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NSR database version of May 30, 2024.

Search: Author = J.L.Adams

Found 18 matches.

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2002NI10      Phys.Rev.Lett. 89, 039901 (2002); see also 1999Ni03

V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk

Editorial Note: Observation of Superheavy Nuclei Produced in the Reaction of 86Kr with 208Pb

doi: 10.1103/PhysRevLett.89.039901
Citations: PlumX Metrics


2002SH02      Phys.Rev. C65, 024612 (2002)

D.A.Shaughnessy, K.E.Gregorich, J.L.Adams, M.R.Lane, C.A.Laue, D.M.Lee, C.A.McGrath, V.Ninov, J.B.Patin, D.A.Strellis, E.R.Sylwester, P.A.Wilk, D.C.Hoffman

Electron-Capture Delayed Fission Properties of 244Es

RADIOACTIVITY 244Es(EC) [from 237Np(12C, 5n)]; measured EC-delayed fission T1/2, Eα, fission fragment energies, mass distribution; deduced delayed fission probability.

NUCLEAR REACTIONS 237Np(12C, 5n), E=81 MeV; measured σ.

doi: 10.1103/PhysRevC.65.024612
Citations: PlumX Metrics


2000LA25      Phys.Rev. C61, 067603 (2000)

C.A.Laue, K.E.Gregorich, R.Sudowe, J.L.Adams, M.R.Lane, D.M.Lee, C.A.McGrath, D.A.Shaughnessy, D.A.Strellis, E.R.Sylwester, P.A.Wilk, D.C.Hoffman

Half-Life of 232Pu and Excitation Function for the 233U (3He, 4n)232Pu Reaction

NUCLEAR REACTIONS 233U(3He, 4n), E=28-47 MeV; measured excitation function.

RADIOACTIVITY 232Pu(α) [from 233U(3He, 4n)]; measured T1/2.

doi: 10.1103/PhysRevC.61.067603
Citations: PlumX Metrics


2000SH10      Phys.Rev. C61, 044609 (2000)

D.A.Shaughnessy, J.L.Adams, K.E.Gregorich, M.R.Lane, C.A.Laue, D.M.Lee, C.A.McGrath, J.B.Patin, D.A.Strellis, E.R.Sylwester, P.A.Wilk, D.C.Hoffman

Electron-Capture Delayed Fission Properties of 242Es

RADIOACTIVITY 242Es(EC), (α) [from 233U(14N, 5n)]; measured ec-delayed fission T1/2, fragment mass yields, total kinetic energies; deduced delayed fission probability.

doi: 10.1103/PhysRevC.61.044609
Citations: PlumX Metrics


2000SY01      Radiochim.Acta 88, 837 (2000)

E.R.Sylwester, K.E.Gregorich, D.M.Lee, B.Kadkhodayan, A.Turler, J.L.Adams, C.D.Kacher, M.R.Lane, C.A.Laue, C.A.McGrath, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk, D.C.Hoffman

On-line gas chromatographic studies of Rf, Zr, and Hf bromides

RADIOACTIVITY 98Zr(β-);162Hf(EC); measured Eγ, Iγ. 261Rf(α); measured Eα, Iα, half-life.


2000WI15      Phys.Rev.Lett. 85, 2697 (2000)

P.A.Wilk, K.E.Gregorich, A.Turler, C.A.Laue, R.Eichler, V.Ninov, J.L.Adams, U.W.Kirbach, M.R.Lane, D.M.Lee, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, H.Nitsche, D.C.Hoffman

Evidence for New Isotopes of Element 107: 266Bh and 267Bh

NUCLEAR REACTIONS 249Bk(22Ne, 4n), (22Ne, 5n), E ≈ 117, 123 MeV; measured α spectra, αα-coin following residual nucleus decay; deduced production σ.

RADIOACTIVITY 266,267Bh(α) [from 249Bk(22Ne, xn)]; measured Eα, T1/2.

doi: 10.1103/PhysRevLett.85.2697
Citations: PlumX Metrics


1999LA14      Phys.Rev. C59, 3086 (1999)

C.A.Laue, K.E.Gregorich, R.Sudowe, M.B.Hendricks, J.L.Adams, M.R.Lane, D.M.Lee, C.A.McGrath, D.A.Shaughnessy, D.A.Strellis, E.R.Sylwester, P.A.Wilk, D.C.Hoffman

New Plutonium Isotope: 231Pu

NUCLEAR REACTIONS 233U(3He, 5n), E=42-47 MeV; measured αα-coin following residual nucleus decay; deduced evidence for 231Pu. Gas transport, chemical separation.

