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NSR database version of April 11, 2024.

Search: Author = G.Hale

Found 77 matches.

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2024LE02      Phys.Rev. C 109, 014601 (2024)

H.Y.Lee, S.A.Kuvin, L.Zavorka, S.Mosby, B.DiGiovine, G.Hale, M.Paris, D.Votaw, M.White

Differential cross sections of the 16O(n, α) reaction at neutron energies from 3.8 to 15 MeV

doi: 10.1103/PhysRevC.109.014601
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2024ME02      Phys.Rev. C 109, 034003 (2024)

K.D.Meaney, M.W.Paris, G.M.Hale, Y.Kim, J.Kuczek, A.C.Hayes

Deuterium-tritium fusion γ-ray spectrum at MeV energies with application to reaction-in-flight inertial confinement fusion measurements

doi: 10.1103/PhysRevC.109.034003
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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
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2021DU11      Phys.Rev. C 103, 064608 (2021)

P.Ducru, B.Forget, V.Sobes, G.Hale, M.Paris

Shadow poles in the alternative parametrization of R matrix theory

NUCLEAR REACTIONS 134Xe(n, X), E=2186.0, 6315.0 eV p-wave resonances; analyzed neutron resonance parameters by R-matrix theory and using generalized Reich-Moore formalism to convert the Reich-Moore parameters into real R-matrix parameters; deduced existence of shadow poles in the alternative parametrization of R-matrix theory, being considered as an alternative to the traditional Wigner-Eisenbud resonance parameters to document nuclear cross-section values in the nuclear data libraries such as ENDF/B-VIII.0. Discussed how the nuclear reaction community could convert present nuclear data libraries featuring both Wigner-Eisenbud parameters and Reich-Moore parameters to alternative parameters. See also follow-up 2021Du12 article by the same authors about Scattering matrix pole expansions in R-matrix theory, and a related article 2021Du13 about windowed multipole representation in R-matrix cross sections.

doi: 10.1103/PhysRevC.103.064608
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2021DU12      Phys.Rev. C 103, 064609 (2021)

P.Ducru, B.Forget, V.Sobes, G.Hale, M.Paris

Scattering matrix pole expansions for complex wave numbers in R-matrix theory

NUCLEAR REACTIONS 134Xe(n, X), E=2186.0, 6315.0 eV p-wave resonances; analyzed radioactive state parameters and the R-matrix parameters to yield an identical Kapur-Peierls operator, and exact reconstruction of the scattering matrix of the nuclear interactions, scattering matrix poles are the Siegert-Humblet radioactive poles; discussed subthreshold cross sections through analytic continuation; conclude with the need for the R-matrix community to come to consensus and agreement to set the analytic continuation as the standard way of computing R-matrix operator, in particular, the shift and penetration functions, in performing nuclear reaction data evaluations for the evaluated libraries such as ENSDF, JEFF, BRONDE, JENDL, CENDL, and TENDEL. See also preceding 2021Du11 article by the same authors about shadow poles in the alternative parametrization in R-matrix theory, and a related article 2021Du13 about windowed multipole representation in R-matrix cross sections.

doi: 10.1103/PhysRevC.103.064609
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2021HO14      Phys.Rev. C 104, 024610 (2021)

C.J.Horsfield, M.S.Rubery, J.M.Mack, H.W.Herrmann, Y.Kim, C.S.Young, S.E.Caldwell, S.C.Evans, T.S.Sedillo, A.M.McEvoy, N.M.Hoffman, M.A.Huff, J.R.Langenbrunner, G.M.Hale, D.C.Wilson, W.Stoeffl, J.A.Church, E.M.Grafil, E.K.Miller, V.Y.Glebov

First spectral measurement of deuterium-tritium fusion γ rays in inertial fusion experiments

NUCLEAR REACTIONS 3H(d, γ)5He*, E not given; measured fusion Eγ, Iγ from deuterium-tritium (DT) inertial confinement fusion (ICF) implosions with Omega laser, branching ratio of γ rays from transitions to an intermediate excited state and the ground state using R-matrix analysis.

doi: 10.1103/PhysRevC.104.024610
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2019TH03      Eur.Phys.J. A 55, 92 (2019)

I.J.Thompson, R.J.deBoer, P.Dimitriou, S.Kunieda, M.T.Pigni, G.Arbanas, H.Leeb, T.Srdinko, G.Hale, P.Tamagno, P.Archier

Verification of R-matrix calculations for charged-particle reactions in the resolved resonance region for the 7Be system

NUCLEAR REACTIONS 4He(3He, 3He)4He; 6Li(p, α0)3He; 6Li(p, p0)6Li, E* below 8 MeV; calculated σ using different R-code algorithms; compared results and possibilities both for total σ and for the individual l-waves.

doi: 10.1140/epja/i2019-12753-y
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2018BR03      Phys.Rev. C 97, 024603 (2018)

C.R.Brune, G.M.Hale, M.W.Paris

Monotonic properties of the shift and penetration factors

doi: 10.1103/PhysRevC.97.024603
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2018BR05      Nucl.Data Sheets 148, 1 (2018)

D.A.Brown, M.B.Chadwick, R.Capote, A.C.Kahler, A.Trkov, M.W.Herman, A.A.Sonzogni, Y.Danon, A.D.Carlson, M.Dunn, D.L.Smith, G.M.Hale, G.Arbanas, R.Arcilla, C.R.Bates, B.Beck, B.Becker, F.Brown, R.J.Casperson, J.Conlin, D.E.Cullen, M.-A.Descalle, R.Firestone, T.Gaines, K.H.Guber, A.I.Hawari, J.Holmes, T.D.Johnson, T.Kawano, B.C.Kiedrowski, A.J.Koning, S.Kopecky, L.Leal, J.P.Lestone, C.Lubitz, J.I.Marquez Damian, C.M.Mattoon, E.A.McCutchan, S.Mughabghab, P.Navratil, D.Neudecker, G.P.A.Nobre, G.Noguere, M.Paris, M.T.Pigni, A.J.Plompen, B.Pritychenko, V.G.Pronyaev, D.Roubtsov, D.Rochman, P.Romano, P.Schillebeeckx, S.Simakov, M.Sin, I.Sirakov, B.Sleaford, V.Sobes, E.S.Soukhovitskii, I.Stetcu, P.Talou, I.Thompson, S.van der Marck, L.Welser-Sherrill, D.Wiarda, M.White, J.L.Wormald, R.Q.Wright, M.Zerkle, G.Zerovnik, Y.Zhu

ENDF/B-VIII.0: The 8 th Major Release of the Nuclear Reaction Data Library with CIELO-project Cross Sections, New Standards and Thermal Scattering Data

COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ.

NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,21,22Ne, 22,23Na, 24,25,26Mg, 26,27Al, 28,29,30,31,32Si, 31P, 32,33,34,35,36S, 35,36,37Cl, 36,37,38,39,40,41Ar, 39,40,41K, 40,41,42,43,44,45,46,47,48Ca, 45Sc, 46,47,48,49,50Ti, 49,50,51V, 50,51,52,53,54Cr, 54,55Mn, 54,55,56,57,58Fe, 58,59Co, 58,59,60,61,62,63,64Ni, 63,64,65Cu, 64,65,66,67,68,69,70Zn, 69,70,71Ga, 70,71,72,73,74,75,76Ge, 73,74,75As, 74,75,76,77,78,79,80,81,82Se, 79,80,81Br, 78,79,80,81,82,83,84,85,86Kr, 85,86,87Rb, 84,85,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,93,94,95,96,97,98,99,100Mo, 98,99Tc, 96,97,98,99,100,101,102,103,104,105,106Ru, 103,104,105Rh, 102,103,104,105,106,107,108,109,110Pd, 107,108,109,110,111,112,113,114,115,116,117,118Ag, 106,107,108,109,110,111,112,113,114,115,116Cd, 113,114,115In, 112,113,114,115,116,117,118,119,120,121,122,123,124,125,126Sn, 121,122,123,124,125,126Sb, 120,121,122,123,124,125,126,127,128,129,130,121,132Te, 127,128,129,130,131,132,133,134,135I, 123,124,125,126,127,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,131,132,133,134,135,136,137,138,139,140Ba, 138,139,140La, 136,137,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,149,150Nd, 143,144,145,146,147,148,149,151Pm, 144,145,146,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,159,160Gd, 158,159,160,161Tb, 154,155,156,157,158,159,160,161,162,163,164Dy, 165,166Ho, 162,163,164,165,166,167,168,170,170Er, 168,169,170,171Tm, 168,169,170,171,172,173,174,175,176Yb, 175,176Lu, 174,175,176,177,178,179,180,181,182Hf, 180,181,182Ta, 180,181,182,183,184,185,186W, 185,186,187Re, 184,185,186,187,188,189,190,191,192Os, 191,192,193Ir, 190,191,192,193,194,195,196,197,198Pt, 197Au, 196,197,198,199,200,201,202,203,204Hg, 203,204,205Tl, 204,205,206,207,208,209,210Pb, 209,210Bi, 208,209,210Po, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VIII.0 evaluated neutron library. Comparison with ENDF/B-VII.1 and KADONIS values.

NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,245,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,248,249,250Bk, 246,247,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.1, JENDL-4.0u+ and Atlas of Neutron Resonances values.

doi: 10.1016/j.nds.2018.02.001
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2018CA07      Nucl.Data Sheets 148, 143 (2018), Erratum Nucl.Data Sheets 163, 280 (2020)

A.D.Carlson, V.G.Pronyaev, R.Capote, G.M.Hale, Z.-P.Chen, I.Duran, F.-J.Hambsch, S.Kunieda, W.Mannhart, B.Marcinkevicius, R.O.Nelson, D.Neudecker, G.Noguere, M.Paris, S.P.Simakov, P.Schillebeeckx, D.L.Smith, X.Tao, A.Trkov, A.Wallner, W.Wang

Evaluation of the Neutron Data Standards

NUCLEAR REACTIONS H, C(n, n), 6Li(n, t), 10B(n, αγ), 197Au(n, γ), 235,238U, 239Pu(n, F), 238U(n, γ), E<20 MeV; analyzed available data; deduced σ and Maxwellian spectrum averaged cross section for the 197Au(n, γ) σ at 30 keV, covariance matrices of the uncertainties.

RADIOACTIVITY 252Cf(SF); analyzed available data; deduced spontaneous fission neutron spectrum.

doi: 10.1016/j.nds.2018.02.002
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2018CH12      Nucl.Data Sheets 148, 189 (2018)

M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck

CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen

NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).

doi: 10.1016/j.nds.2018.02.003
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2018GA21      Phys.Rev.Lett. 121, 042501 (2018)

M.Gatu-Johnson, C.J.Forrest, D.B.Sayre, A.Bacher, J.-L.Bourgade, C.R.Brune, J.A.Caggiano, D.T.Casey, J.A.Frenje, V.Yu.Glebov, G.M.Hale, R.Hatarik, H.W.Herrmann, R.Janezic, Y.H.Kim, J.P.Knauer, O.Landoas, D.P.McNabb, M.W.Paris, R.D.Petrasso, J.E.Pino, S.Quaglioni, B.Rosse, J.Sanchez, T.C.Sangster, H.Sio, W.Shmayda, C.Stoeckl, I.Thompson, A.B.Zylstra

Experimental Evidence of a Variant Neutron Spectrum from the T(t, 2n)α Reaction at Center-of-Mass Energies in the Range of 16-50 KeV

NUCLEAR REACTIONS 3H(t, 2n), E(cm)=16-50 keV; measured reaction products, En, In; deduced neutron spectra inferred from R-matrix analysis of the measured NTOF-spectra.

doi: 10.1103/PhysRevLett.121.042501
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2017ZY01      Phys.Rev.Lett. 119, 222701 (2017)

A.B.Zylstra, J.A.Frenje, M.Gatu-Johnson, G.M.Hale, C.R.Brune, A.Bacher, D.T.Casey, C.K.Li, D.McNabb, M.Paris, R.D.Petrasso, T.C.Sangster, D.B.Sayre, F.H.Seguin

Proton Spectra from 3He+T and 3He+3He Fusion at Low Center-of-Mass Energy, with Potential Implications for Solar Fusion Cross Sections

NUCLEAR REACTIONS 3He(3He, X), E(cm)=165 keV; 3He(t, X), E=86 keV; measured reaction products, Ep, Ip; deduced yields. Comparison with R-matrix calculations.

