NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Williams Found 78 matches. 2009CA12 Phys.Rev. C 79, 045810 (2009) J.D.Carroll, D.B.Leinweber, A.G.Williams, A.W.Thomas Phase transition from quark-meson coupling hyperonic matter to deconfined quark matter
doi: 10.1103/PhysRevC.79.045810
2007WA13 Phys.Rev. C 75, 045202 (2007) P.Wang, A.W.Thomas, A.G.Williams Phase transition from hadronic matter to quark matter
doi: 10.1103/PhysRevC.75.045202
2006LE26 Phys.Rev.Lett. 97, 022001 (2006) D.B.Leinweber, S.Boinepalli, A.W.Thomas, P.Wang, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Strange Electric Form Factor of the Proton NUCLEAR STRUCTURE 1H; calculated strange electric charge radius, form factor.
doi: 10.1103/PhysRevLett.97.022001
2005LE08 Eur.Phys.J. A 24, Supplement 2, 79 (2005) D.B.Leinweber, S.Boinepalli, A.W.Thomas, A.G.Williams, R.D.Young, J.B.Zhang, J.M.Zanotti Systematic uncertainties in the precise determination of the strangeness magnetic moment of the nucleon NUCLEAR STRUCTURE 1n, 1H; analyzed μ, strangeness magnetic moment.
doi: 10.1140/epjad/s2005-04-017-y
2005LE22 Phys.Rev.Lett. 94, 212001 (2005) D.B.Leinweber, S.Boinepalli, I.C.Cloet, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Precise Determination of the Strangeness Magnetic Moment of the Nucleon NUCLEAR MOMENTS 1H; calculated strange magnetic moment. Comparison with data.
doi: 10.1103/PhysRevLett.94.212001
2005WA03 Nucl.Phys. A748, 226 (2005) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams Liquid-gas phase transition and Coulomb instability of asymmetric nuclear systems
doi: 10.1016/j.nuclphysa.2004.10.012
2005WA32 Phys.Rev. C 72, 045801 (2005) P.Wang, S.Lawley, D.B.Leinweber, A.W.Thomas, A.G.Williams Neutron stars and strange stars in the chiral SU(3) quark mean field model
doi: 10.1103/PhysRevC.72.045801
2004LE18 Nucl.Phys. A737, 177 (2004) D.B.Leinweber, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Observing Chiral Nonanalytic Behavior with FLIC Fermions
doi: 10.1016/j.nuclphysa.2004.03.060
2004WA30 Nucl.Phys. A744, 273 (2004) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams New treatment of the chiral SU(3) quark mean field model NUCLEAR STRUCTURE 16O, 208Pb; calculated charge density distributions, single-particle energy levels. 4,5,6He, 7,8,9Li, 7,8,9,10Be, 10,11,12B, 15N, 40Ca, 51V, 89Y; calculated hypernucleus binding energies. Chiral SU(3) quark mean field model.
doi: 10.1016/j.nuclphysa.2004.08.015
2004WA32 Phys.Rev. C 70, 055204 (2004) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams Liquid-gas phase transition in nuclear matter including strangeness
doi: 10.1103/PhysRevC.70.055204
2003LE29 Eur.Phys.J. A 18, 247 (2003) D.B.Leinweber, J.N.Hedditch, W.Melnitchouk, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang FLIC fermions and hadron phenomenology
doi: 10.1140/epja/i2002-10209-3
2003LE33 Prog.Theor.Phys.(Kyoto), Suppl. 151, 138 (2003) D.B.Leinweber, J.N.Hedditch, W.Melnitchouk, A.G.Williams, J.M.Zanotti Nucleon Resonances from FLIC Fermions
doi: 10.1143/PTPS.151.138
2001WI04 Nucl.Phys. A680, 204c (2001) Connections between Lattice QCD and Hadron Phenomenology
doi: 10.1016/S0375-9474(00)00416-4
1999LU11 Phys.Rev. C60, 068201 (1999) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito Electromagnetic Form Factors of the Bound Nucleon NUCLEAR STRUCTURE 4He, 16O, 40Ca, 208Pb; calculated bound proton electric, magnetic form factors.
