NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = R.Fink Found 151 matches. Showing 1 to 100. [Next]2008BA20 J.Phys.(London) B41, 125101 (2008) Z.Bao, R.F.Fink, O.Travnikova, D.Ceolin, S.Svensson, M.N.Piancastelli Detailed theoretical and experimental desription of normal Auger decay in O2 ATOMIC PHYSICS 16O; analyzed Auger electron spectrum of the O2 molecule.
doi: 10.1088/0953-4075/41/12/125101
1993KR25 Hyperfine Interactions 78, 261 (1993) G.Krausch, R.Fink, K.Jacobs, U.Kohl, J.Lohmuller, B.Luckscheiter, R.Platzer, B.-U.Runge, U.Wohrmann, G.Schatz Surface and Interface Studies with Perturbed Angular Correlations RADIOACTIVITY 111In(EC); compiled, reviewed γγ(θ, H) data; deduced 111In/111Cd field gradient distribution relative width on different substitutional step sites.
doi: 10.1007/BF00568148
1991GR12 Nucl.Phys. A530, 401 (1991) J.C.Griffin, R.A.Braga, R.W.Fink, J.L.Wood, H.K.Carter, R.L.Mlekodaj, C.R.Bingham, E.Coenen, M.Huyse, P.Van Duppen Decay of Mass-Separated 3.0 min 195gBi to Levels in 195Pb and Shape Coexistence in the Neutron-Deficient Odd-Mass Pb Isotopes RADIOACTIVITY 195Bi [from 181Ta(20Ne, 6n), E=190 MeV; 185Re(16O, 6n), E=140, 210 MeV]; measured Eγ, Iγ, I(ce), I(X-ray), γγ(t), (ce)γ(t), γ(X-ray)(t), e(X-ray)(t); deduced β+/EC, Q(EC). 195Pb deduced level, J, π, ICC, γ-multipolarity. 199Po [from 191Ir(14N, 6n), E=127 MeV]; measured Eγ, Iγ, Eα, Iα; deduced Qα, Γα. 195Pb deduced levels, J, π. Ge(Li), hyperpure Ge, Si(Li), Si(Au) detectors. Mass-separated sources.
doi: 10.1016/0375-9474(91)90810-S
1990KO25 Phys.Rev. C42, 1267 (1990) M.O.Kortelahti, B.D.Kern, R.A.Braga, R.W.Fink, I.C.Girit, R.L.Mlekodaj Transitional Nuclei in the Rare-Earth Region: Energy levels and structure of 130,132Ce, 132,134Nd, and 134Pm, via β decay of 130,132Pr, 132,134Pm, and 134Sm RADIOACTIVITY 130,132Pr, 132,134Pm, 134Sm [from 92Mo(46Ti, xnyp), 112Sn(28Si, xnyp), E=170-240 MeV]; measured Eγ, Iγ, γγ(t), T1/2. 130,132Ce, 132,134Nd, 134Pm deduced levels, B(E2) ratios. Interacting boson model calculations.
doi: 10.1103/PhysRevC.42.1267
1989KO07 Z.Phys. A332, 229 (1989) M.O.Kortelahti, H.K.Carter, R.A.Braga, R.W.Fink, B.D.Kern Non-Yrast Level Structure of 135Nd via Beta Decay of 135Pm RADIOACTIVITY 135Pm(β+), (EC) [from 92Mo(46Ti, X), E=240 MeV]; measured γγ-coin, I(ce). 135Nd deduced levels, possible J, π.
1988KE03 Z.Phys. A330, 37 (1988); Erratum Z.Phys. A341, 493 (1992) B.D.Kern, R.L.Mlekodaj, M.O.Kortelahti, R.A.Braga, R.W.Fink Energy Levels of 136Pm and 136Nd via Beta Decay of 136Sm and 136Pm RADIOACTIVITY 136Sm(β+), (EC), 136Pm(β+), (EC) [from 92Mo(48Ti, xnyp), 112Sn(28Si, xnyp)]; measured γγ-coin, γ yields. 136Sm deduced T1/2. 136Nd deduced levels, γ-branching. 136Pm deduced levels, γ-branching, tentative isomer J, π.
1988TA03 Phys.Scr. 37, 62 (1988) M.Tan, R.A.Braga, R.W.Fink, P.Venugopala Rao L2, 3 Subshell X-Ray Fluorescence Yields and Coster-Kronig Transition Probabilities of Nd and Yb RADIOACTIVITY 145Pm(α), (EC); 171Tm(β-); measured E(X-ray), I(X-ray), (X-ray)(X-ray)(t); deduced X-ray fluorescence yields, Coster-Kronig transition probabilities, decay branching ratios for Nd, Yb.
doi: 10.1088/0031-8949/37/1/009
1987KE05 Phys.Rev. C36, 1514 (1987) B.D.Kern, R.L.Mlekodaj, G.A.Leander, M.O.Kortelahti, E.F.Zganjar, R.A.Braga, R.W.Fink, C.P.Perez, W.Nazarewicz, P.B.Semmes Transition through Triaxial Shapes of the Light Samarium Isotopes and the Beta Decay of 136,138,140Eu NUCLEAR REACTIONS 92Mo(48Ti, xnp), E=220 MeV; 112Sn(28Si, xnp), E=170, 190 MeV; measured Eγ, Iγ, γγ-coin. Enriched targets, Ge detectors, magnetic isotope separator. RADIOACTIVITY 136,138,140Eu(β+), (EC) [from 92Mo(48Ti, pxn), E=220 MeV; 112Sn(28Si, xnp), E=170, 190 MeV]; measured Eγ, Iγ, γγ-coin. 136,138,140Sm deduced levels. Enriched targets, Ge detectors, magnetic isotope separator. NUCLEAR STRUCTURE 136,138,140Sm; calculated levels. Wood-Saxon Strutinsky, triaxial models, interacting boson approximation.
doi: 10.1103/PhysRevC.36.1514
1987KO24 Z.Phys. A327, 231 (1987) M.Kortelahti, E.F.Zganjar, R.L.Mlekodaj, B.D.Kern, R.A.Braga, R.W.Fink, C.P.Perez Beta-Decay of Light Rare-Earth 130,132Pr and 132,134Pm Nuclei RADIOACTIVITY 130,132Pr, 132,134Pm(β+), (EC) [from 112Sn(28Si, X), E=190, 220 MeV]; measured Eγ, Iγ, γγ-coin. 130,132Ce, 132,134Nd deduced levels, J, π.
