NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = J.P.Lestone

Found 47 matches.

Back to query form



2021LE26      Nucl.Technology 207, s352 (2021)

J.P.Lestone, M.D.Rosen, P.Adsley

Comparison Between Historic Nuclear Explosion Yield Formulas

doi: 10.1080/00295450.2021.1909372
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2016CA03      Nucl.Data Sheets 131, 1 (2016)

R.Capote, Y.-J.Chen, F.-J.Hambsch, N.V.Kornilov, J.P.Lestone, O.Litaize, B.Morillon, D.Neudecker, S.Oberstedt, T.Ohsawa, N.Otuka, V.G.Pronyaev, A.Saxena, O.Serot, O.A.Shcherbakov, N.-C.Shu, D.L.Smith, P.Talou, A.Trkov, A.C.Tudora, R.Vogt, A.S.Vorobyev

Prompt Fission Neutron Spectra of Actinides

NUCLEAR REACTIONS 232Th, 233,234,235,238U, 237Np, 239Pu(n, F), E<30 MeV; calculated prompt fission En, In; Comparison with available data.

doi: 10.1016/j.nds.2015.12.002
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33084.


2016LE02      Nucl.Data Sheets 131, 357 (2016)

J.P.Lestone

Neutron-fragment and Neutron-neutron Correlations in Low-energy Fission

NUCLEAR REACTIONS 235U(n, F), E thermal; calculated fission En, In; Comparison with ENDF/B-VII.1 library prompt-fission neutron-spectra evaluations.

RADIOACTIVITY 252Cf(SF); calculated spontaneous fission En, In; Comparison with ENDF/B-VII.1 library prompt-fission neutron-spectra evaluations.

doi: 10.1016/j.nds.2015.12.007
Citations: PlumX Metrics


2016TA24      Phys.Rev. C 94, 064613 (2016)

P.Talou, T.Kawano, I.Stetcu, J.P.Lestone, E.McKigney, M.B.Chadwick

Late-time emission of prompt fission γ rays

NUCLEAR REACTIONS 235U, 239Pu(n, F), E=thermal; 252Cf(SF); calculated average prompt fission γ-ray spectrum, average prompt γ-ray multiplicity as a function of time, energy spectra of late fission γ rays emitted in the 10 ns to 2 μs time window following fission, cumulative average prompt total γ-ray energy and multiplicity as a function of time, pre-neutron-emission fission fragment mass yields. Hauser-Feshbach formalism using the Monte Carlo Hauser-Feshbach code CGMF. Comparison with experimental data. 134Te; γ-ray spectrum for 162-ns isomer decay in the 10-100 ns coincidence window gated on the post-neutron-emission 134Te fission fragment.

RADIOACTIVITY 252Cf(SF); see keywords above for Nuclear Reactions

doi: 10.1103/PhysRevC.94.064613
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2014LE13      Nucl.Data Sheets 118, 208 (2014)

J.P.Lestone, T.T.Strother

Energy Dependence of Plutonium and Uranium Average Fragment Total Kinetic Energies

NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=0-20 MeV; calculated post-neutron evaporation TKE. Compared to data.

doi: 10.1016/j.nds.2014.04.038
Citations: PlumX Metrics


2014LE23      Nucl.Data Sheets 119, 213 (2014)

J.P.Lestone, E.F.Shores

Uranium and Plutonium Average Prompt-fission Neutron Energy Spectra (PFNS) from the Analysis of NTS NUEX Data

NUCLEAR REACTIONS 235U, 239Pu(n, F), E=1.5, 2.5, 3.5, 4.5, 5.5, 6.5, 7.5, 8.5, 9.5, 10.5 MeV; measured prompt fission En, In at Nevada test site; deduced fission neutron spectra (PFNS); calculated PFNS with Los Alamos fission model.

doi: 10.1016/j.nds.2014.08.059
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14430.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23170.


