NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = E.G.Myers Found 43 matches. 2023ME17 Phys.Rev.Lett. 131, 243002 (2023) Mass Difference of Tritium and Helium-3 ATOMIC MASSES 3H, 3He; measured frequencies; deduced the mass difference between atoms, Q-value. Comparison with with the Atomic Mass Evaluation (AME) 2020 and CODATA 2018. The cyclotron frequency ratios (CFRs), Penning trap.
doi: 10.1103/PhysRevLett.131.243002
2020FI05 Phys.Rev.Lett. 124, 013001 (2020) Deuteron-to-Proton Mass Ratio from the Cyclotron Frequency Ratio of H+2 to D+ with H+2 in a Resolved Vibrational State ATOMIC MASSES 1,2H; measured cyclotron frequencies; deduced mass ratio. Comparison with CODATA values.
doi: 10.1103/PhysRevLett.124.013001
2018SM03 Phys.Rev.Lett. 120, 143002 (2018) J.A.Smith, S.Hamzeloui, D.J.Fink, E.G.Myers Rotational Energy as Mass in H+3 and Lower Limits on the Atomic Masses of D and 3He ATOMIC MASSES 1,2H, 3He; measured cyclotron frequency ratios; deduced mass difference, lower limits on the atomic masses of deuterium and helium-3 with respect to the proton.
doi: 10.1103/PhysRevLett.120.143002
2017HA33 Phys.Rev. A 96, 060501R (2017) S.Hamzeloui, J.A.Smith, D.J.Fink, E.G.Myers Precision mass ratio of 3He+ to HD+ ATOMIC MASSES 3He, 1,2H; measured cyclotron frequency ratio; deduced mass ratio.
doi: 10.1103/PhysRevA.96.060501
2016MY01 Nat.Phys. 12, 986 (2016) A tale of two masses COMPILATION 12C; compiled experimental mass measurements.
doi: 10.1038/nphys3896
2015MY03 Phys.Rev.Lett. 114, 013003 (2015) E.G.Myers, A.Wagner, H.Kracke, B.A.Wesson Atomic Masses of Tritium and Helium-3 ATOMIC MASSES 3H, 3He; measured the cyclotron frequency ratios; deduced masses. Comparison with available data.
doi: 10.1103/PhysRevLett.114.013003
2013HO22 Phys.Rev. A 88, 052502 (2013) Atomic masses of 82, 83Kr and 131, 134Xe ATOMIC MASSES 82,83Kr, 131,134Xe; measured cyclotron frequency ratios; deduced masses. Florida State University Penning Trap.
doi: 10.1103/PhysRevA.88.0525021
2012RA34 Phys.Rev. A 86, 050502 (2012) Atomic masses of strontium and ytterbium ATOMIC MASSES 86,87,88Sr, 170,171,172,173,174,176Yb; measured cyclotron frequency ratios of pairs of ions simultaneously trapped in a Penning trap; deduced masses. Comparison with AME2003 and the upcoming AME2013 evaluations.
doi: 10.1103/PhysRevA.86.050502
2010MO03 Phys.Rev. C 81, 032501 (2010) B.J.Mount, M.Redshaw, E.G.Myers Double-β-decay Q values of 74Se and 76Ge ATOMIC MASSES 74,76Se, 74,76Ge; measured cyclotron frequencies in a Penning-trap system relative to 84Kr, atomic masses and systematic shifts for ion pairs. Comparisons with previous measurements and with AME-2003. RADIOACTIVITY 74Se(2EC), 76Ge(2β-); deduced Q values from measured masses. Discussed resonant enhancement for neutrinoless double-electron capture decay of 74Se.
doi: 10.1103/PhysRevC.81.032501
2010MO29 Phys.Rev. A 81, 064501 (2010) B.J.Mount, H.S.P.Muller, M.Redshaw, E.G.Myers Mass of 17O from Penning-trap mass spectrometry and molecular spectroscopy: A precision test of the Dunham-Watson model in carbon monoxide ATOMIC MASSES 17O; measured average cyclotron frequency ratios; deduced mass. Florida State University precision Penning-trap mass spectrometer, Dunham-Watson model.
