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NSR database version of April 27, 2024.

Search: Author = G.Moore

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2018GH05      Phys.Rev.Lett. 121, 052302 (2018)

J.Ghiglieri, G.D.Moore, D.Teaney

Second-Order Hydrodynamics in Next-to-Leading-Order QCD

doi: 10.1103/PhysRevLett.121.052302
Citations: PlumX Metrics

2018RA24      Nucl.Phys. A979, 21 (2018)

R.Rapp, P.B.Gossiaux, A.Andronic, R.Averbeck, S.Masciocchi, A.Beraudo, E.Bratkovskaya, P.Braun-Munzinger, S.Cao, A.Dainese, S.K.Das, M.Djordjevic, V.Greco, M.He, H.van Hees, G.Inghirami, O.Kaczmarek, Y.-J.Lee, J.Liao, S.Y.F.Liu, G.Moore, M.Nahrgang, J.Pawlowski, P.Petreczky, S.Plumari, F.Prino, S.Shi, T.Song, J.Stachel, I.Vitev, X.-N.Wang

Extraction of heavy-flavor transport coefficients in QCD matter

doi: 10.1016/j.nuclphysa.2018.09.002
Citations: PlumX Metrics

2011LU08      Phys.Rev. C 83, 044901 (2011)

E.Lu, G.D.Moore

Bulk viscosity of a pion gas

doi: 10.1103/PhysRevC.83.044901
Citations: PlumX Metrics

2011MO04      Phys.Rev.Lett. 106, 122302 (2011)

G.D.Moore, K.A.Sohrabi

Kubo Formulas for Second-Order Hydrodynamic Coefficients

doi: 10.1103/PhysRevLett.106.122302
Citations: PlumX Metrics

2010DU01      Phys.Rev. C 81, 034907 (2010)

K.Dusling, G.D.Moore, D.Teaney

Radiative energy loss and v₂ spectra for viscous hydrodynamics

doi: 10.1103/PhysRevC.81.034907
Citations: PlumX Metrics

2009QI08      Nucl.Phys. A830, 459c (2009)

G.-Y.Qin, C.Gale, S.Jeon, G.D.Moore, J.Ruppert

Jet energy loss and high p_T photon production in hot quark-gluon plasma

doi: 10.1016/j.nuclphysa.2009.10.040
Citations: PlumX Metrics

2009QI09      Phys.Rev. C 80, 054909 (2009)

G.-Y.Qin, J.Ruppert, C.Gale, Sa.Jeon, G.D.Moore

Jet energy loss, photon production, and photon-hadron correlations at energies available at the BNL Relativistic Heavy Ion Collider (RHIC)

doi: 10.1103/PhysRevC.80.054909
Citations: PlumX Metrics

2008QI02      Phys.Rev.Lett. 100, 072301 (2008)

G.-Y.Qin, J.Ruppert, C.Gale, S.Jeon, G.D.Moore, M.G.Mustafa

Radiative and Collisional Jet Energy Loss in the Quark-Gluon Plasma at the BNL Relativistic Heavy Ion Collider

doi: 10.1103/PhysRevLett.100.072301
Citations: PlumX Metrics

2007HU10      Phys.Rev.Lett. 98, 172303 (2007)

S.C.Huot, S.Jeon, G.D.Moore

Shear Viscosity in Weakly Coupled N = 4 Super Yang-Mills Theory Compared to QCD

doi: 10.1103/PhysRevLett.98.172303
Citations: PlumX Metrics

2006MO25      Eur.Phys.J. A 29, 53 (2006)

G.D.Moore

Numerical studies of QGP instabilities and implications

doi: 10.1140/epja/i2005-10298-4
Citations: PlumX Metrics

2005AR06      Phys.Rev.Lett. 94, 072302 (2005)

P.Arnold, J.Lenaghan, G.D.Moore, L.G.Yaffe

Apparent Thermalization due to Plasma Instabilities in the Quark-Gluon Plasma

doi: 10.1103/PhysRevLett.94.072302
Citations: PlumX Metrics

2005JE02      Phys.Rev. C 71, 034901 (2005)

