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NSR database version of April 11, 2024.

Search: Author = M.R.Clover

Found 19 matches.

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1986MC04      Phys.Rev.Lett. 56, 2156 (1986)

P.L.McGaughey, K.D.Bol, M.R.Clover, R.M.DeVries, N.J.DiGiacomo, J.S.Kapustinsky, W.E.Sondheim, G.R.Smith, J.W.Sunier, Y.Yariv, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, J.C.Dousse

Dynamics of Low-Energy Antiproton Annihilation in Nuclei as Inferred from Inclusive Proton and Pion Measurements

NUCLEAR REACTIONS 12C, 89Y, 238U(p-bar, π+X), (p-bar, pX), E at 608 MeV/c; measured annihilation production σ for π+, p. Intranuclear cascade models.

doi: 10.1103/PhysRevLett.56.2156
Citations: PlumX Metrics

1985DI01      Phys.Rev. C31, 292 (1985)

N.J.DiGiacomo, M.R.Clover, R.M.DeVries, J.C.Dousse, J.S.Kapustinsky, P.L.McGaughey, W.E.Sondheim, J.W.Sunier, M.Buenerd, D.Lebrun

Inclusive Pion Production in 330, 400 and 500 MeV Proton-Nucleus Collisions

NUCLEAR REACTIONS 12C, 238U(p, π+X), (p, π-X), E=330, 400, 500 MeV; measured σ(θ) vs pion momentum, σ; deduced π+ to π- production ratio.

doi: 10.1103/PhysRevC.31.292
Citations: PlumX Metrics

1984DI02      J.Phys.(London) G10, L119 (1984)

N.J.DiGiacomo, M.R.Clover

The Significance of Positive Kaon Production in Low-Energy p(bar)-Nucleus Annihilations

NUCLEAR REACTIONS 12C, 238U(p-bar, K+), E at 0.6 GeV/c; calculated kaon production σ vs kaon momentum. Intranuclear cascade model.

doi: 10.1088/0305-4616/10/6/003
Citations: PlumX Metrics

1984FR08      Phys.Rev. C30, 720 (1984)

Z.Fraenkel, E.Piasetzky, M.R.Clover

Pion-Nucleus Absorption via the Delta-Nucleon Intermediate State

NUCLEAR REACTIONS 12C(π+, X), (π+, 2p), E=245 MeV; calculated absorption σ. 27Al, 58Ni, 181Ta(π+, p), (π-, p), E=220 MeV; calculated proton yield ratio. Ni(π+, p), E=160 MeV; calculated σ(Ep, θp); deduced isobar intermediate state role. Intranuclear cascade model.

doi: 10.1103/PhysRevC.30.720
Citations: PlumX Metrics

1982BO32      Z.Phys. A308, 121 (1982)

H.G.Bohlen, M.R.Clover, G.Ingold, H.Lettau, W.von Oertzen

Observation of the Nuclear Rainbow Scattering for 12C + 12C at E(lab) = 300 MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=300 MeV; measured σ(θ), σ(E(12C)); deduced optical model, quadrupole deformation parameters, nuclear rainbow scattering. Optical model, coupled-channels analyses, folded potential.

doi: 10.1007/BF01413002
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1679.

1982GA23      Z.Phys. A309, 49 (1982)

A.Gamp, M.Burgel, M.R.Clover, Ch.Egelhaaf, H.Fuchs, B.Gebauer, H.Homeyer, W.Rauch, J.C.Jacmart

Fast Emission of α-Particles in Deep-Inelastic 36Ar + 197Au Collisions

NUCLEAR REACTIONS 197Au(40Ar, αX), E=380 MeV; measured σ(fragment θ, θα); deduced reaction mechanism.

doi: 10.1007/BF01420150
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1981GA19      Z.Phys. A300, 63 (1981)

A.Gamp, M.Burgel, M.R.Clover, C.Egelhaaf, H.Fuchs, B.Gebauer, H.Homeyer, J.C.Jacmart

Light Particle Emission in Quasi-Elastic Heavy-Ion Reactions

NUCLEAR REACTIONS 197Au(36Ar, αX), E=380 MeV; measured αX(θ), (fragment)α energy correlation; deduced reaction mechanism. Quasielastic heavy ion reaction.

doi: 10.1007/BF01412615
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1980BE02      Phys.Rev. C21, 167 (1980)

J.R.Beene, R.M.DeVries, D.Shapira, M.R.Clover

m-Substate Populations in Resonant Heavy-Ion Reactions

NUCLEAR REACTIONS 12C(16O, 12C), E=45-53 MeV; measured σ(E, θ, E(12C)). 12C level deduced spin alignment. 28Si resonances deduced J, π.

doi: 10.1103/PhysRevC.21.167
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1980OS01      Nucl.Phys. A342, 185 (1980)

R.Ost, A.J.Cole, M.R.Clover, B.R.Fulton, B.Sikora

Alpha-Heavy-Ion Angular Correlations from 28Si + 12C

NUCLEAR REACTIONS 12C(28Si, αX), E=87-91.5 MeV; measured σ(E, θ1, θ2), αX(θ) for X=Si, P, S, Cl. Statistical model calculation.

doi: 10.1016/0375-9474(80)90513-8
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1979CL02      J.Phys.(London) G5, L63 (1979)

