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NSR database version of April 11, 2024.

Search: Author = W.T.Milner

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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
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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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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
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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
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1994MC03      Nucl.Phys. A571, 569 (1994)

F.K.McGowan, W.T.Milner

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
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1993MC07      Nucl.Phys. A562, 241 (1993)

F.K.McGowan, W.T.Milner

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
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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
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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
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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
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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
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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, β22(sp), EWSR, intrinsic quadrupole moments.

doi: 10.1016/0092-640X(87)90016-7
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1986ER10      Phys.Lett. 181B, 52 (1986)

K.A.Erb, I.Y.Lee, W.T.Milner

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
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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
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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
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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
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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
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1981MC06      Phys.Rev. C23, 1926 (1981)

F.K.McGowan, W.T.Milner

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1972MI10      Priv.Comm. (July 1972)

W.T.Milner


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
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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
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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
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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
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1971KI14      Nucl.Instrum.Methods 95, 429 (1971)

H.J.Kim, W.T.Milner

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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