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NSR database version of April 26, 2024.

Search: Author = S.F.Mughabghab

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2018HE06      Nucl.Data Sheets 148, 214 (2018)

M.Herman, A.Trkov, R.Capote, G.P.A.Nobre, D.A.Brown, R.Arcilla, Y.Danon, A.Plompen, S.F.Mughabghab, Q.Jing, G.Zhigang, L.Tingjin, L.Hanlin, R.Xichao, L.Leal, B.V.Carlson, T.Kawano, M.Sin, S.P.Simakov, K.Guber

Evaluation of Neutron Reactions on Iron Isotopes for CIELO and ENDF/B-VIII.0

NUCLEAR REACTIONS ⁵⁶Fe(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).

doi: 10.1016/j.nds.2018.02.004
Citations: PlumX Metrics

2014BR09      Nucl.Data Sheets 118, 144 (2014)

D.A.Brown, R.Arcilla, R.Capote, S.F.Mughabghab, M.W.Herman, A.Trkov, H.I.Kim

Zirconium Evaluations for ENDF/B-VII.2 for the Fast Region

COMPILATION ^{90,91,92,93,94,95,96}Zr(n, x), E=0=20 MeV; calculated, evaluated σ, σ(θ) including resonance region using EMPIRE-3.1 code. Compared with available data and evaluated databases.

doi: 10.1016/j.nds.2014.04.021
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2014MU07      Nucl.Data Sheets 118, 287 (2014)

S.F.Mughabghab

Recent Investigations and Findings about the 2d- and 3d- Neutron Strength Functions and the p-wave Scattering Radius

NUCLEAR REACTIONS ⁵⁸Ni(n, x), E=0-14 MeV;¹³⁹La(n, x), E=0-8 MeV;¹⁸²W(n, x), E=0-7 MeV;²⁰⁹Bi(n, x), E=1-6 MeV;²³³U(n, x), E=200 keV-4 MeV; calculated total σ, shape-elastic σ for partial waves. Compared to data.

NUCLEAR STRUCTURE ¹⁶O, Cr, ^54,57Fe, ^58,60Ni, ⁸⁹Y, ⁹⁰Zr, ⁹⁸Mo, ^182,184,186W, ²⁰⁶Pb, ²⁰⁹Bi, ²³²Th, ^233,235,238U, ²³⁷Np, ^239,240,242Pu; calculated s-, p-, d-wave neutron strength functions, s-, p-wave scattering radii. Compared to Atlas of Neutron Resonances.

doi: 10.1016/j.nds.2014.04.060
Citations: PlumX Metrics

2012PR13      Nucl.Data Sheets 113, 3120 (2012)

B.Pritychenko, S.F.Mughabghab

Neutron Thermal Cross Sections, Westcott Factors, Resonance Integrals, Maxwellian Averaged Cross Sections and Astrophysical Reaction Rates Calculated from the ENDF/B-VII.1, JEFF-3.1.2, JENDL-4.0, ROSFOND-2010, CENDL-3.1 and EAF-2010 Evaluated Data Libraries

COMPILATION Z=1-100; A=1-257; compiled, analyzed Maxwellian-averaged neutron capture σ, neutron-induced fission σ, elastic scattering σ, astrophysical reaction rates, Westcott factors, resonance integrals, neutron thermal σ. BNL report, http://arxiv.org/abs/1208.2879, contains complete set of tables.

NUCLEAR REACTIONS ²²²Rn, ^{223,224,225,226,228}Ra, ^{225,226,227,228}Ac, ^{227,228,229,230,231,232,233,234}Th, ^{228,229,230,231,232,233,234}Pa, ^{230,232,232,233,234,235,236,237,238,239,240,241}U, ^{234,235,236,237,238,239}Np, ^{234,236,237,238,239,240,241,242,243,244,245,246,247}Pu, ^{239,240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,249,250}Bk, ^{246,248,249,250,251,252,253,254}Cf, ^{250,251,252,253,254,255,256,257}Es, ^{252,253,255,257}Fm(n, F), E<20 MeV; calculated Maxwellian-averaged σ, astrophysical reaction rates thermal σ, neutron thermal σ, Westcott factors, resonance integrals and their uncertainties using evaluated neutron libraries. Comparison with experimental data and Atlas of Neutron Resonances. BNL report, http://arxiv.org/abs/1208.2879, contains complete set of tables.

