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Search: Author = A.D.Frawley

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2014FR13      Nucl.Phys. A932, 105c (2014)

A.D.Frawley, for the PHENIX Collaboration

PHENIX charmonia: What have we learned from d+Au collisions?

doi: 10.1016/j.nuclphysa.2014.10.032
Citations: PlumX Metrics


2013FR15      Nucl.Phys. 910-911, 123c (2013)

A.D.Frawley, for the PHENIX Collaboration

Cold Nuclear Matter Effects and Heavy Quark Production in PHENIX

doi: 10.1016/j.nuclphysa.2012.12.032
Citations: PlumX Metrics


2013MC06      Phys.Rev. C 87, 054910 (2013)

D.McGlinchey, A.D.Frawley, R.Vogt

Impact-parameter dependence of the nuclear modification of J/ψ production in d+Au collisions at √ sNN=200 GeV

doi: 10.1103/PhysRevC.87.054910
Citations: PlumX Metrics


2013NE01      Phys.Rev. C 87, 014908 (2013)

R.E.Nelson, R.Vogt, A.D.Frawley

Narrowing the uncertainty on the total charm cross section and its effect on the J/ψ cross section

doi: 10.1103/PhysRevC.87.014908
Citations: PlumX Metrics


2013VO11      Nucl.Phys. 910-911, 231c (2013)

R.Vogt, R.E.Nelson, A.D.Frawley

Improving the J/ψ Production Baseline at RHIC and the LHC

doi: 10.1016/j.nuclphysa.2012.12.106
Citations: PlumX Metrics


2011NA32      Phys.Rev. C 84, 044911 (2011)

J.L.Nagle, A.D.Frawley, L.A.Linden Levy, M.G.Wysocki

Modeling of J/ψ modifications in deuteron-nucleus collisions at high energies

doi: 10.1103/PhysRevC.84.044911
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2008CH04      Phys.Rev. C 77, 015209 (2008); Erratum Phys.Rev. C 77, 049903 (2008)

I.Chemakin, V.Cianciolo, B.A.Cole, R.C.Fernow, A.D.Frawley, M.Gilkes, S.Gushue, E.P.Hartouni, H.Hiejima, M.Justice, J.H.Kang, H.G.Kirk, J.M.Link, N.Maeda, R.L.McGrath, S.Mioduszewski, J.Monroe, D.Morrison, M.Moulson, M.N.Namboodiri, G.Rai, K.Read, L.Remsberg, M.Rosati, Y.Shin, R.A.Soltz, M.Sorel, S.Sorensen, J.H.Thomas, Y.Torun, D.L.Winter, X.Yang, W.A.Zajc, Y.Zhang

Pion production by protons on a thin beryllium target at 6.4, 12.3, and 17.5 GeV/c incident proton momenta

NUCLEAR REACTIONS Be(p, π+π-), E at 6.4, 12.3, 17.5 GeV/c; measured cross sections, pion momentum.

doi: 10.1103/PhysRevC.77.015209
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2004FR22      J.Phys.(London) G30, S675 (2004)

A.D.Frawley, for the PHENIX Collaboration

PHENIX highlights

doi: 10.1088/0954-3899/30/8/005
Citations: PlumX Metrics


2003FR06      Nucl.Phys. A715, 687c (2003)

A.D.Frawley, and the PHENIX Collaboration

J/ψ → ee and J/ψ → μμ Measurements in AuAu and pp Collisions at √ SNN = 200 GeV

NUCLEAR REACTIONS 1H(p, X), 197Au(197Au, X), E(cm)=200 GeV/nucleon; measured dilepton spectra, J/ψ production σ.

doi: 10.1016/S0375-9474(02)01467-7
Citations: PlumX Metrics


2002CH05      Phys.Rev. C65, 024904 (2002)

I.Chemakin, V.Cianciolo, B.A.Cole, R.A.Fernow, A.D.Frawley, M.Gilkes, S.Gushue, E.P.Hartouni, H.Hiejima, M.Justice, J.H.Kang, H.G.Kirk, N.Maeda, R.L.McGrath, S.Mioduszewski, D.Morrison, M.Moulson, M.N.Namboodiri, R.B.Palmer, G.Rai, K.Read, L.Remsberg, M.Rosati, Y.Shin, R.A.Soltz, S.Sorensen, J.H.Thomas, Y.Torun, D.L.Winter, X.Yang, W.A.Zajc, Y.Zhang

