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Search: Author = J.D.Fox

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2003RI08      Phys.Rev. C 68, 044309 (2003)

L.A.Riley, P.D.Cottle, M.Brown-Hayes, W.T.Cluff, J.D.Fox, N.Keeley, F.W.Letson, R.A.Kaye, K.W.Kemper, M.T.McEllistrem, S.L.Tabor, J.M.Thompson, D.Walker

Lifetime of the 2⁺₁ state and densities for the 0⁺_g.s → 2⁺₁ transition in ¹⁸Ne

NUCLEAR REACTIONS ³He(¹⁶O, n), E=38 MeV; measured Eγ, Iγ, (neutron)γ-coin, DSA. ¹⁸Ne deduced level T_1/2, B(E2). Comparison with previous results.

doi: 10.1103/PhysRevC.68.044309
Citations: PlumX Metrics

2000GR21      Nucl.Instrum.Methods Phys.Res. A450, 12 (2000)

C.J.Gross, T.N.Ginter, D.Shapira, W.T.Milner, J.W.McConnell, A.N.James, J.W.Johnson, J.Mas, P.F.Mantica, R.L.Auble, J.J.Das, J.L.Blankenship, J.H.Hamilton, R.L.Robinson, Y.A.Akovali, C.Baktash, J.C.Batchelder, C.R.Bingham, M.J.Brinkman, H.K.Carter, R.A.Cunningham, T.Davinson, J.D.Fox, A.Galindo-Uribarri, R.Grzywacz, J.F.Liang, B.D.MacDonald, J.MacKenzie, S.D.Paul, A.Piechaczek, D.C.Radford, A.V.Ramayya, W.Reviol, D.Rudolph, K.Rykaczewski, K.S.Toth, W.Weintraub, C.Williams, P.J.Woods, C.-H.Yu, E.F.Zganjar

Performance of the Recoil Mass Spectrometer and Its Detector Systems at the Holifield Radioactive Ion Beam Facility

doi: 10.1016/S0168-9002(00)00159-5
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1999AH07      Phys.Rev. C60, 064601 (1999)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, C.M.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, Th.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.M.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.R.Young, J.E.Yurkon

Positron-Electron Pairs Produced in Heavy-Ion Collisions

NUCLEAR REACTIONS ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; ¹⁸¹Ta(²³⁸U, X), E=5.95, 6.1, 6.3 MeV/nucleon; measured positron, electron spectra, multiplicities, e^-e⁺-coin, angular correlation; deduced no sharp structure in sum-energy spectra. APEX spectrometer.

doi: 10.1103/PhysRevC.60.064601
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1999RE02      Phys.Rev.Lett. 82, 509 (1999)

P.Reiter, T.L.Khoo, C.J.Lister, D.Seweryniak, I.Ahmad, M.Alcorta, M.P.Carpenter, J.A.Cizewski, C.N.Davids, G.Gervais, J.P.Greene, W.F.Henning, R.V.F.Janssens, T.Lauritsen, S.Siem, A.A.Sonzogni, D.Sullivan, J.Uusitalo, I.Wiedenhover, N.Amzal, P.A.Butler, A.J.Chewter, K.Y.Ding, N.Fotiades, J.D.Fox, P.T.Greenlees, R.-D.Herzberg, G.D.Jones, W.Korten, M.Leino, K.Vetter

Ground-State Band and Deformation of the Z = 102 Isotope ²⁵⁴No

NUCLEAR REACTIONS ²⁰⁸Pb(⁴⁸Ca, 2n), E=215 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. ²⁵⁴No deduced levels, J, π, rotational band, deformation. Gammasphere array, recoil-decay tagging.

doi: 10.1103/PhysRevLett.82.509
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1997AH01      Phys.Rev.Lett. 78, 618 (1997)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.R.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Search for Monoenergetic Positron Emission from Heavy-Ion Collisions at Coulomb-Barrier Energies

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.95-6.3 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; measured positron energy spectra; deduced no structure.

doi: 10.1103/PhysRevLett.78.618
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1997AH04      Phys.Rev. C55, R2755 (1997)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.A.Chishti, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, J.S.Greenberg, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Internal Pair Conversion in Heavy Nuclei

NUCLEAR REACTIONS ²⁰⁶Pb(²⁰⁶Pb, X), E=5.90 MeV/nucleon; measured e⁺e^--sum energy spectra, Doppler corrected Eγ; deduced internal pair conversion to gamma branching ratio. ²³²Th(²⁰⁸Pb, X), E=5.80 MeV/nucleon; ²³⁸U(²⁰⁸Pb, X), E=5.80 MeV/nucleon; ¹⁸¹Ta(²³⁸U, X), E=5.95 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.90 MeV/nucleon; measured e⁺e^--sum energy, Doppler corrected Eγ; deduced no discrete lines evidence in e⁺e^- spectra. ²³⁸U deduced new levels evidence.