2011LE36      Nucl.Data Sheets 112, 3120 (2011)

J.P.Lestone

Energy Dependence of Plutonium Fission-Product Yields

doi: 10.1016/j.nds.2011.11.008
Citations: PlumX Metrics


2010CH41      Nucl.Data Sheets 111, 2923 (2010)

M.B.Chadwick, T.Kawano, D.W.Barr, M.R.Mac Innes, A.C.Kahler, T.Graves, H.Selby, C.J.Burns, W.C.Inkret, A.L.Keksis, J.P.Lestone, A.J.Sierk, P.Talou

Fission Product Yields from Fission Spectrum n+239Pu for ENDF/B-VII.1

NUCLEAR REACTIONS 239Pu(n, F)99Mo/95Zr/140Ba/144Ce/147Nd, E=0.2-2 MeV; measured fission products; deduced fission product yields and its energy dependence. Comparison with ENDF/B-VII.0 library, LANL-ILRR measurements.

doi: 10.1016/j.nds.2010.11.003
Citations: PlumX Metrics


2009LE12      Phys.Rev. C 79, 044611 (2009)

J.P.Lestone, S.G.McCalla

Statistical model of heavy-ion fusion-fission reactions

NUCLEAR REACTIONS 139La, 159Tb, 169Tm, 181Ta(19F, X), E=70-140 MeV; 197Au, 208Pb(16O, X), E=70-140 MeV; 192Os(18O, X), E=70-140 MeV; calculated fusion cross sections, pre-scission neutron multiplicity. 177Hf(9Be, X), E not given; 169Tm, 175Lu(11B, X), E not given; 169Tm, 174Yb, 175Lu, 182W, 198Pt(12C, X), E not given; 165Ho(14N, X), E not given; 165Ho, 170Er, 170Yb, 174Yb, 175Lu, 182W, 188Os(16O, X), E not given; 192Os(18O, X), E not given; 159Tb(22Ne, X), E not given; 160Gd(26Mg, X), E not given; calculated fission cross sections using JOANNE4 formalism; deduced model parameters. Comparison with experimental data. 195Pb; calculated deformation dependence of dissipation constant. 210Po; calculated potential energy surface, ground-state and saddle-point curvatures, fission barriers, and fission lifetimes for compound nucleus.

doi: 10.1103/PhysRevC.79.044611
Citations: PlumX Metrics


2008LE06      Int.J.Mod.Phys. E17, 323 (2008)

J.P.Lestone

An evaporation-based model of thermal neutron induced ternary fission of plutonium

NUCLEAR REACTIONS 239,241Pu(n, F), E not given; calculated ternary fission probabilities, various scission configurations, and particle binding energies for 1H to 30Mg (Z=1-12, A=1-30) fragments. Comparison with experimental data.

doi: 10.1142/S0218301308009045
Citations: PlumX Metrics


2008MC03      Phys.Rev.Lett. 101, 032702 (2008)

S.G.McCalla, J.P.Lestone

Fission Decay Widths for Heavy-Ion Fusion-Fission Reactions

NUCLEAR REACTIONS 159Tb, 169Tm, 181Ta(19F, X), E < 150 MeV; 192Os(18O, X), E < 150 MeV; 197Au(16O, X), E < 150 MeV; calculated fission cross sections and prescission neutron multiplicities using a statistical model.

doi: 10.1103/PhysRevLett.101.032702
Citations: PlumX Metrics


2005LE26      Phys.Rev. C 72, 014604 (2005)

J.P.Lestone

Temperature of low-energy ternary fission from the dependence of particle yields on the mass of the fissioning system

NUCLEAR REACTIONS 233,235U, 239,241Pu(n, F), E=thermal; analyzed ternary fission product yields; deduced nuclear temperature.

RADIOACTIVITY 250,252Cf(SF); analyzed ternary fission product yields; deduced nuclear temperature.

doi: 10.1103/PhysRevC.72.014604
Citations: PlumX Metrics


2004LE31      Phys.Rev. C 70, 021601 (2004)

J.P.Lestone

Combined statistical and dynamical model of ternary nuclear fission

NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated ternary fission probabilities, light charged particles energy spectra. Combined statistical and dynamical model.

doi: 10.1103/PhysRevC.70.021601
Citations: PlumX Metrics


2002BU08      Phys.Rev. C65, 044606 (2002); Erratum Phys.Rev. C65, 069904 (2002)

R.D.Butt, M.Dasgupta, I.Gontchar, D.J.Hinde, A.Mukherjee, A.C.Berriman, C.R.Morton, J.O.Newton, A.E.Stuchbery, J.P.Lestone

Effects on Finite Ground-State Spin on Fission Fragment Angular Distributions following Collisions with Spherical or Deformed Nuclei

