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2018BR05      Nucl.Data Sheets 148, 1 (2018)

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

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

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

NUCLEAR REACTIONS ^1,2H, ³He, ^6,7Li, ⁹Be, ^10,11B, ^12,13C, ^14,15N, ^16,17,18O, ¹⁹F, ^20,21,22Ne, ^22,23Na, ^24,25,26Mg, ^26,27Al, ^{28,29,30,31,32}Si, ³¹P, ^{32,33,34,35,36}S, ^35,36,37Cl, ^{36,37,38,39,40,41}Ar, ^39,40,41K, ^{40,41,42,43,44,45,46,47,48}Ca, ⁴⁵Sc, ^{46,47,48,49,50}Ti, ^49,50,51V, ^{50,51,52,53,54}Cr, ^54,55Mn, ^{54,55,56,57,58}Fe, ^58,59Co, ^{58,59,60,61,62,63,64}Ni, ^63,64,65Cu, ^{64,65,66,67,68,69,70}Zn, ^69,70,71Ga, ^{70,71,72,73,74,75,76}Ge, ^73,74,75As, ^{74,75,76,77,78,79,80,81,82}Se, ^79,80,81Br, ^{78,79,80,81,82,83,84,85,86}Kr, ^85,86,87Rb, ^{84,85,86,87,88,89,90}Sr, ^89,90,91Y, ^{90,91,92,93,94,95,96}Zr, ^93,94,95Nb, ^{92,93,94,95,96,97,98,99,100}Mo, ^98,99Tc, ^{96,97,98,99,100,101,102,103,104,105,106}Ru, ^103,104,105Rh, ^{102,103,104,105,106,107,108,109,110}Pd, ^{107,108,109,110,111,112,113,114,115,116,117,118}Ag, ^{106,107,108,109,110,111,112,113,114,115,116}Cd, ^113,114,115In, ^{112,113,114,115,116,117,118,119,120,121,122,123,124,125,126}Sn, ^{121,122,123,124,125,126}Sb, ^{120,121,122,123,124,125,126,127,128,129,130,121,132}Te, ^{127,128,129,130,131,132,133,134,135}I, ^{123,124,125,126,127,128,129,130,131,132,133,134,135,136}Xe, ^{133,134,135,136,137}Cs, ^{130,131,132,133,134,135,136,137,138,139,140}Ba, ^138,139,140La, ^{136,137,138,139,140,141,142,143,144}Ce, ^141,142,143Pr, ^{142,143,144,145,146,147,148,149,150}Nd, ^{143,144,145,146,147,148,149,151}Pm, ^{144,145,146,147,148,149,150,151,152,153,154}Sm, ^{151,152,153,154,155,156,157}Eu, ^{152,153,154,155,156,157,158,159,160}Gd, ^{158,159,160,161}Tb, ^{154,155,156,157,158,159,160,161,162,163,164}Dy, ^165,166Ho, ^{162,163,164,165,166,167,168,170,170}Er, ^{168,169,170,171}Tm, ^{168,169,170,171,172,173,174,175,176}Yb, ^175,176Lu, ^{174,175,176,177,178,179,180,181,182}Hf, ^180,181,182Ta, ^{180,181,182,183,184,185,186}W, ^185,186,187Re, ^{184,185,186,187,188,189,190,191,192}Os, ^191,192,193Ir, ^{190,191,192,193,194,195,196,197,198}Pt, ¹⁹⁷Au, ^{196,197,198,199,200,201,202,203,204}Hg, ^203,204,205Tl, ^{204,205,206,207,208,209,210}Pb, ^209,210Bi, ^208,209,210Po, ^{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, ^{236,237,238,239,240,241,242,243,244,245,246}Pu, ^{240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,248,249,250}Bk, ^{246,247,248,249,250,251,252,253,254}Cf, ^{251,252,253,254,255}Es, ²⁵⁵Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VIII.0 evaluated neutron library. Comparison with ENDF/B-VII.1 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, ^{236,237,238,239,240,241,242,243,244,245,246}Pu, ^{240,241,242,243,244}Am, ^{240,241,242,243,244,245,246,247,248,249,250}Cm, ^{245,246,247,248,249,250}Bk, ^{246,247,248,249,250,251,252,253,254}Cf, ^{251,252,253,254,255}Es, ²⁵⁵Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.1, JENDL-4.0u+ and Atlas of Neutron Resonances values.

