NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = G.T.Garvey Found 69 matches. 2022HA17 Phys.Rev. C 105, 055502 (2022) A.C.Hayes, J.Friar, G.M.Hale, G.T.Garvey Angular correlations in the e+e- decay of excited states in 8Be NUCLEAR REACTIONS 7Li(p, γ), E=0.1-1.5 MeV; analyzed σ(E) from 1995ZA03 with R-matrix analysis; deduced M1/E1 ratio; calculated e+e- angular distribution from 18.15-MeV resonance in 8Be. Claimed no evidence of axion decay in the 8Be found.
doi: 10.1103/PhysRevC.105.055502
2018HA01 Phys.Rev.Lett. 120, 022503 (2018) A.C.Hayes, G.Jungman, E.A.McCutchan, A.A.Sonzogni, G.T.Garvey, X.B.Wang Analysis of the Daya Bay Reactor Antineutrino Flux Changes with Fuel Burnup NUCLEAR REACTIONS 235U, 239Pu(n, F), E thermal; analyzed available data; deduced origins of discrepancy between model predictions and the Daya Bay results for antineutrino flux and spectrum.
doi: 10.1103/PhysRevLett.120.022503
2014HA12 Phys.Rev.Lett. 112, 202501 (2014) A.C.Hayes, J.L.Friar, G.T.Garvey, G.Jungman, G.Jonkmans Systematic Uncertainties in the Analysis of the Reactor Neutrino Anomaly
doi: 10.1103/PhysRevLett.112.202501
2010GA11 Phys.Rev. C 81, 055212 (2010) Orbital angular momentum in the nucleon
doi: 10.1103/PhysRevC.81.055212
2003CH78 Phys.Rev.Lett. 91, 211801 (2003) T.H.Chang, M.E.Beddo, C.N.Brown, T.A.Carey, W.E.Cooper, C.A.Gagliardi, G.T.Garvey, D.F.Geesaman, E.A.Hawker, X.C.He, L.D.Isenhower, D.M.Kaplan, S.B.Kaufman, D.D.Koetke, P.L.McGaughey, W.M.Lee, M.J.Leitch, J.M.Moss, B.A.Mueller, V.Papavassiliou, J.C.Peng, P.E.Reimer, M.E.Sadler, W.E.Sondheim, P.W.Stankus, R.S.Towell, R.E.Tribble, M.A.Vasiliev, J.C.Webb, J.L.Willis, G.R.Young, and the FNAL E866/NuSea Collaboration J/ψ Polarization in 800-GeV p-Cu Interactions NUCLEAR REACTIONS Cu(p, X), E=800 GeV; measured J/ψ polarization parameter vs xF, transverse momentum.
doi: 10.1103/PhysRevLett.91.211801
2003GA05 Phys.Rev.Lett. 90, 092302 (2003) Partonic Energy Loss and the Drell-Yan Process NUCLEAR REACTIONS 2H, W(p, X), E=50, 120 GeV; calculated relative Drell-Yan yields, effect of parton energy loss.
doi: 10.1103/PhysRevLett.90.092302
2002AU03 Phys.Rev. C66, 015501 (2002) L.B.Auerbach, R.L.Burman, D.O.Caldwell, E.D.Church, J.B.Donahue, A.Fazely, G.T.Garvey, R.M.Gunasingha, R.Imlay, W.C.Louis, R.Majkic, A.Malik, W.Metcalf, G.B.Mills, V.Sandberg, D.Smith, I.Stancu, M.Sung, R.Tayloe, G.J.VanDalen, W.Vernon, N.Wadia, D.H.White, S.Yellin, and the LSND Collaboration Measurements of Charged Current Reaction of νμ on 12C NUCLEAR REACTIONS 12C(ν, μ-), (ν, μ-X), E=spectrum; measured muon spectra, flux-averaged σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.66.015501
2001AU09 Phys.Rev. C64, 065501 (2001) L.B.Auerbach, R.L.Burman, D.O.Caldwell, E.D.Church, J.B.Donahue, A.Fazely, G.T.Garvey, R.M.Gunasingha, R.Imlay, W.C.Louis, R.Majkic, A.Malik, W.Metcalf, G.B.Mills, V.Sandberg, D.Smith, I.Stancu, M.Sung, R.Tayloe, G.J.VanDalen, W.Vernon, N.Wadia, D.H.White, S.Yellin, and the LSND Collaboration Measurements of Charged Current Reactions of νe on 12C NUCLEAR REACTIONS 12C(ν, e), E ≈ 20-50 MeV; measured σ, σ(E), electron spectra. Comparison with model predictions.
