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Search: Author = S.Thornton

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2014PE15      Phys.Rev. C 90, 024317 (2014)

J.C.Pei, G.I.Fann, R.J.Harrison, W.Nazarewicz, Y.Shi, S.Thornton

Adaptive multi-resolution 3D Hartree-Fock-Bogoliubov solver for nuclear structure

NUCLEAR STRUCTURE 110Mo; calculated single-neutron and proton wave functions, one-quasiparticle energies, occupations, chemical potential, and total energy, neutron density distributions, total binding energy, kinetic energy, spin-orbit-Coulomb-energy, mass rms radii and quadrupole moments. Nuclear density functional theory (DFT) based on adaptive multi-resolution 3D Hartree-Fock-Bogoliubov (HFB) solver using MADNESS-HFB. Parallel programming techniques using high-performance supercomputers. Comparison with other theoretical calculations.

doi: 10.1103/PhysRevC.90.024317
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2001BL09      Phys.Rev. C64, 025203 (2001)

G.Blanpied, M.Blecher, A.Caracappa, R.Deininger, C.Djalali, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, A.Kuczewski, F.Lincoln, M.Lowry, M.Lucas, G.Matone, L.Miceli, B.M.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, H.Stroher, C.E.Thorn, S.T.Thornton, J.Tonnison, C.S.Whisnant, H.Zhang, X.Zhao, and the LEGS Collaboration

N → Δ Transition and Proton Polarizabilities from Measurements of p(γ(pol), γ), p(γ(pol), π0), and p(γ(pol), π+)

NUCLEAR REACTIONS 1H(polarized γ, γ), (polarized γ, π0), (polarized γ, π+), E=213-333 MeV; measured σ, σ(E, θ), asymmetries; deduced Δ resonance excitation mixing ratio, helicity amplitudes, quadrupole moment. 1H deduced spin polarizabilities, Baldin sum rule. Multipole analysis, comparison with previous data.

doi: 10.1103/PhysRevC.64.025203
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2000BL02      Phys.Rev. C61, 024604 (2000)

G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, C.Molinari, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, D.Rebreyend, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, and the LEGS Collaboration

Measurement of 2H(γ(pol), p)n with Linearly Polarized Photons in the Δ Resonance Region

NUCLEAR REACTIONS 2H(polarized γ, p), E=110-315 MeV; measured proton spectra, polarization dependent and independent σ(θ), integrated σ, beam asymmetry; deduced Δ resonance role. Coupled-channels calculations, comparisons with previous results.

doi: 10.1103/PhysRevC.61.024604
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0632.


2000HI06      Phys.Rev. C61, 054609 (2000)

K.Hicks, V.Gladyshev, H.Baghaei, A.Caracappa, A.Cichocki, R.Deininger, R.Finlay, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Li, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, D.Willits, L.E.Wright

The 16O(γ(pol), π-p) Reaction at Eγ ≈ 300 MeV

NUCLEAR REACTIONS 16O(polarized γ, π-p), E=290-325 MeV; measured σ(E, θ1, θ2), spin asymmetries. Comparison with DWIA results.

doi: 10.1103/PhysRevC.61.054609
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1997HI01      Phys.Rev. C55, R12 (1997)

K.Hicks, H.Baghaei, A.Caracappa, A.Cichocki, G.Davenport, R.Finlay, V.Gladyshev, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Lee, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, L.E.Wright

Spin Asymmetries from 16O(γ(pol), pπ-) Near Δ Resonance Energies

NUCLEAR REACTIONS 16O(polarized γ, pπ-), E=293 MeV; measured spin asymmetry vs θp, θ(π); deduced Δ-nucleus potential, δ lifetime dependences.

doi: 10.1103/PhysRevC.55.R12
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1996BL03      Phys.Rev.Lett. 76, 1023 (1996)

G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, C.Molinari, B.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, H.Stroher, C.E.Thorn, S.T.Thornton, C.S.Whisnant, H.Zhang, X.Zhao, and the LEGS Collaboration

Polarized Compton Scattering from the Proton

NUCLEAR REACTIONS 1H(polarized γ, γ), E=213-333 MeV; measured σ(θ), asymmetry vs E, Compton scattering; deduced resolution of earlier data problems. Model analysis.

doi: 10.1103/PhysRevLett.76.1023
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0673.


1995AD01      Phys.Rev. C51, 17 (1995)

G.S.Adams, H.Baghaei, A.Caracappa, W.Clayton, A.D'Angelo, S.Hoblit, M.Khandaker, O.C.Kistner, T.Kobayashi, R.Lindgren, L.Miceli, C.Ruth, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

Measurement of γ(pol)d → pnπ0 at Large Nucleon Momenta

NUCLEAR REACTIONS 2H(polarized γ, nπ0), E=290 MeV; measured σ(θn, θp) vs neutron momentum; deduced beam asymmetries. Cascade Monte Carlo calculation.

doi: 10.1103/PhysRevC.51.17
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1995BL13      Phys.Rev. C52, R455 (1995)

G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, K.Hicks, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, D.Rebreyend, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, P.Wilhelm, H.Arenhovel, and the LEGS Collaboration

New Measurements of 2H(polarized γ, p)n and Spin Problems in Coupled NΔ/NN Interactions

NUCLEAR REACTIONS, ICPND 2H(polarized γ, p), E=113-315 MeV; measured σ(θ) vs E, σ(E). Tagged beam. NΔ/NN coupled-channel analysis.

doi: 10.1103/PhysRevC.52.R455
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1994RU04      Phys.Rev.Lett. 72, 617 (1994)

C.Ruth, G.S.Adams, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.-A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.A.Moinester, A.M.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, D.J.Tedeschi, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