doi: 10.1103/PhysRevC.55.R2755
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1997AH05      Z.Phys. A358, 235 (1997)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.Young, J.E.Yurkon, and the APEX Collaboration

The Positron-Electron Peak Puzzle: Results from APEX

NUCLEAR REACTIONS ²³²Th(²³⁸U, X), E=5.78-5.95 MeV/nucleon; ¹⁸¹Ta(²³⁸U, X), E=5.79-6.3 MeV/nucleon; measured total (e⁺)(heavy-ion)-, (e⁺e^-)(heavy-ion)-coin events number; deduced very low light neutral particle production upper limits.

doi: 10.1007/s002180050316
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1996AH05      Acta Phys.Pol. B27, 387 (1996)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.Gazes, A.L.Hallin, T.Happ, N.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, A.Young, J.E.Yurkon, and the APEX Collaboration

The Positron Peak Puzzle - Recent Results from APEX

NUCLEAR REACTIONS ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; ¹⁸¹Ta(²³⁸U, X), E=5.96-6.3 MeV/nucleon; ²⁰⁶Pb(²⁰⁶Pb, X), E not given; analyzed e⁺e^--sum energy spectra. ²³²Th, ²³⁸U(²⁰⁸Pb, X), E=5.8 MeV/nucleon; ²³²Th, ¹⁸¹Ta(²³⁸U, X), E=5.95 MeV/nucleon; ²⁰⁶Pb(²⁰⁶Pb, X), E=5.9 MeV/nucleon; analyzed Doppler reconstructed γ spectra; deduced limits on 1.78 MeV ²³⁸U transition possible contribution to (heavy ion)γ-coin.

1996AH07      Nucl.Instrum.Methods Phys.Res. A370, 539 (1996)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, J.P.Greene, A.L.Hallin, Th.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.M.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.R.Young, J.E.Yurkon

A Solenoidal Spectrometer for Positron-Electron Pairs Produced in Heavy-Ion Collisions

RADIOACTIVITY ⁸⁵Sr(EC); ¹¹³Sn(EC); ²⁰³Hg(β^-); measured electron spectra; deduced apparatus response, efficiency. New solenoidal spectrometer.

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=6.1 MeV/nucleon; measured γ-, positron energy spectra. New solenoidal spectrometer.

doi: 10.1016/0168-9002(95)00829-2
Citations: PlumX Metrics

1995AH01      Nucl.Phys. A583, 247c (1995)

I.Ahmad, S.M.Austin, B.B.Back, D.Bazin, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, J.S.Greenberg, A.L.Hallin, T.Happ, J.Last, N.Kaloskamis, E.Kashy, W.Kutschera, C.J.Lister, M.Liu, M.R.Maier, D.Mercer, A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon

Positron Production in Heavy Ion Collisions: Current status of the problem

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.9-6.3 MeV/nucleon; compiled, analyzed, reviewed electron, positron production data.

doi: 10.1016/0375-9474(94)00667-C
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1995AH06      Phys.Rev.Lett. 75, 2658 (1995)

I.Ahmad, S.M.Austin, B.B.Back, R.R.Betts, F.P.Calaprice, K.C.Chan, A.Chishti, P.Chowdhury, C.Conner, R.W.Dunford, J.D.Fox, S.J.Freedman, M.Freer, S.B.Gazes, A.L.Hallin, T.Happ, D.Henderson, N.I.Kaloskamis, E.Kashy, W.Kutschera, J.Last, C.J.Lister, M.Liu, M.R.Maier, D.J.Mercer, D.Mikolas, P.A.A.Perera, M.D.Rhein, D.E.Roa, J.P.Schiffer, T.A.Trainor, P.Wilt, J.S.Winfield, M.Wolanski, F.L.H.Wolfs, A.H.Wuosmaa, G.Xu, A.Young, J.E.Yurkon, and the APEX Collaboration

Search for Narrow Sum-Energy Lines in Electron-Positron Pair Emission from Heavy-Ion Collisions Near the Coulomb Barrier

NUCLEAR REACTIONS ¹⁸¹Ta(²³⁸U, X), E=5.95-6.3 MeV/nucleon; ²³²Th(²³⁸U, X), E=5.95 MeV/nucleon; measured pair emission sum spectra; deduced no sharp lines evidence, neutral particle isolated decay related features.

doi: 10.1103/PhysRevLett.75.2658
Citations: PlumX Metrics

1995FO09      Z.Phys. A351, 5 (1995)

J.D.Fox, K.W.Kemper, P.D.Cottle

Energy Spectrum of Anomalous Positrons

doi: 10.1007/BF01292777
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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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1989CO18      Phys.Rev. C40, 2028 (1989)

P.D.Cottle, S.M.Aziz, J.D.Fox, K.W.Kemper, S.L.Tabor

Negative-Parity Excitations in ¹⁴⁴Nd

NUCLEAR REACTIONS ¹³⁰Te(¹⁸O, 4n), E=70 MeV; measured γγ-coin, γ(θ). ¹⁴⁴Nd deduced levels, J, π.