doi: 10.1103/PhysRevC.60.068201
1998LU01 Phys.Lett. 417B, 217 (1998) D.H.Lu, A.W.Thomas, K.Tsushima, A.G.Williams, K.Saito In-Medium Electron-Nucleon Scattering
doi: 10.1016/S0370-2693(97)01385-3
1998LU03 Phys.Rev. C57, 2628 (1998) D.H.Lu, A.W.Thomas, A.G.Williams Electromagnetic Form Factors of the Nucleon in an Improved Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors; deduced Lorentz contraction effect. Cloudy bag model. Comparisons with data.
doi: 10.1103/PhysRevC.57.2628
1998LU06 Nucl.Phys. A634, 443 (1998) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito Medium Dependence of the Bag Constant in the Quark-Meson Coupling Model
doi: 10.1016/S0375-9474(98)00181-X
1998LU16 Phys.Lett. 441B, 27 (1998) D.H.Lu, K.Tsushima, A.W.Thomas, A.G.Williams, K.Saito The Neutron Charge Form Factor in Helium-3 NUCLEAR STRUCTURE 1n, 3He; calculated neutron charge form factor; deduced medium effects.
doi: 10.1016/S0370-2693(98)01196-4
1998MO09 Phys.Lett. 419B, 25 (1998) C.L.Morris, J.D.Zumbro, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Reidel, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, J.Ouyang, R.J.Peterson, J.E.Wise Evidence for Δ+ Components in Nuclei NUCLEAR REACTIONS 12,13C, 90Zr, 208Pb(π+, π+p), (π+, π-p), E=500 MeV; measured σ(DCX)/σ(NCX); deduced nuclear wave function Δ+ components.
doi: 10.1016/S0370-2693(97)01453-6
1998SA27 Phys.Lett. 433B, 243 (1998) K.Saito, K.Tsushima, A.W.Thomas, A.G.Williams σ and ω Meson Propagation in a Dense Nuclear Medium
doi: 10.1016/S0370-2693(98)00702-3
1998WI07 Nucl.Phys. A629, 464c (1998) A.G.Williams, H.B.O'Connell, A.W.Thomas On Extracting the ρ-ω Mixing Amplitude from the Pion Form-Factor
doi: 10.1016/S0375-9474(97)00723-9
1998WI12 Nucl.Phys. A631, 553c (1998) Convariant Solutions of the Bethe-Salpeter Equation and an Application to the Nucleon Structure Function
doi: 10.1016/S0375-9474(98)00066-9
1997CL01 Phys.Rev. C55, 625 (1997) B.L.Clausen, T.W.Johnson, R.A.Lindgren, K.Cromer, R.J.Peterson, A.D.Bacher, H.Ward, A.L.Williams Pion Scattering to 6- Stretched States in 32S NUCLEAR REACTIONS 32S(π+, π+), (π-, π-'), E=162 MeV; measured spectra, σ(θ). 32S levels deduced spectroscopic factors, isoscalar, isovector magnetic structure coefficients.
doi: 10.1103/PhysRevC.55.625
1997DR03 Nucl.Phys. A614, 137 (1997) S.Drissi, P.A.Tercier, H.G.Borner, M.Deleze, F.Hoyler, S.Judge, J.Kern, S.J.Mannanal, G.Mouze, K.Schreckenbach, J.P.Vorlet, N.Warr, A.Williams, C.Ythier The 112Cd Laboratory: An extension. E0 strengths, multiphonon states and coupled vibrations NUCLEAR REACTIONS 110Pd(α, 2nγ), E=12.2, 14.9, 16.2, 18 MeV; measured Eγ, Iγ, σ(E, Eγ), γγ-coin. 111Cd(n, γ), E=thermal; measured Eγ, Iγ, I(ce); deduced Q. 112Cd deduced levels, J, π, B(λ). Enriched targets, Compton suppressed Ge detectors, pair-spectrometer, curved-crystal spectrometer, magnetic spectrometer. Interacting boson model.