First Measurement of the Reaction 3He(γ(pol), p)X with Polarized Photons

NUCLEAR REACTIONS 3He(polarized γ, p), E=195-304 MeV; measured σ(θ), photon asymmetry vs proton momentum; deduced three-nucleon absorption evidence. Linear beam polarization.

doi: 10.1103/PhysRevLett.72.617
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1994TE07      Phys.Rev.Lett. 73, 408 (1994)

D.J.Tedeschi, G.S.Adams, G.Audit, H.Baghaei, A.Caracappa, W.B.Clayton, A.D'Angelo, M.A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, J.M.Laget, R.Lindgren, G.Matone, L.Miceli, W.K.Mize, M.Moinester, C.Ruth, A.Sandorfi, C.Schaerf, R.M.Sealock, L.C.Smith, P.Stoler, P.K.Teng, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, E.J.Winhold

Exclusive Photodisintegration of 3He with Polarized Photons

NUCLEAR REACTIONS 3He(polarized γ, np), (polarized γ, 2p), E=235-305 MeV; measured σ(θ1, θ2, p1), asymmetry; deduced reaction mechanism.

doi: 10.1103/PhysRevLett.73.408
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1993DA13      Phys.Rev. C48, 1849 (1993)

D.B.Day, J.S.McCarthy, Z.E.Meziani, R.Minehart, R.Sealock, S.T.Thornton, J.Jourdan, I.Sick, B.W.Filippone, R.D.McKeown, R.G.Milner, D.H.Potterveld, Z.Szalata

Inclusive Electron-Nucleus Scattering at High Momentum Transfer

NUCLEAR REACTIONS 4He, 12C, 27Al, 56Fe, 197Au(e, e'X), E=2.02, 3.595 GeV; measured σ(θ) vs energy loss.

doi: 10.1103/PhysRevC.48.1849
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1993ME01      Nucl.Phys. A553, 701c (1993)

Z.-E.Meziani, J.P.Chen, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.E.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, I.Sick, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

High Momentum Transfer R(T, L) Response Functions for 3,4He

NUCLEAR REACTIONS 3,4He(e, e'X), E=0.9-4.3 GeV; measured inclusive σ; deduced longitudinal, transverse response functions, Coulomb sum rule saturation.

doi: 10.1016/0375-9474(93)90683-O
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1993SM05      Phys.Rev. C48, R485 (1993)

L.C.Smith, R.C.Minehart, O.K.Baker, D.B.Day, K.L.Giovanetti, R.Lourie, R.M.Marshall, B.Milbrath, B.G.Ritchie, R.M.Sealock, D.Tedeschi, S.T.Thornton

Pion Absorption in 4He Above the Delta Resonance

NUCLEAR REACTIONS 4He(π+, 2p), E=500 MeV; measured σ(θ, E); deduced quasifree two-nucleon, four-body absorption. PWIA analysis, isobar-isobar model.

doi: 10.1103/PhysRevC.48.R485
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1992BL12      Phys.Rev.Lett. 69, 1880 (1992)

G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, S.Hoblit, M.Khandaker, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, X.Zhao, M.A.Moinester, and the LEGS Collaboration

p(γ(pol), π0) Reaction and the E2 Excitation of the Δ

NUCLEAR REACTIONS 1H(polarized γ, π0), E=243, 314 MeV; measured σ(θ); deduced E2 δ excitation.

doi: 10.1103/PhysRevLett.69.1880
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1992FI01      Phys.Rev. C45, 1582 (1992)

B.W.Filippone, R.D.McKeown, R.G.Milner, D.H.Potterveld, D.B.Day, J.S.McCarthy, Z.Meziani, R.Minehart, R.Sealock, S.T.Thornton, J.Jourdan, I.Sick, Z.Szalata

Nuclear Structure Functions at x > 1

NUCLEAR REACTIONS C, Fe, 4He, 197Au(e, e'), E=3.595 GeV; measured σ(E, θ); deduced structure functions.

doi: 10.1103/PhysRevC.45.1582
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1992ME08      Phys.Rev.Lett. 69, 41 (1992)

Z.-E.Meziani, J.P.Chen, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.E.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, I.Sick, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

High Momentum Transfer R(T, L) Inclusive Response Functions for 3,4He

NUCLEAR REACTIONS 3,4He(e, e'X), E=0.9-4.3 GeV; measured σ(θ, E(e')); deduced longitudinal, transverse response functions. 3,4He deduced Coulomb sum rule.

doi: 10.1103/PhysRevLett.69.41
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1991BL11      Phys.Rev.Lett. 67, 1206 (1991)

G.S.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, S.Hoblit, O.C.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant, and the LEGS Collaboration

Beam-Polarization Observables in D(γ(pol), p)n and the Nuclear Tensor Force

NUCLEAR REACTIONS 2H(polarized γ, p), E=191-222 MeV; measured σ(θ), asymmetry, polarization difference vs θ; deduced short-range tensor interaction role.

doi: 10.1103/PhysRevLett.67.1206
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1991CH15      Phys.Rev.Lett. 66, 1283 (1991)

J.P.Chen, Z.E.Meziani, D.Beck, G.Boyd, L.M.Chinitz, D.B.Day, L.C.Dennis, G.Dodge, B.W.Filippone, K.L.Giovanetti, J.Jourdan, K.W.Kemper, T.Koh, W.Lorenzon, J.S.McCarthy, R.D.McKeown, R.G.Milner, R.C.Minehart, J.Morgenstern, J.Mougey, D.H.Potterveld, O.A.Rondon-Aramayo, R.M.Sealock, L.C.Smith, S.T.Thornton, R.C.Walker, C.Woodward