doi: 10.1103/PhysRevA.81.064501
2010MO30 Phys.Rev. A 82, 042513 (2010) B.J.Mount, M.Redshaw, E.G.Myers Atomic masses of 6Li, 23Na, 39, 41K, 85, 87Rb, and 133Cs ATOMIC MASSES 6Li, 23Na, 39,41K, 85,87Rb, 133Cs; measured cyclotron frequency ratios of pairs of ions simultaneously trapped in a Penning trap; deduced mass. Comparison with AME2003 and other experimental results.
doi: 10.1103/PhysRevA.82.042513
2009MO23 Phys.Rev.Lett. 103, 122502 (2009) B.J.Mount, M.Redshaw, E.G.Myers Q Value of 115In → 115Sn(3/2+): The Lowest Known Energy β Decay ATOMIC MASSES 115In, 115Sn; measured cyclotron frequency ratios with Penning Trap mass spectrometer; deduced atomic masses, 115In-115Sn Q-value.
doi: 10.1103/PhysRevLett.103.122502
2009RE03 Phys.Rev. A 79, 012506 (2009) M.Redshaw, B.J.Mount, E.G.Myers Improved atomic masses of 84, 86Kr and 129, 132Xe ATOMIC MASSES 84,86Kr, 129,132Xe; measured atomic masses using a cryogenic penning trap.
doi: 10.1103/PhysRevA.79.012506
2009RE07 Phys.Rev.Lett. 102, 212502 (2009) M.Redshaw, B.J.Mount, E.G.Myers, F.T.Avignone III Masses of 130Te and 130Xe and Double-β-Decay Q Value of 130Te ATOMIC MASSES 130Te, 130Xe; Measured atomic masses using precision cryogenic Penning-trap spectrometer; Deduced Q-value for 2β-decay. Compared with energy calibration of CUORICINO and CUORE experiments.
doi: 10.1103/PhysRevLett.102.212502
2009RE15 Phys.Rev. A 79, 012507 (2009) M.Redshaw, B.J.Mount, E.G.Myers Penning-trap measurement of the atomic masses of 18O and 19F with uncertainties < 0.1 parts per 109 ATOMIC MASSES 18O, 19F; measured atomic masses using a cryogenic penning trap.
doi: 10.1103/PhysRevA.79.012507
2008RE16 Phys.Rev.Lett. 100, 093002 (2008) M.Redshaw, J.McDaniel, E.G.Myers Dipole Moment of PH+ and the Atomic Masses of 28Si, 31P by Comparing Cyclotron Frequencies of Two Ions Simultaneously Trapped in a Penning Trap ATOMIC MASSES 28Si, 31P; measured the cyclotron frequency ratios; deduced atomic masses. Cryogenic penning trap.
doi: 10.1103/PhysRevLett.100.093002
2007RE03 Phys.Rev.Lett. 98, 053003 (2007) M.Redshaw, E.Wingfield, J.McDaniel, E.G.Myers Mass and Double-Beta-Decay Q Value of 136Xe ATOMIC MASSES 136Xe; measured mass; deduced Q-value for 2β-decay.
doi: 10.1103/PhysRevLett.98.053003
2006RE19 Int.J. Mass Spectrom. 251, 125 (2006) M.Redshaw, J.McDaniel, W.Shi, E.G.Myers Mass ratio of two ions in a Penning trap by alternating between the trap center and a large cyclotron orbit ATOMIC MASSES 13C, 14N, 28Si, 31P; measured masses and ratio of ionic masses using Penning trap measurement.
doi: 10.1016/j.ijms.2006.01.015
2005RA34 Nature(London) 438, 1096 (2005) S.Rainville, J.K.Thompson, E.G.Myers, J.M.Brown, M.S.Dewey, E.G.Kessler, R.D.Deslattes, H.G.Borner, M.Jentschel, P.Mutti, D.E.Pritchard A direct test of E=mc2 ATOMIC MASSES 28,29Si, 32,33S; measured mass ratios. Penning trap.