S.Jeon, G.D.Moore

Energy loss of leading partons in a thermal QCD medium

doi: 10.1103/PhysRevC.71.034901
Citations: PlumX Metrics

2005MO21      Phys.Rev. C 71, 064904 (2005)

G.D.Moore, D.Teaney

How much do heavy quarks thermalize in a heavy ion collision?

doi: 10.1103/PhysRevC.71.064904
Citations: PlumX Metrics

2005TU06      Phys.Rev. C 72, 014906 (2005)

S.Turbide, C.Gale, S.Jeon, G.D.Moore

Energy loss of leading hadrons and direct photon production in evolving quark-gluon plasma

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E(cm)=200 GeV/nucleon; Pb(Pb, X), E(cm)=5500 GeV/nucleon; calculated pion and photon spectra, nuclear modification factors, role of quark-gluon plasma.

doi: 10.1103/PhysRevC.72.014906
Citations: PlumX Metrics

2004MO35      J.Phys.(London) G30, S775 (2004)

G.D.Moore

Electromagnetic emission and energy loss in the QGP

doi: 10.1088/0954-3899/30/8/017
Citations: PlumX Metrics

1982FO03      Phys.Lett. 108B, 95 (1982)

H.T.Fortune, S.C.Headley, A.Spadafora, J.Sweet, S.LaFrance, M.E.Cobern, G.E.Moore, M.Newcomer, E.Wallash, L.Bland, J.Gilfoyle, R.Gilman, M.Carchidi, G.S.Stephans, L.R.Greenwood, J.R.Erskine, R.E.Segel, T.H.Braid, K.Raghunathan

l Determinations for ¹²C + ¹²C

NUCLEAR REACTIONS ¹²C(¹²C, α), E=33-44 MeV; measured σ(θ) vs E; deduced exit channel characteristic (L). Legendre polynomial analysis.

doi: 10.1016/0370-2693(82)91150-9
Citations: PlumX Metrics

1981CO13      Phys.Rev. C23, 2387 (1981)

M.E.Cobern, L.C.Bland, H.T.Fortune, G.E.Moore, S.Mordechai, R.Middleton

¹⁶O(t, p)¹⁸O to Low-Lying States in ¹⁸O

NUCLEAR REACTIONS ¹⁶O(t, p), E=15 MeV; measured σ(Ep, θ). ¹⁸O deduced levels, L, two-particle transfer amplitudes. Microscopic DWBA.

doi: 10.1103/PhysRevC.23.2387
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0022.

1979FO14      Phys.Rev. C20, 1228 (1979)

H.T.Fortune, G.E.Moore, L.Bland, M.E.Cobern, S.Mordechai, R.Middleton, R.D.Lawson

Reaction ¹⁵N(t, p)¹⁷N

NUCLEAR REACTIONS ¹⁵N(t, p), E=15.0 MeV; measured σ(Ep, θ). ¹⁷N levels deduced L, π, J. Enriched gas target. Comparison with shell model.

doi: 10.1103/PhysRevC.20.1228
Citations: PlumX Metrics

1979LA18      Phys.Rev. C20, 1673 (1979)

S.LaFrance, H.T.Fortune, S.Mordechai, M.E.Cobern, G.E.Moore, R.Middleton, W.Chung, B.H.Wildenthal

²⁰O from ¹⁸O(t, p)

NUCLEAR REACTIONS ¹⁸O(t, p), E=15.0 MeV; measured σ(Ep, θ). ²⁰O deduced levels, L, π, J. DWBA analysis, shell, weak-coupling models. Enriched gas target.

doi: 10.1103/PhysRevC.20.1673
Citations: PlumX Metrics

1978FO05      Phys.Rev. C17, 888 (1978)

H.T.Fortune, M.E.Cobern, G.E.Moore

¹⁸O(d, t)¹⁷O and the Ground-State Wave Function of ¹⁸O

NUCLEAR REACTIONS ¹⁸O(d, t), E=17 MeV; measured σ(Et, θ). ¹⁷O levels deduced S. ¹⁸O ground state deduced wave function. DWBA, CCBA analysis.

doi: 10.1103/PhysRevC.17.888
Citations: PlumX Metrics

1978FO06      Phys.Rev.Lett. 40, 1236 (1978)

