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NSR database version of April 26, 2024.

Search: Author = J.D.Molitoris

Found 15 matches.

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1994DE17      Phys.Rev. C50, R541 (1994)

P.V.Degtyarenko, J.Button-Shafer, L.Elouadrhiri, R.A.Miskimen, G.A.Peterson, K.Wang, V.B.Gavrilov, M.V.Kossov, G.A.Leksin, S.M.Shuvalov, F.S.Dietrich, S.O.Melnikoff, J.D.Molitoris, K.Van Bibber

Multiple Hadron Production by 14.5 GeV Electron and Positron Scattering from Nuclear Targets

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁰Ar(e, e'2p), E=14.5 GeV; measured secondary protons, pions differential multiplicities; deduced spectra phenomenological parameters, their dependence on ν, Q². Deep inelastic nuclear reactions.

doi: 10.1103/PhysRevC.50.R541
Citations: PlumX Metrics

1994EL13      Phys.Rev. C50, R2266 (1994)

L.Elouadrhiri, R.A.Miskimen, J.Button-Shafer, P.Degtyarenko, G.A.Peterson, S.Shuvalov, K.Wang, V.Gavrilov, F.S.Dietrich, S.O.Melnikoff, J.D.Molitoris, K.Van Bibber

Measurements of the (e, e'pπ^-) Reaction on Nuclei in the Nucleon Resonance Region

NUCLEAR REACTIONS ²H, C, O, Ar, Xe(e, e'pπ^-), E=14.5 GeV; measured missing transverse momentum distribution, other aspects; deduced resonance beyond Δ(1232). DWIA analysis.

doi: 10.1103/PhysRevC.50.R2266
Citations: PlumX Metrics

1993MO03      Phys.Rev.Lett. 70, 537 (1993)

J.D.Molitoris, W.E.Meyerhof, Ch.Stoller, R.Anholt, D.W.Spooner, L.G.Moretto, L.G.Sobotka, R.J.McDonald, G.J.Wozniak, M.A.McMahan, L.Blumenfeld, N.Colonna, M.Nessi, E.Morenzoni

Molecular-Orbital Study of Late-Fission Times in Deep-Inelastic ²³⁸U + ²³⁸U Collisions

NUCLEAR REACTIONS ²³⁸U(²³⁸U, X), (²³⁸U, F), E=7.5 MeV/nucleon; measured K-vacancy production probability for no-fission, single-, double fission channels; deduced U-like products late fission time scales.

doi: 10.1103/PhysRevLett.70.537
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1991DA17      Phys.Rev. C44, 2584 (1991)

K.Danzmann, W.E.Meyerhof, A.Belkacem, E.C.Montenegro, E.Dillard, H.P.Hulskotter, N.Guardala, D.W.Spooner, B.Kotlinski, D.Cline, A.Kavka, C.W.Beausang, J.Burde, R.J.McDonald, A.O.Macchiavelli, B.S.Rude, J.D.Molitoris

Search for Narrow-Peak Structure in the Three-Photon Spectrum from 6-MeV/Nucleon U + Th, U + U, and Th + Th Collisions

NUCLEAR REACTIONS Th(Th, X), E=5.75 MeV/nucleon; U(U, X), E=5.95 MeV/nucleon; Th(U, X), E=6.05 MeV/nucleon; measured three-photon production σ upper limit.

doi: 10.1103/PhysRevC.44.2584
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1987NE06      Phys.Rev. C36, 143 (1987)

M.Nessi, Ch.Stoller, E.Morenzoni, W.Wolfli, W.E.Meyerhof, J.D.Molitoris, E.Grosse, Ch.Michel

Time Delay Effects on K X-Ray Production Probability in Deep Inelastic U + U and U + Pb Nuclear Reactions

ATOMIC PHYSICS ²⁰⁸Pb, ²³⁸U(²³⁸U, X), E=7.5 MeV/nucleon; measured E(K X-ray), I(K X-ray); deduced time delay, inner shell ionization probability.

doi: 10.1103/PhysRevC.36.143
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1986ME12      Phys.Rev.Lett. 57, 2139 (1986)

W.E.Meyerhof, J.D.Molitoris, K.Danzmann, D.W.Spooner, F.S.Stephens, R.M.Diamond, E.-M.Beck, A.Schafer, B.Muller

Search for Correlated Narrow-Peak Structure in the Two-Photon Spectrum from 6-MeV/Nucleon U + Th Collisions

NUCLEAR REACTIONS Th(U, xγ), E=6 MeV/nucleon; measured two-photon correlated spectra; deduced two-photon production σ. Ge(Li) pair detectors.

doi: 10.1103/PhysRevLett.57.2139
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1986MO04      Z.Phys. A323, 127 (1986)

J.D.Molitoris, R.Anholt, W.E.Meyerhof, O.K.Baker, S.Andriamonje, E.Morenzoni

K-Vacancy Production in High-Energy U + U and U + Pb Collisions at Small Impact Parameters

NUCLEAR REACTIONS ²³⁸U, ²⁰⁸Pb(²³⁸U, X), E=4.6, 5.8, 7.3 MeV/nucleon; measured E X-ray, I X-ray. ²³⁸U, ²⁰⁸Pb deduced K-vacancy production probabilities.

