NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.Smith Found 127 matches. Showing 1 to 100. [Next]2023BE19 Phys.Rev. C 108, 045503 (2023) E.P.Bernard, E.Mizrachi, J.Kingston, J.Xu, S.V.Pereverzev, T.Pershing, R.Smith, C.G.Prior, N.S.Bowden, A.Bernstein, C.R.Hall, E.Pantic, M.Tripathi, D.N.McKinsey, P.S.Barbeau Thermodynamic stability of xenon-doped liquid argon detectors
doi: 10.1103/PhysRevC.108.045503
2023BR05 Eur.Phys.J. A 59, 165 (2023) C.R.Brune, C.Matei, S.D.Pain, R.Smith Photonuclear reactions with charged particles detection for nuclear astrophysics studies
doi: 10.1140/epja/s10050-023-01082-9
2023LO09 Phys.Lett. B 845, 138149 (2023) J.Lois-Fuentes, B.Fernandez-Dominguez, X.Pereira-Lopez, F.Delaunay, W.N.Catford, A.Matta, N.A.Orr, T.Duguet, T.Otsuka, V.Soma, O.Sorlin, T.Suzuki, N.L.Achouri, M.Assie, S.Bailey, B.Bastin, Y.Blumenfeld, R.Borcea, M.Caamano, L.Caceres, E.Clement, A.Corsi, N.Curtis, Q.Deshayes, F.Farget, M.Fisichella, G.de France, S.Franchoo, M.Freer, J.Gibelin, A.Gillibert, G.F.Grinyer, F.Hammache, O.Kamalou, A.Knapton, Tz.Kokalova, V.Lapoux, B.Le Crom, S.Leblond, F.M.Marques, P.Morfouace, J.Pancin, L.Perrot, J.Piot, E.Pollacco, D.Ramos, D.Regueira-Castro, C.Rodriguez-Tajes, T.Roger, F.Rotaru, M.Senoville, N.de Sereville, R.Smith, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, J.C.Thomas, N.Timofeyuk, M.Vandebrouck, J.Walshe, C.Wheldon Cross-shell states in 15C: A test for p-sd interactions NUCLEAR REACTIONS 2H(16C, t), E=17.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), level energies, J, π, experimental level scheme, single-particle strength, normalised spectroscopic factors. Comparison with the ab initio self-consistent Green's function method employing the NNLOsat interaction. TIARA Silicon array, three MUST2 telescopes, GANIL.
doi: 10.1016/j.physletb.2023.138149
2023RO11 Phys.Rev. C 108, 025811 (2023) H.Rose, N.Kunert, T.Dietrich, P.T.H.Pang, R.Smith, C.Van Den Broeck, S.Gandolfi, I.Tews Revealing the strength of three-nucleon interactions with the proposed Einstein Telescope
doi: 10.1103/PhysRevC.108.025811
2023SM01 Eur.Phys.J. A 59, 166 (2023) R.Smith, R.Menegazzo, C.Aufranc, N.Bez, I.Burrows, M.Cahoreau, G.Debras, L.Gibelin, A.Goasduff, A.Grant, T.Joannem, N.Karkour, M.Karolak, J.Kieffer, A.Lotode, B.Million, P.S.Morrall, L.Ramina, M.Rampazzo, A.Roger, J.Simpson, N.Solenne, O.Stezowski, S.Tzvetkov, L.Zago, M.Zielinska AGATA: mechanics and infrastructures
doi: 10.1140/epja/s10050-023-01046-z
2021AK04 Phys.Rev. C 104, 065501 (2021) D.S.Akerib, A.K.Al Musalhi, S.K.Alsum, C.S.Amarasinghe, A.Ames, T.J.Anderson, N.Angelides, H.M.Araujo, J.E.Armstrong, M.Arthurs, X.Bai, J.Balajthy, S.Balashov, J.Bang, J.W.Bargemann, D.Bauer, A.Baxter, P.Beltrame, E.P.Bernard, A.Bernstein, A.Bhatti, A.Biekert, T.P.Biesiadzinski, H.J.Birch, G.M.Blockinger, E.Bodnia, B.Boxer, C.A.J.Brew, P.Bras, S.Burdin, J.K.Busenitz, M.Buuck, R.Cabrita, M.C.Carmona-Benitez, M.Cascella, C.Chan, N.I.Chott, A.Cole, M.V.Converse, A.Cottle, G.Cox, O.Creaner, J.E.Cutter, C.E.Dahl, L.de Viveiros, J.E.Y.Dobson, E.Druszkiewicz, S.R.Eriksen, A.Fan, S.Fayer, N.M.Fearon, S.Fiorucci, H.Flaecher, E.D.Fraser, T.Fruth, R.J.Gaitskell, J.Genovesi, C.Ghag, E.Gibson, S.Gokhale, M.G.D.van der Grinten, C.B.Gwilliam, C.R.Hall, S.J.Haselschwardt, S.A.Hertel, M.Horn, D.Q.Huang, M.C.I.gnarra, O.Jahangir, R.S.James, W.Ji, J.Johnson, A.C.Kaboth, A.C.Kamaha, K.Kamdin, K.Kazkaz, D.Khaitan, A.Khazov, I.Khurana, D.Kodroff, L.Korley, E.V.Korolkova, H.Kraus, S.Kravitz, L.Kreczko, B.Krikler, V.A.Kudryavtsev, E.A.Leason, J.Lee, D.S.Leonard, K.T.Lesko, C.Levy, J.Liao, J.Lin, A.Lindote, R.Linehan, W.H.Lippincott, X.Liu, M.I.Lopes, E.Lopez Asamar, B.Lopez Paredes, W.Lorenzon, S.Luitz, P.A.Majewski, A.Manalaysay, L.Manenti, R.L.Mannino, N.Marangou, M.E.McCarthy, D.N.McKinsey, J.McLaughlin, E.H.Miller, E.Mizrachi, A.Monte, M.E.Monzani, J.A.Morad, J.D.Morales Mendoza, E.Morrison, B.J.Mount, A.St.J.Murphy, D.Naim, A.Naylor, C.Nedlik, H.N.Nelson, F.Neves, J.A.Nikoleyczik, A.Nilima, I.Olcina, K.C.Oliver-Mallory, S.Pal, K.J.Palladino, J.Palmer, S.Patton, N.Parveen, E.K.Pease, B.Penning, G.Pereira, A.Piepke, Y.Qie, J.Reichenbacher, C.A.Rhyne, A.Richards, Q.Riffard, G.R.C.Rischbieter, R.Rosero, P.Rossiter, D.Santone, A.B.M.R.Sazzad, R.W.Schnee, P.R.Scovell, S.Shaw, T.A.Shutt, J.J.Silk, C.Silva, R.Smith, M.Solmaz, V.N.Solovov, P.Sorensen, J.Soria, I.Stancu, A.Stevens, K.Stifter, B.Suerfu, T.J.Sumner, N.Swanson, M.Szydagis, W.C.Taylor, R.Taylor, D.J.Temples, P.A.Terman, D.R.Tiedt, M.Timalsina, W.H.To, D.R.Tovey, M.Tripathi, D.R.Tronstad, W.Turner, U.Utku, A.Vaitkus, B.Wang, J.J.Wang, W.Wang, J.R.Watson, R.C.Webb, R.G.White, T.J.Whitis, M.Williams, F.L.H.Wolfs, D.Woodward, C.J.Wright, X.Xiang, J.Xu, M.Yeh, P.Zarzhitsky Projected sensitivity of the LUX-ZEPLIN experiment to the two-neutrino and neutrinoless double β decays of 134Xe RADIOACTIVITY 134Xe(2β-); measured recoiling nuclei and electrons, decay energy spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro-luminescence light detected using 494 photomultipliers at Sanford Underground Research Facility (SURF) in South Dakota; deduced lower limits of T1/2 values for 2νββ and 0νββ decay modes.
