NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = K.A.Snover Found 89 matches. 2011AD03 Rev.Mod.Phys. 83, 195 (2011) E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel Solar fusion cross sections. II. The pp chain and CNO cycles NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.
doi: 10.1103/RevModPhys.83.195
2011SA12 Phys.Rev. C 83, 034611 (2011) A.L.Sallaska, C.Wrede, A.Garcia, D.W.Storm, T.A.D.Brown, C.Ruiz, K.A.Snover, D.F.Ottewell, L.Buchmann, C.Vockenhuber, D.A.Hutcheon, J.A.Caggiano, J.Jose Absolute determination of the 22Na( p, γ )23Mg reaction rate in novae NUCLEAR REACTIONS 22Na(p, γ), E=150-700 keV; measured Eγ, Iγ; deduced absolute yields, excitation functions for resonances, resonance strengths and thermonuclear reaction rates. 23Mg; deduced levels, J, π, branching ratios, resonances. Estimated flux of 22Na gamma rays from novae.
doi: 10.1103/PhysRevC.83.034611
2010JU01 Phys.Rev. C 81, 012801 (2010) A.R.Junghans, K.A.Snover, E.C.Mohrmann, E.G.Adelberger, L.Buchmann Updated S factors for the 7Be(p, γ)8B reaction NUCLEAR REACTIONS 7Be(p, γ)8B, E(cm)=0-2500 keV; analyzed previous data for σ using detailed target analysis and improved stopping powers; deduced updated astrophysical S-factors.
doi: 10.1103/PhysRevC.81.012801
2010SA26 Phys.Rev.Lett. 105, 152501 (2010) A.L.Sallaska, C.Wrede, A.Garcia, D.W.Storm, T.A.D.Brown, C.Ruiz, K.A.Snover, D.F.Ottewell, L.Buchmann, C.Vockenhuber, D.A.Hutcheon, J.A.Caggiano Direct Measurements of 22Na(p, γ)23Mg Resonances and Consequences for 22Na Production in Classical Novae NUCLEAR REACTIONS 22Na(p, γ), E not given; measured Eγ, Iγ; deduced proton resonances energies and strengths, σ, reaction rates.
doi: 10.1103/PhysRevLett.105.152501
2007BA41 Phys.Rev. C 75, 058801 (2007) E0 emission in α + 12C fusion at astrophysical energies NUCLEAR REACTIONS 12C(α, γ), E(cm)< 1.5 MeV; calculated the contribution of E0 emission compared to E1 and E2 emissions.
doi: 10.1103/PhysRevC.75.058801
2007BR32 Phys.Rev. C 76, 055801 (2007) T.A.D.Brown, C.Bordeanu, K.A.Snover, D.W.Storm, D.Melconian, A.L.Sallaska, S.K.L.Sjue, S.Triambak 3He+4He → 7Be astrophysical S factor NUCLEAR REACTIONS 3He(α, γ)7Be, E(cm)=0.33-1.23 MeV; measured Eγ, Iγ, cross sections; deduced astrophysical S-factors.
doi: 10.1103/PhysRevC.76.055801
2005ES02 Phys.Rev.Lett. 94, 042502 (2005) H.Esbensen, G.F.Bertsch, K.A.Snover Reconciling Coulomb Dissociation and Radiative Capture Measurements NUCLEAR REACTIONS Pb(8B, p7Be), E=51.9 MeV/nucleon; calculated relative energy spectra, angular distributions. 7Be(p, γ), E=low; analyzed astrophysical S-factor data.
doi: 10.1103/PhysRevLett.94.042502
2005JU03 Nucl.Phys. B(Proc.Supp.) S138, 112 (2005) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.Laird, S.Park, A.Y.Zyuzin The new Seattle-TRIUMF 7Be(p, γ)8B S-factor determination NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1016/j.nuclphysbps.2004.11.028
2005SN03 Nucl.Phys. A758, 685c (2005) K.A.Snover, A.R.Junghans, E.C.Mohrmann, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird The 7Be(p, γ)8B astrophysical S-factor
doi: 10.1016/j.nuclphysa.2005.05.122
2004JU08 Nucl.Phys. A746, 210c (2004) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.R.Buchmann, A.M.Laird, S.Park, A.Y.Zyuzin New determination of the 7Be(p, γ)8B S-factor NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460 MeV; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.09.035
2003HE03 Phys.Lett. B 555, 43 (2003) P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner Low-temperature measurement of the giant dipole resonance width NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured particle spectra, Eγ, Iγ, (particle)γ-coin. 120Sn deduced width of GDR built on excited states, influence of thermal shape fluctuations. Comparison with model predictions.
doi: 10.1016/S0370-2693(03)00017-0
2003JU04 Phys.Rev. C 68, 065803 (2003) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin, A.M.Laird Precise measurement of the 7Be(p, γ)8B S factor NUCLEAR REACTIONS 7Be(p, γ), E(cm)=116-2460; measured σ; deduced astrophysical S-factors. Comparison with previous results.