doi: 10.1038/4381096a
2005SH38 Phys.Rev. A 72, 022510 (2005) Atomic masses of 32, 33S, 84, 86Kr, and 129, 132Xe with uncertainties ≤ 0.1 ppb ATOMIC MASSES 32,33S, 84,86Kr, 129,132Xe; measured masses. Penning trap.
doi: 10.1103/PhysRevA.72.022510
2003KE05 Phys.Rev. C 67, 044604 (2003) N.Keeley, T.L.Drummer, E.E.Bartosz, C.R.Brune, P.D.Cathers, M.Fauerbach, H.J.Karwowski, K.W.Kemper, B.Kozlowska, E.J.Ludwig, F.Marechal, A.J.Mendez, E.G.Myers, D.Robson, K.Rusek, K.D.Veal Multistep processes in the 12C(6Li, d) stripping reaction NUCLEAR REACTIONS 12C(polarized 6Li, d), E=34, 50 MeV; measured σ(E, θ), analyzing powers; deduced multistep transfer contributions. Coupled reaction channels calculations.
doi: 10.1103/PhysRevC.67.044604
2002KE04 Phys.Rev. C65, 044613 (2002) N.Keeley, E.E.Bartosz, P.D.Cathers, M.W.Cooper, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt, K.Rusek 7Li + 12C: Complete sets of analyzing powers for inelastic scattering and single-nucleon stripping NUCLEAR REACTIONS 12C(polarized 7Li, 7Li'), (polarized 7Li, 6Li), (polarized 7Li, 6He), E=34 MeV; measured σ(E, θ), analyzing powers. Coupled channels analysis.
doi: 10.1103/PhysRevC.65.044613
2001CA03 Nucl.Instrum.Methods Phys.Res. A457, 509 (2001); Erratum Nucl.Instrum.Methods Phys.Res. A491, 349 (2002) P.D.Cathers, P.V.Green, E.E.Bartosz, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt Secondary Standards for 7Li Beam Polarimetry NUCLEAR REACTIONS 4He(polarized 7Li, 7Li'), E=31.5 MeV; measured σ(θ), T20, iT11 vs θ, other analyzing powers. Use as secondary polarization standard discussed.
doi: 10.1016/S0168-9002(00)00770-1
2001CA25 Phys.Rev. C63, 064601 (2001) P.D.Cathers, E.E.Bartosz, M.W.Cooper, N.Curtis, N.Keeley, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt, K.Rusek, V.Hnizdo First Complete Set of Spin 3/2 Nuclear Scattering Analyzing Powers NUCLEAR REACTIONS 4He(polarized 7Li, 7Li), E(cm)=11.5, 16.5 MeV; measured σ(θ), analyzing powers. Optical model analysis.
doi: 10.1103/PhysRevC.63.064601
2000MY02 Hyperfine Interactions 127, 323 (2000) E.G.Myers, J.K.Thompson, H.S.Margolis, J.D.Silver, M.R.Tarbutt Lamb shift, fine structure and hyperfine structure in helium-like ions by fast-beam laser spectroscopy NUCLEAR MOMENTS 14,15N, 19F, 24Mg; measured hfs. Doppler-tuned fast-beam laser spectroscopy.
doi: 10.1023/A:1012684710414
1999DR04 Phys.Rev. C59, 2574 (1999) T.L.Drummer, E.E.Bartosz, P.D.Cathers, M.Fauerbach, K.W.Kemper, E.G.Myers, K.Rusek Role of Spin Effects in 12C(6Li(pol), d)16Og.s. NUCLEAR REACTIONS 12C(polarized 6Li, d), E=50 MeV; measured σ(θ), analyzing powers iT11, T20, T21, T22; deduced spin-orbit forces, spectroscopic factors. Finite-range DWBA calculations.