H.T.Fortune, M.E.Cobern, S.Mordechai, G.E.Moore, S.Lafrance, R.Middleton

(sd)² States in ^14,16C

NUCLEAR STRUCTURE ^14,16C; calculated levels. Shell model.

doi: 10.1103/PhysRevLett.40.1236
Citations: PlumX Metrics

1978MA21      Phys.Rev. C17, 2047 (1978)

J.F.Mateja, L.R.Medsker, H.T.Fortune, R.Middleton, G.E.Moore, M.E.Cobern, S.Mordechai, J.D.Zumbro, C.P.Browne

⁷⁶Ge(t, p)⁷⁸Ge Reaction

NUCLEAR REACTIONS ⁷⁶Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). ⁷⁸Ge deduced levels, L, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.17.2047
Citations: PlumX Metrics

1978MO07      J.Phys.(London) G4, 407 (1978)

S.Mordechai, H.T.Fortune, G.E.Moore, M.E.Cobern, R.V.Kollarits, R.Middleton

Spins of States Near 10 MeV Excitation in ¹⁴C

NUCLEAR REACTIONS ¹²C(t, p), E=18 MeV; measured σ(Ep, θ). ¹⁴C levels deduced L, J, π. Enriched targets, DWBA analysis.

doi: 10.1088/0305-4616/4/3/015
Citations: PlumX Metrics

1978MO08      Nucl.Phys. A301, 463 (1978)

S.Mordechai, H.T.Fortune, G.E.Moore, M.E.Cobern, R.V.Kollarits, R.Middleton

Structure of ¹⁴C from ¹²C(t, p)

NUCLEAR REACTIONS ¹²C(t, p), E=18 MeV; measured σ(Ep, θ). ¹⁴C deduced levels, L, J, π. Comparison of data with shell-model calculations. Enriched targets.

doi: 10.1016/0375-9474(78)90062-3
Citations: PlumX Metrics

1978MO18      Phys.Lett. 76B, 192 (1978)

G.E.Moore, M.E.Cobern, H.T.Fortune, S.Mordechai, R.V.Kollarits, R.Middleton

2p-1h States in ¹⁷N

NUCLEAR REACTIONS ¹⁵N, ¹⁶O(t, p), E=15 MeV; measured σ(Ep, θ). ¹⁷N levels deduced J, π.

doi: 10.1016/0370-2693(78)90272-1
Citations: PlumX Metrics

1977FO09      Phys.Lett. 70B, 408 (1977)

H.T.Fortune, R.Middleton, M.E.Cobern, G.E.Moore, S.Mordechai, R.V.Kollarits, H.Nann, W.Chung, B.H.Wildenthal

Spectroscopy of ¹⁶C

NUCLEAR REACTIONS ¹⁴C(t, p), E=15, 17, 18 MeV; measured σ(Ep, θ). ¹⁶C deduced levels, J, π, configuration.

doi: 10.1016/0370-2693(77)90400-2
Citations: PlumX Metrics

1977KE09      Phys.Rev. C15, 1726 (1977)

K.W.Kemper, G.E.Moore, R.J.Puigh, R.L.White

Spectroscopic Information from the ⁹Be(⁷Li, ⁶He)¹⁰B and ⁹Be(⁷Li, ⁶Li)¹⁰Be Reactions

NUCLEAR REACTIONS ⁹Be(⁷Li, ⁷Li), E=30 MeV; ¹⁰B(⁶Li, ⁶Li), E=34 MeV; measured σ(θ); deduced optical model parameters. ⁹Be(⁷Li, ⁶He), E=34 MeV; measured σ(θ); deduced spin transfer. ⁹Be(⁷Li, ⁶Li), E=34 MeV; measured σ(θ). ¹⁰B, ¹⁰Be levels deduced S. Finite range DWBA analysis.

doi: 10.1103/PhysRevC.15.1726
Citations: PlumX Metrics

1977MI08      Phys.Rev. C16, 477 (1977)

R.Middleton, W.E.Stephens, G.E.Moore, M.E.Cobern, H.T.Fortune, H.Paul

Upper Limit for the Presence of Superheavy Elements in Monazite from Madagascar

RADIOACTIVITY A > 200; measured relative elemental concentrations in monazite; deduced upper limit for superheavy elements.

