NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = W.T.Milner Found 61 matches. 2005FI01 Nucl.Phys. A748, 351 (2005) R.Fitzgerald, E.Abbotoy, D.W.Bardayan, J.C.Blackmon, A.E.Champagne, A.A.Chen, U.Greife, D.W.Hill, A.N.James, R.L.Kozub, T.A.Lewis, R.Livesay, Z.Ma, S.L.Mahan, J.W.McConnell, W.T.Milner, B.H.Moazen, P.D.Parker, D.E.Pierce, M.E.Roettger, L.Sahin, D.Shapira, M.S.Smith, F.Strieder, K.B.Swartz, J.S.Thomas, D.W.Visser Studies of (p, γ) reactions with the Daresbury Recoil Separator at ORNL'S HRIBF NUCLEAR REACTIONS 1H(17O, γ), E=12.5 MeV; measured particle spectra; deduced resonance strength. Recoil separator, other reactions discussed.
doi: 10.1016/j.nuclphysa.2004.09.155
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
1998BA13 Phys.Rev. C57, R1042 (1998) J.C.Batchelder, C.R.Bingham, K.Rykaczewski, K.S.Toth, T.Davinson, J.A.McKenzie, P.J.Woods, T.N.Ginter, C.J.Gross, J.W.McConnell, E.F.Zganjar, J.H.Hamilton, W.B.Walters, C.Baktash, J.Greene, J.F.Mas, W.T.Milner, S.D.Paul, D.Shapira, X.J.Xu, C.H.Yu Observation of the Exotic Nucleus 145Tm Via Its Direct Proton Decay RADIOACTIVITY 145Tm(p) [from 92Mo(58Ni, 4np)]; measured Ep, T1/2; deduced spectroscopic factor. 113Cs(p) [from 58Ni(58Ni, 2np)]; measured T1/2. Recoil mass spectrometer. Comparison with calculated values.
doi: 10.1103/PhysRevC.57.R1042
1997JO01 Phys.Rev. C55, 652 (1997) N.R.Johnson, J.C.Wells, Y.Akovali, C.Baktash, R.Bengtsson, M.J.Brinkman, D.M.Cullen, C.J.Gross, H.-Q.Jin, I.-Y.Lee, A.O.Macchiavelli, F.K.McGowan, W.T.Milner, C.-H.Yu Lifetimes of High-Spin States in the πi13/2 Band of 173Re NUCLEAR REACTIONS 150Sm(27Al, 4n), E=132 MeV; measured γγγ-coin. 173Re deduced high-spin levels T1/2, transition quadrupole moments.
doi: 10.1103/PhysRevC.55.652
1994MC03 Nucl.Phys. A571, 569 (1994) Coulomb Excitation of States in 238U NUCLEAR REACTIONS 238U(α, α'γ), E=18 MeV; measured Iγ, Eγ, γ(θ) following Coulomb excitation. 238U levels deduced B(λ), J, π, δ.
doi: 10.1016/0375-9474(94)90226-7
1993MC07 Nucl.Phys. A562, 241 (1993) Coulomb Excitation of States in 232Th NUCLEAR REACTIONS 232Th(α, α'γ), E=18 MeV; measured Iγ, Eγ, γ(θ) following Coulomb excitation. 232Th deduced levels, B(λ), J, π, δ.
doi: 10.1016/0375-9474(93)90198-7
1988BE41 Phys.Scr. 38, 657 (1988) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson, G.A.Leander, C.W.Reich Coulomb Excitation of States in 229Th NUCLEAR REACTIONS 229Th(α, α), (α, α'), E=17 MeV; measured σ(Eα), σ(Eα') following Coulomb excitation. 229Th levels deduced excitation probability, B(E2), intrinsic quadrupole, hexadecapole moments, J, π, K, Nilsson assignments.