NUCLEAR REACTIONS 209Bi(16O, F), E(cm) ≈ 76 MeV; 232Th(10B, F), E(cm) ≈ 46 MeV; 176Lu(31P, F), E(cm) ≈ 122 MeV; 178,178mHf(28Si, X), E ≈ 116 MeV; calculated fission fragments angular distributions, dependence on target spin.

doi: 10.1103/PhysRevC.65.044606
Citations: PlumX Metrics


2000CA48      Phys.Rev. C62, 054612 (2000)

A.L.Caraley, B.P.Henry, J.P.Lestone, R.Vandenbosch

Investigation of the Level Density Parameter using Evaporative α-Particle Spectra from the 19F + 181Ta Reaction

NUCLEAR REACTIONS 181Ta(19F, X), E=121, 154, 179, 195 MeV; measured evaporation residue and fission fragment angular distributions, Ep, Eα, (evaporation residue)p-, (evaporation residue)α-coin; deduced level density parameter excitation energy dependence. Comparisons with model predictions.

doi: 10.1103/PhysRevC.62.054612
Citations: PlumX Metrics


1999KA14      Phys.Rev. C59, 2580 (1999)

S.Kailas, D.M.Nadkarni, A.Chatterjee, A.Saxena, S.S.Kapoor, R.Vandenbosch, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, J.D.Bierman

Fission Fragment Folding Angle Distributions for the Systems 11B + 237Np, 12C + 236U, and 16O + 232Th in the Energy Range 1.1 < E/VB < 2.1

NUCLEAR REACTIONS 232Th(16O, F), E=100-144.8 MeV; 236U(12C, F), E=80-130 MeV; 237Np(11B, F), E=60-118 MeV; measured fission σ, folding angle distributions; deduced momentum transfer components, fission anisotropies. Saddle-point statistical model.

doi: 10.1103/PhysRevC.59.2580
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6138.


1999LE10      Phys.Rev. C59, 1540 (1999)

J.P.Lestone

Calculating Fission Rates at High Spin: Incorporation of rotational degrees of freedom in thermodynamically fluctuating axially symmetric systems

NUCLEAR REACTIONS 197Au, 208Pb(16O, X), E=75-130 MeV; 192Os(18O, X), E=80-125 MeV; calculated fission, evaporation residue σ, prescission neutron multiplicities; deduced role of rotational degrees of freedom. Statistical model calculations. Comparison with data.

doi: 10.1103/PhysRevC.59.1540
Citations: PlumX Metrics


1998LE36      Phys.Rev.Lett. 81, 4776 (1998)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Comment on ' Anomalous Peaklike Structure in the Fission Fragment Anisotropies at Sub-Barrier Energies in 11B, 12C, 16O, 19F + 232Th Reactions '

NUCLEAR REACTIONS 232Th(11B, X), E(cm)=46-66 MeV; measured fission fragments angular distributions; deduced reaction mechanism features, no peaklike structure in anisotropies.

doi: 10.1103/PhysRevLett.81.4776
Citations: PlumX Metrics


1998SO01      Phys.Rev. C57, 722 (1998)

A.A.Sonzogni, J.D.Bierman, M.P.Kelly, J.P.Lestone, J.F.Liang, R.Vandenbosch

Transfer and Surface Vibration Couplings in the Fusion of 40Ca + 46,48,50Ti at Near-Barrier Energies

NUCLEAR REACTIONS 46,48,50Ti(40Ca, X), E=97-150 MeV; measured fusion, quasielastic σ(E, θ); deduced fusion, quasielastic σ(E), barrier distributions, surface vibration coupling parameters. Coupled-channel calculations.

doi: 10.1103/PhysRevC.57.722
Citations: PlumX Metrics


1998SO22      Phys.Rev. C58, R1873 (1998)

A.A.Sonzogni, R.Vandenbosch, A.L.Caraley, J.P.Lestone

Is Quasifission Responsible for Anomalous Fission Fragment Anisotropies ?

