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NSR database version of March 21, 2024.

Search: Author = J.D.Silk

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1997BB09      Hyperfine Interactions 107, 283 (1997)

B.Balko, I.W.Kay, J.Nicoll, J.D.Silk, G.Herling

Inhomogeneous and Homogeneous Broadening Effects on Nuclear Resonance Experiments

doi: 10.1023/A:1012036629223
Citations: PlumX Metrics


1996LA04      Phys.Rev. C53, 1167 (1996)

C.M.Laymon, W.Amos, M.G.Burlein, H.T.Fortune, T.Ekenberg, A.Kotwal, J.M.O'Donnell, J.D.Silk, J.D.Zumbro, C.L.Morris, S.J.Seestrom, K.S.Dhuga, R.Garnett, M.W.Rawool-Sullivan, C.F.Moore, S.L.Morris, D.L.Watson

Pion Elastic and Inelastic 2+1 Scattering on 58,60,62,64Ni at T(π) = 180 MeV

NUCLEAR REACTIONS 58,60,62,64Ni(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ); deduced nucleon radii, deformation parameters. 58,60,62,64Ni levels deduced neutron, proton matrix elements.

doi: 10.1103/PhysRevC.53.1167
Citations: PlumX Metrics


1995BU01      Phys.Rev. C51, 88 (1995)

M.Burlein, H.T.Fortune, W.M.Amos, T.L.Ekenberg, A.Kotwal, P.H.Kutt, J.M.O'Donnell, J.D.Silk, B.Boyer, A.Fuentes, K.Johnson, C.F.Moore, S.H.Yoo, S.Mordechai, C.L.Morris, J.D.Zumbro, D.L.Watson, K.S.Dhuga

Pion Inelastic Scattering to Low-Lying Positive-Parity States in 20Ne

NUCLEAR REACTIONS 20Ne(π+, π+'), E=120, 180 MeV; 20Ne(π-, π-'), E=180 MeV; measured σ(θ). Coupled-channels analysis.

doi: 10.1103/PhysRevC.51.88
Citations: PlumX Metrics


1995SI01      Phys.Rev. C51, 665 (1995)

J.D.Silk, M.Burlein, H.T.Fortune, E.Insko, M.Kagarlis, P.H.Kutt, J.M.O'Donnell, J.D.Zumbro, J.A.Faucett, R.Garnett, M.W.Rawool-Sullivan, C.L.Morris, S.Saini

Nonanalog 40,44Ca(π+, π-)40,44Ti(g.s.) Reactions at Low Energy

NUCLEAR REACTIONS 40,44Ca(π+, π-), E=32-79.26 MeV; measured σ(θ); deduced core polarization, cross shell transitions role.

doi: 10.1103/PhysRevC.51.665
Citations: PlumX Metrics


1994FO07      Phys.Rev. C50, 306 (1994)

H.T.Fortune, G.B.Liu, J.M.O'Donnell, J.D.Silk, S.Mordechai

Energy Dependence of 58Ni(π+, π-)58Zn Double Charge Exchange

NUCLEAR REACTIONS 58Ni(π+, π-), E=120-292 MeV; measured σ(θ, E(π)); deduced double charge exchange σ.

doi: 10.1103/PhysRevC.50.306
Citations: PlumX Metrics


1993BE02      Phys.Rev. C47, 140 (1993)

D.R.Benton, H.T.Fortune, J.M.O'Donnell, R.Crittenden, M.McKinzie, E.Insko, R.Ivie, D.Smith, J.D.Silk

Pion Double Charge Exchange on Nickel Isotopes and Generalized Seniority

NUCLEAR REACTIONS 60,62,64Ni, Ni(π+, π-), E=293.4 MeV; measured σ(θ). Model comparison.

doi: 10.1103/PhysRevC.47.140
Citations: PlumX Metrics


1993HY01      Phys.Rev. C47, 1184 (1993)

S.D.Hyman, D.J.Mack, P.G.Roos, H.Breuer, N.S.Chant, F.Khazaie, B.G.Ritchie, J.D.Silk, G.S.Kyle, P.A.Amaudruz, Th.S.Bauer, C.H.Q.Ingram, D.Renker, R.A.Schumacher, U.Sennhauser, W.J.Burger

Energy Dependence of Two-Nucleon Pion Absorption on 16O

NUCLEAR REACTIONS 16O(π+, pX), (π+, 2p), E=115, 165 MeV; measured σ(θ) vs proton momentum; deduced two-nucleon absorption σ, final state interactions role.