doi: 10.1088/0031-8949/38/5/004
1987LE01 Phys.Rev. C35, 605 (1987) I.Y.Lee, C.Baktash, J.R.Beene, M.P.Fewell, M.L.Halbert, N.R.Johnson, F.K.McGowan, W.T.Milner, H.J.Kim, R.O.Sayer, D.G.Sarantites Distributions of the Total Energy and Multiplicity of Gamma Rays feeding the Discrete Yrast States in Heavy-Ion-Induced Fusion Reactions NUCLEAR REACTIONS 150Sm(12C, 4n), (12C, 3n), E=65 MeV; 100Mo(34S, 4n), E=144 MeV; 70Zn(50Ti, 4n), (50Ti, 3n), E=170 MeV; measured γ-multiplicities, total energy distributions. 158,159Er, 130Ce, 116,117Te deduced entry state distribution width vs yrast transition spin. Ge, NaI detectors, spin spectrometer.
doi: 10.1103/PhysRevC.35.605
1987MC01 Phys.Rev. C35, 968 (1987) F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, R.M.Diamond, F.S.Stephens, M.W.Guidry Test of the Triaxial Rotor Model and the Interacting Boson-Fermion Approximation Model Description of Collective States in 193Ir NUCLEAR REACTIONS 191,193Ir(40Ar, 40Ar'), E=160 MeV; 191,193Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ, relative γ-ray yields following Coulomb excitation. 191,193Ir deduced levels, J, π, K, B(E2). Enriched targets, parallel plate avalanche counters.
doi: 10.1103/PhysRevC.35.968
1987OL01 Nucl.Instrum.Methods Phys.Res. A254, 1 (1987) D.K.Olsen, K.A.Erb, C.M.Jones, W.T.Milner, D.C.Weisser, N.F.Ziegler Calibration of the HHIRF Tandem Accelerator Energy-Analyzing Magnet NUCLEAR REACTIONS 12C(16O, α), E=27.3 MeV; measured σ(Eα). Energy analyzing magnet.
doi: 10.1016/0168-9002(87)90474-8
1987RA01 At.Data Nucl.Data Tables 36, 1 (1987) S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson Transition Probability, B(E2), from the Ground to the First-Excited 2+ State of Even-Even Nuclides COMPILATION A=6-254; compiled, evaluated 2+ level energies, B(E2), T1/2, β2, β2/β2(sp), EWSR, intrinsic quadrupole moments.
doi: 10.1016/0092-640X(87)90016-7
1986ER10 Phys.Lett. 181B, 52 (1986) Evidence for Peak Structure in e+ + Th Interactions NUCLEAR REACTIONS 181Ta, 232Th(e+, e+e-), E ≤ 1.9 MeV; measured e+, e- spectra; deduced structure. Magnetic spectrometer, coincidence method.
doi: 10.1016/0370-2693(86)91253-0
1986MC01 Phys.Rev. C33, 855 (1986) F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, J.Hattula, M.P.Fewell, Y.A.Ellis-Akovali, R.M.Diamond, F.S.Stephens, M.W.Guidry Test of the Triaxial Rotor Model and the Interacting Boson Fermion Approximation Model Description of Collective States in 191Ir NUCLEAR REACTIONS 191Ir(40Ar, 40Ar'), E=160 MeV; 191Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ(θ) following Coulomb excitation. 191Ir deduced levels, J, π, B(λ).
doi: 10.1103/PhysRevC.33.855
1982BE12 Phys.Rev. C25, 1637 (1982) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of Ground Band Rotational States in 249Bk NUCLEAR REACTIONS 249Bk(α, α), (α, α'), E=17.06 MeV; measured σ(Eα, θ=150°). 249Bk levels deduced B(E2), B(M1), quadrupole moment, μ. Enriched target.
doi: 10.1103/PhysRevC.25.1637
1982SA21 Phys.Lett. 115B, 441 (1982) D.G.Sarantites, M.Jaaskelainen, R.Woodward, F.A.Dilmanian, D.C.Hensley, J.H.Barker, J.R.Beene, M.L.Halbert, W.T.Milner Population of the Entry States in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 146Nd(20Ne, 5n), (20Ne, 6n), (20Ne, 7n), E=136 MeV; measured σ vs γ-multiplicity, entry state distributions; deduced entrance channel fusion (L). Statistical model.