NUCLEAR REACTIONS ^1,2,3H, ^3,4He, ^6,7Li, ^7,9,10Be, ^10,11B, C, ^12,13,14C, ^14,15N, ^16,17,18O, ¹⁹F, ^20,21,22Ne, ^22,23,24Na, ^24,25,26,28Mg, ^26,27Al, ^{28,29,30,31,32}Si, ^31,32,33P, ^{32,33,32,33,34,35,36}S, Cl, ^35,36,37Cl, ^{36,37,38,39,40,41,42}Ar, K, ^{39,40,41,42,43}K, Ca, ^{40,41,42,43,44,45,46,47,48}Ca, ^45,46,47,48Sc, ^{44,45,46,47,48,49,50}Ti, V, ^48,49,50,51V, ^{48,50,51,52,53,54}Cr, ^52,53,54,55Mn, ^{52,54,55,56,57,58,59,60}Fe, ^{55,56,57,58,59,60}Co, ^{56,57,58,59,60,61,62,63,64,66}Ni, Cu, ^63,64,65,67Cu, Zn, ^{62,64,65,66,67,68,69,70,72}Zn, Ga, ^{66,67,69,71,72}Ga, Ge, ^{68,69,70,71,72,73,74,75,76,77,78}Ge, ^{71,72,73,74,75,76,77,79}As, ^{72,73,74,75,76,77,78,79,80,82}Se, ^{76,77,79,81,82}Br, ^{76,78,79,80,81,82,83,84,85,86}Kr, ^{82,83,84,85,86,87}Rb, ^{82,83,84,85,86,87,88,89,90,91}Sr, ^{86,87,88,89,90,91,93}Y, ^{86,88,89,90,91,92,93,94,95,96,97}Zr, ^{90,91,92,93,94,95,96}Nb, ^{92,93,94,95,96,97,98,99,100}Mo, ^{95,96,97,98,99}Tc, ^{96,97,98,99,100,101,102,103,104,105,106}Ru, ^{99,100,101,102,103,105}Rh, ^{100,101,102,103,104,105,106,107,108,109,110,112}Pd, Ag, ^{105,106,107,108,109,110,111}Ag, Cd, ^{106,107,108,109,110,111,112,113,114,115,116}Cd, ^{111,113,114,115}In, Sn, ^{112,113,114,115,116,117,118,119,120,122,123,124,125,126,127,128}Sn, ^{121,122,123,124,125,126,127,128}Sb, ^{118,119,120,121,122,123,124,125,126,127,128,129,130,131,132}Te, ^{123,124,125,126,127,128,129,130,131,133,135}I, ^{122,123,124,125,126,127,128,129,130,131,132,133,134,135,136}Xe, ^{127,129,131,133,134,135,136,137}Cs, ^{128,129,130,131,132,133,134,135,136,137,138,139,140}Ba, ^{138,139,140,141}La, ^{134,135,136,137,138,139,140,141,142,143,144}Ce, ^141,142,143Pr, ^{140,141,142,143,144,145,146,147,148,149,150}Nd, ^{143,144,145,146,147,148,149,150,151}Pm, ^{144,145,146,147,148,149,150,151,152,153,154,156}Sm, ^{145,146,147,148,149,150,151,152,153,154,155,156,157}Eu, ^{146,147,148,149,150,151,152,153,154,155,156,157,158,159,160}Gd, ^{151,152,153,154,155,156,157,158,159,160,161}Tb, ^{153,154,155,156,157,158,159,160,161,162,163,164,165,166}Dy, ^{163,164,165,166}Ho, ^{160,161,162,164,165,166,167,168,169,170,171,172}Er, ^{165,166,167,168,169,170,171,172,173}Tm, ^{166,168,169,170,171,172,173,174,175,175}Yb, ^{169,170,171,172,173,174,175,176,177}Lu, ^{170,171,172,173,174,175,176,177,178,179,180,181,182}Hf, ^{175,176,177,179,180,181,182,183,184}Ta, ^{178,180,181,182,183,184,185,186,187,188}W, ^{181,182,183,184,185,186,187,188,189}Re, Os, ^{182,183,184,185,186,187,188,189,190,191,192,193,194}Os, ^{185,186,187,188,189,190,191,192,193,194,196}Ir, Pt, ^{188,189,190,191,192,193,194,195,196,197,198,200,202}Pt, ^{193,194,195,196,197,198,199,200}Au, Hg, ^{193,194,195,196,197,198,199,200,201,202,203,204}Hg, Tl, ^{199,200,201,202,203,204,205}Tl, ^{200,201,202,203,204,205,206,207,208,209,210,212}Pb, ^{203,204,205,206,207,208,209,210}Bi, ^{206,207,208,209,210}Po, ^210,211At, ^211,222Rn, ^{223,224,225,226,228}Ra, ^{225,226,227,228}Ac, ^{227,228,229,230,231,232,233,234}Th, ^{228,229,230,231,232,233,234}Pa, ^{230,232,232,233,234,235,236,237,238,239,240,241}U, ^{234,235,236,237,238,239}Np, ^{234,236,237,238,239,240,241,242,243,244,245,246,247}Pu, ^{239,240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,249,250}Bk, ^{246,248,249,250,251,252,253,254}Cf, ^{250,251,252,253,254,255,256}Es, ^{252,253,255,257}Fm(n, γ), E<20 MeV; calculated Maxwellian-averaged σ, astrophysical reaction rates, neutron thermal σ, Westcott factors, resonance integrals and their uncertainties using evaluated neutron libraries; deduced ENDF/B-VII.1, JEFF-3.1.2, JENDL-4.0, ROSFOND 2010, CENDL-3.1, EAF 2010 neutron-induced reaction σ deficiencies. Comparison with experimental data, KADONIS and Atlas of Neutron Resonances. BNL report, http://arxiv.org/abs/1208.2879, contains complete set of tables.