NUCLEAR REACTIONS 236U(12C, 4n), E=62-73 MeV; measured excitation function; deduced no quasifission competition.

doi: 10.1103/PhysRevC.58.R1873
Citations: PlumX Metrics


1997KE12      Phys.Rev. C56, 3201 (1997)

M.P.Kelly, J.F.Liang, A.A.Sonzogni, K.A.Snover, J.P.S.van Schagen, J.P.Lestone

Preequilibrium Particle Emission and the Giant-Dipole Resonance in Sn Nuclei

NUCLEAR REACTIONS 100Mo(18O, X), E=200 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra; deduced pre-equilibrium emission features. 115In, 118Sn deduced GDR pre-equilibrium emission effects.

doi: 10.1103/PhysRevC.56.3201
Citations: PlumX Metrics


1997LE01      Phys.Rev. C55, R16 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, D.Prindle

Near- and Sub-Barrier 12C + 232Th Fission Fragment Anisotropies

NUCLEAR REACTIONS 232Th(12C, F), E=57.6-75.2 MeV; measured fission σ, fission fragment anisotropies.

doi: 10.1103/PhysRevC.55.R16
Citations: PlumX Metrics


1997LE30      J.Phys.(London) G23, 1349 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Near- and Sub-Barrier Fission Fragment Anisotropies and the Failure ofthe Statistical Theory of Fission Decay Rates

NUCLEAR REACTIONS 232Th(16O, F), (19F, F), E(cm)=70-110 MeV; 238U(16O, F), E(cm)=75-90 MeV; 236,238U, 237Np, 232Th(12C, F), E(cm)=55-80 MeV; 232Th, 238U(11B, F), E(cm)=40-50 MeV; 238U(7Li, F), E(cm)=24-40 MeV; measured fission fragment σ(θ); deduced anisotropy, entrance channel effects, compound nucleus features. Statistical model analysis.

doi: 10.1088/0954-3899/23/10/024
Citations: PlumX Metrics


1997LE31      Phys.Rev. C56, R2907 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Influence of the Ground State Spin of Target Nuclei on the Anomalous Behavior of Fission Fragment Anisotropies

NUCLEAR REACTIONS 235,236,238U(12C, F), E(cm)=57-82 MeV; measured fission σ, fragment σ(θ); deduced K-states equilibration time, anomalous behaviour target spin dependence.

doi: 10.1103/PhysRevC.56.R2907
Citations: PlumX Metrics


1996LE04      Phys.Rev. C53, 2014 (1996)

J.P.Lestone

Analysis of α-Particle Emission from 19F + 181Ta Reactions Leading to Residues

NUCLEAR REACTIONS 181Ta(19F, X), E not given; analyzed α-particle emission analyses; deduced need to use care in statistical model code application.

doi: 10.1103/PhysRevC.53.2014
Citations: PlumX Metrics


1996VA12      Phys.Rev. C54, R977 (1996)

R.Vandenbosch, J.D.Bierman, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, S.Kailas, D.M.Nadkarni, S.S.Kapoor

Disappearance of Entrance Channel Dependence of Fission Fragment Anisotropies at Well-Above-Barrier Energies

NUCLEAR REACTIONS 237Np(11B, F), E=60-118 MeV; 236U(12C, F), E=80-130 MeV; 232Th(16O, F), E=100-145 MeV; measured fission fragment σ(θ), anisotropies; deduced entrance channel independence.

doi: 10.1103/PhysRevC.54.R977
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6138.


1995HI05      Nucl.Phys. A583, 135c (1995); Erratum Nucl.Phys. A587, 853 (1995)

D.J.Hinde, C.R.Morton, M.Dasgupta, J.R.Leigh, J.P.Lestone, R.C.Lemmon, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa

Fusion Barrier Distributions and Fission Anisotropies

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E(cm) ≈ 55-70 MeV; analyzed fusion σ(E). 208Pb(16O, F), (16O, X), E(cm) ≈ 70-85 MeV; measured fission anisotropies, fusion barrier distribution.

doi: 10.1016/0375-9474(94)00647-6
Citations: PlumX Metrics


1995HI07      Phys.Rev.Lett. 74, 1295 (1995)

D.J.Hinde, M.Dasgupta, J.R.Leigh, J.P.Lestone, J.C.Mein, C.R.Morton, J.O.Newton, H.Timmers

Fusion-Fission Versus Quasifission: Effect of nuclear orientation

NUCLEAR REACTIONS 238U(16O, F), E=76-104 MeV; measured fission fragment σ(θ) vs E; deduced quasifission evidence. 238U deduced deformation features role.

doi: 10.1103/PhysRevLett.74.1295
Citations: PlumX Metrics


1995LE02      Phys.Rev. C51, 580 (1995)

