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NSR database version of April 29, 2024.

Search: Author = R.Watson

Found 26 matches.

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1999BE58      Eur.Phys.J. A 6, 329 (1999)

J.Becker, H.G.Andresen, J.R.M.Annand, K.Aulenbacher, K.Beuchel, J.Blume-Werry, Th.Dombo, P.Drescher, M.Ebert, D.Eyl, A.Frey, P.Grabmayr, T.Grossmann, P.Hartmann, T.Hehl, W.Heil, C.Herberg, J.Hoffmann, J.D.Kellie, F.Klein, K.Livingston, M.Leduc, M.Meyerhoff, H.Moller, Ch.Nachtigall, A.Natter, M.Ostrick, E.W.Otten, R.O.Owens, S.Plutzer, E.Reichert, D.Rohe, M.Schafer, H.Schmieden, R.Sprengard, M.Steigerwald, K.-H.Steffens, R.Surkau, Th.Walcher, R.Watson, E.Wilms

Determination of the Neutron Electric Form Factor from the Reaction 3He(e, e'n) at Medium Momentum Transfer

NUCLEAR REACTIONS 3He(polarized e, e'n), E not given; measured σ(θ), asymmetry vs momentum transfer. 1n deduced electric form factor. Polarized target. Comparisons with previous results.

doi: 10.1007/s100500050351
Citations: PlumX Metrics

1999HE16      Eur.Phys.J. A 5, 131 (1999)

C.Herberg, M.Ostrick, H.G.Andresen, J.R.M.Annand, K.Aulenbacher, J.Becker, P.Drescher, D.Eyl, A.Frey, P.Grabmayr, S.J.Hall, P.Hartmann, T.Hehl, W.Heil, J.Hoffmann, D.Ireland, J.D.Kellie, F.Klein, K.Livingston, Ch.Nachtigall, A.Natter, E.W.Otten, R.O.Owens, E.Reichert, D.Rohe, H.Schmieden, R.Sprengard, M.Steigerwald, K.-H.Steffens, Th.Walcher, R.Watson

Determination of the Neutron Electric Form Factor in the D(e, e'n)p Reaction and the Influence of Nuclear Binding

NUCLEAR REACTIONS 2H(e, e'n), E not given; measured recoil polarization ratio. 1n deduced electric form factor.

doi: 10.1007/s100500050268
Citations: PlumX Metrics

1999OS01      Phys.Rev.Lett. 83, 276 (1999)

M.Ostrick, C.Herberg, H.G.Andresen, J.R.M.Annand, K.Aulenbacher, J.Becker, P.Drescher, D.Eyl, A.Frey, P.Grabmayr, P.Hartmann, T.Hehl, W.Heil, J.Hoffmann, D.Ireland, J.D.Kellie, F.Klein, K.Livingston, Ch.Nachtigall, A.Natter, E.W.Otten, R.O.Owens, E.Reichert, D.Rohe, H.Schmieden, R.Sprengard, M.Steigerwald, K.-H.Steffens, Th.Walcher, R.Watson

Measurement of the Neutron Electric Form Factor GE, n in the Quasifree 2H(e(pol), e'n(pol))p Reaction

NUCLEAR REACTIONS 2H(polarized e, e'n), E=855 MeV; measured asymmetries, other polarization observables. 1n deduced electric form factor. Neutron polarimeter.

doi: 10.1103/PhysRevLett.83.276
Citations: PlumX Metrics

1992HO17      Phys.Rev. A46, 2572 (1992)

V.Horvat, G.Sampoll, K.Wohrer, M.Chabot, R.L.Watson

K-Shell Ionization of Intermediate-Z Elements by 30-MeV/amu H, N, Ne, and Ar Ions

NUCLEAR REACTIONS 27Al, Ti, Fe, Cu, Ge, Zr, Mo, Pd, Sn(p, X), (N, X), (Ne, X), (Ar, X), E=30 MeV/nucleon; measured K (X-ray) production σ, double K-shell ionization I X-ray.