doi: 10.1016/j.nds.2018.02.001
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2015MA02      Nucl.Data Sheets 123, 36 (2015)

C.M.Mattoon

Covariances in the Generalized Nuclear Data (GND) Structure

doi: 10.1016/j.nds.2014.12.007
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2015MA69      Eur.Phys.J. A 51, 183 (2015)

C.M.Mattoon, B.R.Beck

Designing a new structure for storing nuclear data - Progress of the Working Party for Evaluation Cooperation subgroup #38

doi: 10.1140/epja/i2015-15183-y
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2014PA35      Nucl.Data Sheets 120, 288 (2014)

N.R.Patel, C.M.Mattoon, B.R.Beck, N.C.Summers, D.A.Brown

Structure for Storing Properties of Particles (PoP)

doi: 10.1016/j.nds.2014.07.069
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2014PA47      Nucl.Data Sheets 118, 596 (2014)

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

Combined Use of Integral Experiments and Covariance Data

doi: 10.1016/j.nds.2014.04.145
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2013CZ01      Phys.Rev. C 87, 034613 (2013)

A.Czeszumska, C.T.Angell, J.T.Burke, N.D.Scielzo, E.B.Norman, R.A.E.Austin, G.Boutoux, R.J.Casperson, P.Chodash, R.O.Hughes, C.M.Mattoon, V.Meot, J.Munson, L.Phair, J.J.Ressler, O.Roig, T.J.Ross, E.Swanberg, B.Wang

Determining the ²³⁹Np(n, f) cross section using the surrogate ratio method

NUCLEAR REACTIONS ^236,238U(³He, pF), E=29 MeV; measured proton, deuteron, triton, ^3,4He spectra, fission events, fission anisotropies, particle-fission time-to-amplitude spectrum, (fission)p-coin using STARS array at LBNL cyclotron facility. ²³⁹Np(n, F), E=0.5-20 MeV; deduced cross section by surrogate ratio method. Comparison with ENDF/B-VII.0, JENDL-4.0, and CENDL-3.1 evaluated libraries. Impact on estimate of ²⁴⁰Pu produced during fuel burnup in calculations using reactor codes.

doi: 10.1103/PhysRevC.87.034613
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14360.

2012MA54      Nucl.Data Sheets 113, 3145 (2012)

C.M.Mattoon, B.R.Beck, N.R.Patel, N.C.Summers, G.W.Hedstrom, D.A.Brown

Generalized Nuclear Data: A New Structure (with Supporting Infrastructure) for Handling Nuclear Data

doi: 10.1016/j.nds.2012.11.008
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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
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2011CH57      Nucl.Data Sheets 112, 2887 (2011)

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

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

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

NUCLEAR REACTIONS ^1,2H, ³He, ^6,7Li, ^7,9Be, ^10,11B, C, ^14,15N, ^16,17O, ¹⁹F, ^22,23Na, ^24,25,26Mg, ²⁷Al, ^28,29,30Si, ³¹P, ^32,33,34,36S, ^35,37Cl, ^36,38,40Ar, ^39,40,41K, ^{40,42,43,44,46,48}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
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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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2011MA62      J.Korean Phys.Soc. 59, 1242s (2011)

C.M.Mattoon, P.Oblozinsky

Issues in Neutron Cross Section Covariances

COMPILATION ⁵⁶Fe(n, γ), (n, n), E=1 keV-20 MeV; evaluated σ uncertainties. ⁵⁵Mn(n, n), E=1 eV-1 MeV;⁵⁶Fe(n, n), E=1 eV-0.3 MeV; evaluated scattering radius uncertainty. ⁵⁸Ni(n, γ), E not given; evaluated σ uncertainties with resonances up to about 1 MeV. ⁶Li(n, ³H), E=1 keV-2.5 MeV; ²³³U(n, n), E=0.01-20 MeV; evaluated σ, σ uncertainties.

doi: 10.3938/jkps.59.1242
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2009MA54      Phys.Rev. C 80, 034318 (2009)

