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NSR database version of April 11, 2024.

Search: Author = S.Davis

Found 24 matches.

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2022EA01      At.Data Nucl.Data Tables 144, 101490 (2022)

W.P.Earwood, S.R.Davis

Ground-state frequency-dependent dipole polarizabilities of 3 ≤ Z ≤ 10 three-electron ions

ATOMIC PHYSICS Z=3-10; calculated frequency-dependent dipole polarizabilities using fully correlated Gaussian expansions.

doi: 10.1016/j.adt.2022.101490
Citations: PlumX Metrics


1993PA07      J.Phys.(London) G19, 861 (1993)

E.S.Paul, S.Davis, P.Vaska, P.J.Bishop, S.A.Forbes, D.B.Fossan, Y.-J.He, J.R.Hughes, I.Jenkins, Y.Liang, R.Ma, M.S.Metcalfe, S.M.Mullins, P.J.Nolan, R.J.Poynter, P.H.Regan, R.Wadsworth, N.Xu

Prolate and Oblate Rotational Bands in 136Sm

NUCLEAR REACTIONS 92Mo(50Cr, 2pα), E=220 MeV; measured γγ-coin, γγ(θ), Iγ ratios. 136Sm deduced levels, J, π, rotational bands. Other data input.

NUCLEAR STRUCTURE 134,136,138Sm; calculated total Routhian surface, alignments, dynamic moments of inertia. Cranked Woods-Saxon model.

doi: 10.1088/0954-3899/19/6/007
Citations: PlumX Metrics


1980KO03      Phys.Rev. C21, 776 (1980)

J.J.Kolata, R.E.Malmin, P.A.DeYoung, S.Davis, R.Luhn

Inclusive α-Particle Production in the 12C + 12C Reaction

NUCLEAR REACTIONS 12C(12C, xα), E(cm)=12-31.5 MeV; measured inclusive α yields. 24Mg deduced evaporation σ for 3α.

doi: 10.1103/PhysRevC.21.776
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1976DA19      Nucl.Phys. A270, 285 (1976)

S.Davis, C.Glashausser, A.B.Robbins, G.Bissinger

Inelastic Scattering of Polarized Protons from 138Ba at Isobaric Analog Resonances

NUCLEAR REACTIONS 138Ba(p, p'), (p, p'γ), (polarized p, p'), (polarized p, p'γ), E=10.00, 10.63, 11.09, 11.45, 11.70 MeV; measured σ(Ep', θ), A(θ), spin-flip. 139La deduced IAS, Γp', S. Compared with theory. Enriched target.

doi: 10.1016/0375-9474(76)90448-6
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1976HA47      Nucl.Phys. A270, 269 (1976)

C.F.Haynes, S.Davis, C.Glashausser, A.B.Robbins

Inelastic Scattering of Polarized Protons from 88Sr at Isobaric Analog Resonances

NUCLEAR REACTIONS 88Sr(p, p'), (p, p'γ), (polarized p, p'), (polarized p, p'γ), E=7.00, 7.08, 7.53 MeV; measured σ(Ep', θ), A(θ), spin flip. 89Y deduced IAS, Γp', S. Compared with theory.

doi: 10.1016/0375-9474(76)90447-4
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1975BA41      Nucl.Phys. A250, 79 (1975)

F.T.Baker, S.Davis, C.Glashausser, A.B.Robbins

Elastic and Inelastic Scattering of 15 MeV Polarized Deuterons from Isotopes of Ca, Cu, Sr, Zr, and Mo

NUCLEAR REACTIONS 48Ca, 63Cu, 88Sr, 90,92Zr, 92Mo(polarized d, d), (polarized d, d'), E=15 MeV; measured σ(θ), iT11(θ); deduced optical model parameters. 48Ca, 88Sr, 90,92Zr, 92Mo levels deduced deformation parameters β(L). 92Zr(d, d), E=15 MeV; measured T20(θ), T22(θ). Enriched targets.

doi: 10.1016/0375-9474(75)90201-8
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1975DA01      Phys.Rev.Lett. 34, 215 (1975)

S.Davis, C.Glashausser, A.B.Robbins, G.Bissinger, R.Albrecht, J.P.Wurm

Correlations in Compound-Nucleus Decay Amplitudes in the Vicinity of Isobaric Analog States

NUCLEAR REACTIONS 92Mo, 106Cd(polarized p, p'γ); measured P(θ), A(θ), σ(E, Eγ, θ).

doi: 10.1103/PhysRevLett.34.215
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1974BA74      Nucl.Phys. A233, 409 (1974)

F.T.Baker, S.Davis, C.Glashausser, A.B.Robbins

Elastic and Inelastic Scattering of 15 MeV Polarized Deuterons from Ti, Cr, Fe and Ni Isotopes

NUCLEAR REACTIONS 48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni(polarized d, d), (polarized d, d'), E=15 MeV; measured σ(θ), iT11(θ); deduced optical model parameters. 48,50Ti, 52Cr, 54,56Fe, 58,60,62,64Ni levels deduced deformation parameters β(L). 54,56Fe, 62Ni(polarized d, d), (polarized d, d'), E=15 MeV; measured t20(θ), t22(θ). 54,56Fe(polarized d, d), (polarized d, d'), E=15 MeV; measured t21(θ). Enriched targets.

doi: 10.1016/0375-9474(74)90466-7
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1974DA14      Phys.Rev. A9, 1494 (1974)

S.J.Davis, J.J.Wright, L.C.Balling

Precision Measurement of g(I)(87Rb+)/g(J)(87Rb)

