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NSR database version of April 29, 2024.

Search: Author = R.M.Wheeler

Found 12 matches.

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1993SU29      Nucl.Instrum.Methods Phys.Res. B79, 186 (1993)

H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, F.D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

M-Shell X-Ray Production Cross Sections of Rare-Earth Elements by 4He2+ Impact in the Energy Range 0.7-7.0 MeV

NUCLEAR REACTIONS 139La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

ATOMIC PHYSICS 139La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

doi: 10.1016/0168-583X(93)95321-U
Citations: PlumX Metrics


1993SU30      Nucl.Instrum.Methods Phys.Res. B79, 194 (1993)

H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

M-Shell Ionization of Rare Earth Elements by Proton Impact in the Energy Range 0.6-4.6 MeV

NUCLEAR REACTIONS La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

ATOMIC PHYSICS La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

doi: 10.1016/0168-583X(93)95323-W
Citations: PlumX Metrics


1991MA66      Nucl.Instrum.Methods Phys.Res. B56/57, 33 (1991)

D.K.Marble, F.D.McDaniel, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.K.Wilson, D.L.Weathers, J.L.Duggan, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki, V.Zoran

Direct Ionization in K-Shell X-Ray Production in Fluorine by Highly-Charged Lithium, Boron, and Oxygen Ions

NUCLEAR REACTIONS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.

ATOMIC PHYSICS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.

doi: 10.1016/0168-583X(91)95964-F
Citations: PlumX Metrics


1991MC02      Nucl.Instrum.Methods Phys.Res. B54, 531 (1991)

F.D.McDaniel, D.K.Marble, J.L.Duggan, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.L.Weathers, P.S.Elliott, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

X-Ray Production in Fluorine by Highly Charged Boron, Carbon, and Oxygen Ions

NUCLEAR REACTIONS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.

ATOMIC PHYSICS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.

doi: 10.1016/0168-583X(91)95433-E
Citations: PlumX Metrics


1975CH25      Phys.Rev. A12, 52 (1975)

R.P.Chaturvedi, R.M.Wheeler, R.B.Liebert, D.J.Miljanic, T.Zabel, G.C.Phillips

L-Shell X-Ray Production Cross Sections of Pd, Ag, and Sn for Incident Proton Energies in the Range 3-12 MeV and Oxygen Ions in the Range 15-40 MeV

NUCLEAR REACTIONS Pd, Ag, Sn(p, p), E=3-12 MeV; Pd, Ag, Sn(16O, 16O), E=15-40 MeV; measured absolute L-shell X-ray σ.

doi: 10.1103/PhysRevA.12.52
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1974GA20      Phys.Rev. C9, 2399 (1974)

D.A.Garber, M.Behar, W.C.King, Z.W.Grabowski, R.P.Scharenberg, P.Sioshansi, R.M.Wheeler

Nuclear g Factors of First 2+ States in Even Tungsten Nuclei Determined by Recoil Implantation into Nickel and Cobalt, and the Hyperfine Field on Tungsten Nuclei in Nickel and Cobalt

NUCLEAR REACTIONS 182,184,186W(16O, 16O'γ), E=36 MeV; measured 16Oγ(θ, H), deduced Hhf for CoW, NiW. 182,184,186W levels deduced g.

doi: 10.1103/PhysRevC.9.2399
Citations: PlumX Metrics


1974VA16      Lett.Nuovo Cim. 10, 461 (1974)

V.Valkovic, R.B.Liebert, R.Plasek, R.M.Wheeler, T.Zabel, G.C.Phillips

Neutron-Proton Coincidences from the 12C(16O, np)26Al Reaction

NUCLEAR REACTIONS 12C(16O, np), E=30, 36 MeV; measured np-coin, deduced missing mass spectrum. 26Al deduced levels.


1973KR25      Nucl.Data Tables 11, 351 (1973)

K.S.Krane, R.M.Steffen, R.M.Wheeler

Directional correlations of gamma radiations emitted from nuclear states oriented by nuclear reactions or cryogenic methods

doi: 10.1016/S0092-640X(73)80016-6
Citations: PlumX Metrics


1972SI03      Phys.Lett. 39B, 343 (1972)

P.Sioshansi, D.A.Garber, W.C.King, R.P.Scharenberg, R.M.Steffen, R.M.Wheeler

Comparison of Impact and Radioactivity Techniques and the Magnetic Dipole Moments of the First 2+ States in 188Os, 190Os, and 192Os

NUCLEAR REACTIONS Os(16O, 16O'γ), E=36 MeV; measured (16O')(γ)(θ, H) in Fe, Ni; deduced internal magnetic fields. 188,190,192Os levels deduced g.

doi: 10.1016/0370-2693(72)90134-7
Citations: PlumX Metrics


1972SI43      Phys.Rev. C6, 2245 (1972)

P.Sioshansi, D.A.Garber, Z.W.Grabowski, R.P.Scharenberg, R.M.Steffen, R.M.Wheeler

Magnetic Dipole Moments of First 2+ States in Even Osmium Nuclei Recoil-Implanted in Nickel

NUCLEAR REACTIONS 186,188,190,192Os(16O, 16O'γ), E=36 MeV; measured σ(E(16O'), Eγ, θ(γ)) in Ni; deduced omegatau. 186,188,190,192Os levels deduced g.

doi: 10.1103/PhysRevC.6.2245
Citations: PlumX Metrics


1970WH02      Phys.Lett. 31B, 206 (1970)

R.M.Wheeler, U.Atzmony, K.A.Hardy, J.C.Walker

Isomer Shift in the 82 keV Transition of 154Sm

NUCLEAR REACTIONS 154Sm(γ, γ), E=82 keV; measured Mossbauer effect; deduced isomer shift.

doi: 10.1016/0370-2693(70)90105-X
Citations: PlumX Metrics


1969WH04      Phys.Rev. 186, 1280 (1969)

R.M.Wheeler, U.Atzmony, J.C.Walker

Magnetic Dipole and Electric Quadrupole Moments of the First 2+ State Of Sm154

NUCLEAR REACTIONS 154Sm(γ, γ), E = 82 keV; measured Mossbauer effect. 154Sm level deduced μ, quadrupole moment.

doi: 10.1103/PhysRev.186.1280
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