NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.J.Horen Found 155 matches. Showing 1 to 100. [Next]2001AU02 Phys.Rev. C63, 034322 (2001) S.M.Austin, E.Adamides, A.Galonsky, T.Nees, W.A.Sterrenburg, D.E.Bainum, J.Rapaport, E.Sugarbaker, C.C.Foster, C.D.Goodman, D.J.Horen, C.A.Goulding, M.B.Greenfield Splitting of the Dipole and Spin-Dipole Resonances NUCLEAR REACTIONS 90,92,94Zr(p, n), E=79.2, 119.4 MeV; measured σ(E, θ); deduced splitting between GDR and spin-dipole resonance. NUCLEAR STRUCTURE 90,92,94Zr, 112,116,124Sn, 208Pb; calculated resonance energies, dipole-spin-dipole splitting.
doi: 10.1103/PhysRevC.63.034322
1996BE02 Nucl.Phys. A596, 137 (1996) J.R.Beene, D.J.Horen, G.R.Satchler Critical Comparison of Folded Potential and Deformed Potential Models of Heavy-Ion Inelastic Scattering NUCLEAR REACTIONS 208Pb(17O, X), E=22, 84 MeV/nucleon; 208Pb(86Kr, X), E=43 MeV/nucleon; 90Zr(17O, X), E=84 MeV/nucleon; 208Pb(12C, X), E=8 MeV/nucleon; 90Zr(α, X), E=35.4 MeV; calculated σ ratio vs multipolarity. 208Pb(17O, 17O'), E=22 MeV/nucleon; analyzed σ(θ); deduced deformed, folded potentials critical comparison.
doi: 10.1016/0375-9474(95)00385-1
1996HO11 Nucl.Phys. A600, 193 (1996) D.J.Horen, G.R.Satchler, S.A.Fayans, E.L.Trykov Microscopic Description of the Excitation of Some States in the 90,92,94,96Zr Isotopes NUCLEAR STRUCTURE 90,92,94,96Zr; calculated neutron, proton transition densities, charge distributions. Realistic self-consistent finite Fermi systems. NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li'), E=70 MeV; 90,92,94,96Zr(α, α'), E=35.4 MeV; 90Zr(17O, 17O'), E=84 MeV/nucleon; analyzed σ(θ). Realistic self-consistent finite Fermi systems.
doi: 10.1016/0375-9474(96)00032-2
1995BE12 Phys.Lett. 344B, 67 (1995) J.R.Beene, D.J.Horen, G.R.Satchler On the ' Hindrance ' of 3- Excitations Induced by Nuclear Scattering NUCLEAR REACTIONS 60Ni, 90Zr, 120Sn, 208Pb(17O, 17O'), E=84 MeV/nucleon; calculated σ ratio, σ(θ), hadronic, hadronic+Coulomb excitation; deduced folding, deformed optical models comparison.
doi: 10.1016/0370-2693(94)01537-M
1995HO14 Phys.Rev. C52, 1554 (1995) D.J.Horen, J.R.Beene, G.R.Satchler Folded Potential Analysis of the Excitation of Giant Resonances by Heavy Ions NUCLEAR STRUCTURE 60Ni, 90Zr, 118,120,124Sn, 208Pb; calculated giant quadrupole resonance, B(λ), density distribution parameters, giant monopole resonance sum rule limits. Folded potential model. NUCLEAR REACTIONS 90Zr, 120Sn, 208Pb, 60Ni(17O, 17O'), E=84 MeV/nucleon; analyzed σ(θ) for giant resonance excitation. Folded potential model.
doi: 10.1103/PhysRevC.52.1554
1995LU01 Phys.Rev. C51, 635 (1995) B.J.Lund, N.P.T.Bateman, S.Utku, D.J.Horen, G.R.Satchler Isospin Character of Transitions to the 2+1 and 3-1 States of 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(α, α), (α, α'), E=35.4 MeV; measured σ(θ); deduced model parameters. 90,92,94,96Zr levels deduced B(λ), deformation length, transition densities, isospin mixing features. Deformed optical, folding model analyses.
doi: 10.1103/PhysRevC.51.635
1995TH03 Phys.Rev. C51, 3148 (1995) M.Thoennessen, E.Ramakrishnan, J.R.Beene, F.E.Bertrand, M.L.Halbert, D.J.Horen, P.E.Mueller, R.L.Varner Dynamical Effects in Fusion Reactions Forming 110Sn NUCLEAR REACTIONS 92Mo(18O, X), E=72 MeV; 60Ni(50Ti, X), E=163 MeV; measured Eγ, Iγ; deduced entrance channel effects, fusion reactions dissipation timescale. 110Sn deduced GDR decay features, Γ, time dependence of deformation, shape. Dissipative dynamics calculations.
doi: 10.1103/PhysRevC.51.3148
1993BE48 Phys.Rev. C48, 3128 (1993) J.R.Beene, D.J.Horen, G.R.Satchler Examination of Inconsistencies between the Deformed Potential Model and Folding Models for Analysis of Inelastic Hadron Scattering
doi: 10.1103/PhysRevC.48.3128
1993HO02 Phys.Rev. C47, 629 (1993) D.J.Horen, R.L.Auble, J.Gomez del Campo, G.R.Satchler, R.L.Varner, J.R.Beene, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen Systematics of Isospin Character of Transitions to the 2+1 and 3-1 States in 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li), (6Li, 6Li'), E=70 MeV; measured σ(θ); deduced model parameters. 90,92,94,96Zr levels deduced B(λ), neutron, proton matrix element ratio. Deformed optical model, folding model analyses.
doi: 10.1103/PhysRevC.47.629
1993HO12 Phys.Rev. C48, 433 (1993) D.J.Horen, R.L.Auble, C.Y.Wu, D.Cline, M.Devlin, R.Ibbotson, M.W.Simon Half-Life of the 2+1 State of 94Zr NUCLEAR REACTIONS 94Zr(32S, 32S'), E=105 MeV; measured γ(32S)-coin, recoil distance. 94Zr level deduced T1/2, B(λ).
doi: 10.1103/PhysRevC.48.433
1993HO19 Phys.Rev. C48, R2131 (1993) D.J.Horen, R.L.Auble, G.R.Satchler, J.R.Beene, I.Y.Lee, C.Y.Wu, D.Cline, M.Devlin, R.Ibbotson, M.W.Simon Lifetime of the 3-1 State and Octupole Collectivity in 96Zr NUCLEAR REACTIONS 96Zr(32S, 32S'), E=105; measured Eγ, Iγ, γ(32S)-coin. 96Zr(6Li, 6Li'), E=70 MeV; analyzed σ(θ). 96Zr level deduced T1/2, B(λ). Model comparisons.
doi: 10.1103/PhysRevC.48.R2131
1993HO22 Phys.Lett. 316B, 463 (1993) D.J.Horen, J.R.Beene, G.R.Satchler A Critique of the ' Implicit Folding Procedure ' for Analyzing Inelastic Hadron Scattering Measurements NUCLEAR STRUCTURE 208Pb, 86Kr, 90Zr; analyzed inelastic hadron scattering data analyses; deduced explicit folding procedure suitability.
