NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 10, 2024.

Search: Author = G.Garvey

Found 72 matches.

Back to query form



2023BY02      Phys.Rev.Lett. 131, 082502 (2023)

W.Byron, H.Harrington, R.J.Taylor, W.DeGraw, N.Buzinsky, B.Dodson, M.Fertl, A.Garcia, G.Garvey, B.Graner, M.Guigue, L.Hayen, X.Huyan, K.S.Khaw, K.Knutsen, D.McClain, D.Melconian, P.Muller, E.Novitski, N.S.Oblath, R.G.H.Robertson, G.Rybka, G.Savard, E.Smith, D.D.Stancil, M.Sternberg, D.W.Storm, H.E.Swanson, J.R.Tedeschi, B.A.VanDevender, F.E.Wietfeldt, A.R.Young, X.Zhu, for the He6-CRES Collaboration

First Observation of Cyclotron Radiation from MeV-Scale e± following Nuclear β Decay

RADIOACTIVITY 6He(β-), 19Ne(β+) [7Li(d, 3He), E=17.8 MeV; 19F(p, n), E=12 MeV]; measured decay products, Eβ, Iβ; deduced β spectra, first direct observation of cyclotron radiation from individual highly relativistic β in a waveguide. The cyclotron radiation emission spectroscopy (CRES) technique, FN-tandem accelerator at the University of Washington.

doi: 10.1103/PhysRevLett.131.082502
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010GA11      Phys.Rev. C 81, 055212 (2010)

G.T.Garvey

Orbital angular momentum in the nucleon

doi: 10.1103/PhysRevC.81.055212
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2003GA05      Phys.Rev.Lett. 90, 092302 (2003)

G.T.Garvey, J.C.Peng

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2002JO02      Phys.Rev. C65, 025203 (2002)

M.B.Johnson, B.Z.Kopeliovich, I.K.Potashnikova, P.L.McGaughey, J.M.Moss, J.C.Peng, G.Garvey, M.Leitch, C.N.Brown, D.M.Kaplan

Energy Loss versus Shadowing in the Drell-Yan Reaction on Nuclei

NUCLEAR REACTIONS 2H, Be, C, Ca, Fe, W(p, X), E at 800 GeV/c; analyzed Drell-Yan production σ; deduced energy loss effects, other reaction mechanism features.

doi: 10.1103/PhysRevC.65.025203
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2001GA58      Prog.Part.Nucl.Phys. 47, 203 (2001)

G.T.Garvey, J.-C.Peng

Flavor Asymmetry of Light Quarks in the Nucleon Sea

doi: 10.1016/S0146-6410(01)00155-7
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000GA26      Prog.Part.Nucl.Phys. 44, 305 (2000)

G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1993GA20      Phys.Rev. C48, 1919 (1993)

G.Garvey, E.Kolbe, K.Langanke, S.Krewald

Role of Strange Quarks in Quasielastic Neutrino Scattering

NUCLEAR REACTIONS 12C(ν, ν'n), (ν, ν'p), (ν-bar, ν-bar'n), (ν-bar, ν-bar'p), E not given; calculated neutron, proton yield ratio; deduced strange quarks role. Continiuum RPA.

doi: 10.1103/PhysRevC.48.1919
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1992GA21      Nucl.Phys. A546, 369c (1992)

G.T.Garvey

Recent Developments in Neutrino Physics

doi: 10.1016/0375-9474(92)90521-K
Citations: PlumX Metrics


1985HE08      Phys.Rev. C31, 2190 (1985)

A.R.Heath, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1978BO30      Phys.Rev. C18, 1447 (1978); Erratum Phys.Rev. C26, 2336 (1982)

T.J.Bowles, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1977OO01      Nucl.Phys. A284, 41 (1977)

M.A.Oothoudt, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1975TR06      Phys.Rev. C12, 967 (1975)

R.E.Tribble, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2721.


1974DE20      Phys.Rev. C10, 680 (1974)

P.T.Debevec, G.T.Garvey

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
Citations: PlumX Metrics


1974TR01      Phys.Rev.Lett. 32, 314 (1974)

R.E.Tribble, G.T.Garvey

Weak Magnetism and Second-Class - Current Interactions in A = 8

RADIOACTIVITY 8Li, 8B; measured βα(θ).

doi: 10.1103/PhysRevLett.32.314
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1971MI03      Nucl.Phys. A163, 65 (1971)

P.S.Miller, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1968CR03      Phys.Rev. 167, 1070 (1968)

G.M.Crawley, G.T.Garvey

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0615.


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
Citations: PlumX Metrics


1967CR07      Phys.Rev. 160, 981 (1967)

G.M.Crawley, G.T.Garvey

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0618.


1966GA21      Bull.Am.Phys.Soc. 11, No.1, 26, BA5 (1966)

G.T.Garvey, J.Cerny, H.Pugh

Isospin Mixing in Be8

NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.


1966GA25      Phys.Rev.Letters 16, 197 (1966)

G.T.Garvey, I.Kelson

New Nuclidic Mass Relationship

doi: 10.1103/PhysRevLett.16.197
Citations: PlumX Metrics


1966KE16      Phys.Letters 23, 689 (1966)

I.Kelson, G.T.Garvey

Masses of Nuclei with Z > n

ATOMIC MASSES A=8-42; calculated masses, binding energies.

doi: 10.1016/0031-9163(66)91102-4
Citations: PlumX Metrics


1965CR06      Phys.Letters 19, 228 (1965)

G.M.Crawley, G.T.Garvey

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0828.


1964CE05      Phys. Letters 12, 234 (1964)

J.Cerny, R.H.Pehl, G.T.Garvey

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
Citations: PlumX Metrics


1964GA01      Bull.Am.Phys.Soc.9, No.1, 44, DC9 (1964)

G.T.Garvey, J.C.Hiebert

Scattering of 63-MeV Li6 from Li6+

NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.


1964GA02      Phys.Rev.Letters 12, 726 (1964)

G.T.Garvey, J.Cerny, R.H.Pehl

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
Citations: PlumX Metrics


1964HI09      Phys.Rev. 135, B346 (1964)

J.C.Hiebert, G.T.Garvey

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1963HI03      Bull.Am.Phys.Soc. 8, No.4, 303, D10 (1963)

J.C.Hiebert, G.T.Garvey

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
Citations: PlumX Metrics


Back to query form


Note: The following list of authors and aliases matches the search parameter G.Garvey: , G.T.GARVEY