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Search: Author = R.A.Naumann

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2008BU14      Nucl.Phys. A809, 129 (2008)

D.G.Burke, P.E.Garrett, T.Qu, R.A.Naumann

Nuclear structure of 229, 231Th studied with the 230, 232Th(d, t) reactions

NUCLEAR REACTIONS 230,232Th(d, t), E=17 MeV; measured triton-spectra, σ(E, θ). 229,231Th deduced levels, J, π, bands. Enriched target, magnetic spectrograph. Quasi-particle configurations. DWBA analysis.

doi: 10.1016/j.nuclphysa.2008.06.009
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1656. Data from this article have been entered in the XUNDL database. For more information, click here.

1997BU03      Nucl.Phys. A612, 91 (1997)

D.G.Burke, W.Kurcewicz, G.Lovhoiden, M.J.G.Borge, M.Cronqvist, H.Gabelmann, H.Gietz, P.Hill, N.Kaffrell, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, J.Rogowski, G.L.Struble, T.F.Thorsteinsen, and the ISOLDE Collaboration

Search for Stable Octupole Deformation in 225Fr

RADIOACTIVITY 225Rn(β-) [from 232Th(p, 3n5p), mass separation]; measured Eγ, Iγ, I(ce), T1/2, γγ-, eγ-coin. 225Fr deduced levels, J, π, ICC, γ multipolarity, B(λ). Other data input.

NUCLEAR REACTIONS 226Ra(t, α), E=18 MeV; measured σ(Eα). 225Fr deduced levels, Q-value, ICC, γ-multipolarity, J, π, rotational bands, B(λ). Ge, Si(Li) detectors, mini-orange spectrometer, magnetic spectrograph, other data input.

doi: 10.1016/S0375-9474(96)00311-9
Citations: PlumX Metrics

1997KU20      Nucl.Phys. A621, 827 (1997)

W.Kurcewicz, I.S.Grant, K.Gulda, A.J.Aas, J.Billowes, M.J.G.Borge, D.G.Burke, P.A.Butler, J.F.C.Cocks, B.Fogelberg, S.J.Freeman, G.D.Jones, E.Hagebo, P.Hoff, J.Honsi, A.Lindroth, G.Lovhoiden, H.Mach, T.Martinez, R.A.Naumann, K.Nybo, G.Nyman, H.Ravn, B.Rubio, J.Simpson, A.G.Smith, J.F.Smith, K.Steffensen, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration

The Nuclear Structure of 227Fr

RADIOACTIVITY 227Rn(β-) [from 232Th(p, n5p), E=1 GeV]; measured Eγ, Iγ, I(ce), T1/2, βγγ(t), γγ-coin. 227Fr deduced levels, J, π, ICC, γ-multipolarity, rotational bands, B(λ). Ge, Si(Li), BGO, plastic, BaF2 detectors, mini-orange spectrometer.

doi: 10.1016/S0375-9474(97)00190-5
Citations: PlumX Metrics

1992BO05      Nucl.Phys. A539, 249 (1992)

M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration

On the Nuclear Structure of 229Ra

RADIOACTIVITY 229Fr(β-); measured T1/2, Eγ, Iγ, E X-ray, I X-ray, I(ce), γγ-coin. 229Ra deduced levels, J, π, γ-multipolarity, ICC, Nilsson assignments.

doi: 10.1016/0375-9474(92)90269-P
Citations: PlumX Metrics

1992GI08      Hyperfine Interactions 75, 189 (1992)

I.C.Girit, F.P.Calaprice, R.A.Naumann, D.Deptuck, M.M.Lowry

Search for Parity and Time Reversal Violations in Hindered Gamma-Decay

NUCLEAR REACTIONS 176Yb(α, 2n), E=35 MeV; measured Eγ, Iγ, γγ(θ), aligned residual nucleus, γ linear polarization.

RADIOACTIVITY 178mHf(IT); measured Eγ, Iγ, γγ(θ), aligned nuclei, γ linear polarization; deduced parity violation in comparison to 180mHf. New detector for P-symmetry tests.

doi: 10.1007/BF02398976
Citations: PlumX Metrics

1992HA15      Nucl.Instrum.Methods Phys.Res. A313, 237 (1992)

F.X.Hartmann, R.A.Naumann

High Temperature Gas Proportional Detector Techniques and Application to the Neutrino Mass Limit using 163Ho

RADIOACTIVITY 163Ho, 55Fe(EC); measured X-ray spectra; deduced electron neutrino mass limit. High temperature gas proportional detector, calorimetric technique, gaseous organometallic 163Ho sources.

doi: 10.1016/0168-9002(92)90102-A
Citations: PlumX Metrics

1992KU03      Nucl.Phys. A539, 451 (1992)

W.Kurcewicz, G.Lovhoiden, T.F.Thorsteinsen, M.J.G.Borge, D.G.Burke, M.Cronqvist, H.Gabelmann, H.Gietz, P.Hill, N.Kaffrell, R.A.Naumann, K.Nybo, G.Nyman, J.Rogowski, and the ISOLDE Collaboration

The Nuclear Structure of 223Fr

RADIOACTIVITY 223Rn(β-) [from 232Th(p, 5n5p), mass separation]; measured Eγ, Iγ, I(ce), γγ-coin. 223Fr deduced levels, ICC, γ-multipolarity, J, π, rotational bands, dipole moment. Ge, Si(Li) detectors, mini-orange spectrometer.

doi: 10.1016/0375-9474(92)90287-T
Citations: PlumX Metrics

1992NA21      Nucl.Instrum.Methods Phys.Res. B70, 80 (1992)

R.A.Naumann, F.W.Loeser, R.B.Vogelaar

The Princeton Separator, Past and Future

RADIOACTIVITY 194,196,198Tl(EC), (β+); measured I(ce). 140Xe(β-); 140Cs(β-); measured γ-spectra. 81Kr(EC); measured X-ray spectra; deduced log ft.

NUCLEAR REACTIONS 207Pb, 159Gd, 158Tb(p, d), E=29.9 MeV; measured σ(Ed).

doi: 10.1016/0168-583X(92)95913-C
Citations: PlumX Metrics

1990BU17      Phys.Rev. C42, R499 (1990)

D.G.Burke, P.E.Garrett, Q.Tao, R.A.Naumann

Additional Evidence for the Proposed Excited State at ≤ 5 eV in 229Th

NUCLEAR REACTIONS 230Th(d, t), E=17 MeV; measured σ(Et), σ(θ). 229Th deduced levels, L-values, spectroscopic strengths, Nilsson assignments. Magnetic spectrograph, enriched target. DWBA analysis.

doi: 10.1103/PhysRevC.42.R499
Citations: PlumX Metrics

1990NA22      Hyperfine Interactions 59, 113 (1990)


Electrical and Inertial Parameters for Th, U, Pu Isotopes

NUCLEAR MOMENTS 232Th, 233,234,235,238U, 239,240,242Pu; analyzed muonic X-ray hfs data. 233,234,235,238U, 239,240,242Pu deduced rms radii ratios relative to 232Th.

