NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = L.C.Dennis Found 46 matches. 1995GA08 Phys.Rev. C51, 1991 (1995) E.P.Gavathas, A.D.Frawley, R.C.Kline, L.C.Dennis Total Cross Section Measurements of 16O + 232Th Incomplete Fusion Followed by Fission at 140 MeV NUCLEAR REACTIONS 232Th(16O, X), (16O, F), E=140 MeV; measured (fragment)(fragment)(θ, φ), incomplete fusion followed by fission. Wilczynski Q(opt) model.
doi: 10.1103/PhysRevC.51.1991
1993GA02 Phys.Rev. C47, 329 (1993) Resonant Characteristics of Statistical Fluctuations in 12C + 12C Reaction Cross Sections NUCLEAR REACTIONS, ICPND 12C(12C, 8Be), E(cm)=14-20 MeV; 12C(12C, α), E(cm)=6-12 MeV; analyzed σ(E); deduced reaction mechanism, statistical fluctuations resonant characteristics. Hauser-Feshbach model.
doi: 10.1103/PhysRevC.47.329
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
1993VI02 Phys.Rev. C47, 2374 (1993) M.F.Vineyard, J.F.Mateja, C.Beck, S.E.Atencio, L.C.Dennis, A.D.Frawley, D.J.Henderson, R.V.J.Janssens, K.W.Kemper, D.G.Kovar, C.F.Maguire, S.J.Padalino, F.W.Prosser, G.S.F.Stephans, M.A.Tiede, B.D.Wilkins, R.A.Zingarelli Energy Dependence of Fusion Evaporation-Residue Cross Sections in the 28Si + 12C Reaction NUCLEAR REACTIONS 12C(28Si, X), E(cm)=18-136 MeV; measured σ(evaporation residue) vs E, fragment velocity distributions. Model comparison. Other reactions analyzed.
doi: 10.1103/PhysRevC.47.2374
1993ZI04 Phys.Rev. C48, 651 (1993) R.A.Zingarelli, L.C.Dennis, M.A.Tiede, R.C.Kline, K.W.Kemper, S.V.Mitchell Complete and Incomplete Momentum Transfer Components in the (nat)Si(16O, X) Reaction at 96.4, 112.4, and 127.8 MeV NUCLEAR REACTIONS 28Si(16O, X), E=96.4-127.8 MeV; measured fusion, incomplete fusion σ. Fusion-evaporation models.
doi: 10.1103/PhysRevC.48.651
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
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
1990PA01 Phys.Rev. C41, 594 (1990) S.J.Padalino, M.A.Putnam, J.A.Constable, T.G.Declerk, L.C.Dennis, R.Zingarelli, R.Kline, K.Sartor Projectile Breakup in the 27Al(16O, X) Reaction at 72, 84, 96, 110, and 125 MeV Bombarding Energies NUCLEAR REACTIONS 27Al(16O, X), E=72-125 MeV; measured σ(fragment θ), σ(θ, E(X)) for X=C, B, Be, Li, N; deduced total breakup σ, reaction mechanism.
doi: 10.1103/PhysRevC.41.594
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
1988MA07 Phys.Rev. C37, 1004 (1988) J.F.Mateja, G.L.Gentry, N.R.Fletcher, L.C.Dennis, A.D.Frawley Fluctuation and Resonance Analysis for 11B + 12C, 7Li + 16O, and 10B + 13C Induced Reactions NUCLEAR REACTIONS 13C(10B, 13C), (10B, α), E=17.16-31.32 MeV; 10B(13C, 8Be), E=20.71-38.18 MeV; 7Li(16O, 7Li), E=20-50.23 MeV; 16O(7Li, α), E=10.3-22.4 MeV; 7Li(16O, 8Be), E=20-51.2 MeV; 12C(11B, 11B), (11B, α), (11B, α), (11B, 8Be), E=18.8-34.1 MeV; measured σ(θ) vs E; deduced model parameters. 23Na deduced heavy-ion resonance formation entrance channel dependence.
