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Search: Author = L.C.Dennis

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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
Citations: PlumX Metrics


1993GA02      Phys.Rev. C47, 329 (1993)

D.L.Gay, L.C.Dennis

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1985PA08      Phys.Rev. C31, 1794 (1985)

S.J.Padalino, L.C.Dennis

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0229.


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
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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
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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
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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
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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
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1982TA23      Nucl.Phys. A391, 458 (1982)

S.L.Tabor, L.C.Dennis, K.Abdo

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0061.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1393.


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
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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
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1981TA22      Phys.Rev. C24, 2552 (1981)

S.L.Tabor, L.C.Dennis, K.Abdo

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
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1980DE18      Phys.Rev. C22, 340 (1980)

L.C.Dennis, S.T.Thornton

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
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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
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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
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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
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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
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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
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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
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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
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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
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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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