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NSR database version of May 10, 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
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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
Citations: PlumX Metrics


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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