doi: 10.1103/PhysRevC.37.1004
1987GA03 Phys.Rev.Lett. 58, 1512 (1987) D.L.Gay, N.R.Fletcher, L.C.Dennis Resonant Fluctuations in Heavy-Ion Reaction Cross Sections: 16O(16O, α)28Si NUCLEAR REACTIONS, ICPND 16O(16O, α), E=12-20 MeV; calculated σ(E), σ(θ). Compound nucleus decay model.
doi: 10.1103/PhysRevLett.58.1512
1987PA12 Phys.Rev. C35, 1692 (1987) S.J.Padalino, K.Sartor, L.C.Dennis, K.W.Kemper Direct and Fusion Carbon Reaction Components in the 6Li + 12C Reaction at 30 MeV NUCLEAR REACTIONS, ICPND 12C(6Li, α), E=30 MeV; measured σ(Eα, θα). 6Li(12C, X), E=60 MeV; calculated fusion product yield vs charge distributions, 12C spectrum, σ(θ). 7Li(12C, 12C), E=58.4 MeV; 6Li(16O, 16O), E=68.6 MeV; calculated spectra. ΔE-E telescope. Statistical model.
doi: 10.1103/PhysRevC.35.1692
1986GA24 Phys.Rev. C34, 2144 (1986) D.L.Gay, L.C.Dennis, N.R.Fletcher Resonances and Compound Fluctuations in the Reactions 16O(16O, α) and 16O(16O, 8Be) NUCLEAR REACTIONS 16O(16O, α), (16O, 8Be), E(cm)=12-20 MeV; measured σ(θ, E). 32S deduced resonances, J, π. Statistical model analysis.
doi: 10.1103/PhysRevC.34.2144
1986MA19 Phys.Rev. C33, 1649 (1986) J.F.Mateja, A.D.Frawley, L.C.Dennis, K.Sartor Comparison of 6Li- and 7Li-Induced Fusion Cross Sections on 16O NUCLEAR REACTIONS, ICPND 16O(6Li, X), E=12-35 MeV; measured σ(fragment θ, E) for X=10-22, fusion σ(E); deduced critical angular momenta. Comparison with (7Li, X) data.
doi: 10.1103/PhysRevC.33.1649
1986PA05 Phys.Rev. C33, 1805 (1986) S.J.Padalino, R.A.Parker, L.C.Dennis Angular Correlation Measurements in the 27Al(16O, α12C) Reaction at 65 MeV Bombarding Energy NUCLEAR REACTIONS 27Al(16O, α12C), E=65 MeV; measured σ(θα, θ(12C)); deduced reaction mechanism.
doi: 10.1103/PhysRevC.33.1805
1986VO12 Phys.Rev. C34, 2180 (1986) G.Vourvopoulos, C.F.Maguire, Z.Kui, L.C.Dennis, K.W.Kemper, D.P.Sanderson Search for Intermediate Structure in the 19F + 12C System NUCLEAR REACTIONS 12C(19F, α), E=41-57 MeV; measured σ(θ) vs E; deduced deviation, correlation functions. Hauser-Feshbach calculations. Natural targets.
doi: 10.1103/PhysRevC.34.2180
1985HA30 Phys.Rev. C32, 1897 (1985) P.S.Haskins, F.E.Dunnam, R.L.Coldwell, A.C.Rester, R.B.Piercey, M.L.Muga, H.A.Van Rinsvelt, R.W.Smart, H.J.M.Aarts, J.D.Fox, L.C.Dennis, C.B.Saw In-Beam Gamma-Ray Spectroscopy of 82Sr NUCLEAR REACTIONS 70Ge(16O, 2n2p), E=80 MeV; measured Eγ, Iγ, γγ(t), γ(θ), polarization. 82Sr deduced levels, J, π, δ.
doi: 10.1103/PhysRevC.32.1897
1985PA08 Phys.Rev. C31, 1794 (1985) Incomplete Fusion Calculations in the 27Al(16O, xy) Reaction at 65, 77, and 87.4 MeV Bombarding Energies NUCLEAR REACTIONS 27Al(16O, α12C), (16O, p12C), E=65, 77, 87.4 MeV; measured σ(θα, θ(12C)), σ(θp, θ(12C)), α12C-, p12C-coin. Incomplete fusion analysis.
