyzed antiproton rapidity distributions. 27Al(p, X), E at 14.6 GeV/c; analyzed pion, p-bar transverse mass spectra; deduced three-body screening mechanism role. Relativistic cascade code.
doi: 10.1103/PhysRevC.47.R1356
1993SC24 Phys.Rev.Lett. 71, 1328 (1993) J.Schaffner, C.B.Dover, A.Gal, C.Greiner, H.Stocker Strange Hadronic Matter NUCLEAR STRUCTURE 132Sn, 208Pb, 56Ni; calculated binding energy per baryon (with these nuclei as core), strange hadronic matter.
doi: 10.1103/PhysRevLett.71.1328
1992CH42 Czech.J.Phys. B42, 1089 (1992) Two-Nucleon Production of Hyperons and the Search for Strange Dibaryons NUCLEAR REACTIONS 3He(K-, π+X), E at 870 MeV/c; measured mass spectra; deduced two-nucleon mechanism dominance.
doi: 10.1007/BF01591396
1992DO01 Phys.Lett. 277B, 23 (1992) C.B.Dover, T.Gutsche, A.Faessler, R.Vinh Mau Production of Q(Q-bar)g Hybrid Mesons in (N-bar)N Annihilation NUCLEAR REACTIONS 1H(p-bar, X), E=low; calculated hybrid meson production rate.
doi: 10.1016/0370-2693(92)90950-9
1992DO14 Nucl.Phys. A547, 27c (1992) Open Problems and Future Prospects for Hypernuclear Physics NUCLEAR REACTIONS 12C(γ, K+), E=2 GeV; 16O(K-, K+), E at 1.1 GeV/c; compiled, reviewed hypernuclei production data, calculations.
doi: 10.1016/0375-9474(92)90707-Q
1991DO02 Phys.Rev. C43, 379 (1991) C.B.Dover, T.Gutsche, A.Faessler Case for Quasinuclear N(Bar)N Bound States NUCLEAR REACTIONS 1H(p-bar, X), (n-bar, X), E not given; calculated (π+π-) mass spectrum following annihilation; deduced (N-bar)N bound states role.
doi: 10.1103/PhysRevC.43.379
1991DO07 Phys.Rev. C44, 1905 (1991) C.B.Dover, D.J.Millener, A.Gal, D.H.Davis Interpretation of a Double Hypernucleus Event NUCLEAR STRUCTURE A=13; analyzed data; deduced double hypernucleus event features.
doi: 10.1103/PhysRevC.44.1905
1991ZH26 Phys.Rev.Lett. 67, 2268 (1991) D.Zhu, C.B.Dover, A.Gal, M.May Formation of Lambda Lambda Hypernuclei by Σ- Capture in Light Nuclei
doi: 10.1103/PhysRevLett.67.2268
1989CH52 Ann.Rev.Nucl.Part.Sci. 39, 113 (1989) Nuclear Systems with Strangeness
doi: 10.1146/annurev.ns.39.120189.000553
1988BR16 Phys.Rev.Lett. 60, 2723 (1988) G.E.Brown, C.B.Dover, P.B.Siegel, W.Weise K+-Nucleus Scattering and the ' Swelling ' of Nucleons in Nuclei NUCLEAR REACTIONS 12C(K+, K+), E at 800 MeV/c; calculated σ(θ); deduced nucleon swelling role.
doi: 10.1103/PhysRevLett.60.2723
1986DO01 Phys.Rev.Lett. 56, 119 (1986) C.B.Dover, A.Gal, L.Klieb, D.J.Millener Definitive Tests of the Σ-Nuclear Spin-Orbit Splitting NUCLEAR REACTIONS 7Li, 13C(K-, π+), 13C(K-, π-), E at rest; calculated relative hypernuclei production yields.
doi: 10.1103/PhysRevLett.56.119
1986DO20 Czech.J.Phys. B36, 329 (1986) Antinucleon Interactions with Light Nuclei
doi: 10.1007/BF01597832
1985BA51 Phys.Rev. C32, 1272 (1985) A.J.Baltz, C.B.Dover, M.E.Sainio, A.Gal, G.Toker Nuclei Containing an Antinucleon NUCLEAR REACTIONS 3,4He, 16O(p-bar, p), E=80-400 MeV; calculated σ(θ); deduced anti-nucleon nuclei formation σ.