doi: 10.1103/PhysRevC.68.065803
2003PA33 Nucl.Phys. A718, 113c (2003) S.H.Park, A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, A.Zyuzin, A.Laird A new measurement of 7Be(p, γ)8B cross section and its astrophysical meaning NUCLEAR REACTIONS 7Be(p, γ), E=221, 1379 keV; measured σ; deduced astrophysical S-factor.
doi: 10.1016/S0375-9474(03)00687-0
2003SN01 Phys.Rev. C 67, 055801 (2003) Is e+e-pair emission important in the determination of the 3He+4He S factor? NUCLEAR REACTIONS 4He(3He, X)7Be, E(cm) ≈ 0-3 MeV; calculated E0 and E1 pair emission and internal conversion contributions to capture σ.
doi: 10.1103/PhysRevC.67.055801
2002JU01 Phys.Rev.Lett. 88, 041101 (2002) A.R.Junghans, E.C.Mohrmann, K.A.Snover, T.D.Steiger, E.G.Adelberger, J.M.Casandjian, H.E.Swanson, L.Buchmann, S.H.Park, A.Zyuzin 7Be(p, γ)8B Astrophysical S Factor from Precision Cross Section Measurements NUCLEAR REACTIONS 7Be(p, γ), E(cm)=186-1200 keV; measured σ; deduced astrophysical S-factor.
doi: 10.1103/PhysRevLett.88.041101
2001HE17 Nucl.Phys. A687, 225c (2001) P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner Temperature Dependence of the GDR Width in 120Sn NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured Eγ, (recoil)γ-coin, excitation energy spectra, preliminary GDR parameters. Comparison with α-induced reaction data.
doi: 10.1016/S0375-9474(01)00625-X
2001KI07 Acta Phys.Pol. B32, 825 (2001) M.Kicinska-Habior, Z.Trznadel, M.P.Kelly, J.P.S.van Schagen, K.A.Snover Giant Dipole Resonance Studied in Heavy-Ion Reactions at Projectile Energies 6-11 MeV/u
2001KU10 Nucl.Phys. A687, 212c (2001) D.Kusnezov, Y.Alhassid, K.A.Snover, W.E.Ormand Giant Dipole Resonances in Hot, Rotating Nuclei: Nuclear shapes and shell corrections NUCLEAR STRUCTURE Sc, Cu, Zr, Mo, Sn, Dy, Pb; calculated GDR width vs temperature and angular momentum. 92,96,100Mo; calculated GDR width as a function of temperature and angular momentum. 44Ti, 90Zr, 120Sn, 168Er, 208Pb; calculated deformation parameters vs temperature and spin for hot rotating nuclei. Shell effects discussed, comparison with data.
doi: 10.1016/S0375-9474(01)00623-6
2001SN01 Nucl.Phys. A687, 337c (2001) The Giant Dipole Resonance Strength and Width at High Temperature NUCLEAR REACTIONS 90Zr(36Ar, X), E not given; calculated compound nucleus γ multiplicities vs excitation energy, GDR widths and GDR inhibition factor. Statistical Model, equilibration times discussed.
doi: 10.1016/S0375-9474(01)00640-6
2001TR09 Nucl.Phys. A687, 198c (2001) Z.Trznadel, M.Kicinska-Habior, M.P.Kelly, J.P.S.van Schagen, K.A.Snover Giant Dipole Resonance in Hot Se Nuclei and Bremsstrahlung Emission in 12C + 58, 64Ni Experiments at 6-11 MeV/u NUCLEAR REACTIONS 58,64Ni(12C, X), E=5.5-11 MeV/nucleon; measured Eγ, Iγ(θ), γγ-coin. 70Se, 76Se deduced GDR parameters. Statistical model calculations including precompound effects.
doi: 10.1016/S0375-9474(01)00621-2
2000KI16 Acta Phys.Pol. B31, 423 (2000) M.Kicinska-Habior, K.A.Snover, J.A.Behr, Z.M.Drebi, O.Kijewska Bremsstrahlung Radiation in Heavy-Ion Collisions 18O + 27Al → 45Sc at 8.3 MeV/u NUCLEAR REACTIONS 27Al(18O, X), E=8.3 MeV/nucleon; measured Eγ, Iγ(θ). 45Sc deduced GDR parameters. Transport model calculations.