doi: 10.1016/S0375-9474(96)00451-4
1997KA22 Phys.Rev. C55, 2533 (1997) G.Kahrimanis, G.Burleson, C.M.Chen, B.C.Clark, K.Dhuga, D.J.Ernst, J.A.Faucett, H.T.Fortune, S.Hama, A.Hussein, M.F.Jiang, K.W.Johnson, L.Kurth Kerr, S.Mathews, J.McGill, C.F.Moore, S.Mordechai, C.L.Morris, J.O'Donnell, M.Snell, M.Rawool-Sullivan, L.Ray, C.Whitley, A.L.Williams Pion-Nucleus Elastic Scattering on 12C, 40Ca, 90Zr, and 208Pb at 400 and 500 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(π+, π+), (π-, π-), E=400, 500 MeV; 90Zr(π+, π+), E=400, 500 MeV; 90Zr(π-, π-), E=400 MeV; measured σ(θ). 208Pb(π+, π+), (π-, π-), E=662.7 MeV; 40Ca(π+, π+), (π-, π-), 12C(π+, π+), E=672.5 MeV; 12C(π-, π-), E=672.5, 486.2 MeV; analyzed σ(θ). Impulse approximation approach.
doi: 10.1103/PhysRevC.55.2533
1997LU04 Phys.Rev. C55, 3108 (1997) D.H.Lu, A.W.Thomas, A.G.Williams Chiral Bag Model Approach to Δ Electroproduction
doi: 10.1103/PhysRevC.55.3108
1997OC02 Nucl.Phys. A623, 559 (1997) H.B.O'Connell, A.W.Thomas, A.G.Williams Extracting the ρ-ω Mixing Amplitude from the Pion Form-Factor
doi: 10.1016/S0375-9474(97)00378-3
1996BY03 Europhys.Lett. 33, 187 (1996) J.Byrne, P.G.Dawber, C.G.Habeck, S.J.Smidt, J.A.Spain, A.P.Williams A Revised Value for the Neutron Lifetime Measured using a Penning Trap RADIOACTIVITY 1n(β-); measured T1/2. Penning trap measurement.
doi: 10.1209/epl/i1996-00319-x
1996MA23 Phys.Lett. 376B, 19 (1996) K.Maltman, H.B.O'Connell, A.G.Williams Analysis of Rho-Omega Interference in the Pion Form-Factor
doi: 10.1016/0370-2693(96)00293-6
1996OC01 Phys.Lett. 370B, 12 (1996) H.B.O'Connell, A.G.Williams, M.Bracco, G.Krein Vector Meson Mixing and Charge Symmetry Violation
doi: 10.1016/0370-2693(95)01579-5
1995OC01 Phys.Lett. 354B, 14 (1995) H.B.O'Connell, B.C.Pearce, A.W.Thomas, A.G.Williams Rho-Omega Mixing and the Pion Electromagnetic Form-Factor
doi: 10.1016/0370-2693(95)00642-X
1995WI09 Phys.Rev. C51, 1144 (1995) A.L.Williams, W.P.Alford, E.Brash, B.A.Brown, S.Burzynski, H.T.Fortune, O.Hausser, R.Helmer, R.Henderson, P.P.Hui, K.P.Jackson, B.Larson, M.G.McKinzie, D.A.Smith, A.Trudel, M.Vetterli Gamow-Teller Strength in 60,62,64Ni(n, p) Reactions at 198 MeV NUCLEAR REACTIONS 60,62,64Ni(n, p), E=198 MeV; measured σ(θ, Ep). 60,62,64Co deduced Gamow-Teller transition strength. Multipole analyses.
doi: 10.1103/PhysRevC.51.1144
1994FO12 Phys.Rev. C50, 2927 (1994) Isospin Dependence of Double Analog Cross Sections at T(π) = 400-500 MeV NUCLEAR STRUCTURE A=14-80; analyzed pion-induced double charge exchange σ(θ) data; deduced isospin dependence.