doi: 10.1103/PhysRevC.32.1272
1984DO04 Phys.Lett. 138B, 337 (1984) C.B.Dover, A.Gal, D.J.Millener Is Isospin a Good Quantum Number for Σ Hypernuclei ( Question ) NUCLEAR REACTIONS 12C(K-, π+), (K-, π-), E=400, 450 MeV/c; analyzed data; deduced isospin mixing in hypernucleus 12C.
doi: 10.1016/0370-2693(84)91911-7
1984DO15 Phys.Lett. 143B, 45 (1984) C.B.Dover, M.A.Franey, W.G.Love, M.E.Sainio, G.E.Walker Antinucleon-Nucleus Inelastic Scattering and the Spin Dependence of the N(bar)N Annihilation Potential NUCLEAR REACTIONS 12C(p-bar, p-bar'), E=175 MeV; calculated σ(θ), polarization; deduced nucleon-antinucleon annihilation potential.
doi: 10.1016/0370-2693(84)90801-3
1982DO04 Phys.Lett. 110B, 433 (1982) The 6Li(K-, π+)6H(Σ) Reaction and Narrow Σ States NUCLEAR REACTIONS 6Li(K-, π+), E at 720 MeV/c; calculated σ(θ); deduced resonance in hyperon continuum.
doi: 10.1016/0370-2693(82)91032-2
1981AU01 Phys.Rev.Lett. 46, 702 (1981) E.H.Auerbach, C.B.Dover, S.H.Kahana Resonance Phenomena in Antiproton-Nucleus Scattering NUCLEAR REACTIONS 40Ca, 16O(p-bar, p-bar), E ≈ 10-126 MeV; calculated σ(E, θ), polarization vs θ; deduced resonance effects. Folded potential, equivalent Woods-Saxon potential.
doi: 10.1103/PhysRevLett.46.702
1981AU05 Phys.Rev.Lett. 47, 1110 (1981) E.H.Auerbach, A.J.Baltz, C.B.Dover, A.Gal, S.H.Kahana, L.Ludeking, D.J.Millener Lambda-Nuclear Properties from the Spectroscopy of 13C Hypernucleus NUCLEAR REACTIONS 13C(K-, π-), E at 800 MeV/c; analyzed σ(θ). Shell model, DWBA calculations.
doi: 10.1103/PhysRevLett.47.1110
1979DO05 Phys.Rev. C19, 1393 (1979) Kaon Inelastic Scattering and Charge Exchange on Nuclei NUCLEAR REACTIONS 12C(K+, K+'), 12C(K-, K-'), E at 300-800 MeV/c; 30Si(K-, K0), E at 300 MeV/c; calculated σ(θ); deduced usefulness of kaons as structure probe. Microscopic particle-hole shell model, DWIA analysis.
doi: 10.1103/PhysRevC.19.1393
1979DO18 Phys.Lett. 89B, 26 (1979) C.B.Dover, A.Gal, G.E.Walker, R.H.Dalitz Angular Distributions for the 12C(K-, π-)12C Reaction NUCLEAR REACTIONS 12C(K-, π-), E at 800 MeV/c; calculated σ(θ). DWIA.
doi: 10.1016/0370-2693(79)90068-6
1979MA26 Phys.Rev. C20, 1340 (1979) L.M.Martz, S.J.Sanders, P.D.Parker, C.B.Dover (6Li, t), (6Li, 3He), and (7Li, t) Reactions into the A = 19 Nuclei NUCLEAR REACTIONS 15N(7Li, t), E=40 MeV; 16O(6Li, t), (6Li, 3He), E=46 MeV; measured σ(θ). 19Ne, 19F deduced levels; calculated triton-cluster states.
doi: 10.1103/PhysRevC.20.1340
1977DO11 Phys.Rev. C16, 1087 (1977) Interaction of K+ Mesons with Nuclei NUCLEAR REACTIONS 12C(K+, X), (K-, X), 1H, 208Pb(K+, X); calculated σ.