Longitudinal and Transverse Response Functions in 56Fe(e, e') at Momentum Transfer Near 1 GeV/c

NUCLEAR REACTIONS 56Fe(e, e'), E=0.9-4.3 GeV; measured longitudinal, transverse response functions. Model comparison.

doi: 10.1103/PhysRevLett.66.1283
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1991HO14      Nucl.Phys. A527, 358c (1991)

S.Hoblit, G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.-A.Duval, G.Giordano, O.C.Kistner, G.Matone, W.K.Mize, L.Miceli, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, K.Vaziri, C.S.Whisnant

Photon-Beam Polarization Asymmetries in d(γ(pol), p)n

NUCLEAR REACTIONS 2H(polarized γ, p), E not given; measured polarization asymmetry; deduced meson exchange, Δ-isobar currents role.

doi: 10.1016/0375-9474(91)90125-P
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1990BL17      J.Phys.(Paris), Colloq.C-6, 483 (1990)

G.Blanpied, M.Blecher, A.Caracappa, C.Djalali, M.A.Duval, G.Giordano, S.Hoblit, O.K.Kistner, G.Matone, L.Miceli, W.K.Mize, B.M.Preedom, A.M.Sandorfi, C.Schaerf, R.M.Sealock, C.E.Thorn, S.T.Thornton, C.S.Whisnant, D.Babusci, L.Casano, S.d'Angelo, B.Girolami, P.Picozza

Physics with Polarized Photons

NUCLEAR REACTIONS 2H(polarized γ, p), E=206 MeV; measured longitudinal, transverse σ(θ) difference. Preliminary results, other data discussed. Model comparison.


1989DA10      Phys.Rev. C40, 1011 (1989)

D.B.Day, J.S.McCarthy, Z.E.Meziani, R.C.Minehart, R.M.Sealock, S.T.Thornton, J.Jourdan, I.Sick, B.W.Filippone, R.D.McKeown, R.G.Milner, D.H.Potterveld, Z.Szalata

Nuclear Matter Response Function

NUCLEAR STRUCTURE A=4-197; analyzed data; deduced nuclear matter response function.

doi: 10.1103/PhysRevC.40.1011
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1989SE02      Phys.Rev.Lett. 62, 1350 (1989)

R.M.Sealock, K.L.Giovanetti, S.T.Thornton, Z.E.Meziani, O.A.Rondon-Aramayo, S.Auffret, J.-P.Chen, D.G.Christian, D.B.Day, J.S.McCarthy, R.C.Minehart, L.C.Dennis, K.W.Kemper, B.A.Mecking, J.Morgenstern

Electroexcitation of the Δ(1232) in Nuclei

NUCLEAR REACTIONS 1H, 4He, C, Fe, W(e, e'X), E=0.96-1.5 GeV; measured inclusive σ(θ); deduced isobar excitation.

doi: 10.1103/PhysRevLett.62.1350
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1988HA26      Phys.Rev. C38, 572 (1988)

B.A.Harmon, D.Shapira, P.H.Stelson, B.L.Burks, K.A.Erb, B.Shivakumar, K.Teh, S.T.Thornton

Effect of Entrance Channel Asymmetry of Fusion Reactions Leading to Compound Nuclei with A = 40, 42

NUCLEAR REACTIONS 12C(28Si, X), E=6.4, 7.8, 9.4 MeV/nucleon; 12C(30Si, X), E=5.2, 5.7, 6.4, 7.5, 8.3 MeV/nucleon; measured fusion σ; deduced entrance channel asymmetry role.

doi: 10.1103/PhysRevC.38.572
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1987DA20      Phys.Rev.Lett. 59, 427 (1987)

D.B.Day, J.S.McCarthy, Z.E.Meziani, R.Minehart, R.Sealock, S.T.Thornton, J.Jourdan, I.Sick, B.W.Filippone, R.D.McKeown, R.G.Milner, D.H.Potterveld, Z.Szalata

y Scaling in Electron-Nucleus Scattering

NUCLEAR REACTIONS 4He, 12C, 27Al, 56Fe, 197Au(e, e'X), E=2.02, 3.595 GeV; measured inclusive σ(E(e'), θ(e')); deduced scaling factor.

doi: 10.1103/PhysRevLett.59.427
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1986HA33      Phys.Rev. C34, 552 (1986)

B.A.Harmon, S.T.Thornton, D.Shapira, J.Gomez del Campo, M.Beckerman

Entrance Channel Limit on the Fusion of 28Si with 12C at High Energy

NUCLEAR REACTIONS, ICPND 12C(28Si, X), E(cm)=39-54 MeV; measured fusion σ(E). 12C(28Si, 36Cl), (28Si, 33S), (28Si, 30Si), E=180 MeV; measured σ(θ) vs ejectile velocity. 12C(28Si, 32S), E=180 MeV; measured σ(fragment θ, E), σ(θ). 40Ca deduced fusion entrance channel limit.

doi: 10.1103/PhysRevC.34.552
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1985BR03      Phys.Lett. 150B, 75 (1985)

M.Brauner, D.Rychel, R.Gyufko, C.A.Wiedner, S.T.Thornton

Mass Excess of 51Ca

NUCLEAR REACTIONS 48Ca(18O, 15O), E=102 MeV; measured σ(E(15O)), Q. 51Ca deduced levels, mass excess.

doi: 10.1016/0370-2693(85)90141-8
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1985GY01      Phys.Lett. 150B, 335 (1985)

R.Gyufko, D.Rychel, M.Steck, C.-A.Wiedner, R.L.Parks, S.T.Thornton

Mass Excess of 147Tb

NUCLEAR REACTIONS 144Sm(14N, 11Be), E=89 MeV; measured σ(E(11Be)), Q. 147Tb deduced mass excess, two-proton separation energy.

