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NSR database version of April 11, 2024.

Search: Author = D.H.Boal

Found 20 matches.

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1990BO02      Phys.Rev. C41, 118 (1990)

D.H.Boal, J.C.K.Wong

Computer Simulation of Reaction Plane Memory via Quasiparticle Dynamics

NUCLEAR REACTIONS 154Sm(14N, pX), (14N, tX), (14N, dX), E=35 MeV/nucleon; calculated light-, heavy fragment spectra, σ(E(X), θ). Reaction plane memory computer simulation.

doi: 10.1103/PhysRevC.41.118
Citations: PlumX Metrics

1990BO21      Phys.Rev. C42, R502 (1990)

D.H.Boal, J.N.Glosli

Fluctuation Growth and Spinodal Decomposition in Heavy Ion Reactions

NUCLEAR STRUCTURE 108Ag; calculated average central density time dependence, radial excitation trajectories. Liquid-vapor phase diagram, Hamiltonian-based model.

doi: 10.1103/PhysRevC.42.R502
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1989BO02      Phys.Rev.Lett. 62, 737 (1989)

D.H.Boal, J.N.Glosli, C.Wicentowich

Computer Simulation of Temperature Measurements in Heavy-Ion Collisions

NUCLEAR REACTIONS 40Ca(40Ca, X), E=100 MeV/nucleon; calculated emitted α kinetic, chemical temperature vs t.

doi: 10.1103/PhysRevLett.62.737
Citations: PlumX Metrics

1989BO59      Phys.Rev. C40, 610 (1989)

D.H.Boal, J.N.Glosli, C.Wicentowich

Temperatures in Heavy Ion Reactions: Simulation via quasiparticle dynamics

doi: 10.1103/PhysRevC.40.610
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1988BO01      Phys.Rev. C37, 91 (1988)

D.H.Boal, J.N.Glosli

From Binary Breakup to Multifragmentation: Computer simulation

NUCLEAR REACTIONS Ag(p, X), E=300 MeV; Ca(Ca, X), E=25, 50 MeV/nucleon; calculated nucleon spectra, σ(θ(N), E(N)). Semi-classical model, computer simulation.

doi: 10.1103/PhysRevC.37.91
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1988BO27      Phys.Rev. C38, 1870 (1988)

D.H.Boal, J.N.Glosli

Quasiparticle Model for Nuclear Dynamics Studies: Ground-state properties

NUCLEAR STRUCTURE A=2-197; calculated binding energy per nucleon, rms radius for select nuclei. Quasiparticle model.

doi: 10.1103/PhysRevC.38.1870
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1987PO03      Phys.Rev. C35, 1695 (1987)

J.Pochodzalla, C.K.Gelbke, W.G.Lynch, M.Maier, D.Ardouin, H.Delagrange, H.Doubre, C.Gregoire, A.Kyanowski, W.Mittig, A.Peghaire, J.Peter, F.Saint-Laurent, B.Zwieglinski, G.Bizard, F.Lefebvres, B.Tamain, J.Quebert, Y.P.Viyogi, W.A.Friedman, D.H.Boal

Two-Particle Correlations at Small Relative Momenta for 40Ar-Induced Reactions on 197Au at E/A = 60 MeV

NUCLEAR REACTIONS 197Au(40Ar, X), E=60 MeV/nucleon; measured σ(fragment E, θ) for X=p, d, t, α, pp-, pt-, p3He-, dt-, pα-, tα-, dα-, 3Heα-, αα-, p7Li-, α7Li-, pd-, dd-, tt-, t3He-correlation functions, coincidence yields, spectra; deduced source radii. ΔE-E telscopes, NaI scintillator. Statistical model.

doi: 10.1103/PhysRevC.35.1695
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1986BO01      Phys.Rev. C33, 549 (1986)

D.H.Boal, J.C.Shillcock

Nuclear Interferometry and Thermal Freeze Out

NUCLEAR REACTIONS 197Au(16O, 2pX), E=400 MeV; calculated pp-correlation function. Nuclear interferometry, thermal freeze out.

doi: 10.1103/PhysRevC.33.549
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1986CH10      Phys.Lett. 172B, 27 (1986)

C.B.Chitwood, C.K.Gelbke, J.Pochodzalla, Z.Chen, D.J.Fields, W.G.Lynch, R.Morse, M.B.Tsang, D.H.Boal, J.C.Shillcock

Energy Dependence of Source Radii and Emission Temperatures for 14N Induced Reactions at E/A = 35 MeV

NUCLEAR REACTIONS 197Au(14N, dα), E=35 MeV/nucleon; measured (αd) correlation function; deduced source radii, emission temperature kinetic energy dependence.

doi: 10.1016/0370-2693(86)90210-8
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1986JE01      Phys.Rev. C33, 1303 (1986)

B.K.Jennings, D.H.Boal, J.C.Shillcock

Two-Particle Correlation Functions in the Thermal Model and Nuclear Interferometry Descriptions

NUCLEAR REACTIONS 2H(p, p), E not given; analyzed phase shifts data; deduced potential parameters, pd-correlation function nuclear term dependence. Thermal model, nuclear interferometry descriptions.