1987SE02 Phys.Rev. C35, 749 (1987) P.B.Semmes, R.A.Braga, J.C.Griffin, R.W.Fink L2-L3 Coster-Kronig Transition Probability for Z = 54 RADIOACTIVITY 131Cs(EC); measured (K X-ray)(L X-ray)-coin; deduced L2-L3 Coster-Kronig transition probability. Ge, Si-Li detectors.
doi: 10.1103/PhysRevC.35.749
1987SE04 Nucl.Phys. A464, 381 (1987) P.B.Semmes, R.A.Braga, R.W.Fink, J.L.Wood, J.D.Cole Decay of Mass-Separated 7.4 Min 203At RADIOACTIVITY 203At(β-) [from Ir(16O, xn), E=125 MeV]; measured T1/2, Eγ, Iγ, I(ce), I X-ray, γγ(t), γ(ce)(t), (ce)(X-ray)(t); deduced I(β+)/I(EC), Q(EC). 203Po deduced levels, J, π, ICC, γ-multipolarity. Ge(Li), hyperpure Ge, Si-Li detectors, mass separated sources.
doi: 10.1016/0375-9474(87)90306-X
1986BR28 Nucl.Phys. A459, 359 (1986) R.A.Braga, P.B.Semmes, W.R.Western, R.W.Fink Decay of Mass-Separated 201mPo and 201gPo RADIOACTIVITY 201Po(EC), (β+), (α) [from 193Ir(14N, 6n), E=116 MeV]; 201Bi(EC), (β+), (α) [from 201Po decays]; measured T1/2, Eγ, Iγ, I(ce), γγ(t), γ(X-ray)(t). 201Bi deduced levels, J, π, ICC, γ-multipolarity. 201Po deduced (EC+β+)/IT branching ratio. Ge(Li), Si-Li detectors, mass separated sources.
doi: 10.1016/0375-9474(86)90139-9
1985LE10 Phys.Rev. C32, 277 (1985) R.S.Lee, J.H.Hamilton, A.V.Ramayya, A.P.de Lima, D.L.Sastry, K.S.R.Sastry, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.-D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, J.L.Weil, B.D.Kern, A.C.Xenoulis, R.W.Fink, Sun Xi-jun, Guo Jun-sheng, Cho Chi-cheng, Pan Zong-you, Guo Ying-xian Decay of 117Xe → 117I → 117Te NUCLEAR REACTIONS 107,109Ag(12C, xn), E=50-70 MeV; measured γ yields. 117I deduced transition. RADIOACTIVITY 117Xe(EC), (β+) [from 104Pd(16O, xn), E=86 MeV]; 117I(EC), (β+) [from 117Xe β-decay]; 117Te(β+), (EC) [from 117I β-decay]; measured Eγ, Iγ, E X-ray, I X-ray, T1/2, γγ-coin. 117I, 117Te deduced levels, relative Iγ. 117Sb(EC), (β+) [from 117Te decay]; measured T1/2. 117Xe, 117I deduced mass difference, Q(EC).
doi: 10.1103/PhysRevC.32.277
1984CO17 Phys.Rev. C30, 1267 (1984) J.D.Cole, J.H.Hamilton, A.V.Ramayya, W.Lourens, B.van Nooijen, H.Kawakami, L.A.Mink, E.H.Spejewski, H.K.Carter, R.L.Mlekodaj, G.A.Leander, L.L.Riedinger, C.R.Bingham, E.F.Zganjar, J.L.Wood, R.W.Fink, K.S.Toth, B.D.Kern, K.S.R.Sastry Decay of 188Tl and Observed Shape Coexistence in the Bands of 188Hg RADIOACTIVITY 188Tl(β+), (EC) [from 181Ta(16O, 9n), E=143-145 MeV; 180W(14N, 6n), E=184-188 MeV]; measured Eγ, Iγ, I(ce), γγ-, γ(ce)-coin. 188Tl levels deduced T1/2. 188Hg deduced levels, J, π, γ-branching, δ, ICC.
doi: 10.1103/PhysRevC.30.1267
1983BR26 Nucl.Phys. A410, 441 (1983) R.A.Braga, B.E.Gnade, R.W.Fink, H.K.Carter Half-Life of the h9/2 Shell-Model Intruder-State Isomer 187mAu RADIOACTIVITY 187mAu(β+), (EC) [from 178Hf(14N, 5n), E=103 MeV]; measured I(ce), T1/2; deduced ICC, B(E3). Si-Li detector, digital clock, mass separated sources.
doi: 10.1016/0375-9474(83)90636-X
1983GN01 Nucl.Phys. A406, 29 (1983) Decay of Mass-Separated 187Au (8.4 min) to 187Pt RADIOACTIVITY 187Au(EC), (β+) [from 181Ta(12C, 6n), E=100 MeV; 178Hf(14N, 5n), E=103 MeV]; measured T1/2, Eγ, Iγ, I(ce), I(X-ray), γγ(t), (ce)(γ)(t), γ(X-ray)(t), (ce)(X-ray)(t); deduced β+/EC, Q(EC), Iβ, log ft. 187Pt deduced levels, J, π, ICC, γ-multipolarity. Mass separated sources, hyperpure Ge, Ge(Li), Si-Li detectors.
doi: 10.1016/0375-9474(83)90283-X
1982BR19 Phys.Rev. C26, 1302 (1982) Lifetime of the 724.3-keV Level and Shell-Model Intruder States in 109Ag RADIOACTIVITY 109Pd(β-) [from 108Pd(n, γ)]; measured γγ(t), βγ(t). 109Ag level deduced T1/2. Hyperpure Ge, Ge(Li), plastic scintillator detectors.
doi: 10.1103/PhysRevC.26.1302
1982TA18 Nucl.Phys. A388, 498 (1982) M.Tan, R.A.Braga, R.W.Fink, P.Venugopala Rao 207Bi L-Subshell Orbital Electron Capture Probabilities and Decay Energy RADIOACTIVITY 207Bi; measured γ(X-ray)-coin; deduced subshell capture probabilities, Q(EC).
doi: 10.1016/0375-9474(82)90473-0
1980BR23 Nucl.Phys. A349, 61 (1980) R.A.Braga, W.R.Western, J.L.Wood, R.W.Fink, R.Stone, C.R.Bingham, L.L.Riedinger Very Slow M4 Transitions and Shell-Model Intruder States in 199,201Bi RADIOACTIVITY 199,201Po [from 191,193Ir(14N, 6n), E=116 MeV], 199,201Bi [from 199,201Po decays]; measured Eγ, Iγ, I(ce), γγ-, γ(X-ray)-coin. 199,201Bi deduced levels, J, π, (EC+β)/IT branching ratio, ICC, K/L, γ-multipolarity, B(M4). Ge(Li), Si(Li) detectors, mass-separated sources.
doi: 10.1016/0375-9474(80)90443-1
1980GN01 Phys.Rev. C21, 2025 (1980) B.E.Gnade, R.A.Braga, R.W.Fink L2, 3-Subshell X-Ray Fluorescence and Coster-Kronig Yields at Z = 64 And 67 RADIOACTIVITY 155Eu, 165Er; measured (L X-ray)(K X-ray)(t), (L X-ray)(K X-ray)-coin; deduced Coster-Kronig transition probability, subshell fluorescence yields. HPGe, Si(Li) detectors.