1999KE02 Phys.Rev.Lett. 82, 3404 (1999) M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel Giant Dipole Resonance in Highly Excited Nuclei: Does the width saturate ? NUCLEAR REACTIONS 100Mo(18O, X), E=122-214 MeV; measured Eγ, Iγ(θ), proton-, α-spectra; deduced pre-equilibrium emission features. 118Sn deduced GDR parameters, no saturation of width.
doi: 10.1103/PhysRevLett.82.3404
1999KE06 Nucl.Phys. A649, 123c (1999) M.P.Kelly, K.A.Snover, J.P.S.van Schagen, M.Kicinska-Habior, Z.Trznadel The GDR Width in Hot Sn Nuclei NUCLEAR REACTIONS 100Mo(18O, xnypzα), E=125, 150, 169, 200, 217 MeV; measured Eγ, Iγ(θ), γ multiplicity, (charged particle)γ-coin; deduced GDR width vs temperature.
doi: 10.1016/S0375-9474(99)00049-4
1999KI14 Nucl.Phys. A649, 130c (1999) M.Kicinska-Habior, Z.Trznadel, A.Maj, M.P.Kelley, J.P.S.van Schagen, K.A.Snover Giant Dipole Resonances Decay and Bremsstrahlung Emission as a Source of High Energy γ-Rays in 12C + 24, 26Mg and 12C + 58, 64Ni Reactions at 6-11 MeV/u NUCLEAR REACTIONS 24,26Mg, 58,64Ni(12C, X), E=6-11 MeV/nucleon; measured Eγ, Iγ(θ); deduced GDR, bremsstrahlung parameters.
doi: 10.1016/S0375-9474(99)00050-0
1999KU14 Nucl.Phys. A649, 193c (1999) D.Kusnezov, Y.Alhassid, K.A.Snover Systematics of the Nuclear Giant Dipole Resonance NUCLEAR STRUCTURE A=45-208; analyzed GDR widths vs temperature, spin, mass; deduced phenomenological function. Liquid drop, Nilsson-Strutinsky approaches.
doi: 10.1016/S0375-9474(99)00059-7
1998AD12 Rev.Mod.Phys. 70, 1265 (1998) E.G.Adelberger, S.M.Austin, J.B.Bahcall, A.B.Balantekin, G.Bogaert, L.S.Brown, L.Buchmann, F.E.Cecil, A.E.Champagne, L.de Braeckeleer, C.A.Duba, S.R.Elliott, S.J.Freedom, M.Gai, G.Goldring, C.R.Gould, A.Gruzinov, W.C.Haxton, K.M.Heeger, E.Henley, C.W.Johnson, M.Kamionkowski, R.W.Kavanagh, S.E.Koonin, K.Kubodera, K.Langanke, T.Motobayashi, V.Pandharipande, P.Parker, R.G.H.Robertson, C.Rolfs, R.F.Sawyer, N.Shaviv, T.D.Shoppa, K.A.Snover, E.Swanson, R.E.Tribble, S.Turck-Chieze, J.F.Wilkerson Solar Fusion Cross Sections NUCLEAR REACTIONS 7Be, 12,13C, 15N, 16,17,18O(p, γ), 14,15N, 17,18O(p, α), 7Li(d, p), 3He(p, e+), (α, γ), (3He, 2p), 1H(p, e+), E=low; compiled, analyzed S-factor data, calculations; deduced implications for solar neutrino flux calculations.
doi: 10.1103/RevModPhys.70.1265
1998KU16 Phys.Rev.Lett. 81, 542 (1998) D.Kusnezov, Y.Alhassid, K.A.Snover Scaling Properties of the Giant Dipole Resonance Width in Hot Rotating Nuclei NUCLEAR STRUCTURE A=45-208; compiled, analyzed GDR widths vs temperature, spin, mass; deduced phenomenological formula.
doi: 10.1103/PhysRevLett.81.542
1997KE12 Phys.Rev. C56, 3201 (1997) M.P.Kelly, J.F.Liang, A.A.Sonzogni, K.A.Snover, J.P.S.van Schagen, J.P.Lestone Preequilibrium Particle Emission and the Giant-Dipole Resonance in Sn Nuclei NUCLEAR REACTIONS 100Mo(18O, X), E=200 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra; deduced pre-equilibrium emission features. 115In, 118Sn deduced GDR pre-equilibrium emission effects.
doi: 10.1103/PhysRevC.56.3201
1997KI13 Acta Phys.Pol. B28, 189 (1997) M.Kicinska-Habior, Z.Trznadel, K.A.Snover, A.Maj, M.P.Kelly New Results in High-Energy γ-Ray Studies from Heavy-Ion Reactions at Around 10 MeV/u NUCLEAR REACTIONS 26Mg(12C, X), E=6, 8.5, 11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced GDR, bremsstrahlung parameters. Statistical models, BUU nuclear transport equation.
