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NSR database version of April 25, 2024.

Search: Author = R.C.Thompson

Found 18 matches.

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2015UL01      J.Phys.(London) B48, 144022 (2015)

J.Ullmann, Z.Andelkovic, A.Dax, W.Geithner, C.Geppert, C.Gorges, M.Hammen, V.Hannen, S.Kaufmann, K.Konig, Y.Litvinov, M.Lochmann, B.Maass, J.Meisner, T.Murbock, R.Sanchez, M.Schmidt, S.Schmidt, M.Steck, T.Stohlker, R.C.Thompson, J.Vollbrecht, C.Weinheimer, W.Nortershauser

An improved value for the hyperfine splitting of hydrogen-like ²⁰⁹BI⁸²⁺

ATOMIC PHYSICS ²⁰⁹Bi; measured time structure of the fluorescence resonance signal; deduced the rest frame transition wavelength and transition energies. Comparison with theoretical calculations.

doi: 10.1088/0953-4075/48/14/144022
Citations: PlumX Metrics

2014LO11      Phys.Rev. A 90, 030501R (2014)

M.Lochmann, R.Johren, C.Geppert, Z.Andelkovic, D.Anielski, B.Botermann, M.Bussmann, A.Dax, N.Frommgen, M.Hammen, V.Hannen, T.Kuhl, Y.A.Litvinov, R.Lopez-Coto, T.Stohlker, R.C.Thompson, J.Vollbrecht, A.Volotka, C.Weinheimer, W.Wen, E.Will, D.Winters, R.Sanchez, W.Nortershauser

Observation of the hyperfine transition in lithium-like bismuth ²⁰⁹Bi⁸⁰⁺ :Towards a test of QED in strong magnetic fields

ATOMIC PHYSICS ²⁰⁹Bi; measured fluorescence emission wavelengths; deduced hyperfine splitting. Comparison with available data.

doi: 10.1103/PhysRevA.90.030501
Citations: PlumX Metrics

1989KA29      Z.Phys. A334, 103 (1989)

W.Kalber, J.Rink, K.Bekk, W.Faubel, S.Goring, G.Meisel, H.Rebel, R.C.Thompson

Nuclear Radii of Thorium Isotopes from Laser Spectroscopy of Stored Ions

NUCLEAR MOMENTS ²³²Th; measured hfs, isotope shifts. ^{232,227,228,229,230}Th deduced mean square charge radii change. Other data input.

RADIOACTIVITY ^{227,228,229,230}Th; measured hfs, isotope shifts. ^{232,227,228,229,230}Th deduced mean square charge radii change. Other data input.

1983TH03      J.Phys.(London) G9, 443 (1983)

R.C.Thompson, M.Anselment, K.Bekk, S.Goring, A.Hanser, G.Meisel, H.Rebel, G.Schatz, B.A.Brown

High-Resolution Measurements of Isotope Shifts and Hyperfine Structure in Stable and Radioactive Lead Isotopes

RADIOACTIVITY ²¹⁰Pb; ²¹²Pb [from ²³²Th decay]; ²⁰⁵Pb [from ²⁰⁴Pb(n, γ)]; ²⁰⁹Pb [from ²⁰⁸Pb(d, p)]; ^{198,199,200,202}Pb [from Hg(α, xn), E=104 MeV]; ^201,202m,203Pb [from Tl(d, xn), E=38, 48 MeV]; measured hfs, isotope shifts. ^{201,202m,205,209}Pb deduced μ, quadrupole moment, rms charge radii. ¹⁹⁹Pb level deduced J, π, μ, quadrupole moment, rms charge radius. ^198,210,212Pb deduced rms charge radius. Droplet model, Skyrme interactions.

NUCLEAR MOMENTS ^204,206,207Pb; measured hfs, isotope shifts; deduced rms charge radii. Droplet model, Skyrme interactions.

doi: 10.1088/0305-4616/9/4/010
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1982AN15      Phys.Rev. C26, 2194 (1982)

A.Andl, K.Bekk, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz, R.C.Thompson

Isotope Shifts and Hyperfine Structure of the 4s^{2 1}S₀-4s4p ¹P₁ Transition in Calcium Isotopes

NUCLEAR MOMENTS ^{40,42,43,44,46,48}Ca, ^41,45,47Ca [from ^40,44,46Ca(n, γ), E=thermal]; measured hfs, isotope shifts. ^41,45,47Ca deduced hyperfine constants, rms charge radii differences, μ. ⁴³Ca deduced hyperfine constants, rms charge radii differences. ^{40,42,44,46,48}Ca deduced rms charge radii differences. Laser spectroscopy, resonance fluorescence technique.

doi: 10.1103/PhysRevC.26.2194
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1982TH05      Z.Phys. A305, 89 (1982)

R.C.Thompson, A.Hanser, K.Bekk, G.Meisel, D.Frolich

High Resolution Measurements of Isotope Shifts in Lead

NUCLEAR MOMENTS ^{200,201,202,203,204,205,206,207,208}Pb; measured hfs. ^{200,202,204,206}Pb deduced isotopes shifts, rms radii. ^{201,203,205,207}Pb deduced isotope shifts, rms radii, μ. High resolution laser spectroscopy.

doi: 10.1007/BF01415085
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1978GR12      Phys.Rev. C18, 671 (1978)

R.D.Griffioen, R.C.Thompson, J.R.Huizenga

Levels of ²³⁵Np Excited by the ²³⁴U(³He, d) and ²³⁴U(α, t) Reactions

NUCLEAR REACTIONS ²³⁴U(³He, d), (α, t), E=30 MeV; measured σ(θ). ²³⁵Np deduced levels, Nilsson configurations. Enriched target.