doi: 10.1016/0370-2693(85)90988-8
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1985SH06      Nucl.Instrum.Methods 228, 259 (1985)

D.Shapira, J.L.C.Ford, Jr., R.Novotny, B.Shivakumar, R.L.Parks, S.T.Thornton

The HHIRF Supersonic Gas Jet Target Facility

NUCLEAR REACTIONS 40Ar(16O, 16O), E=100 MeV; measured σ(θ). 40Ar(16O, 17O), E=100 MeV; measured σ(E(17O)). Supersonic gas jet target.

doi: 10.1016/0168-9002(85)90267-0
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1985SH30      Nucl.Instrum.Methods Phys.Res. B10/11, 436 (1985)

D.Shapira, J.Gomez del Campo, J.L.C.Ford, Jr., B.Shivakumar, P.H.Stelson, B.A.Harmon, R.L.Parks, S.T.Thornton

Nuclear Physics Experiments with the ORNL-HHIRF Supersonic Gas Jet Target

NUCLEAR REACTIONS 14N(28Si, X), E=150 MeV; measured fragment spectra; deduced orbiting process products mass, charge distribution features.

doi: 10.1016/0168-583X(85)90285-X
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1984HA31      Z.Phys. A317, 193 (1984)

R.Haupt, C.-A.Wiedner, G.J.Wagner, K.Wannebo, T.S.Bhatia, H.Hafner, R.Maschuw, W.Saathoff, S.T.Thornton

Mass Excesses of 60,62Fe, 68Ni, 69Cu, 74Zn, 73,75Ga

NUCLEAR REACTIONS 58,62,64Ni, 68,70Zn, 74,76Ge(18O, 20Ne), E=81-84 MeV; 68,70Zn, 72,74,76Ge, 78Se(d, 3He), E=21-24 MeV; measured σ(E(20Ne)), σ(E(3He)), Q. 69Cu, 74Zn, 73,75Ga, 60,62Fe, 58Ni deduced mass excess. Q3D magnetic spectrograph, ΔE-E counter.

doi: 10.1007/BF01421254
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1984SH19      Phys.Rev.Lett. 53, 1634 (1984)

D.Shapira, D.Schull, J.L.C.Ford, Jr., B.Shivakumar, R.L.Parks, R.A.Cecil, S.T.Thornton

Observation of Angular Momentum Saturation in Deep-Inelastic Processes involving Light Heavy Ions

NUCLEAR REACTIONS 12C(28Si, X), E=100-190 MeV; measured recoil projectile like fragment spectra; deduced fragment total kinetic energy vs E, angular momentum saturation.

doi: 10.1103/PhysRevLett.53.1634
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1983WI14      Nucl.Phys. A411, 151 (1983)

C.-A.Wiedner, R.Haupt, W.Saathoff, J.Haas, R.Gyufko, K.R.Cordell, S.T.Thornton, R.A.Cecil, R.L.Parks

Mass Excesses of 79As, 81As, and 80Ge

NUCLEAR REACTIONS 82Se, 64Ni(18O, 20Ne), E=102 MeV; 78,80,82Se, 28Si, 24Mg, 16O(d, 3He), E=23-24 MeV; measured σ(E(20Ne)), σ(E(3He)), Q. 79,81As, 80Ge deduced masses. Comparison with mass model predictions.

doi: 10.1016/0375-9474(83)90513-4
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1982PA02      Phys.Rev. C25, 313 (1982)

R.L.Parks, S.T.Thornton, K.R.Cordell, C.-A.Wiedner

Entrance Channel Effects by Populating Resonances in the 26Al, 29Si, and 30Si Systems

NUCLEAR REACTIONS 13,12C(17O, 17O), (17O, α), E=30-57 MeV; 13C(17O, 13C), 12C(17O, 12C), E=30-57 MeV; 13C(16O, 16O), (16O, 13C), (16O, α), E=29.5-52.6 MeV; 10B(16O, 16O), (16O, 10B), (16O, α), E=42.4-60.1 MeV; measured σ(E); deduced reaction mechanism. 26Al, 29,30Si deduced high-spin nonresonant structures. Hauser-Feshbach analysis.

doi: 10.1103/PhysRevC.25.313
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1981CO03      Nucl.Phys. A352, 485 (1981)

K.R.Cordell, S.T.Thornton, L.C.Dennis, R.R.Doering, R.L.Parks, T.C.Schweizer

Proton-Inclusive Cross Sections from 600-MeV Proton-Nucleus Reactions

NUCLEAR REACTIONS 27Al, 181Ta(p, X), E=600 MeV; measured σ(θ, E). Natural targets.

doi: 10.1016/0375-9474(81)90425-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0061.


1981CO11      Phys.Rev. C23, 2035 (1981)

K.R.Cordell, C.-A.Wiedner, S.T.Thornton

Correlated Structures in the 14N + 12C Reaction

NUCLEAR REACTIONS 12C(14N, 14N), (14N, 12C), (14N, α), E=45-60 MeV; measured σ(E, θ); deduced reaction mechanism, quasimolecular entrance channel resonance, nonstatistical structure. Hauser-Feshbach analysis.

doi: 10.1103/PhysRevC.23.2035
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1981CO12      Nucl.Phys. A362, 431 (1981)

K.R.Cordell, S.T.Thornton, L.C.Dennis, R.R.Doering, R.L.Parks, T.C.Schweizer

Proton Inclusive Cross Sections from 720 MeV α-Nucleus Reactions

NUCLEAR REACTIONS Al, Ta(α, p), E=720 MeV; measured σ(Ep, θ); deduced reaction mechanism. Intranuclear cascade, knockout models.