doi: 10.1103/PhysRevC.64.065501
2001GA58 Prog.Part.Nucl.Phys. 47, 203 (2001) Flavor Asymmetry of Light Quarks in the Nucleon Sea
doi: 10.1016/S0146-6410(01)00155-7
2001JO09 Phys.Rev.Lett. 86, 4483 (2001) M.B.Johnson, B.Z.Kopeliovich, I.K.Potashnikova, P.L.McGaughey, J.M.Moss, J.C.Peng, G.T.Garvey, M.J.Leitch, M.R.Adams, D.M.Alde, H.W.Baer, M.L.Bartlett, C.N.Brown, W.E.Cooper, T.A.Carey, G.Danner, G.W.Hoffmann, Y.B.Hsiung, D.M.Kaplan, A.Klein, C.Lee, J.W.Lillberg, R.L.McCarthy, C.S.Mishra, M.J.Wang, and the FNAL E772 Collaboration Energy Loss of Fast Quarks in Nuclei NUCLEAR REACTIONS 2H, C, Ca, Fe, W(p, X), E at 800 GeV/c; measured dimuon Drell-Yan yields; deduced quark energy loss in nuclear environment.
doi: 10.1103/PhysRevLett.86.4483
2000GA26 Prog.Part.Nucl.Phys. 44, 305 (2000) Measurement and Origin of the (u-bar), (d-bar), Asymmetry in the Nucleon Sea NUCLEAR REACTIONS 1,2H(p, X), E=800 GeV; analyzed Drell-Yan yields, related data; deduced quark asymmetry.
doi: 10.1016/S0146-6410(00)00079-X
1999VA12 Phys.Rev.Lett. 83, 2304 (1999) M.A.Vasiliev, M.E.Beddo, C.N.Brown, T.A.Carey, T.H.Chang, W.E.Cooper, C.A.Gagliardi, G.T.Garvey, D.F.Geesaman, E.A.Hawker, X.C.He, L.D.Isenhower, D.M.Kaplan, S.B.Kaufman, D.D.Koetke, W.M.Lee, M.J.Leitch, P.L.McGaughey, J.M.Moss, B.A.Mueller, V.Papavassiliou, J.C.Peng, G.Petitt, P.E.Reimer, M.E.Sadler, W.E.Sondheim, P.W.Stankus, R.S.Towell, R.E.Tribble, J.C.Webb, J.L.Willis, G.R.Young, and the FNAL E866/NuSea Collaboration Parton Energy Loss Limits and Shadowing in Drell-Yan Dimuon Production NUCLEAR REACTIONS Be, Fe, W(p, X), E at 800 GeV/c; measured Drell-Yan production σ per nucleon; deduced role of nuclear shadowing.
doi: 10.1103/PhysRevLett.83.2304
1997AT02 Phys.Rev. C55, 2078 (1997) C.Athanassopoulos, L.B.Auerbach, R.L.Burman, I.Cohen, D.O.Caldwell, B.D.Dieterle, J.B.Donahue, A.M.Eisner, A.Fazely, F.J.Federspiel, G.T.Garvey, M.Gray, R.M.Gunasingha, R.Imlay, K.Johnston, H.J.Kim, W.C.Louis, R.Majkic, J.Margulies, K.McIlhany, W.Metcalf, G.B.Mills, R.A.Reeder, V.Sandberg, D.Smith, I.Stancu, W.Strossman, R.Tayloe, G.J.VanDalen, W.Vernon, N.Wadia, J.Waltz, Y.-X.Wang, D.H.White, D.Works, Y.Xiao, S.Yellin, and the LSND Collaboration Measurements of the Reactions 12C(ν(e), e-)12N(g.s) 12C(ν(e), e-)12N(*) NUCLEAR REACTIONS 12C(ν, e-), E not given; measured σ(E), σ(θ) for residual ground, excited states. Continuum RPA.