doi: 10.1103/PhysRevC.18.671
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1978JO05      Phys.Rev. C17, 927 (1978)

M.W.Johnson, R.C.Thompson, J.R.Huizenga

States in U²³³ Excited by the ²³⁴U(d, t) and ²³⁴U(³He, α) Reactions

NUCLEAR REACTIONS ²³⁴U(d, t), E=14 MeV; ²³⁴U(³He, α), E=30 MeV; measured σ(θ). ²³³U deduced levels, L, Nilsson configurations, J, π.

doi: 10.1103/PhysRevC.17.927
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1977FE11      Phys.Lett. 69B, 407 (1977)

W.Feix, W.Wilcke, T.W.Elze, H.Rebel, J.R.Huizenga, R.C.Thompson, R.M.Dreizler

Study of Nuclear-Coulomb Interference Effects in Inelastic Deuteron Scattering on ²³⁸U

NUCLEAR REACTIONS ²³⁸U(d, d), (d, d'), E=17 MeV; measured σ(θ). ²³⁸U deduced β.

doi: 10.1016/0370-2693(77)90831-0
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1977TH04      Phys.Rev. C15, 2019 (1977)

R.C.Thompson, W.Wilcke, J.R.Huizenga, W.K.Hensley, D.G.Perry

Levels of Isotopes ^233,235,237Pa and ^229,231Ac Studied by the (t, α) Reaction

NUCLEAR REACTIONS ^234,236,238U, ^230,232Th(t, α), E=15 MeV; measured σ(Eα, θ). ^233,235,237Pa, ^229,231Ac deduced levels, J, S, Nilsson proton configurations. DWBA analysis.

doi: 10.1103/PhysRevC.15.2019
Citations: PlumX Metrics

1977WI07      Nucl.Phys. A286, 297 (1977)

W.Wilcke, W.Feix, T.W.Elze, J.R.Huizenga, R.C.Thompson, R.M.Dreizler

Influence of Form Factors and Multistep Effects on the ²³²Th(d, t)²³¹Th Reaction

NUCLEAR REACTIONS ²³²Th(d, t), E=17 MeV; measured σ(Et, θ). ²³⁰Th(d, p), E=17 MeV; measured σ(Ep, 80°). ²³¹Th levels deduced S.

doi: 10.1016/0375-9474(77)90409-2
Citations: PlumX Metrics

1976TH01      Phys.Rev. C13, 638 (1976)

R.C.Thompson, J.R.Huizenga, T.W.Elze

Collective States in ²³³U, ²³⁵U, ²³⁷Np, and ²³⁹Pu Excited by Inelastic Deuteron Scattering

NUCLEAR REACTIONS ^233,235U, ²³⁷Np, ²³⁹Pu(d, d'), E=16 MeV; measured σ(Ed'). ^233,235U, ²³⁷Np, ²³⁹Pu deduced levels, K, J, π. Enriched targets.

doi: 10.1103/PhysRevC.13.638
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1975TH02      Phys.Lett. 55B, 447 (1975)

R.C.Thompson, A.Ikeda, P.Kleinheinz, R.K.Sheline, P.J.Daly

Nucleon Transfer Cross Sections for Mixed Odd-A Targets

NUCLEAR REACTIONS ¹⁸⁹Os(d, t); calculated σ.

doi: 10.1016/0370-2693(75)90552-3
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1975TH04      Nucl.Phys. A242, 1 (1975)

R.C.Thompson, J.S.Boyno, J.R.Huizenga, D.G.Burke, T.W.Elze

Study of the ¹⁸⁸Os(p, t)¹⁸⁶Os, ¹⁹⁰Os(p, t)¹⁸⁸Os and ¹⁹²Os(p, t)¹⁹⁰Os Reactions

NUCLEAR REACTIONS ^188,190,192Os(p, t), E=18 MeV; measured σ(Et, θ); deduced Q. ^186,188,190Os deduced levels, J, π, L. ¹⁸⁹Os(p, t), E=18 MeV; calculated Q.

doi: 10.1016/0375-9474(75)90029-9
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1975TH11      Phys.Rev. C12, 1227 (1975)

R.C.Thompson, J.R.Huizenga, T.W.Elze

Collective States in ²³⁰Th, ²⁴⁰Pu, ²⁴⁴Pu, and ²⁴⁸Cm Excited by Inelastic Deuteron Scattering

NUCLEAR REACTIONS ²³⁰Th, ^240,244Pu, ²⁴⁸Cm(d, d'), E=16 MeV; measured σ(Ed', θ). ²³⁰Th, ^240,244Pu, ²⁴⁸Cm deduced levels, J, K, π, B(E2), B(E3). Enriched targets.

doi: 10.1103/PhysRevC.12.1227
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1949OS01      The Transuranium Elements: Research Papers, Book 2, Vol.14B, paper 19.11, G.T.Seaborg ed., p.1397 (1949)

D.W.Osborne, R.C.Thompson, Q.Van Winkle

Products of the Deuteron and Helium-Ion Bombardments of Pa²³¹

1948MI12      Phys.Rev. 74, 347 (1948)

D.R.Miller, R.C.Thompson, B.B.Cunningham

Products of High Energy Deuteron and Helium Ion Bombardments of Copper

doi: 10.1103/PhysRev.74.347
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1946OS02      NNES 14B, Paper 19.11 (1946)

D.W.Osborne, R.C.Thompson, Q.Van Winkle

Products of the Deuteron and Helium-Ion Bombardments of Pa²³¹