NUCLEAR REACTIONS ^1,2H, ³He, ^6,7Li, ⁹Be, ^10,11B, C, ^12,13,14C, ^14,15N, ^16,17,18O, ¹⁹F, ^20,21,22Ne, ^22,23,24Na, ^24,25,26,28Mg, ^26,27Al, ^{28,29,30,31,32}Si, ^31,32,33P, S, ^{32,33,34,35,36}S, Cl, ^35,36,37Cl, ^{36,37,38,39,40,41,42}Ar, K, ^{39,40,41,42,43}K, Ca, ^{40,41,42,43,44,45,46,47,48}Ca, ^{44,45,46,47,48}Sc, ^{44,45,46,47,48,49,50}Ti, V, ^48,49,50,51V, ^{48,50,51,52,53,54}Cr, ^52,53,54,55Mn, ^{52,54,55,56,57,58,59,60}Fe, ^{55,56,57,58,59,60}Co, ^{56,57,58,59,60,61,62,63,64,66}Ni, Cu, ^63,64,65,67Cu, Zn, ^{62,64,65,66,67,68,69,70,72}Zn, Ga, ^{66,67,69,71,72}Ga, Ge, ^{68,69,70,71,72,73,74,75,76,77,78}Ge, ^{71,72,73,74,75,76,77,79}As, ^{72,73,74,75,76,77,78,79,80,82}Se, ^{76,77,79,81,82}Br, ^{76,78,79,80,81,82,83,84,85,86}Kr, ^{82,83,84,85,86,87}Rb, ^{82,83,84,85,86,87,88,89,90,91}Sr, ^{86,87,88,89,90,91,93}Y, ^{86,88,89,90,91,92,93,94,95,96,97}Zr, ^{90,91,92,93,94,95,96}Nb, ^{92,93,94,95,96,97,98,99,100}Mo, ^{95,96,97,98,99}Tc, ^{96,97,98,99,100,101,102,103,104,105,106}Ru, ^{99,100,101,102,103,105}Rh, ^{100,101,102,103,104,105,106,107,108,109,110,112}Pd, Ag, ^{105,106,107,108,109,110,111}Ag, Cd, ^{106,107,108,109,110,111,112,113,114,115,116}Cd, ^{111,113,114,115}In, Sn, ^{112,113,114,115,116,117,118,119,120,122,123,124,125,126,127,128}Sn, ^{121,122,123,124,125,126,127,128}Sb, ^{118,119,120,121,122,123,124,125,126,127,128,129,130,131,132}Te, ^{123,124,125,126,127,128,129,130,131,133,135}I, ^{122,123,124,125,126,127,128,129,130,131,132,133,134,135,136}Xe, ^{127,129,131,133,134,135,136,137}Cs, ^{128,129,130,131,132,133,134,135,136,137,138,139,140}Ba, ^{138,139,140,141}La, ^{134,135,136,137,138,139,140,141,142,143,144}Ce, ^141,142,143Pr, ^{140,141,142,143,144,145,146,147,148,149,150}Nd, ^{143,144,145,146,147,148,149,150,151}Pm, ^{144,145,146,147,148,149,150,151,152,153,154,156}Sm, ^{145,146,147,148,149,150,151,152,153,154,155,156,157}Eu, ^{146,147,148,149,150,151,152,153,154,155,156,157,158,159,160}Gd, ^{151,152,153,154,155,156,157,158,159,160,161}Tb, ^{153,154,155,156,157,158,159,160,161,162,163,164,165,166}Dy, ^{163,164,165,166}Ho, ^{160,161,162,164,165,166,167,168,169,170,171,172}Er, ^{165,166,167,168,169,170,171,172,173}Tm, ^{166,168,169,170,171,172,173,174,175,175}Yb, ^{169,170,171,172,173,174,175,176,177}Lu, ^{170,171,172,173,174,175,176,177,178,179,180,181,182}Hf, ^{175,176,177,179,180,181,182,183,184}Ta, W, ^{178,180,181,182,183,184,185,186,187,188}W, ^{181,182,183,184,185,186,187,188,189}Re, Os, ^{182,183,184,185,186,187,188,189,190,191,192,193,194}Os, ^{185,186,187,188,189,190,191,192,193,194,196}Ir, Pt, ^{188,189,190,191,192,193,194,195,196,197,198,200,202}Pt, ^{193,194,195,196,197,198,199,200}Au, Hg, ^{193,194,195,196,197,198,199,200,201,202,203,204}Hg, Tl, ^{199,200,201,202,203,204,205}Tl, ^{200,201,202,203,204,205,206,207,208,209,210,212}Pb, ^{203,204,205,206,207,208,209,210}Bi, ^{206,207,208,209,210}Po, ^210,211At, ^211,222Rn, ^{223,224,225,226,228}Ra, ^{225,226,227,228}Ac, ^{227,228,229,230,231,232,233,234}Th, ^{228,229,230,231,232,233,234}Pa, ^{230,232,232,233,234,235,236,237,238,239,240,241}U, ^{234,235,236,237,238,239}Np, ^{234,236,237,238,239,240,241,242,243,244,245,246,247}Pu, ^{239,240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,249,250}Bk, ^{246,248,249,250,251,252,253,254}Cf, ^{250,251,252,253,254,255,256,257}Es, ^{252,253,255,257}Fm(n, n), E<20 MeV; calculated neutron thermal σ, Westcott factors, resonance integrals and their uncertainties using evaluated neutron libraries; deduced ENDF/B-VII.1, JEFF-3.1.2, JENDL-4.0, ROSFOND 2010, CENDL-3.1, EAF 2010 neutron-induced reaction σ deficiencies. Comparison with experimental data Atlas of Neutron Resonances. BNL report, http://arxiv.org/abs/1208.2879, contains complete set of tables.

doi: 10.1016/j.nds.2012.11.007
Citations: PlumX Metrics

2011CH46      J.Korean Phys.Soc. 59, 847s (2011)

Y.-S.Cho, P.Oblozinsky, S.F.Mughabghab, C.M.Mattoon, M.Herman

Practical Method for Estimating Neutron Cross Section Covariances in the Resonance Region

NUCLEAR REACTIONS ⁵⁵Mn(n, n), (n, γ), E=1-300000 eV; evaluated σ, uncertainties, covariances.