doi: 10.1103/PhysRevC.33.1303
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1986PO07      Phys.Lett. 174B, 36 (1986)

J.Pochodzalla, C.B.Chitwood, D.J.Fields, C.K.Gelbke, W.G.Lynch, M.B.Tsang, D.H.Boal, J.C.Shillcock

Two-Particle Correlations at Small Relative Momenta for 14N Induced Reactions on 197Au at E/A = 35 MeV

NUCLEAR REACTIONS 197Au(14N, X), E=35 MeV/nucleon; measured pp(θ), dd(θ), tt(θ), pα(θ), dα(θ); deduced emission source radii.

doi: 10.1016/0370-2693(86)91124-X
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1985CH02      Phys.Rev.Lett. 54, 302 (1985)

C.B.Chitwood, J.Aichelin, D.H.Boal, G.Bertsch, D.J.Fields, C.K.Gelbke, W.G.Lynch, M.B.Tsang, J.C.Shillcock, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson, G.R.Young

Final-State Interactions between Noncompound Light Particles for 16O-Induced Reactions on 197Au at E/A = 25 MeV

NUCLEAR REACTIONS 197Au(16O, 2d), (16O, 2t), (16O, 2p), E=25 MeV/nucleon; measured (particle-particle) correlation function; deduced final state interactions role.

doi: 10.1103/PhysRevLett.54.302
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1984BO07      Phys.Rev. C29, 973 (1984)

D.H.Boal, J.H.Reid

Thermal Equilibrium in Proton Induced Reactions

NUCLEAR REACTIONS 9Be(p, 2p), E=70-170 MeV; calculated differential multiplicity vs E. 238U(p, p'), E=1.041 GeV; calculated Lorentz invariant σ. Thermal model.

doi: 10.1103/PhysRevC.29.973
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1984BO23      Phys.Rev. C30, 119 (1984)


Experimental Signature Ambiguities in Nuclear Liquid-Gas Phase Transitions

NUCLEAR REACTIONS Ag(p, X), E=480 MeV; calculated fragment temperature vs mass. Ag(p, 7Be), (p, 7Li), E=480 MeV; calculated σ(fragment θ, E).

doi: 10.1103/PhysRevC.30.119
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1984BO34      Phys.Rev. C30, 749 (1984)


Hadronic Thermometry and Final State Interactions

NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; calculated production σ, excited to ground state population ratios for X=7,6Li, 7Be. Expanding fire ball, final state interactions.

doi: 10.1103/PhysRevC.30.749
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1983GR21      Nucl.Phys. A405, 463 (1983)

R.E.L.Green, D.H.Boal, R.L.Helmer, K.P.Jackson, R.G.Korteling

Large-Angle Proton Emission in the 9Be(p, 2p) Reaction at 300 MeV

NUCLEAR REACTIONS Be(p, pX), (p, 2pX), E=300 MeV; measured σ(E(p), θ(p)), σ(E1, θ1, E2, θ2=90°), pp-coin. Comparison with phase-space, direct knockout calculations.

doi: 10.1016/0375-9474(83)90515-8
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1981BO18      Phys.Rev. C23, 2788 (1981)

D.H.Boal, R.E.L.Green, R.G.Korteling, M.Soroushian

Tests of Models for Inclusive Production of Energetic Light Fragments at Intermediate Energies

NUCLEAR REACTIONS Ag(p, α), (p, 12C), (p, 16O), E=480 MeV; calculated σ(θα, Eα), σ(θ(12C), E(12C)), σ(θ(16O), E(16O)). Statistical, coalescence, knockout models.

doi: 10.1103/PhysRevC.23.2788
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1981RO03      Phys.Rev. C23, 1671 (1981)

G.Roy, L.G.Greeniaus, G.A.Moss, D.A.Hutcheon, R.Liljestrand, R.M.Woloshyn, D.H.Boal, A.W.Stetz, K.Aniol, A.Willis, N.Willis, R.McCamis

Inclusive Scattering of Protons on Helium, Nickel, and Tantalum at 500 MeV

NUCLEAR REACTIONS 4He, Ni, 181Ta(polarized p, p), E=500 MeV; measured inclusive σ(Ep, θ), analyzing power vs Ep, θ; deduced reaction mechanism. Knockout model.

doi: 10.1103/PhysRevC.23.1671
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0146.

1980BO12      Phys.Rev. C21, 1913 (1980)


Probing Inclusive Production Mechanisms with the (p, 2p) Reaction

NUCLEAR REACTIONS 6Li, 9Be, 181Ta(p, p'), E=800 MeV; analyzed data. 9Be(p, 2p), E=800 MeV; calculated σ; deduced inclusive production mechanisms. Direct knockout, multiple particle exchange, correlated cluster, cluster recoil models.

doi: 10.1103/PhysRevC.21.1913
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1979BO27      Phys.Rev. C20, 1878 (1979)

D.H.Boal, R.M.Woloshyn

Direct Knockout Model for Nuclear Fragmentaion

NUCLEAR REACTIONS 9Be, 27Al, Ag(p, α), (p, pα), E=300 MeV; calculated double differential σ. Direct knockout model.

doi: 10.1103/PhysRevC.20.1878
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