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
1995DE18 Phys.Rev. C51, 2778 (1995); Erratum Phys.Rev. C52, 3509 (1995) L.De Braeckeleer, E.G.Adelberger, J.H.Gundlach, M.Kaplan, D.Markoff, A.M.Nathan, W.Schieff, K.A.Snover, D.W.Storm, K.B.Swartz, D.Wright, B.A.Brown Radiative Decays of the 16.6 and 16.9 MeV States in 8Be and Tests of the Conservation of the Vector Current in the A = 8 Multiplet NUCLEAR REACTIONS, ICPND 4He(α, γ), E=33-34.7 MeV; measured γ yield vs E, Iγ(θ). 8Be deduced doublet decay features, δ(E2/M1), Γγ, B(λ). Other A=8 nuclei data included in analysis, vector current conservation features discussed.
doi: 10.1103/PhysRevC.51.2778
1995DR05 Phys.Rev. C52, 578 (1995) Z.M.Drebi, K.A.Snover, A.W.Charlop, M.S.Kaplan, D.P.Wells, D.Ye, Y.Alhassid Spin-Induced Shape Changes in Light-Medium Mass Compound Nuclei NUCLEAR REACTIONS 27Al(32S, X), E=90-215 MeV; 45Sc(18O, X), E=54-149 MeV; measured γ(θ), production σ. 59,63Cu deduced GDR characteristics.
doi: 10.1103/PhysRevC.52.578
1995KI13 Acta Phys.Pol. B26, 439 (1995) M.Kicinska-Habior, K.A.Snover, A.Maj, Z.Drebi, D.Ye, M.Kelly Ultradipole Radiation from Low-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 26Mg(12C, X), E=6-11 MeV/nucleon; 24Mg(12C, X), E=11 MeV/nucleon; measured Eγ, Iγ(θ); deduced ultradipole radiation related features.
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
1993AD09 Phys.Lett. 314B, 185 (1993) E.G.Adelberger, L.De Braeckeleer, W.C.Haxton, K.A.Snover Accelerator Calibration of Solar Neutrino Detectors NUCLEAR REACTIONS 12C(p, n), E not given; calculated neutrino flux from 12N source.
doi: 10.1016/0370-2693(93)90447-P
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
1993KI08 Acta Phys.Pol. B24, 433 (1993) Evidence for a Shape Change of Hot, Fast Rotating 45Sc Nuclei from GDR Studies NUCLEAR REACTIONS 27Al(18O, X), E=44.9-109.6 MeV; measured γ-spectral shapes; deduced absorption σ(Eγ). 45Sc deduced structure near GDR, shape change evidence. Hot rotating nuclei.
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
1993SN01 Nucl.Phys. A553, 153c (1993) The Giant Dipole Resonance at High Excitation Energy and Spin NUCLEAR REACTIONS 45Sc, 28,30Si(γ, X), E ≤ 30 MeV; compiled, reviewed σ(E). 92Zr(58Ni, X), E=241 MeV; compiled, reviewed inclusive Eγ, Iγ data, calculations.
doi: 10.1016/0375-9474(93)90621-4
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
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
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
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
1986HA30 Phys.Lett. 176B, 297 (1986) M.N.Harakeh, D.H.Dowell, G.Feldman, E.F.Garman, R.Loveman, J.L.Osborne, K.A.Snover Role of Isospin in the Statistical Decay of the Giant Dipole Resonance Built on Excited States NUCLEAR REACTIONS 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40.2 MeV; 12C(12C, γ), 12,13C(13C, γ), E=40 MeV; measured σ vs Eγ, γ yields. 28Si, 24,25,26Mg deduced GDR, Γ, EWSR, T-mixing parameters.
doi: 10.1016/0370-2693(86)90167-X
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
1984SN01 J.Phys.(Paris), Colloq.C-4, 337 (1984) Giant Resonances Built on Highly Excited States NUCLEAR REACTIONS 27Al(p, γ), E=22 MeV; 28Si(p, γ), E=11-39 MeV; 11B(p, γ), E=29.5 MeV; calculated σ(Eγ, θγ), σ(E). 25Mg(3He, γ), E=11.8 MeV; 12C(16O, γ), E=40 MeV; 64Ni(12C, γ), 58Ni(18O, γ), E not given; calculated σ(Eγ). 28Si(γ, p), E=15.6-22.5 MeV; calculated branching ratios. 130Te(34S, γ), E=141 MeV; 124Sn(29Si, γ), E=127 MeV; 60Ni(18O, γ), E=60 MeV; 28Si(18O, γ), E=40 MeV; calculated transition number per reaction.
1983DO03 Phys.Rev.Lett. 50, 1191 (1983) D.H.Dowell, G.Feldman, K.A.Snover, A.M.Sandorfi, M.T.Collins Excited-State Giant Dipole Resonances in (p, γ): A new probe of single-particle strengths NUCLEAR REACTIONS 27Al(p, γ), E=11-39 MeV; measured Eγ, Iγ, σ(θγ) vs Eγ. 28Si deduced GDR, Γ, configuration.
doi: 10.1103/PhysRevLett.50.1191
1983EA01 Nucl.Phys. A396, 221c (1983) E.D.Earle, A.B.McDonald, E.G.Adelberger, K.A.Snover, H.E.Swanson, R.von Lintig, H.B.Mak, C.A.Barnes Parity Mixing in 21Ne; Evidence for weak neutral currents in nuclei NUCLEAR STRUCTURE 18,19F, 21Ne; analyzed data; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. NUCLEAR REACTIONS 21Ne(p, p'γ), E=4.08 MeV; measured Eγ, Iγ, γ CP; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. 21Ne levels deduced parity mixing matrix element. Parity mixing input from 19,18F data.
