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Search: Author = D.J.Horen

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1205.


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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1176.


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13531.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0518.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0113.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0271.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0166.


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
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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
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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
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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
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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+- 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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1976HO06      Nucl.Data Sheets 17, 367 (1976)

D.J.Horen

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
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1976HO18      Nucl.Data Sheets 19, 383 (1976)

D.J.Horen, B.Harmatz

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
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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
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1975GI11      Nucl.Phys. A252, 509 (1975)

J.Gizon, A.Gizon, D.J.Horen

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
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1975HA15      Nucl.Data Sheets 14, 297 (1975)

B.Harmatz, D.J.Horen

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
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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
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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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