ATOMIC PHYSICS 27Al, Ti, Fe, Cu, Ge, Zr, Mo, Pd, Sn(p, X), (N, X), (Ne, X), (Ar, X), E=30 MeV/nucleon; measured K (X-ray) production σ, double K-shell ionization I X-ray.

doi: 10.1103/PhysRevA.46.2572
Citations: PlumX Metrics

1991HO25      Nucl.Instrum.Methods Phys.Res. B56/57, 61 (1991)

V.Horvat, R.L.Watson, G.Sampoll, T.Lotze, B.Hill

K- Plus L-Shell Ionization of Fourth Row Elements by 30 MeV/amu Ar Ions

NUCLEAR REACTIONS Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn(Ar, X), E=30 MeV/nucleon; measured K X-ray spectra; deduced double-to-single target K-shell ionization probabilities, single-, double K-shell vacancies relative probabilities.

ATOMIC PHYSICS Ti, V, Cr, Fe, 59Co, Ni, Cu, Zn(Ar, X), E=30 MeV/nucleon; measured K X-ray spectra; deduced double-to-single target K-shell ionization probabilities, single-, double K-shell vacancies relative probabilities.

doi: 10.1016/0168-583X(91)95971-F
Citations: PlumX Metrics

1985WA06      Phys.Scr. 31, 184 (1985)

R.L.Watson, B.B.Bandong, J.M.Sanders, K.Parthasaradhi

K X-Ray Spectra of Sodium Excited by Heavy Charged Particles

ATOMIC PHYSICS Na(α, X), E=5.5 MeV; Na(12C, X), E=22 MeV; Na(24Mg, X), E=48 MeV; Na(40Ar, X), E=80 MeV; measured K X-rays. Metallic Na, Na compounds.

doi: 10.1088/0031-8949/31/3/005
Citations: PlumX Metrics

1983MA48      Nucl.Instrum.Methods 214, 117 (1983)

R.J.Maurer, R.L.Watson, G.J.Pedrazzini

Spectra of np-1s Transitions Excited during the Passage of 48 MeV Mg Ions through Thin and Thick Carbon Targets

ATOMIC PHYSICS C(Mg, X), E=48 MeV; measured K X-ray spectra. Thick targets, curved crystal spectrometer.

doi: 10.1016/0167-5087(83)90549-5
Citations: PlumX Metrics

1981NA09      Phys.Rev.Lett. 47, 1114 (1981)

J.B.Natowitz, M.N.Namboodiri, L.Adler, R.P.Schmitt, R.L.Watson, S.Simon, M.Berlanger, R.Choudhury

Particle Emission at a 20Ne Projectile Velocity Comparable to the Fermi Velocity

NUCLEAR REACTIONS Ta, Ag, Ni(20Ne, p), (20Ne, d), (20Ne, 3He), (20Ne, α), E=60 MeV/nucleon; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα); deduced statistical projectile fragmentation dominance.

doi: 10.1103/PhysRevLett.47.1114
Citations: PlumX Metrics

1975WA35      Phys.Rev. A12, 2628 (1975)

R.L.Watson

Calculations of Electron Energy Distributions for Internal Ionization during the Alpha Decay of 210Po Employing the Binary-Encounter Approximation

NUCLEAR STRUCTURE 210Po; calculated electron energy distributions for internal ionization during α decay.

doi: 10.1103/PhysRevA.12.2628
Citations: PlumX Metrics

1974FO03      Nucl.Phys. A220, 505 (1974)

G.S.Foote, D.Branford, R.A.I.Bell, R.B.Watson

The 56Fe(α, γ)60Ni Reaction at Excitation Energies in the Region of the Giant Dipole Resonance

NUCLEAR REACTIONS 56Fe(α, γ), E=8-17.6 MeV; 59Co(p, γ), E=16.6-16.9 MeV; measured σ(E;Eγ, θ). 60Ni deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(74)90131-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0858.