doi: 10.1016/0375-9474(83)90021-0
1983GA19 Phys.Rev. C28, 2554 (1983) E.F.Garman, K.A.Snover, S.H.Chew, S.K.B.Hesmondhalgh, W.N.Catford, P.M.Walker Giant Dipole Resonance in the Statistical Decay of 63Cu, 76Kr, and 127Cs Compound Nuclei NUCLEAR REACTIONS, ICPND 51V, 64Zn, 115In(12C, γ), 45Sc, 58Ni, 109Ag(18O, γ), E=42-60 MeV; measured σ vs Eγ. 63Cu, 76Kr, 127Cs deduced average angular momentum, GDR parameters. Statistical model.
doi: 10.1103/PhysRevC.28.2554
1983HO05 Phys.Rev. C27, 1244 (1983) C.D.Hoyle, E.G.Adelberger, J.S.Blair, K.A.Snover, H.E.Swanson, R.D.Von Lintig Isospin Mixing in 24Mg RADIOACTIVITY 24Al(β+) [from 24Mg(p, n)]; measured βγ CP asymmetry, Eγ, Iγ; deduced isospin forbidden transition matrix element. 24Mg levels deduced isospin mixing.
doi: 10.1103/PhysRevC.27.1244
1983KU01 Phys.Rev. C27, 948 (1983) E.Kuhlmann, K.A.Snover, G.Feldman, M.Hindi Alpha Capture into the Giant Quadrupole Resonance in 28Si NUCLEAR REACTIONS, ICPND 24Mg(α, γ), E=4.3-14 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ); deduced E1, E2 capture σ. 28Si deduced E1, E2 transition strengths. Enriched target. Hauser-Feshbach formalism, isospin effects.
doi: 10.1103/PhysRevC.27.948
1983SN02 Phys.Rev. C27, 493 (1983) K.A.Snover, G.Feldman, M.M.Hindi, E.Kuhlmann, M.N.Harakeh, M.Sasao, M.Noumachi, Y.Fujita, M.Fujiwara, K.Hosono 27Al(p, γ)28Si and 27Al(3He, d)28Si to the Stretched 11.58 MeV (6-, 0) and 14.36 MeV (6-, 1) Levels NUCLEAR REACTIONS 27Al(p, γ), E ≈ 2876 keV; measured σ(Eγ, E). 28Si resonance deduced Γ, Γp, Γγ, configuration, B(M1). 27Al(3He, d), E=40, 60 MeV; measured σ(θ); deduced optical model parameters. 28Si levels deduced S, configuration. DWBA analysis.
doi: 10.1103/PhysRevC.27.493
1983SN03 Phys.Rev. C27, 1837 (1983) K.A.Snover, E.G.Adelberger, P.G.Ikossi, B.A.Brown Proton Capture to Excited States of 16O: M1, E1, and Gamow-Teller transitions and shell model calculations NUCLEAR STRUCTURE 16N; calculated levels, B(M1); deduced IAS. 16O, 16C; calculated M1, E1, Gamow-Teller, (p, n) transition rates. 15C, 17,18N; calculated Gamow-Teller transition rates. Shell model. NUCLEAR REACTIONS 15N(p, γ), (p, p'γ), (p, αγ), (polarized p, γ), (polarized p, p'γ), (polarized p, αγ), E=2.5-9.5 MeV; measured capture σ(Eγ), σ(θγ), Eγ, Iγ, analyzing power vs θ. 16O deduced resonances, J, π, T, Γ, ΓpΓγ/Γ, B(M1) ratios, Γp/Γ, M1, E1 transition strengths. Shell model.
doi: 10.1103/PhysRevC.27.1837
1982PR05 Phys.Lett. 115B, 291 (1982) D.M.Pringle, E.F.Garman, S.H.Chew, K.A.Snover, W.N.Catford, S.K.B.Hesmondhalgh, K.W.Allen Decay of the Lowest T = 2 State in 40Ca NUCLEAR REACTIONS 36Ar(α, γ), E=5.495-5.505 MeV; measured Eγ, Iγ, γ yields. 40Ca deduced γ-transitions, B(M1), ΓαΓγ/Γ, Γγ/Γ, Γγ.
doi: 10.1016/0370-2693(82)90372-0
1980HE04 Nucl.Phys. A336, 219 (1980) R.L.Helmer, M.D.Hasinoff, J.E.Bussoletti, K.A.Snover, T.A.Trainor Investigation of the Electric Quadrupole Strength in 13N Using the 12C(p, γ0)13N Reaction NUCLEAR REACTIONS 12C(polarized p, γ), E=10-17 MeV; measured σ(Ep, θγ), asymmetry. 13N deduced E1, E2 σ. Enriched target.