J.P.Lestone

Fast Method for Obtaining Finite Range Corrected Potential Energy Surfaces

NUCLEAR STRUCTURE 208Pb; calculated surface, Coulomb energies. 160Dy, 180Ta, 200Hg, 220Fr, 240Pu, 158Er, 176Os, 229Np; calculated fission barrier vs angular momentum, equilibrium, saddle points moment of inertia. Liquid drop, finite range models.

doi: 10.1103/PhysRevC.51.580
Citations: PlumX Metrics


1995LE25      Phys.Rev. C52, 1118 (1995)

J.P.Lestone

Temperature Dependence of the Level Density Parameter

NUCLEAR STRUCTURE A=210; calculated nucleon density profile. A=60; A=210; calculated thermal excitation energy vs (temperature)2. Thomas-Fermi calculational procedure.

doi: 10.1103/PhysRevC.52.1118
Citations: PlumX Metrics


1995LE34      Phys.Rev. C52, 3151 (1995)

J.R.Leigh, M.Dasgupta, D.J.Hinde, J.C.Mein, C.R.Morton, R.C.Lemmon, J.P.Lestone, J.O.Newton, H.Timmers, J.X.Wei, N.Rowley

Barrier Distributions from the Fusion of Oxygen Ions with 144,148,154Sm and 186W

NUCLEAR REACTIONS, ICPND 186W, 144,148,154Sm(16O, X), 144Sm(17O, X), E=50-110 MeV; measured fusion σ(E), σ(evaporation residue, θ) vs E; deduced fusion barrier distributions. Enriched targets. Coupled-channels analysis.

doi: 10.1103/PhysRevC.52.3151
Citations: PlumX Metrics


1995MO22      Phys.Rev. C52, 243 (1995)

C.R.Morton, D.J.Hinde, J.R.Leigh, J.P.Lestone, M.Dasgupta, J.C.Mein, J.O.Newton, H.Timmers

Resolution of the Anomalous Fission Fragment Anisotropies for the 16O + 208Pb Reaction

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), (16O, F), E(cm)=71-85 MeV; measured evaporation residue, fission σ, fission fragment anisotropies, Eα, Iα; deduced fusion barrier distribution, σ(E). Transition state model.

doi: 10.1103/PhysRevC.52.243
Citations: PlumX Metrics


1994LE01      Phys.Rev. C49, 372 (1994)

J.P.Lestone, A.Gavron

Statistical Model Analysis of Fast-Neutron-Induced Fission of U Isotopes

NUCLEAR REACTIONS 232,233,234,235,236,238U(n, F), E ≤ 20 MeV; analyzed fission σ(E). 235,238U(n, 2n), (n, 3n), E ≤ 20 MeV; analyzed σ(E); deduced γ-deformation associated collective level density enhancement washing out. Statistical model.

doi: 10.1103/PhysRevC.49.372
Citations: PlumX Metrics


1994LE11      Nucl.Sci.Eng. 116, 213 (1994)

J.P.Lestone, A.Gavron

Statistical Model Calculation of the 237U Fission Cross Section

NUCLEAR REACTIONS 232U(n, F), E < 10 MeV; 233,234,235,236,238U(n, F), E < 20 MeV; 237U(n, F), E ≤ 20 MeV; calculated fission σ(E). 238U(γ, F), E ≈ 5.5-10 MeV; calculated fission probability vs E. Statistical model.

doi: 10.13182/NSE94-A19814
Citations: PlumX Metrics


1994LE31      Yad.Fiz. 57, No 7, 1268 (1994); Phys.Atomic Nuclei 57, 1200 (1994)

J.P.Lestone, A.Gavron

Neutron-Induced Fission of Uranium Isotopes up to 100 MeV

NUCLEAR REACTIONS 232,233,234,235,236,238U(n, F), E ≤ 20 MeV; 238,235U(n, 2n), (n, 3n), E ≈ 5-20 MeV; analyzed fission, reaction σ(E); deduced scaling factor necessity, energy dependence. Nilsson model based state densities, spin cut-off parameters, statistical model.