doi: 10.1103/PhysRevC.55.2078
1997AT03 Phys.Rev. C56, 2806 (1997) C.Athanassopoulos, L.B.Auerbach, R.L.Burman, D.O.Caldwell, E.Church, I.Cohen, B.D.Dieterle, J.B.Donahue, A.M.Eisner, A.Fazely, F.J.Federspiel, G.T.Garvey, M.Gray, R.M.Gunasingha, R.Imlay, K.Johnston, H.J.Kim, W.C.Louis, R.Majkic, K.McIlhany, W.Metcalf, G.B.Mills, R.A.Reeder, V.Sandberg, D.Smith, I.Stancu, W.Strossman, R.Tayloe, G.J.VanDalen, W.Vernon, N.Wadia, J.Waltz, Y.-X.Wang, D.H.White, D.Works, Y.Xiao, S.Yellin, and the LSND Collaboration Measurements of the Reactions 12C(ν(μ), μ-)12N(g.s.) and 12C(ν(μ), μ-)X NUCLEAR REACTIONS 12C(ν, μ-), E=0-300 MeV spectrum; measured exclusive, inclusive flux-averaged σ; deduced deficit with respect to theory. Pion decay-in-flight neutrino source. Countinuum RPA calculation.
doi: 10.1103/PhysRevC.56.2806
1996AT06 Phys.Rev. C54, 2685 (1996) C.Athanassopoulos, L.B.Auerbach, R.L.Burman, I.Cohen, D.O.Caldwell, B.D.Dieterle, J.B.Donahue, A.M.Eisner, A.Fazely, F.J.Federspiel, G.T.Garvey, M.Gray, R.M.Gunasingha, R.Imlay, K.Johnston, H.J.Kim, W.C.Louis, R.Majkic, J.Margulies, K.McIlhany, W.Metcalf, G.B.Mills, R.A.Reeder, V.Sandberg, D.Smith, I.Stancu, W.Strossman, R.Tayloe, G.J.VanDalen, W.Vernon, N.Wadia, J.Waltz, Y.-X.Wang, D.H.White, D.Works, Y.Xiao, S.Yellin, and the LSND Collaboration Evidence for Neutrino Oscillations from Muon Decay at Rest NUCLEAR REACTIONS 1H(ν-bar, e+), E from μ-decay; measured neutrino oscillation probability.
doi: 10.1103/PhysRevC.54.2685
1995AL03 Phys.Rev. C51, R1065 (1995) M.Albert, C.Athanassopoulos, L.B.Auerbach, D.Bauer, R.Bolton, B.Boyd, R.L.Burman, I.Cohen, D.O.Caldwell, B.D.Dieterle, J.B.Donahue, A.M.Eisner, A.Fazely, F.J.Federspiel, G.T.Garvey, R.M.Gunasingha, V.Highland, J.Hill, R.Imlay, K.Johnston, W.C.Louis, A.Lu, A.K.Mann, J.Margulies, K.McIlhany, W.Metcalf, R.A.Reeder, V.Sandberg, M.Schillaci, D.Smith, I.Stancu, W.Strossman, M.K.Sullivan, G.J.VanDalen, W.Vernon, Y.-X.Wang, D.H.White, D.Whitehouse, D.Works, Y.Xiao, S.Yellin Measurement of the Reaction 12C(ν(μ), μ-)X Near Threshold NUCLEAR REACTIONS 12C(ν, μ-X), E=123.7-280 MeV; measured flux averaged inclusive σ. Fermi gas model, RPA comparison.
doi: 10.1103/PhysRevC.51.R1065
1994LO15 Phys.Lett. 340B, 115 (1994) J.T.Londergan, G.T.Garvey, G.Q.Liu, E.N.Rodionov, A.W.Thomas Drell-Yan Processes as a Probe of Charge Symmetry Violation in the Pion and the Nucleon NUCLEAR STRUCTURE 1,2H; analyzed π+-, π-induced reactions data; deduced pion, nucleon charge symmetry violation features. Drell-Yan processes.