doi: 10.1103/PhysRevLett.119.222701
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2015BR07      Phys.Rev. C 92, 014003 (2015)

C.R.Brune, J.A.Caggiano, D.B.Sayre, A.D.Bacher, G.M.Hale, M.W.Paris

R-matrix description of particle energy spectra produced by low-energy 3H + 3H reactions

NUCLEAR REACTIONS 3H(t, 2n)4He, E(cm)=16, 57 keV; 3He(3He, 2p)4He, E(cm)=165 keV; calculated neutron, proton and α-particle energy distributions for different reaction channels, fits to experimental neutron time-of-flight spectra, proton and α spectra. Phenomenological R-matrix analysis for the three-body final states. 5He; deduced fits to the 3/2- ground and 1/2- first excited states.

doi: 10.1103/PhysRevC.92.014003
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2015CA01      Nucl.Data Sheets 123, 27 (2015)

A.D.Carlson, V.G.Pronyaev, R.Capote, G.M.Hale, F.-J.Hambsch, T.Kawano, S.Kunieda, W.Mannhart, R.O.Nelson, D.Neudecker, P.Schillebeeckx, S.Simakov, D.L.Smith, P.Talou, X.Tao, A.Wallner, W.Wang

Recent Work Leading Towards a New Evaluation of the Neutron Standards

NUCLEAR REACTIONS H, C(n, n), 3He(n, p), 6Li(n, t), 10B(n, α), (n, αγ), Au(n, γ), 235,238U(n, F), E<20 MeV; analyzed available data; deduced neutron σ standards.

doi: 10.1016/j.nds.2014.12.006
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2015HA02      Nucl.Data Sheets 123, 165 (2015)

G.M.Hale, M.W.Paris

Data Covariances from R-Matrix Analyses of Light Nuclei

NUCLEAR REACTIONS 4He(n, n), 3H(d, d), (d, n), (d, γ), E<28 MeV; 12C(n, n), (n, n'), E<6.45 MeV; calculated σ covariances. R-matrix analysis code EDA.

doi: 10.1016/j.nds.2014.12.029
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2015KU03      Nucl.Data Sheets 123, 159 (2015)

S.Kunieda, T.Kawano, M.Paris, G.M.Hale, K.Shibata, T.Fukahori

Covariance of Neutron Cross Sections for 16O through R-matrix Analysis

NUCLEAR REACTIONS 16O(n, X), E<5 MeV; calculated σ and covariances. R-matrix analysis, comparison with available data.

doi: 10.1016/j.nds.2014.12.028
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2014BR02      Phys.Rev. C 89, 014622 (2014)

L.S.Brown, G.M.Hale

Field theory of the d + t → n + α reaction dominated by a 5He* unstable particle

NUCLEAR REACTIONS 3H(d, n)4He, E(cm)<0.10 MeV; analyzed astrophysical S(E) factor from a fit of 2665 experimental data points. Effective, nonrelativistic quantum field theory method providing a description of the d+t fusion process, with the assumption that an intermediate 5He* unstable spin-3/2+ resonance dominates the d+t-fusion reaction.

doi: 10.1103/PhysRevC.89.014622
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2014CH24      Nucl.Data Sheets 118, 1 (2014)

M.B.Chadwick, E.Dupont, E.Bauge, A.Blokhin, O.Bouland, D.A.Brown, R.Capote, A.Carlson, Y.Danon, C.De Saint Jean, M.Dunn, U.Fischer, R.A.Forrest, S.C.Frankle, T.Fukahori, Z.Ge, S.M.Grimes, G.M.Hale, M.Herman, A.Ignatyuk, M.Ishikawa, N.Iwamoto, O.Iwamoto, M.Jandel, R.Jacqmin, T.Kawano, S.Kunieda, A.Kahler, B.Kiedrowski, I.Kodeli, A.J.Koning, L.Leal, Y.O.Lee, J.P.Lestone, C.Lubitz, M.MacInnes, D.McNabb, R.McKnight, M.Moxon, S.Mughabghab, G.Noguere, G.Palmiotti, A.Plompen, B.Pritychenko, V.Pronyaev, D.Rochman, P.Romain, D.Roubtsov, P.Schillebeeckx, M.Salvatores, S.Simakov, E.Sh.Soukhovitskii, J.C.Sublet, P.Talou, I.Thompson, A.Trkov, R.Vogt, S.van der Marck

The CIELO Collaboration: Neutron Reactions on 1H, 16O, 56Fe, 235, 238U, and 239Pu

COMPILATION 1H, 16O, 56Fe, 235,238U, 239Pu(n, x), E≈0-20 MeV; analyzed available data on σ, neutron multiplicity, criticality using ENDF/B-VII.1, JENDL-4.0, JEFF-3.1, ROSFOND 2010, CENDL-3.1, EAF-2010 evaluated nuclear libraries, Atlas of Neutron Resonances, Neutron Cross Section Standards evaluations; deduced recommendations for CIELO library, parameters, Maxwellian-averaged, thermal, californium σ, Westcott factors, resonance integrals. Compared with available data.

doi: 10.1016/j.nds.2014.04.002
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2014HA03      Phys.Rev. C 89, 014623 (2014)

G.M.Hale, L.S.Brown, M.W.Paris

Effective field theory as a limit of R-matrix theory for light nuclear reactions

NUCLEAR REACTIONS 3H(d, n)4He, E(cm)<0.10 MeV; analyzed astrophysical S(E) factor by single level four-parameter R-matrix fit. Corresponds to nonrelativistic effective quantum field theory description in companion (2014Br02) article for d+t fusion reaction.

doi: 10.1103/PhysRevC.89.014623
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2014HA18      Nucl.Data Sheets 118, 165 (2014)

G.M.Hale, P.G.Young

n+12C Cross Sections from an R-matrix Analysis of Reactions in the 13C System

NUCLEAR REACTIONS 12C(n, n), (n, n'), E=0-6.5 MeV; calculated total σ, σ to the first excited state using R-matrix code EDA; deduced correlations, standard errors.

doi: 10.1016/j.nds.2014.04.027
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2014KU13      Nucl.Data Sheets 118, 250 (2014)