M.R.Clover, B.R.Fulton, R.Ost, R.M.DeVries

Comparison of Entrance, Exit and Reaction Channel Data at Backward Angles for 28Si(12C, 16O)24Mg

NUCLEAR REACTIONS 28Si(12C, 16O), E(cm)=23.6-34.1 MeV; 24Mg(16O, 16O), E(cm)=21.4-30.7 MeV; measured σ(E, θ). 40Ca deduced no definite molecular resonances.

doi: 10.1088/0305-4616/5/4/004
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1979CL06      Phys.Rev.Lett. 43, 256 (1979)

M.R.Clover, T.M.Cormier, B.R.Fulton, B.J.Herman

Resonance in the Two-Nucleon Transfer Reaction 12C(12C, 10B)14N

NUCLEAR REACTIONS 12C(12C, 10B), E(cm)=22-42 MeV; measured σ(E, θ). 24Mg deduced resonances, J, π, reduced partial widths.

doi: 10.1103/PhysRevLett.43.256
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1979FO22      Phys.Lett. 89B, 48 (1979)

J.L.C.Ford, Jr., J.Gomez del Campo, D.Shapira, M.R.Clover, R.M.DeVries, B.R.Fulton, R.Ost, C.F.Maguire

Systematics of Back Angle 12C Scattering - The 12C + 20Ne and 12C + 24Mg Systems

NUCLEAR REACTIONS 12C(20Ne, 12C), E=55-80 MeV; 12C(24Mg, 12C), E(cm)=17-30 MeV; measured σ(E, θ). Legendre polynomial analysis.

doi: 10.1016/0370-2693(79)90073-X
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1979OS01      Phys.Rev. C19, 740 (1979)

R.Ost, M.R.Clover, R.M.DeVries, B.R.Fulton, H.E.Gove, N.J.Rust

Resonant Heavy-Ion Elastic Scattering from s-d Shell Model

NUCLEAR REACTIONS 12C(28Si, 28Si), (28Si, 28Si'), (32S, 32S), (32S, 32S'), (40Ca, 40Ca), (40Ca, 40Ca'), 9Be, 13C(28Si, 28Si), (28Si, 28Si'), E(cm)=20-30 MeV; measured σ(θ, E). 40Ca, 44Ti, 52Fe, 37Ar, 41Ca resonances deduced J, π. Legendre polynomial analysis.

doi: 10.1103/PhysRevC.19.740
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1978CL01      Phys.Lett. 72B, 427 (1978)

M.R.Clover, O.Zohni

Microscopic Folding-Type Estimates of Fusion Barriers in Heavy-Ion Collisions

NUCLEAR REACTIONS 12C(12C, X), E=126, 102.1 MeV; 12C(16O, X), E(cm)=72 MeV; 16O(16O, X), E=140.4 MeV; 28Si(12C, X), E=131.5, 186.4 MeV; 28Si(16O, X), E=142.5, 215.2 MeV; calculated potentials.

doi: 10.1016/0370-2693(78)90725-6
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1978CL02      Phys.Rev.Lett. 40, 1008 (1978)

M.R.Clover, R.M.DeVries, R.Ost, N.J.A.Rust, R.N.Cherry, Jr., H.E.Gove

Resonant Backward-Angle Heavy-Ion Elastic Scattering

NUCLEAR REACTIONS 13,12C(28Si, X), E(cm)=17.5-33 MeV; measured σ(θ). 9Be(28Si, X), E(cm)=24.3 MeV; measured σ.

doi: 10.1103/PhysRevLett.40.1008
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1978SH01      Phys.Rev.Lett. 40, 371 (1978)

D.Shapira, R.M.DeVries, M.R.Clover, R.N.Boyd, R.N.Cherry, Jr.

Possible Mechanism for the Resonances in the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, 16O'), E=50-70 MeV; measured σ(E, θ). 28Si deduced resonances, J, π.

doi: 10.1103/PhysRevLett.40.371
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1977DE12      Phys.Lett. 67B, 19 (1977)

R.M.DeVries, D.Shapira, M.R.Clover, H.E.Gove, J.D.Garrett, G.Sorensen

A Search for Alpha-Particle Vibrational States in 208Pb

NUCLEAR REACTIONS 204Hg(16O, 12C), E=88 MeV; measured σ(θ). 208Pb deduced levels, Γα.

doi: 10.1016/0370-2693(77)90793-6
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1977SH16      Phys.Lett. 71B, 293(1977)

D.Shapira, R.M.DeVries, M.R.Clover, R.N.Boyd, R.N.Cherry, Jr.

Spins of Resonances in the 12C+16O System

NUCLEAR REACTIONS 12C(16O, 16O'), E=52 MeV; measured σ(θ). 28Si resonances deduced J, π.

doi: 10.1016/0370-2693(77)90219-2
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1975DE10      Nucl.Phys. A243, 528 (1975)

R.M.DeVries, M.R.Clover

Coulomb Potentials in Heavy-Ion Interactions

NUCLEAR REACTIONS 208Pb(16O, 16O'); calculated point charge approximation for Coulomb potential.

doi: 10.1016/0375-9474(75)90294-8
Citations: PlumX Metrics

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