doi: 10.3938/jkps.59.847
Citations: PlumX Metrics

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, ^{40,42,43,44,46,48}Ca, ⁴⁵Sc, ^{46,47,48,49,50}Ti, ^50,51V, ^50,52,53,54Cr, ⁵⁵Mn, ^54,56,57,58Fe, ^58,59Co, ^{58,59,60,61,62,64}Ni, ^63,65Cu, ^{65,66,67,68,70}Zn, ^69,71Ga, ^{70,72,73,74,76}Ge, ^74,75As, ^{74,76,77,78,79,80,82}Se, ^79,81Br, ^{78,80,82,83,84,85,86}Kr, ^85,86,87Rb, ^{84,86,87,88,89,90}Sr, ^89,90,91Y, ^{90,91,92,93,94,95,96}Zr, ^93,94,95Nb, ^{92,94,95,96,97,98,99,100}Mo, ⁹⁹Tc, ^{96,98,99,100,101,102,103,104,105,106}Ru, ^103,105Rh, ^{102,104,105,106,107,108,110}Pd, ^{107,109,110,111}Ag, ^{106,108,110,111,112,113,114,115,116}Cd, ^113,115In, ^{112,113,114,115,116,117,118,119,120,122,123,124,125,126}Sn, ^{121,123,124,125,126}Sb, ^{120,122,123,124,125,126,127,128,129,130,132}Te, ^{127,129,130,131,135}I, ^{123,124,126,128,129,130,131,132,133,134,135,136}Xe, ^{133,134,135,136,137}Cs, ^{130,132,133,134,135,136,137,138,140}Ba, ^138,139,140La, ^{136,138,139,140,141,142,143,144}Ce, ^141,142,143Pr, ^{142,143,144,145,146,147,148,150}Nd, ^{147,148,149,151}Pm, ^{144,147,148,149,150,151,152,153,154}Sm, ^{151,152,153,154,155,156,157}Eu, ^{152,153,154,155,156,157,158,160}Gd, ^159,160Tb, ^{156,158,160,161,162,163,164}Dy, ^165,166Ho, ^{162,164,166,167,168,170}Er, ^168,169,170Tm, ^175,176Lu, ^{174,176,177,178,179,180}Hf, ^180,181,182Ta, ^{180,182,183,184,186}W, ^185,187Re, ^191,193Ir, ¹⁹⁷Au, ^{196,198,199,200,201,202,204}Hg, ^203,205Tl, ^{204,206,207,208}Pb, ²⁰⁹Bi, ^{223,224,225,226}Ra, ^225,226,227Ac, ^{227,228,229,230,231,232,233,234}Th, ^{229,230,231,232,233}Pa, ^{230,231,232,233,234,235,236,237,238,239,240,241}U, ^{234,235,236,237,238,239}Np, ^{236,237,238,239,240,241,242,243,244,246}Pu, ^{240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,249,250}Bk, ^{246,248,249,250,251,252,253,254}Cf, ^{251,252,253,254,255}Es, 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 ^{227,228,229,230,231,232,233,234}Th, ^{229,230,231,232,233}Pa, ^{230,231,232,233,234,235,236,237,238,239,240,241}U, ^{234,235,236,237,238,239}Np, ^{236,237,238,239,240,241,242,243,244,246}Pu, ^{240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,249,250}Bk, ^{246,248,249,250,251,252,253,254}Cf, ^{251,252,253,254,255}Es, 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.

2011HO19      Nucl.Data Sheets 112, 3075 (2011)

S.Hoblit, Y.-S.Cho, M.Herman, C.M.Mattoon, S.F.Mughabghab, P.Oblozinsky, M.T.Pigni, A.A.Sonzogni

Neutron Cross Section Covariances for Structural Materials and Fission Products

doi: 10.1016/j.nds.2011.11.006
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2011KA31      Nucl.Data Sheets 112, 2997 (2011)

A.C.Kahler, R.E.MacFarlane, R.D.Mosteller, B.C.Kiedrowski, S.C.Frankle, M.B.Chadwick, R.D.McKnight, R.M.Lell, G.Palmiotti, H.Hiruta, M.Herman, R.Arcilla, S.F.Mughabghab, J.C.Sublet, A.Trkov, T.H.Trumbull, M.Dunn

ENDF/B-VII.1 Neutron Cross Section Data Testing with Critical Assembly Benchmarks and Reactor Experiments

doi: 10.1016/j.nds.2011.11.003
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2011MU13      J.Korean Phys.Soc. 59, 821 (2011)

S.F.Mughabghab

What do s- and p-wave neutron average radiative widths reveal?

NUCLEAR REACTIONS ⁴⁰Ca, ⁵⁵Mn, ⁷⁴Se, ^90,91Zr, ^122,124Sn, ^151,153Eu, ^155,157Gd, ¹⁵⁹Tb, ^161,163Dy, ¹⁶⁷Er, ¹⁶⁹Tm, ¹⁷⁶Lu, ¹⁷⁹Hf, ¹⁸¹Ta, ^184,186W, ²⁰⁵Tl, ²³²Th, ^236,238U, ²³⁷Np, ^240,242Pu, ²⁴³Am(n, γ), E not given; analyzed resonance region data; deduced p-wave capture widths of neutron resonances, resonance-like structures, Pygmy Giant Resonance. Generalized Fermi liquid model.

doi: 10.3938/jkps.59.821
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2010PR07      At.Data Nucl.Data Tables 96, 645 (2010)

B.Pritychenko, S.F.Mughabghab, A.A.Sonzogni

Calculations of Maxwellian-averaged cross sections and astrophysical reaction rates using the ENDF/B-VII.0, JEFF-3.1, JENDL-3.3, and ENDF/B-VI.8 evaluated nuclear reaction data libraries

COMPILATION Z=1-100; A=1-255; compiled, analyzed Maxwellian averaged neutron capture σ, neutron-induced fission σ, astrophysical reaction rates.