doi: 10.1103/PhysRevC.47.1184
Citations: PlumX Metrics


1993SM01      Phys.Rev. C47, 1053 (1993)

D.A.Smith, H.T.Fortune, J.M.O'Donnell, J.D.Silk, B.Gluckman, R.Crittenden, N.Claytor, C.L.Morris, J.A.McGill

Pion Double Charge Exchange on 56Fe at T(π) = 400 MeV

NUCLEAR REACTIONS 56Fe(π+, π-), E=400 MeV; measured σ(θ). 56Ni deduced double dipole resonance components J, π, excitation σ.

doi: 10.1103/PhysRevC.47.1053
Citations: PlumX Metrics


1992GA02      Phys.Rev. C45, 780 (1992)

G.Garino, M.Saber, R.E.Segel, D.F.Geesaman, R.Gilman, M.C.Green, R.J.Holt, J.P.Schiffer, B.Zeidman, E.J.Beise, G.W.Dodson, S.Hoibraten, L.D.Pham, R.P.Redwine, W.W.Sapp, C.F.Williamson, S.A.Wood, N.S.Chant, P.G.Roos, J.D.Silk, M.Deady, X.K.Maruyama

Proton Propagation in Nuclei Studied in the (e, e'p) Reaction

NUCLEAR REACTIONS 12C, 27Al, 58Ni, 181Ta(e, e'p), E=779.5 MeV; measured σ(θ(e), θp) vs missing energy; deduced transmission, medium effects role. PWIA.

doi: 10.1103/PhysRevC.45.780
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1992MA09      Phys.Rev. C45, 1767 (1992)

D.J.Mack, P.G.Roos, H.Breuer, N.S.Chant, S.D.Hyman, F.Khazaie, B.G.Ritchie, J.D.Silk, G.S.Kyle, P.A.Amaudruz, Th.S.Bauer, C.H.Q.Ingram, D.Renker, R.A.Schumacher, U.Sennhauser, W.J.Burger

Dominance of the Two-Nucleon Mechanism in 16O(π, pp) at 115 MeV

NUCLEAR REACTIONS 16O(π+, 2p), E=115 MeV; measured σ(E1, θ1, E2, θ2); deduced two-nucleon absorption σ. DWIA analysis.

doi: 10.1103/PhysRevC.45.1767
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1992OD01      Phys.Rev. C46, 2259 (1992)

J.M.O'Donnell, H.T.Fortune, J.D.Silk, S.Mordechai, C.L.Morris, J.D.Zumbro, S.H.Yoo, C.F.Moore

T = 13 Double Isobaric Analog State in 138Ce via Pion-Induced Double Charge Exchange

NUCLEAR REACTIONS 138Ba(π+, π-), E=292 MeV; measured pion spectra, σ(θ); deduced Q. 138Ce deduced double IAS excitation. Systematics, isobaric multiplet mass equation comparisons.

doi: 10.1103/PhysRevC.46.2259
Citations: PlumX Metrics


1991WA04      Phys.Rev. C43, 1318 (1991)

D.L.Watson, R.Gilman, C.L.Morris, J.D.Zumbro, S.Mordechai, M.Burlein, J.M.O'Donnell, H.T.Fortune, A.Kotwal, J.Puttz, J.D.Silk, J.S.McDonald, C.F.Moore, A.L.Williams, S.Y.Yoo

Pion-Induced Double Charge Exchange on 12C, 24Mg, 32S, and 40Ca

NUCLEAR REACTIONS 12C, 24Mg, 32S, 40Ca(π+, π-), E=164 MeV; measured σ(θ). Isobar-nucleon interaction mechanism.

doi: 10.1103/PhysRevC.43.1318
Citations: PlumX Metrics


1990BU08      Phys.Rev. C41, 2215 (1990)

W.J.Burger, E.Beise, S.Gilad, R.P.Redwine, P.G.Roos, N.S.Chant, H.Breuer, G.Ciangaru, J.D.Silk, G.S.Blanpied, B.M.Preedom, B.G.Ritchie, M.Blecher, K.Gotow, D.M.Lee, H.Ziock

Reaction 58Ni(π+, pp) at Tπ+ = 160 MeV

NUCLEAR REACTIONS 58Ni(π+, 2p), E=160 MeV; 58Ni(π-, 2p), E not given; measured σ(θ1, θ2); deduced pion absorption mechanism.