doi: 10.1103/PhysRevC.40.2028
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1989DE36      Phys.Rev. C40, R1851 (1989)

M.R.Deakin, J.D.Fox, K.W.Kemper, E.G.Myers, W.N.Shelton, J.G.Skofronick

Search for Cold Fusion using X-Ray Detection

NUCLEAR REACTIONS ²H(d, X), E=low; measured X-ray spectra; deduced cold fusion rate upper limit.

doi: 10.1103/PhysRevC.40.R1851
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1989FO03      Phys.Rev. C39, 288 (1989)

J.D.Fox, K.W.Kemper, P.D.Cottle, R.A.Zingarelli

Search for Anomalous e⁺-e^- Annihilation from ¹⁴⁰Pr

RADIOACTIVITY ¹⁴⁰Pr(β⁺), (EC) [from ¹⁴⁰Nd-decay]; measured γ spectra following pair annihilation in medium; deduced implications for U+Th collision γ-pair.

doi: 10.1103/PhysRevC.39.288
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1986AB08      Nucl.Phys. A456, 457 (1986)

K.M.Abdo, M.A.Abdulmonem, J.D.Fox

Energy Dependence of the Elastic Scattering ⁴⁰Ca(³He, ³He) in the Energy Range 10.0 to 18.0 MeV

NUCLEAR REACTIONS ⁴⁰Ca(³He, ³He), E=18, 16, 14, 12, 10 MeV; measured σ(E, θ), σ(E); deduced optical-model parameters. Natural Ca target.

doi: 10.1016/0375-9474(86)90405-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1350.

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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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.

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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1981HA28      Phys.Rev. C24, 786 (1981)

D.Halderson, K.W.Kemper, J.D.Fox, R.O.Nelson, E.G.Bilpuch, C.R.Westerfeldt, G.E.Mitchell

Width of the 6^-, T = 1, E(x) = 14.36 MeV State in ²⁸Si and Its Relationship to Intermediate Energy Inelastic Scattering

NUCLEAR REACTIONS ²⁷Al(p, p'), E=2.7-3.06 MeV; measured σ(Ep, θ). ²⁸Si resonance deduced Γ. R-matrix analysis.

doi: 10.1103/PhysRevC.24.786
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1981HN04      Phys.Rev. C24, 1495 (1981)

V.Hnizdo, J.Szymakowski, K.W.Kemper, J.D.Fox

Folding-Model Description of Elastic and Inelastic Scattering of ⁹Be by ^40,44Ca and ³⁹K at 40 MeV

NUCLEAR REACTIONS ³⁹K, ^40,44Ca(⁹Be, ⁹Be), (⁹Be, ⁹Be'), E=40 MeV; measured σ(θ). ^40,44Ca, ³⁹K deduced deformation length. DWBA analysis, double folding model.

doi: 10.1103/PhysRevC.24.1495
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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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1979LU02      Phys.Rev. C19, 785 (1979)

A.H.Lumpkin, L.H.Harwood, J.D.Fox, K.W.Kemper

Enhancements in the p and d Exit Channels of ¹²C + ¹²C: E(c.m.) = 14.3 and 25.2 MeV

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E(cm)=14.3 MeV; measured Ep, Eγ, pγ-coin. ¹²C(¹²C, dγ), E(cm)=25.2 MeV; measured Ed, Eγ, dγ-coin. ^22,23Na deduced resonances, J, π.

doi: 10.1103/PhysRevC.19.785
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1978CL08      Phys.Rev. C18, 1262 (1978)

M.E.Clark, K.W.Kemper, J.D.Fox

Location of High Spin 4p-3h Strength in ¹⁷O

NUCLEAR REACTIONS ¹³C(⁶Li, d), (⁷Li, t), E=34, 36 MeV; measured σ(θ). ¹⁷O deduced levels, J, π.

doi: 10.1103/PhysRevC.18.1262
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1978HA39      Phys.Rev. C18, 2145 (1978)

L.H.Harwood, K.W.Kemper, J.D.Fox, A.H.Lumpkin

Cluster Nature and Parity of the 9.155 MeV State in ¹⁵N

NUCLEAR REACTIONS ¹²C(⁶Li, ³Heγ), E=34 MeV; ¹²C(⁷Li, αγ), E=28 MeV; measured σ, (particle)γ-coin. ¹⁵N 9.155-MeV level deduced π, T_1/2. Comparison with cluster, shell models.

doi: 10.1103/PhysRevC.18.2145
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1978LU01      Phys.Rev.Lett. 40, 104 (1978)

A.H.Lumpkin, G.R.Morgan, J.D.Fox, K.W.Kemper

Possible Identification of 10⁺ Levels in ²⁴Mg at E(X) ≥ 20 MeV

NUCLEAR REACTIONS ¹²C(¹⁶O, α), E=50-70 MeV; measured σ(E, Eα, Eγ). ²⁴Mg deduced levels, J, π.