doi: 10.1016/0375-9474(80)90621-1
1980SN01 Phys.Rev.Lett. 44, 927 (1980) K.A.Snover, P.G.Ikossi, E.G.Adelberger, K.T.Lesko Unique Determination of the Amplitude and Phase for the Population of The Giant-Dipole Resonance in the Reaction 12C(p(pol), γ0)13N NUCLEAR REACTIONS 12C(polarized p, γ), E=5-30 MeV; measured σ(E). 13N deduced GDR, T=3/2 M1(E2) interference.
doi: 10.1103/PhysRevLett.44.927
1979AD01 Phys.Rev. C19, 1 (1979) E.G.Adelberger, R.E.Marrs, K.A.Snover Isospin Nonconserving Proton Decays of 13N(T = 3/2) to Negative Parity States of 12C NUCLEAR REACTIONS 11B(3He, np), E=7 MeV; measured np-coin. 12C levels deduced isospin-forbidden excitation by proton decay from lowest T=3/2 level in 13N.
doi: 10.1103/PhysRevC.19.1
1979IK02 Nucl.Phys. A319, 109 (1979) P.G.Ikossi, K.A.Snover, J.L.Osborne, E.G.Adelberger, A.B.McDonald The α-Width of the Lowest T = 2 State in 28Si NUCLEAR REACTIONS 24Mg(α, α), E=5.9-6.25 MeV; measured σ(Eα, θ). 28Si deduced resonances, L, J, π, Γ, Γα, T. Enriched target.
doi: 10.1016/0375-9474(79)90174-X
1979SN01 Phys.Rev.Lett. 43, 117 (1979) K.A.Snover, P.G.Ikossi, T.A.Trainor Observation of Magnetic Dipole Strength in 16O NUCLEAR REACTIONS 15N(polarized p, γ), E=4-9 MeV; measured σ(θ), A(θ). 16O deduced M1 strength between 16-20 MeV excitation, B(M1), Γp, Γ, Γγ.
doi: 10.1103/PhysRevLett.43.117
1978BL04 Phys.Rev.Lett. 41, 1712 (1978) J.S.Blair, P.Dyer, K.A.Snover, T.A.Trainor Nuclear 'Time-Delay' and X-Ray-Proton Coincidences Near a Nuclear Scattering Resonance NUCLEAR REACTIONS 58Ni(p, p), E=3.13-3.18 MeV; measured pX-coin; deduced interference between nuclear scattering amplitude, products of atomic ionization.
doi: 10.1103/PhysRevLett.41.1712
1978DI08 Phys.Rev. C18, 1973 (1978) P.A.Dickey, P.L.Dyer, K.A.Snover, E.G.Adelberger Gamma Decays of the First T = 3/2 States in 9Be and 9B NUCLEAR REACTIONS 7Li(3He, pγ), E=7.5 MeV; 7Li(3He, nγ), E=13 MeV; measured pγ-, nγ-coin. 9Be, 9B levels deduced γ-branching, Γ.
doi: 10.1103/PhysRevC.18.1973
1978MI10 Phys.Rev. C18, 1878 (1978) D.J.Millener, E.K.Warburton, K.A.Snover, R.von Lintig, P.G.Ikossi Electromagnetic Transitions between the Low-Lying Levels of 21Ne and their Relation to Parity Mixing of the 2.80-MeV 1/2± Doublet NUCLEAR STRUCTURE 21Ne; calculated γ CP. 21Ne, 21Na; calculated nuclear wave functions, electromagnetic, parity-mixing matrix elements. NUCLEAR REACTIONS 18O(α, n), E=5.1 MeV; measured γγ(θ). 21Ne deduced δ E3/M2.
doi: 10.1103/PhysRevC.18.1878
1978OS04 Nucl.Phys. A305, 144 (1978) J.L.Osborne, E.G.Adelberger, K.A.Snover Total Width of the Lowest T = 2 State in 24Mg NUCLEAR REACTIONS 23Na(p, γ), E=3906 keV; 27Al(p, γ), E=3671 keV; measured σγ(Ep, θ=90°). 24Mg T=2 resonance, 28Si resonance deduced Γ(cm). Natural targets.
doi: 10.1016/0375-9474(78)90168-9
1978SN01 Phys.Rev.Lett. 41, 145 (1978) K.A.Snover, R.von Lintig, E.G.Adelberger, H.E.Swanson, T.A.Trainor, A.B.McDonald, E.D.Earle, C.A.Barnes Upper Limit on Parity Mixing in 21Ne NUCLEAR REACTIONS 21Ne(p, p'), E=4.08 MeV; measured parity nonconserving γ-CP. 21Ne levels deduced parity-mixing matrix element.
doi: 10.1103/PhysRevLett.41.145
1977AD02 Phys.Rev. C15, 484 (1977) E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti Radiative Transitions and Isospin Mixing in 12C NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured pγ-coin. 11B(p, γ), E=163 keV; measured σ(Eγ). 12C resonances deduced Γγ, isospin mixing.