doi: 10.1103/PhysRevC.104.065501
2021BA19 Eur.Phys.J. A 57, 108 (2021) S.Bailey, T.Kokalova, M.Freer, C.Wheldon, R.Smith, J.Walshe, N.Soic, L.Prepolec, V.Tokic, F.M.Marques, L.Achouri, F.Delaunay, M.Parlog, Q.Deshayes, B.Fernandez-Dominguez, B.Jacquot The identification of α-clustered doorway states in 44, 48, 52Ti using machine learning NUCLEAR REACTIONS 4He(40Ca, α), (44Ca, α), (48Ca, α), E not given; analyzed available σ(θ) data; deduced Random Forest Classifier (RFC) toclassify spectra as either clustered or not clustered.
doi: 10.1140/epja/s10050-021-00357-3
2021PI06 Eur.Phys.J. A 57, 150 (2021) S.Pirrie, C.Wheldon, Tz.Kokalova, J.Bishop, Th.Faestermann, R.Hertenberger, H.F.Wirth, S.Bailey, N.Curtis, D.Dell'Aquila, D.Mengoni, R.Smith, D.Torresi, A.Turner Precision branching-ratio measurements in 18O NUCLEAR REACTIONS 12C(7Li, p), E=44 MeV; measured reaction products; deduced energy levels, J, π, branching ratios, resonance parameters. Comparison with available data, Monte-Carlo techniques, Q3D magnetic spectrograph.
doi: 10.1140/epja/s10050-021-00431-w
2020PE15 Phys.Lett. B 811, 135939 (2020) X.Pereira-Lopez, B.Fernandez-Dominguez, F.Delaunay, N.L.Achouri, N.A.Orr, W.N.Catford, M.Assie, S.Bailey, B.Bastin, Y.Blumenfeld, R.Borcea, M.Caamano, L.Caceres, E.Clement, A.Corsi, N.Curtis, Q.Deshayes, F.Farget, M.Fisichella, G.de France, S.Franchoo, M.Freer, J.Gibelin, A.Gillibert, G.F.Grinyer, F.Hammache, O.Kamalou, A.Knapton, T.Kokalova, V.Lapoux, J.A.Lay, B.Le Crom, S.Leblond, J.Lois-Fuentes, F.M.Marques, A.Matta, P.Morfouace, A.M.Moro, T.Otsuka, J.Pancin, L.Perrot, J.Piot, E.Pollacco, D.Ramos, C.Rodriguez-Tajes, T.Roger, F.Rotaru, M.Senoville, N.de Sereville, R.Smith, O.Sorlin, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, T.Suzuki, J.C.Thomas, N.Timofeyuk, M.Vandebrouck, J.Walshe, C.Wheldon Low-lying single-particle structure of 17C and the N=14 sub-shell closure NUCLEAR REACTIONS 2H(16C, p)17C, E=17.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), γ-ray energies, J, π, level scheme, spectroscopic factors. Comparison with shell model and particle-core model calculations.
doi: 10.1016/j.physletb.2020.135939
2020PI14 Phys.Rev. C 102, 064315 (2020) S.Pirrie, C.Wheldon, Tz.Kokalova, J.Bishop, Th.Faestermann, R.Hertenberger, H.-F.Wirth, S.Bailey, N.Curtis, D.Dell'Aquila, D.Mengoni, R.Smith, D.Torresi, A.Turner Search for evidence of rotational cluster bands in 18O NUCLEAR REACTIONS 12C(7Li, p)18O*, E=44.0 MeV; measured reaction products, recoil protons, (18O break-up particle)α-coin using the Q3D magnetic spectrograph, and the Birmingham large-angular-coverage DSSD array at the Maier-Leibnitz Laboratory (MLL) in Garching. 18O; deduced levels, J, π, total widths, Γα/Γ branching ratios, barrier penetration, θα2, bands, no evidence of consistent (14C+α or 12C+2n+α) cluster structure for any of the bands. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.102.064315
2020SM01 Phys.Rev. C 101, 021302 (2020) R.Smith, M.Gai, M.W.Ahmed, M.Freer, H.O.U.Fynbo, D.Schweitzer, S.R.Stern Stringent upper limit on the direct 3α decay of the Hoyle state in 12C NUCLEAR REACTIONS 12C(γ, α)8Be, E=9.6 MeV; analyzed experimental data in 2013Zi03 and other studies for the energy, width and decay of the second 2+ Hoyle state; deduced upper limit of direct 3α decay mode of the Hoyle state from the experimental value for the upper limit Γ3α for the second 2+ Hoyle state at ≈10 MeV, R-matrix analysis, and semiclassical Wenzel-Kramers-Brillouin approach. Comparison with measured experimental upper limit.
doi: 10.1103/PhysRevC.101.021302
2019BA45 Phys.Rev. C 100, 051302 (2019) S.Bailey, T.Kokalova, M.Freer, C.Wheldon, R.Smith, J.Walshe, N.Curtis, N.Soic, L.Prepolec, V.Tokic, F.M.Marques, L.Achouri, F.Delaunay, Q.Deshayes, M.Parlog, B.Fernandez-Dominguez, B.Jacquot, A.Soylu Extracting the spectral signature of α clustering in 44, 48, 52Ti using a continuous wavelet transform NUCLEAR REACTIONS 4He(40Ca, α)44Ti*, E=180 MeV; 4He(44Ca, α)48Ti*, E=207 MeV; 4He(48Ca, α)52Ti*, E=234 MeV; measured scattered α particles, Eα, Iα, differential σ using double-sided silicon strip detectors at the GANIL radioactive beam facility; deduced continuous wavelet transform (CWT) of the measured spectra, and compared with simulated spectra using the simplified R matrix for spinless particles. 44Ti; deduced high-lying α-clustered levels J, π and compared with previous measurements. Present technique combined thick target inverse kinematics (TTIK) approach and the resonant scattering measurements with the continuous wavelet transform (CWT).
doi: 10.1103/PhysRevC.100.051302
2019BI05 Phys.Rev. C 100, 034320 (2019) J.Bishop, Tz.Kokalova, M.Freer, L.Acosta, M.Assie, S.Bailey, G.Cardella, N.Curtis, E.De Filippo, D.Dell'Aquila, S.De Luca, L.Francalanza, B.Gnoffo, G.Lanzalone, I.Lombardo, N.S.Martorana, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, F.Rizzo, P.Russotto, L.Quattrocchi, R.Smith, I.Stefan, A.Trifiro, M.Trimarchi, G.Verde, M.Vigilante, C.Wheldon Experimental investigation of α condensation in light nuclei NUCLEAR REACTIONS 12C(16O, 28Si)4He/6Li/7Li/7Be/9Be/10B/11B/11C/12C/13C/11N/12C/15O/15N/16O/F/Ne/20Ne/24Mg/28Si, E=160, 280, 400 MeV from the K800 cyclotron at the LNS-Catania accelerator facility; measured reaction product yields, σ, Eα, Iα using the Charged Heavy Ion Mass and Energy Resolving Array (CHIMERA) and Femtoscope Array for Correlation and Spectroscopy (FARCOS); deduced raw α-particle multiplicity, particle-identification plots (PIDs), interaction time plot, distribution of α-particle energies, excitation functions, Q values for different reaction channels, branching ratios for the 7-α breakup modes. Experiments aimed at search for α-gas states in 12C, 16O, 20Ne, 24Mg, 28Si. Results described by a hybrid of sequential decays and multiparticle breakup mechanisms, as no signatures for α condensation observed. Comparison of measured yields to the extended Hauser-Feshbach (EHF), and comparison of 7-α particle states to Fermi breakup model predictions.
doi: 10.1103/PhysRevC.100.034320
2017SM03 Phys.Rev.Lett. 119, 132502 (2017) R.Smith, Tz.Kokalova, C.Wheldon, J.E.Bishop, M.Freer, N.Curtis, D.J.Parker New Measurement of the Direct 3α Decay from the 12C Hoyle State NUCLEAR REACTIONS 12C(α, 3α)4He, E=40 MeV; measured reaction products, Eα, Iα; deduced Dalitz plots, upper limit for the rare direct 3α decay branch. Comparison with theoretical calculations.