doi: 10.1103/PhysRevC.50.2927
1994JE02 Phys.Rev. C49, 1981 (1994) H.-C.Jean, J.Piekarewicz, A.G.Williams Medium Modifications to the (Omega)-Meson Mass in the Walecka Model
doi: 10.1103/PhysRevC.49.1981
1994MC02 Phys.Rev. C49, 2054 (1994) M.G.McKinzie, H.T.Fortune, P.Hui, R.Ivie, C.Laymon, X.Li, S.Loe, D.A.Smith, A.L.Williams, J.M.O'Donnell, S.Blanchard, G.R.Burleson, B.Lail Interference Effects in Nonanalog Pion Double Charge Exchange NUCLEAR REACTIONS 27Al(π+, π-), E=100-293 MeV; measured σ(θ) vs E; deduced nonanalog pion double charge exchange interference effects.
doi: 10.1103/PhysRevC.49.2054
1994OC01 Phys.Lett. 336B, 1 (1994) H.B.O'Connell, B.C.Pearce, A.W.Thomas, A.G.Williams Constraints on the Momentum Dependence of Rho-Omega Mixing
doi: 10.1016/0370-2693(94)00991-0
1994RA02 Phys.Rev. C49, 627 (1994) M.W.Rawool-Sullivan, C.L.Morris, J.M.O'Donnell, R.M.Whitton, B.K.Park, G.R.Burleson, D.L.Watson, J.Johnson, A.L.Williams, D.A.Smith, D.J.Ernst, C.M.Chen Pion Elastic Scattering on 28Si at T(π) = 400 MeV NUCLEAR REACTIONS 28Si(π+, π+), (π-, π-), E=400 MeV; measured σ(θ), σ(E(π), θ(π)). Momentum-space first-order optical model.
doi: 10.1103/PhysRevC.49.627
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
1993BE18 Phys.Lett. 305B, 13 (1993) D.P.Beatty, R.Gilman, Q.Sun, H.T.Fortune, A.L.Williams, D.A.Smith, P.Hui, S.Loe, M.A.Landau, J.M.O'Donnell, M.Rawool-Sullivan, J.Urbina, D.L.Watson Pion Double Charge Exchange on 16O Above the Δ(1232) Resonance NUCLEAR REACTIONS 16O(π+, π-), E=100-300 MeV; measured σ(θ) vs E.
doi: 10.1016/0370-2693(93)91098-8
1993BE34 Phys.Rev. C48, 1428 (1993) D.P.Beatty, G.R.Burleson, M.Rawool-Sullivan, M.El-Ghossain, H.T.Fortune, A.L.Williams, D.A.Smith, C.L.Morris, R.Garnett, D.L.Watson, J.Johnson, H.Ward, C.Whitley, S.K.Matthews, M.Palarczyk, C.Edwards, M.Espy, O.Hashimoto, H.Tomoyuki Pion Double Charge Exchange on 16O at T(π) = 300-500 MeV NUCLEAR REACTIONS 16O(π+, π-), E=300-500 MeV; measured σ(θ) vs E; deduced reaction mechanism.
doi: 10.1103/PhysRevC.48.1428
1993DE01 Nucl.Phys. A551, 269 (1993) M.Deleze, S.Drissi, J.Kern, P.A.Tercier, J.P.Vorlet, J.Rikovska, T.Otsuka, S.Judge, A.Williams Systematic Study of the Mixed Ground-State and ' Intruder ' Bands in 110,112,114Cd NUCLEAR REACTIONS 110Pd(α, 2nγ), E=19.8-29.9 MeV; measured Eγ, Iγ, σ(E, Eγ, θ), γγ-coin, γ(t); 111Cd(n, γ), E=thermal; measured Eγ, Iγ, I(ce). 112Cd deduced levels, J, π, δ, B(λ). Enriched targets, Ge detectors, BGO-NaI(Tl) anti-Compton shield, magnetic spectrometer. Interacting-boson model.
doi: 10.1016/0375-9474(93)90482-D
1993HA05 Z.Phys. A345, 143 (1993) A.Harder, S.Michaelsen, K.P.Lieb, A.P.Williams Thermal Neutron Capture γ-Ray Spectroscopy of 59Ni and 61Ni NUCLEAR REACTIONS 58,60Ni(n, γ), E=thermal; measured Eγ, Iγ. 59,61Ni deduced levels, J, π, γ-transitions, neutron binding energies. NUCLEAR STRUCTURE A=30-80; compiled level density parameters; deduced shell structure effects.
