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Search: Author = J.F.Mateja

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1994VI01      Phys.Rev. C49, 948 (1994)

M.F.Vineyard, S.E.Atencio, J.F.Crum, G.P.Gilfoyle, B.G.Glagola, D.J.Henderson, D.G.Kovar, C.F.Maguire, J.F.Mateja, R.G.Ohl, F.W.Prosser, J.H.Rollinson, R.S.Trotter

Light-Particle Correlations with Evaporation Residues in the 40Ca + 12C Reaction at E(40Ca) = 450 MeV

NUCLEAR REACTIONS 12C(40Ca, X), E=450 MeV; measured α(evaporation residue)-, p(evaporation residue)-coin, α-multiplicity vs θα, Eα, p-multiplicity vs θp, Ep; deduced pre-equilibrium α-, p-emission. Statistical model.

doi: 10.1103/PhysRevC.49.948
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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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1992VI01      Phys.Rev. C45, 1784 (1992)

M.F.Vineyard, J.S.Bauer, J.F.Crum, C.H.Gosdin, R.S.Trotter, D.G.Kovar, C.Beck, D.J.Henderson, R.V.F.Janssens, B.D.Wilkins, C.F.Maguire, J.F.Mateja, F.W.Prosser, G.S.F.Stephans

Fusion Evaporation-Residue Cross Sections for 28Si + 40Ca at E(28Si) = 309, 397, and 452 MeV

NUCLEAR REACTIONS 40Ca(28Si, X), E=309-452 MeV; measured σ(evaporation residue θ); deduced entrance channel mass-asymmetry role. Model comparison.

doi: 10.1103/PhysRevC.45.1784
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1991CA01      Phys.Rev. C43, 205 (1991)

D.D.Caussyn, G.L.Gentry, J.A.Liendo, N.R.Fletcher, J.F.Mateja

Search for High Spin Collective States in 12C(*) → 3α

NUCLEAR REACTIONS 12C(12C, 3α), E=7.5 MeV/nucleon; measured αα-coin. 12C deduced levels, J, π, α-decay branching.

doi: 10.1103/PhysRevC.43.205
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1990VI01      Phys.Rev. C41, 1005 (1990)

M.F.Vineyard, J.S.Bauer, C.H.Gosdin, R.S.Trotter, D.G.Kovar, C.Beck, D.J.Henderson, R.V.F.Janssens, B.D.Wilkins, G.Rosner, P.Chowdhury, H.Ikezoe, W.Kuhn, J.J.Kolata, J.D.Hinnefeld, C.F.Maguire, J.F.Mateja, F.W.Prosser, G.S.F.Stephans

Energy Dependence of Fusion Evaporation-Residue Cross Sections in the 28Si + 28Si Reaction

NUCLEAR REACTIONS, ICPND 28Si(28Si, X), E=174-452 MeV; measured σ(E, θ); deduced critical angular momenta, fusion σ(E). Fusion evaporation residues, complete, incomplete fusion.

doi: 10.1103/PhysRevC.41.1005
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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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1987ME19      Phys.Rev. C36, 1785 (1987)

L.R.Medsker, H.T.Fortune, J.D.Zumbro, C.P.Browne, J.F.Mateja

112Cd from 110Cd(t, p)

NUCLEAR REACTIONS, MECPD 110Cd(t, p), E=15 MeV; measured σ(θ), σ(Et); deduced model parameters. 112Cd deduced levels, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.36.1785
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1302.

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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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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1983KO01      Phys.Rev. C27, 158 (1983)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, J.W.Olness, E.K.Warburton

Lifetimes of Levels in 20,21F, 22Ne, and 16N

NUCLEAR REACTIONS 7Li(18O, α), (18O, nα), (18O, t), E=10-60 MeV; 7Li(11B, np), E=7-35 MeV; measured Eγ, Iγ, recoil. 21F, 22Ne levels deduced T1/2. 16N, 20F levels deduced T1/2, B(λ). Shell model.

doi: 10.1103/PhysRevC.27.158
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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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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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1982ZU02      Phys.Rev. C26, 965 (1982)

J.D.Zumbro, C.P.Browne, J.F.Mateja, H.T.Fortune, R.Middleton

176Yb(t, p)178Yb Reaction

NUCLEAR REACTIONS 176Yb(t, p), E=15 MeV; measured σ(Ep), σ(θ); deduced Q. 178Yb deduced levels, L, J, π, band structure. Magnetic spectrograph. DWBA analysis.

doi: 10.1103/PhysRevC.26.965
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1304.

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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1981KO08      Phys.Rev. C23, 1571 (1981)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, E.K.Warburton

Electromagnetic Transitions in 14C and 14N

NUCLEAR REACTIONS 7Li(9Be, pn), E=5.5 MeV; 9Be(7Li, pn), (7Li, 2n), E=3.8-7.8 MeV; measured Eγ, Iγ, recoil. 14C, 14N levels deduced T1/2. Shell model, SU(3) basis.