doi: 10.1016/0370-2693(93)91028-L
1993TH02 Phys.Rev.Lett. 70, 4055 (1993) M.Thoennessen, J.R.Beene, F.E.Bertrand, C.Baktash, M.L.Halbert, D.J.Horen, D.G.Sarantites, W.Spang, D.W.Stracener Evidence for Long Formation Times of Near-Barrier Fusion Reactions NUCLEAR REACTIONS 148Sm(16O, X), E=82 MeV; 100Mo(64Ni, X), E=232 MeV; measured γ spectra, γ-multiplicity. 164Yb deduced excited state built GDR, widths, decay features.
doi: 10.1103/PhysRevLett.70.4055
1992CH33 Phys.Rev. C46, 1951 (1992) R.J.Charity, J.Barreto, L.G.Sobotka, D.G.Sarantites, D.W.Stracener, A.Chbihi, N.G.Nicolis, R.Auble, C.Baktash, J.R.Beene, F.Bertrand, M.Halbert, D.C.Hensley, D.J.Horen, C.Ludemann, M.Thoennessen, R.Varner Mechanism for the Disassembly of Excited 16O Projectiles into Four Alpha Particles NUCLEAR REACTIONS 159Tb(16O, 16O'X), E=25 MeV/nucleon; measured α-, light charged particle spectra; deduced projectile 4α-decay mechanism. 4π counter.
doi: 10.1103/PhysRevC.46.1951
1992HO08 Phys.Rev. C46, 499 (1992) D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.
doi: 10.1103/PhysRevC.46.499
1992HO12 Phys.Lett. 296B, 18 (1992) D.J.Horen, R.L.Auble, J.Gomez del Campo, R.L.Varner, J.R.Beene, G.R.Satchler, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen Different Effects of Valence Neutrons on the Isospin Character of Transitions to the First 2+ and 3- States of 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li'), E=70 MeV; measured σ(θ). 90,92,94,96Zr levels deduced neutron, proton matrix element ratio.
doi: 10.1016/0370-2693(92)90797-8
1992TH05 Phys.Lett. 282B, 288 (1992) M.Thoennessen, J.R.Beene, F.E.Bertrand, C.Baktash, M.L.Halbert, D.J.Horen, D.C.Hensley, D.G.Sarantites, W.Spang, D.W.Stracener, R.L.Varner Large Deformation in A ≈ 170 Nuclei at High Excitation Energies NUCLEAR REACTIONS 159Tb(16O, X), (16O, F), E=160 MeV; measured γ(evaporation residue)-, fission(fragment)γ-coin. 175Ta deduced GDR splitting, deformation.
doi: 10.1016/0370-2693(92)90640-P
1991HO13 Phys.Rev. C44, 128 (1991) D.J.Horen, R.L.Auble, J.R.Beene, F.E.Bertrand, M.L.Halbert, G.R.Satchler, M.Thoennessen, R.L.Varner, V.R.Brown, P.L.Anthony, V.A.Madsen Isospin Character of Transitions to Bound States in 204,206,208Pb using Inelastic Scattering of 17O Ions NUCLEAR REACTIONS 204,206,208Pb(17O, 17O'), E=375 MeV; measured σ(θ); deduced optical model parameters. 204,206,208Pb levels deduced B(λ), neutron, proton matrix element ratio. Enriched targets. DWBA analysis. NUCLEAR STRUCTURE 204,206,208Pb; calculated B(λ), neutron, proton matrix element ratio. RPA method.
doi: 10.1103/PhysRevC.44.128
1991HO20 Phys.Rev. C44, 2385 (1991) D.J.Horen, F.E.Bertrand, J.R.Beene, G.R.Satchler, W.Mittig, A.C.C.Villari, Y.Schutz, Z.Wenlong, E.Plagnol, A.Gillibert Isospin Character of the Giant Quadrupole Transition in 124Sn NUCLEAR REACTIONS 124Sn(17O, 17O'), E=1428 MeV; measured σ(E, θ); deduced optical model parameters. 124Sn deduced Mn/Mp for GQR, B(λ), giant monopole resonance. Enriched target, DWA analysis.
doi: 10.1103/PhysRevC.44.2385
1991RO05 Phys.Rev. C44, 2006 (1991) M.L.Roberts, P.D.Felsher, G.J.Weisel, Z.Chen, C.R.Howell, W.Tornow, R.L.Walter, D.J.Horen Measurement of A(y)(θ) for n + 208Pb from 6 to 10 MeV and the Neutron-Nucleus Interaction Over the Energy Range from Bound States at - 17 MeV Up to Scattering at 40 MeV NUCLEAR REACTIONS 208Pb(polarized n, n), (polarized n, n'), E=6-10 MeV; measured analyzing power vs E, θ, σ(θ); deduced optical model parameters. Hartree-Fock potential, dispersive terms of nuclear mean field, single-particle, single-hole energies.
doi: 10.1103/PhysRevC.44.2006
1991TH01 Phys.Rev. C43, R12 (1991) M.Thoennessen, J.R.Beene, F.E.Bertrand, D.J.Horen, M.L.Halbert, D.C.Hensley, J.E.Lisantti, W.Mittig, Y.Schutz, N.Alamanos, F.Auger, J.Barrette, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien, A.M.Nathan High-Energy Target Excitations in Heavy Ion Inelastic Scattering NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured γ(17O')-coin. 208Pb deduced GDR built on highly excited states.
doi: 10.1103/PhysRevC.43.R12
1990AU02 Phys.Rev. C41, 2620 (1990) R.L.Auble, J.R.Beene, F.E.Bertrand, J.L.Blankenship, D.J.Horen, J.Lisantti, R.L.Varner, A.D'Onofrio Excitation and Fission Decay of 238U Using the (17O, 17O') Reaction NUCLEAR REACTIONS 238U(17O, 17O'F), E=375 MeV; measured σ(θ), fission (fragment)17O'(θ). 238U deduced GQR resonance parameters, fission probability.
doi: 10.1103/PhysRevC.41.2620
1990BE03 Phys.Rev. C41, 920 (1990) J.R.Beene, F.E.Bertrand, D.J.Horen, R.L.Auble, B.L.Burks, J.Gomez del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien Heavy-Ion Coulomb Excitation and Photon Decay of the Giant Dipole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured σ(E(17O)), γ(particle)(θ, φ) following Coulomb excitation, σ(θ). 208Pb deduced giant resonance decay features, B(λ), M(n)/M(p).