doi: 10.1007/BF01293337
1993JO03 Phys.Rev. C47, 2571 (1993) J.D.Johnson, G.R.Burleson, C.Edwards, M.El'Ghossain, M.A.Espy, R.Garnett, A.Hussein, K.Johnson, C.F.Moore, C.L.Morris, J.M.O'Donnell, M.Palarczyk, M.Rawool-Sullivan, H.Ward, D.Watson, C.Whitley, A.L.Williams Search for an (Eta) Bound State in Pion Double Charge Exchange on 18O NUCLEAR REACTIONS 18O(π+, π-), E=350-440 MeV; measured missing mass spectra, σ(θ) vs E; deduced no structure near eta production threshold.
doi: 10.1103/PhysRevC.47.2571
1993KA03 Phys.Rev. C47, 1219 (1993) M.A.Kagarlis, H.T.Fortune, P.Hui, S.Loe, D.A.Smith, A.L.Williams, J.Urbina Double Charge Exchange in 93Nb(π+, π-)93Tc at T(π) = 164, 230, and 294 MeV NUCLEAR REACTIONS 93Nb(π+, π-), E=164-294 MeV; measured spectra, σ(θ). 93Tc deduced levels, double IAS excitation.
doi: 10.1103/PhysRevC.47.1219
1993MI04 Nucl.Phys. A552, 232 (1993) S.Michaelsen, A.Harder, K.P.Lieb, G.Graw, R.Hertenberger, D.Hofer, P.Schiemenz, E.Zanotti, H.Lenske, A.Weigel, H.H.Wolter, S.J.Robinson, A.P.Williams Complete Spectroscopy of 90Y via the 89Y(n, γ) and 89Y(d(pol), p) Reactions NUCLEAR REACTIONS 89Y(n, γ), E=thermal; measured Eγ, Iγ. 89Y(polarized d, p), E=22 MeV; measured σ(θ), vector analyzing power A(y)(θ). 90Y deduced levels, J, π, neutron binding energy, level density. Comparison with shell model, RPA calculations.
doi: 10.1016/0375-9474(93)90465-A
1993WI15 Phys.Rev. C48, 1840 (1993) J.E.Wise, M.R.Braunstein, S.Hoibraten, M.D.Kohler, B.J.Kriss, J.Ouyang, R.J.Peterson, J.A.McGill, C.L.Morris, S.J.Seestrom, R.M.Whitton, J.D.Zumbro, C.M.Edwards, A.L.Williams Quasifree Pion Scattering at 500 MeV NUCLEAR REACTIONS C(π+, π+), (π-, π-), E=500 MeV; measured σ(θ) vs energy loss, σ(θ). Ca, Zr, Pb(π+, π+), (π-, π-), E=500 MeV; measured σ(θ); deduced surface single nucleon knockout evidence.
doi: 10.1103/PhysRevC.48.1840
1993ZU01 Phys.Rev.Lett. 71, 1796 (1993) J.D.Zumbro, C.L.Morris, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Edwards, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, R.J.Peterson, J.Ouyang, J.E.Wise, W.R.Gibbs Inclusive Scattering of 500-MeV Pions from Carbon NUCLEAR REACTIONS C(π+, π+X), (π-, π-X), E=500 MeV; measured inclusive σ(θ, E(π)); deduced comparison with (e, e'X).
doi: 10.1103/PhysRevLett.71.1796
1992HA21 Z.Phys. A343, 7 (1992) A.Harder, S.Michaelsen, A.Jungclaus, K.P.Lieb, A.P.Williams, H.G.Borner, M.Trautmannsheimer Double Neutron Capture in 62Ni NUCLEAR REACTIONS 62Ni(n, γ), E=thermal; measured Eγ, Iγ. 63,64Ni deduced levels, J, π, transition Iγ. Double neutron capture on 62Ni leads to 63Ni(n, γ) reaction.
doi: 10.1007/BF01291590
1992JO03 Phys.Rev. C46, 52 (1992) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction Near the P33 π-Nucleon Resonance NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.