C.M.Mattoon, F.Sarazin, C.Andreoiu, A.N.Andreyev, R.A.E.Austin, G.C.Ball, R.S.Chakrawarthy, D.Cross, E.S.Cunningham, J.Daoud, P.E.Garrett, G.F.Grinyer, G.Hackman, D.Melconian, C.Morton, C.Pearson, J.J.Ressler, J.Schwarzenberg, M.B.Smith, C.E.Svensson

Line-shape analysis of Doppler-broadened γ lines following the β decay of ¹¹Li

RADIOACTIVITY ¹¹Li(β^-), (β^-n) [from Ta(p, X), E=500 MeV]; measured Eγ, Iγ, γγ-, βγ-coin, half-lives by line-shape method using 8pi array. ^10,11Be; deduced levels, J, π, branching ratios, B(E1), delayed neutron emission probabilities.

doi: 10.1103/PhysRevC.80.034318
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Data from this article have been entered in the XUNDL database. For more information, click here.

2008FI07      Phys.Rev. C 78, 025502 (2008)

P.Finlay, G.C.Ball, J.R.Leslie, C.E.Svensson, I.S.Towner, R.A.E.Austin, D.Bandyopadhyay, A.Chaffey, R.S.Chakrawarthy, P.E.Garrett, G.F.Grinyer, G.Hackman, B.Hyland, R.Kanungo, K.G.Leach, C.M.Mattoon, A.C.Morton, C.J.Pearson, A.A.Phillips, J.J.Ressler, F.Sarazin, H.Savajols, M.A.Schumaker, J.Wong

High-precision branching ratio measurement for the superallowed β⁺ emitter ⁶²Ga

RADIOACTIVITY ⁶²Ga(β⁺); measured Eγ, Iγ, Eβ, βγ-coin, branching ratios; deduced ft values. ⁶²Zn; deduced levels, J, π. ¹⁰C, ¹⁴O, ²²Mg, ^26mAl, ³⁴Cl, ³⁴Ar, ^38mK, ⁴²Sc, ⁴⁶V, ⁵⁰Mn, ⁵⁴Co, ⁶²Ga, ⁷⁴Rb; systematics of superallowed β decays and ft values.

doi: 10.1103/PhysRevC.78.025502
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Data from this article have been entered in the XUNDL database. For more information, click here.

2008GR03      Phys.Rev. C 77, 015501 (2008)

G.F.Grinyer, P.Finlay, C.E.Svensson, G.C.Ball, J.R.Leslie, R.A.E.Austin, D.Bandyopadhyay, A.Chaffey, R.S.Chakrawarthy, P.E.Garrett, G.Hackman, B.Hyland, R.Kanungo, K.G.Leach, C.M.Mattoon, A.C.Morton, C.J.Pearson, A.A.Phillips, J.J.Ressler, F.Sarazin, H.Savajols, M.A.Schumaker, J.Wong

High-precision half-life determination for the superallowed β⁺ emitter ⁶²Ga

RADIOACTIVITY ⁶²Ga(β⁺) [from Zr(p, γ), E=500 MeV]; measured Eγ, β⁺ particles; deduced half-life.

doi: 10.1103/PhysRevC.77.015501
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Data from this article have been entered in the XUNDL database. For more information, click here.

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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2007MA04      Phys.Rev. C 75, 017302 (2007)

C.M.Mattoon, F.Sarazin, G.Hackman, E.S.Cunningham, R.A.E.Austin, G.C.Ball, R.S.Chakrawarthy, P.Finlay, P.E.Garrett, G.F.Grinyer, B.Hyland, K.A.Koopmans, J.R.Leslie, A.A.Phillips, M.A.Schumaker, H.C.Scraggs, J.Schwarzenberg, M.B.Smith, C.E.Svensson, J.C.Waddington, P.M.Walker, B.Washbrook, E.Zganjar

β decay of ³²Na

RADIOACTIVITY ³²Na(β^-), (β^-n), (β^-2n) [from Ta(p, X)]; measured Eγ, Iγ, γγ-, βγ-coin. ³²Mg deduced levels, J, π. ^30,31Mg deduced transitions.

doi: 10.1103/PhysRevC.75.017302
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