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Search: Author = N.M.Larson

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

2009CA28      Nucl.Data Sheets 110, 3215 (2009)

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

International Evaluation of Neutron Cross Section Standards

doi: 10.1016/j.nds.2009.11.001
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2009DE04      Nucl.Sci.Eng. 161, 131 (2009)

H.Derrien, A.Courcelle, L.C.Leal, N.M.Larson

R-Matrix Analysis of ²³⁸U High-Resolution Neutron Transmissions and Capture Cross Sections in the Energy Range 0 to 20 keV

NUCLEAR REACTIONS ²³⁸U(n, γ), E=0-20 keV; analyzed capture cross sections;deduced resonance parameters. R-matrix analysis.

doi: 10.13182/NSE161-131
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2008DE20      Nucl.Sci.Eng. 160, 149 (2008)

H.Derrien, L.C.Leal, N.M.Larson

R-Matrix Analysis of ²³²Th Neutron Transmissions and Capture Cross Sections in the Energy Range Thermal to 4 keV

NUCLEAR REACTIONS ²³²Th(n, γ), (n, X), E < 4 keV; analyzed cross sections using the SAMMY R-matrix analysis code.

doi: 10.13182/NSE160-149
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2007CO16      Nucl.Sci.Eng. 156, 391 (2007)

A.Courcelle, H.Derrien, L.C.Leal, N.M.Larson

Evaluation of the ²³⁸U Neutron Cross Section in the Unresolved Resonance Range

NUCLEAR REACTIONS ²³⁸U(n, X), E=20-150 keV; analyzed cross sections in the unresolved resonance range. Deduced average resonance parameters. Compared results to existing evaluations.

doi: 10.13182/NSE07-A2706
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2006SA17      Phys.Rev. C 73, 044603 (2006)

R.O.Sayer, K.H.Guber, L.C.Leal, N.M.Larson, T.Rauscher

R-matrix analysis of Cl neutron cross sections up to 1.2 MeV

NUCLEAR REACTIONS Cl, ^35,37Cl(n, X), E=0.02-1250 keV; analyzed σ. ^35,37Cl deduced resonance energies, widths, neutron strength functions. Multilevel Reich-Moore R-matrix formalism, comparison with previous results.

doi: 10.1103/PhysRevC.73.044603
Citations: PlumX Metrics

1999LE69      Nucl.Sci.Eng. 131, 230 (1999)

L.C.Leal, H.Derrien, N.M.Larson, R.Q.Wright

R-Matrix Analysis of ²³⁵U Neutron Transmission and Cross-Section Measurements in the 0- to 2.25-keV Energy Range

NUCLEAR REACTIONS ²³⁵U(n, X), E=0-2250 eV; analyzed fission, capture, transmission σ; deduced resonance parameters. R-matrix analysis.

doi: 10.13182/NSE99-A2031
Citations: PlumX Metrics

1997BO46      Nucl.Sci.Eng. 127, 105 (1997)

O.Bouland, H.Derrien, N.M.Larson, L.C.Leal

R-Matrix Analysis of the ²⁴⁰Pu Neutron Cross Sections in the Thermal to 5700-eV Energy Range

NUCLEAR REACTIONS ²⁴⁰Pu(n, X), E=0.02-5700 eV; analyzed transmission, fission, total σ; deduced parameters. R-matrix analysis.

doi: 10.13182/NSE127-105
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1993PE03      Phys.Rev. C47, 1143 (1993)

C.M.Perey, F.G.Perey, J.A.Harvey, N.W.Hill, N.M.Larson, R.L.Macklin, D.C.Larson

⁵⁸Ni + n Transmission, Differential Elastic Scattering, and Capture Measurements and Analysis up to 813 keV

NUCLEAR REACTIONS ⁵⁸Ni(n, X), E ≤ 20 MeV; measured transmission. ⁵⁸Ni(n, n), E=0.01-5 MeV; measured σ(θ). ⁵⁸Ni(n, γ), E=0.0026-2.5 MeV; measured capture σ(E). ⁵⁹Ni deduced resonances, Γn, (gΓnΓγ/Γ), J, π.

doi: 10.1103/PhysRevC.47.1143
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12972.