ATOMIC PHYSICS, Mesic-Atoms 232Th, 233,234,235,238U, 239,240,242Pu; analyzed muonic X-ray hfs data. 233,234,235,238U, 239,240,242Pu deduced rms radii ratios relative to 232Th.

doi: 10.1007/BF02401202
Citations: PlumX Metrics

1989AN02      Nucl.Phys. A491, 290 (1989)

E.Andersen, M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration

Measurements of Multipolarities in 225Ra

RADIOACTIVITY 225Fr(β-) [from Th, U(p, X)]; measured I(ce), γγ-, eγ-coin. 225Ra deduced levels, ICC, γ multipolarity, J, π. On-line mass separation, UC2, ThC2 targets, Ge, Si(Li) detectors, mini-orange spectrometer.

doi: 10.1016/0375-9474(89)90704-5
Citations: PlumX Metrics

1989HA05      Phys.Rev. C39, 1039 (1989); Erratum Phys.Rev. C40, 468 (1989)

F.X.Hartmann, Y.Y.Sharon, R.A.Naumann

Broken SU(3) Symmetry Applied to Rotational Nuclei: Cylindrical intrinsic states in the interacting boson model

NUCLEAR STRUCTURE 156Gd, 168Er, 168Yb; calculated levels, bandhead energies. Broken SU(3) symmetry.

doi: 10.1103/PhysRevC.39.1039
Citations: PlumX Metrics

1989MA28      Phys.Rev. C39, 2180 (1989)

L.G.Mann, R.G.Lanier, G.L.Struble, S.W.Yates, R.A.Naumann, R.T.Kouzes

148Gd(p, t)146Gd Reaction: Neutron states in 146Gd

NUCLEAR REACTIONS, ICPND 148Gd(p, t), E=34.6, 24.9 MeV; measured σ(θ), σ(Et); deduced total σ. 146Gd deduced levels, transfer L, partial σ. QDDD spectrometer, target from isotope separator. DWBA analysis, pairing vibrational model.

doi: 10.1103/PhysRevC.39.2180
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2675.

1988AX01      Phys.Lett. 210B, 249 (1988)

H.Axelsson, M.Cronqvist, A.De Rujula, P.G.Hansen, L.Johannsen, B.Jonson, R.A.Naumann, G.Nyman, J.W.Petersen, H.L.Ravn, K.Riisager, J.A.Scircle, and the ISOLDE Collaboration

Candidates for Electron-Neutrino Mass Measurements. The Case of 81Kr

RADIOACTIVITY 81Kr(EC) [from 81Rb-decay]; measured (X-ray)(X-ray)-coin, relative Iγ; deduced Q(EC), branching ratio, ν(e) mass relevance.

doi: 10.1016/0370-2693(88)90380-2
Citations: PlumX Metrics

1988MA18      Phys.Rev. C37, 1407 (1988)

H.E.Martz, R.K.Sheline, R.G.Lanier, R.W.Hoff, G.L.Struble, D.J.Decman, D.G.Burke, R.R.Chasman, R.A.Naumann

Octupole Deformation in 227Ac by Single-Proton Stripping Reactions: 226Ra(α, t)227Ac and 226Ra(3He, d)227Ac

NUCLEAR REACTIONS 226Ra(α, t), (3He, d), E=30 MeV; measured σ(θ). 227Ac deduced levels, J, π. Nilsson model reflection-symmetric and Leander model reflection-asymmetric calculations. Radioactive target.

doi: 10.1103/PhysRevC.37.1407
Citations: PlumX Metrics

1987BA85      Z.Phys. D7, 165 (1987)

M.Barboza-Flores, O.Redi, P.Schonberger, H.H.Stroke, R.A.Naumann

HFS and Isotope Shift in the Atomic Spectrum of 205Pb

RADIOACTIVITY 205Pb [from 204Pb+n]; measured hfs, isotope shift; deduced hyperfine constants. 205Pb deduced μ. Dispersive spectroscopy.

doi: 10.1007/BF01384583
Citations: PlumX Metrics

1987BO04      Nucl.Phys. A464, 189 (1987)

M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration

Measurements of Multipolarities in 227Ra as Tests of Evidence for Stable Octupole Deformation

RADIOACTIVITY 227Fr(β-) [from U(p, X)]; measured I(ce), γγ-, eγ-coin. 227Ra deduced levels, ICC, γ-multipolarity. Uranium carbide target, on-line mass separation, Ge, Si-Li detector, mini-orange spectrometer.

doi: 10.1016/0375-9474(87)90334-4
Citations: PlumX Metrics

1987LO06      Phys.Rev. C35, 1950 (1987)

M.M.Lowry, R.T.Kouzes, F.Loeser, A.B.McDonald, R.A.Naumann

Electron Capture Decay of 81mKr

RADIOACTIVITY 81mKr(EC) [from 81Rb(β++EC)-decay]; measured E X-ray, I X-ray, (ce)(X-ray)-coin; deduced log ft, solar neutrino capture rate reduction. 81Br deduced EC-branching ratio.

doi: 10.1103/PhysRevC.35.1950
Citations: PlumX Metrics

1987WH01      Phys.Rev. C35, 81 (1987)

D.H.White, H.G.Borner, R.W.Hoff, K.Schreckenbach, W.F.Davidson, T.von Egidy, D.D.Warner, P.Jeuch, G.Barreau, W.R.Kane, M.L.Stelts, R.E.Chrien, R.F.Casten, R.G.Lanier, R.W.Lougheed, R.T.Kouzes, R.A.Naumann, R.Dewberry

Nuclear Structure of 231Th from Neutron Capture and (d, p) Reaction Measurements

NUCLEAR REACTIONS 230Th(n, γ), E=thermal, 2 keV; 230Th(d, p), E=20 MeV; measured Eγ, Iγ, I(ce), σ(θp), σ(Ep). 231Th deduced levels, J, π, rotational bands, Nilsson assignments, K. Enriched target, curved crystal, Q3D spectrometer.

doi: 10.1103/PhysRevC.35.81
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0204.