doi: 10.1103/PhysRevC.15.484
1977DI01 Phys.Rev.Lett. 38, 156 (1977) F.S.Dietrich, D.W.Heikkinen, K.A.Snover, K.Ebisawa Investigation of E2 and E3 Radiation Above the Giant Dipole Resonance in 89Y(p, γ0)90Zr NUCLEAR REACTIONS 89Y(p, γ), E=14-27 MeV; measured σ(E, Eγ, θ). 90Zr deduced resonances, λ.
doi: 10.1103/PhysRevLett.38.156
1977MA07 Nucl.Phys. A277, 429 (1977) R.E.Marrs, E.G.Adelberger, K.A.Snover Gamma Decays of Some T = 0, T = 1 and T = 2 States Above E(x) = 9.5 MeV in 20Ne NUCLEAR REACTIONS 19F(3He, dγ), E=15.0 MeV; measured dγ-coin. 16O(α, γ), (α, α'γ), E=6.93, 9.2-9.7 MeV; measured σ(E, θ). 20Ne deduced levels, J, π, T, γ-branching, Γ, Γγ, Γα. NaI spectrometer.
doi: 10.1016/0375-9474(77)90711-4
1977MA16 Phys.Rev. C16, 61 (1977) R.E.Marrs, E.G.Adelberger, K.A.Snover Electromagnetic Transitions in 13C and 13N NUCLEAR REACTIONS 12C(p, γ), E ≈ 14.25 MeV; measured thick target yield. 11B(3He, pγ), E=5.3 MeV; 11B(3He, nγ), E=7.0 MeV; measured particle γ-coin. 13C, 13N levels deduced partial, total Γ, B(λ).
doi: 10.1103/PhysRevC.16.61
1977SN01 Nucl.Phys. A285, 189 (1977) Radiative Proton Capture to the Ground State and First Three Excited States of 12C NUCLEAR REACTIONS 11B(p, γ), E=6-23 MeV; measured σ(90°) for transitions to the 01+, 2+, 02+, , 3- levels in 12C. 11B(p, γ), E=12.4, 14.4 MeV; measured σ(θ). Enriched target.
doi: 10.1016/0375-9474(77)90245-7
1976AD03 Phys.Lett. 62B, 29 (1976) E.G.Adelberger, R.E.Marrs, K.A.Snover, J.E.Bussoletti Isospin Mixing in 12C NUCLEAR REACTIONS 10B(3He, pγ), E=4.1 MeV; measured γγ-coin. 11B(p, γ); measured resonance γ. 12C levels deduced γ-branching.
doi: 10.1016/0370-2693(76)90039-3
1976MA01 Nucl.Phys. A256, 1 (1976) R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper Upper Limits for Isospin-Forbidden γ-Decays of T=2 States in 20Ne NUCLEAR REACTIONS 19F(p, γ), E ≈ 4.09, 5.88 MeV; measured σ(E, Eγ). 20Ne deduced isospin-forbidden transition strengths, T=2 levels.
doi: 10.1016/0375-9474(76)90090-7
1976SN01 Phys.Rev.Lett. 37, 273 (1976) K.A.Snover, J.E.Bussoletti, K.Ebisawa, T.A.Trainor Application of the Direct-Semidirect Model to the Interpretation of E1 And E2 Strength NUCLEAR REACTIONS 14C(polarized p, γ), E=10-18 MeV; measured σ(E, Eγ, θ).
doi: 10.1103/PhysRevLett.37.273
1975BR07 Phys.Rev. C11, 1122 (1975) B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover Recoil-Distance Lifetime Measurements of 48V Levels NUCLEAR REACTIONS 45Sc(α, nγ), E=9.5 MeV; measured nγ-coin, recoil distance. 48V deduced levels, π, T1/2, B(λ).
doi: 10.1103/PhysRevC.11.1122
1975HA06 Phys.Rev. C11, 998 (1975) M.N.Harakeh, P.Paul, K.A.Snover E1 Transitions in 17F. I. The Low-Lying T = 3/2 States NUCLEAR REACTIONS 16O(p, γ), E=14.8 MeV; measured σ(Eγ, θ). 17F deduced resonances, level-width, B(E1).
doi: 10.1103/PhysRevC.11.998
1975MA21 Phys.Rev.Lett. 35, 202 (1975) R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper Mirror γ Decays in 13C and 13N NUCLEAR REACTIONS 12C(p, γ), E=14.2-14.3 MeV; measured resonance γ-yield. 11B(3He, pγ), (3He, nγ); measured pγ-, nγ-coin. 13N level deduced γ-mixing, B(λ).