doi: 10.1016/0370-2693(94)91306-4
1994SZ02 Nucl.Phys. A570, 765 (1994) A.Szczurek, J.Speth, G.T.Garvey Meson Cloud in the Nucleon and (d-bar)-(u-bar) Asymmetry from the Drell-Yan Processes NUCLEAR REACTIONS 1H(p, X), (p-bar, X), E not given; calculated differential σ for Δ++ production. Meson cloud model.
doi: 10.1016/0375-9474(94)90082-5
1993GA15 Phys.Rev. C48, 761 (1993) G.T.Garvey, W.C.Louis, D.H.White Determination of Proton Strange Form Factors from νp Elastic Scattering NUCLEAR REACTIONS 1H(ν, ν), (ν-bar, ν-bar), E not given; analyzed data. 1H deduced strange form factors.
doi: 10.1103/PhysRevC.48.761
1992BO01 Phys.Rev.Lett. 68, 780 (1992) J.D.Bowman, G.T.Garvey, C.R.Gould, A.C.Hayes, M.B.Johnson Parity Violation in the Compound Nucleus: The Role of Distant States NUCLEAR STRUCTURE 232Th; calculated parity violating asymmetry; deduced distant states role.
doi: 10.1103/PhysRevLett.68.780
1992DU05 Nucl.Instrum.Methods Phys.Res. A322, 13 (1992) M.Duren, Z.Moroz, M.Veltri, K.Zapfe, H.Mairon, M.Metzger, B.Povh, K.Rith, E.Steffens, F.Stock, D.Toporkov, F.Zetsche, T.-A.Shibata, D.Fick, W.Korsch, G.Graw, W.Haeberli, G.T.Garvey Test of a Polarized Hydrogen Gas Target Based on the Storage Cell Technique NUCLEAR REACTIONS 1H(α, α), E=34.5 MeV; measured integrated yield; deduced target areal density. Polarized target, storage rings usage.
doi: 10.1016/0168-9002(92)90352-5
1992GA14 Phys.Lett. 289B, 249 (1992) G.T.Garvey, S.Krewald, E.Kolbe, K.Langanke Strange Quark Contributions to Neutrino Induced Quasielastic Scattering NUCLEAR REACTIONS 12C(ν, ν'n), (ν, ν'p), E=200 MeV; calculated angle integrated σ, proton-to-neutron yield ratio; deduced strange quark axial form factor sensitivity to yield ratio.
doi: 10.1016/0370-2693(92)91214-T
1992GA21 Nucl.Phys. A546, 369c (1992) Recent Developments in Neutrino Physics
doi: 10.1016/0375-9474(92)90521-K
1985HE08 Phys.Rev. C31, 2190 (1985) Measurement of the 16N(2-, g.s.) → 16O(0+, g.s.) + e- + (ν-Bar(e)) Beta-Decay Branching Ratio RADIOACTIVITY 16N(β-); measured βγ-coin. 16N level deduced β-decay rate. 16O levels deduced β-decay branching ratio. Flatfield magnetic spectrometer, multi-wire position sensitive proportional detector.
doi: 10.1103/PhysRevC.31.2190
1983GA03 Phys.Rev. C27, 1353 (1983) C.A.Gagliardi, G.T.Garvey, N.Jarmie, R.G.H.Robertson 0+ → 0- Beta Decay of 16C RADIOACTIVITY 16C(β-), (β-n) [from 14C(t, p), E=6 MeV]; measured β(t), γ(t), βγ-coin; deduced log ft. 16N levels deduced β-branching ratio.
doi: 10.1103/PhysRevC.27.1353
1983GA18 Phys.Rev. C28, 2423 (1983) C.A.Gagliardi, G.T.Garvey, J.R.Wrobel, S.J.Freedman 16N(0-) Beta Decay and Weak Axial Vector Meson Exchange Currents NUCLEAR REACTIONS 19F(p, α), E=3 MeV; measured σ(Eα), σ(θ). RADIOACTIVITY 16N(β-) [from 15N(d, p), E=3.8 MeV]; measured Eγ, Iγ, Eβ, Iβ, β-decay rate vs t; deduced (gp/g(A)). 16N level deduced β-decay probability. 16O levels deduced Iβ. Calibration with 19F(p, α) reaction. Comparison with theory.