1986BO35      Z.Phys. A325, 429 (1986)

M.J.G.Borge, D.G.Burke, F.Calaprice, O.C.Jonsson, G.Lovhoiden, R.A.Naumann, K.Nybo, G.Nyman, H.L.Ravn, T.F.Thorsteinsen, and the ISOLDE collaboration

New Isotope 227Rn and Revised Halflives for 223Rn and 226Rn

RADIOACTIVITY 223Rn(β-), (EC); 226Rn(β-); 227Rn(β-) [from Th(p, X), E=600 MeV]; measured Eγ, Iγ, I(ce), T1/2. 223Fr deduced γ transition energies, multipolarity. 4π plastic scintillation counter.

NUCLEAR REACTIONS Th(p, X)199Rn/200Rn/201Rn/202Rn/203Rn/204Rn/205Rn/206Rn/207Rn/208Rn/209Rn/210Rn/211Rn/218Rn/219Rn/220Rn/222Rn/223Rn/224Rn/225Rn/226Rn/227Rn/228Rn, E=600 MeV; measured production yields. On-line separator.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0835.

1986MA40      Phys.Rev. C34, 729 (1986)

L.G.Mann, R.G.Lanier, G.L.Struble, R.A.Naumann, R.T.Kouzes

Mass of 146Gd

NUCLEAR REACTIONS 148Gd(p, t), E=34.6 MeV; measured σ(Et); deduced Q. 146Gd deduced mass excess. QDDD spectrometer, isotope separated target.

doi: 10.1103/PhysRevC.34.729
Citations: PlumX Metrics

1986ZU01      Phys.Lett. 167B, 383 (1986)

J.D.Zumbro, R.A.Naumann, M.V.Hoehn, W.Reuter, E.B.Shera, C.E.Bemis, Jr., Y.Tanaka

E2 and E4 Deformations in 232Th and 239,240,242Pu

NUCLEAR MOMENTS 232Th, 239,240,242Pu; measured muonic X-ray data; deduced quadrupole, hexadecapole moments, charge parameters, rms radii. 239Pu deduced E2 martix elements. Adiabatic rotation model.

ATOMIC PHYSICS, Mesic-Atoms 232Th, 239,240,242Pu; measured muonic X-ray data.

doi: 10.1016/0370-2693(86)91285-2
Citations: PlumX Metrics

1985AL02      Phys.Rev. C31, 360 (1985); Erratum Phys.Rev. C32, 665 (1985)

T.Altzitzoglou, R.T.Kouzes, F.W.Loeser, M.M.Lowry, R.A.Naumann, R.E.Chrien

Measurement of the 158Tb Electron-Capture Q Value

NUCLEAR REACTIONS 158Tb, 207Pb, 158Gd(p, d), E=29.9 MeV; measured σ(Ed), Q. 158Tb deduced Q(EC). Radioactive 158Tb target, Q3D magnetic spectrometer.

doi: 10.1103/PhysRevC.31.360
Citations: PlumX Metrics

1985HA12      Phys.Rev. C31, 1594 (1985)

F.X.Hartmann, R.A.Naumann

Observation of N and M Orbital-Electron Capture in the Decay of 163Ho

RADIOACTIVITY 163Ho(EC) [from 162Er(n, γ)163Er(decay)]; measured N, M orbital EC capture ratio; deduced Q(EC), neutrino mass limits.

doi: 10.1103/PhysRevC.31.1594
Citations: PlumX Metrics

1985JO04      Phys.Lett. 161B, 75 (1985)

M.W.Johnson, E.B.Shera, M.V.Hoehn, R.A.Naumann, J.D.Zumbro, C.E.Bemis, Jr.

241Am and 243Am Charge Distributions from Muonic X-Ray Spectroscopy and the Quadrupole Moment of the 240Am Fission Isomer

NUCLEAR REACTIONS 241,243Am(μ-, X), E at rest; measured muonic E X-ray, I X-ray. 241,243Am deduced intrinsic quadrupole moment, Barrett radii. 240Am deduced fission isomer quadrupole moment. Optical isotope shift data input.

ATOMIC PHYSICS, Mesic-Atoms 241,243Am(μ, X), E at rest; measured muonic X-rays.

doi: 10.1016/0370-2693(85)90612-4
Citations: PlumX Metrics

1985WA10      Phys.Rev. C31, 1211 (1985)

E.K.Warburton, C.J.Lister, J.W.Olness, P.E.Haustein, S.K.Saha, D.E.Alburger, J.A.Becker, R.A.Dewberry, R.A.Naumann

High Spin States of 86Zr

RADIOACTIVITY 86Nb(β+), (EC) [from 58Ni(32S, n3p), E=130-150 MeV]; measured γγ-, βγ-coin, γ(θ), recoil, σ(E), DSA. 86Zr deduced levels, T1/2, J, π, γ-branching, B(E2).

NUCLEAR REACTIONS 60Ni(29Si, n2p), E=70-120 MeV; measured γγ-coin, γ(θ), recoil, σ(E), DSA. 58Ni(32S, n3p), E=130-150 MeV; measured γγ-, βγ-coin, σ(Eγ). 86Zr deduced levels, T1/2, J, π, γ-branching, B(E2).

doi: 10.1103/PhysRevC.31.1211
Citations: PlumX Metrics

1984ZU02      Phys.Rev.Lett. 53, 1888 (1984)

J.D.Zumbro, E.B.Shera, Y.Tanaka, C.E.Bemis, Jr., R.A.Naumann, M.V.Hoehn, W.Reuter, R.M.Steffen

E2 and E4 Deformations in 233,234,235,238U

NUCLEAR MOMENTS 233,234,235,238U; measured muonic X-rays. 234,238U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, rms radii. 233,235U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, B(E2).

ATOMIC PHYSICS, Mesic-Atoms 233,234,235,238U; measured muonic X-rays.

doi: 10.1103/PhysRevLett.53.1888
Citations: PlumX Metrics

1983BA32      Phys.Rev. C28, 337 (1983)

P.A.Baisden, D.H.Sisson, S.Niemeyer, B.Hudson, C.L.Bennett, R.A.Naumann

Measurement of the Half-Life of 163Ho

RADIOACTIVITY 163Ho(EC) [from 162Er(n, γ)163Er(EC-decay)]; measured T1/2; deduced Q(EC). Isotope dilution mass spectrometry.

doi: 10.1103/PhysRevC.28.337
Citations: PlumX Metrics

1983DE03      Phys.Rev. C27, 892 (1983)

R.A.Dewberry, R.T.Kouzes, R.A.Naumann

Mass of 104Cd

NUCLEAR REACTIONS 106Cd(p, t), E=34.6 MeV; measured Et, Q. 104Cd deduced mass excess. Q3D spectrograph.

doi: 10.1103/PhysRevC.27.892
Citations: PlumX Metrics

1983DE19      Nucl.Phys. A399, 1 (1983)

R.A.Dewberry, R.T.Kouzes, R.A.Naumann, R.G.Lanier, H.G.Borner, R.Hoff

The 249Bk(p, t)247Bk Reaction

NUCLEAR REACTIONS 249Bk(p, t), E=15 MeV; measured σ(Et, θ). 247Bk deduced levels, J, π, K.

doi: 10.1016/0375-9474(83)90591-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1319.