doi: 10.1103/PhysRevC.46.52
1991BR21 Phys.Rev. C44, 2031 (1991) B.Brinkmoller, C.L.Blilie, D.Dehnhard, M.K.Jones, G.M.Martinez, S.K.Nanda, S.M.Sterbenz, Y.-F.Yen, L.G.Atencio, S.J.Greene, C.L.Morris, S.J.Seestrom, G.R.Burleson, K.S.Dhuga, J.A.Faucett, R.W.Garnett, K.Maeda, C.F.Moore, S.Mordechai, A.Williams, S.H.Yoo, L.C.Bland Elastic Scattering of π+ and π- from 4He between 90 and 240 MeV NUCLEAR REACTIONS 4He(π+, π+), (π-, π-), E=90-240 MeV; measured σ(θ); deduced phase shifts. Optical model analysis.
doi: 10.1103/PhysRevC.44.2031
1991MO02 Phys.Rev. C43, 1111 (1991) S.Mordechai, C.L.Morris, J.M.O'Donnell, M.A.Kagarlis, D.Fink, H.T.Fortune, D.L.Watson, R.Gilman, H.Ward, A.Williams, S.H.Yoo, C.F.Moore Analog of the T(>) Giant Dipole Resonance in Light Nuclei NUCLEAR REACTIONS 13C, 27Al, 59Co(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 13O, 27P, 59Cu deduced giant resonances, Γ, T.
doi: 10.1103/PhysRevC.43.1111
1991OA01 Phys.Rev. C44, 2058 (1991) D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore Energy Dependence of Pion Inelastic Scattering from 208Pb NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=120, 250 MeV; calculated σ(θ). 208Pb levels deduced proton, neutron matrix elements ratio. Different structure models.
doi: 10.1103/PhysRevC.44.2058
1991WA04 Phys.Rev. C43, 1318 (1991) D.L.Watson, R.Gilman, C.L.Morris, J.D.Zumbro, S.Mordechai, M.Burlein, J.M.O'Donnell, H.T.Fortune, A.Kotwal, J.Puttz, J.D.Silk, J.S.McDonald, C.F.Moore, A.L.Williams, S.Y.Yoo Pion-Induced Double Charge Exchange on 12C, 24Mg, 32S, and 40Ca NUCLEAR REACTIONS 12C, 24Mg, 32S, 40Ca(π+, π-), E=164 MeV; measured σ(θ). Isobar-nucleon interaction mechanism.
doi: 10.1103/PhysRevC.43.1318
1991WI03 Phys.Rev. C43, 766 (1991) A.L.Williams, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, D.S.Oakley, M.Burlein, H.T.Fortune, J.M.O'Donnell, G.P.Kahrimanis, C.F.Moore Pion Double Charge Exchange on 42,44,48Ca for 300 ≤ T(π) ≤ 550 MeV NUCLEAR REACTIONS 42,44,48Ca(π+, π-), E=300-550 MeV; measured σ(θ), σ(E(π)); deduced two-amplitude model parameters.
doi: 10.1103/PhysRevC.43.766
1991WI13 Phys.Rev. C44, 2025 (1991) A.L.Williams, K.W.Johnson, G.P.Kahrimanis, H.Ward, C.F.Moore, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, M.Rawool-Sullivan, D.S.Oakley, M.Burlein, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith Mass Dependence of High-Energy Pion Double Charge Exchange NUCLEAR REACTIONS 26Mg, 46,50Ti, 54,56Fe, 52Cr, 80Se, 90Zr, 197Au, 208Pb(π+, π-), E=450, 500 MeV; measured σ(θ), θ=5°; deduced mass dependence, two-amplitude model parameters. Double isobaric analog state excitation.
doi: 10.1103/PhysRevC.44.2025
1991YE01 Phys.Rev.Lett. 66, 1959 (1991) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.1959
1990BY05 Phys.Rev.Lett. 65, 289 (1990) J.Byrne, P.G.Dawber, J.A.Spain, A.P.Williams, M.S.Dewey, D.M.Gilliam, G.L.Greene, G.P.Lamaze, R.D.Scott, J.Pauwels, R.Eykens, A.Lamberty Measurement of Neutron Lifetime by Counting Trapped Protons
doi: 10.1103/PhysRevLett.65.289
1990JO04 Phys.Rev. C42, R807 (1990) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction: Quasifree and resonance scattering NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π+)/σ(π-). DWIA calculation.
doi: 10.1103/PhysRevC.42.R807
1990YE06 J.Phys.(Paris), Colloq.C-6, 587 (1990) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.