NUCLEAR REACTIONS ^1,2H, ³He, ^6,7Li, 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, ^{40,42,43,44,46,48}Ca, ⁴⁵Sc, ^{46,47,48,49,50}Ti, V, ^50,52,53,54Cr, ⁵⁵Mn, ^54,56,57,58Fe, ^58,59Co, ^{58,59,60,61,62,64}Ni, ^63,65Cu, ^69,71Ga, ^{70,72,73,74,76}Ge, ^74,75As, ^{74,76,77,78,79,80,82}Se, ^79,81Br, ^{78,80,82,83,84,85,86}Kr, ^85,86,87Rb, ^{84,86,87,88,89,90}Sr, ^89,90,91Y, ^{90,91,92,93,94,95,96}Zr, ^93,94,95Nb, ^{92,94,95,96,97,98,99,100}Mo, ⁹⁹Tc, ^{96,98,99,100,101,102,103,104,105,106}Ru, ^103,105Rh, ^{102,104,105,106,107,108,110}Pd, ^{107,109,110,111}Ag, ^{106,108,110,111,112,113,114,115,116}Cd, ^113,115In, ^{112,113,114,115,116,117,118,119,120,122,123,124,125,126}Sn, ^{121,123,124,125,126}Sb, ^{120,122,123,124,125,126,127,128,129,130,132}Te, ^{127,129,130,131,135}I, ^{123,124,126,128,129,130,131,132,133,134,135,136}Xe, ^{133,134,135,136,137}Cs, ^{130,132,133,134,135,136,137,138,140}Ba, ^138,139,140La, ^{136,138,139,140,141,142,143,144}Ce, ^141,142,143Pr, ^{142,143,144,145,146,147,148,150}Nd, ^{147,148,149,151}Pm, ^{144,147,148,149,150,151,152,153,154}Sm, ^{151,152,153,154,155,156,157}Eu, ^{152,153,154,155,156,157,158,160}Gd, ^159,160Tb, ^{156,158,160,161,162,163,164}Dy, ^165,166Ho, ^{162,164,166,167,168,170}Er, ^175,176Lu, ^{174,176,177,178,179,180}Hf, ^181,182Ta, ^{182,183,184,186}W, ^185,187Re, ^191,193Ir, ¹⁹⁷Au, ^{196,198,199,200,201,202,204}Hg, ^{204,206,207,208}Pb, ²⁰⁹Bi, ^{223,224,225,226}Ra, ^225,226,227Ac, ^{227,228,229,230,232,233,234}Th, ^231,232,233Pa, ^{232,233,234,235,236,237,238,239,240,241}U, ^{235,236,237,238,239}Np, ^{236,237,238,239,240,241,242,243,244,246}Pu, ^{241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^247,249,250Bk, ^{249,250,251,252,253,254}Cf, ^253,254,255Es, ²⁵⁵Fm(n, γ), E=0.001-1 MeV; calculated Maxwellian-averaged σ and astrophysical reaction rates using evaluated neutron libraries; deduced ENDF/B-VII.0, JENDL-3.3, JEFF-3.1, ENDF/B-VI.8 neutron-induced reaction σ deficiencies. Comparison with experimental data and KADONIS.

NUCLEAR REACTIONS ^223,226Ra, ²²⁷Ac, ^{227,228,229,230,232,233,234}Th, ^231,232,233Pa, ^{232,233,234,235,236,237,238,239,240,241}U, ^{235,236,237,238,239}Np, ^{236,237,238,239,240,241,242,243,244,246}Pu, ^{241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^247,249,250Bk, ^{249,250,251,252,253,254}Cf, ^254,255Es, ²⁵⁵Fm(n, F), E=0.001-1 MeV; calculated Maxwellian-averaged σ and astrophysical reaction rates using evaluated neutron libraries.

doi: 10.1016/j.adt.2010.05.002
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2008HE14      Nucl.Data Sheets 109, 2752 (2008)

M.Herman, M.T.Pigni, P.Oblozinsky, S.F.Mughabghab, C.M.Mattoon, R.Capote, Y.-S.Cho, A.Trkov

Development of Covariance Capabilities in EMPIRE Code

NUCLEAR REACTIONS ⁸⁹Y(n, 2n), E < 35 MeV; ⁹³Nb(n, X), E < 15 MeV; analyzed cross sections.

doi: 10.1016/j.nds.2008.11.005
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2008KI12      Nucl.Sci.Eng. 160, 168 (2008)

H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, D.Rochman, Y.-O.Lee

Evaluation of Neutron Cross Sections for a Complete Set of Nd Isotopes

NUCLEAR REACTIONS ^{142,143,144,145,146,147,148,150}Nd(n, X), E < 20 MeV; analyzed cross sections.

doi: 10.13182/NSE160-168
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2008KI15      Nucl.Instrum.Methods Phys.Res. B266, 3513 (2008)

H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, Y.-O.Lee

Evaluation of neutron cross sections for a complete set of Dy isotopes

NUCLEAR REACTIONS ^{156,158,160,161,162,163,164}Dy(n, X), E= 10^- eV - 20 MeV; analyzed neutron σ; comparison with experimental data and ENDF/B-VI.8, JEFF-3.1 data libraries; EMPIRE-2.19.