doi: 10.1103/PhysRevC.21.2025
1979BR12 Phys.Rev. C19, 2305 (1979) R.A.Braga, J.L.Wood, G.M.Gowdy, R.W.Fink Decay of Mass-Separated 197Tl (2.83 h) to 197Hg RADIOACTIVITY 197Tl [from W(16O, pxn), E=143 MeV]; 197Pb [from W(16O, xn), E=143 MeV; Re(16O, pxn), E=129, 141 MeV]; measured T1/2, Eγ, Iγ, I(ce), I(X-ray), γX-coin, γX-ray-coin, ICC; deduced Iβ, β+/ϵ. 197Hg deduced levels, J, π, γ-multiplicities. Mass, radiochemically separated sources. Particle-vibrator model.
doi: 10.1103/PhysRevC.19.2305
1979RA04 Nucl.Phys. A315, 163 (1979) M.S.Rapaport, R.W.Fink, L.L.Riedinger, L.L.Collins, G.D.O'Kelley Half-Lives and Decay of 197Pb Isomers RADIOACTIVITY 197m,197Pb [from natural Re(16O, pxn), mass separation]; measured γce(t), Eγ, T1/2. Ge(Li), Si(Li) detection.
doi: 10.1016/0375-9474(79)90641-9
1979VI02 Phys.Rev. C19, 282 (1979) A.Visvanathan, E.F.Zganjar, J.L.Wood, R.W.Fink, L.L.Riedinger, F.E.Turner Fast Beta Transition in 183Pt and the Systematics of Nilsson States in the N = 105 Isotones RADIOACTIVITY 183Pt [from 180W(14N, p10n), 180W(14N, α7n), E=187 MeV; decay of 183Hg, 183Au]; measured Eγ, Iγ(t). 183Pt [from 181Ta(16O, xn), E=160-200 MeV]; measured T1/2, Eγ, γγ, γX-coin; deduced log ft. 183Ir levels deduced J, π. Nilsson model. He gas-jet recoil transport, mass separation.
doi: 10.1103/PhysRevC.19.282
1978GO15 Nucl.Phys. A312, 56 (1978) Decay of Mass-Separated 195Tl(1.13 h) to 195Hg RADIOACTIVITY 195Tl [from W(16O, xnp), E=125, 143 MeV; 195Pb decay]; measured T1/2, Eγ, Iγ, I(ce), I(X), γγ-coin; deduced Iβ, β+/ϵ, log ft. 195Hg deduced levels, J, π, ICC, γ-multiplicity. Ge(Li), Si(Li) detectors. Mass, chemically separated sources.
doi: 10.1016/0375-9474(78)90575-4
1978PE08 Nucl.Phys. A302, 1 (1978) Orbital Electron Capture Ratios in the Decay of 205Pb RADIOACTIVITY 205Pb [from 204Pb(n, γ)]; measured M/L, N/M EC ratios; deduced T1/2, Q(EC), multiwire proportional counter. Enriched 204Pb target.
doi: 10.1016/0375-9474(78)90283-X
1977SC03 Phys.Lett. 66B, 133 (1977) A.G.Schmidt, R.L.Mlekodaj, E.L.Robinson, F.T.Avignone, J.Lin, G.M.Gowdy, J.L.Wood, R.W.Fink New Isomers of 185,187Tl and the Departure of the h9/2 Intruder State
doi: 10.1016/0370-2693(77)90158-7
1976BI09 Phys.Rev. C14, 1586 (1976) C.R.Bingham, L.L.Riedinger, F.E.Turner, B.D.Kern, J.L.Weil, K.J.Hofstetter, J.Lin, E.F.Zganjar, A.V.Ramayya, J.H.Hamilton, J.L.Wood, G.M.Gowdy, R.W.Fink, E.H.Spejewski, W.D.Schmidt-Ott, R.L.Mlekodaj, H.K.Carter, K.S.R.Sastry Decay of Mass-Separated 190Tl and 190Hg RADIOACTIVITY 190,190mTl, 190Hg [from Ta, W(16O, X)]; measured Eγ, Iγ, I(ce), Eβ, γX-ray-coin, γγ-coin, T1/2; deduced log ft, Q, ICC. 190Hg, 190Au deduced levels, J, π, λ.
doi: 10.1103/PhysRevC.14.1586
1976GO02 Phys.Rev. C13, 1601 (1976) G.M.Gowdy, A.C.Xenoulis, J.L.Wood, K.R.Baker, R.W.Fink, J.L.Weil, B.D.Kern, K.J.Hofstetter, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, K.S.R.Sastry, A.V.Ramayya, J.H.Hamilton On-Line Mass Separator Investigation of the New Isotope 2.9-sec 116I RADIOACTIVITY 116I, 116Xe; measured Eγ, Iγ, T1/2, βγ(t); deduced Q, log ft. 116I deduced J, π. 116Te, 116Xe deduced levels, J, π.
doi: 10.1103/PhysRevC.13.1601
1976HA25 Izv.Akad.Nauk SSSR, Ser.Fiz. 40, 2 (1976); Bull.Acad.Sci.USSR, Phys.Ser. 40, No.1, 1 (1976) J.H.Hamilton, K.R.Baker, C.R.Bingham, E.L.Bosworth, H.K.Carter, J.D.Cole, R.W.Fink, G.Garcia Bermudez, G.W.Gowdy, K.J.Hofstetter, M.A.Ijaz, A.C.Kahler, B.D.Kern, W.Lourens, B.Martin, R.L.Mlekodaj, A.V.Ramayya, L.L.Riedinger, W.D.Schmidt-Ott, E.H.Spejewski, B.N.Subba Rao, E.L.Robinson, K.S.Toth, F.Turner, J.L.Weil, J.L.Wood, A.Xenoulis, E.F.Zganjar New Isotope 193Pb and the Structure of 193Tl; Shape Coexistence in 188Hg and in 189Au; and a New Ion Source: Recent UNISOR Research RADIOACTIVITY 193Pb; measured T1/2, Eγ, Iγ, γγ-coin. 188Tl; measured Eγ, Iγ, γγ-coin, I(ce), γce-coin. 189Tl, 189Hg; measured Eγ, Iγ, γγ-, γX-, γce-coin. 188,189Hg, 193Tl deduced levels, J, π, shape isomers.