doi: 10.1016/0375-9474(81)90503-0
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1981DE09      Nucl.Phys. A357, 521 (1981)

L.C.Dennis, K.R.Cordell, R.R.Doering, R.L.Parks, S.T.Thornton, J.L.C.Ford, Jr., J.Gomez Del Campo, D.Shapira

Search for Resonances in 12C(9Be, α)17O

NUCLEAR REACTIONS 12C(9Be, α), E=9-20 MeV; measured σ(E, θ); 12C(9Be, α), E=16.1, 17, 17.9 MeV; measured σ(θ). Natural targets. Hauser-Feshbach calculations, compound plus resonance, compound plus direct mechanisms.

doi: 10.1016/0375-9474(81)90234-7
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1980DE18      Phys.Rev. C22, 340 (1980)

L.C.Dennis, S.T.Thornton

Nonstatistical Structure in 12C(14N, α)22Na

NUCLEAR REACTIONS 12C(14N, α), E(cm)=10.1-15.9 MeV; measured σ(E); deduced correlated nonstatistical structure.

doi: 10.1103/PhysRevC.22.340
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1980PA19      Nucl.Phys. A348, 350 (1980)

R.L.Parks, S.T.Thornton, L.C.Dennis, K.R.Cordell

Comparison of Fusion Cross Sections for 12C+12C → 24Mg and 14N+10B → 24Mg

NUCLEAR REACTIONS 12C(12C, X), E=52.1, 72.1, 82.1, 92.1 MeV; 10B(14N, X), E=26.9, 50.9, 62.9, 74.9 MeV; measured σ(fragment θ, E, Z); deduced critical angular momenta for fusion, entrance channel effects. Statistical model residue cross sections, macroscopic model total fusion σ.

doi: 10.1016/0375-9474(80)90342-5
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1980TH02      Phys.Lett. 91B, 196 (1980)

S.T.Thornton, L.C.Dennis, K.R.Cordell

Resonances: Population of Low-Level Density Regions < Question >

NUCLEAR REACTIONS 14N, 12C, 10,11B, 7Li(14N, X), 16O, 15N, 11B(10B, X), 9Be, 12,13C(12C, X), 16O(9Be, X), 19F, 20Ne(6Li, X), E not given; 16O(12C, X), E(cm) ≈ 20 MeV; calculated excitation energy of yrast line. 28Si, 26Al, 25,24Mg, 21Ne deduced resonances. Entrance channel nuclear binding energies, shell model level densities.

doi: 10.1016/0370-2693(80)90429-3
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1980WI19      Phys.Lett. B97, 37 (1980)

C.-A.Wiedner, K.R.Cordell, W.Saathoff, S.T.Thornton, J.Bolger, E.Boschitz, G.Proebstle, J.Zichy

Neutron and Proton Components of Nuclear Transitions in Pion Inelastic Scattering on 26Mg

NUCLEAR REACTIONS 26Mg(π+, π+), (π-, π-), (π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ). 26Mg levels deduced neutron, proton nuclear transition matrix element ratio.

doi: 10.1016/0370-2693(80)90541-9
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1979CO11      Nucl.Phys. A323, 147 (1979)

K.R.Cordell, S.T.Thornton, L.C.Dennis, P.G.Lookadoo, T.C.Schweizer, J.L.C.Ford, Jr., J.Gomez del Campo, D.Shapira

The 12C(13C, α)21Ne Reaction: High-Spin States, Resonances and Coherence Widths

NUCLEAR REACTIONS 12C(13C, α), E=18.2-32.0 MeV; measured σ(E). 12C(13C, α), E=29-31 MeV; measured σ(θ). 21Ne deduced levels, J, π. 25Mg deduced coherence width, moment of inertia.

doi: 10.1016/0375-9474(79)90420-2
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1979DE08      Phys.Rev. C19, 777 (1979)

L.C.Dennis, S.T.Thornton, K.R.Cordell

Critical Analysis of Statistical Methods Used to Detect Resonances in Nuclear Reactions

NUCLEAR REACTIONS 12C(12C, α), E(cm)=18.0-25.5 MeV; 12C(14N, α), E(cm)=10.2-18.1 MeV; 12C(15N, α), E(cm)=9.5-17.3 MeV; measured nothing; calculated σ(E). Statistical model. Detection of resonances based on deviation functions, summed σ, distribution of maxima.

doi: 10.1103/PhysRevC.19.777
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1979SC08      Phys.Rev. C19, 1408 (1979)

T.C.Schweizer, R.R.Doering, S.T.Thornton, L.C.Dennis, K.R.Cordell, R.L.Parks

Nuclear Fragment Production from 720-MeV Alpha-Induced Reactions

NUCLEAR REACTIONS Al, Ag, Ta(α, Li), (α, 11B), (α, 12C), (α, 14N), (α, 16O), E=720 MeV; measured σ(E, θ). Analysis in terms of thermodynamic, evaporation, firestreak, pre-equilibrium emission models.

doi: 10.1103/PhysRevC.19.1408
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1979TH01      Phys.Rev. C19, 913 (1979)

S.T.Thornton, K.R.Cordell, L.C.Dennis, R.R.Doering, T.C.Schweizer

Back-Angle Production of Light Ions from 720-MeV α-Nucleus Collisions

NUCLEAR REACTIONS Al, Ag, Ta(α, p), (α, d), (α, t), (α, 3He), (α, α), E=720 MeV; measured σ(E, θ=150°). Natural targets. Compared with coalescence, fireball, firestreak, thermodynamic model calculations.

doi: 10.1103/PhysRevC.19.913
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1978CO04      Nucl.Phys. A296, 278 (1978)

K.R.Cordell, S.T.Thornton, L.C.Dennis, T.C.Schweizer, J.Gomez del Campo, J.L.C.Ford, Jr.

