NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.A.Gossett Found 21 matches. 1996BE13 Phys.Rev. C53, 1759 (1996) J.A.Behr, K.A.Snover, C.A.Gossett, G.Feldman, J.H.Gundlach, M.Kicinska-Habior Nonstatistical γ Emission in 3He- and α-Induced Reactions NUCLEAR REACTIONS 61Ni, 95Mo, 119,124Sn, 148,154Sm, 181Ta(α, γ), E=11-28 MeV; C, O, 61,62Ni, 95,96Mo, 120,124Sn, 148Sm, 181Ta(3He, γ), E=11-28 MeV; measured γ-ray production σ(Eγ) at θγ=90°; deduced systematics of nonstatistical γ-ray yields. Statistical model, direct plus semdirect excitation of the giant dipole resonance, including Coulomb, projectile excitation.
doi: 10.1103/PhysRevC.53.1759
1995ZE01 Phys.Rev. C51, 1494 (1995) V.J.Zeps, E.G.Adelberger, A.Garcia, C.A.Gossett, H.E.Swanson, W.Haeberli, P.A.Quin, J.Sromicki Parity Mixing of the 0+-0- I = 1 Doublet in 14N NUCLEAR REACTIONS, ICPND 13C(polarized p, p), E=1.1-2.2 MeV; 13C(p, γ), E=0.45-3 MeV; measured σ(E). 14N levels deduced ΔI=0 parity-mixing matrix element, levels parameters. Enriched targets. S-matrix analysis.
doi: 10.1103/PhysRevC.51.1494
1994KI03 Nucl.Phys. A569, 17c (1994) M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, Z.M.Drebi, M.S.Kaplan, D.P.Wells Shape Changes and Isospin Purity in Highly Excited Light Mass Nuclei NUCLEAR REACTIONS 27Al(12C, X), (18O, X), (19F, X), E not given; analyzed γ-spectra, σ(Eγ), Iγ(θ) data; deduced shape changes, isospin purity in hot nuclei. Other data discussed.
doi: 10.1016/0375-9474(94)90092-2
1994KO06 Phys.Rev. C49, 1715 (1994) M.Kohler, B.E.King, N.R.Stevenson, R.B.Schubank, Y.M.Shin, R.A.Ristinen, P.Amaudruz, P.P.J.Delheij, D.C.Healey, B.K.Jennings, D.F.Ottewell, G.Sheffer, G.R.Smith, G.D.Wait, J.T.Brack, A.Feltham, M.Hanna, R.R.Johnson, F.M.Rozon, V.Sossi, D.Vetterli, P.Weber, N.Grion, R.Rui, E.L.Mathie, R.Tacik, M.Yeomans, C.A.Gossett, G.J.Wagner, J.M.Lee, K.S.Chung Vector Analyzing Power iT11 in πd Elastic Scattering at 49 MeV NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E=49 MeV; measured iT11(θ); deduced πNP11 amplitude role. Model comparison. Dynamically polarized target, magnetic spectrometer.
doi: 10.1103/PhysRevC.49.1715
1993BE17 Phys.Rev.Lett. 70, 3201 (1993) J.A.Behr, K.A.Snover, C.A.Gossett, M.Kicinska-Habior, J.H.Gundlach, Z.M.Drebi, M.S.Kaplan, D.P.Wells Restoration of Isospin Symmetry in Highly Excited Compound Nuclei NUCLEAR REACTIONS 12C, 13C(16O, X), (18O, X), (13C, X), (14N, X), (15N, X), E=22-108 MeV; measured γ production σ. 28Si, 26Al deduced isospin admixture, spreading widths.
doi: 10.1103/PhysRevLett.70.3201
1993FE01 Phys.Rev. C47, 1436 (1993) G.Feldman, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, M.Kicinska-Habior Statistical γ Decay of the Giant Dipole Resonance in Highly Excited 46Ti and 52Cr NUCLEAR REACTIONS 27Al(19F, X), E=30-60 MeV; 48Ti(α, X), E=12-28 MeV; measured inclusive γ production σ(E). 46Ti, 52Cr deduced GDR built on excited states, parameters.
doi: 10.1103/PhysRevC.47.1436
1993KI12 Phys.Lett. 308B, 225 (1993) M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, Y.Alhassid, N.Whelan Search for a Phase Transition in the Nuclear Shape at Finite Temperature and Rapid Rotation NUCLEAR REACTIONS 27Al(18O, X), E=44.9-109.6 MeV; measured Eγ, Iγ; deduced σ(E). 45Sc deduced GDR strength function, deformation features. Liquid drop model.