1983DE43      Phys.Rev. C28, 2259 (1983)

R.A.Dewberry, R.A.Naumann

Two-Quasiparticle Excited Neutron Levels in 180Ta

NUCLEAR STRUCTURE 180Ta; calculated levels, rotational band structure. Nilsson model, two-quasineutron excitation.

NUCLEAR REACTIONS 181Ta(d, t), E=17.4 MeV; measured σ(θ), σ(Et). 180Ta deduced levels, J, π, K, configurations. Q3D spectrometer. DWBA analysis.

doi: 10.1103/PhysRevC.28.2259
Citations: PlumX Metrics

1982HA49      Z.Phys. A308, 103 (1982)

F.J.Hartmann, R.Bergmann, H.Daniel, T.von Egidy, G.Fottner, R.A.Naumann, J.J.Reidy, W.Wilhelm

Muonic Coulomb Capture Ratios in Fluorides and Sulfides

ATOMIC PHYSICS, Mesic-Atoms B, Al, Ca, Fe, Zn, As, Sr, Mo, Ag, Cd, Sb, Ba, Pb, Ca, Na; measured muonic Coulomb capture ratios in flouorides, sulfides.

doi: 10.1007/BF01412998
Citations: PlumX Metrics

1982SA34      Phys.Rev. C26, 2654 (1982)

S.K.Saha, P.E.Haustein, D.E.Alburger, C.J.Lister, J.W.Olness, R.A.Dewberry, R.A.Naumann

Identification and Decay of 84Zr

NUCLEAR REACTIONS 58Ni(28Si, 2p), E=80-96 MeV; measured σ(Eγ) vs E; deduced evidence for 84Zr.

RADIOACTIVITY 84Zr(EC), (β+) [from 58Ni(28Si, 2p), E=92 MeV; 58Ni(29Si, n2p), E=96 MeV]; measured Eγ, Iγ, T1/2, γγ-, γ(X-ray)-coin; deduced T1/2. 84Y deduced transitions. Helium jet recoil transfer, Ge(Li), Ge detectors, enriched targets.

doi: 10.1103/PhysRevC.26.2654
Citations: PlumX Metrics

1981BE56      Phys.Lett. 107B, 19 (1981)

C.L.Bennett, A.L.Hallin, R.A.Naumann, P.T.Springer, M.S.Witherell, R.E.Chrien, P.A.Baisden, D.H.Sisson

The X-ray Spectrum following 163Ho M Electron Capture

RADIOACTIVITY 163Ho [from 162Er(n, γ)163Er(β-decay)]; measured E(X-ray), I(X-ray); deduced Q(EC) lower limit.

doi: 10.1016/0370-2693(81)91137-0
Citations: PlumX Metrics

1981GI01      Phys.Lett. B98, 29 (1981)

F.Girshick, K.Krien, R.A.Naumann, G.L.Struble, R.G.Lanier, L.G.Mann, J.A.Cizewski, E.R.Flynn, T.Nail, R.K.Sheline

The 176Lu(t, p)178Lu Reaction. The Influence of Shell Gaps and Blocking on L = 0 Strength

NUCLEAR REACTIONS 176Lu(t, p), E=17 MeV; measured σ(θ); deduced possible gap in Nilsson spectrum at N=108. 178Lu deduced levels, J, π, enhanced L=0 strength.

doi: 10.1016/0370-2693(81)90360-9
Citations: PlumX Metrics

1981KA36      Hyperfine Interactions 9, 289 (1981)

E.N.Kaufmann, R.S.Raghavan, P.Raghavan, E.J.Ansaldo, R.A.Naumann

The Sign and Magnitude of the EFG at Cd in Hf

RADIOACTIVITY 111Ag [from 111mPd decay]; measured βγ(θ, t) in Hf; deduced electric field gradient for Cd in Hf.

doi: 10.1007/BF01020933
Citations: PlumX Metrics

1980BE44      Phys.Rev. C22, 2245 (1980)

C.L.Bennett, M.M.Lowry, R.A.Naumann, F.Loeser, W.H.Moore

Feasibility of 81Br as a Solar Neutrino Detector

RADIOACTIVITY 81mKr [from Kr(p, n), E=22 MeV]; measured E(X-ray), I(X-ray), (X-ray)e-coin, anticoincidence; deduced log ft. 81Br deduced feasibility as solar neutrino detector.

doi: 10.1103/PhysRevC.22.2245
Citations: PlumX Metrics

1979VI12      Hyperfine Interactions 7, 247 (1979)

R.Vianden, E.N.Kaufmann, R.A.Naumann, G.Schmidt

The Quadrupole Interaction of 100Rh in Various Intermetallic Compounds of Palladium

RADIOACTIVITY 100Pd [from 103Rh(p, 4n), E=40 MeV, chemical separation]; measured γγ(θ, H, t). 100Rh level deduced quadrupole interaction frequencies in PdHg, Pd, Pb2, PbSb, PdTe.

doi: 10.1007/BF01021507
Citations: PlumX Metrics

1978DI10      Phys.Rev. C18, 2506 (1978)

L.E.Dinescu, D.Mueller, R.A.Naumann

Multiplet Structure in 203Pb

NUCLEAR REACTIONS 205Pb(p, t), E=35 MeV; measured σ(θ). 203Pb deduced levels, L, J, π. DWBA analysis. Radioactive target.

doi: 10.1103/PhysRevC.18.2506
Citations: PlumX Metrics

1978ST04      Phys.Rev.Lett. 40, 615 (1978)

G.L.Struble, R.G.Lanier, L.G.Mann, R.T.Kouzes, D.Mueller, R.A.Naumann, F.Girshick, I.C.Oelrich, W.H.Moore

(p, t) Reaction as a Probe for the Structure of Odd-Odd Nuclei: Levels In 174Lu

NUCLEAR REACTIONS 176Lu(p, t), E=34.1 MeV; measured σ(Et, θ). 174Lu deduced levels, population intensities, L.

doi: 10.1103/PhysRevLett.40.615
Citations: PlumX Metrics

1978ST09      Phys.Rev. C17, 1564 (1978)

G.L.Struble, R.G.Lanier, L.G.Mann, R.K.Sheline, R.T.Kouzes, W.H.Moore, D.Mueller, R.A.Naumann, I.C.Oelrich

Levels in 189Ir and 191Ir Observed in the (p, t) Reaction

NUCLEAR REACTIONS 191,193Ir(p, t), E=34.7 MeV; measured σ(Et, θ). 189,191Ir deduced levels, L, J, π. Enriched targets.