1976NI04 Z.Phys. A278, 239 (1976) The L2-L3 Coster-Kronig Transition Probability at Z = 96 ATOMIC PHYSICS Cm; measured L2-L3 Coster-Kronig transition probability.
doi: 10.1007/BF01409173
1976SA22 Z.Phys. A279, 27 (1976) A.I.Saleh, R.A.Braga, R.W.Fink The K-Shell Conversion Coefficient of the 135.5 keV M4 Transition in 193mPt Decay RADIOACTIVITY 193mPt; measured ICC. X-ray/γ technique.
doi: 10.1007/BF01409088
1976WO10 Phys.Rev. C14, 682 (1976) J.L.Wood, R.W.Fink, E.F.Zganjar, J.Meyer ter Vehn Symmetry between Particle and Hole Level Systems in 189Au RADIOACTIVITY 189,189mHg; measured Eγ, Iγ, γγ-coin, γX-ray(t), γ(t). 198Au deduced levels, K, J, π.
doi: 10.1103/PhysRevC.14.682
1975HA27 Phys.Rev.Lett. 35, 562 (1975) J.H.Hamilton, A.V.Ramayya, E.L.Bosworth, W.Lourens, J.D.Cole, B.Van Nooijen, G.Garcia-Bermudez, B.Martin, B.N.Subba Rao, H.Kawakami, L.L.Riedinger, C.R.Bingham, F.Turner, E.F.Zganjar, E.H.Spejewski, H.K.Carter, R.L.Mlekodaj, W.D.Schmidt-Ott, K.R.Baker, R.W.Fink, G.M.Gowdy, J.L.Wood, A.Xenoulis, B.D.Kern, K.J.Hofstetter, J.L.Weil, K.S.Toth, M.A.Ijaz, K.F.R.Faftry Crossing of Near-Spherical and Deformed Bands in 186,188Hg and New Isotopes 186,188Tl RADIOACTIVITY 186,188Tl [from 181Ta(16O, 9nγ), (16O, 11nγ), E=143-145 MeV]; measured T1/2, Eγ, Iγ, γce-, γγ-coin, γ(t); deduced ICC. 186,188Hg deduced levels, J, π, K.
doi: 10.1103/PhysRevLett.35.562
1975NI05 Z.Phys. A273, 305 (1975) An Investigation of the L2-L3 Coster-Kronig Transition Probability for 63 ≤ Z ≤ 96 RADIOACTIVITY 198Au, 203Hg, 207Bi, 233Pa; measured Coster-Kronig transition probabilities.
doi: 10.1007/BF01435571
1975PA04 Z.Phys. A272, 169 (1975) J.C.Pate, K.R.Baker, R.W.Fink, D.A.McClure, N.S.Kendrick, Jr. A γγ Coincidence Study of Transitions in 239Np and 239Pu from Decay of 243Am RADIOACTIVITY 243Am; measured Eγ, Iγ, γγ-coin. 239Np, 239Pu deduced levels.
doi: 10.1007/BF01408144
1975ZG01 Phys.Lett. 58B, 159 (1975) E.F.Zganjar, J.L.Wood, R.W.Fink, L.L.Riedinger, C.R.Bingham, B.D.Kern, J.L.Weil, J.H.Hamilton, A.V.Ramayya, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott Rotation-Aligned Coupling and Axial Asymmetry in 189-195Au RADIOACTIVITY 189,189m,191,191m,193Hg; measured γγ(t), γ X-ray(t), Eγ, Iγ, I(ce); deduced ICC. 189,191,193Au deduced levels. 189,191,193,195Au deduced systematics.
doi: 10.1016/0370-2693(75)90627-9
1974BA53 Z.Phys. 270, 1 (1974) K.R.Baker, F.Tolea, R.W.Fink, J.J.Pinajian Mean M-Subshell Fluorescence Yields at Z = 88, 90, 92, and 94 RADIOACTIVITY 228Th, 232U, 238Pu, 244Cm; measured ML(X-ray)-coin; deduced M-subshell fluorescence yields.
doi: 10.1007/BF01676786
1974BA54 Z.Phys. 270, 9 (1974) K.R.Baker, F.Tolea, R.W.Fink, J.J.Pinajian An Experimental Investigation of the Onset of the L2-L3M4 and L2-L3M5 Coster-Kronig Transitions for Z > 90 RADIOACTIVITY 244Cm, 238Pu, 232U; measured XX-coin; deduced Coster-Kronig transition probabilities.
doi: 10.1007/BF01676787
1974CH06 Nucl.Phys. A218, 372 (1974) W.M.Chew, A.C.Xenoulis, R.W.Fink, J.J.Pinajian Nuclear Matrix Elements from L/K Electron Capture Ratios in 59Ni Decay RADIOACTIVITY 59Ni [from 58Ni(n, γ)]; measured L/K EC ratio; calculated (L1+L2)/K ratio; deduced L3/K ratio, nuclear matrix element ratio; multiwire proportional counter; isotope separated sources. Enriched 58Ni target.
doi: 10.1016/0375-9474(74)90010-4
1974CH40 Nucl.Phys. A229, 79 (1974) W.M.Chew, A.C.Xenoulis, R.W.Fink, F.J.Schima, W.B.Mann The L/K Electron Capture Ratio in First-Forbidden 81gKr Decay RADIOACTIVITY 81gKr [from (n, γ)]; measured L/K EC ratio; deduced Q(EC), log ft, J, π. Multiwire proportional counter; isotope separated sources. Enriched 80Kr target.
doi: 10.1016/0375-9474(74)90677-0
1974HA10 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2036 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 22 (1974) J.H.Hamilton, E.H.Spejewski, R.L.Mlekodaj, W.-D.Schmidt-Ott, R.W.Fink, A.Xenoulis, K.R.Baker, J.L.Wood, G.Gowdy, H.K.Carter, B.D.Kern, K.J.Hofstetter, J.L.Weil, E.F.Zganjar, K.S.R.Sastry, F.T.Avignone, C.R.Bingham, L.L.Riedinger, L.Harwood, F.Turner, I.A.Sellin, D.J.Pegg, J.Lin, A.V.Ramayya, S.Lee, G.Garcia-Bermudez, E.Bosworth, K.S.Toth, N.R.Johnson Initial UNISOR Research: New Isotopes 186Tl, 188Tl, 116I; Decays of 189,190Tl, 117Xe, and 117I; and Off-Line Atomic and Nuclear Studies RADIOACTIVITY 116,117Xe, 116,117I, 186,188,189,190Tl; measured T1/2, Eγ, Iγ, γγ, Eβ; deduced Q(β). 126I measured γγ(θ, H). 117I, 116Te, 188,190Hg deduced levels, J, π. 126Xe level deduced g. On-line isotope separator UNISOR.