doi: 10.1103/PhysRevC.28.2423
1982GA05 Phys.Rev.Lett. 48, 914 (1982) C.A.Gagliardi, G.T.Garvey, J.R.Wrobel, S.J.Freedman Demonstration of the Need for Meson Exchange Currents in the Beta Decay of 16N(0-) RADIOACTIVITY 16N [from 15N(d, p), E=3.4 MeV]; measured Eβ, Eγ, Iγ, β-decay rate; deduced pseudoscalar, axial vector coupling constant ratio, pion exchange current evidence.
doi: 10.1103/PhysRevLett.48.914
1980MC07 Phys.Rev. C22, 738 (1980); Erratum Phys.Rev. C26, 2336 (1982) R.D.McKeown, G.T.Garvey, C.A.Gagliardi Beta-Alpha Angular Correlations in Mass 8 RADIOACTIVITY 8Li, 8B; measured βα(θ); deduced final state energy dependence. Conserved vector current, second class current tests.
doi: 10.1103/PhysRevC.22.738
1978BO30 Phys.Rev. C18, 1447 (1978); Erratum Phys.Rev. C26, 2336 (1982) Isovector Radiative Decays and Second-Class Currents in Mass 8 Nuclei NUCLEAR REACTIONS 4He(α, γ), E=32-36 MeV; measured σ(E, θ). 8Be resonances deduced radiative widths, δ. Model independent test of CVC, second-class currents.
doi: 10.1103/PhysRevC.18.1447
1977FR08 Phys.Lett. 67B, 165 (1977) S.J.Freedman, R.D.Cousins, Jr., C.A.Gagliardi, G.T.Garvey, J.F.Greenhalgh Beta-Alpha Correlation in the Decay of 20Na RADIOACTIVITY 20Na; measured βα(θ).
doi: 10.1016/0370-2693(77)90093-4
1977LI02 Nucl.Phys. A276, 25 (1977) J.M.Lind, G.T.Garvey, R.E.Tribble Isospin Mixing in 12C NUCLEAR REACTIONS 12C(d, d'), E=24-29 MeV; measured σ(θ), ratio of isospin forbidden to isospin allowed yield. 10B(α, d), E=40 MeV; measured σ(θ), ratio isospin forbidden to isospin allowed yield. 13C(d, t), 13C(d, 3He), E=24-26 MeV; measured σ(θ); 12C, 12B levels deduced S; charge dependent matrix element. DWBA analysis.
doi: 10.1016/0375-9474(77)90157-9
1977OO01 Nucl.Phys. A284, 41 (1977) Isospin-Mixed States in 8Be NUCLEAR REACTIONS 9Be(d, t), (d, 3He), E=27.97 MeV; measured σ(θ). 8Be deduced levels, L, S, T-mixing. Natural target.
doi: 10.1016/0375-9474(77)90684-4
1976DE14 Phys.Rev. C13, 2089 (1976) R.M.Del Vecchio, S.J.Freedman, G.T.Garvey, M.A.Oothoudt Jπ Assignment to the 4.841 MeV Level in 208Pb NUCLEAR REACTIONS 208Pb(α, α'γ), E=35 MeV; measured α'γ(θ). 208Pb level deduced J, π.
doi: 10.1103/PhysRevC.13.2089
1976FR21 Phys.Rev.Lett. 37, 1606 (1976) S.J.Freedman, C.A.Gagliardi, G.T.Garvey, M.A.Oothoudt, B.Svetitsky Magnetic Dipole States in 208Pb NUCLEAR REACTIONS 208Pb(p, p'γ), (d, d'γ), E=24 MeV; measured p'γ-, d'γ-coin. 208Pb deduced B(M1).