doi: 10.1103/PhysRevLett.40.104
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1978LU02      Phys.Rev. C17, 376 (1978)

A.H.Lumpkin, L.H.Harwood, L.A.Parks, J.D.Fox

Assignment of a Heavy-Ion Produced High-Spin Cascade to a Rh Isotope

NUCLEAR REACTIONS ⁹⁰Zr(¹²C, X), E=56 MeV; ⁹¹Zr(¹¹B, X), E=40 MeV; measured Eγ, particle γ-coin. ⁹⁹Pd, ⁹⁹Rh, ^99,98,97,96Ru, ⁹⁸Rh, ³⁸Ar, ¹⁹⁷Au deduced transitions.

doi: 10.1103/PhysRevC.17.376
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1977KE05      Phys.Rev. C15, 664 (1977)

G.J.KeKelis, A.H.Lumpkin, K.W.Kemper, J.D.Fox

Spectroscopy of High Spin States in ²³Na Using the ¹²C(¹²C, pγ)²³Na Reaction

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E=38.82 MeV; measured pγ(θ, t). ²³Na levels deduced J, π, T_1/2, γ-branching, δ, B(λ).

doi: 10.1103/PhysRevC.15.664
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1977LU02      Phys.Rev. C15, 1152 (1977)

A.H.Lumpkin, G.J.KeKelis, K.W.Kemper, J.D.Fox

Jπ of the E(x) = 4.52 MeV State in ²²Na via the ¹²C(¹²C, dγ)²²Na Reaction

NUCLEAR REACTIONS ¹²C(¹²C, dγ), E=38.82 MeV; measured DSA, dγ-coin, dγ(θ). ²²Na level deduced J, π, T_1/2 limit.

doi: 10.1103/PhysRevC.15.1152
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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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1976FL05      Phys.Rev. C13, 1173 (1976)

N.R.Fletcher, J.D.Fox, G.J.Kekelis, G.R.Morgan, G.A.Norton

Resonant Structures in the ¹²C(¹²C, ⁸Be)¹⁶O Reaction, E(c.m.) = 9 to 20 MeV

NUCLEAR REACTIONS ¹²C(¹²C, ⁸Be), E(cm)=9-20 MeV; measured σ(E, θ); deduced anomalies. ¹⁶O resonances deduced L.

doi: 10.1103/PhysRevC.13.1173
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1976FO08      Phys.Rev.Lett. 37, 629 (1976)

J.D.Fox, W.J.Courtney, K.W.Kemper, A.H.Lumpkin, N.R.Fletcher, L.R.Medsker

Comment on Evidence for Primordial Superheavy Elements

NUCLEAR REACTIONS ¹⁴⁰Ce(p, nγ), E=5.7 MeV; measured Eγ, E(X-ray). ¹⁴⁰Pr deduced transition which could interfere with observation of X-rays from superheavy element Z=126.

doi: 10.1103/PhysRevLett.37.629
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1976GU04      Phys.Rev. C13, 595 (1976)

G.D.Gunn, J.D.Fox, G.J.KeKelis

Levels of ⁵³Mn with the ⁵²Cr(³He, d)⁵³Mn and ⁵²Cr(⁷Li, ⁶He)⁵³Mn Reactions

NUCLEAR REACTIONS ⁵²Cr(³He, d), E=24 MeV; ⁵²Cr(⁷Li, ⁶He), E=34 MeV; measured σ(θ). ⁵³Mn levels deduced L, J, π, S.

doi: 10.1103/PhysRevC.13.595
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1975KE07      Phys.Rev.Lett. 35, 710 (1975)

G.J.KeKelis, A.H.Lumpkin, J.D.Fox

Gamma Decay of the 9.042- and 9.805-MeV States in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E=38.82 MeV; measured pγ(θ). ²³Na levels deduced J, π, γ-branching, δ.

doi: 10.1103/PhysRevLett.35.710
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1974CO33      Phys.Rev. C10, 1922 (1974)

W.J.Courtney, C.I.Delaune, J.W.Nelson, J.D.Fox

Half-Life of the 257 keV 1⁺ → 4^- Transition in ⁹⁰Nb

NUCLEAR REACTIONS ⁹⁰Zr(p, n), E=8 MeV; measured ce(t). ⁹⁰Nb level deduced T_1/2.

doi: 10.1103/PhysRevC.10.1922
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1974GU18      Nucl.Phys. A232, 176 (1974)

G.D.Gunn, K.W.Kemper, J.D.Fox

Study of Structure in the ²⁸Si(p, n)²⁸P and ²⁸Si(p, α)²⁵Al Excitation Functions

NUCLEAR REACTIONS ²⁸Si(p, n), E=15.8-18.2 MeV; measured σ(E). ²⁸Si(p, α), E=16.0-18.2 MeV; measured σ(E, Eα, θ). ²⁹P resonances deduced n-width, α-width.