1973WA08      Nucl.Phys. A203, 209 (1973)

R.B.Watson, D.Branford, J.L.Black, W.J.Caelli

The 36Ar(α, γ0)40Ca Reaction at Excitation Energies in the Region of The Giant Dipole Resonance

NUCLEAR REACTIONS 36Ar(α, γ), E=6-17 MeV; measured (E; Eγ, θ). 40Ca deduced levels J, π, (2j+1)gamma(αgammaγ)/level-width. Enriched target.

doi: 10.1016/0375-9474(73)90433-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0605.

1972WA32      Phys.Rev. C6, 2189 (1972)

R.L.Watson, E.T.Chulick, R.W.Howard

Probability of K-Shell Internal Ionization in the Beta Decay of 99Tc

RADIOACTIVITY 99Tc; measured I(K X-ray); deduced K-shell ionization probability.

doi: 10.1103/PhysRevC.6.2189
Citations: PlumX Metrics

1971WA28      Nucl.Phys. A178, 201 (1971)

R.L.Watson, T.K.Li

Energies and Intensities of Cm L X-Rays Emitted in Coincidence with the α-Decay of 252Cf

RADIOACTIVITY 252Cf, 241Am; measured E(L X-ray), I(L X-ray). 252Cf; measured Eγ, Iγ. 248Cm transition deduced ICC. Np; measured I(L X-ray). Cm; measured E(L X-ray) , I(L X-ray); deduced l2, l3 fluorescence yields.

doi: 10.1016/0375-9474(71)90198-9
Citations: PlumX Metrics

1970BL09      Phys.Rev.Lett. 25, 877 (1970)

J.L.Black, W.J.Caelli, R.B.Watson

Systematic Search for the Lowest T = 2 State of 12C Using Deuteron- and 3He-Induced Reactions

NUCLEAR REACTIONS 10B(d, γ), (d, p), (d, α), E=2.605-2.960 MeV; 9Be(3He, γ), E=1.670-1.770 MeV; measured σ(E). 12C deduced resonance, level-width, T.

doi: 10.1103/PhysRevLett.25.877
Citations: PlumX Metrics

1970BL10      Nucl.Phys. A153, 233 (1970)

J.L.Black, W.J.Caelli, W.F.Davidson, R.B.Watson

A Study of the Reaction 11B(3He, γ0)14N in the Energy Range E = 0.9-2.6 MeV

NUCLEAR REACTIONS 11B(3He, γ0), E=0.9-2.6 MeV; measured σ(E(3He), θ). 14N deduced resonance, J, π. Enriched target.

doi: 10.1016/0375-9474(70)90768-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0466.

1970SW05      Phys.Rev. B1, 146 (1970)

J.C.Swartz, L.J.Swartzendruber, L.H.Bennett, R.E.Watson

Nuclear Magnetic Resonance of 51Fe in the Paramagnetic Alloys TiFe(1-x)Co(x)

NUCLEAR MOMENTS 57Fe; measured NMR. 59Co deduced μ.

doi: 10.1103/PhysRevB.1.147
Citations: PlumX Metrics

1970WA05      Nucl.Phys. A141, 449 (1970)

R.L.Watson, J.B.Wilhelmy, R.C.Jared, C.Rugge, H.R.Bowman, S.G.Thompson, J.O.Rasmussen

A Study of the Low-Energy Transitions Arising from the Prompt de-Excitation of Fission Fragments

RADIOACTIVITY, Fission 252Cf(SF); measured E(ce), I(ce), E(X-ray), I(X-ray), I(ce)(t), (fragment)(fragment)(ce)(X)-coin. 102Zr, 106Mo, 108,109Tc, 110Ru, 116Rh, 140Cs, 144Ba, 146La, 148Ce, 149,150Pr; measured E(ce), I(ce); deduced Eγ, K/L, T1/2 (level). Detector - Si(Li), Si(P) fragment detectors.

doi: 10.1016/0375-9474(70)90982-6
Citations: PlumX Metrics

1970WA12      Phys.Rev. C1, 1866 (1970)