doi: 10.1103/PhysRevC.16.1087
1977MO17 Phys.Rev. C16, 1857 (1977) P.J.Moffa, C.B.Dover, J.P.Vary Folding Model Description of Heavy Ion Inelastic Scattering NUCLEAR REACTIONS 208Pb(12C, 12C'), E=96 MeV; 16O(12C, 12C'), (12C, 12C), E=168 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.16.1857
1976CA23 Phys.Rev. C14, 635 (1976) A.S.Carroll, I-H.Chiang, C.B.Dover, T.F.Kycia, K.K.Li, P.O.Mazur, D.N.Michael, P.M.Mockett, D.C.Rahm, R.Rubinstein Pion-Nucleus Total Cross Sections in the (3, 3) Resonance Region NUCLEAR REACTIONS Li, C, Al, Fe, Sn, Pb(π+, X), (π-, X), E=60-320 MeV; measured total transmission σ(E).
doi: 10.1103/PhysRevC.14.635
1976MO02 Phys.Rev. C13, 147 (1976) P.J.Moffa, C.B.Dover, J.P.Vary Localization in Heavy-Ion Elastic, Inelastic, and Transfer Reactions NUCLEAR REACTIONS 60Ni(13C, 13C), (13C, 13C'), (13C, 12C), E=60.8 MeV; 28Si(16O, 16O), E=81 MeV; calculated σ. Optical model, DWBA analysis.
doi: 10.1103/PhysRevC.13.147
1976SC38 Ann.Rev.Nucl.Part.Sci. 26, 239 (1976) G.Scharff-Goldhaber, C.B.Dover, A.L.Goodman The Variable Moment of Inertia (VMI) Model and Theories of Nuclear Collective Motion NUCLEAR STRUCTURE 4He, 14,16O, 14C, 40Ca, 72Ge, 96Zr, 98Mo, 208Pb; analyzed available data; deduced J, π, level energy systematics for the first-excited states in even-even nuclei.
doi: 10.1146/annurev.ns.26.120176.001323
1975BA05 Phys.Rev. C11, 360 (1975) S.Barshay, C.B.Dover, J.P.Vary Nucleus-Nucleus Cross Sections and the Validity of the Factorization Hypothesis at Intermediate and High Energies NUCLEAR REACTIONS 208Pb, 90Zr, 16O, 58Ni, 12C(α, X), (α, α), 208Pb, 90Zr, 16O, 58Ni, 14N(12C, X), (12C, 12C), (14N, X), (14N, 14N), 208Pb, 90Zr, 58Ni(16O, X), (16O, 16O), 90Zr, 208Pb, 58Ni(40Ar, X), (40Ar, 40Ar), 208Pb, 120Sn(90Zr, X), (90Zr, 90Zr), 208Pb(120Sn, X), (120Sn, 120Sn), 4He(3He, X), (3He, 3He), E=1.05 GeV/particle; calculated σ. 3,4He, 6Li, 9Be, 12C, 14N, 16,18O, 24Mg, 28Si, 32S, 40Ar, 48Ti, 58Ni, 68Zn, 90Zr, 120Sn, 140Ce, 197Au, 208Pb(p, X), (p, p), E=800 MeV; calculated σ.
doi: 10.1103/PhysRevC.11.360
1975BU03 Phys.Rev. C11, 1803 (1975) Simple Potential Model for Cluster States in Light Nuclei NUCLEAR STRUCTURE 15N, 16O, 20Ne; calculated levels, J, π, B(E2) values, α-widths, radii in cluster model with folded potential.
doi: 10.1103/PhysRevC.11.1803
1975DO03 Phys.Lett. 56B, 4 (1975) C.B.Dover, P.J.Moffa, J.P.Vary Inelastic Heavy Ion Scattering in a Folding Model NUCLEAR REACTIONS 58Ni(16O, 16O'), E=50, 60, 70 MeV; calculated σ; deduced form factor, deformation length.
doi: 10.1016/0370-2693(75)90485-2
1975MO23 Phys.Rev.Lett. 35, 992 (1975) P.J.Moffa, J.P.Vary, C.B.Dover, C.W.Towsley, R.G.Hanus, K.Nagatani Confirmation of the Predicted L Dependence in the Radial Form Factor for Nucleus-Nucleus Inelastic Scattering NUCLEAR REACTIONS 12C, 16O(14N, 14N'), E=155 MeV; measured σ(E(14N'), θ). 12C, 16O levels deduced form factors.
doi: 10.1103/PhysRevLett.35.992
1974BA40 Phys.Lett. 51B, 5 (1974) S.Barshay, C.B.Dover, J.P.Vary The Validity of the Factorization Hypothesis for Nucleus-Nucleus Cross Sections at High Energies NUCLEAR REACTIONS 208Pb, 90Zr, 58Ni(α, X), (14N, X), (16O, X), (40Ar, X), 16O(α, X), (14N, X), 3He(α, X), calculated σ, elastic slopes at 2.1 GeV/nucleon.