doi: 10.1103/PhysRevC.41.2215
Citations: PlumX Metrics


1990HY01      Phys.Rev. C41, R409 (1990)

S.D.Hyman, D.J.Mack, H.Breuer, N.S.Chant, F.Khazaie, B.G.Ritchie, P.G.Roos, J.D.Silk, P.-A.Amaudruz, Th.S.Bauer, C.H.Q.Ingram, G.S.Kyle, D.Renker, R.A.Schumacher, U.Sennhauser, W.J.Burger

16O(π+, 2p) Reaction at 165 MeV

NUCLEAR REACTIONS 16O(π+, 2p), E=165 MeV; measured σ(θp1, θp2, Ep1, Ep2), pp-coin; deduced total absorption σ. DWIA, phase space analyses.

doi: 10.1103/PhysRevC.41.R409
Citations: PlumX Metrics


1989BU14      Phys.Rev. C40, 785 (1989)

M.Burlein, H.T.Fortune, W.M.Amos, T.L.Ekenberg, A.Kotwal, P.H.Kutt, J.M.O'Donnell, J.D.Silk, B.Boyer, A.Fuentes, K.Johnson, C.F.Moore, S.H.Yoo, S.Mordechai, J.D.Zumbro, D.L.Watson, K.S.Dhuga

Pion Inelastic Scattering to the Low-Lying Broad 2+ in 20Ne

NUCLEAR REACTIONS 20Ne(π+, π+'), E=120, 180 MeV; 20Ne(π-, π-'), E=180 MeV; measured σ(θ), σ(E(π')). 20Ne deduced resonances, J, π, Γ.

doi: 10.1103/PhysRevC.40.785
Citations: PlumX Metrics


1989GE04      Phys.Rev.Lett. 63, 734 (1989)

D.F.Geesaman, R.Gilman, M.C.Green, R.J.Holt, J.P.Schiffer, B.Zeidman, G.Garino, M.Saber, R.E.Segel, E.J.Beise, G.W.Dodson, S.Hoibraten, D.L.Pham, R.P.Redwine, W.W.Sapp, C.F.Williamson, S.A.Wood, N.S.Chant, P.G.Roos, J.D.Silk, M.Deady, X.K.Maruyama

Proton Propagation in Nuclei Studied in the A Dependence of the (e, e'p) Reaction in the Quasifree Region

NUCLEAR REACTIONS 12C, 27Al, 58Ni, 181Ta(e, e'p), E=780 MeV; measured σ(θ(e'), θp) vs missing energy; deduced proton mean free path.

doi: 10.1103/PhysRevLett.63.734
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1989WI02      Phys.Lett. 216B, 11 (1989)

A.L.Williams, L.Agnew, L.G.Atencio, H.W.Baer, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, G.S.Kyle, J.A.McGill, C.F.Moore, C.L.Morris, S.Mordechai, J.M.O'Donnell, M.W.Rawool, S.Schilling, J.D.Silk, J.D.Zumbro

Pion Double Charge Exchange Above the Δ(1232) Resonance

NUCLEAR REACTIONS 14C, 18O(π+, π-), E=300, 400, 500 MeV; measured σ(E(π), θ(π)). 14N, 18Ne deduced double IAS excitation.

doi: 10.1016/0370-2693(89)91360-9
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1988MO15      Phys.Rev.Lett. 61, 531 (1988)

S.Mordechai, N.Auerbach, M.Burlein, H.T.Fortune, S.J.Greene, C.F.Moore, C.L.Morris, J.M.O'Donnell, M.W.Rawool, J.D.Silk, D.L.Watson, S.H.Yoo, J.D.Zumbro

Pion Double Charge Exchange to the Double Dipole Resonance

NUCLEAR REACTIONS 32S(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 32Ar deduced resonances, Γ.

doi: 10.1103/PhysRevLett.61.531
Citations: PlumX Metrics


1988SC14      Phys.Rev. C38, 2205 (1988)

R.A.Schumacher, P.A.Amaudruz, C.H.Q.Ingram, U.Sennhauser, H.Breuer, N.S.Chant, A.E.Feldman, B.S.Flanders, F.Khazaie, D.J.Mack, P.G.Roos, J.D.Silk, G.S.Kyle