doi: 10.1016/j.nimb.2008.05.020
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2008NO08      Nucl.Sci.Eng. 160, 108 (2008)

G.Noguere, D.Bernard, C.De Saint Jean, B.Iooss, F.Gunsing, K.Kobayashi, S.F.Mughabghab, P.Siegler

Assessment and Propagation of the ²³⁷Np Nuclear Data Uncertainties in Integral Calculations by Monte Carlo Techniques

NUCLEAR REACTIONS ²³⁷Np(n, γ), (n, X), E<10 eV; analyzed available data; deduced level energies, J, π, resonance parameters, thermal neutron σ, resonance integrals.

doi: 10.13182/NSE160-108
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2008RO01      Nucl.Sci.Eng. 158, 68 (2008)

D.Rochman, M.Herman, S.F.Mughabghab, P.Oblozinsky

New Evaluation of the ⁹⁹Tc Neutron-Induced Cross Sections for the ENDF/B-VII.0 Library

NUCLEAR REACTIONS ⁹⁹Tc(n, γ), E=0-11 MeV; ⁹⁹Tc(n, n'), (n, 2n), E=0-20 MeV; ⁹⁹Tc(n, p), E=4-20 MeV; ⁹⁹Tc(n, α), E=5-20 MeV; ⁹⁹Tc(n, X), E=2-20 MeV; analyzed total and elastic cross sections, capture cross sections, resonance integrals, inelastic cross sections.

doi: 10.13182/NSE08-A2739
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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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2005TR08      Nucl.Sci.Eng. 150, 336 (2005)

A.Trkov, G.L.Molnar, Zs.Revay, S.F.Mughabghab, R.B.Firestone, V.G.Pronyaev, A.L.Nichols, M.C.Moxon

Revisiting the 238U Thermal Capture Cross Section and Gamma-Ray Emission Probabilities from ²³⁹Np Decay

NUCLEAR REACTIONS ²³⁸U(n, γ), E=thermal; analyzed data; deduced thermal capture σ.

RADIOACTIVITY ²³⁹Np(β^-); analyzed data; deduced γ-ray emission probabilities.

doi: 10.13182/NSE05-A2520
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2002MU07      Phys.Rev. C65, 044620 (2002)

S.F.Mughabghab, A.A.Sonzogni

Damping Width of Giant Dipole Resonances of Cold and Hot Nuclei: A macroscopic model

NUCLEAR STRUCTURE ⁴⁵Sc, ^109,118Sn, ¹⁴⁷Eu, ¹⁹⁴Hg; calculated GDR widths, quadrupole deformation vs temperature. Phenomenological macroscopic model, comparisons with data.

doi: 10.1103/PhysRevC.65.044620
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2000MU16      Phys.Lett. 487B, 155 (2000)

S.F.Mughabghab, C.L.Dunford

A Dipole-Quadrupole Interaction Term in E1 Photon Transitions

NUCLEAR STRUCTURE ⁶⁰Co, ⁸⁰Br, ^144,146Nd, ^148,150Sm, ^156,158Gd, ¹⁶⁶Ho, ¹⁶⁴Dy, ¹⁶⁸Er, ^172,174Yb, ¹⁷⁶Lu, ¹⁸⁰Hf, ¹⁸²Ta, ¹⁸⁸Os, ¹⁹²Ir, ¹⁹⁶Pt, ¹⁹⁸Au; analyzed γ spectra from average resonance capture, E1 transitions strengths; deduced role of dipole-quadrupole term, deformation effects, GDR temperature dependence. Generalized Fermi liquid model.

doi: 10.1016/S0370-2693(00)00792-9
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2000MU18      Trans.Bulg.Nucl.Soc. 5, 99 (2000)

S.F.Mughabghab, C.Dunford

On the Questions of the Nuclear Level Density and the E1 Photon Strength Functions

NUCLEAR STRUCTURE A=30-250; analyzed neutron resonance data; deduced level density parameters, pairing and shell effects. ¹⁴⁶Nd, ¹⁹⁸Au, ¹⁷²Yb, ¹⁸²Ta; calculated E1 strength functions. ^144,146Nd, ^148,150Sm, ^156,158Gd, ¹⁶⁴Dy, ^172,174Yb, ¹⁹²Ir, ¹⁹⁶Pt, ¹⁹⁸Au, ^234,236U, ^240,242Pu; calculated total radiative widths. Comparisons with data.

1998MU22      Phys.Rev.Lett. 81, 4083 (1998)

S.F.Mughabghab, C.Dunford

Nuclear Level Density and the Effective Nucleon Mass

NUCLEAR STRUCTURE A=30-240; analyzed neutron resonance data; deduced spin dispersion parameters, level density parameters, pairing and shell effects, enhanced nucleon effective mass at Fermi surface.

doi: 10.1103/PhysRevLett.81.4083
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1998ZU03      Nucl.Sci.Eng. 129, 180 (1998)

M.S.Zucker, N.Tsoupas, P.E.Vanier, U.von Wimmersperg, S.F.Mughabghab, E.Schmidt

Spallation Neutron Production Measurements

NUCLEAR REACTIONS Pb, W(p, nX), E=0.8, 1.0, 1.2, 1.4 GeV; measured thick target neutron yields. Comparison with high-energy transport code predictions.

doi: 10.13182/NSE129-180
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0554.