doi: 10.1103/physrevlett.119.132502
2017TI07 Nucl.Instrum.Methods Phys.Res. A871, 66 (2017) A.Tillett, J.Dermigny, M.Emamian, Y.Tonin, I.Bucay, R.L.Smith, M.Darken, C.Dearing, M.Orbon, C.Iliadis A low-background γγ-coincidence spectrometer for radioisotope studies RADIOACTIVITY 26Al(EC); measured decay products, Eγ, Iγ, γ-γ-coin; deduced cosmogenic activity, decay constant. Comparison with available data.
doi: 10.1016/j.nima.2017.07.057
2017TO06 Acta Phys.Pol. B48, 319 (2017) V.Tokic, N.Soic, S.Blagus, S.Fazinic, D.Jelavic-Malenica, T.Mijatovic, D.Miljanic, L.Prepolec, N.Skukan, S.Szilner, M.Uroic, M.Milin, A.Di Pietro, P.Figuera, J.P.Fernandez-Garcia, M.Fisichella, M.Lattuada, V.Scuderi, E.Strano, D.Torresi, S.Bailey, N.Curtis, M.Freer, R.Smith, J.Walshe, V.Ziman, L.Acosta, I.Martel, G.Marquinez-Duran, A.M.Sanchez-Benitez, E.Fioretto Structure of 24Mg Excited States and Their Influence on Nucleosynthesis NUCLEAR REACTIONS 12C(16O, α)24Mg, E=94 MeV; measured decay channels of 24Mg (emission of α, proton, breakup to 12C+12C and to 8Be+16O). 24Mg; deduced excitation energies of resonances. 4He(20Ne, α)20Ne, E=44, 52, 60 MeV; measured reaction products. 24Mg; deduced σ(θ), resonances; calculated σ(θ) using R-matrix fit to the data at 44 MeV. Further R-matrix calculations in progress.
doi: 10.5506/APhysPolB.48.319
2016SM02 Phys.Rev. C 94, 014320 (2016) R.Smith, C.Wheldon, M.Freer, N.Curtis, Tz.Kokalova, S.Almaraz-Calderon, A.Aprahamian, N.I.Ashwood, M.Barr, B.Bucher, P.Copp, M.Couder, X.Fang, G.Goldring, F.Jung, S.R.Lesher, W.Lu, J.D.Malcolm, A.Roberts, W.P.Tan, V.A.Ziman Evidence for a 3.8 MeV state in 9Be NUCLEAR REACTIONS 9Be(α, n3α), E=22, 26 MeV; measured Eα, Iα using an array of double-sided silicon strip detectors (DSSSDs) at the Notre Dame FN Tandem Van de Graaff accelerator facility; extracted sum energy spectra for all four final-state particles, assumed to be 3α+n, 9Be excitation spectrum. 9Be; deduced levels, new state at 3.8 MeV, J, π, width, ratios of reduced widths to Wigner limits (decays to 8Be ground state). 9Be, 9B; comparison of levels and widths in mirror nuclei.
doi: 10.1103/PhysRevC.94.014320
2015CA08 Rom.J.Phys. 60, 738 (2015) M.A.Caprio, P.Maris, J.P.Vary, R.Smith Emergence of Rotational Collectivity in Ab Initio no-Core Configuration Interaction Calculations NUCLEAR STRUCTURE 7,8,9,10,11,12Be; calculated band energy parameters. ab initio no-core configuration interaction (NCCI).
2015CA22 Int.J.Mod.Phys. E24, 1541002 (2015) M.A.Caprio, P.Maris, J.P.Vary, R.Smith Collective rotation from ab initio theory NUCLEAR STRUCTURE 7,8,9Be; calculated electric quadrupole transition strengths, level energies, quadrupole and dipole matrix element observables, natural parity yrast, band energy parameters. Comparison with available data.
doi: 10.1142/S0218301315410025
2011DI16 J.Korean Phys.Soc. 59, 1697s (2011) F.Ditroi, S.Takacs, F.Tarkanyi, R.W.Smith, M.Baba Investigation of Proton and Deuteron Induced Reactions on Cobalt NUCLEAR REACTIONS 59Co(p, X)55,56,57,58Co, E=48-75 MeV;59Co(p, X)52Mn, E=55-70 MeV;59Co(p, 4n), E=60-70 MeV;59Co(d, X)57,58,60Co, E=0-50 MeV;59Co(d, p)60Co, E=13-40 MeV; measured Eγ, Iγ using stacked foil technique (incident energies 70 MeV for protons, 40 MeV deuterons); deduced σ. 59Co(d, p), E=4-38 MeV; measured Eγ, Iγ using stacked foil technique; deduced physical yield. 58Co(d, X), E=25 MeV; measured thin layer activity distribution (θ=300, 900). Compared with other data, TENDL-2009 (TALYS-based Evaluated Nuclear Data Library).
doi: 10.3938/jkps.59.1697
2002CA55 Hyperfine Interactions 143, 37 (2002) J.J.Carroll, J.Burnett, T.Drummond, J.Lepak, R.Propri D.Smith, S.A.Karamian, J.Adam, F.Stedile, F.J.Agee Initial Search for Triggered Gamma Emission from 178Hfm2 Using the YSU Miniball Array NUCLEAR REACTIONS 178mHf(γ, γ'), E=100 keV bremsstrahlung; measured Eγ, Iγ, γγ-coin; deduced upper limit for triggered emission rate.
doi: 10.1023/A:1024033601402
2000ZW01 Phys.Rev.Lett. 84, 2634 (2000) J.Zweiback, R.A.Smith, T.E.Cowan, G.Hays, K.B.Wharton, V.P.Yanovsky, T.Ditmire Nuclear Fusion Driven by Coulomb Explosions of Large Deuterium Clusters NUCLEAR REACTIONS 2H(d, nX), E not given; measured neutron spectra following laser irradiation of deuterium; deduced fusion yields.
doi: 10.1103/PhysRevLett.84.2634
2000ZW04 Phys.Rev.Lett. 85, 3640 (2000) J.Zweiback, T.E.Cowan, R.A.Smith, J.H.Hartley, R.Howell, C.A.Steinke, G.Hays, K.B.Wharton, J.K.Crane, T.Ditmire Characterization of Fusion Burn Time in Exploding Deuterium Cluster Plasmas NUCLEAR REACTIONS 2H(d, nX), E not given; measured neutron spectra following laser-induced fusion, temporal features. Femtosecond laser pulses, application as neutron source discussed.
doi: 10.1103/PhysRevLett.85.3640
1999AL01 Phys.Rev.Lett. 82, 41 (1999) T.Alexopoulos, L.Antoniazzi, M.Arenton, H.C.Ballagh, H.Bingham, A.Blankman, M.Block, A.Boden, G.Bonomi, Z.L.Cao, T.Y.Chen, K.Clark, D.Cline, S.Conetti, M.Cooper, G.Corti, B.Cox, P.Creti, E.C.Dukes, C.Durandet, V.Elia, A.R.Erwin, L.Fortney, V.Golovatyuk, E.Gorini, F.Grancagnolo, K.Hagan-Ingram, M.Haire, P.Hanlet, M.He, G.Introzzi, M.Jenkins, D.Judd, W.Kononenko, W.Kowald, K.Lau, A.Ledovskoy, G.Liguori, J.Lys, P.O.Mazur, A.P.McManus, S.Misawa, G.H.Mo, C.T.Murphy, K.Nelson, M.Panareo, V.Pogosyan, S.Ramachandran, J.Rhoades, W.Selove, R.P.Smith, L.Spiegel, J.G.Sun, S.Tokar, P.Torre, J.Trischuk, L.Turnbull, D.E.Wagoner, C.R.Wang, C.Wei, W.Yang, N.Yao, N.J.Zhang, B.T.Zou Measurement of the b(b-bar) Cross Section in 800 GeV/c Proton-Silicon Interactions NUCLEAR REACTIONS Si(p, X), E at 800 GeV/c; measured b(b-bar) production σ.
