NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.T.Thornton Found 77 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1980DE18 Phys.Rev. C22, 340 (1980) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1973ET01 Z.Phys. 264, 187 (1973) 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
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
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
1972FO07 Nucl.Phys. A187, 624 (1972) 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
1972FO17 Nucl.Phys. A192, 391 (1972) 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
1972SM03 Nucl.Phys. A186, 161 (1972) 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
1972SM04 Can.J.Phys. 50, 783 (1972) 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
1972SM05 Nucl.Phys. A187, 433 (1972) 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
1972TH07 Phys.Lett. 39B, 623 (1972) 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
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
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
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
1969TH04 Nucl.Phys. A137, 531 (1969) 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
1969TH05 Nucl.Phys. A136, 25 (1969) 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
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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