1994MO24      Phys.Rev.Lett. 72, 4074 (1994)

C.R.Morton, M.Dasgupta, D.J.Hinde, J.R.Leigh, R.C.Lemmon, J.P.Lestone, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa

Clear Signatures of Specific Inelastic and Transfer Channels in the Distribution of Fusion Barriers

NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E=61-100 MeV; measured fusion σ(E); deduced fusion barrier distribution structure, specific transfer channels signature.

doi: 10.1103/PhysRevLett.72.4074
Citations: PlumX Metrics


1993LE05      Phys.Rev.Lett. 70, 2245 (1993)

J.P.Lestone

Determination of the Time Evolution of Fission from Particle Emission

NUCLEAR REACTIONS 164Er(28Si, F), E=185 MeV; analyzed prescission particle emission data following fission. 192Pb deduced fission time scale. Other reactions included.

doi: 10.1103/PhysRevLett.70.2245
Citations: PlumX Metrics


1993LE11      Nucl.Phys. A559, 277 (1993)

J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, M.Zielinska-Pfabe

Pre-Scission Charged-Particle Multiplicities following the Reactions 164,167,170Er + 28Si

NUCLEAR REACTIONS 164,167,170Er(28Si, F), E=140-185 MeV; measured fission (fragment)p-, (fragement)α-coin, σ(fragment, θ, E(α, p)); deduced pre-, post-fission proton and alpha multiplicities. 192,195,198Pb deduced statistical model level-density parameters, dynamical effects.

doi: 10.1016/0375-9474(93)90192-Z
Citations: PlumX Metrics


1992RO03      Phys.Rev. C45, 719 (1992)

H.Rossner, D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, J.X.Wei, S.Elfstrom

Influence of Pre-Fission Particle Emission on Fragment Angular Distributions Studied for 208Pb(16O, f)

NUCLEAR REACTIONS 208Pb(16O, F), E=80-130 MeV; measured σ(fragment θ, En); deduced pre-, post-scission multiplicities. 224Th deduced fission yield vs decay time, temperature.

doi: 10.1103/PhysRevC.45.719
Citations: PlumX Metrics


1991HI08      Phys.Lett. 258B, 35 (1991)

D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, S.Elfstrom, J.X.Wei, M.Zielinska-Pfabe

The Effect of the Angular Momentum Dependence of the Fission Probability on the Determination of Fission Time Scales from Fission Excitation Functions

NUCLEAR REACTIONS 197Au(16O, F), 181Ta(19F, F), E not given; calculated fission probability vs excitation energy; deduced angular momentum role in fission time scales determination.

doi: 10.1016/0370-2693(91)91204-9
Citations: PlumX Metrics


1991LE21      Phys.Rev.Lett. 67, 1078 (1991)

J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, D.G.Popescu

Fission Time Scales from Prescisson Charged-Particle Multiplicities

NUCLEAR REACTIONS 164,167,170Er(28Si, X), E=140-185 MeV; measured proton, α-spectra, multiplicities; deduced reaction mechanism. 192,195,198Pb deduced fission characteristics.

doi: 10.1103/PhysRevLett.67.1078
Citations: PlumX Metrics


1991WE19      Nucl.Instrum.Methods Phys.Res. A306, 557 (1991)

J.X.Wei, J.R.Leigh, D.C.Weisser, J.O.Newton, S.Elfstrom, J.P.Lestone, J.X.Chen, D.G.Popescu, D.J.Hinde

A Compact Velocity Filter for Evaporation Residue Measurements

NUCLEAR REACTIONS 130Te(28Si, X), E=100-160 MeV; 170Er(16O, X), E=110 MeV; 176Yb(16O, X), E=100 MeV; 186W(16O, X), E=70 MeV; 154Sm(16O, X), E=60 MeV; measured σ(evaporation residue θ). Velocity filter.

doi: 10.1016/0168-9002(91)90052-R
Citations: PlumX Metrics


1990LE07      Nucl.Phys. A509, 178 (1990)

J.P.Lestone, J.R.Leigh, J.O.Newton, J.X.Wei

Fission Fragment Angular Distributions following Transfer Reactions for 232Th + 16O

NUCLEAR REACTIONS 232Th(16O, F), E=80-92 MeV; measured fission fragment σ(E, θ), (fragment)(particle)-coin, σ(fragment φ, θ) following transfer, X=C, N.

doi: 10.1016/0375-9474(90)90380-5
Citations: PlumX Metrics


Back to query form


Note: The following list of authors and aliases matches the search parameter J.P.Lestone: , J.P.LESTONE