doi: 10.1103/PhysRevC.41.920
1990BE08 Phys.Rev. C41, R1332 (1990) J.R.Beene, F.E.Bertrand, D.J.Horen, J.L.Lisantti, M.L.Halbert, D.C.Hensley, W.Mittig, Y.Schutz, J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, B.Haas, J.P.Vivien, A.M.Nathan Compound and Precompound Effects in Photon Decay of the Giant Dipole Resonance NUCLEAR REACTIONS 208Pb, 209Bi(17O, 17O'), E=84 MeV/nucleon; measured γ-spectra, γ yield vs excitation; deduced γ production σ vs excitation. 208Pb, 209Bi deduced GDR decay features.
doi: 10.1103/PhysRevC.41.R1332
1990HO20 Phys.Rev. C42, 2412 (1990) D.J.Horen, F.E.Bertrand, J.R.Beene, G.R.Satchler, W.Mittig, A.C.C.Villari, Y.Schutz, Z.Wenlong, E.Plagnol, A.Gillibert Isospin Character of the ' Isoscalar ' Giant Quadrupole Resonance in 118Sn NUCLEAR REACTIONS 118Sn(17O, 17O'), E=84 MeV/nucleon; measured σ(θ). 118Sn deduced resonances, J, π, neutron, proton matrix element ratio, B(λ), giant resonances Γ.
doi: 10.1103/PhysRevC.42.2412
1990RA08 Phys.Rev. C41, 1920 (1990) J.Rapaport, C.C.Foster, C.D.Goodman, C.A.Goulding, T.N.Taddeucci, D.J.Horen, E.R.Sugarbaker, C.Gaarde, J.Larsen, J.A.Carr, F.Petrovich, M.J.Threapleton (p, n) Reaction on Li Isotopes for E(p) = 60-200 MeV NUCLEAR REACTIONS 7,6Li(p, n), (polarized p, n), E=60-200 MeV; measured σ(θ). 6Be deduced Gamow-Teller transition strength. 7Be deduced branching ratio, Gamow-Teller transition strength. DWIA analysis.
doi: 10.1103/PhysRevC.41.1920
1990TA11 Phys.Rev. C41, 2548 (1990) T.N.Taddeucci, W.P.Alford, M.Barlett, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, C.A.Goulding, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker, C.A.Whitten, Jr. Zero-Degree Cross Sections for the 7Li(p, n)7Be(g.s.+0.43-MeV) Reaction in the Energy Range 80-795 MeV NUCLEAR REACTIONS 7Li(p, n), E=80-795 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.41.2548
1990TA15 Phys.Rev. C42, 935 (1990) T.N.Taddeucci, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, E.Sugarbaker, I.J.Van Heerden, C.A.Whitten, Jr. Gamow-Teller Transition Strengths from the 11B(p, n)11C Reaction in the Energy Range 160-795 MeV NUCLEAR REACTIONS 11B(p, n), E=160-795 MeV; measured σ(En, θ=0°). 11C levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.42.935
1989BE06 Phys.Rev. C39, 1307 (1989) J.R.Beene, F.E.Bertrand, M.L.Halbert, R.L.Auble, D.C.Hensley, D.J.Horen, R.L.Robinson, R.O.Sayer, T.P.Sjoreen Heavy-Ion Excitation and Photon Decay of Giant Resonances in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), E=381 MeV; measured σ(E(17O'), θ(17O')), γ-spectra, γγ(θ). 208Pb deduced giant resonances, decay, γ-branching, B(λ).
doi: 10.1103/PhysRevC.39.1307
1989BR03 Phys.Rev. C39, 725 (1989) A.Bracco, J.R.Beene, F.E.Bertrand, M.L.Halbert, D.C.Hensley, R.L.Auble, D.J.Horen, R.L.Robinson, R.O.Sayer Neutron Decay from the Giant Respnance Region in 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O'), E=378 MeV; measured γ-spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1103/PhysRevC.39.725
1989CH39 Nucl.Phys. A505, 670 (1989) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Xu, Z.Tang, D.M.Drake, I.Bergqvist, A.Brockstedt, J.Lisantti, F.Bertrand, D.J.Horen, K.Hicks, M.Vetterli, M.J.Iqbal Analyzing Powers and Cross Sections of Inclusive Polarized Proton Scattering on 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290, 500 MeV; measured σ(θ), analyzing power vs θ. DWBA, relativistic impulse approximation analyses.
doi: 10.1016/0375-9474(89)90037-7
1989HO11 Z.Phys. A333, 39 (1989) D.J.Horen, J.Lisantti, R.L.Auble, F.E.Bertrand, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson T = 1, Spin-Dipole Strength in 40Ca NUCLEAR REACTIONS 40Ca(p, p'), E=500 MeV; measured σ(θ), σ(Ep). 40Ca deduced T=1 spin-dipole transition strength distribution.
1989LI03 Phys.Rev. C39, 568 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Collective Model Distored-Wave Born Approximation Analysis of 500-MeV Proton Scattering form 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; analyzed σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca levels deduced deformation lengths, multipole matrix elements. Relativistic, non-relativistic DWBA analysis.
doi: 10.1103/PhysRevC.39.568
1989LI15 Phys.Rev. C40, 211 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Giant Resonance Strength Distribution in 40Ca from Inelastic Scattering of 500 MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; measured σ(θp, Ep), σ(θ). 40Ca deduced giant resonance strength distribution.
doi: 10.1103/PhysRevC.40.211
1989SW01 Phys.Rev. C40, 246 (1989) L.W.Swenson, X.Y.Chen, J.Lisantti, D.K.McDaniels, I.Bergqvist, F.E.Bertrand, D.J.Horen, E.E.Gross, C.Glover, R.O.Sayer, B.L.Burks, O.Hausser, K.Hicks, M.J.Iqbal Different Continuum Approaches to Giant Resonances in 208Pb with 400-MeV Protons NUCLEAR REACTIONS 208Pb(p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200 MeV; measured σ(θ). 208Pb deduced giant resonance L, Γ, EWSR. DWBA analysis, continuum models comparison.
doi: 10.1103/PhysRevC.40.246
1988BA39 Phys.Lett. 209B, 182 (1988) J.Barrette, N.Alamanos, F.Auger, B.Fernandez, A.Gillibert, D.J.Horen, J.R.Beene, F.E.Bertrand, R.L.Auble, B.L.Burks, J.Gomez Del Campo, M.L.Halbert, R.O.Sayer, W.Mittig, Y.Schutz, B.Haas, J.P.Vivien Coulomb Excitation of Giant Resonances in 208Pb by E = 84 MeV/Nucleon 17O Projectiles NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), E=1428 MeV; measured σ(θ). 208Pb deduced giant resonance excitation mechanism, B(λ), EWSR.
doi: 10.1016/0370-2693(88)90929-X
1988BE14 Nucl.Phys. A482, 287c (1988) F.E.Bertrand, J.R.Beene, D.J.Horen Heavy Ion Excitation of Giant Resonances - The Next Generation NUCLEAR REACTIONS 208Pb(17O, 17O'), E=22, 84 MeV/nucleon; measured σ(θ, E(17O)), σ(θ) following Coulomb excitation. 208Pb deduced giant resonance excitation.