doi: 10.1016/0375-9474(74)90651-4
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1974KE16      Phys.Rev. C10, 2613 (1974)

G.KeKelis, J.D.Fox

Study of the Reaction ¹²C(¹²C, d)²²Na

NUCLEAR REACTIONS ¹²C(¹²C, d), (¹²C, p), E=37-44 MeV; measured σ(E, Ed), σ(E, Ep), dγ-, pγ-coin. ^22,23Na deduced resonances.

doi: 10.1103/PhysRevC.10.2613
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1974RO34      Phys.Rev.Lett. 33, 1181 (1974)

B.L.Roberts, C.R.Cox, M.Eckhause, J.R.Kane, R.E.Welsh, D.A.Jenkins, W.C.Lam, P.D.Barnes, R.A.Eisenstein, J.Miller, R.B.Sutton, A.R.Kunselman, R.J.Powers, J.D.Fox

New Value for the Magnetic Moment of the Antiproton

NUCLEAR MOMENTS ¹H; measured antiproton μ.

doi: 10.1103/PhysRevLett.33.1181
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1973OL04      Phys.Rev. C8, 2144 (1973)

D.W.Oliver, K.W.Kemper, J.D.Fox

²⁴Mg(α, d)²⁶Al Reaction at 25 and 50 MeV

NUCLEAR REACTIONS ²⁴Mg(α, d), E=24.0-25.0, 50 MeV; measured σ(Ed, θ). ²⁴Mg(α, α), (α, α'), E=22.0-25.4 MeV; measured σ(E, θ). ²⁶Al deduced levels, J, π.

doi: 10.1103/PhysRevC.8.2144
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1972KE05      Phys.Rev. C5, 1257 (1972)

K.W.Kemper, J.D.Fox, D.W.Oliver

Search for Nondirect Effects in the ²⁸Si(p, p₀, ₁, ₂)²⁸Si Excitation Function from 16-18.2 MeV

NUCLEAR REACTIONS ²⁸Si(p, p), (p, p'), E=16-18.2 MeV; measured σ(E). ²⁸Si deduced deformation parameters β(L).

doi: 10.1103/PhysRevC.5.1257
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1972KE31      Nucl.Instrum.Methods 105, 333 (1972)

K.W.Kemper, J.D.Fox

Comparative Pulse-Height Anomaly for Protons and Alpha-Particles in Silicon Surface Barrier Detectors

doi: 10.1016/0029-554X(72)90579-4
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1972MC02      Phys.Rev. C5, 145 (1972)

C.M.McKenna, K.W.Kemper, J.D.Fox, J.W.Nelson, J.B.Ball

Levels of ⁵⁰Mn from the Reaction ⁵⁰Cr(³He, t)⁵⁰Mn

NUCLEAR REACTIONS ⁵⁰Cr(³He, t), E=39.45 MeV; measured σ(Et, θ). ⁵⁰Mn deduced levels, J, π.

doi: 10.1103/PhysRevC.5.145
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1972SH04      Nucl.Phys. A183, 21 (1972)

R.Shoup, J.D.Fox, R.A.Brown, G.Vourvopoulos, S.Maripuu

Study of the Electromagnetic Transitions in the ⁵⁵Co Nucleus

NUCLEAR REACTIONS ⁵⁴Fe(³He, dγ), E=18 MeV; measured σ(Ed, Eγ), Iγ. ⁵⁵Co deduced γ-branching, J, π. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(72)90928-1
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1971RI11      Nucl.Phys. A174, 273 (1971)

P.Richard, C.F.Moore, J.D.Fox

Fine Structure in Isobaric Analogue Resonances

NUCLEAR REACTIONS ⁹⁰Zr(p, p), ⁹²Mo(p, p), E=5.1-6.1 MeV; measured σ(E). ⁹¹Nb, ⁹³Tc deduced isobaric analog resonances, level-width.

doi: 10.1016/0375-9474(71)90662-2
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1970RE05      Nucl.Phys. A147, 183 (1970)

R.Repnow, V.Metag, J.D.Fox, P.von Brentano

Evidence for a Direct Reaction Mechanism in the Production of Fission Isomers

NUCLEAR REACTIONS ²³⁵U(d, p), E=13-20 MeV; measured σ delayed fission. Enriched target. ²³⁶U(d, pn), E=11-20 MeV; measured σ delayed fission. Enriched target. ²³⁸U(d, pn), E=11-20 MeV; measured σ delayed fission. Natural target. ²³³U(d, X), ²³⁶U(p, X), E = 14, 20 MeV; E upper limits σ delayed fission. Enriched targets. ²³⁸U(p, X), E=14-20 MeV; measured upper limits σ delayed fission. Natural target.