doi: 10.1103/PhysRevLett.82.41
1997KE06 Nucl.Phys. A621, 243c (1997) V.V.Ketlerov, A.A.Goverdovsky, V.A.Khryachkov, V.F.Mitrofanov, Yu.B.Ostapenko, R.C.Haight, P.E.Koehler, S.M.Grimes, R.S.Smith Detailed Study of Double-Differential Cross-Sections for the 17O(n, α)14C Reaction NUCLEAR REACTIONS 17O(n, γ), E < 1.01 MeV; measured α spectra, σ(θ).
doi: 10.1016/S0375-9474(97)00246-7
1995BA06 Nucl.Phys. A584, 315 (1995) M.J.Balbes, M.M.Farrell, R.N.Boyd, X.Gu, M.Hencheck, J.D.Kalen, C.A.Mitchell, J.J.Kolata, K.Lamkin, R.Smith, R.Tighe, K.Ashktorab, F.D.Becchetti, J.Brown, D.Roberts, T.-F.Wang, D.Humphrey, G.Vourvopoulos, M.S.Islam Cross Sections and Reaction Rates of d + 8Li Reactions Involved in Big Bang Nucleosynthesis NUCLEAR REACTIONS 2H(8Li, 7Li), (8Li, 9Be), (8Li, 9Li), E=8-14 MeV; measured σ(E, θ); deduced reaction rates.
doi: 10.1016/0375-9474(94)00484-5
1993BA57 Phys.Rev.Lett. 71, 3931 (1993) M.J.Balbes, M.M.Farrell, R.N.Boyd, X.Gu, M.Hencheck, J.D.Kalen, C.A.Mitchell, J.J.Kolata, K.Lamkin, R.Smith, R.Tighe, K.Ashktorab, F.D.Becchetti, J.Brown, D.Roberts, T.-F.Wang, D.Humphrey, G.Vourvopoulos, M.S.Islam 2H Induced Reactions on 8Li and Primordial Nucleosynthesis NUCLEAR REACTIONS, ICPND 2H(8Li, 7Li), (8Li, 8Be), E(cm)=2.4 MeV; 8Li(d, t), (d, n), E(cm)=1.5-2.75 MeV; measured σ(E); deduced primordial nucleosynthesis yields.
doi: 10.1103/PhysRevLett.71.3931
1993BE22 Phys.Rev. C48, 308 (1993) F.D.Becchetti, W.Z.Liu, K.Ashktorab, J.F.Bajema, J.A.Brown, J.W.Janecke, D.A.Roberts, J.J.Kolata, K.L.Lamkin, A.Morsad, R.J.Smith, X.J.Kong, R.E.Warner Systematics of 8Li-Induced Radioactive Beam Reactions: E = 13-20 MeV NUCLEAR REACTIONS 2H, 9Be, 13,12C, 14N, 27Al, 58Ni(8Li, 7Li), (8Li, 8Li), E ≈ 13-20 MeV; 9Be, 12C(8Li, α), E ≈ 13-20 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.48.308
1993CA04 Phys.Rev. C47, 387 (1993) D.D.Caussyn, N.R.Fletcher, K.W.Kemper, E.E.Towers, J.J.Kolata, K.Lamkin, R.J.Smith, F.D.Becchetti, J.A.Brown, J.W.Janecke, D.A.Roberts, D.L.Gay Cross Section for the Primordial Reaction 8Li(p, n)8Be(g.s.) at E(cm) = 1.5 MeV NUCLEAR REACTIONS 8Li(p, n), E(cm)=1.5 MeV; measured σ(θ); deduced σ. Hauser-Feshbach calculation.
doi: 10.1103/PhysRevC.47.387
1992BE46 Nucl.Phys. A550, 507 (1992) F.D.Becchetti, J.A.Brown, W.Z.Liu, J.W.Janecke, D.A.Roberts, J.J.Kolata, R.J.Smith, K.Lamkin, A.Morsad, R.E.Warner, R.N.Boyd, J.D.Kalen Reaction Rates for 8Li(p, α) and 8Li(p, n, α) and Their Effect on Primordial Nucleosynthesis NUCLEAR REACTIONS 1H(8Li, α), E(cm)=1.5 MeV; measured σ(Eα), σ(θ); deduced 8Li destruction thermonuclear reaction rate, p+8Li total reaction rate. Radioactive beam.
doi: 10.1016/0375-9474(92)90020-K
1992KO14 Phys.Rev.Lett. 69, 2631 (1992) J.J.Kolata, M.Zahar, R.Smith, K.Lamkin, M.Belbot, R.Tighe, B.M.Sherrill, N.A.Orr, J.S.Winfield, J.A.Winger, S.J.Yennello, G.R.Satchler, A.H.Wuosmaa Quasielastic Scattering of 11Li and 11C from 12C at 60 MeV/Nucleon NUCLEAR REACTIONS 12C(11Li, X), (11C, X), E=60 MeV/nucleon; measured quasielastic σ(θ); deduced enhanced refraction need for 11Li projectile. Coupled-channels approach.
doi: 10.1103/PhysRevLett.69.2631
1991BE49 Nucl.Instrum.Methods Phys.Res. B56/57, 554 (1991) F.D.Becchetti, J.A.Brown, K.Ashktorab, J.W.Janecke, W.Z.Liu, D.A.Roberts, R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, R.E.Warner Production and Use of 6He, 7Be, 8Li, 12B and Metastable Nuclear Beams NUCLEAR REACTIONS 9Be(7Li, 8Li), (7Li, α), (7Li, 6He), E=17 MeV; 1H(10B, 7Be), E=23.5 MeV; 9Be(7Li, 6He), E=14.63 MeV; 1H(10B, 7Be), E=23.5 MeV; 12C(3He, 7Be), E=22.5 MeV; 10B(6Li, 7Be), E=23 MeV; 12C(17O, 18F), E=70 MeV; measured secondary beam production yields. 197Au, C, Ni(8Li, 8Li), (8Li, 8Li'), E=13.8-14.9 MeV; measured σ(E(8Li)). 197Au, Ti, 2H, 27Al, C, 9Be(6He, 6He), E=8.8-9.3 MeV; measured σ(θ). Other reactions discussed.
doi: 10.1016/0168-583X(91)96094-2
1991BR14 Phys.Rev.Lett. 66, 2452 (1991) J.A.Brown, F.D.Becchetti, J.W.Janecke, K.Ashktorab, D.A.Roberts, J.J.Kolata, R.J.Smith, K.Lamkin, R.E.Warner Coulomb Excitation of 8Li NUCLEAR REACTIONS Ni(8Li, 8Li'), (8Li, 8Li), E ≈ 14.6 MeV; measured σ(θ) following Coulomb excittion. 8Li deduced level excitation probability, B(E2).
doi: 10.1103/PhysRevLett.66.2452
1991FO04 Nuovo Cim. 104A, 151 (1991) B.Fornal, F.Gramegna, W.Hering, G.Prete, G.Nebbia, R.Smith, G.D'Erasmo, L.Fiore, A.Pantaleo, G.Viesti, P.Blasi, F.Lucarelli, I.Iori, A.Moroni The Origin of Symmetric Splitting Events in the 32S + 58,64Ni Reactions at 160 and 180 MeV NUCLEAR REACTIONS 64,58Ni(32S, X), E=160, 180 MeV; measured (fragment)(fragment)-coin, γ-multiplicity; deduced missing charge, symmetric splitting origin.
doi: 10.1007/BF02910873
1991HA01 Phys.Rev. C43, 230 (1991) O.Hausser, M.C.Vetterli, R.W.Fergerson, C.Glashausser, R.C.Jeppesen, R.D.Smith, R.Abegg, F.T.Baker, A.Celler, R.L.Helmer, R.Henderson, K.Hicks, M.J.Iqbal, K.P.Jackson, K.W.Jones, J.Lisantti, J.Mildenberger, C.A.Miller, R.S.Sawafta, S.Yen Nuclear Response in the 54Fe(p(pol), p(pol)') Reaction at 290 MeV NUCLEAR REACTIONS 54Fe(polarized p, p'), E=290 MeV; measured σ(θ), spin observables, analyzing power, spin-flip probabilities. 54Fe(n, p), E=298 MeV; analyzed data. 54Fe deduced isovector giant dipole, isoscalar giant quadrupole resonance. 54Mn deduced Gamow-Teller transition strength, quenching. Surface RPA model.