Statistical Model Analysis of the 12C(14N, α) Reaction and Coherence Widths in 26Al

NUCLEAR REACTIONS 12C(14N, α), E=22-39.2 MeV; measured σ(E). 26Al deduced average coherence Γ, moment of inertia. Hauser-Feshbach calculations.

doi: 10.1016/0375-9474(78)90073-8
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1978DO05      Phys.Rev.Lett. 40, 1433 (1978)

R.R.Doering, T.C.Schweizer, S.T.Thornton, L.C.Dennis, K.R.Cordell, K.O.H.Ziock, J.C.Comiso

Correlated Energy Spectra of Light Fragments from 720-MeV α-Induced Reactions

NUCLEAR REACTIONS 27Al, 107,109Ag, 181Ta(α, p), (α, d), (α, t), (α, 3He), (α, α), E=720 MeV; measured σ.

doi: 10.1103/PhysRevLett.40.1433
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1978TH01      Phys.Rev. C17, 576 (1978)

S.T.Thornton, D.E.Gustafson, K.R.Cordell, L.C.Dennis, T.C.Schweizer, J.L.C.Ford, Jr.

Levels in 23Na Populated by the 12C(15N, α) Reaction

NUCLEAR REACTIONS 12C(15N, α), E=36.0-39.2 MeV; measured σ(E, θ). 23Na deduced levels, K, J, π. Hauser-Feshbach analysis, natural target.

doi: 10.1103/PhysRevC.17.576
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1977RE08      Nucl.Phys. A283, 149 (1977)

H.Reiss, H.V.Klapdor, G.Rosner, J.L.C.Ford, Jr., S.T.Thornton

Enhanced 9Be Production in the 14N + 11B Reaction

NUCLEAR REACTIONS 11B(14N, 9Be), E=50 MeV; measured σ(E(9Be), θ). Hauser-Feshbach analysis.

doi: 10.1016/0375-9474(77)90704-7
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1976FR02      Nucl.Phys. A256, 93 (1976)

E.Friedland, M.Goldschmidt, C.A.Wiedner, J.L.C.Ford, Jr., S.T.Thornton

Spectroscopic Investigation of the 144Sm(3He, α)143Sm Reaction

NUCLEAR REACTIONS 144Sm(3He, α), (3He, 3He), E=30 MeV; measured σ(θ). 143Sm deduced levels, L, J, π, spectroscopic factors. Enriched target, θ=10-70°, Δθ=2.6°.

doi: 10.1016/0375-9474(76)90096-8
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1976GO07      Nucl.Phys. A262, 125 (1976)

J.Gomez del Campo, M.E.Ortiz, A.Dacal, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the Coherence Widths Γ in 28Si Measured by the 12C(16O, α) Reaction

NUCLEAR REACTIONS 12C(16O, α), E=40-46 MeV; measured σ(E) for θ=7°. 24Mg levels deduced Γ. 28Si deduced coherence widths. Hauser-Feshbach calculations, fluctuation analysis.

doi: 10.1016/0375-9474(76)90444-9
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1976GU05      Phys.Rev. C13, 691 (1976)

D.E.Gustafson, S.T.Thornton, T.C.Schweizer, J.L.C.Ford, Jr., P.D.Miller, R.L.Robinson, P.H.Stelson

High-Spin States of the Kπ = 3/2+ and 1/2+ Bands of 23Na

NUCLEAR REACTIONS 12C(15N, α), E=36-39.2 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π, K. Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.13.691
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1976TH04      Phys.Rev. C13, 1502 (1976)

S.T.Thornton, D.E.Gustafson, J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley

Inelastic Scattering and Transfer Reactions from 12C Ions on 90Zr

NUCLEAR REACTIONS 90Zr(12C, 12C), (12C, 11C), (12C, 11B), E=98 MeV; measured σ(θ); deduced optical model parameters. 90Zr deduced β. 91Zr, 91Nb levels deduced S.

doi: 10.1103/PhysRevC.13.1502
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1976TH05      Phys.Rev. C13, 1936 (1976)

S.T.Thornton, T.C.Schweizer, D.E.Gustafson, J.L.C.Ford, Jr., M.J.LeVine

Nuclear Structure Study of 141Nd, 143Nd, and 143Pm by 13C-Induced Reactions on 142Nd

NUCLEAR REACTIONS 142Nd(13C, 14C), (13C, 12C), (13C, 12B), E=67.5 MeV; measured σ(θ). 141,143Nd, 143Pm levels deduced L, J, π, S. DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.13.1936
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1976TH15      Nucl.Phys. A270, 428 (1976)

S.T.Thornton, T.C.Schweizer, D.E.Gustafson, J.L.C.Ford, Jr., M.J.Levine

Nuclear and Coulomb Deformation Parameters of 142Nd

NUCLEAR REACTIONS 142Nd(13C, 13C), (13C, 13C'), E=67.5 MeV; measured σ(E, θ). 142Nd levels deduced β(L), DWBA analyses. Enriched target. Resolution 70 keV; θ lab=20-75°, Δθ=1°.

doi: 10.1016/0375-9474(76)90455-3
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1976TO08      Phys.Rev. C14, 1471 (1976)

K.S.Toth, J.L.C.Ford, Jr., G.R.Satchler, E.E.Gross, D.C.Hensley, S.T.Thornton, T.C.Schweizer

Measurements and Analysis of the 208Pb(12C, 13C), (12C, 11B), and (12C, 14C) Reactions