doi: 10.1103/PhysRevC.59.2574
1997KE04 Phys.Rev. C55, 2441 (1997) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, B.G.Schmidt Analyzing Powers for Mirror States in 12C(6Li, 7Li/7Be) at E(6Li) = 50 MeV: Evaluation of channel coupling NUCLEAR REACTIONS 12C(polarized 6Li, 7Li), (polarized 6Li, 7Be), E=50 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced optical model, double folding, coupling strength parameters, spectroscopic amplitudes. Finite-range DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.55.2441
1996GR08 Phys.Rev. C53, 2862 (1996) P.V.Green, K.V.Kemper, P.L.Kerr, K.Mohajeri, E.G.Myers, D.Robson, K.Rusek, I.J.Thompson Analyzing Powers in 4He(6Li(pol), 6Li)4He NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E ≤ 27.8 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. Optical model with, without α exchange process.
doi: 10.1103/PhysRevC.53.2862
1996KE09 Phys.Rev. C54, 1267 (1996) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, B.G.Schmidt, V.Hnizdo 6Li(pol) + 12C Inelastic Scattering at 30 and 50 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30, 50 MeV; measured iT11(θ), T20(θ), T21(θ), T22(θ), σ(θ). 6Li(12C, 12C), E=100 MeV; measured σ(θ); deduced optical model parameters. 6Li, 12C levels deduced deformation length parameters. Coupled channels method.
doi: 10.1103/PhysRevC.54.1267
1996ME08 Phys.Rev.Lett. 76, 4899 (1996) E.G.Myers, D.J.H.Howie, J.K.Thompson, J.D.Silver Hyperfine-Induced 1s2s1S0-1s2p3P0 Transition and Fine-Structure Measurement in Heliumlike Nitrogen
doi: 10.1103/PhysRevLett.76.4899
1995KE10 Phys.Rev. C52, 1924 (1995) P.L.Kerr, K.W.Kemper, P.V.Green, K.Mohajeri, E.G.Myers, D.Robson, B.G.Schmidt Tensor Effects in 6Li(pol) + 12C Scattering NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=30, 50 MeV; 4He(polarized 6Li, α), E=50 MeV; measured σ(θ), complete set of analyzing powers; deduced optical model parameters.
doi: 10.1103/PhysRevC.52.1924
1995ME02 Phys.Rev. C51, 651 (1995) A.J.Mendez, K.W.Kemper, P.V.Green, P.L.Kerr, E.G.Myers, E.L.Reber, D.Robson Analyzing Powers for the 12C(6Li(pol), α)14N(*) Reaction at 33 MeV NUCLEAR REACTIONS 12C(polarized 6Li, α), E=33 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 14N levels deduced configurations, spectroscopic amplitudes. DWBA, finite-range deuteron cluster factor.
doi: 10.1103/PhysRevC.51.651
1994KE02 Phys.Lett. 321B, 183 (1994) K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, E.L.Reber, K.Rusek, G.Tungate J Dependence in 12C(6Li(pol), 3He) NUCLEAR REACTIONS 12C(polarized 6Li, 3He), E=34 MeV; measured σ(θ), σ(E(3He)), iT11(θ); deduced model parameters. 15N level deduced possible J, π. Coupled-channels Born approximation, cluster transfer.
doi: 10.1016/0370-2693(94)90461-8
1994ME04 Nucl.Phys. A567, 655 (1994) A.J.Mendez, P.V.Green, K.W.Kemper, P.L.Kerr, E.G.Myers, E.L.Reber, B.G.Schmidt An Absolute Standard for 6Li Vector Analyzing Powers NUCLEAR REACTIONS 12C(polarized 6Li, d), E=33 MeV; measured σ(θ), Eα, tensor analyzing power vs θ; deduced 6Li vector analyzing power absolute standard.
doi: 10.1016/0375-9474(94)90030-2
1994RE01 Phys.Rev. C49, R1 (1994) E.L.Reber, K.W.Kemper, P.V.Green, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt Spin-Orbit and Tensor Potentials from Polarized 6Li Scattering NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=30 MeV; measured σ(θ), vector, tensor analyzing power vs θ; deduced model parameters, tensor potential need.