R.L.Watson, R.C.Jared, S.G.Thompson

Distribution of K X-Rays as a Function of Mass and Atomic Number in the Spontaneous Fission of 252Cf

RADIOACTIVITY, Fission 252Cf(SF); measured (fission fragment)(K X-ray)-coin; deduced I(K X-ray)(A, Z).

doi: 10.1103/PhysRevC.1.1866
Citations: PlumX Metrics

1970WA27      Nucl.Phys. A154, 561 (1970)

R.L.Watson, C.W.Lewis, J.B.Natowitz

X-Ray Emission Induced by 30 to 80 MeV Alpha Particles

ATOMIC PHYSICS Fe, Ni, Cu, Zr, Nb, Rh, Pd, Ag, Sn + α, E=30-80 MeV; measured I(X-ray)(Kα+Kβ)/Iα. Sn, Tm, Ta, Au + α, E = 30-80 MeV; measured I(X-ray)(L)/Iα; deduced X-ray emission, ionization σ for Eα=30-80 MeV. Detector - Si(Li).

doi: 10.1016/0375-9474(70)90127-2
Citations: PlumX Metrics

1969BL04      Nucl.Phys. A125, 545 (1969)

J.L.Black, W.J.Caelli, R.B.Watson

The Low-Lying Excited States of 103Rh

NUCLEAR REACTIONS 103Rh(16O, 16O'γ), E=34, 40 MeV; measured Eγ, Iγ, γγ-coin. 103Rh deduced levels, J, π, T1/2, B(E2). Natural targets. Ge(Li), NaI(Tl) detectors. 103Rh(p, p'), E=10, 11.75 MeV; measured σ(E;Ep, θ). 103Rh deduced levels. Natural targets, magnetic spectrograph.

doi: 10.1016/0375-9474(69)90747-7
Citations: PlumX Metrics

1969BL14      Phys.Letters 30B, 100 (1969)

J.L.Black, W.J.Caelli, D.L.Livesey, R.B.Watson

Search for the Lowest T = 2 State of 8Be: Experimental

NUCLEAR REACTIONS 6Li(d, d), (d, p), (d, α), E = 6.33-7.14 MeV; measured σ(E;θ). 8Be deduced resonance, level-width.

doi: 10.1016/0370-2693(69)90408-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1427.

1966WA01      Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.423 (1966)

R.L.Watson, H.R.Bowman, S.G.Thompson, J.O.Rasmussen

Internal Conversion Electrons from Primary Fission Fragments

NUCLEAR STRUCTURE 252Cf; measured not abstracted; deduced nuclear properties.

1964BE42      Phys. Rev. 135, A588 (1964)

N.Bessis, H.Lefebvre-Brion, C.M.Moser, A.J.Freeman, R.K.Nesbet, R.E.Watson

Calculation of Magnetic Hyperfine Constant of P31

NUCLEAR STRUCTURE 31P; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.135.A588
Citations: PlumX Metrics

1963FR08      Phys.Rev. 131, 2566 (1963)

A.J.Freeman, R.E.Watson

Antishielding of Magnetic and Electric Hyperfine Interactions in Open Shell Ions

doi: 10.1103/PhysRev.131.2566
Citations: PlumX Metrics

1963FR09      Phys.Rev. 132, 706 (1963)

A.J.Freeman, R.E.Watson

Electric Quadrupole Interactions in Rare-Earth Ions

doi: 10.1103/PhysRev.132.706
Citations: PlumX Metrics

1962FR14      Phys.Rev. 127, 2058 (1962)

A.J.Freeman, R.E.Watson

Theoretical Investigation of Some Magnetic and Spectroscopic Properties of Rare-Earth Ions

NUCLEAR STRUCTURE 143Nd, 147Sm, 141Pr, 173Yb, 167Er, 165Ho; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.2058
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter R.Watson: , R.B.WATSON, R.E.WATSON, R.L.WATSON