RADIOACTIVITY, Fission ^236,238U deduced T_1/2 (SF-isomer). ^234,237U deduced no SF-isomer.

doi: 10.1016/0375-9474(70)90520-8
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1969ME11      Z.Physik 226, 1 (1969)

V.Metag, R.Repnow, P.Von Brentano, J.D.Fox

Fission Isomerism Induced by Helium Ions

NUCLEAR REACTIONS ^{233,235,236,238}U, ²³⁷Np, ²³⁹Pu(α, 2n), E=26.1 MeV; measured α. ^{235,237,238,240}Pu, ²³⁹Am, ²⁴¹Cm deduced T_1/2 (SF-isomer). ²³⁹Pu(³He, 2np), E=30 MeV; measured σ. ²³⁹Am deduced T_1/2(SF-isomer). ²³⁶U(α, n), E=26 MeV; measured σ. ²³⁹Pu deduced T_1/2(SF-isomer). ²³⁷Np(³He, p)(³He, np), (³He, 2np), E=26, 30 MeV; measured σ. ^237,238,239Pu deduced T_1/2 (SF-isomer).

doi: 10.1007/BF01392778
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1969SH14      Nucl.Phys. A135, 689 (1969)

R.Shoup, J.D.Fox, G.Vourvopoulos

Proton Particle-Hole States in ¹¹⁶Sn from the ¹¹⁵In(³He, d)¹¹⁶Sn Reaction

NUCLEAR REACTIONS ¹¹⁵In(³He, d), E = 25.3 MeV; measured σ(Ed, θ). ¹¹⁶Sn deduced levels, L(p), S. Natural target.

doi: 10.1016/0375-9474(69)90013-X
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1969VO03      Phys.Rev. 177, 1558(1969)

G.Vourvopoulos, J.D.Fox

Experimental Study of the T=T(Z) States in ⁹⁰Zr via a (³He, d) Reaction

NUCLEAR REACTIONS ⁸⁹Y(³He, d), E=25 MeV; measured σ(Ed, θ). ⁹⁰Zr deduced levels, L(p), S, isobaric analog.

doi: 10.1103/PhysRev.177.1558
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1969VO04      Phys.Rev. 177, 1789(1969)

G.Vourvopoulos, J.D.Fox, B.Rosner

Analysis of the T < States in ⁵⁵Co

NUCLEAR REACTIONS ⁵⁴Fe(³He, d), E=16.5 MeV; ⁵⁵Co deduced levels, J, π, L(p), isobaric analog. Reanalysis of previous data.

doi: 10.1103/PhysRev.177.1789
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1968LO04      Phys.Rev. 167, 1131 (1968)

D.D.Long, J.D.Fox

Isobaric Analog States in Heavy Nuclei. V. Resonances in Zr⁹⁰ from Proton Inelastic Scattering

NUCLEAR STRUCTURE ⁹⁰Zr, ⁸⁹Y; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.167.1131
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1967VO06      Phys.Letters 25B, 543 (1967)

G.Vourvopoulos, J.D.Fox

Identification of the T < Component for Single-Proton Single-Proton Hole States in ⁹⁰Zr

NUCLEAR STRUCTURE ⁹⁰Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90140-2
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1966LO09      Phys.Rev. 149, 906 (1966)

D.D.Long, P.Richard, C.F.Moore, J.D.Fox

Coulomb Displacement Energies from Isobaric Analogue Resonances

doi: 10.1103/PhysRev.149.906
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1966MO06      Phys.Rev. 141, 1166 (1966)

C.F.Moore, P.Richard, C.E.Watson, D.Robson, J.D.Fox

Isobaric Analogue States in Heavy Nuclei. I. Molybdenum Isotopes

NUCLEAR STRUCTURE ⁹³Tc, ¹⁰¹Tc, ⁹⁵Tc, ⁹⁶Tc, ⁹⁷Tc, ⁹⁸Tc, ⁹⁹Tc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.141.1166
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1966RI06      Phys.Rev. 145, 971 (1966)

P.Richard, C.F.Moore, J.A.Becker, J.D.Fox

Isobaric Analogue States in Heavy Nuclei. III. Tin Isotopes

NUCLEAR STRUCTURE ¹¹⁷Sb, ¹¹³Sb, ¹¹⁵Sb, ¹¹⁹Sb, ¹¹⁸Sb, ¹²³Sb, ¹²¹Sb, ¹²⁰Sb, ¹²⁵Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.145.971
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1966VO02      Phys.Rev. 141, 1180 (1966)

G.Vourvopoulos, J.D.Fox

Isobaric Analogue States in Heavy Nuclei. II. Resonances in Ga⁶⁹

NUCLEAR STRUCTURE ⁶⁹Ga; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.141.1180
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1965FO03      Bull.Am.Phys.Soc. 10, No.1, 52, DC9 (1965)

J.D.Fox, C.F.Moore, D.Robson

Nuclear Reactions Through Isobaric Analog Resonances in Zr⁹⁰

NUCLEAR STRUCTURE ⁹⁰Zr; measured not abstracted; deduced nuclear properties.