doi: 10.1016/0370-2693(82)90388-4
1981BE54 Phys.Rev. C24, 2723 (1981) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of Rotational States and Ground-State Quadrupole Moment for 243Am NUCLEAR REACTIONS 243Am(α, α'), E=17 MeV; measured σ(Eα', θ=150°), Coulomb excitation. 243Am levels deduced B(E2), B(E4), quadrupole moment. Enriched target.
doi: 10.1103/PhysRevC.24.2723
1981MC06 Phys.Rev. C23, 1926 (1981) Reduced M1, E1, E2, and E3 Transition Probabilities for Transitions in 156-160Gd and 160-164Dy NUCLEAR REACTIONS 156,158,160Gd, 160,162,164Dy(α, α'), E=13.5 MeV; measured Iγ, Eγ, γ(θ), Coulomb excitation. 156,158,160Gd, 160,162,164Dy levels deduced B(λ), T1/2, J, π, δ. Enriched targets. Interacting boson model.
doi: 10.1103/PhysRevC.23.1926
1980RO02 Phys.Rev. C21, 603 (1980) R.L.Robinson, H.J.Kim, R.O.Sayer, W.T.Milner, R.B.Piercey, J.H.Hamilton, A.V.Ramayya, J.C.Wells, Jr., A.J.Caffrey High-Spin Levels and Band Structure in 78Kr NUCLEAR REACTIONS 68Zn(12C, 2n), E=33-38 MeV; measured Eγ, Iγ, γ(θ), Doppler broadening, linear polarization. 78Kr levels deduced J, π, δ, γ-branching, T1/2.
doi: 10.1103/PhysRevC.21.603
1979MC04 Phys.Rev. C20, 2093 (1979) F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, D.Shapira, P.H.Stelson Coulomb Excitation of 183W NUCLEAR REACTIONS 183W(α, α'γ), E=15 MeV; 183W(α, α'), E=13 MeV; measured Eγ, Iγ, γ(θ), σ(Eα'; θ). 183W levels deduced B(E2), B(M1), J, π, δ. Enriched targets.
doi: 10.1103/PhysRevC.20.2093
1978MC02 Nucl.Phys. A297, 51 (1978) F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson, Z.W.Grabowski Coulomb Excitation of Vibrational-Like States in 166-170Er NUCLEAR REACTIONS 166,168,170Er(α, α'γ), E=14 MeV; measured Iγ, Eγ, γ(θ). 166,168,170Er levels deduced B(E2), B(M1), B(E3), J, π, δ. Enriched targets.
doi: 10.1016/0375-9474(78)90198-7
1978SI12 ATOMKI Kozlem. 20, 207 (1978) N.C.Singhal, R.O.Sayer, J.H.Hamilton, A.V.Ramayya, W.T.Milner, R.L.Robinson, N.R.Johnson, G.J.Smith Recoil Distance Lifetime Measurements in 72Se NUCLEAR REACTIONS 58Ni(16O, 2p), E=44-46 MeV; measured DSA. 72Se yrast levels deduced T1/2, B(E2), rms deformation β2.
1977DA12 Nucl.Phys. A284, 484 (1977) W.K.Dagenhart, P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, S.Raman, W.K.Tuttle III Coulomb Excitation of 115Sn NUCLEAR REACTIONS 115Sn(α, α'γ), (α, α'), E=7.0-10.6 MeV; 115Sn(16O, 16O'γ), E=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening, Eα'. 115Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.
