NSR Query Results

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NSR database version of April 11, 2024.

Search: Author = M.White

Found 53 matches.

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2024LE02      Phys.Rev. C 109, 014601 (2024)

H.Y.Lee, S.A.Kuvin, L.Zavorka, S.Mosby, B.DiGiovine, G.Hale, M.Paris, D.Votaw, M.White

Differential cross sections of the ¹⁶O(n, α) reaction at neutron energies from 3.8 to 15 MeV

doi: 10.1103/PhysRevC.109.014601
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2023KE09      Phys.Rev. C 108, 024603 (2023)

K.J.Kelly, M.Devlin, J.M.O'Donnell, D.Neudecker, A.E.Lovell, R.C.Haight, C.Y.Wu, R.Henderson, E.A.Bennett, T.Kawano, J.L.Ullmann, N.Fotiades, J.Henderson, S.M.Mosby, T.N.Taddeucci, P.Talou, M.C.White, J.A.Gomez, H.Y.Lee

Measurement of the ²³⁸U(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons with 1.5-20 MeV energy

NUCLEAR REACTIONS ²³⁸U(n, F), E=1.5-20 MeV; measured fission fragments, En, In, neutron time-of-flight, (fragment)n-coin; deduced prompt fission neutron spectrum (PFNS). Systematic trends in PFNS and PFNS ratios for ²³⁹Pu, ²³⁵U, and ²³⁸U obtained in series of Chi-Nu experiments. Comparison to other experimental results, CGMF calculations and data from JEFF-3.3, JENDL-5.0. ENDF/B-VIII libraries. Pulsed white neutron source at Weapons Neutron Research (WNR) facility of the Los Alamos Neutron Science Center (LANSCE). Li-glass array consisting of 22 detectors and liquid scintillator array consisting of 54 detector used for neutron detection, while PPAC used for detecting fission fragments in the frame of Chi-Nu experiment.

doi: 10.1103/PhysRevC.108.024603
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2023NE11      Eur.Phys.J. N 9, 32 (2023)

D.Neudecker, M.Devlin, R.C.Haight, K.J.Kelly, P.Marini, A.D.Carlson, J.Taieb, M.C.White

Templates of expected measurement uncertainties for prompt fission neutron spectra

RADIOACTIVITY ²⁵²Cf(SF); analyzed available data; deduced prompt-fission neutron spectrum (PFNS), ratio to a Maxwellian function.

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<20 MeV; analyzed available data; deduced prompt-fission neutron spectrum (PFNS), ratio to a Maxwellian function.

doi: 10.1051/epjn/2023013
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2022KE01      Phys.Rev. C 105, 044615 (2022)

K.J.Kelly, J.A.Gomez, M.Devlin, J.M.O'Donnell, D.Neudecker, A.E.Lovell, R.C.Haight, C.Y.Wu, R.Henderson, T.Kawano, E.A.Bennett, S.M.Mosby, J.L.Ullmann, N.Fotiades, J.Henderson, T.N.Taddeucci, H.Y.Lee, P.Talou, M.C.White

Measurement of the ²³⁵U(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons of energy from 1 MeV to 20 MeV

NUCLEAR REACTIONS ²³⁵U(n, F), E=0.01-10 MeV; measured In, En, neutron time-of-flight, fission fragments, neutrons angular distributions, (fragment)n-coin; deduced prompt fission neutron spectrum (PFNS), components corresponding to first-, second-, and third-chance fission as well as pre-equilibrium neutron emission preceding fission, mean PFNS energy, ratio to PFNMS obtained in ²³⁹Pu(n, F) reaction. Experiment performed as a part of Chi-Nu project aimed to measure the PFNS of major actinides with the Weapons Neutron Research (WNR) facility at the Los Alamos Neutron Science Center (LANSCE). The results are compared with other experimental data, CGMF calculations and selected nuclear data evaluations - ENDF/B-VIII.0, JEFF-3.3, JENDL-5.0.

doi: 10.1103/PhysRevC.105.044615
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2022KU12      Phys.Rev. C 105, 044608 (2022)

S.A.Kuvin, H.Y.Lee, B.DiGiovine, C.Eiroa-Lledo, A.Georgiadou, M.Herman, T.Kawano, V.Mocko, S.Mosby, C.Vermeulen, D.Votaw, M.White, L.Zavorka, G.Perdikakis, P.Tsintari, H.I.Kim