doi: 10.1016/0375-9474(88)90591-X
1988BU15 Phys.Rev. C38, 1680 (1988) B.L.Burks, M.A.G.Fernandes, G.R.Satchler, D.J.Horen, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen Optical Model and Coupled-Channels Analyses of the Elastic and Inelastic Scattering of 18O from 28Si at 352 MeV NUCLEAR REACTIONS 28Si(18O, 18O), (18O, 18O'), E=351.7 MeV; measured σ(θ). Optical model, coupled-channels analyses.
doi: 10.1103/PhysRevC.38.1680
1988CH13 Phys.Lett. 205B, 436 (1988) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Tang, Z.Xu, D.M.Drake, I.Bergqvist, A.Brockstedt, F.E.Bertrand, D.J.Horen, J.Lisantti, K.Hicks, M.Vetterli, M.J.Iqbal Relativistic Medium Effects for 208Pb(p(pol), p') at Intermediate Energies NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290 MeV; measured σ(θp', Ep'), analyzing power vs θ; deduced relativistic medium effects.
doi: 10.1016/0370-2693(88)90973-2
1988HO04 Phys.Rev. C37, 888 (1988) D.J.Horen, J.R.Beene, F.E.Bertrand Comment on the Characterization of the Giant Quadrupole Resonance in 208Pb as Reported from π+/π- Scattering NUCLEAR REACTIONS 208Pb(17O, 17O'), E=1428 MeV; measured σ(θ). 208Pb deduced GQR B(E2), inconsistencies with excitation by pions.
doi: 10.1103/PhysRevC.37.888
1988LI18 Phys.Rev. C37, 2408 (1988) J.Lisantti, F.E.Bertrand, D.J.Horen, B.L.Burks, C.W.Glover, D.K.McDaniels, L.W.Swenson, X.Y.Chen, O.Hausser, K.Hicks Excitation of Giant Resonances in 28Si with 250 MeV Protons NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=250 MeV; measured σ(θ). 28Si deduced level deformation lengths, giant resonance EWSR.
doi: 10.1103/PhysRevC.37.2408
1988WA07 Nucl.Phys. A480, 285 (1988) D.Wang, J.Rapaport, D.J.Horen, B.A.Brown, C.Gaarde, C.D.Goodman, E.Sugarbaker, T.N.Taddeucci The 52, 54Cr(p, n)52, 54Mn and 57, 58Fe(p, n)57, 58Co Reactions at E(p) = 120 MeV NUCLEAR REACTIONS, MECPD 52,54Cr, 57,58Fe(p, n), E=120 MeV; measured σ(θ). 52,54Mn, 57,58Co deduced Gamow-Teller resonances, transition strengths. Enriched targets. DWIA analysis.
doi: 10.1016/0375-9474(88)90398-3
1987BE02 Phys.Rev. C35, 111 (1987) F.E.Bertrand, R.O.Sayer, R.L.Auble, M.Beckerman, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, J.Gomez del Campo, D.Shapira, H.P.Morsch Excitation of the High Energy Nuclear Continuum in 208Pb by 22 MeV/Nucleon 17O and 32S NUCLEAR REACTIONS 208Pb(17O, 17O'), (32S, 32S'), E=22 MeV/nucleon; measured σ(E(17O)), σ(E(32S)). Enriched targets, magnetic spectrograph.
doi: 10.1103/PhysRevC.35.111
1987BE23 Phys.Rev. C36, 657 (1987) M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, R.O.Sayer, G.R.Satchler, D.Shapira, Y.Sugiyama, R.L.Varner Elastic and Inelastic Scattering of 58Ni + 208Pb at Bombarding Energies from 598 to 1011 MeV NUCLEAR REACTIONS 208Pb(58Ni, 58Ni), (58Ni, 58Ni'), E=598-1011 MeV; measured σ(E), σ(θ). 208Pb, 58Ni levels deduced B(E2), Coulomb deformation constants. Optical model, DWBA, coupled-channels calculations.
doi: 10.1103/PhysRevC.36.657
1987FE04 Phys.Rev. C36, 108 (1987) M.A.G.Fernandes, F.E.Bertrand, R.L.Auble, R.O.Sayer, B.L.Burks, D.J.Horen, E.E.Gross, J.L.Blankenship, D.Shapira, M.Beckerman Single-Nucleon Transfer Reactions Induced by 376-MeV 17O on 208Pb NUCLEAR REACTIONS 208Pb(17O, 16O), (17O, 18F), E=376 MeV; measured σ(θ); deduced model parameters. 209Pb, 207Tl levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.36.108
1987HA11 Phys.Lett. 184B, 316 (1987) O.Hausser, K.Hicks, C.W.Glover, R.Abegg, A.Celler, C.Gunther, R.L.Helmer, R.Henderson, D.J.Horen, C.J.Horowitz, K.P.Jackson, J.Lisantti, D.K.McDaniels, C.A.Miller, R.Sawafta, L.W.Swenson Spin Observables for 208Pb(p(pol), p(pol)) Elastic Scattering at 290 MeV NUCLEAR REACTIONS 208Pb(polarized p, p), E=290 MeV; measured polarizations, transfer coefficients vs momentum transfer; deduced elastic scattering amplitudes, spin rotation parameters. Focal-plane polarimeter. Dirac calculations.
doi: 10.1016/0370-2693(87)90172-9
1987HO18 Z.Phys. A328, 189 (1987) D.J.Horen, M.A.G.Fernandes, G.R.Satchler, B.L.Burks, R.L.Auble, F.E.Bertrand, E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira Transfer Reactions at High Energy and Ambiguities in Heavy-Ion Potentials NUCLEAR REACTIONS 28Si(16O, 16O), E=56, 351.7 MeV; calculated σ(θ); deduced optical potential parameters. 28Si(18O, 17O), E=352 MeV; 28Si(18O, 19F), E=352 MeV; analyzed data; deduced model parameters. 29Si, 29Al levels deduced spectroscopic factors.