doi: 10.1016/0370-2693(74)90136-1
1973VA21 Phys.Rev.Lett. 31, 1510 (1973) Simple Potential Model for Nucleus-Nucleus Interactions NUCLEAR REACTIONS 40Ca(13C, 13C), (14N, 14N), (13C, 12C), E=68 MeV; 40Ca, 208Pb(α, α), E=104 MeV; 48Ca(13C, 13C), (14N, 14N), (14N, 13C), E=50 MeV; 58,60,62,64Ni(16O, 16O), (18O, 18O), E=61, 62, 63 MeV; 58,60,62,64Ni(18O, 16O), E=65 MeV; calculated σ(θ). 20Ne calculated levels, J, π, level-width.
doi: 10.1103/PhysRevLett.31.1510
1972DO10 Ann.Phys.(New York) 70, 458 (1972) C.B.Dover, R.H.Lemmer, F.J.W.Hahne Damping of Nuclear Dipole States
doi: 10.1016/0003-4916(72)90275-8
1972DO11 Nucl.Phys. A190, 373 (1972) The Nucleon-Nucleus Potential in the Hartree-Fock Approximation with Skyrme's Interaction
doi: 10.1016/0375-9474(72)90148-0
1972DO12 Lett.Nuovo Cim. 4, 487 (1972) A Chew-Low Approach to Pion-Nucleus Scattering
doi: 10.1007/BF02757150
1971DO06 Nucl.Phys. A166, 461 (1971) C.B.Dover, S.Cierjacks, G.J.Kirouac, J.Nebe, H.H.Dubenkropp, R.Putzki, B.Zeitnitz Neutron Scattering from 15N (II). Coupled Channel Calculations NUCLEAR REACTIONS 15N(n, n), E < 12 MeV; calculated σ(E;θ). Coupled-channel theory.
doi: 10.1016/0375-9474(71)90901-8
1971DO15 Nucl.Phys. A177, 559 (1971) Low-Energy Neutron Scattering by a Hartree-Fock Field NUCLEAR REACTIONS 12C, 16O, 40Ca(n, X), (n, n), E=0.8-1.8 MeV; calculated σ(nT), σ(θ). 17O resonances deduced level-width.
doi: 10.1016/0375-9474(71)90308-3
1971ZE02 Nucl.Phys. A166, 443 (1971) B.Zeitnitz, H.Dubenkropp, R.Putzki, G.J.Kirouac, S.Cierjacks, J.Nebe, C.B.Dover Neutron Scattering from 15N (I). R-Matrix and Phase-Shift Analyses NUCLEAR REACTIONS 15N(n, X), (n, n), E=0.9-32 MeV; measured σ(nt)(E), σ(E), σ(E, θ), P(E, θ). R-matrix, phase-shift analyses. 16N deduced resonances, J, π, Γ. Enriched target.
doi: 10.1016/0375-9474(71)90900-6
1970DO03 Phys.Lett. 32B, 253 (1970) Photoexcitation of Isobaric Analogue Resonances in 208Pb NUCLEAR REACTIONS 208Pb(γ, p), E=24.9 MeV; measured σ(Ep). 208Pb deduced isobaric analog resonance, level-width.
doi: 10.1016/0370-2693(70)90520-4
1969DO05 Phys.Letters 29B, 405 (1969) Coupled Channel Calculations for the Reaction 15N(n, n')15N* NUCLEAR REACTIONS 15N(n, n), (n, n'), E=0-12 MeV; calculated σ(E), coupled channels method. 16N deduced resonances, level-width.
doi: 10.1016/0370-2693(69)90231-7
1969DO12 Nucl.Phys. A135, 481 (1969) RPA Calculations in the Continuum (I). Cross Sections for 207Pb(n, n')207*Pb NUCLEAR REACTIONS 207Pb(n, n), (n, n'), E =1.5-7 MeV; calculated σ(E;θ).
doi: 10.1016/0375-9474(69)90001-3
1969DO13 Nucl.Phys. A135, 515 (1969) RPA Calculations in the Continuum (II). Bound States and Resonance Energies in 208Pb NUCLEAR STRUCTURE 208Pb; calculated bound states, resonance widths.
doi: 10.1016/0375-9474(69)90002-5
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