doi: 10.1103/PhysRevC.17.1564
Citations: PlumX Metrics

1977AN01      Phys.Rev. C15, 123 (1977)

R.E.Anderson, J.J.Kraushaar, I.C.Oelrich, R.M.DelVecchio, R.A.Naumann, E.R.Flynn, C.E.Moss

Excitation of Particle-Vibration Multiplets in the A = 110 Region by Two-Neutron Stripping Reactions

NUCLEAR REACTIONS 103Rh, 106,108Pd, 107,109Ag(t, p), E=17.0 MeV; measured σ(Ep, θ). 105Rh, 108,110Pd, 109,111Ag deduced levels, L, J, π, enhancement. Enriched targets, magnetic spectrograph, DWBA analysis, weak coupling model.

doi: 10.1103/PhysRevC.15.123
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1977KR02      Phys.Rev. C15, 1288 (1977)

K.Krien, I.C.Oelrich, R.M.DelVecchio, R.A.Naumann

108,106Pd(p, t) Reactions and the Core-Coupling Model

NUCLEAR REACTIONS 106,108Pd(p, t), E=30 MeV; measured σ(Et, θ). 104,106Pd deduced levels, L, J, π. Enriched targets.

doi: 10.1103/PhysRevC.15.1288
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1976OE02      Phys.Rev. C14, 563 (1976)

I.C.Oelrich, K.Krien, R.M.DelVecchio, R.A.Naumann

Evidence for Core-Coupled States in 87Y from a 89Y(p, t)87Y and 88Sr(p, t)86Sr Comparison

NUCLEAR REACTIONS 88Sr, 89Y(p, t), E=42 MeV; measured σ(Et, θ). 86Sr, 87Y deduced levels, J, π, L. Core-coupling model. Enriched targets.

doi: 10.1103/PhysRevC.14.563
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1976RA09      Phys.Rev. B13, 2835 (1976)

P.Raghavan, E.N.Kaufmann, R.S.Raghavan, E.J.Ansaldo, R.A.Naumann

Sign and Magnitude of the Quadrupole Interaction of 111Cd in Noncubic Metals: Universal Correlation of Ionic and Electronic Field Gradients

RADIOACTIVITY 111Ag; measured βγ(θ, H, t). 111Cd level deduced quadrupole interaction in non-cubic metals.

doi: 10.1103/PhysRevB.13.2835
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1975CA01      Nucl.Phys. A239, 83 (1975)

V.R.Casella, J.D.Knight, R.A.Naumann

E3 Isomers of 93Y and 101Ag

RADIOACTIVITY 93mY [from 94Zr(t, α)], 101mAg [from 102Pd(p, 2n)]; measured Eγ, T1/2. Enriched targets.

doi: 10.1016/0375-9474(75)91134-3
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1975DE27      Phys.Rev. C12, 845 (1975)

R.M.Del Vecchio, I.C.Oelrich, R.A.Naumann

Study of 105Ag and 107Ag with the (p, t) Reaction

NUCLEAR REACTIONS 107,109Ag(p, t), E=30 MeV; measured σ(Et, θ). 105,107Ag deduced levels, L, J, π.

doi: 10.1103/PhysRevC.12.845
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1975HU15      Phys.Rev. C12, 2013 (1975)

H.Hubel, K.Freitag, E.Schoeters, R.E.Silverans, L.Vanneste, R.A.Naumann

Magnetic Moment of the Iπ = 25/2- Isomer in 179Hf and Anomalous Orbital Proton g Factor

RADIOACTIVITY 177Lu, 179mHf; measured γ(θ) polarized nuclei, γ(θ, H); deduced g, δ, magnetic hyperfine interaction μH.

doi: 10.1103/PhysRevC.12.2013
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1975KA12      Phys.Rev.Lett. 34, 1558 (1975)

E.N.Kaufmann, P.Raghavan, R.S.Raghavan, E.J.Ansaldo, R.A.Naumann

Preferred Sites of Impurities Implanted in Be: Lattice Location and Quadrupole Interactions

RADIOACTIVITY 111In, 111Ag; measured βγ-, γγ-coin. 111Cd level deduced quadrupole interaction.

doi: 10.1103/PhysRevLett.34.1558
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1975ST02      Phys.Lett. 53B, 432 (1975)

L.L.Sterna, P.E.Haustein, E.J.Ansaldo, R.A.Naumann, T.E.Ward

The Radioactive Decay of 170Re

RADIOACTIVITY 170,172,174Re; measured Eγ, Iγ, γγ-coin. 170,172Re; measured T1/2. 170Re deduced EC+β+ branching. 170W deduced levels.

doi: 10.1016/0370-2693(75)90210-5
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1974CU03      Phys.Rev. C10, 739 (1974)

J.B.Cumming, P.E.Haustein, R.W.Stoenner, L.Mausner, R.A.Naumann

Spallation of Cu by 3.9-GeV 14N Ions and 3.9-GeV Protons

NUCLEAR REACTIONS 63,65Cu(14N, spallation), (p, spallation), E=3.9 GeV; measured relative yields A=3-76, deduced charge dispersion.

doi: 10.1103/PhysRevC.10.739
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0542.

1973DJ01      Phys.Rev. C8, 323 (1973)

F.Djadali, K.Krien, R.A.Naumann, E.H.Spejewski

Isomeric States in Light Even Pb Isotopes

NUCLEAR REACTIONS 198Hg(α, xnγ), E=40 MeV; 198,200,202Hg(3He, xnγ), E=65 MeV; measured Eγ, Iγ, αγ(t), 3Heγ(t), γγ(t). 194,196,198,200Pb levels deduced T1/2.

doi: 10.1103/PhysRevC.8.323
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1973KR10      Phys.Rev. C7, 2484 (1973)

K.Krien, F.Djadali, R.A.Naumann, H.Hubel, E.H.Spejewski

Spectroscopic Investigation of Even-Even Neutron-Deficient Gd Isotopes

RADIOACTIVITY 148,150Tb; measured Eγ, Iγ. 148,150Gd deduced levels.