1974TO04 Z.Phys. 268, 289 (1974) F.Tolea, K.R.Baker, W.D.Schmidt-Ott, R.W.Fink The Electron Capture Decay of 125I and 145Pm RADIOACTIVITY 145Pm; measured Xγ-coin, Eγ, Iγ; deduced Q. 125I; measured Xγ-coin. 125Te deduced omegak.
doi: 10.1007/BF01669463
1974VA02 Nucl.Phys. A219, 595 (1974) E.Vatai, A.C.Xenoulis, K.R.Baker, F.Tolea, R.W.Fink The Electron Capture Decay of 85gSr RADIOACTIVITY 85gSr [from 84Sr(n, γ), chem]; measured Eγ, Iγ, T1/2, γγ-, X-γ coin; deduced K-capture probability P(K) ratio, Q, log ft. 85Rb deduced level, T1/2. Ge(Li), NaI(Tl) detectors. Enriched target.
doi: 10.1016/0375-9474(74)90120-1
1973MC07 J.Phys. (London), B6, 573 (1973) J.C.McGeorge, D.W.Nix, R.W.Fink Coster-Kronig and Fluorescence Yields for the L2 and L3 Subshells in The High-Z Region RADIOACTIVITY 223Ra, 227Th, 239Np; measured XX-coin; deduced fluorescence, Koster-Kronig yields.
doi: 10.1088/0022-3700/6/3/026
1973NI07 Phys.Lett. 46A, 205 (1973) D.W.Nix, J.C.McGeorge, R.W.Fink X-Ray Intensity Ratio I(Lα)/I(Ll) in the Region 55 < Z < 94 RADIOACTIVITY 133Ba, 139Ce, 145Pm, 159Dy, 181W, 207Bi; measured I(L-X rays).
doi: 10.1016/0375-9601(73)90136-9
1972BB16 Rev.Mod.Phys. 44, 716 (1972) W.Bambynek, B.Crasemann, R.W.Fink, H.-U.Freund, H.Mark, C.D.Swift, R.E.Price, P.Venugopala Rao X-Ray Fluorescence Yields, Auger, and Coster-Kronig Transition Probabilities
doi: 10.1103/RevModPhys.44.716
1972HA01 Nucl.Phys. A180, 157 (1972) A.K.Hankla, R.W.Fink, J.H.Hamilton Neutron Activation Cross Sections at 14.4 MeV for Some Naturally Occurring Heavy Elements in the Region 76 < Z < 82 NUCLEAR REACTIONS 192Os, 192,198Pt, 197Au, 196,198,200,204Hg, 203Tl, 204Pb(n, 2n), 199Hg, 204Pb(n, n'), 197Au(n, 3n), 199Hg(n, np+pn+d), E =14.4 MeV; measured σ by activation. Enriched Hg target, natural targets.
doi: 10.1016/0375-9474(72)90162-5
1972HA21 Z.Phys. 249, 373 (1972) J.S.Hansen, J.C.McGeorge, R.W.Fink, R.E.Wood, P.V.Rao, J.M.Palms Precision Determination of High-Z K-Shell Fluorescence Yields from 195Au, 207Bi, and 235Np Decays RADIOACTIVITY 195Au, 207Bi, 235Np; measured I(X-ray), I(Auger). Pt, Pb, U deduced K-shell fluorescence yields.
doi: 10.1007/BF01386769
1972MC07 Z.Phys. 250, 293 (1972) The L1 Subshell Fluorescence and Coster-Kronig Yields for Z = 96 RADIOACTIVITY 249Cf; measured Xlce-coin, Xlγ-coin, XlXk-coin. Cm deduced L1 fluorescence, Coster-Kronig yields. ATOMIC PHYSICS Cm; measured L1 fluorescence, Coster-Kronig yields.
doi: 10.1007/BF01395051
1972MC25 Z.Phys. 255, 335 (1972) J.C.McGeorge, D.W.Nix, R.W.Fink, J.H.Landrum L-Subshell Fluorescence and Coster-Kronig Yields at Z = 92 and the Decay of 235Np RADIOACTIVITY 235Np; measured (K X-ray)(L X-ray)-coin, L/K EC ratio deduced Q(EC), Pl/Pk, Pk. U deduced L-subshell fluorescence, Coster-Kronig yields.
doi: 10.1007/BF01392538
1972NI16 Z.Phys. 256, 131 (1972) D.W.Nix, J.C.McGeorge, R.W.Fink Mean L-Shell X-Ray Fluorescence Yields at Z = 47, 60, and 63 RADIOACTIVITY 109Cd, 145Pm, 153Gd; measured I(L X-ray)/I(K X-ray) ratios. Ag, Pm, Eu deduced L-shell fluorescence yields.
doi: 10.1007/BF01400485
1972PE06 Phys.Rev. C5, 2007 (1972) J.G.Pengra, H.Genz, J.P.Renier, R.W.Fink Orbital-Electron-Capture Ratios in the Decay of 55Fe RADIOACTIVITY 55Fe; measured M/L, L/K EC ratios; deduced EC probability ratios.
doi: 10.1103/PhysRevC.5.2007
1972SC08 Z.Phys. 249, 286 (1972) The Determination by an Independent Method of P(K) Electron Capture Probabilities in 133Ba and 139Ce Decays. Gamma Decay of 133Ba RADIOACTIVITY 133Ba, 139Ce; measured Xγ-coin, ceXk-coin; deduced Q, K-capture probability P(K). 133Ba; measured Eγ, Iγ. 133Cs transitions deduced ICC. Ge(Li) detectors.
doi: 10.1007/BF01379722
1972SC11 Z.Phys. 250, 191 (1972) W.-D.Schmidt-Ott, J.S.Hansen, R.W.Fink Relative X-Ray Transition Probabilities to the K-Shell for Z = 81, 92, 94, and 96 ATOMIC PHYSICS Tl, U, Pu, Cm; measured I(K X-ray); deduced relative X-ray transition probabilities. Ge(Li) detectors.
doi: 10.1007/BF01387455
1972SC25 Z.Phys. 253, 13 (1972) Gamma Branching and Total Conversion Coefficients of Intraband Transitions in the Groundstate Rotational Band of 245Cm RADIOACTIVITY 249Cf; measured γγ-coin. 245Cm transitions deduced ICC, γ-branching.
doi: 10.1007/BF01387165
1972SC42 Z.Phys. 254, 281 (1972) The K-Conversion Coefficient Near Threshold of the 30 keV Isomeric Transition in 108mAg Decay RADIOACTIVITY 108mAg; measured Xγ-coin, Eγ, Iγ, I(X-ray). 108Ag transition deduced ICC.
doi: 10.1007/BF01390257
1972SC44 Z.Phys. 255, 161 (1972) W.-D.Schmidt-Ott, J.C.McGeorge, R.W.Fink Multipolarity Determination from L X-Ray Spectra in the Decays of 227Th, 243Am, and 249Cf RADIOACTIVITY 227Th, 243Am, 249Cf; measured (L X-ray)(γ)-coin. 239Np, 245Cm, 223Ra transitions deduced γ-mixing.
doi: 10.1007/BF01394524
1971FI04 Phys.Rev. C3, 1701 (1971) Bismuth L-Subshell Fluorescence and Coster-Kronig Yields from Decay of Pb210 (RaD) RADIOACTIVITY 210Pb; measured nothing; reanalyzed data. Bi deduced L-subshell fluorescence, Coster-Kronig yields Bi; measured nothing; reanalyzed data; deduced L-subshell fluorescence, Coster-Kronig yields.