doi: 10.1103/PhysRevC.43.230
1991SM01 Phys.Rev. C43, 761 (1991) R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, K.Ashktorab, F.D.Becchetti, J.A.Brown, J.W.Janecke, W.Z.Liu, D.A.Roberts Scattering of 6He from 197Au, (nat)Ti, 27Al, (nat)C, and 9Be at E = 8-9 MeV NUCLEAR REACTIONS 197Au, Ti, 27Al, C(6He, 6He), E=8.8-9.3 MeV; measured σ(θ); deduced model parameters. Beam from 9Be(7Li, 6He) reaction.
doi: 10.1103/PhysRevC.43.761
1991SM02 Phys.Rev. C43, 2346 (1991) R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, F.D.Becchetti, J.A.Brown, W.Z.Liu, J.W.Janecke, D.A.Roberts, R.E.Warner Elastic and Inelastic Scattering of 8Li from 12C NUCLEAR REACTIONS C, 197Au(8Li, 8Li), (8Li, 8Li'), E=14 MeV; measured σ(θ); deduced model parameters. 8Li level deduced B(E2).
doi: 10.1103/PhysRevC.43.2346
1990BA14 Phys.Lett. 237B, 337 (1990) F.T.Baker, L.Bimbot, B.Castel, R.W.Fergerson, C.Glashausser, A.Green, O.Hausser, K.Hicks, K.Jones, C.A.Miller, S.K.Nanda, R.D.Smith, M.Vetterli, J.Wambach, R.Abegg, D.Beatty, V.Cupps, C.Djalali, R.Henderson, K.P.Jackson, R.Jeppesen, J.Lisantti, M.Morlet, R.Sawafta, W.Unkelbach, A.Willis, S.Yen The Nuclear Spin Response to Intermediate Energy Protons NUCLEAR REACTIONS 12C, 90Zr, 40,44,48Ca, 24Mg, 54Fe(polarized p, p'), E ≈ 300 MeV; 40Ca(polarized p, p'), E=800 MeV; measured spin-flip transition probability; deduced enhanced spin response features. Continuum RPA.
doi: 10.1016/0370-2693(90)91185-E
1990BE31 Phys.Rev. C42, R801 (1990) F.D.Becchetti, K.Ashktorab, J.A.Brown, J.W.Janecke, D.A.Roberts, J.van Klinken, W.Z.Liu, J.J.Kolata, K.Lamkin, R.J.Smith, R.E.Warner Production of an Isomeric, Excited Radioactive Nuclear Beam NUCLEAR REACTIONS 12C(17O, 18F), E=50-80 MeV; measured σ, production rate of 18mF.
doi: 10.1103/PhysRevC.42.R801
1990FO01 Phys.Rev. C41, 127 (1990) B.Fornal, F.Gramegna, G.Prete, G.Nebbia, R.Smith, G.D'Erasmo, L.Fiore, A.Pantaleo, G.Viesti, P.Blasi, F.Lucarelli, I.Iori, A.Moroni Test of Statistical Model Predictions for Alpha-Particle Decay of 90,92,94,96Ru Compound Nuclei NUCLEAR REACTIONS 58,60,62,64Ni(32S, X), E=135-185 MeV; measured σ(Eα, θα); deduced model parameters. 90Ru deduced yrast plot.
doi: 10.1103/PhysRevC.41.127
1990SM04 Nucl.Instrum.Methods Phys.Res. A294, 26 (1990) R.J.Smith, J.J.Kolata, K.Lamkin, A.Morsad, K.Ashktorab, F.D.Becchetti, J.Brown, J.W.Janecke, W.Z.Liu, D.A.Roberts Production and Use of Radioactive 7Be Beams NUCLEAR REACTIONS 1H(10B, 7Be), E=23.5 MeV; 12C(3He, 7Be), E=22.5 MeV; measured σ(E(7Be)), yields. Radioactive beam production. 12C, 197Au(7Be, 7Be), E=8.5-22.4 MeV; measured σ(θ), ratio to Rutherford scattering. Radioactive beam.
doi: 10.1016/0168-9002(90)91824-U
1989HJ01 Phys.Rev.Lett. 62, 870 (1989) E.L.Hjort, F.P.Brady, J.L.Romero, J.R.Drummond, M.A.Hamilton, B.McEachern, R.D.Smith, V.R.Brown, F.Petrovich, V.A.Madsen Pb(n, n'X) at 65 MeV and the Isospin Structure of the Giant Quadrupole Resonance Region NUCLEAR REACTIONS 208Pb(n, n'X), E=65 MeV; measured σ(θn, En). 208Pb deduced GQR isospin structure. Other data input.
doi: 10.1103/PhysRevLett.62.870
1989KO23 Phys.Lett. 227B, 310 (1989) A Deep Potential Description of the 16O + 16O System NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=15-35 MeV; calculated σ(θ) vs E, absorption σ(E); deduced model parameters. 32S deduced possible quasimolecular states.
doi: 10.1016/0370-2693(89)90935-0
1989SM02 Phys.Rev. C39, 1751 (1989) Quasifree Scattering in the Preequilibrium Region NUCLEAR REACTIONS, ICPND 58Ni(p, p'), E=164, 90 MeV; 54Fe(p, p'), E=62 MeV; 27Al(p, p'), E=200 MeV; calculated σ(θp, Ep). 27Al(p, n), E=113 MeV; calculated σ(θn, En); 58Ni, 27Al, 90Zr, 209Bi(p, p'), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; calculated angle integrated σ. Quasifree scattering, preequilibrium region.
doi: 10.1103/PhysRevC.39.1751
1988CO14 Nucl.Phys. A485, 61 (1988) G.Co, K.F.Quader, R.D.Smith, J.Wambach Charge Response in 12C and 40Ca NUCLEAR REACTIONS 12C(γ, X), E ≈ 20-60 MeV; 16O(γ, X), E ≈ 15-60 MeV; 40Ca(γ, X), E=15-30 MeV; calculated photoabsorption σ(E). Nonrelativistic many-body theory. NUCLEAR STRUCTURE 12C, 40Ca; calculated charge response. Nonrelativistic many-body theory.
doi: 10.1016/0375-9474(88)90522-2
1988FI04 Nucl.Phys. A484, 117 (1988) L.K.Fifield, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, P.J.Woods, B.R.Fulton, R.A.Cunningham, P.V.Drumm The Mass of 37P NUCLEAR REACTIONS 48Ca(36S, 37P), E=198 MeV; measured σ(E(37P)); deduced σ(θ), Q. 37P deduced mass excess.
doi: 10.1016/0375-9474(88)90144-3
1988HA27 Phys.Rev.Lett. 61, 822 (1988) O.Hausser, R.Abegg, R.G.Jeppesen, R.Sawafta, A.Celler, A.Green, R.L.Helmer, R.Henderson, K.Hicks, K.P.Jackson, J.Mildenberger, C.A.Miller, M.C.Vetterli, S.Yen, M.J.Iqbal, R.D.Smith Complete Spin Observables for Quasielastic Proton Scattering from 54Fe at 290 MeV NUCLEAR REACTIONS 54Fe(polarized p, p'X), E=290 MeV; measured σ(θ, Ep'), spin-transfer σ(θ, Ep'), analyzing power, spin observables; deduced Fermi motion, nuclear response function, nucleon-nucleon interaction role. Relativistic, non-relativistic models, impulse approximation.
doi: 10.1103/PhysRevLett.61.822
1988HE06 Nucl.Phys. A481, 161 (1988) D.F.Hebbard, J.Nurzynski, T.R.Ophel, P.V.Drumm, Y.Kondo, B.A.Robson, R.Smith The 20Ne(16O, 16O)20Ne Excitation Function at θ(cm) = 90° and Parity-Dependent Interactions NUCLEAR REACTIONS 20Ne(16O, 16O), (16O, 16O'), E(cm)=21.5-31.2 MeV; measured σ(E); deduced optical model parameters. 36Ar resonances deduced parity. Extended optical model analysis.