doi: 10.1103/PhysRevC.16.477
Citations: PlumX Metrics

1977MO13      Nucl.Phys. A289, 36 (1977)

S.Mordechai, M.E.Cobern, G.E.Moore, H.T.Fortune

Study of ⁷⁸As with the ⁸⁰Se(d, α) Reaction

NUCLEAR REACTIONS ⁸⁰Se(d, α), E=16.0 MeV; measured σ(Eα, θ); deduced Q. ⁷⁸As deduced levels, L, J, π.

doi: 10.1016/0375-9474(77)90518-8
Citations: PlumX Metrics

1976MO20      Z.Naturforsch. 31a, 668 (1976)

G.L.Moore, F.R.Buskirk, E.B.Dally, J.N.Dyer, X.K.Maruyama, R.Pitthan

The Widths of the E2 (ΔT = 0 and ΔT = 1) Giant Resonances in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(e, e'), E=60-105 MeV; measured σ(E). ¹⁶⁵Ho deduced giant resonances, Γ.

1976MO24      Phys.Rev. C14, 977 (1976)

G.E.Moore, K.W.Kemper

Possible Evidence for Exchange Effects in the ¹⁶O(⁶Li, α)¹⁸F Reaction at E = 34 MeV

NUCLEAR REACTIONS ¹⁶O(⁶Li, α), E=34 MeV; measured σ(Eα, θ); deduced possible exchange effects, zero-range normalization. ¹⁸F levels deduced S. DWBA analysis, shell model.

doi: 10.1103/PhysRevC.14.977
Citations: PlumX Metrics

1976NO01      Phys.Rev. C13, 1211 (1976)

G.A.Norton, K.W.Kemper, G.E.Moore, R.J.Puigh, M.E.Williams-Norton

States in ¹⁵N Populated by the ¹¹B(⁶Li, d) and ¹¹B(⁷Li, t) Reactions

NUCLEAR REACTIONS ¹¹B(⁶Li, d), (⁷Li, t), E=34 MeV; measured σ(θ). ¹⁵N deduced levels.

doi: 10.1103/PhysRevC.13.1211
Citations: PlumX Metrics

1976ZE04      Phys.Rev. C14, 2162 (1976)

A.F.Zeller, M.E.Williams-Norton, R.J.Puigh, G.E.Moore, K.W.Kemper, G.M.Hudson

¹²C + ¹⁴N Reaction at E(lab) = 53 MeV

NUCLEAR REACTIONS ¹²C(¹⁴N, ⁶Li), (¹⁴N, ⁹Be), (¹⁴N, ¹⁰B), (¹⁴N, ¹²C), E=52.4-53.6 MeV; measured σ(E, θ); deduced reaction mechanism. Hauser Feshbach analysis. Natural targets.

doi: 10.1103/PhysRevC.14.2162
Citations: PlumX Metrics

1975HU10      Phys.Rev. C12, 474 (1975)

G.M.Hudson, K.W.Kemper, G.E.Moore, M.E.Williams

Structure of ⁷Be and ⁶³Cu Determined from the ⁶³Cu(⁶Li, ⁷Be)⁶²Ni Reaction

NUCLEAR REACTIONS ⁶³Cu(⁶Li, ⁷Be), E=34 MeV; measured σ(E(⁷Be), θ). ⁶²Ni(⁷Li, ⁷Li), ⁶³Cu(⁷Li, ⁷Li); re-analyzed data. ⁷Be, ⁶²Ni levels deduced S.

doi: 10.1103/PhysRevC.12.474
Citations: PlumX Metrics

1975MO07      Phys.Rev. C11, 1099 (1975); Erratum Phys.Rev. C12, 1375 (1975)

G.E.Moore, K.W.Kemper, L.A.Charlton

Reactions (⁷Li, ⁷Li), (⁷Li, ⁶Li), and (⁷Li, ⁶He) on the Deformed Target ²⁴Mg at E = 34 MeV

NUCLEAR REACTIONS ²⁴Mg(⁷Li, ⁷Li), E=34 MeV; measured σ(θ); deduced optical parameters. ²⁴Mg deduced deformation lengths. ²⁴Mg(⁷Li, ⁶Li), (⁷Li, ⁶He), E=34 MeV; measured σ(θ). ²⁵Mg, ²⁵Al deduced levels, L, J, π, S.