doi: 10.1103/PhysRevC.3.1701
1971GE02 Phys.Rev. C3, 172 (1971) H.Genz, J.P.Renier, J.G.Pengra, R.W.Fink Multiwire-Proportional-Counter Measurement of the M/L Orbital-Electron-Capture Ratio in 71Ge Decay RADIOACTIVITY 71Ge; measured I(ce), M/L EC ratio, T1/2, L/K EC ratio.
doi: 10.1103/PhysRevC.3.172
1971KA48 Phys.Rev. A4, 1695 (1971) E.Karttunen, H.U.Freund, R.W.Fink M-Subshell Fluorescence Yields and the L1-L3 Radiative Transition at Z = 93 and 96 from Am241 and Cf249 Decays RADIOACTIVITY 241Am, 249Cf; measured XX-coin. Np, Cm deduced M-subshell fluorescence yields, L1 - L3 radiative transitions.
doi: 10.1103/PhysRevA.4.1695
1971LU10 Phys.Rev. C4, 1173 (1971) Applicability of the Constant-Nuclear-Temperature Approximation in Statistical-Model Calculations of Neutron Cross Sections at 14.4 MeV for Medium-Z Nuclei NUCLEAR REACTIONS 58Ni, 90,96Zr, 92,100Mo, 96,98,104Ru, 103Rh, 102,110Pd, 106,108,110,116Cd, 112,114Sn, 121,123Sb, 122,128,130Te, 127I, 133Cs, 130,132Ba, 136,140,142Ce(n, 2n), 58Ni, 92Zr, 96,97Mo, 96Ru, 103Rh, 105,106,108Pd, 106,112Cd, 112,117Sn, 138Ba, 140Ce(n, p), 94Zr, 92,98Mo, 106,108Pd, 133Cs, 138Ba, 142Ce(n, α), E=14.4 MeV; calculated σ. Statistical model, constant nuclear temperature approximation.
doi: 10.1103/PhysRevC.4.1173
1971MC24 Z.Phys. 248, 208 (1971) L2 and L3 Subshell Fluorescence and Coster-Kronig Yields for Z=96 from the Decay of 249Cf RADIOACTIVITY 249Cf, 244Cm, 238Pu; measured I(L X-ray), U, Pu, Cm deduced L2, L3 fluorescence, Coster-Kronig yields.
doi: 10.1007/BF01396477
1971RA02 Phys.Rev. C3, 629 (1971) P.V.Rao, R.E.Wood, J.M.Palms, R.W.Fink Neutron Activation Cross Sections for As, Br, Rb, and Sr Isotopes at 14.4 MeV NUCLEAR REACTIONS As, Rb, Br, Sr(n, 2n), (n, p), (n, α), E=14.4 MeV; measured activation σ.
doi: 10.1103/PhysRevC.3.629
1971SC14 Z.Phys. 245, 191 (1971) W.-D.Schmidt-Ott, R.W.Fink, P.V.Rao Gamma Radiation in the Decay of 249Cf RADIOACTIVITY 249Cf; measured Eγ, Iγ, I(K X-ray), γγ-coin, Xγ-coin. 245Cm deduced transitions.
doi: 10.1007/BF01395230
1970HA06 Nucl.Phys. A142, 604 (1970) J.S.Hansen, H.U.Freund, R.W.Fink Relative X-Ray Transition Probabilities to the K-Shell ATOMIC PHYSICS Cl, Cr, Fe, As, Sr, Ag, Te, Xe, Ba, La, Eu, Tb, Yb, Ta, Pt, Tl, Pb; measured I(X-ray)(Kβ)/I(X-ray)(Kα); deduced Kβ/Kα ratio for 18 < Z < 90. Tl, Pb; measured Kα2/Kα1, Kβ1/Kα1, Kβ2/Kα1. Ge(Li), Si(Li) detectors; carrier-free sources.
doi: 10.1016/0375-9474(70)90816-X
1970HA44 Nucl.Phys. A153, 465 (1970) J.S.Hansen, H.U.Freund, R.W.Fink Relative K X-Ray Transition Probabilities at Z = 96 from 249Cf Decay ATOMIC PHYSICS Cm; measured Kβ/Kα, Kα2/Kα1, K'β1/Kα1K'β2/Kα1 X-ray intensity ratios at Z=96 from 249Cf source. Ge(Li) detector.
doi: 10.1016/0375-9474(70)90785-2
1970LU18 Phys.Rev. C 1, 350 (1970) Activation Cross Sections for (n, 2n) Reactions at 14.4 MeV in the Region Z=40-60. Precision Measurements and Systematics NUCLEAR REACTIONS 90Zr(n, 2n), 96Zr(n, 2n), 93Nb(n, 2n), 92Mo(n, 2n), 100Mo(n, 2n), 96Ru(n, 2n), 98Ru(n, 2n), 104Ru(n, 2n), 103Rh(n, 2n), 102Pd(n, 2n), 110Pd(n, 2n), 108Cd(n, 2n), 110Cd(n, 2n), 111Cd(n, n'), 112Cd(n, 2n), 116Cd(n, 2n), 112Sn(n, 2n), 112Sn(n, np), 114Sn(n, 2n), 117Sn(n, n'), 118Sn(n, 2n), 121Sb(n, 2n), 123Sb(n, 2n), 122Te(n, 2n), 123Te(n, n'), 124Te(n, 2n), 128Te(n, 2n), 130Te(n, 2n), 127I(n, 2n), 133Cs(n, 2n), 130Ba(n, 2n), 130Ba(n, np), 132Ba(n, 2n), 134Ba(n, 2n), 135Ba(n, n'), 136Ba(n, 2n), 136Ce(n, 2n), 138Ce(n, 2n), 140Ce(n, 2n), 142Ce(n, 2n), E=14.4 MeV; measured products, 89Zr, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry 10497.
doi: 10.1103/PhysRevC.1.350
1970LU19 Phys.Rev. C 1, 358 (1970) Activation Cross Sections for (n, p), ((n, np)+(n, pn)+ (n, d)), and (n, α) Reactions in the Region of Z=40 to 58 at 14.4 MeV NUCLEAR REACTIONS 90Zr(n, p), 91Zr(n, p), 92Zr(n, p), 94Zr(n, α), 93Nb(n, α), 92Mo(n, α), 92Mo(n, p), 96Mo(n, p), 97Mo(n, p), 98Mo(n, α), 98Mo(n, p), 96Ru(n, d), 96Ru(n, np), 96Ru(n, p), 103Rh(n, p), 105Pd(n, p), 106Pd(n, α), 106Pd(n, p), 108Pd(n, α), 108Pd(n, p), 112Cd(n, p), 116Sn(n, p), 117Sn(n, p), 133Cs(n, α), 138Ba(n, α), 138Ba(n, p), 140Ce(n, p), 142Ce(n, α), E=14.4 MeV; measured products, 90Y, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry 10145.