doi: 10.1103/PhysRevC.31.1794
1985PA24 Phys.Rev. C32, 1563 (1985) R.A.Parker, A.D.Frawley, L.C.Dennis Optical Model Plus Resonance Analysis of 12C + 12C Elastic Scattering NUCLEAR REACTIONS, ICPND 12C(12C, 12C), E(cm)=17.5-21.5 MeV; measured σ(θ), σ(E). 24Mg deduced intermediate resonances, J, π. Optical model plus multi-level resonance calculation.
doi: 10.1103/PhysRevC.32.1563
1984CO05 Nucl.Phys. A415, 114 (1984) J.Cook, L.C.Dennis, K.W.Kemper, T.R.Ophel, A.F.Zeller, C.F.Maguire, Z.Kui Large-Angle Enhancements in the 16O(6Li, α)18F Reaction at 48 MeV NUCLEAR REACTIONS 16O(6Li, 6Li), (6Li, α), E=48 MeV; measured σ(θ); deduced optical model parameters. Finite-range DWBA analysis including exchange.
doi: 10.1016/0375-9474(84)90602-X
1984MA28 Phys.Rev. C30, 134 (1984) J.F.Mateja, J.Garman, D.E.Fields, R.L.Kozub, A.D.Frawley, L.C.Dennis Fusion Cross Sections for Four Heavy-Ion Entrance Channels leading to the 23Na Compound Nucleus NUCLEAR REACTIONS, ICPND 16O(7Li, X), E=12-34 MeV; 9Be(14N, X), E=15-57 MeV; measured residual fragment production σ vs mass, compound nucleus excitation, fusion σ(E), reaction σ(E). 23Na level deduced entrance channel spin.
doi: 10.1103/PhysRevC.30.134
1983FR04 Nucl.Phys. A394, 292 (1983) A.D.Frawley, N.R.Fletcher, L.C.Dennis, K.M.Abdo Resonances in 12C + 13C at E(cm) = 9.4 and 10.3 MeV Observed in the Total Fusion Cross Section NUCLEAR REACTIONS, ICPND 12C(13C, X), E(cm)=8.8-10.9 MeV; measured fusion σ(E). 25Mg deduced resonances. Optical model analysis.
doi: 10.1016/0375-9474(83)90174-4
1983FR14 Phys.Rev. C27, 2482 (1983) A.D.Frawley, J.D.Fox, L.C.Dennis, K.W.Kemper, N.R.Fletcher Search for a 3- State at 9.85 MeV Excitation in 16O via the 16O(α, α')16O*(9.85 MeV)(α0)12C Angular Correlation NUCLEAR REACTIONS 16O(α, α'), E=22-27.5 MeV; measured σ(Eα), relative yields, αα(θ), σ(Eα1, Eα2). 16O deduced no evidence for predicted 3- state.
doi: 10.1103/PhysRevC.27.2482
1982AB02 Nucl.Phys. A377, 281 (1982) K.M.Abdo, L.C.Dennis, A.D.Frawley, K.W.Kemper Direct and Compound Nuclear Contributions to the 13C(6Li, t) Reaction at E = 25 MeV NUCLEAR REACTIONS, ICPND 13C(6Li, t), E=24-26 MeV; measured σ(θ, E), σ(θ), σ(Et); 13C(6Li, t), E=9-35 MeV; measured fusion σ (E); 6Li(13C, t), E=54.2 MeV; measured σ(Et), σ(θ); deduced compound nucleus contributions. 16O levels deduced L, S. Finite-range DWBA analysis.
doi: 10.1016/0375-9474(82)90334-7
1982DE30 Phys.Rev. C26, 981 (1982) L.C.Dennis, K.M.Abdo, A.D.Frawley, K.W.Kemper Fusion of Li and C and a Search for Entrance Channel Limitations to Fusion Cross Sections NUCLEAR REACTIONS 12C(6Li, X), E=10-36 MeV; 13C(6Li, X), E=9.23-35.08 MeV; 12C(7Li, X), E=10-38 MeV; 13C(7Li, X), E=10-34 MeV; measured σ(fragment θ, E), production σ(E) for A=9-19; deduced σ(fusion) vs E.