doi: 10.1103/PhysRevLett.37.1606
1975DE07 Phys.Rev.Lett. 34, 1296 (1975) R.Del Vecchio, S.Freedman, G.T.Garvey, M.Oothoudt Spin and Parity of the 4.841-MeV Level of 208Pb NUCLEAR REACTIONS 208Pb(α, α'), E=34.6 MeV; measured σ(Eα'), 208Pb level deduced π.
doi: 10.1103/PhysRevLett.34.1296
1975NA12 Phys.Rev.Lett. 35, 1137 (1975) A.M.Nathan, G.T.Garvey, P.Paul, E.K.Warburton M1 Decay Rates and Second-Class Currents in Mass 8 NUCLEAR REACTIONS 4He(α, γ), E=33-36 MeV; measured σ(E, Eγ). 8Be levels deduced M1 Γ.
doi: 10.1103/PhysRevLett.35.1137
1975TR06 Phys.Rev. C12, 967 (1975) Induced Weak Currents and β±-α Angular Correlations in A = 8 RADIOACTIVITY 8Li, 8Be; measured βα(θ); deduced induced weak currents.
doi: 10.1103/PhysRevC.12.967
1974CE03 Nucl.Phys. A232, 22 (1974) F.E.Cecil, G.T.Garvey, W.J.Braithwaite Search for Giant Spin-Flip Transitions in 90Zr and 208Pb NUCLEAR REACTIONS 90Zr, 208Pb(p, p'), (p, p'γ), E=24 MeV; 90Zr, 208Pb(α, α'), E=48 MeV; measured σ(Ep', θ), σ(Eα', θ), pγ-coin. 90Zr deduced levels, J, π, γ-branching ratio. 208Pb deduced levels, π.
doi: 10.1016/0375-9474(74)90643-5
1974DE20 Phys.Rev. C10, 680 (1974) Reaction 42Ca(p, t)40Ca and the Structure of 40Ca NUCLEAR REACTIONS 42Ca(p, t), E=41.7 MeV; measured σ(Et, θ). 40Ca deduced levels, J, π, L, S.
doi: 10.1103/PhysRevC.10.680
1974TR01 Phys.Rev.Lett. 32, 314 (1974) Weak Magnetism and Second-Class - Current Interactions in A = 8 RADIOACTIVITY 8Li, 8B; measured βα(θ).
doi: 10.1103/PhysRevLett.32.314
1973TR05 Phys.Lett. 44B, 366 (1973) R.E.Tribble, G.T.Garvey, J.R.Comfort Particle-Hole Nature of the Two Lowest 3- States in 24Mg NUCLEAR REACTIONS 25Mg(p, d), Ep=28 MeV; 23Na(3He, d), E(3He)=20 MeV; measured σ(Ed, θ). 24Mg deduced levels, L, S, J, π.
doi: 10.1016/0370-2693(73)90408-5
1972AD10 Phys.Rev.Lett. 29, 883 (1972) E.G.Adelberger, P.T.Debevec, G.T.Garvey, R.Ohanian Failure of the Coexistence Model to Account for Observed Two-Neutron Pickup Cross Sections NUCLEAR REACTIONS 18O, 42Ca(p, t), E=41.7 MeV; measured σ(θ); deduced pickup amplitudes, failure of coexistence model.
doi: 10.1103/PhysRevLett.29.883
1972BR27 Phys.Rev.Lett. 29, 376 (1972) W.J.Braithwaite, J.E.Bussoletti, F.E.Cecil, G.T.Garvey Large Isospin-Mixing Matrix Element in 12C NUCLEAR REACTIONS 12C(d, d'), E=27.2, 27.6, 28 MeV; 13C(d, t), (d, 3He), E=28 MeV; measured σ(Ed'), σ(θ). 12C levels deduced isospin mixing, S, β.
doi: 10.1103/PhysRevLett.29.376
1971DE08 Phys.Lett. 34B, 497 (1971) P.T.Debevec, G.T.Garvey, B.E.Hingerty Isospin Purity of the T = 1 States in 6Li NUCLEAR REACTIONS 7Li(d, t), (d, 3He), E=23.6 MeV; measured σ(Et), σ(E(3He)). 6Li levels deduced high isospin purity.