doi: 10.1103/PhysRevC.1.358
1970MC21 Nucl.Phys. A154, 526 (1970) J.C.McGeorge, H.U.Freund, R.W.Fink Decay of 159Dy: L-Subshell X-Ray Fluorescence and Coster-Kronig Yields at Z = 65; Branching Ratio, and K-Conversion of the 58 keV Transition in 159Tb RADIOACTIVITY 159Dy; measured I(K X-ray), Iγ, X(K)γ-, X(K)X(K)-, XlXk-coin; deduced EC-branching. 159Tb transition deduced α(K), γ-mixing. Tb deduced L-subshell fluorescence, Coster-Kronig yields. Ge(Li), Si(Li) detectors.
doi: 10.1016/0375-9474(70)90124-7
1970MO07 Phys.Rev. C1, 254 (1970) S.Mohan, H.U.Freund, R.W.Fink, P.V.Rao Decays of Tm170 and Tm171: L2 and L3 Subshell-Fluorescence Yields, Coster-Kronig Transition Probabilities, and K-Shell Conversion Coefficients in Yb RADIOACTIVITY 170,171Tm; measured Iγ, I(X-ray), XkXl-coin. 170Tm deduced EC-branching. Yb deduced L-subshell fluorescence yields, Coster-Kronig transition probabilities. 170Yb transitions deduced ICC. 171Yb transition deduced ICC, γ-mixing.
doi: 10.1103/PhysRevC.1.254
1970MO34 Z.Phys. 239, 423 (1970) S.Mohan, R.W.Fink, R.E.Wood, J.M.Palms, P.Venugopala Rao Electron Capture Decay of 181W: L Subshell Fluorescence and Coster-Kronig Yields in Ta RADIOACTIVITY 181W; measured I(L X-ray), (L X-ray)(K X-ray)-, (L X-ray)(γ)-coin; deduced L-shell fluorescence, Coster-Kronig yields. Ta; measured L-subshell fluorescence, Coster-Kronig yields.
doi: 10.1007/BF01401197
1969FI05 Phys.Rev. 180, 1220 (1969) M/L Orbital-Electron Capture Ratios in Cd109 Decay RADIOACTIVITY 109Cd, 113Sn; deduced M/L capture ratio. NUCLEAR REACTIONS 62Ni(p, X), E=14.3 MeV; 59Co(α, X), E=15.4 MeV; 59Co(p, X), E=14.3 MeV; 56Fe(α, X), E=18.6 MeV; measured σ(Ep', Eα), σ(Eα', Ep); deduced violation of hypothesis of compound nucleus decay, formation independence. 60Ni, 63Cu compound nuclei deduced formation, decay mode relation.
doi: 10.1103/PhysRev.180.1220
1969FR07 Phys.Rev. 178, 1952 (1969) Bismuth L-Subshell Fluorescence Yields and Coster-Kronig Transition Probabilities from Decay of Pb210 (RaD) RADIOACTIVITY 210Pb; measured I(X-ray), E(X-ray). ATOMIC PHYSICS Bi;deduced Auger, fluorescence, Coster-Kronig yields.
doi: 10.1103/PhysRev.178.1952
1969FR16 Nucl.Phys. A138, 200 (1969) H.U.Freund, H.Genz, J.B.Siberts, R.W.Fink Precision Determination of the K-Shell Fluorescence Yield of Gallium RADIOACTIVITY 71Ge; measured I(K X-ray), I(Auger). ATOMIC PHYSICS Ga; deduced K-shell fluorescence yield.
doi: 10.1016/0375-9474(69)90392-3
1969KA08 Nucl.Phys. A131, 343 (1969) E.Karttunen, H.U.Freund, R.W.Fink The K-Fluorescence Yield of Te and the Total and K-Shell Conversion Coefficients of the 35.48 keV Transition in 125I Decay RADIOACTIVITY 125I; measured Iγ, I(X-ray), Xγ-, XX-coin, ICC. Ge(Li) detector. ATOMIC PHYSICS Te; measured K-fluoresence yield.
doi: 10.1016/0375-9474(69)90539-9
1969RA01 Nucl.Phys. A127, 683 (1969) N.RanaKumar, R.W.Fink, P.V.Rao K-Shell Conversion Coefficient of the 40.58 keV Transition in 99Mo Decay RADIOACTIVITY 99Mo; measured ICC. 99Tc deduced γ-multipolarity.
doi: 10.1016/0375-9474(69)91041-0
1969RA13 Phys.Rev. 178, 1997 (1969) P.V.Rao, R.E.Wood, J.M.Palms, R.W.Fink Electron-Capture Decay of Bi207: L-Subshell Fluorescence Yields and Coster-Kronig Transition Probabilities of Pb RADIOACTIVITY 207Bi; measured I(X-ray), E(X-ray), XX-coin, Xγ-coin, Xce-coin. Ge(Li) detector. Pb; deduced L-subshell fluorescence yields, Coster-Kronig yields.
doi: 10.1103/PhysRev.178.1997
1969RA37 Nucl.Phys. A128, 333 (1969) N.RanaKumar, E.Karttunen, R.W.Fink Thermal and 14.4 MeV Neutron Activation Cross Sections of Argon NUCLEAR REACTIONS 40Ar(n, γ), E=th; 38,40Ar(n, p), 40Ar(n, X), 40Ar(n, α), En=14.4 MeV; measured σ by activation; Ge(Li) detector; solid quinolclathrate target; mixed powder method.
doi: 10.1016/0375-9474(69)90996-8
1968FI02 Nucl.Phys. A110, 379 (1968) Comparison with theory of Experimental Values of L/K Orbital Electron Capture Ratios for Allowed and First-Forbidden Transitions
doi: 10.1016/0375-9474(68)90547-2
1968HA51 ORO-3346-40 (1968) A.K.Hankla, J.H.Hamilton, R.W.Fink Total Conversion Coefficient of the 375 keV Transition in 199mHg Decay RADIOACTIVITY 199mHg; measured Iγ; deduced ICC, γ-multipolarity.