doi: 10.1016/0370-2693(93)91276-S
1992KI01 Phys.Rev. C45, 569 (1992) M.Kicinska-Habior, K.A.Snover, J.A.Behr, C.A.Gossett, J.H.Gundlach, G.Feldman Comparison of Giant Dipole Resonance Decay in Stiff 92Mo and Soft 100Mo Excited Nuclei NUCLEAR REACTIONS 76Se(17O, X), E=50, 72.2 MeV; 82Se(18O, X), E=49.1-72.8 MeV; measured σ(Eγ), θ=90°. 92,100Mo deduced GDR built on excited states, decay features.
doi: 10.1103/PhysRevC.45.569
1991LU03 Phys.Rev. C44, 1548 (1991) S.J.Luke, C.A.Gossett, R.Vandenbosch Search for High Energy γ Rays from the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured γγ-, fission fragment(γ)-coin; deduced γ-production mechanism. Classical model, fission fragment Coulomb acceleration.
doi: 10.1103/PhysRevC.44.1548
1990GO23 Phys.Rev. C42, R1800 (1990) C.A.Gossett, J.A.Behr, S.J.Luke, B.T.McLain, D.P.Rosenzweig, K.A.Snover, W.T.Hering High-Energy Gamma Emission in Heavy-Ion Collisions at 9-14 MeV/Nucleon NUCLEAR REACTIONS 92,100Mo(12C, X), E=9-14 MeV/nucleon; measured σ(E, Eγ); 92,100Mo(12C, X), E=11 MeV/nucleon; measured σ(θ, Eγ); 92,100Mo(13C, X), E=10, 11 MeV/neucleon; measured σ(Eγ). Enriched targets. Comparision with collective and nucleon-nucleon bremsstrahlung photon production mechanisms.
doi: 10.1103/PhysRevC.42.R1800
1990GU20 Phys.Rev.Lett. 65, 2523 (1990) J.H.Gundlach, K.A.Snover, J.A.Behr, C.A.Gossett, M.Kicinska-Habior, K.T.Lesko Oblate Deformed Shapes of Hot Rotating Nuclei Deduced from Giant-Dipole-Resonance Decay Studies NUCLEAR REACTIONS 72Ge(18O, X), E=50, 74 MeV; 64Ni(28Si, X), E=137 MeV; measured Eγ, Iγ, σ(Eγ), γ(θ). 90Zr, 92Mo deduced GDR parameters, shape features. Hot rotating nuclei.
doi: 10.1103/PhysRevLett.65.2523
1990KI04 Phys.Rev. C41, 2075 (1990) M.Kicinska-Habior, K.A.Snover, J.A.Behr, G.Feldman, C.A.Gossett, J.H.Gundlach Spin Dependence of the Giant-Dipole-Resonance Strength Function in Highly Excited Nuclei in the Mass Region A = 39-45 NUCLEAR REACTIONS, ICPND 27Al(12C, X), E=33.8-62.7 MeV; 27Al(13C, X), E=39.7 MeV; 27Al(15N, X), E=29.2, 44.7 MeV; 27Al(18O, X), E=31.5-72.5 MeV; measured continuum Eγ, Iγ, γ(θ); deduced fusion σ. 39,40K, 42Ca, 45Sc deduced GDR strength function.
doi: 10.1103/PhysRevC.41.2075
1990ST24 Phys.Rev.Lett. 65, 1987 (1990) N.R.Stevenson, R.B.Schubank, Y.M.Shin, P.Amaudruz, P.P.J.Delheij, D.C.Healey, B.K.Jennings, D.F.Ottewell, G.Sheffer, G.R.Smith, G.D.Wait, J.T.Brack, A.Feltham, M.Hanna, R.R.Johnson, F.M.Rozon, V.Sossi, D.Vetterli, P.Weber, N.Grion, R.Rui, M.Kohler, R.A.Ristinen, E.L.Mathie, R.Tacik, M.Yeomans, C.A.Gossett, G.J.Wagner Role of the πN P11 Interaction in πd Elastic Scattering at 50 MeV NUCLEAR REACTIONS 2H(π+, π+), E=50 MeV; measured iT11(θ); deduced πN(P11) interaction amplitude role. Dynamically polarized target.
doi: 10.1103/PhysRevLett.65.1987
1990ST33 J.Phys.(Paris), Colloq.C-6, 391 (1990) N.R.Stevenson, R.B.Schubank, Y.M.Shin, P.Amaudruz, P.P.J.Delheij, D.C.Healey, B.K.Jennings, D.F.Ottewell, G.Sheffer, G.R.Smith, G.D.Wait, N.Grion, R.Rui, J.T.Brack, A.Feltham, M.Hanna, R.R.Johnson, F.M.Rozon, V.Sossi, D.Vetterli, P.Weber, M.Kohler, R.A.Ristinen, E.L.Mathie, R.Tacik, M.Yeomans, C.A.Gossett, G.J.Wagner, B.E.King Analyzing Power Measurements in πd Elastic Scattering at 50 MeV NUCLEAR REACTIONS 2H(π, π), E=50 MeV; measured iT11(θ); deduced πN(P11) potential role.