NUCLEAR STRUCTURE 14C, 14N; calculated levels, B(λ), δ, Γγ, T1/2, γ-branching. Shell model, SU(3) basis.

doi: 10.1103/PhysRevC.23.1571
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1370.

1981MA12      Phys.Rev. C23, 2435 (1981)

J.F.Mateja, L.R.Medsker, C.P.Browne, J.D.Zumbro, H.T.Fortune, R.Middleton, J.B.McGrory

(t, p) Studies of 52Ti, 53V, and 57Mn and Tests of Mixed-Configuration Shell-Model Calculations

NUCLEAR REACTIONS 50Ti, 51V(t, p), E=15 MeV; measured σ(θ, Ep). 52Ti, 53V levels deduced L, J, π, enhancement factors. 55Mn(t, p), E not given; analyzed data. 57Mn levels deduced L, J, π, enhancement factors. Mixed-configuration shell model, DWBA analysis.

doi: 10.1103/PhysRevC.23.2435
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0023.

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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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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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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1978MA21      Phys.Rev. C17, 2047 (1978)

J.F.Mateja, L.R.Medsker, H.T.Fortune, R.Middleton, G.E.Moore, M.E.Cobern, S.Mordechai, J.D.Zumbro, C.P.Browne

76Ge(t, p)78Ge Reaction

NUCLEAR REACTIONS 76Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). 78Ge deduced levels, L, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.17.2047
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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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1978TA18      Phys.Rev. C18, 2190 (1978)

N.B.J.Tannous, J.F.Mateja, D.C.Wilson, L.R.Medsker, R.H.Davis

59Co(16O, 16O)59Co Elastic Scattering

NUCLEAR REACTIONS 59Co(16O, 16O), E=36, 40, 45.5, 49, 52, 56 MeV; measured σ(E, θ). Optical model analysis.

doi: 10.1103/PhysRevC.18.2190
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1977MA12      Phys.Rev. C15, 1708 (1977)

J.F.Mateja, C.P.Browne, C.E.Moss, J.B.McGrory

Level Structure of 57Mn from a 55Mn(t, p)57Mn Reaction Study and a Mixed-Configuration Shell Model Calculation

NUCLEAR REACTIONS 55Mn(t, p), E=17.0 MeV; measured σ(Ep, θ); deduced Q. 57Mn deduced levels, J, π, L, enhancement factors.

doi: 10.1103/PhysRevC.15.1708
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1977WI08      Phys.Rev. C16, 2070 (1977)

D.C.Wilson, L.R.Medsker, L.A.Parks, J.F.Mateja, L.H.Fry, Jr., J.D.Fox

Low-Lying Levls in 81Kr

NUCLEAR REACTIONS 81Br(p, nγ), E=5 MeV; measured Eγ, Iγ, γγ-coin. 81Kr deduced levels, J, π. Enriched target.

doi: 10.1103/PhysRevC.16.2070
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1976MA03      Phys.Rev. C13, 118 (1976)

J.F.Mateja, G.F.Neal, J.D.Goss, P.R.Chagnon, C.P.Browne

Low-Lying Levels of 57Mn from the 54Cr(α, p) Reaction

NUCLEAR REACTIONS 54Cr(α, p), E=15-24 MeV; measured σ(E, Ep, θ); deduced Q. 54Cr(α, pγ), E=11-11.5 MeV; measured pγ(θ), pγ-coin. 57Mn deduced levels, J, δ, γ-branching.

doi: 10.1103/PhysRevC.13.118
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1976MA24      Phys.Rev. C13, 2269 (1976)

J.F.Mateja, J.A.Bieszk, J.T.Meek, J.D.Goss, A.A.Rollefson, P.L.Jolivette, C.P.Browne

Energy Levels of 57, 59, 61Co Using the 60, 62, 64Ni(p, α) Reaction and Level Densities of Cobalt Isotopes

NUCLEAR REACTIONS 60,62,64Ni(p, α), E=13-16 MeV; measured σ(E, Eα, θ). 57,59,61Co deduced levels, J, level densities. Enriched targets.

doi: 10.1103/PhysRevC.13.2269
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1975CO09      Phys.Rev. C11, 1925 (1975)

W.K.Collins, D.S.Longo, J.F.Mateja, P.R.Chagnon, E.D.Berners, G.F.Neal, C.P.Browne, P.L.Jolivette, A.A.Rollefson, J.D.Goss

Levels of 38K: The 40Ca(d, α), 40Ca(d, αγ), and 36Ar(3He, πγ) Reactions

NUCLEAR REACTIONS 40Ca(d, αγ), E=7.84-16.0 MeV; measured Eγ, Eα, αγ-coin, αγ(θ), DSA. 36Ar(3He, pγ), E=8.34 MeV; measured Eγ, pγ-coin, pγ(θ). 38K deduced levels, J, π, T, T1/2, γ-mixing, γ-branching.

doi: 10.1103/PhysRevC.11.1925
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