1987JO04 Phys.Rev. C36, 2252 (1987) C.H.Johnson, D.J.Horen, C.Mahaux Unified Description of the Neutron-208Pb Mean Field between - 20 and + 165 MeV from the Dispersion Relation Constraint NUCLEAR REACTIONS 208Pb(n, n), (polarized n, n), E=1-25 MeV; measured σ(θ), analyzing power vs θ, σ(E). 208Pb deduced single particle densities, spectroscopic factors, rms radii, occupation numbers. Unified model, dispersion relation constraint.
doi: 10.1103/PhysRevC.36.2252
1987KR10 Phys.Lett. 189B, 299 (1987) D.Krofcheck, E.Sugarbaker, A.J.Wagner, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, C.Gaarde, D.J.Horen, T.Carey, T.N.Taddeucci Gamow-Teller Strength Distribution in 81Kr and the Consequences for a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 81Br(p, n), E=190, 200 MeV; measured σ(En). 81Kr transitions deduced Gamow-Teller transition strength distribution. Tof.
doi: 10.1016/0370-2693(87)91436-5
1987MC03 Nucl.Phys. A467, 557 (1987) D.K.McDaniels, J.Lisantti, I.Bergqvist, L.W.Sewnson, X.Y.Chen, D.J.Horen, F.E.Bertrand, E.E.Gross, C.Glover, R.Sayer, B.L.Burks, O.Hausser, K.Hicks Validity of Collective Model DWBA Analysis for Intermediate Energy Proton Scattering to Low-Lying States of 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=200, 400 MeV; measured σ(θ). 208Pb levels deduced deformation lengths, multipole moments, neutron, proton matrix element ratio. DWBA analysis.
doi: 10.1016/0375-9474(87)90386-1
1986BE14 Phys.Rev. C34, 45 (1986) F.E.Bertrand, E.E.Gross, D.J.Horen, R.O.Sayer, T.P.Sjoreen, D.K.McDaniels, J.Lisantti, J.R.Tinsley, L.W.Swenson, J.B.McClelland, T.A.Carey, K.Jones, S.J.Seestrom-Morris Giant Resonance Structure in 208Pb Measured using the (p, p') Reaction at 334 MeV NUCLEAR REACTIONS 208Pb(polarized p, p'), E=334 MeV; measured σ(Ep), σ(θ); deduced model parameters. 208Pb deduced giant resonances, Γ, L, EWSR, B(λ). DWBA analysis.
doi: 10.1103/PhysRevC.34.45
1986FE03 Phys.Rev. C33, 1971 (1986) M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen One-Nucleon-Transfer Reactions Induced by 352-MeV 18O on 28Si NUCLEAR REACTIONS 28Si(18O, 17O), (18O, 19F), E=352 MeV; measured σ(θ); deduced model parameters. 29Si, 27Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.33.1971
1986HO19 Phys.Rev. C34, 429 (1986) D.J.Horen, C.H.Johnson, J.L.Fowler, A.D.MacKellar, B.Castel 208Pb + n Reaction and the Mean Nuclear Field near Threshold NUCLEAR REACTIONS 208Pb(n, X), 208Pb(n, n), E=50-1005 keV; measured transmission, σ(E), σ(θ); deduced model parameters. 209Pb deduced resonances, J, π, Γn, neutron reduced width, strength function. Optical model, R-matrix analysis.
doi: 10.1103/PhysRevC.34.429
1986HO27 Phys.Lett. 181B, 38 (1986) D.J.Horen, B.L.Burks, M.A.G.Fernandes, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, G.R.Satchler, D.Shapira, T.P.Sjoreen, F.Petrovich Investigation of the One-Step Direct Contribution to the 28Si(18O, 18F)28Al Reaction at 19.6 MeV/Nucleon NUCLEAR REACTIONS, MECPD 28Si(18O, 18F), E=352 MeV; measured σ(E(18F)), σ(θ); deduced reaction mechanism. Magnetic spectrometer system, particle identification ionization chamber. Microscopic DWIA calculations.
doi: 10.1016/0370-2693(86)91250-5
1986MC06 Phys.Rev. C33, 1943 (1986) D.K.McDaniels, J.R.Tinsley, J.Lisantti, D.M.Drake, I.Bergqvist, L.W.Swenson, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen, R.Liljestrand, H.Wilson Cross Section and Analyzing Power Measurements for the Giant Resonance Region in 208Pb with 200-MeV Protons NUCLEAR REACTIONS 208Pb(polarized p, p'), (p, p'), E=200 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. 208Pb deduced isoscalar GQR, monopole resonance, isovector GDR, J, π, B(λ), hexadecapole transition EWSR, Γ.
doi: 10.1103/PhysRevC.33.1943
1986TA05 Phys.Rev. C33, 746 (1986) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker Spin-Flip Decomposition of the Spectrum for 90Zr(p, n) at E(p) = 160 MeV NUCLEAR REACTIONS 90Zr(polarized p, n), E=160 MeV; measured σ(θ=0°), transverse polarization transfer. 90Nb deduced ΔL=0, ΔL=1 resonance excitations, transition strengths.
doi: 10.1103/PhysRevC.33.746
1985GO02 Phys.Rev.Lett. 54, 877 (1985); Erratum Phys.Rev.Lett. 54, 2060 (1985) C.D.Goodman, R.C.Byrd, I.J.Van Heerden, T.A.Carey, D.J.Horen, J.S.Larsen, C.Gaarde, J.Rapaport, T.P.Welch, E.Sugarbaker, T.N.Taddeucci Measurements of Gamow-Teller Strength Distributions in Masses 13 and 15 NUCLEAR REACTIONS 13C, 15N(polarized p, n), E=160 MeV; measured σ(θ), spin-flip probabilities. 13N, 15O deduced quenched Gamow-Teller transition strengths. Shell model comparison.
doi: 10.1103/PhysRevLett.54.877
1985HO14 Phys.Rev. C31, 2049 (1985) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Cross Sections and Analyzing Powers for Quenched Spin Excitations in 40,48Ca at E(p) = 334 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p'), E=334 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. 40Ca level deduced B(M2). Microscopic DWIA.
doi: 10.1103/PhysRevC.31.2049
1985HO23 Phys.Lett. 161B, 217 (1985) D.J.Horen, C.H.Johnson, A.D.Mackellar lJ-Dependence of the Real Optical Potential near Neutron Threshold NUCLEAR REACTIONS 208Pb(n, X), (n, n), E=0.05-1.005 MeV; measured transmission, σ(θ). 208Pb(n, n), E=4, 7 MeV; analyzed σ(θ); deduced optical model parameters, l-, j-dependences.
doi: 10.1016/0370-2693(85)90748-8
1985KR10 Phys.Rev.Lett. 55, 1051 (1985) D.Krofcheck, E.Sugarbaker, J.Rapaport, D.Wang, J.N.Bahcall, R.C.Byrd, C.C.Foster, C.D.Goodman, I.J.Van Heerden, C.Gaarde, J.S.Larsen, D.J.Horen, T.N.Taddeucci Gamow-Teller Strength Function in 71Ge via the (p, n) Reaction at Medium Energies NUCLEAR REACTIONS 71Ga(p, n), E=120, 200 MeV; measured σ(En), σ(θ, En); deduced neutrino capture σ corrections in 71Ga detector. 71Ge deduced Gamow-Teller strength function, transition strength fragmentation.
doi: 10.1103/PhysRevLett.55.1051
1985MC06 Phys.Lett. 162B, 277 (1985) D.K.McDaniels, J.Lisantti, J.Tinsley, I.Bergqvist, L.W.Swenson, F.E.Bertrand, E.E.Gross, D.J.Horen On the Validity of Microscopic Calculations for Inelastic Proton Scattering NUCLEAR REACTIONS 208Pb(polarized p, p'), E=200, 334 MeV; analyzed σ(θ). 208Pb level deduced B(E2).