doi: 10.1103/PhysRevC.11.1099
Citations: PlumX Metrics

1975PU01      Nucl.Phys. A237, 1 (1975)

R.J.Puigh, K.W.Kemper, G.E.Moore, R.L.White

The ⁹Be(α, d)¹¹B Reaction at E = 27 MeV

NUCLEAR REACTIONS ⁹Be(α, d), E=26.5-27.5 MeV; measured σ(E, Ed, θ), θ=7.5°-120°(cm). ¹¹B transitions deduced L. Compared with DWBA.

doi: 10.1016/0375-9474(75)90458-3
Citations: PlumX Metrics

1975WI30      Phys.Rev. C12, 1899 (1975)

M.E.Williams-Norton, G.M.Hudson, K.W.Kemper, G.E.Moore, G.A.Norton, R.J.Puigh, A.F.Zeller

Low-Lying States in ²⁰Ne Populated by the ¹⁹F(⁷Li, ⁶He)²⁰Ne Reaction at 34 MeV

NUCLEAR REACTIONS ¹⁹F(⁶Li, ⁶Li), (⁷Li, ⁷Li), E=20, 34 MeV; measured σ(θ); deduced optical model parameters. ¹⁹F(⁷Li, ⁶He), E=34 MeV; measured σ(E(⁶He), θ). ²⁰Ne levels deduced S. DWBA analysis.

doi: 10.1103/PhysRevC.12.1899
Citations: PlumX Metrics

1974CO13      Phys.Rev. C9, 1273 (1974)

W.J.Courtney, K.W.Kemper, G.E.Moore, R.L.White

¹³C(⁶Li, α₀)¹⁵N Reaction for E = 7-17 MeV

NUCLEAR REACTIONS ¹³C(⁶Li, α), E=7-17 MeV; measured σ(E, θ). ¹⁹F deduced resonances.

doi: 10.1103/PhysRevC.9.1273
Citations: PlumX Metrics

1974KE06      Nucl.Phys. A222, 173 (1974)

K.W.Kemper, S.Cotanch, G.E.Moore, A.W.Obst, R.J.Puigh, R.L.White

Anomalous Results for the ⁹Be(α, t)¹⁰B and ¹³C(α, t)¹⁴N Reactions at E = 27 MeV

NUCLEAR REACTIONS ⁹Be, ¹³C(α, t), E=26-27.5 MeV; measured σ(Et, θ); compared with DWBA. ¹⁰B, ¹⁴N levels deduced relative S.

doi: 10.1016/0375-9474(74)90592-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2335.

1974KE15      Phys.Lett. 52B, 179 (1974)

K.W.Kemper, R.L.White, L.A.Charlton, G.D.Gunn, G.E.Moore

A Useful Spectroscopic Tool: The (⁷Li, ⁶He) Reaction

NUCLEAR REACTIONS ²⁴Mg, ⁵²Cr(⁷Li, ⁶He), E=34 MeV; measured σ(E(⁶He), θ). ²⁵Al, ⁵³Mn levels deduced L.

doi: 10.1016/0370-2693(74)90083-5
Citations: PlumX Metrics

1972BB15      Izv.Akad.Nauk SSSR, Ser.Fiz. 36, 2213 (1972); Bull.Acad.Sci.USSR, Phys.Ser. 36, 1941 (1973)

R.Bangert, B.Gonsior, G.Moore, M.Roth, B.Steinmetz, A.Stromich

Proton Reactions with Tellurium Isotopes, Isobar-Analog States of Iodine Nuclei

NUCLEAR REACTIONS ^126,128,130Te(p, p'), E=9.7-10.5 MeV; measured σ(E;Ep'). ^126,128,130Te(p, p), E=9.7-10.5 MeV; measured vector analyzing power. ^126,128,130Te(p, np'), E=14-17 MeV; measured σ(E;Ep', θ). ^127,129,131I deduced analog resonances, J, π.

Note: The following list of authors and aliases matches the search parameter G.Moore: , G.D.MOORE, G.E.MOORE, G.L.MOORE