doi: 10.1016/0370-2693(71)90664-2
1971GA01 Nucl.Phys. A160, 25 (1971) G.T.Garvey, K.W.Jones, L.E.Carlson, D.A.Hutcheon, A.G.Robertson, D.F.H.Start Lifetimes of the First Four Excited States of 32S NUCLEAR REACTIONS 32S(α, α'), E=14.39, 14.50 MeV; measured Doppler shift attenuation. 32S levels deduced T1/2.B(E2).
doi: 10.1016/0375-9474(70)90171-5
1971GA17 Phys.Lett. 35B, 563 (1971) G.T.Garvey, K.W.Jones, D.Schwalm, E.K.Warburton Branching in the β+ Decay of the 42Sc Ground State NUCLEAR REACTIONS 42Ca(p, nγ), E=7.8-9 MeV; measured σ(E;Eγ). 42Sc deduced β+-branching.
doi: 10.1016/0370-2693(71)90287-5
1971HA10 Nucl.Phys. A162, 552 (1971) J.C.Hardy, J.M.Loiseaux, J.Cerny, G.T.Garvey The Reactions 11B(p, 3He)9Be and 11B(p, t)9B: Is There Strong Isospin Mixing in Mass 9 (Question) NUCLEAR REACTIONS 11B(p, t), (p, 3He), E=45 keV; measured σ(Et, θ), σ(E(3He), θ). 9B, 9Be deduced levels J, π, T, L, isobaric analogs. Enriched target.
doi: 10.1016/0375-9474(71)90254-5
1971MI03 Nucl.Phys. A163, 65 (1971) Charge Exchange in Medium Mass Nuclei as Observed by the (p, np) Reaction NUCLEAR REACTIONS 67Zn, 77Se, 91Zr, 95,97Mo, 105Pd, 110,111,113Cd, 115,116,117,119Sn, 123,125Te(p, np), E=12.8-18 MeV; measured σ(E;Ep'θ(p)). 67Ga, 77Br, 91Nb, 95,97Tc, 105Ag, 110,111,113In, 115,116,117,119Sb, 123,125I deduced isobaric analog states, p-width/level-width.
doi: 10.1016/0375-9474(71)90522-7
1971TO08 Ann.Phys.(N.Y.) 66, 674 (1971) I.S.Towner, E.K.Warburton, G.T.Garvey Hindrance Phenomena in Unique First- and Third-Forbidden β-Decay RADIOACTIVITY 16,17N, 19O, 37,38S, 38,39,40Cl, 39,41Ar, 40,42,43,45K, 41,45,47Ca; analayzed 1st-forbidden unique β-decay data; deduced f1t, β-moments.
doi: 10.1016/0003-4916(71)90074-1
1971WI07 Nucl.Phys. A166, 661 (1971) D.H.Wilkinson, D.E.Alburger, D.R.Goosman, K.W.Jones, E.K.Warburton, G.T.Garvey, R.L.Williams Properties of 13B and 20Na: The Second-Class Current Problem RADIOACTIVITY 13B, 20Na; measured T1/2; deduced ft ratios. 20Ne(p, n), E approx threshold; measured σ(E); deduced threshold, Q. 20Na deduced mass.
doi: 10.1016/0375-9474(71)90912-2
1970WA11 Ann.Phys.(N.Y.) 57, 174 (1970) E.K.Warburton, G.T.Garvey, I.S.Towner Unique Second- and Third-Forbidden β Decay RADIOACTIVITY 10Be, 22Na, 26Al; calculated unique second-forbidden matrix elements. Shell, unified models. 40K; calculated unique third-forbidden matrix elements. Shell model.
doi: 10.1016/0003-4916(70)90275-7
1969GA04 Phys.Letters 29B, 108 (1969) G.T.Garvey, K.W.Jones, L.E.Carlson, A.G.Robertson, D.F.H.Start The Spin, Parity and Lifetime of the 4.46 MeV State of 32S NUCLEAR REACTIONS 32S(α, α'γ), E = 11.4 MeV; measured α'γ(θ), Doppler shift attenuation. 32S level deduced J, π, T1/2, γ-mixing. Ge(Li) detector.