1988GO05 J.Phys.(London) G14, Supplement S267 (1988) C.A.Gossett, J.A.Behr, G.Feldman, J.H.Gundlach, M.Kicinska-Habior, K.A.Snover Systematic Behaviour of the Giant Dipole Resonance in Highly Excited Nuclei NUCLEAR REACTIONS 154Sm(12C, X), E=61.2 MeV; calculated σ(Eγ, E). 166Er deduced GDR role. NUCLEAR STRUCTURE 108Sn, 140Ce, 156,166Er; calculated photoabsorption σ; deduced GDR role.
doi: 10.1088/0305-4616/14/S/028
1988MU06 J.Phys.(London) G14, Supplement S275 (1988) T.Murakami, C.A.Gossett, I.Halpern, D.P.Rosenzweig, D.W.Storm, D.R.Tieger, P.T.Debevec, A.Freytag, L.J.Morford, S.A.Wender, D.H.Dowell Photoneutron Studies of the Giant Isovector Quadrupole Resonance in Calcium, Cadmium, and Lead NUCLEAR REACTIONS Ca, Cd, Pb(γ, n), E=28-39 MeV bremsstrahlung; measured σ(θ), neutron asymmetry; deduced electric dipole, quadrupole amplitude interference role.
doi: 10.1088/0305-4616/14/S/029
1987KI17 Phys.Rev. C36, 612 (1987) M.Kicinska-Habior, K.A.Snover, C.A.Gossett, J.A.Behr, G.Feldman, H.K.Glatzel, J.H.Gundlach, E.F.Garman Statistical Giant Dipole Resonance Decay of Highly Excited States of 63Cu NUCLEAR REACTIONS 59Co(α, γ), E=17.8-28.4 MeV; 57Fe(6Li, X), E=13.9-36 MeV; 51V(12C, X), E=26.3-64.7 MeV; 45Sc(18O, X), E=39.9-75.1 MeV; measured σ(Eγ). 63Cu deduced giant dipole resonance parameters. 62,63Cu, 60,62Ni, 59Co, 56Fe deduced level densities. NaI detector. Statistical model analyses.
doi: 10.1103/PhysRevC.36.612
1987ST26 Can.J.Phys. 65, 677 (1987) D.W.Storm, I.Halpern, C.A.Gossett, T.Murakami, D.P.Rosenzweig, D.R.Tieger, P.T.Debevec, A.Freytag, L.J.Morford, S.A.Wender, D.H.Dowell (γ, n) Studies of the Giant Isovector E2 Resonance in Lead, Cadmium, and Calcium NUCLEAR REACTIONS Ca, Cd, Pb(γ, n), E=20-40 MeV; measured σ(En), σ(θn), asymmetries; deduced giant isovector, quadrupole resonance parameters. Natural targets. Direct semdirect calculations.
doi: 10.1139/p87-096
1985AD10 Phys.Rev.Lett. 55, 2129 (1985) E.G.Adelberger, P.B.Fernandez, C.A.Gossett, J.L.Osborne, V.J.Zeps Does the Cabibbo Angle Vanish in Fermi Matrix Elements of High-J States ( Question ) RADIOACTIVITY 24Al(β+) [from 24Mg(p, n), E=18 MeV]; measured Eγ, Iγ, T1/2; deduced ft, vector coupling constant, no evidence for Cabibbo angle vanishing in high spin states. 24Mg levels deduced absolute β+-branching ratios.
doi: 10.1103/PhysRevLett.55.2129
1985GO04 Phys.Rev.Lett. 54, 1486 (1985) C.A.Gossett, K.A.Snover, J.A.Behr, G.Feldman, J.L.Osborne Deformation of Heated Nuclei Observed in the Statistical Decay of the Giant Dipole Resonance NUCLEAR REACTIONS 154,148Sm(12C, X), E=63 MeV; measured Eγ, Iγ, continuum spectra, σ(Eγ). 160,166Er deduced excited state based GDR parameters, splitting, deformation at high temperature.
doi: 10.1103/PhysRevLett.54.1486
1981GO05 Phys.Rev. C23, 1815 (1981) C.A.Gossett, L.D.Knutson, P.A.Quin Configuration of States in 201Bi from 209Bi(d(pol), p) NUCLEAR REACTIONS 209Bi(polarized d, p), E=12 MeV; measured σ(θ), iT11(θ). Natural target.
doi: 10.1103/PhysRevC.23.1815
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