1968KO13 Nucl.Phys. A120, 329 (1968) E.Kondaiah, N.RanaKumar, R.W.Fink Thermal Neutron Activation Cross Sections for Kr and Xe Isotopes NUCLEAR REACTIONS 78,80,82,84Kr, 124,126,128,130,132,134,136Xe(n, γ). E=thermal; measured σ; deduced isomer cross-section ratio, spin cutoff parameter. Solid quinol-clathrate targets.
doi: 10.1016/0375-9474(68)90769-0
1968KO28 Nucl.Phys. A120, 337 (1968) E.Kondaiah, N.Ranakumar, R.W.Fink Neutron Activation Cross Sections At 14.4 Mev For Kr And Xe Isotopes NUCLEAR REACTIONS 78Kr(n, 2n), 80Kr(n, 2n), 80Kr(n, p), 82Kr(n, 2n), 82Kr(n, p), 84Kr(n, p), 86Kr(n, 2n), 86Kr(n, α), 124Xe(n, 2n), 126Xe(n, 2n), 128Xe(n, 2n), 130Xe(n, 2n), 130Xe(n, p), 131Xe(n, p), 132Xe(n, 2n), 132Xe(n, p), 134Xe(n, 2n), 134Xe(n, p), 136Xe(n, 2n), E=14.4 MeV; measured products, 77Kr, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry 11884.
doi: 10.1016/0375-9474(68)90770-7
1968KO30 Bull.Am.Phys.Soc. 13, 602 DE6 (1968) E.Kondaiah, N.Ranakumar, R.W.Fink 14-MeV neutron cross sections for Krypton Isotopes NUCLEAR REACTIONS 78,80,82,86Kr(n, 2n), 80,82,84Kr(n, p), 86Kr(n, α), E=14.4 MeV; measured reaction products, Eγ, Iγ; deduced σ using 27Al and 56Fe monitors. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11884. 1968NG02 Phys.Rev. 176, 1329 (1968) A.Ng, R.E.Wood, J.M.Palms, P.V.Rao, R.W.Fink Gamma Rays from the Decay of 75Ge and 77Ge RADIOACTIVITY 75,77Ge; measured Eγ, Iγ, γγ-coin. 75,77As deduced levels. Ge(Li) detector.
doi: 10.1103/PhysRev.176.1329
1968RA20 Nucl.Phys. A122, 679 (1968) N.RanaKumar, E.Kondaiah, R.W.Fink Neutron Activation Cross Sections at 14.4 MeV for Si and Zn Isotopes NUCLEAR REACTIONS 27Al, 28,29,30Si, 64,66,68Zn(n, p), 30Si, 68Zn(n, α) 64,66,70Zn(n, 2n), E=14.4 MeV; measured σ.
doi: 10.1016/0375-9474(68)90587-3
1968RA35 Phys.Letters 26B, 618 (1968) K-Shell Conversion Coefficient of the 102.7 keV Transition in the 81Se-m Decay
doi: 10.1016/0370-2693(68)90433-4
1968RE02 Phys.Rev. 166, 935 (1968) J.P.Renier, H.Genz, K.W.D.Ledingham, R.W.Fink M/L Orbital-Electron-Capture Ratio in Ar37 Decay and the Fraction of Kα X Rays in the K Series of Chlorine NUCLEAR STRUCTURE 37Ar; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.166.935
1967FI10 Arkiv Fysik 36, 471 (1967) R.W.Fink, T.H.Braid, A.W.Friedman Delayed Protons Following He3 Reactions with Oxygen, Silicon, and Sulfur Targets
1967RA08 Phys.Rev. 154, 1028 (1967) Gamma Decay of Se73m,73gSe and Se81m,81gSe Isomeric Pairs NUCLEAR STRUCTURE 73Se, 81Se; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.154.1028
1967RA11 Nucl.Phys. A103, 385 (1967) Levels in 106Pd from Decay of 8.5-d 106Ag, 24-min 106Ag and 30-sec 106Rh RADIOACTIVITY 106,106mAg [from Ag(n, 2n)], 106Rh [from 106Ru(β-)]; measured Eγ, Iγ, γγ-, Xγ-coin. 106Pd deduced levels, J, π, ICC, log ft. Ge(Li) detector.
doi: 10.1016/0375-9474(67)90259-X
1967VE12 Phys.Rev. 154, 1023 (1967) Neutron Reaction Cross Sections of Selenium and Iron at 14.4 MeV NUCLEAR REACTIONS 54Fe(n, α), 54Fe(n, p), 74Se(n, 2n), 74Se(n, p), 76Se(n, 2n), 76Se(n, p), 78Se(n, α), 78Se(n, p), 80Se(n, 2n), 80Se(n, α), 82Se(n, 2n), E=14.4 MeV; measured products, 51Cr, 4He, 54Mn, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry 11722.
doi: 10.1103/PhysRev.154.1023
1967WO09 Phys.Rev. 154, 1108 (1967) R.E.Wood, W.S.Cook, J.R.Goodgame, R.W.Fink Activation Cross Sections Of Germanium For 14.4-Mev Neutrons NUCLEAR REACTIONS 70Ge(n, 2n), 72Ge(n, α), 72Ge(n, p), 73Ge(n, p), 74Ge(n, α), 74Ge(n, p), 76Ge(n, 2n), E=14.4 MeV; measured products, 69Ge, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry 11825.
doi: 10.1103/PhysRev.154.1108
1966FI08 Rev.Mod.Phys. 38, 513 (1966) R.W.Fink, R.C.Jopson, H.Mark, C.D.Swift Atomic Fluorescence Yields
doi: 10.1103/RevModPhys.38.513
1966SC21 Z.Physik 197, 124 (1966) The Reactions N14(n, α)B11 and N14(n, t)C12 Observed with a Gridded Ionization Chamber NUCLEAR STRUCTURE 14N, 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01326742
1966WO09 Bull.Am.Phys.Soc. 11, 808 AD2 (1966), Priv.Comm. R.E.Wood, W.S.Cook, J.R.Goodgame, R.W.Fink Activation Cross Sections of Germanium for 14.4-Mev Neutrons NUCLEAR REACTIONS Ge(n, X)69Ge/75Ge/72Ga/73Ga/74Ga/69Zn/71Zn, E=14.4 MeV; measured reaction products; deduced ground and isomeric states σ and uncertainties. Comparison with systematics.
1965BR03 Bull.Am.Phys.Soc. 10, No.1, 120, KC13 (1965) T.H.Braid, A.M.Friedman, R.W.Fink Delayed Proton Emission from Isotopes of Neon, Sulfur, and Argon NUCLEAR STRUCTURE 17Ne, 28S; measured not abstracted; deduced nuclear properties.
1965MO06 Phys.Rev. 139, B282 (1965); See Also 69Fi05 M/L- and L/K-Orbital Electron-Capture Ratios and Transition Energy in Cd109 Decay NUCLEAR STRUCTURE 109Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B282
1965NU02 Phys.Lett. 14, 136 (1965) A New Short-Lived Isotope of Gallium NUCLEAR STRUCTURE 63Ga; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90453-1
1964BA36 Phys. Rev. 136, B603 (1964) E.L.Bahn, Jr., B.D.Pate, R.D.Fink, C.D.Coryell Decay of 20-Minute Ag115 NUCLEAR STRUCTURE 115Ag; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B603
1964FI01 Priv.Comm. (January 1964) NUCLEAR STRUCTURE 63Ga; measured not abstracted; deduced nuclear properties.
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