doi: 10.1016/0370-2693(69)90258-5
1969GA32 Rev.Mod.Phys. 41, S1 (1969) G.T.Garvey, W.J.Gerace, R.L.Jaffe, I.Talmi, I.Kelson Set of Nuclear-Mass Relations and a Resultant Mass Table
doi: 10.1103/RevModPhys.41.S1
1969WA17 Nucl.Phys. A136, 160 (1969) E.K.Warburton, L.E.Carlson, G.T.Garvey, D.A.Hutcheon, K.P.Jackson Lifetime of the 22Na 3708 keV Level NUCLEAR REACTIONS 19F(α, n); E = 9, 11 MeV: measured Eγ, Doppler shift attenuation. 22Na level deduced T1/2. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90045-1
1968CR03 Phys.Rev. 167, 1070 (1968) Inelastic Scattering in the 2s-1d Shell. II. Odd-A Nuclei NUCLEAR STRUCTURE 31P, 23Na, 19F, 27Al, 25Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.167.1070
1968TH04 Phys.Letters 27B, 504 (1968) T.D.Thomas, G.M.Raisbeck, P.Boerstling, G.T.Garvey, R.P.Lynch New Isotopes, 19N and 21O, Produced in High-Energy Nuclear Reactions NUCLEAR STRUCTURE 19N, 21O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90207-4
1967CR07 Phys.Rev. 160, 981 (1967) Inelastic Scattering in the 2s-1d Shell. I. Even-A Nuclei NUCLEAR STRUCTURE 28Si, 32S, 16O, 24Mg, 26Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.160.981
1966GA21 Bull.Am.Phys.Soc. 11, No.1, 26, BA5 (1966) Isospin Mixing in Be8 NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
1966GA25 Phys.Rev.Letters 16, 197 (1966) New Nuclidic Mass Relationship
doi: 10.1103/PhysRevLett.16.197
1966KE16 Phys.Letters 23, 689 (1966) Masses of Nuclei with Z > n ATOMIC MASSES A=8-42; calculated masses, binding energies.
doi: 10.1016/0031-9163(66)91102-4
1965CR06 Phys.Letters 19, 228 (1965) A Change from Strong to Weak Coupling Between 25Mg and 27Al NUCLEAR STRUCTURE 25Mg, 27Al; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90081-8
1964CE05 Phys. Letters 12, 234 (1964) T=2 States in the T(Z)=0 Nuclei O16-Ne20 and the T(Z)=1 Nuclei N16-F20
doi: 10.1103/PhysRevLett.12.619
1964GA01 Bull.Am.Phys.Soc.9, No.1, 44, DC9 (1964) Scattering of 63-MeV Li6 from Li6+ NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.
1964GA02 Phys.Rev.Letters 12, 726 (1964) T = 2 States in Mg24, Ti44, and Fe52 NUCLEAR STRUCTURE 24Mg, 44Ti, 52Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.12.726
1964HI09 Phys.Rev. 135, B346 (1964) Elastic and Inelastic Scattering at 168 MeV in the O16-C12 System NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B346
1963GA05 Phys.Rev. 130, 2397 (1963) G.T.Garvey, A.M.Smith, J.C.Hiebert Enhanced Excitation of T = 0, S = 0 States of the Ground State Configuration in C12-C12 Scattering at 126 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.2397
1963HI03 Bull.Am.Phys.Soc. 8, No.4, 303, D10 (1963) Elastic and Inelastic Scattering of 168-MeV O16 Ions from C12 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
1962GA01 Bull.Am.Phys.Soc. 7, No.1, 36, JA3 (1962) G.T.Garvey, A.M.Smith, J.C.Hiebert, F.E.Steigert Reaction C12(C12, C12*)C12* NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962GA02 Phys.Rev.Letters, 8, 25 (1962) G.T.Garvey, A.M.Smith, J.C.Hiebert, F.E.Steigert Mutual Excitation via a Two-Phonon Surface Interaction in C12(C12, C12*)C12* NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.8.25
Back to query form |