Inclusive Soft Pion Production from 12.3 and 17.5 GeV/c Protons on Be, Cu, and Au

NUCLEAR REACTIONS Be, Cu, 197Au(p, π+X), (p, π-X), E at 12.3, 17.5 GeV/c; measured pion production σ(E, θ).

doi: 10.1103/PhysRevC.65.024904
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2000CH48      Phys.Rev.Lett. 85, 4868 (2000)

I.Chemakin, V.Cianciolo, B.A.Cole, R.Fernow, A.D.Frawley, M.Gilkes, S.Gushue, E.P.Hartouni, H.Hiejima, M.Justice, J.H.Kang, H.Kirk, N.Maeda, R.L.McGrath, S.Mioduszewski, D.Morrison, M.Moulson, M.N.Namboodiri, G.Rai, K.Read, L.Remsberg, M.Rosati, Y.Shin, R.A.Soltz, S.Sorensen, J.H.Thomas, Y.Torun, D.Winter, X.Yang, W.A.Zajc, Y.Zhang

Semi-Inclusive Λ and KS Production in p-Au Collisions at 17.5 GeV/c

NUCLEAR REACTIONS 197Au(p, X), E at 17.5 GeV/c; measured hyperon, kaon rapidity density distributions, multiplicities, centrality dependence.

doi: 10.1103/PhysRevLett.85.4868
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1995FR17      Phys.Rev. C52, 1565 (1995)

A.D.Frawley

Fission following Complete Fusion for 16O + 232Th at 140 MeV

NUCLEAR REACTIONS 232Th(16O, F), E=140 MeV; analyzed fission fragment σ(θ); deduced parameters. Saddle point transition state model.

doi: 10.1103/PhysRevC.52.1565
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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
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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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1990TR02      Phys.Rev. C41, 2134 (1990)

D.E.Trcka, A.D.Frawley, K.W.Kemper, D.Robson, J.D.Fox, E.G.Myers

Angular Momentum Dependent Absorption in 6Li Scattering

NUCLEAR REACTIONS 12C(6Li, 6Li), E=20, 50 MeV; 9Be, 16O, 12C(6Li, 6Li'), 9Be, 16O(6Li, 6Li), E=50 MeV; measured σ(θ); deduced model parameters. Optical model.

doi: 10.1103/PhysRevC.41.2134
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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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1986MA13      Phys.Rev. C33, 1307 (1986)

J.F.Mateja, A.D.Frawley, R.A.Parker, K.Sartor

Experimental Search for Nonfusion Yield in the Heavy Residues Emitted in the 11B + 12C Reaction

NUCLEAR REACTIONS, ICPND 12C(11B, X), E=48 MeV; 11B(12C, X), E=52.36 MeV; measured σ(fragment θ, E) vs mass in range 11-22; deduced σ, fusion-evaporation strength. 12C(11B, 11B), (11B, 12C), E=48 MeV; 11B(12C, 11B), E not given; measured σ(θ).

doi: 10.1103/PhysRevC.33.1307
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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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1985MA10      Phys.Rev. C31, 867 (1985)

J.F.Mateja, A.D.Frawley, D.G.Kovar, D.Henderson, H.Ikezoe, R.V.F.Janssens, G.Rosner, G.S.F.Stephans, B.Wilkins, K.T.Lesko, M.F.Vineyard

10B + 13C and 11B + 12C Reactions from 4 to 9 MeV/Nucleon

NUCLEAR REACTIONS, ICPND 12C(11B, X), (11B, 11B), 13C(10B, 10B), (10B, X), E=4-9 MeV/nucleon; measured σ(θ), σ(fragment E) for fragment mass=15, 20, 11, 6, fusion σ vs E; deduced nonfusion σ for mass 6-13, entrance channel role in fusion. 23Na deduced critical L vs excitation energy.

doi: 10.1103/PhysRevC.31.867
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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.


