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NSR database version of April 11, 2024.

Search: Author = A.M.Rushton

Found 12 matches.

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1984LI18      Phys.Rev. C30, 1740 (1984)

J.R.Lindemuth, M.Eckhause, K.L.Giovanetti, J.R.Kane, M.S.Pandey, A.M.Rushton, W.F.Vulcan, R.E.Welsh, R.G.Winter, P.D.Barnes, J.N.Craig, R.A.Eisenstein, J.D.Sherman, R.B.Sutton, W.R.Wharton, J.P.Miller, B.L.Roberts, A.R.Kunselman, R.J.Powers

Antiprotonic Atoms in Gaseous H2 and He and in Liquid H2

ATOMIC PHYSICS 1H, He(p-bar, X), E at rest; measured E(X-ray), I(X-ray), X-ray yields; deduced strong interaction widths in antiprotonic He 3D state. Gaseous targets.

doi: 10.1103/PhysRevC.30.1740
Citations: PlumX Metrics

1983CA09      Phys.Lett. 124B, 465 (1983)

A.L.Carter, C.R.Cox, M.S.Dixit, G.W.Dodson, M.Eckhause, C.K.Hargrove, E.P.Hincks, J.R.Kane, H.Mes, A.M.Rushton, R.T.Siegel, R.E.Welsh

Search for Two-Photon Emission from 2S States of Low-Z Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms Li, Be, B, N, O; measured metastable 2S-state yield; deduced two γ-emission quenching, possible mechanisms. Metal, hydrid, gas targets.

doi: 10.1016/0370-2693(83)91552-6
Citations: PlumX Metrics

1979HA08      Nucl.Phys. A314, 361 (1979)

A.A.Hahn, J.P.Miller, R.J.Powers, A.Zehnder, A.M.Rushton, R.E.Welsh, A.R.Kunselman, P.Roberson, H.K.Walter

An Experimental Study of Muonic X-Ray Transitions in Mercury Isotopes

NUCLEAR MOMENTS 198,199,200,201,202,204Hg; measured muonic X-rays, isotope shift; deduced nuclear charge distribution. 198,200Hg deduced quadrupole moment. 199,201Hg deduced quadrupole moment, B(E2).

doi: 10.1016/0375-9474(79)90604-3
Citations: PlumX Metrics

1977RO23      Phys.Rev. C16, 1945 (1977)

P.Roberson, T.King, R.Kunselman, J.Miller, R.J.Powers, P.D.Barnes, R.A.Eisenstein, R.B.Sutton, W.C.Lam, C.R.Cox, M.Eckhause, J.R.Kane, A.M.Rushton, W.F.Vulcan, R.E.Welsh

Strong Interaction and Mass Measurements Using Antiprotonic Atoms

NUCLEAR REACTIONS 6,7Li, C, Si, P, Fe, Y, Zr, Cs, Yb(p-bar, X), E=0 MeV; measured antiprotonic X-ray spectra; deduced strong interaction shifts, widths, effective scattering length, antiproton mass.

doi: 10.1103/PhysRevC.16.1945
Citations: PlumX Metrics

1975CL04      Phys.Rev.Lett. 35, 757 (1975)

B.T.Cleveland, W.R.Leo, C.S.Wu, L.R.Kasday, A.M.Rushton, P.J.Gollon, J.D.Ullman

Lepton Conservation in the Double β Decay of 82Se

RADIOACTIVITY 82Se; measured T1/2 of the lepton-nonconserving nutrinoless double β decay mode.

doi: 10.1103/PhysRevLett.35.757
Citations: PlumX Metrics

1972CH07      Nucl.Phys. A181, 25 (1972)

M.Y.Chen, S.C.Cheng, W.Y.Lee, A.M.Rushton, C.S.Wu

Resonance Processes and Nuclear Excitation in Muonic 205Tl

NUCLEAR REACTIONS 205Tl(μ-, Xγ), E approx 0; measured Eγ, Iγ, E(X-ray), I(X-ray), hfs M1 constants; deduced isomer shift. 205Tl levels deduced μ, quadrupole moment, B(λ).