1965MO02      Bull.Am.Phys.Soc. 10, No.1, 52, DC10 (1965)

C.F.Moore, C.E.Watson, P.Richard, D.Robson, J.D.Fox

Analog Comparisons in Reactions on the Molybdenum Isotopes

NUCLEAR STRUCTURE Mo; measured not abstracted; deduced nuclear properties.

1965RI01      Bull.Am.Phys.Soc. 10, No.1, 52, DC11 (1965)

P.Richard, D.Robson, J.D.Fox

Fine Structure in Isobaric Analog of Mo⁹³ and Zr⁹¹

NUCLEAR STRUCTURE ⁹¹Nb, ⁹¹Mo, ⁹³Tc; measured not abstracted; deduced nuclear properties.

1965RO23      Phys.Lett. 18, 86 (1965)

D.Robson, J.D.Fox, P.Richard, C.F.Moore

Reactions Involving Simple Isobaric Analogue Resonances

NUCLEAR REACTIONS ⁹²Zr(p, p), E(cm) ≈ 5.8-6.2 MeV; measured σ(E). ⁹²Zr(p, n), E ≈ 5.7-6.3 MeV; analyzed data. ⁹³Zr deduced resonance, Γp, Γ₀.

doi: 10.1016/0031-9163(65)90039-9
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1964BE05      Bull. Am. Phys. Soc. 9, No. 1, 107, KC6 (1964)

J.A.Becker, V.Nealy, C.F.Moore, D.Robson, J.D.Fox

Direct Excitation of Isobaric Analog States in the Isotopes of Antimony

NUCLEAR STRUCTURE ¹¹⁹Sn, ¹¹⁸Sn, ¹¹⁷Sn, ¹¹⁶Sn, ¹¹²Sn, ¹²⁰Sn, ¹²²Sn, ¹²⁴Sn; measured not abstracted; deduced nuclear properties.

1964FO03      Phys.Rev.Lett. 12, 198 (1964)

J.D.Fox, C.F.Moore, D.Robson

Excitation of Isobaric Analog States in ⁸⁹Y and ⁹⁰Zr

NUCLEAR STRUCTURE ⁹⁰Zr, ⁸⁹Y; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.12.198
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1964MO04      Bull.Am.Phys.Soc. 9, No.1, 106, KC3 (1964)

C.F.Moore, C.E.Watson, D.Robson, J.D.Fox

Experimental Studies of Analog States in Technetium

NUCLEAR STRUCTURE ⁹²Tc, ⁹³Tc, ⁹⁴Tc; measured not abstracted; deduced nuclear properties.

1964MO09      Bull.Am.Phys.Soc. 9, No.4, 483, JA5 (1964)

C.F.Moore, J.D.Fox

Excitation of Isobaric Analog-States in the Isotopes of Niobium

NUCLEAR STRUCTURE ⁹⁴Nb, ⁹⁶Nb, ⁹²Nb, ⁹⁰Nb, ⁹¹Nb; measured not abstracted; deduced nuclear properties.

1963BE18      Nucl.Phys. 42, 669 (1963)

J.A.Becker, J.D.Fox

Capture of Protons by B¹¹ in the Giant Resonance Region

NUCLEAR STRUCTURE ¹¹B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90769-7
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1963CH31      Phys.Rev. 131, 2149 (1963)

G.R.Choppin, J.R.Meriwether, J.D.Fox

Low-Energy Charged-Particle-Induce fission

NUCLEAR REACTIONS ²³²Th, ²³⁸U(p, F), (d, F), E<16 MeV; measured reaction products, Eγ, Iγ, Eβ, Iβ; deduced σ. Comparison with available data.

doi: 10.1103/PhysRev.131.2149
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1963FO04      Bull.Am.Phys.Soc. 8, No.4, 375, U5 (1963)

J.D.Fox, C.F.Moore, J.A.Becker, C.E.Watson

Proton Reactions in Y⁸⁹ Near Neutron Threshold

NUCLEAR STRUCTURE ⁸⁹Zr; measured not abstracted; deduced nuclear properties.

1963FO08      Conf.Compd.Nucl.States, Gatlinburg, Tenn., p.8, A11 (1963)

J.D.Fox, F.Robson, C.F.Moore, P.Richard

Prominent Compound Nuclear States in Zr⁹⁰ Near the Neutron Binding Energy

NUCLEAR STRUCTURE ⁸⁹Y, ⁹⁰Zr; measured not abstracted; deduced nuclear properties.

1963SN01      Priv.Comm. (October 1963)

S.G.Snow, J.D.Fox

Search for Excited States of C¹³ at 5.51 and 6.10 MeV

NUCLEAR STRUCTURE ¹³C; measured not abstracted; deduced nuclear properties.

1962BE10      Bull.Am.Phys.Soc. 7, No.8, 570, D8 (1962)

J.A.Becker, J.D.Fox

Giant Resonance in the B¹¹(p, γ₁)C^12* Reaction at 11.7 MeV

NUCLEAR STRUCTURE ¹¹B; measured not abstracted; deduced nuclear properties.