doi: 10.1016/0370-2693(85)90922-0
1985TA23 Nucl.Instrum.Methods 241, 448 (1985) T.N.Taddeucci, C.D.Goodman, R.C.Byrd, T.A.Carey, D.J.Horen, J.Rapaport, E.Sugarbaker A Neutron Polarimeter for (p, n) Measurements at Intermediate Energies NUCLEAR REACTIONS 14C(polarized p, n), E=80, 120, 160 MeV; measured transverse polarization transfer, σ(En). Large volume, large acceptance neutron polarimeter, plastic scintillator.
doi: 10.1016/0168-9002(85)90597-2
1984HO11 Phys.Rev. C29, 2126 (1984) D.J.Horen, R.L.Macklin, J.A.Harvey, N.W.Hill Measurements of the Neutron Transmission and Capture Cross Sections in 204Pb NUCLEAR REACTIONS 204Pb(n, n), (n, γ), E=0.4-105 keV; measured total σ(E), capture σ(E); deduced stellar temperature capture < σ >. 205Pb deduced resonances, J, π, L, (gΓn), (gΓnΓγ/Γ), Γγ, s-wave strength function.
doi: 10.1103/PhysRevC.29.2126
1984HO16 Phys.Rev. C30, 709 (1984) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Excitation of E2 Transitions in 40Ca by 334-MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=334 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca deduced levels, J, π, L admixture, deformation lengths, B(E2). Macroscopic DWBA analysis.
doi: 10.1103/PhysRevC.30.709
1984LI19 Phys.Lett. 147B, 23 (1984) J.Lisantti, J.R.Tinsley, D.M.Drake, I.Bergqvist, L.W.Swenson, D.K.McDaniels, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen Analyzing Power for the Inelastic Continuum with 200 MeV Protons NUCLEAR REACTIONS 60Ni, 90Zr, 208Pb(p, p'X), (polarized p, p'X), E=200 MeV; measured inclusive σ(Ep'), σ(θ), analyzing power vs θ; deduced reaction mechanism excitation energy dependence.
doi: 10.1016/0370-2693(84)90584-7
1984RA22 Nucl.Phys. A431, 301 (1984) J.Rapaport, C.Gaarde, J.Larsen, C.Goulding, C.D.Goodman, C.Foster, D.J.Horen, T.Masterson, E.Sugarbaker, T.N.Taddeucci The 19F(p, n)19Ne and 39K(p, n)39Ca Reactions at Intermediate Energies and Quenching of the Gamow-Teller Strength NUCLEAR REACTIONS 19F, 39K(p, n), E=120, 160 MeV; measured σ(En), σ(θ). 19Ne, 39Ca levels deduced Gamow-Teller transition strength distribution. DWBA analysis.
doi: 10.1016/0375-9474(84)90177-5
1984SJ01 Phys.Rev. C29, 1370 (1984) T.P.Sjoreen, F.E.Bertrand, R.L.Auble, E.E.Gross, D.J.Horen, D.Shapira, D.B.Wright Inelastic Excitation of Giant Resonances by 400-MeV 16O NUCLEAR REACTIONS 208Pb, 90Zr(16O, 16O'), E=350, 400 MeV; measured σ(θ, E(16O')), σ(θ). 208Pb, 16O deduced giant monopole, dipole, quadrupole resonance excitation.
doi: 10.1103/PhysRevC.29.1370
1984TA07 Phys.Rev.Lett. 52, 1960 (1984) T.N.Taddeucci, T.A.Carey, C.Gaarde, J.Larsen, C.D.Goodman, D.J.Horen, T.Masterson, J.Rapaport, T.P.Welch, E.Sugarbaker Measurement of the Tranverse Spin-Transfer Coefficient D(NN)(0°) for (p(pol), n(pol)) Reactions at 160 MeV NUCLEAR REACTIONS 6,7Li, 12,13,14C, 90Zr(polarized p, n), E=160 MeV; measured transverse spin transfer coefficient D(NN)(θ=0°), polarized neutrons. 6,7Be, 12,13,14N, 90Nb deduced L=0 Gamow-Teller transition expected average value.
doi: 10.1103/PhysRevLett.52.1960
1983BR16 Phys.Lett. 127B, 151 (1983) B.A.Brown, D.J.Horen, B.Castel, H.Toki Core Excitations and M1 Strengths in the Ca Isotopes NUCLEAR STRUCTURE 40Ca; calculated positive parity T=0, 1 states, isovector B(M1). 16,18,20,22O; calculated B(M1) vs excitation energy. Shell model. 42,44Ca; calculated M1 transition strength reduction, fragmentation. Weak-coupling extension.
doi: 10.1016/0370-2693(83)90864-X
1983RA30 Nucl.Phys. A410, 371 (1983) J.Rapaport, T.Taddeucci, T.P.Welch, C.Gaarde, J.Larsen, D.J.Horen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Giant Spin-Isospin Multipole Vibrations in 54,56Fe and 58,60Ni NUCLEAR REACTIONS 58Ni(p, n), E=120 MeV; 54,56Fe, 58,60Ni(p, n), E=160 MeV; measured σ(θ, En), θ < 6°, σ(θ). 58Cu, 54,56Co deduced L=0 transition strengths, Gamow-Teller state strengths. Shell model.
doi: 10.1016/0375-9474(83)90632-2
1983TA16 Phys.Rev. C28, 2511 (1983) T.N.Taddeucci, J.Rapaport, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Spin Excitations in 40C(p, n) NUCLEAR REACTIONS 40Ca(p, n), E=59.3, 118.3, 159.3 MeV; measured σ(θ), σ(En). 40Sc level deduced Gamow-Teller transition strength. 42Ca(p, n), E=159.3 MeV; measured σ(θ). DWIA analyses.
doi: 10.1103/PhysRevC.28.2511
1983TI03 Phys.Rev. C28, 1417 (1983) J.R.Tinsley, D.K.McDaniels, J.Lisantti, L.W.Swenson, R.Liljestrand, D.M.Drake, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen Observation of 2(h-bar x omega) Hexadecapole Strength in Lead Nuclei from 200 MeV Inelastic Proton Scattering NUCLEAR REACTIONS 206,208Pb(p, p'), E=200 MeV; measured σ(Ep'), σ(θ). 208Pb deduced isosclar giant resonance L, Γ, B(E4).
doi: 10.1103/PhysRevC.28.1417
1982RA30 Phys.Lett. 119B, 61 (1982) J.Rapaport, T.Taddeucci, T.P.Welch, D.J.Horen, J.B.McGrory, C.Gaarde, J.Larsen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Gamow-Teller Resonances in A = 58 Nuclei NUCLEAR REACTIONS 58Ni(p, n), E=120, 160 MeV; measured σ(En, θ=0°). 58Cu deduced levels, isovector Gamow-Teller transition strength.