doi: 10.1016/0375-9474(77)90398-0
1977MC11 Nucl.Phys. A289, 253 (1977) F.K.McGowan, W.T.Milner, R.O.Sayer, R.L.Robinson, P.H.Stelson Coulomb Excitation of 182,184,186W and 166Er with 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(α, α'γ), E=15 MeV; 186W(16O, 16O'γ), E=42 MeV; 166Er(α, α'γ), E=13.5 MeV; 166Er(16O, 16O'γ), E=42 MeV; measured Iγ, Eγ, γ(θ), αγ-coin, 16Oγ-coin. 182W levels deduced J. 184W levels deduced B(EL), J. 186W levels deduced B(EL), J, quadrupole moment. 166Er deduced quadrupole moment. Enriched, natural targets.
doi: 10.1016/0375-9474(77)90532-2
1977MI11 Phys.Rev. C16, 1686 (1977) W.T.Milner, C.E.Bemis, Jr., F.K.McGowan Quadrupole and Hexadecapole Deformations in the Actinide Nuclei NUCLEAR STRUCTURE 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm; calculated model dependent β.
doi: 10.1103/PhysRevC.16.1686
1977WE10 Phys.Rev. C16, 2259 (1977) J.C.Wells, Jr., L.G.Fugate, R.O.Sayer, R.L.Robinson, H.J.Kim, W.T.Milner, G.J.Smith, R.M.Ronningen High-Spin States in 64Zn NUCLEAR REACTIONS 51V(16O, 2np), E=36-46 MeV; 59Co(7Li, 2n), E=18 MeV; measured Eγ, Iγ, γ(θ), DSA recoil distance. 64Zn deduced levels, J, π, T1/2, δ, γ-branching, B(E2).
doi: 10.1103/PhysRevC.16.2259
1976RO06 Phys.Rev. C13, 1922 (1976) R.L.Robinson, H.J.Kim, J.B.McGrory, G.J.Smith, W.T.Milner, R.O.Sayer, J.C.Wells, Jr., J.Lin High-Spin States in 42Ca NUCLEAR REACTIONS 28Si(16O, 2p), E=36-42 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), γ(θ). 42Ca deduced levels, J, π, δ, γ-branching, B(E2).
doi: 10.1103/PhysRevC.13.1922
1976TU02 Phys.Rev. C13, 1036 (1976) W.K.Tuttle III, P.H.Stelson, R.L.Robinson, W.T.Milner, F.K.McGowan, S.Raman, W.K.Dagenhart Coulomb Excitation of 113,115In NUCLEAR REACTIONS 113,115In(α, α'γ), E=9.4, 10, 10.6 MeV; 113,115In(16O, 16O'γ), E=42, 45 MeV; measured Coulomb excitation, DSA, Eγ, Iγ, γ(θ). 113,115In deduced levels, J, π, T1/2, B(E2), B(M1).
doi: 10.1103/PhysRevC.13.1036
1975KI05 Phys.Rev. C11, 1468 (1975) H.J.Kim, R.L.Robinson, W.T.Milner Lifetime of the 3.830-MeV State of 41Ca NUCLEAR REACTIONS 28Si(16O, n2pγ), E=40 MeV; measured nγ(t). 41Ca level deduced T1/2.
doi: 10.1103/PhysRevC.11.1468
1975KI07 Phys.Rev. C11, 2108 (1975) H.J.Kim, R.L.Robinson, W.T.Milner 44Ca Yrast Levels NUCLEAR REACTIONS 30Si(16O, 2pγ), E=30-40 MeV; measured Eγ, Iγ, γγ-coin. 44Ca deduced levels, J, π.
doi: 10.1103/PhysRevC.11.2108
1975LE22 Phys.Rev. C12, 1483 (1975) I.Y.Lee, J.X.Saladin, J.Holden, J.O'Brien, C.Baktash, C.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle Deformation Parameters of the Charge Distribution and the Optical Potential for Some Nuclei in and Near the Rare Earth Region NUCLEAR REACTIONS 154Sm(α, α'), E=11-19 MeV; 166Er(α, α'), E=12.5-19.5 MeV; 182W(α, α'), E=13-21 MeV; measured σ(Eα'). 168Er(α, α'), E=13-19 MeV; 184W(α, α'), E=12.5-19 MeV; 186W(α, α'), E=13.25-19 MeV; measured σ(Eα', θ). 154Sm, 166,168Er, 182,184,186W deduced M(E2), M(E4), charge deformations, optical potential deformations.