S.Kunieda, T.Kawano, M.Paris, G.Hale, K.Shibata, T.Fukahori

R-matrix Analysis for n +16O Cross-sections up to En=6.0 MeV with Covariances

NUCLEAR REACTIONS 16O(n, α), E=0.5-4.7 MeV;13C(α, n), E=0.7-4.7 MeV; calculated σ using multi-channel R-matrix with care for covariances; deduced resonances. Compared to ENDF/B-VII.1 and Harisopulos data.

doi: 10.1016/j.nds.2014.04.050
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2014PA34      Nucl.Data Sheets 120, 184 (2014)

M.Paris, G.Hale, A.Hayes-Sterbenz, G.Jungman

R-matrix Analysis of Reactions in the 9B Compound System

NUCLEAR REACTIONS 6Li(3He, 3He), (3He, p), (3He, d), (3He, γ), 2H(7Be, X)9B, E<6 MeV; analyzed available data.; deduced σ, σ(θ), resonance widths. Two-body unitary R-matrix method using the code EDA.

doi: 10.1016/j.nds.2014.07.041
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2014PA47      Nucl.Data Sheets 118, 596 (2014)

G.Palmiotti, M.Salvatores, G.Aliberti, M.Herman, S.D.Hoblit, R.D.McKnight, P.Oblozinsky, P.Talou, G.M.Hale, H.Hiruta, T.Kawano, C.M.Mattoon, G.P.A.Nobre, A.Palumbo, M.Pigni, M.E.Rising, W.-S.Yang, A.C.Kahler

Combined Use of Integral Experiments and Covariance Data

doi: 10.1016/j.nds.2014.04.145
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2014WE04      Phys.Rev. C 89, 054001 (2014)

G.J.Weisel, W.Tornow, A.S.Crowell, J.H.Esterline, G.M.Hale, C.R.Howell, P.D.O'Malley, J.R.Tompkins, H.Witala

Neutron-deuteron analyzing power data at En = 22.5 MeV

NUCLEAR REACTIONS 2H(polarized n, n), [polarized neutrons from 2H(polarized d, n) reaction], E=22.5 MeV; measured E(n), I(n), n-d analyzing power Ay(θ) using ABPIS facility at TUNL. Monte-Carlo simulations. Comparison with Faddeev calculations using several different NN potentials. Discussed three-nucleon analyzing power puzzle.

doi: 10.1103/PhysRevC.89.054001
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14395.


2012BR11      Phys.Rev. C 86, 014617 (2012)

P.A.Bradley, G.P.Grim, A.C.Hayes, Gerard Jungman, R.S.Rundberg, J.B.Wilhelmy, G.M.Hale, R.C.Korzekwa

Neutron reactions in the hohlraum at the LLNL National Ignition Facility

NUCLEAR REACTIONS 197Au, 238U(n, γ), 197Au(n, n')197mAu, 197Au, 238U(n, 2n), (n, 3n), (n, 4n), 238U(n, F), E=0-30 MeV; analyzed techniques to measure neutron yields and neutron fluence spectra from (d, t) reaction at the LLNL National Ignition Facility for deuterium-tritium (DT) inertial confinement fusion. Neutron diagnostics and dosimetry.

doi: 10.1103/PhysRevC.86.014617
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2012KI10      Phys.Rev. C 85, 061601 (2012)

Y.Kim, J.M.Mack, H.W.Herrmann, C.S.Young, G.M.Hale, S.Caldwell, N.M.Hoffman, S.C.Evans, T.J.Sedillo, A.McEvoy, J.Langenbrunner, H.H.Hsu, M.A.Huff, S.Batha, C.J.Horsfield, M.S.Rubery, W.J.Garbett, W.Stoeffl, E.Grafil, L.Bernstein, J.A.Church, D.B.Sayre, M.J.Rosenberg, C.Waugh, H.G.Rinderknecht, M.G.Johnson, A.B.Zylstra, J.A.Frenje, D.T.Casey, R.D.Petrasso, E.K.Miller, V.Yu.Glebov, C.Stoeckl, T.C.Sangster

Determination of the deuterium-tritium branching ratio based on inertial confinement fusion implosions

NUCLEAR REACTIONS 3H(d, γ)5He, 3H(d, n)4He, E(cm)=14-24 keV; measured absolute neutron and γ-ray yields in inertial confinement fusion (ICF) conditions; deduced branching ratio of γ-to-neutron in d+t reaction. Measurement of γ-to-proton branching ratio in 3He(d, γ)5Li and 3He(d, p)4He reactions used for cross calibration. Comparison with previous studies.

doi: 10.1103/PhysRevC.85.061601
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2011BO25      J.Korean Phys.Soc. 59, 833s (2011)

O.Bouland, G.M.Hale, J.E.Lynn, P.Talou, D.Bernard, O.Litaize, G.Noguere, C.De saint Jean, O.Serot

Towards Consistent Nuclear Models and Comprehensive Nuclear Data Evaluations

NUCLEAR REACTIONS 12C(n, X), E=0-6.5 MeV; analyzed σ using R matrix; deduced resonance widths. A=60-175(n, n'), E not given; calculated average prompt neutron multiplicity.

doi: 10.3938/jkps.59.833
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2011CH57      Nucl.Data Sheets 112, 2887 (2011)

M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young

ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data

COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ.

NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values.

NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.

doi: 10.1016/j.nds.2011.11.002
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2009CA28      Nucl.Data Sheets 110, 3215 (2009)

A.D.Carlson, V.G.Pronyaev, D.L.Smith, N.M.Larson, Z.Chen, G.M.Hale, F.-J.Hambsch, E.V.Gai, S.-Y.Oh, S.A.Badikov, T.Kawano, H.M.Hofmann, H.Vonach, S.Tagesen

International Evaluation of Neutron Cross Section Standards

doi: 10.1016/j.nds.2009.11.001
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2008CA28      Nucl.Data Sheets 109, 2834 (2008)

A.D.Carlson, S.A.Badikov, Z.Chen, E.Gai, G.M.Hale, F.-J.Hambsch, H.M.Hofmann, T.Kawano, N.M.Larson, S.Y.Oh, V.G.Pronyaev, D.L.Smith, S.Tagesen, H.Vonach

Covariances Obtained from an Evaluation of the Neutron Cross Section Standards

NUCLEAR REACTIONS 6Li(n, t), E < 1 MeV; 10B(n, α), E < 1 MeV; analyzed cross sections.