NUCLEAR REACTIONS 208Pb(12C, 13C), (12C, 11B), E=77.4, 97.9, 116.4 MeV; 208Pb(12C, 14C), E=97.9 MeV; 207Pb(13C, 13C), E=86.1 MeV; 209Bi(11B, 11B), E=74.6 MeV; measured σ(θ). 209Bi, 207Pb levels deduced S. Optical model, DWBA analysis.

doi: 10.1103/PhysRevC.14.1471
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1975SA17      Phys.Lett. 60B, 43 (1975)

G.R.Satchler, J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley, E.E.Gross, D.E.Gustafson, S.T.Thornton

A Microscopic Description of Inelastic 12C Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(12C, 12C'), E=98 MeV; measured σ(E(12C'), θ). 208Pb deduced levels, J.

doi: 10.1016/0370-2693(75)90522-5
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1975TH09      Phys.Rev. C12, 877 (1975)

S.T.Thornton, J.L.C.Ford, Jr., E.Friedland, C.A.Wiedner, M.Goldschmidt

13C + 144Sm Neutron-Transfer Reaction

NUCLEAR REACTIONS 144Sm(13C, 13C), E=66 MeV; measured σ(θ); deduced optical model parameters. 144Sm(13C, 12C), E=66, 72 MeV; measured σ(E(12C), θ). 144Sm(13C, 14C), E=66, 72 MeV; measured σ(E(14C), θ). 143,145Sm levels deduced J, π, S.

doi: 10.1103/PhysRevC.12.877
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1974FO11      Nucl.Phys. A226, 189 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

States in 24Mg Populated by the 10B(16O, d)24Mg and 12C(16O, α)24Mg Reactions

NUCLEAR REACTIONS 10B(16O, d), E=44-46 MeV; 12C(16O, α), E=40-46 MeV; measured σ(E). 24Mg deduced levels, J.

doi: 10.1016/0375-9474(74)90401-1
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1974FO15      Z.Phys. 269, 147 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

Measurements and Hauser-Feshbach Analysis of the 10B(16O, 6Li)20Ne Reaction

NUCLEAR REACTIONS 10B(16O, 6Li), E=44.4-46 MeV; measured σ(E, E(6Li)). 20Ne deduced levels. Hauser-Feshbach calculations.

doi: 10.1007/BF01669056
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1974FO22      Phys.Rev. C10, 1429 (1974)

J.L.C.Ford, Jr., K.S.Toth, G.R.Satchler, D.C.Hensley, L.W.Owen, R.M.DeVries, R.M.Gaedke, P.J.Riley, S.T.Thornton

Single-Nucleon Transfer Reactions Induced by 11B Ions on 208Pb: A test of the distorted-wave born approximation

NUCLEAR REACTIONS 208Pb(11B, 10B), (11B, 12B), (11B, 10Be), (11B, 12C), E=72.2 MeV; measured σ(E(10B), θ), σ(E(12B), θ), σ(E(10Be), θ), σ(E(12C), θ). 209,207Pb, 209Bi, 207Tl levels deduced S.

doi: 10.1103/PhysRevC.10.1429
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1974GO10      Phys.Rev. C9, 1258 (1974)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the 10B(16O, α)22Na Reaction

NUCLEAR REACTIONS 10B(16O, α), E(16O)=40-46 MeV, measured σ(E) for θ(lab)=7°; E(16O)=46 MeV, measured σ(θ). 22Na deduced levels. Fluctuation analysis. Hauser-Feshbach calculations, suggested J values. Enriched targets.

doi: 10.1103/PhysRevC.9.1258
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1974MO03      Phys.Rev. C9, 924 (1974)

C.L.Morris, T.K.O'Malley, J.W.May, Jr., S.T.Thornton

Neutron-Proton Polarization Measurements Near 20-MeV Incident Neutron Energy

NUCLEAR REACTIONS 1H(polarized n, n), E=16.9, 21.1 MeV; measured P(θ).

doi: 10.1103/PhysRevC.9.924
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1974MO07      Phys.Rev. C9, 1687 (1974)

C.L.Morris, R.Rotter, W.Dean, S.T.Thornton

Polarization in n-d Scattering at 16.8- and 21.1-MeV Incident Neutron Energy

NUCLEAR REACTIONS 2H(polarized n, n), E=16.8, 21.1 MeV; measured P(θ).

doi: 10.1103/PhysRevC.9.1687
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1974TH02      Z.Phys. 266, 329 (1974)

S.T.Thornton, R.C.Jordan, C.L.Morris, R.P.Rotter

Neutron Polarizations from the 9Be(d, n)10B and 11B(d, n)12C Reactions

NUCLEAR REACTIONS 9Be, 11B(d, n), E=5.47, 5.34 MeV; measured n-polarization(θ).

doi: 10.1007/BF01674826
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1973ET01      Z.Phys. 264, 187 (1973)

M.P.Etten, S.T.Thornton

Investigation of States in 17F by the 15N(3He, n)17F Reaction

NUCLEAR REACTIONS 15N(3He, n), E=3.8, 4.8 MeV; measured σ(En, θ). 17F deduced levels, J, π, L, S.

doi: 10.1007/BF01396275
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1973FO17      Phys.Rev. C8, 1912 (1973)

J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley, R.M.Gaedke, P.J.Riley, S.T.Thornton

Interference between Coulomb and Nuclear Excitation in the Inelastic Scattering of 11B Ions from 208Pb

NUCLEAR REACTIONS 208Pb(11B, 11B), (11B, 11B'), E=72.2 MeV; measured σ(θ). Studied Coulomb, nuclear interference. DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.8.1912
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1973GO32      Phys.Lett. 46B, 180 (1973)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, J.B.McGrory, S.T.Thornton

Population of High Spin States in 22Na by Means of the 10B(16O, α) Reaction

NUCLEAR REACTIONS 10B(16O, α), E=46 MeV; measured σ(Eα, θ). 22Na deduced levels of high J.