RADIOACTIVITY 231Pu(α), (EC); measured Eα, T1/2, branching ratio; deduced logft, Q(α).

doi: 10.1103/PhysRevC.59.3086
Citations: PlumX Metrics


1999NI03      Phys.Rev.Lett. 83, 1104 (1999); Erratum Phys.Rev.Lett. 89, 039901 (2002); see also 2002GrZZ

V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk

Observation of Superheavy Nuclei Produced in the Reaction of 86Kr with 208Pb

NUCLEAR REACTIONS 208Pb(86Kr, n), E=449 MeV; measured α-spectra, (recoil)α-, αα-coin following residual nucleus decay, production σ; deduced evidence for 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg. Gas-filled separator.

RADIOACTIVITY 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs(α) [from 208Pb(86Kr, n) and subsequent α-decay]; measured Eα, T1/2.

doi: 10.1103/PhysRevLett.83.1104
Citations: PlumX Metrics


1979AD04      Phys.Rev. C20, 1542 (1979)

J.L.Adams

68Cu in the Core-Coupling Model

NUCLEAR STRUCTURE 65,67,68Cu, 69Zn, 67Ni; calculated energy levels. Core-coupling model.

doi: 10.1103/PhysRevC.20.1542
Citations: PlumX Metrics


1974HO23      Nucl.Phys. A229, 365 (1974)

P.Hoffmann-Pinther, J.L.Adams

90Y in the Core-Coupling Model

NUCLEAR STRUCTURE 89Sr, 89,90Y; calculated levels.

doi: 10.1016/0375-9474(74)90658-7
Citations: PlumX Metrics


1973WE06      Phys.Rev. C8, 1 (1973)

G.D.Westin, J.L.Adams

Two-Level R-Matrix Theories and Calculations

NUCLEAR REACTIONS 12C, 16O(n, n), E=2.4, 3 MeV; analyzed resonances of same J, π, R-matrix theory.

doi: 10.1103/PhysRevC.8.1
Citations: PlumX Metrics


1972CH47      Phys.Rev. C6, 2237 (1972)

C.Chen, J.L.Adams

Analysis of Analog Resonances in 115In(p, p)115In between 6.6 and 7.6 MeV

NUCLEAR REACTIONS 115In(p, p), E=6.6-7.6 MeV; measured σ(E). 116Sn deduced IAR, J, π, level-width.

doi: 10.1103/PhysRevC.6.2237
Citations: PlumX Metrics


1971WE08      Phys.Rev. C4, 363 (1971)

G.D.Westin, J.L.Adams

Potential Scattering and Spectroscopic Factors in R-Matrix Theory

NUCLEAR REACTIONS 12C, 16O(n, n), E=0.5-4 MeV; calculated σ(E). 13C, 17O resonances deduced S.

doi: 10.1103/PhysRevC.4.363
Citations: PlumX Metrics


1970LA21      Phys.Rev. C2, 2097 (1970)

R.O.Lane, C.E.Nelson, J.L.Adams, J.E.Monahan, A.J.Elwyn, F.P.Mooring, A.Langsdorf, Jr.

States in 12B Observed in the Scattering of Neutrons by 11B

NUCLEAR REACTIONS 11B(polarized n, n), E=0.075-2.2 MeV; measured σ(E;θ), P(E;θ). 12B deduced resonances, J, π, isobaric analogs.

doi: 10.1103/PhysRevC.2.2097
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10093.


1969BE03      Phys.Rev.Letters 22, 476(1969); Priv.Comm. (1970)

E.M.Bernstein, L.S.Michelman, T.I.Bonner, J.L.Adams, C.Chen

Spins and Orbital Angular Momentum Configurations of Levels in 90Y

NUCLEAR REACTIONS 89Y(p, p), E=7.0-7.6 MeV; measured σ(E; θ), polarization P(E; θ). 90Zr deduced resonances, J, π, isobaric analog.

doi: 10.1103/PhysRevLett.22.476
Citations: PlumX Metrics


1969MI18      Phys.Rev. 185, 1485 (1969)

L.S.Michelman, T.I.Bonner, E.M.Bernstein, J.L.Adams, C.Chen

Polarization in the 89Y(p, p)89Y Reaction Near the d3/2 Isobaric Spin Doublet

NUCLEAR REACTIONS 89Y(p, p), E = 7.1-7.6 MeV; measured σ(E;θ), P(E;θ). 90Zr deduced resonances, J, π, isobaric analogs.

doi: 10.1103/PhysRev.185.1485
Citations: PlumX Metrics


1968TH07      Phys.Rev. 173, 975 (1968); Erratum Phys.Rev. C7, 1273 (1973)

W.J.Thompson, J.L.Adams, D.Robson

Neutron Spectroscopic Factors from Isobaric Analog States

NUCLEAR REACTIONS 90Zr(p, p), E=5.7-7.0 MeV; 92Zr(p, p), (p, n), E=5.8-6.3 MeV; measured σ(E). 91,93Nb deduced isobar analog resonances, level-width, spreading widths.

doi: 10.1103/PhysRev.173.975
Citations: PlumX Metrics


1962MO11      MIT LNS Progr. Report p.63 (May 1962)

K.Moriyasu, J.L.Adams, H.A.Enge

NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.


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