NUCLEAR MOMENTS 87Rb; measured g-ratio. Optical pumping.

doi: 10.1103/PhysRevA.9.1494
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1972BO40      Phys.Rev.Lett. 29, 955 (1972)

R.N.Boyd, D.Slater, R.Avida, H.F.Glavish, C.Glashausser, G.Bissinger, S.Davis, C.F.Haynes, A.B.Robbins

Observation of Polarization-Analyzing Power Inequality in the Reaction 88Sr(p, p'γ)88Sr Using Polarized Protons

NUCLEAR REACTIONS 88Sr(p, p'γ), E=7.00, 7.08, 7.53 MeV; measured σ(θ), analyzing power(θ), spin-flip probability(θ). 89Y deduced isobaric analog resonance level-width, wave functions.

doi: 10.1103/PhysRevLett.29.955
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1972CO10      Phys.Rev. C5, 1397 (1972)

R.L.Covey, S.P.Davis

Hyperfine Structure and Isomeric Shift of Hg199m

NUCLEAR MOMENTS 199mHg; measured a, isotope shift; deduced μ. Optical spectroscopy.

doi: 10.1103/PhysRevC.5.1397
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1971BO43      Phys.Rev.Lett. 27, 1590 (1971)

R.Boyd, S.Davis, C.Glashausser, C.F.Haynes

Analyzing Power, Polarization, and Spin Flip in Inelastic Scattering at Isobaric Analog Resonances

NUCLEAR REACTIONS 88Sr(polarized p, p'), E not given; measured σ(θ), analyzing power(θ). 89Y deduced isobaric analog resonances, level-width.

doi: 10.1103/PhysRevLett.27.1590
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1971DA05      Phys.Rev. A3, 1220 (1971)

S.J.Davis, J.J.Wright, L.C.Balling

Hyperfine Structure of the Ground State of Mn55

NUCLEAR MOMENTS 55Mn; measured a, b, c, d, E. Spin-exchange optical pumping.

doi: 10.1103/PhysRevA.3.1220
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1969GO21      Phys.Rev. 188, 1897 (1969)

D.Goorvitch, S.P.Davis, H.Kleiman

Isotope Shift and Hyperfine Structure of the Neutron-Deficient Thallium Isotopes

NUCLEAR MOMENTS 194,195,196Tl; measured a. 195Tl deduced μ.

doi: 10.1103/PhysRev.188.1897
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1967GO13      Nucl.Phys. A99, 1(1967)

D.Goorvitch, H.Kleiman, S.P.Davis

The Isomer Shift of 198Tl

ATOMIC PHYSICS 197,198,198m,205Tl; measured optical spectra; deduced isotope, isomer shift .

doi: 10.1016/0375-9474(67)90203-5
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1966DA07      Phys.Rev. 147, 861 (1966)

S.P.Davis, T.Aung, H.Kleiman

Isotope Shifts of Neutron-Deficient Mercury Isotopes

NUCLEAR STRUCTURE 193Hg, 195Hg, 192Hg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.861
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1966DA15      J.Opt.Soc.Amer. 56, 1604 (1966)

S.P.Davis, H.Kleiman, D.Goorvitch, T.Aung

Hyperfine Structure, Nuclear Moments, and Isotope Shifts of 197Tl and 198Tl

NUCLEAR STRUCTURE 197Tl; measured not abstracted; deduced nuclear properties.

doi: 10.1364/JOSA.56.001604
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1964KL01      Phys.Letters 13, 212 (1964); Erratum Phys.Letters 15, 296 (1965)

H.Kleiman, S.P.Davis, T.Aung

The Spin and Moments of Hg193

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

doi: 10.1016/0031-9163(64)90455-X
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1963KL03      J.Opt.Soc.Am. 53, 822 (1963)

H.Kleiman, S.P.Davis

Hyperfine Structures, Isotope Shifts, and Nuclear Moments of Hg195, Hg195m, and Hg194

NUCLEAR STRUCTURE 194Hg, 195Hg; measured not abstracted; deduced nuclear properties.

doi: 10.1364/JOSA.53.000822
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1963RE10      J.Opt.Soc.Am. 53, 431 (1963)

J.Reader, S.P.Davis

Promethium 147 Hyperfine Structure under High Resolution

NUCLEAR STRUCTURE 147Pm; measured not abstracted; deduced nuclear properties.

doi: 10.1364/JOSA.53.000431
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1959ME82      Phys.Rev. 115, 130 (1959)

A.C.Melissinos, S.P.Davis

Dipole and Quadrupole Moments of the Isomeric Hg197* Nucleus; Isomeric Isotope Shift

doi: 10.1103/PhysRev.115.130
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1958ME80      Bull.Am.Phys.Soc. 3, No.7, 371, M5 (1958)

A.C.Melissinos, S.P.Davis

Dipole and Quadrupole Moments of Isomeric Radioactive Hg-197; Isomeric Isotope Shift


1954BI92      Phys.Rev. 96, 1531 (1954)

F.Bitter, S.P.Davis, B.Richter, J.E.R.Young

Optical Studies of Radioactive Mercury

doi: 10.1103/PhysRev.96.1531
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1954DA05      Phys.Rev. 93, 159 (1954)

S.P.Davis

Nuclear Spins and Band Spectra of the Selenium Isotopes

doi: 10.1103/PhysRev.93.159
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Note: The following list of authors and aliases matches the search parameter S.Davis: , S.A.DAVIS, S.D.DAVIS, S.J.DAVIS, S.L.DAVIS, S.P.DAVIS, S.R.DAVIS