Direct measurement of ⁵⁹Ni(n, p) ⁵⁹Co and ⁵⁹Ni(n, α)⁵⁶Fe at fast-neutron energies from 500 keV to 10 MeV

NUCLEAR REACTIONS ⁵⁹Ni(n, p), (n, α), E=0.5-10 MeV; measured Ep, Ip, Eα, Iα, neutron time of flight, np-coin, nα-coin; deduced Q, inclusive and exclusive σ(E). Comparison to statistical Hauser-Feschbach calculations (TALYS, CoH3), evaluated data (ENDF/B-VIII.0, JEFF-3.3, JENDL-4.0) and other experimental results. Low Energy (n, z) (LENZ) setup consisting of annular double-sided silicon strip detectors at the WNR facility at the Los Alamos Neutron Science Center (LANSCE).

doi: 10.1103/PhysRevC.105.044608
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14787.

2021HE28      Ann.Nucl.Energy 163, 108494 (2021)

M.Herman, D.A.Brown, R.Capote, M.B.Chadwick, W.Haeck, J.D.Hutchinson, T.Kawano, D.Neudecker, G.Palmiotti, M.Salvatores, P.Talou, A.Trkov, M.C.White

Infrastructure for the new paradigm of nuclear reaction evaluation

NUCLEAR REACTIONS ¹⁰⁵Pd(n, γ), ²³⁵U, ²³⁹Pu(n, F), E<20 MeV; analyzed available data; deduced pilot assimilation project needs.

doi: 10.1016/j.anucene.2021.108494
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2021KE05      Nucl.Data Sheets 173, 42 (2021)

K.J.Kelly, P.Marini, J.Taieb, M.Devlin, D.Neudecker, R.C.Haight, G.Belier, B.Laurent, P.Morfouace, J.M.O'Donnell, E.Bauge, M.B.Chadwick, A.Chatillon, D.Etasse, P.Talou, M.C.White, C.Y.Wu, E.A.Bennett

Comparison of Results from Recent NNSA and CEA Measurements of the ²³⁹Pu(n, f) Prompt Fission Neutron Spectrum

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<20 MeV; analyzed the NNSA and CEA data; deduced prompt fission neutron spectrum (PFNS), systematic differences.

doi: 10.1016/j.nds.2021.04.003
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2021KU19      Phys.Rev. C 104, 014603 (2021)

S.A.Kuvin, H.Y.Lee, B.DiGiovine, A.Georgiadou, S.Mosby, D.Votaw, M.White, L.Zavorka

Validation of neutron-induced reactions on natural carbon using an active target at neutron energies up to 22 MeV at LANSCE

NUCLEAR REACTIONS ¹²C(n, α)⁹Be, (n, p), (n, pd), ¹³C(n, α)¹⁰Be, E=6-22 MeV; measured reaction products, relative σ(E) using natural carbon target and LENZ annular silicon detectors with the flux monitor ionization chamber at Weapons Neutron Research (WNR) facility at the Los Alamos Neutron Science Center (LANSCE). Comparison with GEANT4 simulations using the ENDF/B-VIII.0 evaluated nuclear data library up to E(n)=20 MeV, and with previous experimental data.

doi: 10.1103/PhysRevC.104.014603
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14711.

2021NE02      Ann.Nucl.Energy 159, 108345(2021)

D.Neudecker, O.Cabellos, A.R.Clark, W.Haeck, R.Capote, A.Trkov, M.C.White, M.E.Rising

Which nuclear data can be validated with LLNL pulsed-sphere experiments?

doi: 10.1016/j.anucene.2021.108345
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2020KE05      Phys.Rev. C 102, 034615 (2020)

K.J.Kelly, M.Devlin, J.M.O'Donnell, J.A.Gomez, D.Neudecker, R.C.Haight, T.N.Taddeucci, S.M.Mosby, H.Y.Lee, C.Y.Wu, R.Henderson, P.Talou, T.Kawano, A.E.Lovell, M.C.White, J.L.Ullmann, N.Fotiades, J.Henderson, M.Q.Buckner

Measurement of the ²³⁹Pu(n, f) prompt fission neutron spectrum from 10 keV to 10 MeV induced by neutrons of energy 1-20 MeV

NUCLEAR REACTIONS ²³⁹Pu(n, F), E=1-20 MeV; measured outgoing prompt fission neutron spectrum (PFNS) in the range of E(n)=0.01-10 MeV, I(n) using Li-glass detector array and 54-detector EJ-309 liquid scintillator array in Chi-Nu experiment at the WNR-LANSCE-Los Alamos facility; deduced correlation matrix for PFNS from the Li-glass and the liquid scintillator. Comparison of present PFNS results with previous experimental results, and with evaluated data in ENDF/B-VIII.0 and JEFF-3.3 libraries.

doi: 10.1103/PhysRevC.102.034615
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14682.