1992DE15      Ann.Nucl.Energy 19, 393 (1992)

G.de Saussure, N.M.Larson, J.A.Harvey, N.W.Hill

Multilevel Resonance Analysis of ⁵⁹Co Neutron Transmission Measurements

NUCLEAR REACTIONS ⁵⁹Co(n, X), E=0.002-100 keV; analyzed transmission data; deduced total, thermal capture σ. ⁶⁰Co deduced resonance parameters. Multi-level analysis.

doi: 10.1016/0306-4549(92)90033-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12988.

1989DE37      Nucl.Sci.Eng. 103, 109 (1989)

G.de Saussure, L.C.Leal, R.B.Perez, N.M.Larson, M.S.Moore

A New Resonance Region Evaluation of Neutron Cross Sections for ²³⁵U

NUCLEAR REACTIONS ²³⁵U(n, F), (n, γ), E ≤ 110 eV; calculated fission, capture σ(E).

1989MO21      Nucl.Phys. A502, 443c (1989)

M.S.Moore, L.C.Leal, G.de Saussure, R.B.Perez, N.M.Larson

Resonance Structure in the Fission of (²³⁵U + n)

NUCLEAR REACTIONS ²³⁵U(n, F), (n, γ), (n, n), E=low, resonance; analyzed data. R-matrix, Pattenden-Postma constraints.

doi: 10.1016/0375-9474(89)90681-7
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1987CO23      Nucl.Phys. A469, 480 (1987)

G.P.Coddens, M.Salah, J.A.Harvey, N.W.Hill, N.M.Larson

Resonance Structure of ³³S + n from Transmission Measurements

NUCLEAR REACTIONS ³³S(n, n), E=0.010-2 MeV; measured σ(E). ³⁴S deduced resonances, J, π, Γn, Γα, s-, p-wave strength function. Spherical optical model.

doi: 10.1016/0375-9474(87)90034-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12967.

1987DE09      Nucl.Sci.Eng. 96, 58 (1987)

H.Derrien, N.M.Larson, G.de Saussure, R.B.Perez

R-Matrix Analysis of the ²⁴¹Pu Cross Sections up to 100 eV

NUCLEAR REACTIONS ²⁴¹Pu(n, F), (n, n), (n, γ), E ≤ 100 eV; analyzed total, fission σ(E). ²⁴²Pu deduced neutron resonance parameters. R-matrix analysis.

doi: 10.13182/NSE87-A16365
Citations: PlumX Metrics

1986LA34      Radiat.Eff. 96, 251 (1986)

N.M.Larson

Uncertainty Propagation from Raw Data to Final Results

NUCLEAR REACTIONS Fe, Ni(n, n), (n, n'), (n, γ), E=2-80 MeV; calculated σ(E); deduced uncertainty propagation.

doi: 10.1080/00337578608211746
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1986PE03      Nucl.Sci.Eng. 93, 31 (1986)

R.B.Perez, G.de Saussure, N.M.Larson, R.L.R.Macklin

Multilevel Analysis of the Low-Energy ²³⁹Pu Cross Sections

NUCLEAR REACTIONS ²³⁹Pu(n, γ), (n, F), E ≤ 30 eV; analyzed σ(E). ²⁴⁰Pu deduced resonances, Γγ, Γn, fission widths.

doi: 10.13182/NSE83-A17414
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1983JO07      Phys.Rev. C27, 1913 (1983)

C.H.Johnson, N.M.Larson, C.Mahaux, R.R.Winters

Calculation of the Energy-Averaged Scattering Function from High Resolution Low-Energy Neutron Scattering Data

NUCLEAR REACTIONS ³²S(n, n), E ≈ 0.2-0.9 MeV; calculated σ(compound nucleus), σ(shape elastic) vs E. Optical model scattering function, energy averaging, p-wave neutrons.

doi: 10.1103/PhysRevC.27.1913
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