doi: 10.1016/j.nds.2008.11.019
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2008HA40      Nucl.Data Sheets 109, 2812 (2008)

G.M.Hale

Covariances from Light-Element R-Matrix Analyses

NUCLEAR REACTIONS 1H(n, X), E < 40 MeV; 6Li(n, t), E < 5 MeV; analyzed cross sections.

doi: 10.1016/j.nds.2008.11.015
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2008HO04      Phys.Rev. C 77, 044002 (2008)

H.M.Hofmann, G.M.Hale

4He experiments can serve as a database for determining the three-nucleon force

NUCLEAR REACTIONS 3H(p, p), (polarized p, p), (p, n), E<11 MeV; 3He(n, n), (polarized n, n), E<10 MeV; 2H(polarized d, p), (polarized d, n), (polarized d, d), (d, p), (d, n), (d, d), E<10 MeV; calculated phase shifts, angular momentum, σ(θ), analyzing powers. Microscopic calculations for 4He compound system using relativistic nucleon-nucleon and three-nucleon forces. R-matrix analysis. Comparisons with experimental data.

doi: 10.1103/PhysRevC.77.044002
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2008KA38      Nucl.Data Sheets 109, 2817 (2008)

T.Kawano, P.Talou, P.G.Young, G.Hale, M.B.Chadwick, R.C.Little

Evaluation of Covariances for Actinides and Light Elements at LANL

doi: 10.1016/j.nds.2008.11.016
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2008LI51      Nucl.Data Sheets 109, 2828 (2008)

R.C.Little, T.Kawano, G.D.Hale, M.T.Pigni, M.Herman, P.Oblozinsky, M.L.Williams, M.E.Dunn, G.Arbanas, D.Wiarda, R.D.McKnight, J.N.McKamy, J.R.Felty

Low-fidelity Covariance Project

doi: 10.1016/j.nds.2008.11.018
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2007NO10      Phys.Rev.Lett. 99, 022502 (2007)

K.M.Nollett, S.C.Pieper, R.B.Wiringa, J.Carlson, G.M.Hale

Quantum Monte Carlo Calculations of Neutron-α Scattering

doi: 10.1103/PhysRevLett.99.022502
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2006CH50      Nucl.Data Sheets 107, 2931 (2006)

M.B.Chadwick, P.Oblozinsky, M.Herman, N.M.Greene, R.D.McKnight, D.L.Smith, P.G.Young, R.E.MacFarlane, G.M.Hale, S.C.Frankle, A.C.Kahler, T.Kawano, R.C.Little, D.G.Madland, P.Moller, R.D.Mosteller, P.R.Page, P.Talou, H.Trellue, M.C.White, W.B.Wilson, R.Arcilla, C.L.Dunford, S.F.Mughabghab, B.Pritychenko, D.Rochman, A.A.Sonzogni, C.R.Lubitz, T.H.Trumbull, J.P.Weinman, D.A.Brown, D.E.Cullen, D.P.Heinrichs, D.P.McNabb, H.Derrien, M.E.Dunn, N.M.Larson, L.C.Leal, A.D.Carlson, R.C.Block, J.B.Briggs, E.T.Cheng, H.C.Huria, M.L.Zerkle, K.S.Kozier, A.Courcelle, V.Pronyaev, S.C.van der Marck

ENDF/B-VII.0: Next Generation Evaluated Nuclear Data Library for Nuclear Science and Technology

doi: 10.1016/j.nds.2006.11.001
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2003BL11      Nucl.Phys. A718, 127c (2003)

J.C.Blackmon, D.W.Bardayan, W.Bradfield-Smith, R.Brummitt, A.E.Champagne, A.A.Chen, T.Davinson, L.Dessieux, M.W.Guidry, K.I.Hahn, G.M.Hale, W.R.Hix, R.L.Kozub, Z.Ma, P.D.Parker, G.Rajbaidya, R.C.Runkle, C.M.Rowland, A.C.Shotter, M.S.Smith, L.A.Van Wormer, D.W.Visser, P.J.Woods

The 14O(α, p)17F Reaction Rate

NUCLEAR REACTIONS 1H(17F, 17F), (17F, 17F'), (17F, 14O), E(cm) ≈ 1-4 MeV; measured particle spectra. 17F(p, p'), E(cm)=2-2.5 MeV; deduced σ. 14O(α, p), E=low; deduced astrophysical reaction rate. R-matrix analysis.

doi: 10.1016/S0375-9474(03)00689-4
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2003HO14      Phys.Rev. C 68, 021002 (2003)

H.M.Hofmann, G.M.Hale

Microscopic calculation of the spin-dependent neutron scattering lengths on 3He

NUCLEAR REACTIONS 3He(n, p), E(cm) ≈ 1-40 keV; calculated σ. 3He(n, X), E not given; calculated spin-dependent scattering lengths. R-matrix analysis, microscopic calculation using realistic two- and three-nucleon forces.

doi: 10.1103/PhysRevC.68.021002
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2002FL03      Phys.Rev. C 66, 057601 (2002)

K.A.Fletcher, C.R.Brune, B.M.Fisher, R.P.Fitzgerald, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, R.C.Runkle, M.H.Wood, W.H.Geist, K.D.Veal, G.M.Hale

Kyy'(O°) for 3He(d, p)4He near the Jπ=3/2+ resonance

NUCLEAR REACTIONS 3He(polarized d, p), E=520, 890, 1490 keV; measured polarization transfer coefficient. 5Li deduced resonance.

doi: 10.1103/PhysRevC.66.057601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0943.


2002FO05      Few-Body Systems 31, 139 (2002)

A.C.Fonseca, G.Hale, J.Haidenbauer

Four-Nucleon States in the Continuum: A means to probe the nucleon-nucleon interaction

NUCLEAR REACTIONS 3He(polarized n, n), E=1-8 MeV; calculated σ, σ(θ), Ay(θ), resonance features. Comparison with data, several nucleon-nucleon interactions considered.

doi: 10.1007/s006010200012
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2002TI10      Nucl.Phys. A708, 3 (2002)

D.R.Tilley, C.M.Cheves, J.L.Godwin, G.M.Hale, H.M.Hofmann, J.H.Kelley, C.G.Sheu, H.R.Weller

Energy Levels of Light Nuclei A = 5, 6, 7

COMPILATION 5,6n, 5,6,7H, 5,6,7He, 5,6,7Li, 5,6,7Be, 6,7B, 6C; compiled, evaluated structure data.

doi: 10.1016/S0375-9474(02)00597-3
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This article is in the ENSDF database. For more information, select a mass: 5 , 6 , 7 .