doi: 10.1016/0370-2693(73)90677-1
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1972FO07      Nucl.Phys. A187, 624 (1972)

R.P.Fogel, S.T.Thornton

The 14N(d, n)15O Reaction at E = 5.16 MeV

NUCLEAR REACTIONS 14N(d, n), E=5.16 MeV; measured neutron P(En, θ); performed DWM analysis; studied reaction mechanism. Gas target.

doi: 10.1016/0375-9474(72)90686-0
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1972FO17      Nucl.Phys. A192, 391 (1972)

R.P.Fogel, S.T.Thornton

The Investigation of 16O States by the 15N(d, polarized n)16O Reaction

NUCLEAR REACTIONS 15N(d, n), E=4.83 MeV; measured neutron P(En, θ); performed DWM analysis; studied reaction mechanism. 16O levels deduced S. Gas target.

doi: 10.1016/0375-9474(72)90267-9
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1972SM03      Nucl.Phys. A186, 161 (1972)

J.R.Smith, S.T.Thornton

Measurements of 3H(p, n)3He Neutron Polarizations for E = 1.5 to 5.0 Mev

NUCLEAR REACTIONS 3H(p, n) , Ep=1.50, 1.75, 1.90, 2.26, 2.46, 2.70, 3.12, 3.50, 3.90, 4.41, 5.00 MeV; measured neutron P(En, θ); calculated Legendre polynomial expansion coefficients for σ(θ), P(θ)σ(θ). Gas target.

doi: 10.1016/0375-9474(72)90132-7
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1972SM04      Can.J.Phys. 50, 783 (1972)

J.R.Smith, S.T.Thornton

Measurements of D(d, n)3He Neutron Polarizations for Deuteron Energies from 0.87 to 5.00 MeV

NUCLEAR REACTIONS 2H(d, n), E=0.87-5.00 MeV; measured P(n)(E;θ); deduced Legendre coefficients.

doi: 10.1139/p72-111
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1972SM05      Nucl.Phys. A187, 433 (1972)

J.R.Smith, S.T.Thornton

Measurements of 3H(d, n)4He Neutron Polarizations for E = 1.0 to 5.0 Mev

NUCLEAR REACTIONS 3H(d, n), Ed=1.00, 1.50, 2.00, 3.00, 4.00, 4.35, 5.00 MeV; measured neutronp(En, θ). A contour map of P(θ) was produced from Legendre polynomial fits. Gas target.

doi: 10.1016/0375-9474(72)90587-8
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1972TH07      Phys.Lett. 39B, 623 (1972)

S.T.Thornton

Observation of a Missing State in 17F

NUCLEAR REACTIONS 15N(3He, n), E=3.79, 4.00, 4.80 MeV; measured σ(En, θ). 17F deduced 5.18 MeV level.

doi: 10.1016/0370-2693(72)90013-5
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1971TH03      Phys.Rev. C3, 1065 (1971)

S.T.Thornton, C.M.Jones, J.K.Bair, M.D.Mancusi, H.B.Willard

Test of Time-Reversal Invariance in the Reactions 16O(d, α)14N and 14N(α, d)16O

NUCLEAR REACTIONS 16O(d, α), E=3.6-5.3 MeV; 14N(α, d), 8.5-10 MeV; measured σ(E;θ); deduced consistency with detailed balance.

doi: 10.1103/PhysRevC.3.1065
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1971TH07      Nucl.Phys. A169, 131 (1971)

S.T.Thornton, C.L.Morris, J.R.Smith, R.P.Fogel

7Li(p, n)7Be Neutron Polarization Measurements for E = 3.0 to 5.5 MeV

NUCLEAR REACTIONS 7Li(p, n), Ep=3.0, 3.5, 4.0, 4.5, 5.0, 5.5 MeV; measured neutron P(En, θ). Contour maps of P(θ), P2(θ)σ(θ) are produced from Legendre polynomial fits.

doi: 10.1016/0375-9474(71)90567-7
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1971TH10      Nucl.Phys. A170, 485 (1971)

S.T.Thornton, R.P.Fogel, C.L.Morris

Polarization of Neutrons from the 16O(d, n)17F Reaction

NUCLEAR REACTIONS 16O(d, n), E=3.96-5.35 MeV; measured P(En, θ), P(E;En, θ=30° lab); studied reaction mechanism. Gas target.

doi: 10.1016/0375-9474(71)90230-2
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1969TH04      Nucl.Phys. A137, 531 (1969)

S.T.Thornton

The 16O(d, n)17F Reaction at E=8.0 and 9.3 MeV

NUCLEAR REACTIONS 16O(d, n), E = 8.0, 9.3 MeV; measured σ(En, θ). 17F levels deduced S. Natural target.

doi: 10.1016/0375-9474(69)90091-8
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1969TH05      Nucl.Phys. A136, 25 (1969)

S.T.Thornton

The D(d, n)3He Reaction from E = 5 to 10 MeV

NUCLEAR REACTIONS 2H(d, 3He), E = 5, 5.8, 9, 10 MeV; 2H(d, n), E = 5, 5.8 MeV; measured σ(En, θ); deduced Legendre polynomial fit.

doi: 10.1016/0375-9474(69)90036-0
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1966TH10      Phys.Rev.Lett. 17, 701 (1966)

S.T.Thornton, J.K.Bair, C.M.Jones, H.B.Willard

Search for the Trineutron

NUCLEAR REACTIONS 3H(n, p), E=20.8 MeV; measured reaction products, Ep, Ip; deduced lack of evidence for of bound 3n system.

doi: 10.1103/PhysRevLett.17.701
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