ATOMIC PHYSICS, Mesic-Atoms 205Tl; measured μ-mesic Eγ, Iγ, I(K X-ray), I(L X-ray), I(M X-ray), hfs M1 constant; deduced isomer shift.

doi: 10.1016/0375-9474(72)90898-6
Citations: PlumX Metrics

1972LE07      Nucl.Phys. A181, 14 (1972)

W.Y.Lee, M.Y.Chen, S.C.Cheng, E.R.Macagno, A.M.Rushton, C.S.Wu

Nuclear Excitation in Muonic 209Bi

NUCLEAR REACTIONS 209Bi(μ-, Xγ), E approx 0; measured I(K X-ray), I(L X-ray), I(M X-ray), hfs constants; deduced isomer shift. 209Bi levels deduced μ, quadrupole moment, B(λ).

ATOMIC PHYSICS, Mesic-Atoms 209Bi; measured μ-mesic I(K X-ray), I(L X-ray), I(M X-ray), hfs constants; deduced isomer shift.

doi: 10.1016/0375-9474(72)90897-4
Citations: PlumX Metrics

1971CH17      Phys.Lett. 34B, 615 (1971)

S.C.Cheng, M.Y.Chen, J.W.Kast, W.Y.Lee, E.R.Macagno, A.M.Rushton, C.S.Wu

Magnetic Dipole Hyperfine Structure in Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms 93Nb, 139La; measured μ-mesic I(X-ray); deduced nuclear finite-size effect in M1 hfs.

doi: 10.1016/0370-2693(71)90153-5
Citations: PlumX Metrics

1971KA12      Nucl.Phys. A169, 62 (1971)

J.W.Kast, S.Bernow, S.C.Cheng, D.Hitlin, W.Y.Lee, E.R.Macagno, A.M.Rushton, C.S.Wu

The Isotope Shift in Muonic X-Rays in the Tin Region

ATOMIC PHYSICS, Mesic-Atoms 114Cd, 115In, 116Sn, 124Sn, 126Te, 127I; measured μ-mesic E(K X-ray), E(L X-ray); deduced nuclear charge distributions.

doi: 10.1016/0375-9474(71)90558-6
Citations: PlumX Metrics

1971LE15      Nucl.Phys. A167, 652 (1971)

W.Y.Lee, S.Bernow, M.Y.Chen, S.C.Cheng, D.Hitlin, J.W.Kast, E.R.Macagno, A.M.Rushton, C.S.Wu

The Resonance Process and the Intensity Anomaly in Muonic 127I

ATOMIC PHYSICS, Mesic-Atoms 127I; measured μ-mesic X-ray spectra. 127I deduced quadrupole moment, transition moments, charge distribution.

doi: 10.1016/0375-9474(71)90068-6
Citations: PlumX Metrics

1970BU29      Phys.Rev.Lett. 24, 604 (1970)

B.Budick, S.C.Cheng, E.R.Macagno, A.M.Rushton, C.S.Wu

Muon- and Pion-Induced Fission of Uranium Isotopes

NUCLEAR REACTIONS 233,235,238U(μ-, F), E=0 MeV; measured prompt, delayed fission. 233,235,238U deduced T1/2.

doi: 10.1103/PhysRevLett.24.604
Citations: PlumX Metrics

1969LE13      Phys.Rev.Letters 23, 648 (1969)

W.Y.Lee, S.Bernow, M.Y.Chen, S.C.Cheng, D.Hitlin, J.W.Kast, E.R.Macagno, A.M.Rushton, C.S.Wu, B.Budick

Finite Distribution of Nuclear M1 and E2 Moments in Muonic 115In, 133Cs, and 141Pr

ATOMIC PHYSICS, Mesic-Atoms 115In, 133Cs, 141Pr; measured E(X-ray), I(X-ray); deduced a, B. Ge(Li) detector.

doi: 10.1103/PhysRevLett.23.648
Citations: PlumX Metrics

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