2001HE22      Nucl.Phys. A688, 499c (2001)

M.Heil, A.Couture, J.Daly, R.Detwiler, J.Gorres, G.Hale, F.Kappeler, R.Reifarth, U.Giesen, E.Stech, P.Tischhauser, C.Ugalde, M.Wiescher

A Measurement of the 13C(α, α) Differential Cross Section and Its Application to the 13C(α, n) Reaction

NUCLEAR REACTIONS 13C(α, α), E=2.6-6.2 MeV; measured σ(θ). 13C(α, n), E=0-2 MeV; calculated σ, S-factor following r-matrix analysis of elastic scattering data. Comparison with earlier results for s-process conditions.

doi: 10.1016/S0375-9474(01)00768-0
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2001JO16      Nucl.Phys. A688, 566c (2001)

A.S.Johnson, G.M.Hale

Recent R-Matrix Results for np-Capture

NUCLEAR REACTIONS 1H(n, γ), E=0.01-40 MeV; calculated σ following R-matrix fit. Comparison with data and with ENDF values.

doi: 10.1016/S0375-9474(01)00789-8
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2001PF02      Phys.Rev. C64, 044003 (2001)

B.Pfitzinger, H.M.Hofmann, G.M.Hale

Elastic p-3He and n-3H Scattering with Two- and Three-Body Forces

NUCLEAR REACTIONS 3He(p, p), 3H(n, n), E(cm)=0-5 MeV; calculated phase shifts, σ(θ), σ. Two- and three-nucleon forces, R-matrix analysis.

doi: 10.1103/PhysRevC.64.044003
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2000CR01      Phys.Rev. C61, 034006 (2000)

B.J.Crowe III, C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, A.C.Fonseca, G.M.Hale, K.A.Fletcher

Analyzing Powers for 2H(d(pol), d)2H at Deuteron Energies of 3.0, 4.75, and 6.0 MeV

NUCLEAR REACTIONS 2H(polarized d, d), E=3.0, 4.75, 6.0 MeV; measured tensor analyzing powers vs θ; deduced nucleon-nucleon p-wave contributions. R matrix parameterization, microscopic four-body calculations.

doi: 10.1103/PhysRevC.61.034006
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1999CH14      Nucl.Sci.Eng. 131, 293 (1999)

M.B.Chadwick, P.G.Young, S.Chiba, S.C.Frankle, G.M.Hale, H.G.Hughes, A.J.Koning, R.C.Little, R.E.MacFarlane, R.E.Prael, L.S.Waters

Cross-Section Evaluations to 150 MeV for Accelerator-Driven Systems and Implementation in MCNPX

NUCLEAR REACTIONS H, C, N, O, 27Al, Si, P, Ca, Cr, Fe, Ni, Cu, Nb, W, Hg, Pb(n, X), (p, X), E < 150 MeV; compiled, evaluated σ, σ(θ).

doi: 10.13182/NSE98-48
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1999CS02      Phys.Rev. C59, 1207 (1999); Erratum Phys.Rev. C62, 049901 (2000)

A.Csoto, G.M.Hale

Search for Excited States in 3H and 3He

NUCLEAR STRUCTURE 3H, 3He; calculated d+N scattering matrices; deduced virtual excited states. Phenomenological interactions.

doi: 10.1103/PhysRevC.59.1207
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1999GE19      Phys.Rev. C60, 054003 (1999); Erratum Phys.Rev. C67, 059904 (2003)

W.H.Geist, C.R.Brune, H.J.Karwowski, E.J.Ludwig, K.D.Veal, G.M.Hale

The 3He(d(pol), p)4He Reaction at Low Energies

NUCLEAR REACTIONS 3H(polarized d, p), E=60-641 keV; measured σ(E, θ), Ay(E, θ), Azz(E, θ), Ayy(E, θ), Axz(E, θ); deduced low-energy S-factor, electron screening potential. 5Li deduced levels, J, π. R-matrix analysis.

doi: 10.1103/PhysRevC.60.054003
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1998CH33      Phys.Rev. C58, 2205 (1998); Erratum Phys.Rev. C59, 558 (1999)

S.Chiba, K.Togasaki, M.Ibaraki, M.Baba, S.Matsuyama, N.Hirakawa, K.Shibata, O.Iwamoto, A.J.Koning, G.M.Hale, M.B.Chadwick

Measurement and Theoretical Analysis of Neutron Elastic Scattering and Inelastic Reactions Leading to a Three-Body Final State for 6Li at 10 to 20 MeV

NUCLEAR REACTIONS 6Li(n, n), (n, n'), E=11.5, 14.1, 18.0 MeV; measured neutron spectra, σ(E, θ); deduced optical model parameters, breakup channel final state interaction features.

doi: 10.1103/PhysRevC.58.2205
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1998CS02      Nucl.Phys. A631, 783c (1998)

A.Csoto, G.M.Hale

S-Matrix Studies of Resonances in A = 3, 4, 5, 6 and 12 Nucleon Systems

doi: 10.1016/S0375-9474(98)00109-2
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1998WI25      Few-Body Systems 24, 27 (1998)

W.S.Wilburn, C.R.Gould, G.M.Hale, P.R.Huffman, C.D.Keith, N.R.Roberson, W.Tornow

Measurements at Low Energies of the Polarization-Transfer Coefficient Kyy' for the Reaction 3H(p(pol), n(pol))3He at 0°

NUCLEAR REACTIONS 3H(polarized p, n), E=1.9, 5.2, 5.8 MeV; measured polarization transfer. Polarized neutron source application discussed. Comparison with R-matrix predictions.

doi: 10.1007/s006010050074
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1997CS01      Phys.Rev. C55, 536 (1997)

A.Csoto, G.M.Hale

S-Matrix and R-Matrix Determination of the Low-Energy 5He and 5Li Resonance Parameters

NUCLEAR REACTIONS 4He(n, n), (p, p), E(cm) ≤ 15 MeV; analyzed phase shifts vs E. 5He, 5Li deduced resonance parameters. Microscopic cluster model.