1988MU05      J.Phys.(London) G14, Supplement S231 (1988)

S.F.Mughabghab

Spin-Spin and Isospin Interactions from Capture Measurements

NUCLEAR REACTIONS ⁹Be(n, γ), E not given; analyzed σ; deduced spin-spin potential parameter.

doi: 10.1088/0305-4616/14/S/025
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1986MU05      Radiat.Eff. 94, 297 (1986)

S.F.Mughabghab

Spin Dependence of the Coherent Scattering Lengths of ²⁷Al and Admixture of S- and D- Partial Waves

NUCLEAR REACTIONS ²⁷Al(polarized n, γ), E=thermal; analyzed σ(E); deduced spin-dependent interactions role. ²⁸Al deduced s-wave resonances.

doi: 10.1080/00337578608208396
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1985MA33      Phys.Rev. C32, 379 (1985)

R.L.Macklin, S.F.Mughabghab

Neutron Capture by ³¹P

NUCLEAR REACTIONS ³¹P(n, γ), E=2.6-500 keV; measured σ(E); deduced stellar reaction σ. ³²P levels deduced (gΓnΓγ)/Γ, Γ. Direct reaction mechanism.

doi: 10.1103/PhysRevC.32.379
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12942.

1985MU03      Phys.Rev.Lett. 54, 986 (1985)

S.F.Mughabghab

Evidence for a Nucleon-Nucleus Spin-Spin Interaction in ⁹Be

NUCLEAR REACTIONS ⁹Be(n, γ), E=thermal; analyzed E1 transitions following capture; deduced spin-spin potential parameters. ¹⁰Be levels deduced spectroscopic amplitudes, phases. Direct capture model.

doi: 10.1103/PhysRevLett.54.986
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1983HA12      Phys.Rev. C28, 24 (1983)

J.A.Harvey, W.M.Good, R.F.Carlton, B.Castel, J.B.McGrory, S.F.Mughabghab

Neutron Spectroscopy as a High-Resolution Probe: Identification of the missing (1/2)⁺ states in ³¹Si

NUCLEAR STRUCTURE ³¹Si; calculated levels, spectroscopic strengths. Shell model.

NUCLEAR REACTIONS ³⁰Si(n, X), E=0.2-1400 keV; measured transmission, σ(E). ³¹Si deduced resonances, J, π, Γn, level densities, s-, p-, d-wave strength functions.

doi: 10.1103/PhysRevC.28.24
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1982MU14      Phys.Rev. C26, 2698 (1982)

S.F.Mughabghab, M.A.Lone, B.C.Robertson

Quantitative Test of the Lane-Lynn Theory of Direct Radiative Capture of Thermal Neutrons by ¹²C and ¹³C

NUCLEAR REACTIONS ^12,13C(n, γ), E=thermal; measured σ(Eγ), Iγ; deduced capture mechanism. ^12,13C levels deduced S.

doi: 10.1103/PhysRevC.26.2698
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1980CA02      Phys.Rev. C21, 65 (1980)

R.F.Casten, G.J.Smith, M.R.Macphail, D.Breitig, W.R.Kane, M.L.Stelts, S.F.Mughabghab, J.A.Cizewski, H.G.Borner, W.F.Davidson, K.Schreckenbach

¹⁰⁹Pd: Difficulties in Particle-Rotor Models for Unique-Parity States And Revision of Spectroscopic Factors

NUCLEAR REACTIONS ¹⁰⁸Pd(n, γ), E=thermal, 2.96 eV, 2 keV, 24 keV; measured Eγ, Iγ, Iγ(θ), I(ce). ¹⁰⁹Pd levels deduced J, π, multipolarities, S, ICC. Critical review of particle rotor model.

doi: 10.1103/PhysRevC.21.65
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1979MU02      Phys.Lett. 81B, 93 (1979)

S.F.Mughabghab

Verifications of the Lane-Lynn Theory of Direct Neutron Capture

NUCLEAR REACTIONS ¹³⁶Xe, ¹⁴⁴Sm(n, γ), E=thermal; calculated capture σ, coherent scattering lengths, neutron S. Lane-Lynn theory of direct capture. ¹³⁷Xe, ¹⁴⁵Sm levels deduced J.

doi: 10.1016/0370-2693(79)90496-9
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1973CA22      Phys.Rev. C8, 1035 (1973)

R.F.Casten, D.Breitig, W.R.Kane, S.F.Mughabghab

K = 0 Rotational Bands in ¹⁷⁴Yb

NUCLEAR REACTIONS ¹⁷³Yb(n, γ), E=4.53, 17.7 eV; measured Eγ, γγ-coin, Iγ. ¹⁷⁴Yb deduced levels, J, π, B(E2), K, γ-branching, band mixing.

doi: 10.1103/PhysRevC.8.1035
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1973MU01      Priv.Comm. (February 1973)

S.F.Mughabghab

1973MU02      Priv.Comm. (February 1973)

S.F.Mughabghab

1973MU14      BNL-325(ED.3)(VOL.1) (1973); Priv. Comm.

S.F.Mughabghab, D.I.Garber

Neutron Cross Sections, Volume 1, Resonance Parameters

COMPILATION A=1-254; compiled neutron σ, resonance parameters.