doi: 10.1103/PhysRevC.49.R1
1994RE15 Phys.Rev. C50, 2917 (1994) E.L.Reber, K.W.Kemper, P.V.Green, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 12C at 30 MeV NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=30 MeV; measured σ(θ), vector, tensor analyzing power vs θ. 6Li, 12C levels deduced deformation lengths. Coupled-channels analysis.
doi: 10.1103/PhysRevC.50.2917
1993ME11 Nucl.Instrum.Methods Phys.Res. A329, 37 (1993) A.J.Mendez, E.G.Myers, K.W.Kemper, P.L.Kerr, E.L.Reber, B.G.Schmidt Determination of the On-Target Polarization of an Optically-Pumped Polarized Lithium Ion Beam NUCLEAR REACTIONS 12C(polarized 6Li, α), E=33 MeV; measured σ(Eα), on-target t20(θ) for beam. Optically pumped polarized lithium ion source.
doi: 10.1016/0168-9002(93)90920-D
1993MY01 Nucl.Instrum.Methods Phys.Res. A334, 271 (1993) E.G.Myers, A.J.Mendez, K.W.Kemper, P.L.Kerr, E.L.Reber, B.G.Schmidt Transport of Polarized Ions Through a Tandem-Superconducting-Linac Heavy-Ion Accelerator NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=20 MeV; measured on target beam polarization variation; deduced beam polarization loss mechanisms.
doi: 10.1016/0168-9002(93)90784-F
1993RE04 Phys.Rev. C47, 2190 (1993) E.L.Reber, K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, N.M.Clarke Analyzing Powers for 9Be(6Li(pol), 6He)9B NUCLEAR REACTIONS 9Be(polarized 6Li, 6He), E=32 MeV; measured σ(θ), vector, tensor analyzing powers vs θ. 9B levels deduced spectroscopic amplitudes. Shell model.
doi: 10.1103/PhysRevC.47.2190
1993RE08 Phys.Rev. C48, 285 (1993) E.L.Reber, K.W.Kemper, P.L.Kerr, A.J.Mendez, E.G.Myers, B.G.Schmidt, V.Hnizdo Analyzing Powers for Elastic and Inelastic Scattering of Polarized 6Li from 9Be at 32 MeV NUCLEAR REACTIONS 9Be(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=32 MeV; measured vector, tensor analyzing power vs θ; deduced optical potential constraints, parameters. Coupled-channels calculations.
doi: 10.1103/PhysRevC.48.285
1990TR02 Phys.Rev. C41, 2134 (1990) D.E.Trcka, A.D.Frawley, K.W.Kemper, D.Robson, J.D.Fox, E.G.Myers Angular Momentum Dependent Absorption in 6Li Scattering NUCLEAR REACTIONS 12C(6Li, 6Li), E=20, 50 MeV; 9Be, 16O, 12C(6Li, 6Li'), 9Be, 16O(6Li, 6Li), E=50 MeV; measured σ(θ); deduced model parameters. Optical model.
doi: 10.1103/PhysRevC.41.2134
1989DE36 Phys.Rev. C40, R1851 (1989) M.R.Deakin, J.D.Fox, K.W.Kemper, E.G.Myers, W.N.Shelton, J.G.Skofronick Search for Cold Fusion using X-Ray Detection NUCLEAR REACTIONS 2H(d, X), E=low; measured X-ray spectra; deduced cold fusion rate upper limit.
doi: 10.1103/PhysRevC.40.R1851
1987MU13 Phys.Rev.Lett. 59, 1088 (1987) D.E.Murnick, E.G.Myers, M.M.Lowry, F.P.Calaprice Laser-Induced Change in Nuclear Reaction Rate: 6Li(α, γ)10B NUCLEAR REACTIONS 6Li(α, γ), E=1276 keV; measured reaction σ; deduced target polarization dependence. Laser-polarized lithium vapor, NaI detectors.
doi: 10.1103/PhysRevLett.59.1088
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