doi: 10.1016/0375-9474(88)90478-2
1988LA20 Phys.Rev. C38, 1961 (1988) A.R.Lampis, J.Stevenson, W.Benenson, J.Clayton, D.Cebra, Y.Chen, D.Fox, E.Kashy, D.J.Morrissey, M.Samuel, R.Smith, C.L.Tam, G.D.Westfall, K.Wilson, J.S.Winfield Correlations between High-Energy Gamma Rays and Light Fragments in Heavy Ion Collisions NUCLEAR REACTIONS Zn(14N, pγ), (14N, dγ), (14N, tγ), E=40 MeV/nucleon; measured (particle)γ-coin, σ(Ep, θp, θγ).
doi: 10.1103/PhysRevC.38.1961
1988LI01 Phys.Lett. 200B, 263 (1988) C.S.Lim, M.D.Rebgetz, R.H.Spear, W.J.Vermeer, M.P.Fewell, B.A.Robson, R.Smith Energy Dependence of the 16O-208Pb Effective Interaction NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=57-79 MeV; measured σ(ratio). 208Pb level deduced excitation probability. Effective interaction description, Coulomb-nuclear interference effects.
doi: 10.1016/0370-2693(88)90768-X
1988SM03 Phys.Rev. C38, 100 (1988) Damping of the Continuum Response from 2p-2h Excitations NUCLEAR REACTIONS 54Fe(n, p), E=300 MeV; calculated σ(θp, Ep). 54Fe(p, p'), E=290 MeV; calculated spin-flip σ(θ) vs E. Continuum response damping.
doi: 10.1103/PhysRevC.38.100
1988WI09 Phys.Lett. 203B, 345 (1988) J.S.Winfield, S.M.Austin, G.M.Crawley, C.Djalali, C.A.Ogilvie, R.J.Smith, Z.Chen, M.Torres Energy Dependence of 12C + 12C Single-Neutron Transfer Cross Sections NUCLEAR REACTIONS 12C(12C, 13C), E=25, 35, 50 MeV/nucleon; measured σ(θ); deduced σ(E), model parameters.
doi: 10.1016/0370-2693(88)90180-3
1987GL02 Phys.Rev.Lett. 58, 2404 (1987) C.Glashausser, K.Jones, F.T.Baker, L.Bimbot, H.Esbensen, R.W.Fergerson, A.Green, S.Nanda, R.D.Smith Enhancement of the Relative (ΔS = 1)/(ΔS = 0) Response of 40Ca at High Excitation Energies NUCLEAR REACTIONS 40Ca(polarized p, p'), E=319 MeV; measured σ(Ep', θp'), spin-flip probabilities, σ vs excitation energy. 40Ca deduced nuclear response function vs excitation energy. Focal-plane polarimeter. Espensen-Bertsch slab response model.
doi: 10.1103/PhysRevLett.58.2404
1987SM08 Phys.Rev. C36, 2704 (1987) One- and Two-Step Contributions to the 90Zr(p, n)90Nb Cross Section at 0° NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(θ=0°, E); deduced one-, two-step contributions, missing Gamow-Teller transition strength implications. RPA, eikonal approximation.
doi: 10.1103/PhysRevC.36.2704
1986DR11 Aust.J.Phys. 39, 369 (1986) P.V.Drumm, D.F.Hebbard, T.R.Ophel, J.Nurzynski, Y.Kondo, B.A.Robson, R.Smith Excitation Function for 16O + 24Mg Elastic Scattering at θ(c.m.) = 90° NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=53-75.5 MeV; measured σ(E(16O)), σ(θ) vs E. Enge split-pole magnetic spectrometer. Optical model analysis.
doi: 10.1071/PH860369
1986NU01 J.Phys.(London) G12, 383 (1986) J.Nurzynski, D.F.Hebbard, T.R.Ophel, Y.Kondo, B.A.Robson, R.Smith Excitation Functions for 24Mg(16O, 16O')24Mg(*) (0 ≤ E(x) ≤ 8.4 MeV) Scattering at Forward Angles NUCLEAR REACTIONS 24Mg(16O, 16O'), E(cm)=33.6-49.2 MeV; measured σ(E(16O)), σ(θ) vs E. 16O, 24Mg levels deduced possible excitation. Enriched target, magnetic spectrometer. Coupled channels calculations.
doi: 10.1088/0305-4616/12/5/005
1986SM02 Phys.Rev. C33, 847 (1986) R.D.Smith, V.R.Brown, V.A.Madsen Isovector Deformation Parameters from Coupled-Channel Analysis of (p, n) Reactions NUCLEAR REACTIONS 54,55Fe(p, n), (p, p'), E=35 MeV; 54,55Fe(n, n), (n, n'), E=26 MeV; calculated σ(θ); deduced reaction mechanism. 54,56Fe deduced isovector deformation parameter. Lane model, optical potential, vibrational model couplings.
doi: 10.1103/PhysRevC.33.847
1986SM05 Z.Phys. A324, 283 (1986) R.J.Smith, P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, B.R.Fulton, R.A.Cunningham Use of the 64Ni(36S, 34,35Si)66,65Zn Reactions to Measure the Masses of 34Si and 35Si NUCLEAR REACTIONS 64Ni(36S, 35Si), (36S, 34Si), E=198 MeV; measured σ(E(35Si)), σ(E(34Si)). 34,35Si deduced mass excess. Model prediction comparison. Gas filled focal plane detector, QMG/2 magnetic spectrometer.
1986SM12 Phys.Lett. 182B, 283 (1986) Effect of Nuclear Binding and Fermi Motion on the Ratio R(A) = σ(L)/σ(T) in Deep-Inelastic Electron Scattering NUCLEAR STRUCTURE 56Fe; calculated transverse to longitudinal structure function ratio. Convolution model.
doi: 10.1016/0370-2693(86)90091-2
1986ST07 Phys.Rev.Lett. 57, 555 (1986) J.Stevenson, K.B.Beard, W.Benenson, J.Clayton, E.Kashy, A.Lampis, D.J.Morrissey, M.Samuel, R.J.Smith, C.L.Tam, J.S.Winfield High-Energy Gamma-Ray Emission in Heavy-Ion Collisions NUCLEAR REACTIONS Pb, Zn, C(14N, X), E=20, 30, 40 MeV/nucleon; measured Eγ, Iγ, γ(θ); deduced model parameters. Individual neutron-proton collision induced bremsstrahlung.
doi: 10.1103/PhysRevLett.57.555
1986WO07 Phys.Lett. 182B, 297 (1986) P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, B.R.Fulton, R.A.Cunningham, P.V.Drumm, L.K.Fifield The Mass of 33Al NUCLEAR REACTIONS 48Ca(36S, 33Al), E=198 MeV; measured σ(E(33Al)). 33Al deduced mass excess. Enriched target, magnetic spectrometer. Mass, large basis shell models.
doi: 10.1016/0370-2693(86)90094-8
1985BU13 Nucl.Phys. A442, 289 (1985) S.M.Burnett, A.M.Baxter, S.Hinds, F.Pribac, R.Smith, R.H.Spear, M.P.Fewell Octupole Vibrational States in the Even-Mass Barium Isotopes NUCLEAR REACTIONS 130,132,134,136,138Ba(α, α'), E=20 MeV; measured σ(E(α')). 132,134,136,138Ba(α, α'), E=20 MeV; measured σ(Eα, θ). 132,134,136,138Ba deduced levels, J, π, L, β2, β3. 130Ba deduced levels. Enriched targets.
doi: 10.1016/0375-9474(85)90146-0
1985KO38 Phys.Lett. 162B, 39 (1985) Y.Kondo, B.A.Robson, R.Smith, H.H.Wolter Transfer Contribution to Elastic 16O + 20Ne Scattering and Parity-Dependent Interactions NUCLEAR REACTIONS 20Ne(16O, 16O), E(cm)=22-40 MeV; calculated σ(θ); deduced potential parameters, reaction mechanism.
doi: 10.1016/0370-2693(85)91057-3
1985KO43 Nucl.Phys. A437, 117 (1985) Coupled-Channel Description of Resonant Structures in the 16O + 20Ne System NUCLEAR REACTIONS, ICPND 20Ne(16O, 16O), (16O, 16O'), E(cm)=24.5-35.5 MeV; analyzed σ(θ), σ(E), reaction σ(E). 36S deduced resonances, J, π. Coupled-channels model.
