NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.M.Hale Found 66 matches. 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
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
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
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
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
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
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
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
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
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
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
2015HA02 Nucl.Data Sheets 123, 165 (2015) 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
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
2014BR02 Phys.Rev. C 89, 014622 (2014) 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
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
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
2014HA18 Nucl.Data Sheets 118, 165 (2014) 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
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
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
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
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
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
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
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
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
2008HA40 Nucl.Data Sheets 109, 2812 (2008) 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
2008HO04 Phys.Rev. C 77, 044002 (2008) 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
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
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
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
2003HO14 Phys.Rev. C 68, 021002 (2003) 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
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
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
2001JO16 Nucl.Phys. A688, 566c (2001) 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
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
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
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
1999CS02 Phys.Rev. C59, 1207 (1999); Erratum Phys.Rev. C62, 049901 (2000) 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
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
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
1998CS02 Nucl.Phys. A631, 783c (1998) S-Matrix Studies of Resonances in A = 3, 4, 5, 6 and 12 Nucleon Systems
doi: 10.1016/S0375-9474(98)00109-2
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
1997CS01 Phys.Rev. C55, 536 (1997) 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
1997CS03 Phys.Rev. C55, 2366 (1997) 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
1997HA37 Nucl.Phys. A621, 177c (1997) 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
1997HO01 Nucl.Phys. A613, 69 (1997) 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
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
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
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
1992BO47 Nucl.Fusion 32, 611 (1992), Erratum Nucl.Fusion 33, 1919, (1993) Improved Formulas for Fusion Cross-Sections and Thermal Reactivities
doi: 10.1088/0029-5515/32/4/I07
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
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
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
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
1987BR10 Phys.Rev. C35, 1999 (1987); Erratum Phys.Rev. C36, 1220 (1987) 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
1987HA20 Phys.Rev.Lett. 59, 763 (1987) 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
1987HA44 Phys.Rev.Lett. 59, 2819 (1987) Hale, Brown, and Jarmie Reply:
doi: 10.1103/PhysRevLett.59.2819
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
1986HA45 Radiat.Eff. 95, 97 (1986) 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
1983ZA01 Phys.Rev. C27, 419 (1983) 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
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
1981ZA06 Phys.Rev. C24, 1384 (1981) 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
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
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
1970HA53 Nucl.Phys. A156, 570 (1970) 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
Back to query form |