1986MO29      Z.Phys. D2, 91 (1986)

J.D.Molitoris, Ch.Stoller, R.Anholt, W.E.Meyerhof, D.W.Spooner, R.J.McDonald, L.G.Sobotka, G.J.Wozniak, L.G.Moretto, M.A.McMahan, E.Morenzoni, M.Nessi, W.Wolfli

K-Shell Ionization in 7.5- and 8.6-MeV/a.m.u. U + U Collisions at Very Small Impact Parameters

NUCLEAR REACTIONS ²³⁸U(²³⁸U, X), E=7.5, 8.6 MeV/nucleon; measured X-ray spectra; deduced K-vacancy production probability.

doi: 10.1007/BF01438230
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1984ST19      Phys.Rev.Lett. 53, 1329 (1984)

Ch.Stoller, M.Nessi, E.Morenzoni, W.Wolfli, W.E.Meyerhof, J.D.Molitoris, E.Grosse, Ch.Michel

Nuclear Reaction Times in the Deep-Inelastic U + U Collision deduced from K-Shell Ionization Proabilities

NUCLEAR REACTIONS U(U, X), E=7.5 MeV/nucleon; measured K-shell ionization probability.

doi: 10.1103/PhysRevLett.53.1329
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1983CH41      Phys.Lett. 130B, 246 (1983)

J.F.Chemin, S.Andriamonje, E.Morenzoni, Ch.Stoller, R.Anholt, W.E.Meyerhof, O.K.Baker, J.D.Molitoris

Compound Elastic Cross Sections in the Isobaric Analog Resonances ⁸⁸Sr(p, p₀) at 5.06 MeV and ⁸⁶Sr(p, p₀) at 6.02 MeV

NUCLEAR REACTIONS ⁸⁸Sr(p, p), E=5-5.2 MeV; ⁸⁶Sr(p, p), E=5.95-6.1 MeV; measured σ(θ), K-shell ionization probability vs E in IAR region. ^89,87Y deduced IAR compound elastic contribution.

doi: 10.1016/0370-2693(83)91134-6
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1982AN14      Z.Phys. A308, 189 (1982)

R.Anholt, W.E.Meyerhof, J.D.Molitoris, Xu Jun-Shan

Pb K-Shell Ionization Probability in High-Energy Xe + Pb Collisions

ATOMIC PHYSICS Pb(Xe, X), E=5.9, 7.2, 8.5 MeV/nucleon; measured K-shell ionization probability.

doi: 10.1007/BF01418279
Citations: PlumX Metrics

1982BE06      Phys.Rev. C25, 837 (1982)

M.Beckerman, M.Salomaa, A.Sperduto, J.D.Molitoris, A.DiRienzo

Sub-Barrier Fusion of ^58,64Ni with ⁶⁴Ni and ⁷⁴Ge

NUCLEAR REACTIONS ⁶⁴Ni, ⁷⁴Ge(⁵⁸Ni, X), (⁶⁴Ni, X), E=171-215 MeV; measured σ(evaporation residue θ) vs E; deduced fusion process dynamics. Complete fusion, barrier penetration analysis.

doi: 10.1103/PhysRevC.25.837
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1982CH24      Phys.Rev. A26, 1239 (1982)

J.-F.Chemin, W.E.Meyerhof, R.Anholt, J.D.Molitoris, Ch.Stoller

Measurement of the K-Shell Ionization Probability across a Wide Resonance: ⁸⁸Sr(p, p₀) at 6.06 MeV

NUCLEAR REACTIONS ⁸⁸Sr(p, p), E=6.06 MeV; measured σ(θ), K-shell ionization probability vs E; deduced nuclear resonance role in ionization probability time delay. Blair-Anholt theory.

doi: 10.1103/PhysRevA.26.1239
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1981BE14      Phys.Rev. C23, 1581 (1981)

M.Beckerman, J.Ball, H.Enge, M.Salomaa, A.Sperduto, S.Gazes, A.DiRienzo, J.D.Molitoris

Near- and Sub-Barrier Fusion of ⁵⁸Ni with ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, X), E=187.6-220 MeV; measured σ(evaporation residue θ, E), σ(fusion) vs E. Standard barrier penetration models.

doi: 10.1103/PhysRevC.23.1581
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1980BE37      Phys.Rev.Lett. 45, 1472 (1980)

M.Beckerman, M.Salomaa, A.Sperduto, H.Enge, J.Ball, A.DiRienzo, S.Gazes, Y.Chen, J.D.Molitoris, M.Nai-Feng

Dynamic Influence of Valence Neutrons upon the Complete Fusion of Massive Nuclei

NUCLEAR REACTIONS ^58,64Ni(⁵⁸Ni, X), ⁶⁴Ni(⁶⁴Ni, X), E(cm)=90-110 MeV; measured complete σ(E, fusion); deduced valence neutron effects. Generalized liquid drop model.

doi: 10.1103/PhysRevLett.45.1472
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