1990YO02 J.Phys.(London) G16, L89 (1990) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom, M.Jones, S.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 208Pb(π±, π±'n) Reaction in the Giant-Resonance Region NUCLEAR REACTIONS 208Pb(π+, π+'n), (π-, π-'n), E=180 MeV; measured σ(θn, θπ), missing mass spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1088/0954-3899/16/5/002
1989BY04 Nucl.Instrum.Methods Phys.Res. A284, 116 (1989) J.Byrne, P.G.Dawber, J.A.Spain, M.S.Dewey, D.M.Gilliam, G.L.Greene, G.P.Lamaze, A.P.Williams, J.Pauwels, R.Eykens, J.Van Gestel, A.Lamberty, R.D.Scott Determination of the Neutron Lifetime by Counting Trapped Protons RADIOACTIVITY 1n(β-); measured T1/2. In-beam trapped proton counting technique.
doi: 10.1016/0168-9002(89)90261-1
1989WI02 Phys.Lett. 216B, 11 (1989) A.L.Williams, L.Agnew, L.G.Atencio, H.W.Baer, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, G.S.Kyle, J.A.McGill, C.F.Moore, C.L.Morris, S.Mordechai, J.M.O'Donnell, M.W.Rawool, S.Schilling, J.D.Silk, J.D.Zumbro Pion Double Charge Exchange Above the Δ(1232) Resonance NUCLEAR REACTIONS 14C, 18O(π+, π-), E=300, 400, 500 MeV; measured σ(E(π), θ(π)). 14N, 18Ne deduced double IAS excitation.
doi: 10.1016/0370-2693(89)91360-9
1989YO06 Phys.Rev.Lett. 63, 738 (1989) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom-Morris, M.K.Jones, S.M.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 12C(π±, π±'p)11B Reaction Near the Giant Dipole Region NUCLEAR REACTIONS 12C(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θ(p), E(π)); deduced σ(π+, π+p)/σ(π-, π-p) near GDR. DWIA analysis.
doi: 10.1103/PhysRevLett.63.738
1988AS04 Phys.Lett. 215B, 41 (1988) D.Ashery, J.Lichtenstadt, E.Piasetzky, C.L.Morris, J.D.Zumbro, R.Gilman, M.W.Rawool, S.Mordechai, B.Boyer, A.Fuentes, K.Johnson, J.W.McDonald, M.J.Smithson, A.Williams, S.H.Yoo, C.F.Moore A Search for πNN Bound Systems NUCLEAR REACTIONS 2H(π+, π-), (π-, π+), E=260 MeV; measured possible (πNN) system mass; deduced σ upper limit.
doi: 10.1016/0370-2693(88)91066-0
1988BE29 Phys.Rev. C38, 779 (1988) Model Dependence of Charge-Symmetry Breaking in the Neutron-Proton Interaction NUCLEAR REACTIONS 1n(polarized p, p), E=477 MeV; 1H(polarized n, n), E=477 MeV; calculated analyzing power difference; deduced charge symmetry breaking model dependence. One boson exchange model, DWBA calculation.
doi: 10.1103/PhysRevC.38.779
1988OA03 Phys.Rev. C38, 2978 (1988) D.S.Oakley, R.J.Peterson, D.J.Rilett, C.L.Morris, S.J.Greene, B.Boyer, K.Johnson, A.H.Fuentes, J.W.McDonald, M.J.Smithson, A.L.Williams, S.H.Yoo, C.F.Moore Energy Dependence of Pion Inelastic Scattering to the 1+ States in 12C NUCLEAR REACTIONS 12C(π-, π-'), (π+, π+'), E=80-295 MeV; measured σ(θ); deduced isobar excitation role. 12C levels deduced σ ratio.