doi: 10.1016/0370-2693(82)90243-X
1982TA03 Phys.Rev. C25, 1094 (1982) T.N.Taddeucci, J.Rapaport, D.E.Bainum, C.D.Goodman, C.C.Foster, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Energy Dependence of the Ratio of Isovector Effective Interaction Strengths [J(στ)/J(τ)] from 0° (p, n) Cross Sections NUCLEAR REACTIONS 7Li, 13,14C, 26Mg, 37Cl, 42Ca(p, n), E=60-200 MeV; measured σ(θ=0°); deduced isovector effective interaction strength ratio. 7Be, 13,14N, 26Al, 37Ar, 42Sc levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.25.1094
1981BE06 Phys.Lett. 99B, 213 (1981) F.E.Bertrand, J.R.Beene, C.E.Bemis, Jr., E.E.Gross, D.J.Horen, J.R.Wu, W.P.Jones Measurement of the Fission Decay of the Giant Quadrupole Resonance in 238U NUCLEAR REACTIONS, Fission 238U(α, α'F), E=152 MeV; measured σ(Eα', θ), α(fragment)-coin, fission probability vs excitation energy. 238U deduced Γf/Γ for GQR, possible K conservation.
doi: 10.1016/0370-2693(81)91110-2
1981BE33 Phys.Lett. 103B, 326 (1981) F.E.Bertrand, E.E.Gross, D.J.Horen, J.R.Wu, J.Tinsley, D.K.McDaniels, L.W.Swenson, R.Liljestrand Excitation of Giant Resonance Modes in 90Zr and 120Sn by 200 MeV Protons NUCLEAR REACTIONS 90Zr, 120Sn(p, p'), E=200 MeV; measured σ(Ep, θ). 90Zr deduced M1 transition strength. 90Zr, 120Sn deduced GDR, isoscalar GQR, giant octupole resonance, hexadecapole strength upper limit. Broad-range magnetic spectrograph.
doi: 10.1016/0370-2693(81)90235-5
1981GA26 Nucl.Phys. A369, 258 (1981) C.Gaarde, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, D.E.Bainum, C.A.Goulding, M.B.Greenfield, D.J.Horen, E.Sugarbaker Excitation of Giant Spin-Isospin Multipole Vibrations NUCLEAR REACTIONS 40Ca, 90Zr, 112,124Sn, 208Pb, 169Tm(p, n), E=200 MeV; measured σ(En, θ). 40Sc, 90Nb, 112,124Sb, 169Yb, 208Bi deduced resonances, L, Gamow-Teller resonance characteristics, giant spin-isospin multipole vibrations. Enriched targets, time-compensated large volume detectors.
doi: 10.1016/0375-9474(81)90019-1
1981GO18 Phys.Lett. 107B, 406 (1981) C.D.Goodman, C.C.Foster, D.E.Bainum, S.D.Bloom, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, S.Grimes, J.Rapaport, T.N.Taddeucci, E.Sugarbaker Missing Gamow-Teller Strength in Mass 42 NUCLEAR REACTIONS 42Ca(p, n), E=160 MeV; measured σ(θ, En). 42Sc deduced Gamow-Teller transition strength distribution. Shell model.
doi: 10.1016/0370-2693(81)91217-X
1981HO03 Phys.Lett. 99B, 383 (1981) D.J.Horen, C.D.Goodman, D.E.Bainum, C.C.Foster, C.Gaarde, C.A.Goulding, M.B.Greenfield, J.Rapaport, T.N.Taddeucci, E.Sugarbaker, T.Masterson, S.M.Austin, A.Galonsky, W.Sterrenburg Energy Systematics of the Giant Gamow-Teller Resonance and a Charge-Exchange Dipole Spin-Flip Resonance NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn, 169Tm, 208Pb(p, n), E=120, 160, 200 MeV; measured σ(En, θ). 90,92,94Nb, 112,116,124Sb, 169Yb, 208Bi deduced giant Gamow-Teller, charge exchange dipole spin-flip resonance energy systematics. Tof.
doi: 10.1016/0370-2693(81)90553-0
1981HO28 Phys.Rev. C24, 1961 (1981) D.J.Horen, J.A.Harvey, N.W.Hill 206Pb + n Resonances for E = 600-900 keV: Neutron strength functions NUCLEAR REACTIONS 206Pb(n, X), (n, n), E=600-900 keV; measured σ(E, θ), σ(total, E); deduced optical model parameters. 207Pb deduced resonance parameters, J, π, Γn, strength functions.
doi: 10.1103/PhysRevC.24.1961
1981WU02 Phys.Rev. C24, 500 (1981) J.R.Wu, J.R.Beene, C.E.Bemis, Jr., F.E.Bertrand, E.E.Gross, D.J.Horen, W.P.Jones Fission Probability of 239U at High Excitation Measured with the 238U(α, 3Hef) Reaction NUCLEAR REACTIONS, Fission 238U(α, 3HeF), E=152 MeV; measured σ(θ(3He), E(3He)), σ(θ(3He), E(3He), fragment θ), 3He(fragment)(fragment)-coin; deduced reaction mechanism. 239U deduced fission probability vs excitation energy.
doi: 10.1103/PhysRevC.24.500
1980BA16 Phys.Rev.Lett. 44, 1751 (1980) D.E.Bainum, J.Rapaport, C.D.Goodman, D.J.Horen, C.C.Foster, M.B.Greenfield, C.A.Goulding Observation of Giant Particle-Hole Resonances in 90Zr(p, n)90Nb NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; measured σ(En, θn). 90Nb deduced T=4, 5 components of Gamow-Teller strength, E1 resonance. Tof, macroscopic DWBA analysis.
doi: 10.1103/PhysRevLett.44.1751
1980BE50 Phys.Rev. C22, 1832 (1980) F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles NUCLEAR REACTIONS 208Pb, 120Sn, 90Zr, 58Ni, 46Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). 46Ti, 58Ni, 90Zr, 120Sn, 208Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.
doi: 10.1103/PhysRevC.22.1832
1980HO21 Phys.Lett. B95, 27 (1980) D.J.Horen, C.D.Goodman, C.C.Foster, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, E.Sugarbaker, T.G.Masterson, F.Petrovich, W.G.Love Search for Isobaric Analogues of M1 States and Giant Spinflip Resonance NUCLEAR REACTIONS 208Pb(p, n), E=120, 160 MeV; measured σ(θ, En). 209Bi deduced resonances, Γ, J, π, analog M1 states, giant spinflip resonance. Tof, enriched target.
doi: 10.1016/0370-2693(80)90391-3
1979BE04 Phys.Lett. 80B, 198 (1979) F.E.Bertrand, G.R.Satchler, D.J.Horen, A.van der Woude Systematics of the Isoscalar Giant Monopole Resonance from 60 MeV Inelastic Proton Scattering NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr, 120Sn, 144,154Sm, 197Au, 208Pb(p, p'), E=60 MeV; calculated σ(θ); deduced parameters of isoscalar GQR, GMR. DWBA.