doi: 10.1103/PhysRevC.55.536
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1997CS03      Phys.Rev. C55, 2366 (1997)

A.Csoto, G.M.Hale

Nature of the First Excited State of 4He

NUCLEAR REACTIONS 3H(p, p), E(cm) ≤ 1.5 MeV; analyzed σ(θ). 4He deduced level energy, width. Extended R-matrix method, cluster model, A=3 system distortions.

doi: 10.1103/PhysRevC.55.2366
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1997HA37      Nucl.Phys. A621, 177c (1997)

G.M.Hale

Extrapolation of α + Carbon Reaction Cross Sections to Astrophysical Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), 13C(α, n), E not given; analyzed reaction σ data; deduced astrophysical S-factor vs E, extrapolation methods accuracy. Astrophysical implications, 16N β-delayed α-decay data also considered.

doi: 10.1016/S0375-9474(97)00234-0
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1997HO01      Nucl.Phys. A613, 69 (1997)

H.M.Hofmann, G.M.Hale

Microscopic Calculation of the 4He System

NUCLEAR STRUCTURE 4He; calculated point Coulomb form factors, levels. Resonating group model.

NUCLEAR REACTIONS 3He(n, n), 3H(p, p), 2H(d, d), E(cm) ≤ 12.5 MeV; calculated phase shifts vs E. 3H(p, p), (polarized p, p), 3H(p, n), 3He(n, n), 3He(polarized n, n), E(cm)=3 MeV; analyzed σ(θ), analyzing power data. 2H(d, p), (d, n), E(cm)=2.11 MeV; analyzed σ(θ). 2H(polarized d, p), E(cm)=2-11 MeV; analyzed iT11(θ), T20(θ), T21(θ), T22(θ). 2H(polarized d, n), E(cm)=2.11 MeV; analyzed vector analyzing power vs θ. 2H(d, d), E(cm)=3.11 MeV; analyzed σ(θ). 2H(polarized d, d), E(cm)=3.11 MeV; analyzed iT11(θ), T20(θ), T21(θ), T22(θ). Resonating group model.

doi: 10.1016/S0375-9474(96)00418-6
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1994FL03      Phys.Rev. C49, 2305 (1994)

K.A.Fletcher, Z.Ayer, T.C.Black, R.K.Das, H.J.Karwowski, E.J.Ludwig, G.M.Hale

Tensor Analyzing Power for 2H(d, p)3H and 2H(d, n)3He at Deuteron Energies of 25, 40, 60, and 80 keV

NUCLEAR REACTIONS 2H(polarized d, p), (polarized d, n), E=25-80 keV; measured σ(θ), tensor analyzing power vs θ; deduced implications for neutron-lean fusion reaction, entrance channel quintent S-state role.

doi: 10.1103/PhysRevC.49.2305
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1994KE09      Phys.Rev. C50, 237 (1994)

C.D.Keith, C.R.Gould, D.G.Haase, N.R.Roberson, W.Tornow, G.M.Hale, H.M.Hofmann, H.Postma

Sensitivity of Polarized Neutron-Polarized 3He Scattering to the Excited Level Structure of 4He

NUCLEAR REACTIONS 3He(polarized n, n), (n, n), E=0.1-10 MeV; calculated σ(E), total longitudinal, transverse σ differences; deduced sensitivity to 4He level structure. Multi-channel resonating group model, polarized target.

doi: 10.1103/PhysRevC.50.237
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1993CE02      Phys.Rev. C47, 1178 (1993)

F.E.Cecil, H.Liu, J.S.Yan, G.M.Hale

Measurement of Branching Ratios of Low Energy Deuteron-Induced Nuclear Reactions on 2H, 6Li, and 10B

NUCLEAR REACTIONS, ICPND 2H(d, p), (d, n), E(cm)=3-15 keV; 6Li(d, p), (d, α), E(cm)=20-135 keV; 10B(d, p), (d, α), E(cm)=58-142 keV; measured spectra, yield ratios.

doi: 10.1103/PhysRevC.47.1178
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1992BO47      Nucl.Fusion 32, 611 (1992), Erratum Nucl.Fusion 33, 1919, (1993)

H.-S.Bosch, G.M.Hale

Improved Formulas for Fusion Cross-Sections and Thermal Reactivities

doi: 10.1088/0029-5515/32/4/I07
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1992TI02      Nucl.Phys. A541, 1 (1992)

D.R.Tilley, H.R.Weller, G.M.Hale

Energy Levels of Light Nuclei A = 4

COMPILATION 4H, 4He, 4Li; compiled, evaluated structure data.

doi: 10.1016/0375-9474(92)90635-W
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1991BO23      Phys.Rev. C44, 1289 (1991)

L.N.Bogdanova, G.M.Hale, V.E.Markushin

Analytical Structure of the S Matrix for the Coupled Channel Problem d + t → n + α n + α → d + t and the Interpretation of the J(π) = (3/2)+ Resonance in 5He

NUCLEAR REACTIONS, ICPND 3H(d, d), E ≤ 0.2 MeV; calculated σ(θ), astrophysical S-factor vs E. 5He deduced resonance role, parameters.

doi: 10.1103/PhysRevC.44.1289
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1990HA23      Phys.Rev. C42, 438 (1990)

G.M.Hale, D.C.Dodder, J.D.Seagrave, B.L.Berman, T.W.Phillips

Neutron-Triton Cross Sections and Scattering Lengths Obtained from p-3He Scattering

NUCLEAR REACTIONS 3H(n, n), E ≤ 10 MeV; calculated σ(E), scattering lengths. Coulomb corrected, charge symmetric R-matrix.

doi: 10.1103/PhysRevC.42.438
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1989YO11      Trans.Amer.Nucl.Soc. 60, 271 (1989)

P.G.Young, E.D.Arthur, M.Bozoian, T.R.England, G.M.Hale, R.J.LaBauve, R.C.Little, R.E.MacFarlane, D.G.Madland, R.T.Perry, W.B.Wilson

7. Transport data libraries for incident proton and neutron energies to 100 MeV

NUCLEAR REACTIONS 1H, 9Be, C, O, 27Al, Si, Fe, W, 238U(p, X), 1H, 9Be, C, O, 27Al, Si, Ca, Fe, W, 238U(n, X), E<100 MeV; analyzed available data; deduced σ for transport libraries.


