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Search: Author = C.B.Dover

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1995DO01      Phys.Rev. C51, 541 (1995)

C.B.Dover, H.Feshbach, A.Gal

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
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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
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1995GA11      Nucl.Phys. A585, 1c (1995)

A.Gal, C.B.Dover

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
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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
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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
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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
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1994GO18      Phys.Rev. C50, 1594 (1994)

C.Gobbi, C.B.Dover, A.Gal

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
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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
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1993DO12      Nucl.Phys. A560, 559 (1993)

C.B.Dover, A.Gal

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
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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
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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
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1992CH42      Czech.J.Phys. B42, 1089 (1992)

R.E.Chrien, C.B.Dover, A.Gal

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
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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
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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
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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
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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
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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
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1989CH52      Ann.Rev.Nucl.Part.Sci. 39, 113 (1989)

R.E.Chrien, C.B.Dover

Nuclear Systems with Strangeness

doi: 10.1146/annurev.ns.39.120189.000553
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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
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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
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1986DO20      Czech.J.Phys. B36, 329 (1986)


Antinucleon Interactions with Light Nuclei

doi: 10.1007/BF01597832
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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
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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
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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
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1982DO04      Phys.Lett. 110B, 433 (1982)

C.B.Dover, A.Gal

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
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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
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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
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1979DO05      Phys.Rev. C19, 1393 (1979)

C.B.Dover, G.E.Walker

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
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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
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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
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1977DO11      Phys.Rev. C16, 1087 (1977)

C.B.Dover, P.J.Moffa

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
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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
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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
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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
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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
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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
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1975BU03      Phys.Rev. C11, 1803 (1975)

B.Buck, C.B.Dover, J.P.Vary

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
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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
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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
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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
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1973VA21      Phys.Rev.Lett. 31, 1510 (1973)

J.P.Vary, C.B.Dover

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
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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
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1972DO11      Nucl.Phys. A190, 373 (1972)

C.B.Dover, N.V.Giai

The Nucleon-Nucleus Potential in the Hartree-Fock Approximation with Skyrme's Interaction

doi: 10.1016/0375-9474(72)90148-0
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1972DO12      Lett.Nuovo Cim. 4, 487 (1972)

C.B.Dover, R.H.Lemmer

A Chew-Low Approach to Pion-Nucleus Scattering

doi: 10.1007/BF02757150
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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
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1971DO15      Nucl.Phys. A177, 559 (1971)

C.B.Dover, N.Van Giai

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
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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
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1970DO03      Phys.Lett. 32B, 253 (1970)

C.B.Dover, J.Hufner

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
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1969DO05      Phys.Letters 29B, 405 (1969)

C.B.Dover, P.Sandner

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
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1969DO12      Nucl.Phys. A135, 481 (1969)

C.B.Dover, K.Dietrich

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
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1969DO13      Nucl.Phys. A135, 515 (1969)

C.B.Dover, F.J.W.Hahne

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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