doi: 10.1103/PhysRevLett.35.202
1974BR04 Phys.Rev. C9, 1033 (1974) B.A.Brown, D.B.Fossan, J.M.McDonald, K.A.Snover Lifetime Measurements and E2 Effective Charges for Nuclei in the 1f7/2 Shell NUCLEAR REACTIONS 39K(α, n), E=10.4 MeV; 16O, 40Ca(3He, p), E=10.5 MeV; 40Ca, 41K(α, p), E=14.0 MeV; 45Sc(α, p), E=10.0 MeV; 46Ti(α, p), E=11.0 MeV; 40Ca(16O, 2pα), E=47 MeV; 49Ti(α, n), E=14.5 MeV; 40Ca(16O, 3p), E=47 MeV; 40Ca(16O, 2p), E=47 MeV; measured recoil distance. 18F, 42,43Sc, 44Ca, 48Ti, 49V, 50,52Cr, 51,53Mn levels deduced T1/2, B(E2). Deduced 40 < A < 56 effective charges. Natural, enriched targets, Ge(Li) detector.
doi: 10.1103/PhysRevC.9.1033
1974SN01 Phys.Rev.Lett. 32, 317 (1974) K.A.Snover, K.Ebisawa, D.R.Brown, P.Paul Evidence for a Collective E2 Resonance in the Reaction 208Pb(p, γ)209Bi NUCLEAR REACTIONS 208Pb(p, γ), E=17.5-25 MeV; measured γ(θ). 209Bi deduced resonance.
doi: 10.1103/PhysRevLett.32.317
1974SN02 Phys.Rev.Lett. 32, 1061 (1974) K.A.Snover, E.G.Adelberger, D.R.Brown Isoscalar Electric Quadrupole Strength in 16O NUCLEAR REACTIONS 12C(α, γ), E=7-27.5 MeV; measured σ(E). 16O deduced giant E2 resonance.
doi: 10.1103/PhysRevLett.32.1061
1972WA18 Phys.Rev. C6, 375 (1972) E.K.Warburton, H.M.Kuan, D.E.Alburger, P.Paul, K.A.Snover Comment on a Possible Jπ = 0+, T = 2 Resonance in Be9(He3, γγ)C12 NUCLEAR REACTIONS 9Be(3He, γ), E approx 1.74 MeV; measured σ(E;Eγ). 12C deduced no T=2 resonance, upper limit for level-width.
doi: 10.1103/PhysRevC.6.375
1971PA30 Phys.Rev.Lett. 27, 1013 (1971) Symmetry Energy for Collective Dipole Excitation NUCLEAR REACTIONS 48Ca(p, γ), E=4-18 MeV; 63Cu(p, γ), E=2-18 MeV; measured σ(E;Eγ). 49Sc, 64Zn deduced giant dipole resonance structure, separation energies of T+1, T components.
doi: 10.1103/PhysRevLett.27.1013
1971SN01 Phys.Rev. C4, 398 (1971) K.A.Snover, J.M.McDonald, D.B.Fossan, E.K.Warburton Gamma-Ray Decay of the Low-Lying Levels of Cl34 NUCLEAR REACTIONS 32S(3He, pγ), E=6.8 MeV; measured Eγ, Iγ, Doppler shift attenuation. 31P(α, nγ), E=8-11 MeV; measured recoil distance. 34Cl deduced levels, T1/2, γ-branching.
doi: 10.1103/PhysRevC.4.398
1971SN03 Phys.Lett. 37B, 29 (1971) K.A.Snover, J.F.Amann, W.Hering, P.Paul Proton Radiative Capture into 209Bi Through Giant Resonances and Analog Resonances NUCLEAR REACTIONS 208Pb(p, γ), E=8-18 MeV; calculated σ(E;Eγ). 209Bi deduced giant dipole/analog resonance interference, E1 strengths.
doi: 10.1016/0370-2693(71)90561-2
1970GO04 Phys.Rev. C1, 123 (1970) D.R.Goosman, E.G.Adelberger, K.A.Snover T = 3/2 Levels in 11B from the 10Be(p, γ0)11B Reaction NUCLEAR REACTIONS 10Be(p, γ), E=0.6-6.3 MeV; measured σ(E;Eγ, θ(γ)). 11B deduced isobaric analog resonances, J, π, level-width.
doi: 10.1103/PhysRevC.1.123
1969SN01 Phys.Rev.Letters 22, 239(1969) K.A.Snover, D.W.Heikkinen, F.Riess, H.M.Kuan, S.S.Hanna Lowest T = 2 Level in 28Si Observed as a Highly Forbidden Compound-Nucleus Resonance NUCLEAR REACTIONS 24Mg(α, γ), (α, α'), E=6.09-6.13 MeV; measured σ(E;Eγ), σ(E;Eα', θ). 28Si deduced resonances, level-width.
doi: 10.1103/PhysRevLett.22.239
1968PA09 Phys.Rev. 173, 919 (1968) Magnetic Dipole Transitions and Isospin in Be8 NUCLEAR STRUCTURE 8Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.173.919
1967KU06 Phys.Letters 25B, 217 (1967) H.M.Kuan, D.W.Heikkinen, K.A.Snover, F.Riess, S.S.Hanna Observation of T = 2 Level in 20Ne as a Compound Nucleus Resonance NUCLEAR STRUCTURE 20Ne, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90043-3
Back to query form |