doi: 10.1016/0370-2693(79)90197-7
1979HO01 Phys.Rev. C19, 549 (1979) D.J.Horen, R.T.Kouzes, D.Mueller, F.Calaprice, R.P.Hall Evidence for Negative Parity for the 7064-keV Level in 208Pb NUCLEAR REACTIONS 207Pb(d, p), E=26.2 MeV; measured σ(Ep, θ). 208Pb deduced levels, J, π.
doi: 10.1103/PhysRevC.19.549
1979HO16 Phys.Rev. C20, 478 (1979) D.J.Horen, J.A.Harvey, N.W.Hill 206Pb + n Resonances for E = 25-600 keV: s-, p-, and d-Wave Doorway States and M1 Ground-State Radiative Strength in 207Pb NUCLEAR REACTIONS 206Pb(n, X), (n, n), E=25-600 keV; measured total σ(E), σ(E, θ). 207Pb deduced s-, p-, d-wave doorway states, resonance parameters, J, π, Γn, level densities, n strength functions, M1 radiative strength.
doi: 10.1103/PhysRevC.20.478
1978BE55 Phys.Rev. C18, 2788 (1978) F.E.Bertrand, G.R.Satchler, D.J.Horen, A.van der Woude Excitation of the Giant Isoscalar Monopole Resonance in 144Sm via Inelastic Proton Scattering NUCLEAR REACTIONS 144,154Sm(p, p'), E=67 MeV; measured σ(Ep', θ). 144,154Sm levels deduced L, β(L); discussed giant multipole resonance structure. DWBA analysis.
doi: 10.1103/PhysRevC.18.2788
1978HO10 Phys.Rev. C18, 722 (1978) D.J.Horen, J.A.Harvey, N.W.Hill Doorway States in s-, p-, and d-Wave Entrance Channels in 207Pb + n Reaction NUCLEAR REACTIONS 207Pb(n, X), (n, n), E=3-485 keV; measured total σ(E), σ(E, θ). 208Pb deduced doorway states, L, J, π, resonance parameters, Γn, neutron strength functions.
doi: 10.1103/PhysRevC.18.722
1978HO15 Phys.Lett. 79B, 39 (1978) D.J.Horen, G.F.Auchampaugh, J.A.Harvey On the Question of a Giant M1 Resonance Near 8 MeV in 208Pb NUCLEAR REACTIONS 207Pb(n, X), E=600-627 keV; measured σ(θ). 208Pb deduced levels, L, J, π, Γ, E1 character of levels near 8 MeV. R matrix analysis. Enriched targets.
doi: 10.1016/0370-2693(78)90430-6
1977HO05 Phys.Rev. C15, 1168 (1977) D.J.Horen, J.A.Harvey, N.W.Hill Angular Momentum Determination of Resonances in 24Mg + n by Elastic Neutron Scattering NUCLEAR REACTIONS 24Mg(n, n), E=0.4-1.8 MeV; measured σ(θ). 25Mg resonances deduced L.
doi: 10.1103/PhysRevC.15.1168
1977HO06 Phys.Rev.Lett. 38, 1344 (1977) D.J.Horen, J.A.Harvey, N.W.Hill Giant Magnetic Dipole States in 208Pb Observed in the 207Pb = n Reaction NUCLEAR REACTIONS 207Pb(n, n), (n, n'γ), E=3 keV-several MeV; measured σ(E), transmission σ(E). 208Pb deduced resonances, GDR.
doi: 10.1103/PhysRevLett.38.1344
1977HO07 Phys.Lett. 67B, 268 (1977) D.J.Horen, J.A.Harvey, N.W.Hill First Observation of (s+d)-Wave Mixing in Low-Energy Elastic Neutron Scattering NUCLEAR REACTIONS 207Pb(n, n), E=180, 256, 320 keV; measured transmission spectrum; deduced L wave mixing. 208Pb deduced resonances, J, π.
doi: 10.1016/0370-2693(77)90367-7
1976HO06 Nucl.Data Sheets 17, 367 (1976) Nuclear Data Sheets for A = 228 COMPILATION 228Fr, 228Ra, 228Ac, 228Th, 228Pa, 228U; compiled, evaluated structure data.
doi: 10.1016/S0090-3752(76)80042-7
1976HO18 Nucl.Data Sheets 19, 383 (1976) Nuclear Data Sheets for A = 176 COMPILATION 176Tm, 176Yb, 176Lu, 176Hf, 176Ta, 176W, 176Re, 176Os, 176Ir, 176Pt, 176Au; compiled, evaluated structure data.
doi: 10.1016/S0090-3752(76)80067-1
1975AR16 Nucl.Phys. A247, 238 (1975) J.Arvieux, M.Buenerd, A.J.Cole, P.De Saintignon, G.Perrin, D.J.Horen Giant Resonances in f-p Shell Nuclei Studied by Inelastic Scattering Of 80 MeV 3He Ions NUCLEAR REACTIONS 48Ti, 56Fe, 59Co, 60Ni(3He, 3He'), E=80 MeV; measured σ(E(3He'), θ). 48Ti, 56Fe giant resonances deduced L.
doi: 10.1016/0375-9474(75)90634-X
1975GI11 Nucl.Phys. A252, 509 (1975) Band Structure in 131,132,133Ba Observed by (12C, xn) Reactions NUCLEAR REACTIONS 122,124Sn(12C, 3nγ), 124Sn(12C, 4nγ), E=46-57 MeV; measured σ(E;Eγ, θ), γγ-coin, γγ-delay. 131,132,133Ba deduced levels, J, π, δ, prolate shape. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90516-3
1975HA15 Nucl.Data Sheets 14, 297 (1975) Nuclear Data Sheets for A = 173 COMPILATION 173Er, 173Tm, 173Yb, 173Lu, 173Hf, 173Ta, 173W; compiled, evaluated structure data.
doi: 10.1016/S0090-3752(75)80040-8
1975HA32 Phys.Rev. C12, 1083 (1975) B.Harmatz, D.J.Horen, Y.A.Ellis Ground States in the Neutron-Deficient 165 ≤ A ≤ 185 Region NUCLEAR STRUCTURE 171,173Ta, 177W, 181Os; analyzed data; deduced Nilsson assignments.
doi: 10.1103/PhysRevC.12.1083
1975HO05 Phys.Rev. C11, 1247 (1975) D.J.Horen, J.Arvieux, M.Buenerd, J.Cole, G.Perrin, P.de Saintignon Giant Resonance Region Observed in 3He Scattering by 144,154Sm, 159Tb, 165Ho, 169Tm, and 208Pb NUCLEAR REACTIONS 144,154Sm, 165Ho(3He, 3He'), E=80 MeV; measured σ(E, E(3He'), θ). 159Tb, 169Tm, 208Pb(3He, 3He'), E=80 MeV; measured σ(E(3He')). 144,154Sm, 159Tb, 165Ho, 169Tm, 208Pb deduced giant resonance character.
doi: 10.1103/PhysRevC.11.1247
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