1988KO03      Phys.Rev. C37, 917 (1988)

P.E.Koehler, C.D.Bowman, F.J.Steinkruger, D.C.Moody, G.M.Hale, J.W.Starner, S.A.Wender, R.C.Haight, P.W.Lisowski, W.L.Talbert

7Be(n, p)7Li Total Cross Section from 25 MeV to 13.5 keV

NUCLEAR REACTIONS 7Be(n, p), E=0.025-13500 eV; measured σ. 8Be levels deduced Γp, Γn, Γ. Calculated astrophysical reaction rate. R-matrix analysis.

doi: 10.1103/PhysRevC.37.917
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1987BR10      Phys.Rev. C35, 1999 (1987); Erratum Phys.Rev. C36, 1220 (1987)

R.E.Brown, N.Jarmie, G.M.Hale

Fusion-Energy Reaction 3H(d, α)n at Low Energies

NUCLEAR REACTIONS, ICPND 3H(d, α), E=80-116 keV; measured σ(E); deduced astrophysical S-factor vs E. 5He deduced resonances, Γα, Γd. Flowing gas target, Si surface barrier detectors.

doi: 10.1103/PhysRevC.35.1999
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1252.


1987HA20      Phys.Rev.Lett. 59, 763 (1987)

G.M.Hale, R.E.Brown, N.Jarmie

Pole Structure of the J(π) = (3/2)+ Resonance in 5He

NUCLEAR REACTIONS 3H(d, d), E(cm) ≤ 100 keV; calculated S-matrix amplitudes; deduced S-matrix poles. 5He deduced resonance, parameters Γ, Γn, Γd. R-matrix.

doi: 10.1103/PhysRevLett.59.763
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1987HA44      Phys.Rev.Lett. 59, 2819 (1987)

G.M.Hale, R.E.Brown, N.Jarmie

Hale, Brown, and Jarmie Reply:

doi: 10.1103/PhysRevLett.59.2819
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1986CA28      Radiat.Eff. 96, 87 (1986)

A.D.Carlson, W.P.Poenitz, G.M.Hale, R.W.Peelle

The Neutron Cross Section Standards Evaluations for ENDF/B-VI

NUCLEAR REACTIONS 6Li(n, n), (n, t), 10B(n, α), 197Au(n, γ), 235,238U, 239Pu(n, F), 238U(n, γ), E ≤ 20 MeV; compiled, evaluated reaction, fission σ(E). Simultaneous evaluation method.

doi: 10.1080/00337578608211720
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1986HA45      Radiat.Eff. 95, 97 (1986)

G.M.Hale

R-Matrix Analysis of the 7Li System with Peripheral Channel Overlap Exchange Effects

NUCLEAR REACTIONS 4He(t, t), E=3.21 MeV; calculated σ(θ). R-matrix calculations.

doi: 10.1080/00337578608208672
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1983ZA01      Phys.Rev. C27, 419 (1983)

H.Zankel, G.M.Hale

Difference of Neutron and Proton Analyzing Powers in Elastic N - d Scattering between 5 and 14 MeV

NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), E=5-14 MeV; analyzed A(θ) data; deduced Coulomb distortion role. Faddeev amplitudes.

doi: 10.1103/PhysRevC.27.419
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1981DO10      Nucl.Phys. A371, 225 (1981)

Sr.M.A.Doyle, H.W.Clark, L.J.Dries, J.L.Regner, T.R.Donoghue, G.M.Hale

Comparison of Analyzing Power and Polarization in the Reaction 3H(p, n)3He (I). New Analyzing Power Results below 4 MeV

NUCLEAR REACTIONS 3H(polarized p, n), E=1.75-4 MeV; measured A(E, θ). 4He deduced levels, J, π, T. Charge-independent R-matrix fits.

doi: 10.1016/0375-9474(81)90065-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0538.


1981ZA06      Phys.Rev. C24, 1384 (1981)

H.Zankel, G.M.Hale

Approximate Coulomb Correction to Elastic N - d Scattering

NUCLEAR REACTIONS 2H(polarized n, n), (polarized p, p), E=5 MeV; calculated σ(θ), A(θ); 1n, 1H(polarized d, d), E=10 MeV; calculated iT11(θ), T21(θ), T20(θ), T22(θ). T-matrix, Coulomb correction.

doi: 10.1103/PhysRevC.24.1384
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1977DO01      Phys.Rev. C15, 518 (1977)

D.C.Dodder, G.M.Hale, N.Jarmie, J.H.Jett, P.W.Keaton, Jr., R.A.Nisley, K.Witte

Elastic Scattering of Protons by Helium 4: New Experiments and Analysis

NUCLEAR REACTIONS 4He(p, p), E=11-14 MeV; measured σ(E, θ); deduced R-matrix parameters for E=1-17 MeV.

doi: 10.1103/PhysRevC.15.518
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1126.


1972BO15      Phys.Rev.Lett. 28, 1285 (1972)

M.Bolsterli, G.Hale

Modified Phase-Shift Analysis for p-3He Elastic Scattering

NUCLEAR REACTIONS 3He(p, p), E < 13.7 MeV; calculated phase shifts; deduced normalization parameters.

doi: 10.1103/PhysRevLett.28.1285
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1971DO11      Phys.Rev.Lett. 27, 947 (1971)

T.R.Donoghue, R.C.Haight, G.P.Lawrence, J.E.Simmons, D.C.Dodder, G.M.Hale

Polarization Transfer in the Reaction T(p, n)3He at 0° for E in the Range 3 to 16 MeV

NUCLEAR REACTIONS 3H(p, n), E=3-16 MeV; measured P(n)(E, θ=0°).

doi: 10.1103/PhysRevLett.27.947
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1970HA53      Nucl.Phys. A156, 570 (1970)

G.M.Hale, R.K.Umerjee

A Coupled Channel Schrodinger Equation Model for Four Nucleons

NUCLEAR REACTIONS 3H(p, p), (p, n), (p, d), E=5.5, 6.4 MeV; 3He(n, n), (n, p), (n, d), E=6 MeV; 2H(d, d), (d, n), (d, p), E=1.50 MeV; calculated σ(θ). Coupled-channel model.

doi: 10.1016/0375-9474(70)90253-8
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Note: The following list of authors and aliases matches the search parameter G.Hale: , G.D.HALE, G.M.HALE