doi: 10.1103/PhysRevC.12.1483
1974MC15 Phys.Rev. C10, 1146 (1974) F.K.McGowan, C.E.Bemis, Jr., W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson Coulomb Excitation of Vibrational-Like States in the Even-A Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 236,238U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα'). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm levels deduced B(E2), B(E3). Enriched targets.
doi: 10.1103/PhysRevC.10.1146
1973BE40 Phys.Rev. C8, 1934 (1973) C.E.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle Interference between Direct Nuclear Reactions and Coulomb Excitation with Alpha Particles on 154Sm, 166Er, and 182W NUCLEAR REACTIONS 154Sm, 166Er, 182W(α, α), (α, α'), E=11-21 MeV; measured σ(E;Eα'). 154Sm, 166Er levels deduced E2, E4 matrix elements.
doi: 10.1103/PhysRevC.8.1934
1973BE44 Phys.Rev. C8, 1466 (1973) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, P.H.Stelson, R.L.Robinson E2 and E4 Transition Moments and Equilibrium Deformations in the Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 236U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-19 MeV; 238U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα', θ). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm deduced B(E2), B(E4), β.
doi: 10.1103/PhysRevC.8.1466
1973RA32 Phys.Lett. 47B, 19 (1973) S.Raman, R.L.Auble, W.T.Milner An E5 Transition in 123Te and E5 Transitions in General RADIOACTIVITY 123mTe; measured Eγ, Iγ, T1/2. 123Te levels deduced γ-hindrance, E5 transitions.
doi: 10.1016/0370-2693(73)90558-3
1972MI10 Priv.Comm. (July 1972)
1972RA14 Nucl.Phys. A184, 138 (1972) S.Raman, R.L.Auble, W.T.Milner, J.B.Ball, F.K.McGowan, P.H.Stelson, R.L.Robinson Nuclear Spectroscopy of 50Cr RADIOACTIVITY 50Mn; measured T1/2, Eγ, Iγ. NUCLEAR REACTIONS 50Cr(p, p'γ), E=8.4 MeV; measured Eγ, Iγ. 52Cr(p, t), E=31.4 MeV; measured σ(Et, θ). 50Cr(35Cl, 35Cl'γ), E=54 MeV; measured B(E2), Doppler shift attenuation. 50Cr deduced levels, J, π, γ-branching, T1/2.
doi: 10.1016/0375-9474(72)90449-6
1972RO27 Nucl.Phys. A193, 14 (1972) R.L.Robinson, F.K.McGowan, W.T.Milner, P.H.Stelson Coulomb Excitation of 81Br NUCLEAR REACTIONS 81Br(α, α'γ), E=2.5-8.2 MeV; 81Br(16O, 16O'γ), E=33 MeV; measured σ(E;Eγ, θ(γ), θ(γγ)), Iγ, Doppler broadening. 81Br deduced levels, J, π, B(E2), B(M1), T1/2.
doi: 10.1016/0375-9474(72)90231-X
1972ST16 Nucl.Phys. A190, 197 (1972) P.H.Stelson, W.T.Milner, F.K.McGowan, R.L.Robinson, S.Raman Coulomb Excitation of 117,119Sn NUCLEAR REACTIONS 117,119Sn(α, α'γ), 117,119Sn(16O, 16O'γ)Eα=10, 10.5, 11 MeV;E(16O)=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening. 117,119Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.
doi: 10.1016/0375-9474(72)90137-6
1971FO17 Phys.Rev.Lett. 27, 1232 (1971) J.L.C.Ford, Jr., P.H.Stelson, C.E.Bemis, Jr., F.K.McGowan, R.L.Robinson, W.T.Milner Precise Coulomb Excitation B(E2) Values for First 2+ States of the Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf(α, α'), E=17, 18 MeV; measured B(E2). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf deduced B(E2). 252Cf deduced level.