Exclusive Quasi-Deuteron Absorption of Pions in 16O and 18O at 116 MeV

NUCLEAR REACTIONS 18,16O(π+, 2p), E=116 MeV; measured σ(E(2p)), σ(θ1, θ2), σ(θ1, θ2, E1); deduced reaction mechanism.

doi: 10.1103/PhysRevC.38.2205
Citations: PlumX Metrics


1988SI01      Phys.Rev. C37, 158 (1988)

J.D.Silk, H.D.Holmgren, D.L.Hendrie, T.J.M.Symons, G.D.Westfall, P.H.Stelson, S.Raman, R.L.Auble, J.R.Wu, K.Van Bibber

Fragmentation of 16O Projectiles at 100 MeV per Nucleon

NUCLEAR REACTIONS 27Al(16O, 12CX), E=100 MeV/nucleon; measured invariant σ vs rapidity. 27Al(16O, X), E=100 MeV/nucleon; measured σ(fragment θ), σ vs fragment mass for X=7,9,10Be, 10,11,12B, 10,11,12,13,14C, 13,14,15N; deduced reaction mechanism.

doi: 10.1103/PhysRevC.37.158
Citations: PlumX Metrics


1986BU06      Phys.Rev.Lett. 57, 58 (1986)

W.J.Burger, E.Beise, S.Gilad, R.P.Redwine, P.G.Roos, N.S.Chant, H.Breuer, G.Ciangaru, J.D.Silk, G.S.Blanpied, B.M.Preedom, B.G.Ritchie, M.Blecher, K.Gotow, D.M.Lee, H.Ziock

Reaction 58Ni(π+, 2p) at 160 MeV

NUCLEAR REACTIONS 58Ni(π+, 2p), E=160 MeV; measured σ(θ1, θ2) vs excitation; deduced pion absorption mechanism.

doi: 10.1103/PhysRevLett.57.58
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1983AU06      Phys.Rev. C28, 1552 (1983)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, C.Y.Wong, D.L.Hendrie, H.D.Holmgren, J.D.Silk

Light Ion Emission from Reactions Induced by 0.8-2.4 GeV 16O Projectiles

NUCLEAR REACTIONS Ni(16O, X), E=0.8, 1.6, 2.4 GeV; Au(16O, X), E=1.6, 2.4 GeV; Al, Sn(16O, X), E=1.6 GeV; measured σ(E, θ) for X=p, d, t, 3He, 4He; deduced model parameters.

doi: 10.1103/PhysRevC.28.1552
Citations: PlumX Metrics


1983GU04      Phys.Rev. C27, 1521 (1983)

A.Guterman, G.Ciangaru, C.C.Chang, J.D.Silk, D.L.Hendrie, T.J.M.Symons, J.Mahoney

Giant Resonance Excitation in the 27Al(6Li, 6He)27Si Reaction at 93 MeV

NUCLEAR REACTIONS 27Al(6Li, 6He), E=93 MeV; measured σ(θ), σ(E(6He)). 27Si deduced levels, giant resonance multipolarity.

doi: 10.1103/PhysRevC.27.1521
Citations: PlumX Metrics


1982AU07      Phys.Rev.Lett. 49, 441 (1982)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, D.L.Hendrie, H.D.Holmgren, J.D.Silk, H.Breuer

Target-A Dependence of Light-Ion Emission from Reactions Induced by 100-MeV/u 16O

NUCLEAR REACTIONS Al, Ni, Sn, Au(16O, p), (16O, d), (16O, t), (16O, 3He), (16O, α), E=100 MeV/nucleon; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα), inclusive reactions; deduced reaction mechanism, moving source parameters, target mass effects.

doi: 10.1103/PhysRevLett.49.441
Citations: PlumX Metrics


1980CO19      Phys.Rev.Lett. 45, 1930 (1980)

A.A.Cowley, C.C.Chang, H.D.Holmgren, J.D.Silk, D.L.Hendrie, R.W.Koontz, P.G.Roos, C.Samanta, J.R.Wu

Energy Dissipation Process for 100-MeV Protons and the Nucleon-Nucleon Interactions in Nuclei

NUCLEAR REACTIONS 58Ni(p, 2p), E=100 MeV; measured pp-coin, σ(Ep1, Ep2, θ1, θ2); deduced reaction mechanism, energy dissipation process. DWIA analysis, quasifree scattering.

doi: 10.1103/PhysRevLett.45.1930
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