NUCLEAR REACTIONS 144,148Sm(α, 2nγ), E=30 MeV; 148Sm(α, 4nγ), E=48 MeV; measured Eγ, Iγ, Iγ(θ), γγ-coin, αγ(t). 146,148,150Gd deduced levels, T1/2, γ-branching, J, π.

doi: 10.1103/PhysRevC.7.2484
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1973KR12      Nucl.Phys. A209, 572 (1973)

K.Krien, R.A.Naumann, J.O.Rasmussen, I.Rezanka

High-Spin States in 155Dy and 154Dy from (12C, xnγ) Studies

NUCLEAR REACTIONS 146Nd(12C, 3nγ), E=57-109 MeV; 146Nd(12C, 4nγ), E=57-109 MeV; measured Eγ, Iγ(θ), γγ-coin. Enriched Nd target. 155Dy, 154Dy deduced levels, J, π, K.

doi: 10.1016/0375-9474(73)90847-6
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1973RA35      Phys.Rev. B7, 4132 (1973)

R.S.Raghavan, P.Raghavan, E.N.Kaufmann, K.Krien, R.A.Naumann

Time-Differential-Perturbed-Angular-Correlation Measurement of the Hyperfine Field at Hg in Iron

RADIOACTIVITY 199Tl; measured γγ(θ, H, t). 199Hg level deduced g.

NUCLEAR REACTIONS 198,200,202,204Hg(X, X'γ), E not given; measured nothing, analyzed IMPAC results. 198,200,202,204Hg deduced g (2+ states), hyperfine field at Hg in Fe.

doi: 10.1103/PhysRevB.7.4132
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1972HO09      Nucl.Phys. A184, 497 (1972)

P.K.Hopke, H.Hubel, R.A.Naumann, E.H.Spejewski, A.T.Strigachev

The Decay of 195mPb and 197mPb

RADIOACTIVITY 195Pb, 197Pb[from 238U(p, spallation)]; measured Eγ, Iγ, I(ce), γγ-coin; deduced J, π, log ft. 195,197Tl deduced levels, J, π, ICC, γ-multipolarity.

doi: 10.1016/0375-9474(72)90424-1
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1972KR08      Phys.Rev. C5, 1751 (1972)

K.Krien, E.H.Spejewski, R.A.Naumann, H.Hubel

Properties of Levels in 198Pb and 200Pb

RADIOACTIVITY 198,200Bi; measured Eγ, Iγ, I(ce), Xγ-, γγ-delay. 198,200Pb deduced levels, J, π, T1/2, ICC, γ-multipolarity.

doi: 10.1103/PhysRevC.5.1751
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1972KR28      Phys.Rev. C6, 1847 (1972)

K.Krien, E.H.Spejewski, R.A.Naumann, H.Hubel

Electron-Capture Decay of 105mAg

RADIOACTIVITY 105mAg; measured Eγ, Iγ; deduced log ft, EC branching ratio. 105Pd deduced levels, J, π.

doi: 10.1103/PhysRevC.6.1847
Citations: PlumX Metrics

1971HO17      Phys.Rev. C4, 606 (1971)

P.K.Hopke, R.A.Naumann

193Pt L-Electron-Capture Half-Life

RADIOACTIVITY 193Pt; measured T1/2(EC); deduced log ft.

doi: 10.1103/PhysRevC.4.606
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1971HU02      Phys.Rev. C3, 756 (1971)

H.Hubel, R.A.Naumann, E.H.Spejewski

Levels in 184Pt, 186Pt, and 188Pt

RADIOACTIVITY 184Hg, 184Au; measured Eγ, Iγ, γγ-coin. 186Hg, 186Au; measured Eγ, Iγ, I(ce), γγ-coin. 188Hg, 188Au; measured Eγ, Iγ, I(ce), γγ-coin. 184Pt deduced levels, J, π, γ-branching. 186,188Pt deduced levels, ICC, γ-multipolarity, J, π, γ-branching.

doi: 10.1103/PhysRevC.3.756
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1971HU14      Phys.Rev. C4, 2272 (1971); Erratum Phys.Rev. C5, 1438 (1972)

H.Hubel, R.A.Naumann, E.H.Spejewski

Decay of a Three-Quasiparticle State in 177Ta

NUCLEAR REACTIONS 175,176Lu(α, xnγ), E=24-48 MeV; measured Eγ, Iγ, αγ-delay. 177mTa deduced T1/2, J, π, γ-mixing.

doi: 10.1103/PhysRevC.4.2272
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1971SP03      Priv.Comm. (April 1971)

E.H.Spejewski, R.A.Naumann

1970DI11      Nucl.Phys. A155, 209 (1970)

F.S.Dietrich, B.Herskind, R.A.Naumann, R.G.Stokstad

Hole-Vibration Coupling in 115In

NUCLEAR REACTIONS 115In(d, d'), E=12 MeV; measured σ(Ed', θ). 115In(16O, 16O'γ), E=41-55 MeV; measured σ(E;E(16O'), Eγ). 115In deduced levels, J, π, B(E2), branching ratios. Natural targets.

doi: 10.1016/0375-9474(70)90087-4
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1970HA18      Nucl.Phys. A148, 249 (1970)

P.G.Hansen, H.L.Nielsen, K.Wilsky, M.Alpsten, M.Finger, A.Lindahl, R.A.Naumann, O.B.Nielsen

Studies of the α-Active Isotopes of Mercury, Gold, and Platinum

RADIOACTIVITY 179,180,181,182,183,184,185,186,187Hg[from Pb(p, X)]; 181,182,183,184,185Au, 175,176,177,178,179Pt[from Hg decay]; measured T1/2, Eα, Iα, αγ-coin; deduced Qα, α-branching, T1/2(α). 177,178,180,181,183Pt, 174Os deduced levels. Si surface-barrier detector, NaI(Tl)-Ge(Li) coin.

doi: 10.1016/0375-9474(70)90622-6
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1970HO15      Nucl.Phys. A149, 63 (1970)

P.K.Hopke, R.A.Naumann, E.H.Spejewski

Decay of 205At

RADIOACTIVITY 205At[from proton spallation of uranium]; measured Eγ, I(ce), K/(L+M); deduced log ft. 205Po deduced level, J, π. 205At deduced J, π.

doi: 10.1016/0375-9474(70)90379-9
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1970HU04      Phys.Rev. C1, 1845 (1970)

H.Hubel, R.A.Naumann, M.L.Andersen, J.S.Larsen, O.B.Nielsen, N.O.R.Poulsen

New High-Spin Isomer 179m2Hf and Intraband Branchings in the Ground-State Rotational Sequence of 179Hf

RADIOACTIVITY 179mHf[from 176Yb(α, n)]; measured Eγ, Iγ, T1/2, γγ-coin. 179Hf deduced high-spin isomer, levels, J, π, gR, gK, α(K), γ-multipolarity.

doi: 10.1103/PhysRevC.1.1845
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1970HU15      Phys.Rev. C2, 1447 (1970)

H.Hubel, R.A.Naumann, P.K.Hopke

Isomeric Transitions in 29-Day 179m2Hf

RADIOACTIVITY 179mHf; measured E(ce), I(ce). 179mHf levels deduced ICC, J, π, γ-multipolarity.