doi: 10.1103/PhysRevC.26.981
1982FR04 Phys.Rev. C25, 860 (1982) A.D.Frawley, N.R.Fletcher, L.C.Dennis Resonances in the 16O + 12C Fusion Cross Section between E(cm) = 12 and 20 MeV NUCLEAR REACTIONS, ICPND 12C(16O, X), E(cm)=12-20 MeV; measured σ(fragment θ, E, mass); deduced fusion σ vs fragment mass, E. 28Si deduced resonances.
doi: 10.1103/PhysRevC.25.860
1982FR10 Phys.Rev. C25, 2935 (1982) A.D.Frawley, J.D.Fox, K.W.Kemper, L.C.Dennis Reexamination of 12C + α Scattering near 9.85 MeV Excitation in 16O NUCLEAR REACTIONS 12C(α, α), E=3.5-3.62 MeV; measured σ(θ) vs E. 16O deduced level, J, π. R-matrix analysis.
doi: 10.1103/PhysRevC.25.2935
1982MA20 Phys.Rev. C25, 2963 (1982) J.F.Mateja, A.D.Frawley, L.C.Dennis, K.Abdo, K.W.Kemper 11B + 12C and 10B + 13C Fusion Cross Sections NUCLEAR REACTIONS, ICPND 12C(11B, X), E=14-54 MeV; 12C(11B, 11B), E=25, 40, 50 MeV; 13C(10B, X), E=14-48 MeV; 13C(10B, 10B), E=18, 25, 32, 39, 46 MeV; measured σ(fragment θ, E) for A=9-22; deduced fusion σ vs E. 23Na deduced L(critical) vs excitation. Optical model, Monte Carlo, Hauser Feshbach calculations.
doi: 10.1103/PhysRevC.25.2963
1982TA23 Nucl.Phys. A391, 458 (1982) Projectile Breakup and Total Reaction Strengths in Li-Induced Reactions NUCLEAR REACTIONS, ICPND 12,13C, 27Al(6Li, p), (6Li, d), (6Li, t), (6Li, α), (7Li, p), (7Li, d), (7Li, t), (7Li, α), (7Li, 6Li), E=36, 32, 28 MeV; measured yield vs particle energy, σ(θ), fusion σ, breakup σ vs E; deduced reaction mechanism. Optical, simple breakup model analyses.
doi: 10.1016/0375-9474(82)90620-0
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
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
1981DE15 Nucl.Phys. A359, 455 (1981) L.C.Dennis, A.Roy, A.D.Frawley, K.W.Kemper 12C + 7Li Reaction Measurements and the 12C(7Li, t)16O Reaction NUCLEAR REACTIONS 12C(7Li, X), E=10-38 MeV; measured σ(θ, E) for all X with masses A=9-18; 7Li(12C, t), E=54-62 MeV; measured σ(E); deduced σ(fusion), critical angular momenta. Hauser-Feshbach calculations.
doi: 10.1016/0375-9474(81)90249-9
1981MA18 Phys.Rev.Lett. 47, 311 (1981) J.F.Mateja, A.D.Frawley, L.C.Dennis, K.Abdo, K.W.Kemper Entrance-Channel Limitations to 10B + 13C and 11B + 12C Fusion NUCLEAR REACTIONS 12C(11B, X), 13C(10B, X), E=10-54 MeV; measured σ(fusion, E), σ(evaporation residue, θ); deduced entrance channel effects.
doi: 10.1103/PhysRevLett.47.311
1981TA16 Phys.Rev. C24, 960 (1981) S.L.Tabor, L.C.Dennis, K.W.Kemper, J.D.Fox, K.Abdo, G.Neuschaefer, D.G.Kovar, H.Ernst Fragmentation of 16O and 18O Projectiles NUCLEAR REACTIONS 12C, 27Al, 46Ti(16O, X), (18O, X), E=72, 141 MeV; measured σ(fragment E, θ), σ(θ) for Li, Be, B, C, N; deduced projectile fragmentation vs E. Simple breakup model.
doi: 10.1103/PhysRevC.24.960
1981TA22 Phys.Rev. C24, 2552 (1981) Absorptive Breakup of 14N Projectiles NUCLEAR REACTIONS 27Al(14N, X), E=62 MeV; measured σ(θ, fragment E) for X=Li, Be, B, C. Serber-type projectile breakup model.
doi: 10.1103/PhysRevC.24.2552
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
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
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