1983MA53      Phys.Rev. C28, 1579 (1983)

J.F.Mateja, J.Garman, A.D.Frawley

Fast Light-Particle Production for the 11B + 12C and 10B + 13C Reactions

NUCLEAR REACTIONS, ICPND 12C(11B, p), (11B, d), (11B, t), (11B, α), (11B, 6Li), (11B, 7Li), (11B, 7Be), (11B, 9Be); 13C(10B, p), (10B, d), (10B, t), (10B, α), (10B, 6Li), (10B, 7Li), (10B, 7Be), (10B, 9Be), E=54 MeV; measured σ(θ), σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, Eα), σ(θ, E(6Li)), σ(θ, E(7Li)), σ(θ, E(7Be)), σ(θ, E(9Be)); deduced σ, reaction mechanisms. Projectile breakup model.

doi: 10.1103/PhysRevC.28.1579
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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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.


1981FR11      Nucl.Phys. A363, 280 (1981)

A.D.Frawley, A.Roy, J.F.Mateja, N.R.Fletcher

Search for 8+ Strength in 16O via the 12C(α, α2)12C*(7.66 MeV) Reaction

NUCLEAR REACTIONS 12C(α, α), E=17.39-20.5 MeV; measured σ(Eα, θ). 16O deduced resonance J, π. Natural target.

doi: 10.1016/0375-9474(81)90256-6
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1981MA02      Nucl.Phys. A351, 509 (1981)

J.F.Mateja, D.P.Stanley, L.V.Theisen, A.D.Frawley, P.L.Pepmiller, L.R.Medsker, P.B.Nagel

A Woods-Saxon and Double-Folding Optical-Model Description of 14N Elastic and Inelastic Scattering from 24Mg, 27Al and 28Si

NUCLEAR REACTIONS 27Al(14N, 14N), E=52.3 MeV; 24Mg, 28Si(14N, 14N), (14N, 14N'), E=53, 53.4 MeV; measured σ(θ); deduced Woods-Saxon and double-folding optical model parameters. 24Mg, 28Si deduced deformation lengths.

doi: 10.1016/0375-9474(81)90185-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1370.


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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1981SZ02      Nucl.Phys. A355, 221 (1981)

J.Szymakowski, K.W.Kemper, A.D.Frawley

Elastic Scattering of 6Li by 39K at 28 and 34 MeV

NUCLEAR REACTIONS 39K(6Li, 6Li), E=28, 34, 37 MeV; measured σ(θ); deduced Woods-Saxon and double folding optical-model parameters. Natural target.

doi: 10.1016/0375-9474(81)90139-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1353.


1980FR05      Phys.Rev.Lett. 44, 1377 (1980)

A.D.Frawley, A.Roy, N.R.Fletcher

Transparency to the l = 9 Partial Wave in the Region of the 14.7-MeV Resonance in 12C + 16O

NUCLEAR REACTIONS 12C(16O, 16O), (16O, X), E=20, 32.6-35.3 MeV; measured σ(θ), total reaction σ. 28Si resonance deduced Γ(partial)/Γ vs residual mass, L. Partial wave analysis.

doi: 10.1103/PhysRevLett.44.1377
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1980GL07      Phys.Rev. C22, 522 (1980)

C.W.Glover, K.W.Kemper, A.D.Frawley

11B+40Ca Single-Nucleon Transfer Reactions E(lab)=51.5 MeV

NUCLEAR REACTIONS 40Ca(11B, 12C), (11B, 10B), E=51.5 MeV; measured σ(θ); deduced optical model parameters. 39K, 41Ca levels deduced C2S. DWBA analysis, Woods-Saxon, double-folding optical potentials.

doi: 10.1103/PhysRevC.22.522
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1980HU07      Phys.Rev. C22, 528 (1980)

J.R.Hurd, N.R.Fletcher, A.D.Frawley, J.F.Mateja

Intermediate Structures and Their Dominant l Values in 16O(12C, 8Be)20Ne Reactions, E(c.m.)=11.5 to 18.6 MeV

NUCLEAR REACTIONS 16O(12C, 8Be), E(cm)=11.5-18.6 MeV; measured σ(E, θ). 28Si deduced resonances, J, π, Γ.

doi: 10.1103/PhysRevC.22.528
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1979FR05      Phys.Rev. C19, 2215 (1979)

A.D.Frawley, J.F.Mateja, A.Roy, N.R.Fletcher

Resonances in the 11B + 12C System

NUCLEAR REACTIONS 12C(11B, 8Be), (11B, α), (11B, 11B), (11B, 11B'), E(cm)=9.4-17.8 MeV; measured σ(E, θ). 23Na deduced resonances.