1972MU01      Priv.Comm. (January 1972)

S.F.Mughabghab

1972MU05      Priv.Comm. (April 1972)

S.F.Mughabghab

1971MU07      Phys.Rev.Lett. 26, 1118 (1971)

S.F.Mughabghab, R.E.Chrien, O.A.Wasson, G.W.Cole, M.R.Bhat

Reaction Mechanism for p-Wave Neutron Capture in Mo⁹² and Mo⁹⁸

NUCLEAR REACTIONS ^92,98Mo(n, γ), E=resonance; measured Eγ, Iγ; deduced reaction mechanism. ^93,99Mo deduced resonances, level-width, J, π.

doi: 10.1103/PhysRevLett.26.1118
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1971MU25      Priv.Comm. (December 1971)

S.F.Mughabghab

1970MU08      Phys.Rev. C1, 1850 (1970)

S.F.Mughabghab, R.E.Chrien

Study of Radiation Widths and Neutron Strength Functions of Dy Isotopes

NUCLEAR REACTIONS ^{161,162,163,164}Dy(n, X), E=1 eV-15 keV; measured transmission; deduced potential scattering radii. ^{162,163,164,165}Dy deduced resonances, level-width, binding energy, strength functions.

doi: 10.1103/PhysRevC.1.1850
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1970MU19      Phys.Rev.Lett. 25, 1670 (1970)

S.F.Mughabghab, R.E.Chrien, O.A.Wasson

Evidence for Nonstatistical Effects in the Reaction Dy¹⁶³(n, γ)Dy¹⁶⁴

NUCLEAR REACTIONS ¹⁶³Dy(n, γ), E=resonance; measured Eγ, Iγ; deduced nonstatistical effects. ¹⁶⁴Dy deduced resonance structure.

doi: 10.1103/PhysRevLett.25.1670
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1969MU04      Phys.Rev. 180, 1131 (1969)

S.F.Mughabghab, R.E.Chrien

S-Wave Neutron Strength Functions of the Gd Isotopes

NUCLEAR REACTIONS ^{155,156,157,158,160}Gd(n, X), E=0.015-18 eV; measured σ, transmission. ^{156,157,158,159,161}Gd deduced resonance parameters, strength functions, potential scattering radii.

doi: 10.1103/PhysRev.180.1131
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1968MU05      Phys.Rev. 174, 1400 (1968)

S.F.Mughabghab, R.E.Chrien

Neutron Cross Sections and Resonance Parameters of Yb Isotopes

NUCLEAR STRUCTURE ¹⁷³Yb, ¹⁷²Yb, ¹⁷⁵Yb, ¹⁷⁴Yb, ¹⁷¹Yb, ¹⁷⁷Yb, ¹⁶⁹Yb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.174.1400
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1967MU17      Phys.Rev. 162, 1130 (1967)

S.F.Mughabghab, R.E.Chrien, M.R.Bhat

Neutron Resonance Parameters of the Erbium Isotopes

NUCLEAR REACTIONS ^{162,164,166,167,168}Er(n, X), E=0-1.5 keV; measured σ(nt)(E). ^{163,165,167,168,169}Er deduced res param, strength functions, level densities. ^162,164,167Er(n, X), E=thermal; measured σ(nt). ¹⁶⁸Er deduced paramagnetic scattering σ.

doi: 10.1103/PhysRev.162.1130
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1966CH26      Proc.Intern.Conf.Study of Nucl.Struct.with Neutrons, Antwerp, Belgium (1965), M.N.de Mevergnies, P.Van Assche, J.Vervier, Eds., North-Holland Publishing Co., Amsterdam, p.524 (1966); EANDC-50-S, Paper 69

R.E.Chrien, S.F.Mughabghab

Search for J-Dependent Neutron Strength Functions in the Rare Earth Region

1966GO29      BNL-325, 2nd Ed., Suppl.No.2, Vol.IIB (1966)

M.D.Goldberg, S.F.Mughabghab, S.N.Purohit, B.A.Magurno, V.M.May

Neutron Cross Sections, Z = 41 to 60

1966GO30      BNL-325, 2nd Ed., Suppl.No.2, Vol.IIA (1966)

M.D.Goldberg, S.F.Mughabghab, B.A.Magurno, V.M.May

Neutron Cross Sections, Z = 21 to 40

1966GO31      BNL-325, 2nd Ed., Suppl.No.2, Vol.IIC (1966)

M.D.Goldberg, S.F.Mughabghab, S.N.Purohit, B.A.Magurno, V.M.May

Neutron Cross Sections, Z = 61 to 87

1966MU05      Bull.Am.Phys.Soc. 11, No.3, 334, DB2 (1966)

S.F.Mughabghab, R.E.Chrien, M.R.Bhat

Neutron-Resonance Structure in Er¹⁶²

NUCLEAR STRUCTURE ¹⁶²Er; measured not abstracted; deduced nuclear properties.

1965CH25      WASH-1064, p.18 (1965); and Priv.Comm. (1966)

R.E.Chrien, M.R.Bhat, S.F.Mughabghab, H.Palevsky

Fast Chopper

1965MU06      Bull.Am.Phys.Soc. 10, No.4, 513, HB6 (1965)

S.F.Mughabghab, R.E.Chrien

Neutron Strength Functions of the Ytterbium Isotopes

NUCLEAR STRUCTURE ¹⁷⁴Yb; measured not abstracted; deduced nuclear properties.

1964MU12      Phys.Rev. 133, B660 (1964)

S.F.Mughabghab, W.E.Stephens

Energy and angular distributions of photoneutrons from Oxygen-18

NUCLEAR REACTIONS ¹⁸O(γ, n), E=9.7-20 MeV; measured products, ¹⁷O, Eν, Iν; deduced σ(θ, E). Data were imported from EXFOR entry M0322.

doi: 10.1103/PhysRev.133.B660
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