doi: 10.1103/PhysRevC.2.1447
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1969HA03      Phys.Lett. 28B, 415 (1969); Erratum Phys.Lett. 28B, 663 (1969)

P.G.Hansen, P.Hornshoj, H.L.Nielsen, K.Wilsky, H.Kugler, G.Astner, E.Hagebo, J.Hudis, A.Kjelberg, F.Munnich, P.Patzelt, M.Alpsten, G.Andersson, A.Appelqvist, B.Bengtsson, R.A.Naumann, O.B.Nielsen, E.Beck, R.Foucher, J.P.Husson, J.Jastrzebski, A.Johnson, J.Alstad, T.Jahnsen, A.C.Pappas, T.Tunaal, R.Henck, P.Siffert, G.Rudstam

Decay Characteristics of Short-Lived Radio-Nuclides Studied by On-Line Isotope Separator Techniques

RADIOACTIVITY 43Ar, 101Cd, 109Sn, 115I, 115Xe, 205,225,226Rn, 224,225,226Fr; measured T1/2. 75Kr, 119I, 119Xe, 186Pt, 186,188Au, 187,188Hg; measured Eγ. 198,200,202Po; measured Iα. 102,103Cd, 116,117,118I, 116,117,118Xe, 184Pt, 184Au; measured T1/2, Eγ. 79,81Kr, 125,127Xe; measured T1/2, Eγ, I(ce). 103Ag; measured T1/2, Eγ, I(ce), γγ-delay. 187,189,191Pt, 189Au, 206Hg; measured Eγ, γγ-delay. 181Hg; measured T1/2, Eα. 182,183,185Hg; measured T1/2, Eα, Iα. 184,186Hg; measured T1/2, Eα, Iα, Eγ. 202,204,206Rn; measured T1/2, Iα. 103Pd, 187,189,191Ir, 189Pt, 206Tl deduced levels, T1/2.

doi: 10.1016/0370-2693(69)90337-2
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1969HO03      Phys.Rev. 177, 1802 (1969)

P.K.Hopke, R.A.Naumann, E.H.Spejewski

Spin of the 1029-keV Level in Hg200

RADIOACTIVITY 200Tl [from Pb(3-BeV p)]; measured Eγ, Iγ. 200Hg level deduced J, π, ICC. Ge(Li) detector.

doi: 10.1103/PhysRev.177.1802
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1969HO14      Phys.Rev. 185, 1565 (1969)

P.K.Hopke, R.A.Naumann

Decay of Pt193

RADIOACTIVITY 193Pt; measured T1/2, internal bremstrahlung endpoint; deduced Q(EC).

doi: 10.1103/PhysRev.185.1565
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1969HO36      Phys.Rev. 187, 1704 (1969)

P.K.Hopke, R.A.Naumann, E.H.Spejewski, A.T.Strigachev

E3 Isomer in Ag105

RADIOACTIVITY 105mAg; measured T1/2, Eγ, Iγ. 105Ag; deduced J, π. 105Pd; deduced log ft, EC-branching.

doi: 10.1103/PhysRev.187.1704
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1969HO37      Phys.Rev. 187, 1709 (1969); Supersedes PPAR-15

P.K.Hopke, R.A.Naumann, E.H.Spejewski

Levels in Bi203, Bi205, and Bi207

RADIOACTIVITY 203,205,207Po; measured Eγ, Iγ, γγ-coin, I(ce); deduced log ft, Q. 203,205,207Bi deduced levels, J, π, ICC, γ-multipolarities.

doi: 10.1103/PhysRev.187.1709
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1969NA10      Nucl.Phys. A137, 689 (1969)

R.A.Naumann, R.F.Petry, J.S.Evans

Decay of 188Au and 190Au

RADIOACTIVITY 188,190Au[from spallation of Pb]; measured Eγ, Iγ, γγ-coin., ceγ-coin. 188,190Pt deduced levels. 190Hg; measured T1/2.

doi: 10.1016/0375-9474(69)90102-X
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1968AB01      Nucl.Phys. A106, 225 (1968)

A.Abdul-Malek, R.A.Naumann

Levels in 134Ba Populated by the Decay of 134Cs

RADIOACTIVITY 134Cs[from 133Cs(n, γ)]; measured Eγ, Iγ, I(ce), γγ-coin. 134Ba deduced levels, J, π, ICC. Ge(Li) detector.

doi: 10.1016/0375-9474(67)90841-X
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1968AB02      Nucl.Phys. A108, 401 (1968)

A.Abdul-Malek, R.A.Naumann

Energy Levels in Some Doubly Even Barium Isotopes

RADIOACTIVITY 134La[from 134Ce(EC)];measured T1/2, Eγ, Iγ, γγ-coin. 132La[from 132Ce(EC)];measured Eγ, Iγ, I(ce), γγ-, γce-coin. 132,133Ce[from La(p, xn), Pb(p, F)]; measured Eγ, I(ce). 130Ce, 130La; measured Eγ. 130,132,134Ba, 132La deduced levels. Ge(Li) detector, mass-separated 130,132,133,134Ce sources.

doi: 10.1016/0375-9474(68)90099-7
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1968AB03      Phys.Rev. 166, 1194 (1968)

A.Abdul-Malek, R.A.Naumann

Energy Levels of La135

NUCLEAR STRUCTURE 135Ce; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.166.1194
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1968AL06      Phys.Rev. 167, 1105 (1968)

T.Alvager, R.A.Naumann, R.F.Petry, G.Sidenius, T.D.Thomas

On-Line Studies of Mass-Separated Xenon Fission Products

NUCLEAR STRUCTURE 138Cs, 139Ba, 138Xe, 139Xe, 139Cs, 137Xe, 140Xe, 140Ba, 140Cs, 141La, 141Cs, 141Xe, 140La, 141Ba, 142Xe, 142La, 142Cs, 142Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.167.1105
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1968BO22      Nucl.Phys. A115, 14 (1968)

J.Borggreen, R.A.Naumann

M2 Isomer in 199Au

RADIOACTIVITY 199mAu [from 198Pt(d, n)]; measured T1/2, Eγ. 199Au deduced levels, γ-multipolarity, mixing ratio. Enriched target.

doi: 10.1016/0375-9474(68)90638-6
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1968GR01      Nucl.Phys. A106, 193 (1968)

B.Greenebaum, A.D.Jackson, Jr., R.A.Naumann

Measurement of a Spin 2 State in 102Ag and the Decay of 102Ag

RADIOACTIVITY 102Ag[from 102Pd(p, n)]; measured Eγ, Iγ, T1/2. 102Pd deduced levels. Isotope-separated source, Ge(Li) detector. 102Ag measured J.

doi: 10.1016/0375-9474(67)90837-8
Citations: PlumX Metrics

1968HO17      Phys.Rev. 171, 1290 (1968)

P.K.Hopke, J.S.Evans, R.A.Naumann

Decay of Ho163

RADIOACTIVITY 163Ho; measured T1/2, M/L EC ratio; deduced Qβ.

doi: 10.1103/PhysRev.171.1290
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1968NA14      Bull. Am. Phys. Soc. 13, No. 11, 1469, FE16 (1968)

R.A.Naumann, P.K.Hopke

Decay of Pt193

NUCLEAR STRUCTURE 193Pt; measured not abstracted; deduced nuclear properties.