doi: 10.1103/PhysRevC.19.2215
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1979MA21      Phys.Rev. C20, 176 (1979)

J.F.Mateja, A.D.Frawley, P.B.Nagel, L.A.Parks

12C(9Be, 9Be)12C (g.s., 4.43 MeV) Reaction

NUCLEAR REACTIONS 12C(9Be, 9Be), E=40-45 MeV; measured σ(E, θ); deduced reaction mechanism. Enriched target. Hauser-Feshbach, coupled-channel, exchange analysis.

doi: 10.1103/PhysRevC.20.176
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1979RO11      Phys.Rev. C20, 2143 (1979)

A.Roy, A.D.Frawley, K.W.Kemper

Structure in the 180° Scattering of 12C by 27Al

NUCLEAR REACTIONS 27Al, 28Si(12C, 12C), (12C, 12C'), E(cm)=14-25 MeV; measured σ(E, θ); deduced optical model parameters. DWBA analysis.

doi: 10.1103/PhysRevC.20.2143
Citations: PlumX Metrics


1978FR04      Nucl.Phys. A294, 161 (1978)

A.D.Frawley, K.H.Bray, T.R.Ophel

Energy Levels of 16O Near 15 MeV Excitation from 15N + p Reactions

NUCLEAR REACTIONS 15N(p, p), (p, α), E=2.88-3.64 MeV; measured σ(E, θ). 16O deduced levels, J, π, Γ. Enriched target.

doi: 10.1016/0375-9474(78)90401-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0460.


1978FR11      Z.Phys. A286, 307 (1978)

A.D.Frawley, G.M.Crawley, C.L.Hollas

Fluctuations in Inelastic Proton Scattering from 58Ni in the Energy Range 17.1 to 20.6 MeV

NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=17.1-20.6 MeV; measured σ(E, θ). 59Cu levels deduced Γ. Enriched target.

doi: 10.1007/BF01408262
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1978FR20      Phys.Rev.Lett. 41, 846 (1978)

A.D.Frawley, J.F.Mateja, A.Roy, N.R.Fletcher

Resonances in 11B + 12C Elastic Scattering

NUCLEAR REACTIONS 12C(11B, 11B), E=18.8-34.1 MeV; measured σ(E). 23Na deduced resonances.

doi: 10.1103/PhysRevLett.41.846
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1978MA44      Phys.Rev. C18, 2622 (1978)

J.F.Mateja, A.D.Frawley, A.Roy, J.R.Hurd, N.R.Fletcher

Resonances in 12C + 9Be

NUCLEAR REACTIONS 12C(9Be, 9Be), (9Be, 9Be'), (9Be, α), 9Be(12C, 8Be), E(cm)=10-15 MeV; measured σ(θ). 21Ne deduced resonances, widths, L-transfer.

doi: 10.1103/PhysRevC.18.2622
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1977BR32      Nucl.Phys. A288, 334 (1977)

K.H.Bray, A.D.Frawley, T.R.Ophel, F.C.Barker

Levels of 16O Near 13 MeV Excitation from 15N + p Reactions

NUCLEAR REACTIONS 15N(p, α0), 15N(p, αγ), E=0.9-1.25 MeV; measured σ(Ep, θ), Doppler profiles. 16O deduced levels, J, π, Γ. Enriched target.

doi: 10.1016/0375-9474(77)90139-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0710.


1976OP02      Nucl.Phys. A273, 397 (1976)

T.R.Ophel, A.D.Frawley, P.B.Treacy, K.H.Bray

A Remeasurement of the 12C(α, γ0) Excitation Function in the Vicinity of the 12.44 and 13.1 MeV Levels of 16O

NUCLEAR REACTIONS 12C(α, γ), E=6.5-8.5 MeV; measured σ(E, Eγ). 16O deduced resonance. Enriched target.

doi: 10.1016/0375-9474(76)90599-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0709.


1975BR21      Aust.J.Phys. 28, 235 (1975)

K.H.Bray, A.D.Frawley, T.R.Ophel, P.B.Treacy

6Li(d, d'): Direct Breakup Effects and Parameters of the First 2+ Level of 6Li

NUCLEAR REACTIONS 6Li(d, d'), E=20, 25 MeV; measured σ(Ed'). 6Li deduced level parameters.

doi: 10.1071/PH750235
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