doi: 10.1103/PhysRevC.38.2978
1987DH01 Phys.Rev. C35, 1148 (1987) K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, Z.F.Wang, J.W.McDonald, C.F.Moore, S.Mordechai, A.L.Williams, P.A.Seidl, M.A.Bryan, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro Sensitivity of Large-Angle Pion Elastic Scattering to Medium Modifications NUCLEAR REACTIONS 12C, 16O(π+, π+), E=100-240 MeV; measured σ(θ); deduced model parameter modifications. Optical model.
doi: 10.1103/PhysRevC.35.1148
1987WI17 Phys.Rev. C36, 1956 (1987) A.G.Williams, A.W.Thomas, G.A.Miller Charge-Symmetry Breaking in Neutron-Proton Elastic Scattering NUCLEAR REACTIONS 1n(polarized p, p), E=188-800 MeV; analyzed analyzing power difference vs θ. One-boson exchange potentials, charge symmetry breaking.
doi: 10.1103/PhysRevC.36.1956
1986WI03 Phys.Rev. C33, 1070 (1986) Color-Dielectric Model as an Explanation of Nolen-Schiffer Anomaly NUCLEAR STRUCTURE 15,17O, 15N, 17F, 39,41Ca, 39K, 41Sc; calculated proton, neutron binding energy differences in Z(>) nuclei; deduced Nolen-Schiffer anomaly parameters. Color-dielectric model, mirror nuclei.
doi: 10.1103/PhysRevC.33.1070
1974GO26 Int.J.Appl.Radiat.Isotop. 25, 373 (1974) I.W.Goodier, J.L.Makepeace, A.Williams The Branching Ratio in the Decay of Beryllium-7 RADIOACTIVITY 7Be; measured βγ-coin; deduced β-branching ratio.
doi: 10.1016/0020-708X(74)90069-6
1973LE18 Metrologia 9, 14 (1973) V.E.Lewis, D.Smith, A.Williams Correlation Counting Applied to the Determination of Absolute Disintegration Rates for Nuclides with Delayed States RADIOACTIVITY 67Ga; measured Xγ(t). 67Zn level deduced T1/2.
doi: 10.1088/0026-1394/9/1/004
1971SM06 Int.J.Appl.Radiat.Isotop. 22, 615 (1971) A 4πβ-γ Coincidence Method for Mixed Electron-Capture/Positron Emitters: The Absolute Measurement of 68Ga RADIOACTIVITY 68Ga; measured T1/2.
doi: 10.1016/0020-708X(71)90029-9
1970WI14 Nucl.Phys. A153, 665 (1970) The Ratio of Electron Capture to Positon Emission in the Decay of 58Co RADIOACTIVITY 58Co; measured Iβ/Iγ; deduced capture to positon ratio.
doi: 10.1016/0375-9474(70)90800-6
1969RO38 J.Nucl.Energy 23, 205 (1969) J.C.Robertson, T.B.Ryves, E.J.Axton, I.Goodier, A.Williams A Measurement of the Radiative Capture Cross Section of Gold at an Energy of 966 keV NUCLEAR REACTIONS 197Au(n, γ), E=966 keV; measured σ.
doi: 10.1016/0022-3107(69)90002-1
1968WI13 Nucl.Phys. A117, 238 (1968) A Comment on Leutz and Wenninger's Paper on the 22Na Branching Ratio NUCLEAR STRUCTURE 22Na; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90872-5
1966GO22 Nature 210, 614 (1966) Measurement of the Absolute Disintegration Rate of Technetium-99m NUCLEAR STRUCTURE 99Tc; measured not abstracted; deduced nuclear properties.
doi: 10.1038/210614b0
1964WI04 Nucl.Phys. 52, 324 (1964) Measurement of the Ratio of Electron Capture to Positon Emission in the Decay of Na-22 NUCLEAR STRUCTURE 22Na; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90696-0
1950WI10 Phys.Rev. 78, 822 (1950) Correlation in the Direction and Polarization of Two Successive Quanta For Rh106, Co60, and Cs134
doi: 10.1103/PhysRev.78.822
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