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NSR database version of April 11, 2024.

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 T1/2, B(E2). Comparison with previous results.

doi: 10.1103/PhysRevC.68.044309
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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
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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
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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, T1/2. 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, T1/2, 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, T1/2 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 T1/2.

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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2623.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2621.


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 T1/2 (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 233,235,236,238U, 237Np, 239Pu(α, 2n), E=26.1 MeV; measured α. 235,237,238,240Pu, 239Am, 241Cm deduced T1/2 (SF-isomer). 239Pu(3He, 2np), E=30 MeV; measured σ. 239Am deduced T1/2(SF-isomer). 236U(α, n), E=26 MeV; measured σ. 239Pu deduced T1/2(SF-isomer). 237Np(3He, p)(3He, np), (3He, 2np), E=26, 30 MeV; measured σ. 237,238,239Pu deduced T1/2 (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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2055.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0357.


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetP0028.


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)C12* 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'γ4.43)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

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12209.


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
Citations: PlumX Metrics


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