doi: 10.1103/PhysRevLett.27.1232
1971KI14 Nucl.Instrum.Methods 95, 429 (1971) Short Nuclear Lifetime Measurements via the Pulse Beam Delayed-Coincidence Technique NUCLEAR REACTIONS 113Cd(p, nγ), E approx 3.8 MeV; measured pγ-delay. 113In levels deduced T1/2.
doi: 10.1016/0029-554X(71)90541-6
1971MC14 Ann.Phys.(N.Y.) 63, 549 (1971) F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of 197Au and a Core-Excitation Analysis NUCLEAR REACTIONS 197Au(α, α'γ), E=9.94-14 MeV; 197Au(16O, 16O'γ), E=42-45 MeV; measured σ(E;Eγ, θ(γ)), γγ-coin. 197Au levels deduced B(E2), B(M1), γ-mixing, g. Coulomb excitation;core-excitation analysis.
doi: 10.1016/0003-4916(71)90028-5
1971MC21 Phys.Rev.Lett. 27, 1741 (1971) F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Equilibrium Quadrupole and Hexadecapole Deformations in 230Th and 238U NUCLEAR REACTIONS 230Th, 238U(α, α), (α, α'), E=17, 18 MeV; measured σ(Eα'). 230Th, 238U deduced B(EL), equilibrium deformation parameters.
doi: 10.1103/PhysRevLett.27.1741
1971MI08 Nucl.Phys. A177, 1 (1971) W.T.Milner, F.K.McGowan, R.L.Robinson, P.H.Stelson, R.O.Sayer Coulomb Excitation of 182,184,186W, 186,188,190,192Os and 192,194,196,198Pt with Protons, 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(p, p'γ), E=5 MeV;182,184,186W(α, α'γ), E=14, 15 MeV; 182,184,186W(16O, 16O'γ), E=45.5 MeV; 188,190,192Os(p, p'γ), E=4.56-5.08 MeV; 186Os(α, α'γ), E=3-5 MeV; 188,190,192Os(α, α'γ), E=15 MeV; 186,188,190,192Os(16O, 16O'γ), E=42, 45.1, 45.5 MeV; 192,194,196,198Pt(p, p'γ), E=4.5 MeV; 192,194,196,198Pt(16O, 16O'γ), E=43.75 MeV; measured Iγ, Eγ, (16O)(γ)-coin, 182,184,186W, 186,188,190,192Os, 192,196,194,198Pt deduced B(E2), B(M1), J. Enriched, natural targets.
doi: 10.1016/0375-9474(71)90161-8
1971RO09 Nucl.Phys. A166, 141 (1971) R.L.Robinson, W.T.Milner, F.K.McGowan, P.H.Stelson, M.A.Ludington E2/M1 Admixture of the 2'→2 Transition in 108Pd NUCLEAR REACTIONS 108Pd(α, α'γγ), Eα=10.1 MeV; measured γγ(θ). 108Pd transition deduced γ-mixing, B(E2), B(M1). Enriched target.
doi: 10.1016/0375-9474(71)90418-0
1970RO14 Nucl.Phys. A150, 225 (1970) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Coulomb Excitation of 107,109Ag NUCLEAR REACTIONS 107,109Ag(α, α'γ), E=10.0, 10.7 MeV; 107,109Ag(16O, 16O'γ), E=45.5 MeV; measured σ(Eγ, θ(γ)), γγ-triple correlation, Doppler broadening. 107,109Ag deduced levels, B(E2), B(M1), B(E1), T1/2, J, π, γ-mixing, γ-branching.