1962KA05      Phys.Rev. 125, 2037 (1962)

W.R.Kane, N.F.Fiebiger, J.D.Fox

Coincidence Studies of the Thermal Neutron Capture Gamma Rays of Chromium

NUCLEAR STRUCTURE ⁵¹Cr, ⁵³Cr, ⁵⁴Cr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.2037
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1961AD01      Bull.Am.Phys.Soc. 6, No.3, 250, GA14 (1961)

H.S.Adams, J.D.Fox, N.P.Heydenburg, G.M.Temmer

Studies of (p, α) Reactions up to 12 MeV

NUCLEAR STRUCTURE ²⁰Ne; measured not abstracted; deduced nuclear properties.

1961AD04      Phys.Rev. 124, 1899 (1961)

H.S.Adams, J.D.Fox, N.P.Heydenburg, G.M.Temmer

Angular Distributions of 4.43-MeV Gamma Radiation from C¹²(p, p'γ)C¹²

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.124.1899
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1961BE02      Bull.Am.Phys.Soc. 6, No.1, 47, Q5 (1961)

J.A.Becker, J.D.Fox

Determination of (p, n) Thresholds for Cr⁵²

NUCLEAR STRUCTURE ⁵²Cr; measured not abstracted; deduced nuclear properties.

1961ST17      Bull.Am.Phys.Soc. 6, No.6, 506, E6 (1961)

R.F.Sturgeon, Jr., J.A.Becker, J.D.Fox

Excitation Function of O¹⁶(p, p'γ) to 10.6 MeV

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.

1960AD04      Bull.Am.Phys.Soc. 5, No.6, 404, B4 (1960)

H.S.Adams, J.A.Becker, J.D.Fox, N.P.Heydenburg, G.M.Temmer

C¹²(p, p'γ_4.43)C¹² Excitation Function between 5 and 11 MeV

NUCLEAR STRUCTURE ¹³N; measured not abstracted; deduced nuclear properties.

1960AX01      NP-8479 (1960)

P.Axel, J.D.Fox

The Photoneutron Cross Section Near Threshold

NUCLEAR STRUCTURE ⁹⁰Zr, ⁹²Mo, ⁹¹Mo, ⁸⁹Zr, ⁷⁹Br, ⁸⁰Br, ⁸¹Br; measured not abstracted; deduced nuclear properties.

1960FO08      Thesis, University of Illinois (1960); Dissertation Abstr. 20, 4690 (1960); See Also 60Ax01

J.D.Fox

The Photoneutron Cross Section Near Threshold

NUCLEAR STRUCTURE ⁸¹Br, ⁷⁹Br, ⁹⁰Zr, ⁹²Mo; measured not abstracted; deduced nuclear properties.

1960NE10      Bull.Am.Phys.Soc. 5, No.6, 424, P7 (1960)

J.W.Nelson, H.S.Adams, R.H.Davis, J.D.Fox, N.P.Heydenburg, H.S.Plendl, R.K.Sheline, G.M.Temmer

(p, n) Thresholds in Ti⁴⁸, Fe⁵⁶, and Sr⁸⁸

NUCLEAR STRUCTURE ⁸⁸Y, ⁴⁸V, ⁵⁶Ni, ⁵⁶Co; measured not abstracted; deduced nuclear properties.

1959BR11      Bull.Am.Phys.Soc. 4, No.1, 34, M9 (1959)

M.K.Brussel, J.D.Fox

Capture γ Rays from Neutron Resonances

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1959FO46      Bull.Am.Phys.Soc. 4, No.4, 271, SA7 (1959)

J.D.Fox, M.K.Brussel, D.J.Hughes, R.E.Chrien

Interpretation of Resonance Capture Measurements

1959FO57      BNL-4334 (1959)

J.D.Fox, W.R.Kane, W.Kley

1959HU21      Phys.Rev.Letters 2, 505 (1959)

D.J.Hughes, M.K.Brussel, J.D.Fox, R.L.Zimmerman

Strengths of High-Energy Capture Gamma Rays in W¹⁸⁴

doi: 10.1103/PhysRevLett.2.505
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1958FO45      Bull.Am.Phys.Soc. 3, No.3, 176, F6 (1958)

J.D.Fox, M.K.Brussell, R.E.Chrien, R.L.Zimmerman, D.J.Hughes

Capture Gamma Rays in Individual Neutron Resonances

1958FO69      Phys.Rev. 110, 1472 (1958)

J.D.Fox, R.L.Zimmerman, D.J.Hughes, H.Palevsky, M.K.Brussel, R.E.Chrien

Measurement of Spins of Levels Excited by Slow Neutron Capture

doi: 10.1103/PhysRev.110.1472
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1955AX02      Phys.Rev. 97, 975 (1955)

P.Axel, J.D.Fox, R.H.Parker

Identification of Mo⁹¹ and Mo⁹¹m

doi: 10.1103/PhysRev.97.975
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