1968PE13      Phys.Rev. 174, 1441 (1968)

R.F.Petry, R.A.Naumann, J.S.Evans

Levels in Even-Even Hg192, Hg194, Hg196, and Hg198

RADIOACTIVITY 192,194,196,198Tl; measured Eγ, Iγ, I(ce), ceγ-, γγ-coin, T1/2. 192,194,196,198Hg deduced levels, J, π, ICC, γ-multipolarity, γ-mixing.

doi: 10.1103/PhysRev.174.1441
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1967CO26      Nucl.Phys. A104, 213 (1967)

T.W.Conlon, R.A.Naumann, A.L.McCarthy

Hindered E1 transitions in 159Dy, 165Tm, 172Lu, 173Lu and 180W

RADIOACTIVITY 159Dy, 165Tm, 172,173Lu, 180W [from (p, xn) reactions]; measured T1/2, Eγ, Iγ, I(ce); deduced levels, multipolarities, K, J, π. Ge(Li) detector. 159Tb, 173Yb(p, n); 166Er, 173Yb, 181Ta(p, 2n), E=5-17.5 MeV; measured σ(E; Eγ), pγ-delay. Natural, enriched targets.

doi: 10.1016/0375-9474(67)90765-8
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1967NA02      Nucl.Phys. A94, 151(1967)

R.A.Naumann, R.F.Petry, J.S.Evans

The Half-Life and Decay of 189Au

RADIOACTIVITY 189Hg [from spallation of Pb]; measured T1/2. 189Au, measured T1/2, Eγ, Iγ. 189Pt deduced levels.

doi: 10.1016/0375-9474(67)90815-9
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1967NA08      Phys.Rev. 160, 1035 (1967)

R.A.Naumann, P.K.Hopke

Decay of Terbium-157

NUCLEAR STRUCTURE 157Tb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.1035
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1967NA14      Ark.Fys. 36, 177 (1967)

R.A.Naumann, R.F.Petry, J.S.Evans

Nuclear Spectroscopy of Light Platinum and Mercury Isotopes

NUCLEAR STRUCTURE 196Tl, 198Tl, 194Tl, 188Au, 192Tl; measured not abstracted; deduced nuclear properties.

1966JA12      Phys.Rev. 151, 956 (1966)

A.D.Jackson, Jr., J.S.Evans, R.A.Naumann, J.D.McCullen

Decay of Ag103

NUCLEAR STRUCTURE 103Ag; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.151.956
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1966NA01      Bull.Am.Phys.Soc. 11, No.3, 408, KB5 (1966); and Oral Report

R.A.Naumann, R.F.Petry, J.S.Evans

Identification and Half-Life of Au189

NUCLEAR STRUCTURE 189Au, 189Hg; measured not abstracted; deduced nuclear properties.

1965EV02      Bull.Am.Phys.Soc. 10, No.1, 81, GC3 (1965)

J.S.Evans, R.A.Naumann

Decay of Pd100

NUCLEAR STRUCTURE 100Pd; measured not abstracted; deduced nuclear properties.

1965EV04      Phys.Rev. 138, B9 (1965)

J.S.Evans, E.Kashy, R.A.Naumann, R.F.Petry

Levels in Rh101 Populated by the Decay of Pd101

NUCLEAR STRUCTURE 101Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B9
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1965EV05      Phys.Rev. 138, B1017 (1965); Erratum Phys.Rev. 139, AB4 (1965)

J.S.Evans, R.A.Naumann

Decay of Pd100 to Odd-Odd Rh100

NUCLEAR STRUCTURE 100Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B1017
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1965EV06      Phys.Rev. 140, B559 (1965)

J.S.Evans, R.A.Naumann

Decay of Rh101m and Rh101g

NUCLEAR STRUCTURE 101Rh; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B559
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1965MA34      Phys.Rev. 140, B264 (1965)

E.Matthias, D.A.Shirley, J.S.Evans, R.A.Naumann

Half-Life and g Factor of the 75-keV Level of Rh100

NUCLEAR STRUCTURE 100Rh, 100Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B264
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1965PE02      Bull.Am.Phys.Soc. 10, No.1, 82, GC4 (1965)

R.F.Petry, J.S.Evans, E.Kashy, R.A.Naumann

Levels in Rh101 Populated by the Decay of Pd101

NUCLEAR STRUCTURE 101Pd; measured not abstracted; deduced nuclear properties.

1964LE07      Phys.Rev. 134, B322 (1964)

H.R.Lewis, Jr., R.A.Naumann, J.M.Prospero, D.Thomas

Study of the Pt189 → Ir189 → Os189 Decay Chain

NUCLEAR STRUCTURE 189Ir, 189Pt; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.B322
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1964WI01      Bull.Am.Phys.Soc. 9, No.1, 18, BB13 (1964)

D.C.Williams, R.A.Naumann

Decay of Os194

NUCLEAR STRUCTURE 194Os; measured not abstracted; deduced nuclear properties.

1964WI07      Phys.Rev. 135, B289 (1964)

D.C.Williams, R.A.Naumann

Decay of Os194

NUCLEAR STRUCTURE 194Os; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.135.B289
Citations: PlumX Metrics

1962GR02      Can.J.Phys. 40, 296 (1962)

R.L.Graham, J.S.Geiger, R.A.Naumann, J.M.Prospero

Evidence for a 789.99-keV Level in Os188

NUCLEAR STRUCTURE 188Ir; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p62-029
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1962NA01      Bull.Am.Phys.Soc. 7, No.1, 34, J9 (1962)

R.A.Naumann, O.B.Nielsen, O.Skilbreid

Radioactive Decay of Terbium 157 and 158

NUCLEAR STRUCTURE 158Tb, 157Tb; measured not abstracted; deduced nuclear properties.

1961DI01      Bull.Am.Phys.Soc. 6, No.1, 73, XA12 (1961)

R.M.Diamond, J.M.Hollander, D.J.Horen, R.A.Naumann

Identification of Neutron-Deficient Irdium Isotopes: Ir182, Ir183, and Ir184

NUCLEAR STRUCTURE 184Ir, 183Ir, 182Ir; measured not abstracted; deduced nuclear properties.

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