doi: 10.1016/0375-9474(70)90946-2
1970SA09 Phys.Rev. C1, 1525 (1970) R.O.Sayer, P.H.Stelson, F.K.McGowan, W.T.Milner, R.L.Robinson Multiple Coulomb Excitation of 152Sm, 166Er, and 172,174,176Yb NUCLEAR REACTIONS 152Sm, 166Er, 172,174,176Yb(α, α'γ), E=7, 8, 9, 10 MeV; 152Sm, 166Er, 172,174,176Yb(16O, 16O'γ), E=25-52 MeV; measured σ(E;Eα', Eγ), σ(E;E(16O'), Eγ). 152Sm, 166Er, 172,174,176Yb levels deduced B(E2).
doi: 10.1103/PhysRevC.1.1525
1970ST20 Phys.Rev. C2, 2015 (1970) P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner Static Quadrupole Moment of the First 2+ States of the Even Tin Nuclei NUCLEAR REACTIONS 112,116,118,120,122,124Sn(α, α'γ), E=10 MeV; 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=46 MeV; measured σ(Eα', Eγ), σ(E(16O'), Eγ). 112,116,118,120,122,124Sn levels deduced quadrupole moment, B(E2).
doi: 10.1103/PhysRevC.2.2015
1969MI07 Nucl.Phys. A129, 687 (1969) W.T.Milner, F.K.McGowan, P.H.Stelson, R.L.Robinson, R.O.Sayer Coulomb Excitation of the Even-A Cadmium Nuclei NUCLEAR REACTIONS 106,108,110,112,114,116Cd(p, p'γ), E=2.7, 3.0 MeV; 106,108,110,112,114,116Cd(α, α'γ), E=9-11 MeV; 106,108Cd(16O, 16O'γ), E=42-49 MeV; measured Iγ, Eγ, γγ-coin, γ(θ). 106,108,110,112,114,116Cd deduced levels, B(E2), B(M1), J. Enriched targets.
doi: 10.1016/0375-9474(69)90710-6
1969RO03 Nucl.Phys. A123, 193 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Gamma-Gamma Angular Correlations Following Coulomb Excitation NUCLEAR REACTIONS 107,109Ag, 110Pd, 117Sn(α, α'γ), E=9.5-10 MeV; 190,192Os(p, p'γ), E=4.5 MeV; measured γγ(θ). 107,109Ag, 110Pd, 117Sn, 190,192Os deduced levels, J, γ-mixing ratio. Enriched target.
doi: 10.1016/0375-9474(69)90899-9
1969RO05 Nucl.Phys. A124, 553 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Coulomb Excitation of 106,108,110Pd NUCLEAR REACTIONS 106,108,110Pd(α, α'γ), E=9-10 MeV; 106,108,110Pd(16O, 16O'γ), E=42-49 MeV, measured Iγ, Eγ, γγ-coin., γ(θ). 106,108,110Pd deduced levels B(E2), B(M1), T1/2, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90650-2
1968MC08 Nucl.Phys. A113, 529 (1968) F.K.McGowan, R.L.Robinson, P.H.Stelson, W.T.Milner Coulomb Excitation of States in the Even-Mass Ruthenium Nuclei with 16O and 4He Ions NUCLEAR REACTIONS 98,100,102,104Ru(16O, 16O'γ), E=42-49 MeV; 98,100,102,104Ru(α, α'γ), E=10 MeV; measured σ(Eγ, θ), γγ-coin; deduced B(E2), B(M1), J. Enriched targets.
doi: 10.1016/0375-9474(68)90161-9
1968ST14 Phys.Rev. 170, 1172 (1968) P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, R.O.Sayer Coulomb Excitation of the Even Tin Nuclei NUCLEAR STRUCTURE 112Sn, 118Sn, 116Sn, 120Sn, 122Sn, 124Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.1172
1967RO03 Nucl.Phys. A96, 6 (1967) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Low-Lying Levels of 79Br RADIOACTIVITY 79Kr [from 79Br(p, n), 78Kr(n, γ)]; measured Eγ, Iγ, γγ coin. 79Br deduced levels, B(E2), B(M1), T1/2, J, π, log ft. 79Br(α, α'γ), E = 2.5-7 MeV; 79Br(16O, 16O'γ), E = 36 MeV; measured Eγ, Iγ, γγ coin, γ(θ). Enriched target.