doi: 10.1016/0375-9474(85)90229-5
1985SM06 Phys.Rev. C32, 1654 (1985) Spin Observables in Quasi-Elastic Proton-Nucleus Scattering near 1 GeV NUCLEAR REACTIONS 12C(polarized p, p'), E=800 MeV; calculated σ(θ) vs proton momentum, analyzing power, other polarization observables vs θ. Glauber multiple scattering theory including spin, multiple knockout collisions.
doi: 10.1103/PhysRevC.32.1654
1985WO07 Z.Phys. A321, 119 (1985) P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, N.E.Sanderson, B.R.Fulton, R.A.Cunningham Use of the 64Ni(36S, 34Si)66Zn Reaction to Measure the Mass of 34Si NUCLEAR REACTIONS 64Ni(36S, 34Si), E=198 MeV; measured 34Si ion momentum spectra. 34Si deduced mass. Mass, shell models comparison.
doi: 10.1007/BF01411955
1984AM03 J.Phys.(London) G10, 331 (1984) Interacting Boson-Fermion Models and Transition Densities NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; 112,114,116,118,120,122,124Sn(n, n'), E=24 MeV; calculated σ(θ). 20Ne(e, e'), E not given; calculated form factor. Interacting boson model spectroscopic amplitudes, B(E2) matching. NUCLEAR STRUCTURE 20Ne, 112,114,116,118,120,122,124Sn; calculated BCS level occupancies, spectroscopic amplitudes. Interacting boson approximation.
doi: 10.1088/0305-4616/10/3/009
1984NE06 J.Radioanal.Nucl.Chem. 84, 149 (1984) G.W.A.Newton, V.J.Robinson, E.M.Shaw, R.J.Smith, H.E.Sims Single Neutron Transfer Reactions in the Systems: 139La + 16O, 93Nb + 12C, 14N, 16O and 20Ne NUCLEAR REACTIONS, ICPND 139La(16O, 15O), E=105.8-153.1 MeV; 93Nb(12C, 13C), E=88.7-171.2 MeV; 93Nb(14N, 15N), E=89.4-145.6 MeV; 93Nb(16O, 17O), E=117.3-183.6 MeV; 93Nb(20Ne, 21Ne), E=112.2-191.4 MeV; measured σ(E), residuals yields, isomer production σ; deduced reaction mechanism.
doi: 10.1007/BF02038191
1984WI05 Phys.Rev. C29, 1207 (1984) R.B.Wiringa, R.A.Smith, T.L.Ainsworth Nucleon-Nucleon Potentials with and without Δ(1232) Degrees of Freedom NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 25-400 MeV; calculated phase shifts vs E. Nucleon-nucleon potentials with, without isobar degrees of freedom. NUCLEAR STRUCTURE 2H; calculated wave function, binding energy, quadrupole, magnetic moments, D-state probability. Nucleon-nucleon potentials with, without isobar degrees of freedom.
doi: 10.1103/PhysRevC.29.1207
1983KO31 Nucl.Phys. A410, 289 (1983) Resonant Structures in the 16O + 20Ne System NUCLEAR REACTIONS 20Ne(16O, 16O), E(cm)=24.5-35.5 MeV; 20Ne(16O, 12C), E(cm)=22.8-38.6 MeV; analyzed σ(θ) vs E. 24Mg(12C, 12C), E(cm)=26.67 MeV; analyzed σ(θ); deduced optical model parameters. Exact finite-range DWBA calculations.
doi: 10.1016/0375-9474(83)90203-8
1983NU01 Nucl.Phys. A399, 259 (1983) J.Nurzynski, C.H.Atwood, T.R.Ophel, D.F.Hebbard, B.A.Robson, R.Smith The 24Mg(16O, 16O') Reaction and Triaxial Structures in 24Mg NUCLEAR REACTIONS 24Mg(16O, 16O'), E=43.5 MeV; measured σ(θ); deduced optical model parameters. 24Mg levels deduced B(E2), quadrupole moment, β4/β2, shape parameters. Asymmetric rotor model, coupled-channels analysis.
doi: 10.1016/0375-9474(83)90607-3
1983RO05 Phys.Lett. 123B, 160 (1983) Resonant Structures in the 24Mg(16O, 12C)28Si Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=28-50 MeV; analyzed σ(θ) vs E. 40Ca deduced resonances, J, π. Exact, finite-range DWBA, spin-, parity-dependent term in entrance channel potentials.
doi: 10.1016/0370-2693(83)90413-6
1982RI05 Aust.J.Phys. 35, 9 (1982); Corrigendum Aust.J.Phys. 35, 351 (1982) L.Rikus, S.F.Collins, K.A.Amos, B.M.Spicer, G.G.Shute, I.Morrison, V.C.Officer, R.Smith, D.W.Devins, D.L.Friesel, W.P.Jones Excitation of the 9.50 MeV (9/2+) States of 13C in Intermediate Energy Scattering Experiments NUCLEAR REACTIONS 13C(p, p'), E=135 MeV; measured σ(θ). 13C state deduced total angular momentum transfer, configuration. Microscopic DWBA analysis.
1982SC20 Nucl.Phys. A381, 195 (1982) Wave Functions for Low-Lying States of Light Deformed Nuclei using a Realistic Hamiltonian and Their Test by Inelastic Scattering: The case of 20Ne NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; calculated σ(θ), spectroscopic factors. Deformed particle-hole model, microscopic antisymmetrized DWBA.
doi: 10.1016/0375-9474(82)90140-3
1981AM01 Phys.Rev. C23, 1 (1981) Intermediate Giant Resonance Excitation Effects in Direct Reaction (p, 2p) Correlations NUCLEAR REACTIONS 12C(p, 2p), E=98.7, 150 MeV; calculated σ(θ1, θ2, E1); deduced optical resonance effects. Semi-direct scattering, resonance effects, asymmetric energy sharing geometry.
doi: 10.1103/PhysRevC.23.1
1981AM08 Aust.J.Phys. 34, 493 (1981) K.Amos, I.Morrison, R.Smith, K.W.Schmid The Spectrum of 12C in a Multi-Configuration Hartree-Fock Basis NUCLEAR STRUCTURE 12C; calculated levels, B(E2). Shell model, realistic g-matrix, projected Hartree-Fock, one-particle, one-hole basis. NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal, transverse form factors, isoscalar, isovector excitations.
doi: 10.1071/PH810493
1981BA12 J.Phys.(London) G7, 657 (1981) F.C.Barker, R.Smith, I.Morrison, K.Amos 4- States of 16O in the Region of 19 MeV Excitation NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; calculated σ(θ). DWBA, isospin mixing model, pion scattering, nucleon pickup data input.
doi: 10.1088/0305-4616/7/5/010
1981BA45 Nucl.Phys. A369, 25 (1981) A.M.Baxter, S.Hinds, R.H.Spear, T.H.Zabel, R.Smith Octupole Vibrations in the Even Mercury and Lead Isotopes NUCLEAR REACTIONS 198,200,202,204Hg, 204,206,208Pb(α, α'), E=24, 27 MeV; measured σ(Eα'). 198,200,202,204Hg, 204,206,208Pb deduced levels. 204Hg, 204,206,208Pb(α, α'), E=27 MeV; measured σ(Eα, θ). 204Hg, 204,206,208Pb levels deduced J, π, L, β2, β3. Enriched targets.
doi: 10.1016/0375-9474(81)90004-X
1981LO08 Nucl.Phys. A361, 399 (1981) J.Lomnitz-Adler, V.R.Pandharipande, R.A.Smith Monte Carlo Calculations of Triton and 4He Nuclei with the Reid Potential NUCLEAR STRUCTURE 3H, 4He; calculated binding energy, density distribution. Reid potential, Monte Carlo calculations.