doi: 10.1016/0375-9474(67)90690-2
1967RO14 Nucl.Phys. A104, 401 (1967) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Coulomb Excitation of 75As NUCLEAR REACTIONS 75As(α, α'γ), E=3.5-8.1 MeV; 75As(16O, 16O'γ), E=36-38 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 75As deduced levels, B(E2), B(M1), T1/2, J, π.
doi: 10.1016/0375-9474(67)90564-7
1966MC18 Proc.Conf.Bases for Nucl.Spin-Parity Assignments, Gatlinburg, Tenn. (1966), N.B.Gove, R.L.Robinson, Eds., Academic Press, New York, p.222 (1966) F.K.McGowan, P.H.Stelson, R.L.Robinson, W.T.Milner, J.L.C.Ford, Jr. Coulomb Excitation of States in the Chromium Nuclei NUCLEAR REACTIONS 50,52,53,54Cr(16O, 16O'γ), E=33 MeV; measured σ(Eγ, θ). 50,52,53,54Cr deduced levels, J, π, B(E2), B(M1). Enriched targets.
1965RO09 Nucl.Phys. 74, 281 (1965) R.L.Robinson, P.H.Stelson, F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner Gamma Ray Energies Determined with a Lithium-Drifted Germanium Detector NUCLEAR REACTIONS 48Ti, 50Cr, 56Fe, 64,66,68,70Zn, 70,72,74,76Ge, 75As, 76,78,80,82Se(α, α'γ), 79Br, 94,96,98,100Mo, 96,100,104Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116,117,118,120,122,124Sn, 121,123Sb, 122,124,126,128,130Te, 195Pt(α, α'γ), E=6-9 MeV; measured Eγ. 77Se, 119Sn(α, α'γ), E=6-9 MeV; measured Eγ, Iγ. 18O(α, nγ), E=6-9 MeV; measured Eγ. 21Ne deduced level. Enriched targets. RADIOACTIVITY 7Be, 22Na, 51Cr, 54Mn, 60Co, 65Zn, 88Y, 137Cs, 198Au, 203Hg, 207Bi; measured Eγ. 102,106Rh; measured Eγ, Iγ.
doi: 10.1016/0029-5582(65)90082-9
1964MC03 Bull.Am.Phys.Soc.9, No.1, 107, KC5 (1964) F.K.McGowan, R.L.Robinson, P.H.Stelson, J.L.C.Ford, W.T.Milner Coulomb Excitation of Vibrational Triplet States and Octupole States in Even Cadmium Nuclei NUCLEAR STRUCTURE 114Cd, 116Cd, 112Cd, 110Cd; measured not abstracted; deduced nuclear properties.
1964MC10 ORNL-CPX-1 (1964) F.K.McGowan, W.T.Milner, H.J.Kim Nuclear Cross Sections for Charged-Particle Induced Reactions Mn, Fe, Co
1964MC18 ORNL-3582, p.107 (1964) F.K.McGowan, P.H.Stelson, R.L.Robinson, J.L.C.Ford, W.T.Milner Coulomb Excitation of Vibrational Triplet States and Octupole States in the Even Cadmium Nuclei NUCLEAR STRUCTURE 114Cd, 116Cd, 112Cd, 110Cd; measured not abstracted; deduced nuclear properties.
1964MC19 ORNL-CPX-2 (1964) F.K.McGowan, W.T.Milner, H.J.Kim Nuclear Cross Sections for Charged-Particle Induced Reactions Ni, Cu
1963RO27 WASH-1044, p.65 (1963) R.L.Robinson, F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, P.H.Stelson Coulomb Excitation NUCLEAR STRUCTURE 112Cd, 114Cd; measured not abstracted; deduced nuclear properties.
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