doi: 10.1016/0375-9474(81)90642-4
1981NU02 Nucl.Phys. A363, 253 (1981) J.Nurzynski, T.R.Ophel, P.D.Clark, J.S.Eck, D.F.Hebbard, D.C.Weisser, B.A.Robson, R.Smith Energy Dependence of the 24Mg(16O, 12C)28Si Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E=32.4-48.6 MeV; measured σ(E, θ); 24Mg(16O, 16O), E=37.5, 40.2 MeV; measured σ(θ); deduced optical model parameters. 40Ca resonances deduced J. DWBA analysis, band crossing model.
doi: 10.1016/0375-9474(81)90465-6
1980MO19 Phys.Lett. B95, 13 (1980) Alpha Spectroscopic Factors for the Te(d, 6Li)Sn and Sn(d, 6Li) Reactions in the IBA Model NUCLEAR REACTIONS 122,130Te(d, 6Li), 118,116Sn(d, 6Li), E=33 MeV; calculated Sα. Interacting boson model.
doi: 10.1016/0370-2693(80)90387-1
1980MO25 Nucl.Phys. A350, 89 (1980) The Interacting Boson Approximation and the Spectroscopy of the Even Cadmium and Tin Isotopes NUCLEAR STRUCTURE 108,110,112,114,116Cd, 114,116,118,120,122,124Sn; calculated levels, B(E2), static quadrupole moment. Interacting boson approximation. NUCLEAR REACTIONS 116,118,120,122,124Sn(p, p'), E=16, 24.5 MeV; 110,114,116Cd(p, p'), E=55.16 MeV; calculated σ(θ). Distorted wave formalism, interacting boson approximation, inelastic spectroscopic factors.
doi: 10.1016/0375-9474(80)90390-5
1980SM03 Aust.J.Phys. 33, 1 (1980) Analysis of the (p, 2p) Reaction in an Asymmetric Energy-Sharing Mode NUCLEAR REACTIONS 12C(p, 2p), E=98.7 MeV; analyzed symmetric, asymmetric energy-sharing data. Central, tensor T-matrix operators, intermediate giant resonance excitation.
doi: 10.1071/PH800001
1979SM07 Aust.J.Phys. 32, 155 (1979) A Comparison of Effective Two-Nucleon Interactions Appropriate for Use in Analyses of Inelastic Nucleon Scattering NUCLEAR REACTIONS 89Y(p, p'), E=24.5, 61.4 MeV; 90Zr(p, p'), E=22.97, 35 MeV; 28Si(p, p'), E=135 MeV; calculated σ(θ); effective two-nucleon interactions from realistic potentials, DWBA analysis.
doi: 10.1071/PH790155
1978AM03 Aust.J.Phys. 31, 1 (1978) K.Amos, J.Morton, I.Morrison, R.Smith Analyses of Inelastic Proton Scattering to High Spin States of Unnatural Parity NUCLEAR REACTIONS 24Mg, 28Si(p, p'), E=135 MeV; calculated σ to unnatural parity high-spin states. DWA calculations.
doi: 10.1071/PH780001
1978AM04 Nucl.Phys. A304, 191 (1978) K.Amos, A.Faessler, I.Morrison, R.Smith, H.Muther Self-Consistent Models of Collective and Single-Particle Structures and their Test by Inelastic Scattering: The Case of 54Fe NUCLEAR STRUCTURE 54Fe; calculated spectroscopic amplitudes, B(λ).
doi: 10.1016/0375-9474(78)90103-3
1978MO06 Phys.Rev. C17, 1485 (1978) I.Morrison, R.Smith, P.Nesci, K.Amos Low Excitation Structure of 18O NUCLEAR STRUCTURE 18O; calculated levels, J, π, transition rates. Hartree-Fock analysis.
doi: 10.1103/PhysRevC.17.1485
1977AM01 Phys.Rev.Lett. 38, 1055 (1977) A.A.Amsden, J.N.Ginocchio, F.H.Harlow, J.R.Nix, M.Danos, E.C.Halbert, R.K.Smith, Jr. Comparison of Macroscopic and Microscopic Calculations of High-Energy 20Ne + 238U Collisions NUCLEAR REACTIONS 238U(20Ne, X), E=250 MeV/nucleon; calculated σ(θ) for outgoing protons.
doi: 10.1103/PhysRevLett.38.1055
1977MO21 J.Phys.(London) G3, 1689 (1977) A Simple Model of 90Zr NUCLEAR STRUCTURE 90Zr; calculated levels. NUCLEAR REACTIONS 90Zr(p, p'), E=61.2 MeV; calculated σ(θ).
doi: 10.1088/0305-4616/3/12/009
1977RI11 Nucl.Phys. A286, 494 (1977) L.Rikus, R.Smith, I.Morrison, K.Amos A Microscopic Model Analysis of the 90Zr(p, n) IAS Transition NUCLEAR REACTIONS 90Zr(p, n), E=18.5-45 MeV; calculated σ(E, θ) to IAS.
doi: 10.1016/0375-9474(77)90598-X
1976AM04 Aust.J.Phys. 29, 233 (1976) Direct Reaction Inelastic Proton Scattering from 20Ne NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; calculated σ(θ), scattering amplitudes.
doi: 10.1071/PH760233
1976BA49 Nucl.Sci.Eng. 60, 369 (1976) D.M.Barton, B.C.Diven, G.E.Hansen, G.A.Jarvis, P.G.Koontz, R.K.Smith Measurement of the Uranium-235 Fission Cross Section over the Neutron Energy Range 1 to 6 MeV NUCLEAR REACTIONS 235U(n, F), E=1-6 MeV; measured σ(E) relative to 1H(n, n).
doi: 10.13182/NSE76-A26898
1976CU01 Phys.Rev.Lett. 36, 1166 (1976) R.Y.Cusson, R.K.Smith, J.A.Maruhn Time-Dependent Hartree-Fock Calculation of the Reaction 16O + 16O in Three Dimensions NUCLEAR REACTIONS 16O(16O, X); calculated reaction parameters. Time-dependent Hartree-Fock.
doi: 10.1103/PhysRevLett.36.1166
1975MO16 Nucl.Phys. A244, 189 (1975) Inelastic Proton Scattering and the Spectroscopy of 54Fe and 56Fe NUCLEAR REACTIONS 54,56Fe(p, p'), E=49.35 MeV; calculated σ(Ep', θ). 54,56Fe levels deduced B(λ), S.
doi: 10.1016/0375-9474(75)90055-X
1975NE08 Aust.J.Phys. 28, 659 (1975) P.Nesci, R.Smith, K.Amos, H.V.Geramb Shell Structure of the Even Tellurium Isotopes and Inelastic Proton Scattering NUCLEAR REACTIONS 122,126,128,130Te(p, p'), E=51.9 MeV; calculated σ(θ). Shell structure of Te isotopes.
doi: 10.1071/PH750659
1975SM01 Phys.Lett. 55B, 162 (1975) Giant Resonance Effects in the Analysing Power from Inelastic Proton Scattering NUCLEAR REACTIONS 16O(polarized p, p), E=30.4 MeV; analyzed σ, A.
doi: 10.1016/0370-2693(75)90433-5
1974AM03 Nucl.Phys. A226, 519 (1974) Spin-Dependent Effects in Inelastic Scattering NUCLEAR REACTIONS 54Fe(p, p'), E=10, 19.6, 30.4, 40, 49.35 MeV; 56Fe(p, p'), E=19.6 MeV; calculated σ(θ), A(θ), spin-flip probability.
doi: 10.1016/0375-9474(74)90498-9
1973SM16 Aust.J.Phys. 26, 575 (1973) An Analysis of Inelastic Scattering to the 2+ State in 54Fe at 1.409 MeV NUCLEAR REACTIONS 54Fe(p, p'), E=19.6 MeV; measured nothing, analyzed data.
doi: 10.1071/PH730575
1967SM02 Nucleonics 25, No.4, 7 (1967) GA Data on Ca47 NUCLEAR STRUCTURE 47Ca; measured not abstracted; deduced nuclear properties.
1966HO06 Nucl.Phys. 83, 9 (1966) Radiative Transition Probability from the 3/2+ State to the 3/2- State in 5He NUCLEAR STRUCTURE 5He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90338-5
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