2020KU17      Phys.Rev. C 102, 024623 (2020)

S.A.Kuvin, H.Y.Lee, T.Kawano, B.DiGiovine, A.Georgiadou, C.Vermeulen, M.White, L.Zavorka, H.I.Kim

Nonstatistical fluctuations in the ³⁵Cl(n, p)³⁵S reaction cross section at fast-neutron energies from 0.6 to 6 MeV

NUCLEAR REACTIONS ³⁵Cl(n, p), (n, α), E=0.6-6 MeV spallation neutrons; measured charged particles from (n, p) and (n, α) reactions using the low energy LENZ experimental setup, flight path length using a sCVD diamond detector by measuring the neutron time of flight at the WNR facility of the Los Alamos Neutron Science Center (LANSCE); deduced Q value of the reaction from detected charged particle energy of the outgoing proton or α particle, and the corresponding neutron time-of-flight, σ(θ, E) for different reaction channels, angle-integrated partial cross section data for (n, p) and (n, α) channels. Comparison with statistical model HF calculation using the COH3 code, and Koning-Delaroche spherical optical potential and Kunieda coupled channel potential, and with evaluated cross section data in ENDF/B-VIII.0. ⁶³Cu, ⁶⁴Zn(n, p), (n, α), E=0.6-6 MeV; measured charged particles, σ(E) from the brass backing for background contributions, and to validate MCNP simulations using data from the present experiment, ENDF/B-VIII.0 evaluations, and from previous experiments.

doi: 10.1103/PhysRevC.102.024623
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14683.

2020NE03      Nucl.Data Sheets 163, 228 (2020)

D.Neudecker, D.L.Smith, F.Tovesson, R.Capote, M.C.White, N.S.Bowden, L.Snyder, A.D.Carlson, R.J.Casperson, V.Pronyaev, S.Sangiorgio, K.T.Schmitt, B.Seilhan, N.Walsh, W.Younes

Applying a Template of Expected Uncertainties to Updating ²³⁹Pu(n, f) Cross-section Covariances in the Neutron Data Standards Database

doi: 10.1016/j.nds.2019.12.005
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2020TR01      Nucl.Data Sheets 163, 1 (2020)

A.Trkov, P.J.Griffin, S.P.Simakov, L.R.Greenwood, K.I.Zolotarev, R.Capote, D.L.Aldama, V.Chechev, C.Destouches, A.C.Kahler, C.Konno, M.Kostal, M.Majerle, E.Malambu, M.Ohta, V.G.Pronyaev, V.Radulovic, S.Sato, M.Schulc, E.Simeckova, I.Vavtar, J.Wagemans, M.White, H.Yashima

IRDFF-II: A New Neutron Metrology Library

doi: 10.1016/j.nds.2019.12.001
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2019KE04      Phys.Rev.Lett. 122, 072503 (2019)

K.J.Kelly, T.Kawano, J.M.O'Donnell, J.A.Gomez, M.Devlin, D.Neudecker, P.Talou, A.E.Lovell, M.C.White, R.C.Haight, T.N.Taddeucci, S.M.Mosby, H.Y.Lee, C.Y.Wu, R.Henderson, J.Henderson, M.Q.Buckner

Preequilibrium Asymmetries in the ²³⁹Pu(n, f) Prompt Fission Neutron Spectrum

NUCLEAR REACTIONS ²³⁹Pu(n, F), E=15-17.5 MeV; measured reaction products, En, In; deduced neutron excess of the preequilibrium prefission distribution above the postfission neutron spectrum. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.122.072503
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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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2018DE08      Nucl.Data Sheets 148, 322 (2018)

M.Devlin, J.A.Gomez, K.J.Kelly, R.C.Haight, J.M.O'Donnell, T.N.Taddeucci, H.Y.Lee, S.M.Mosby, B.A.Perdue, N.Fotiades, J.L.Ullmann, C.Y.Wu, B.Bucher, M.Q.Buckner, R.A.Henderson, D.Neudecker, M.C.White, P.Talou, M.E.Rising, C.J.Solomon

The Prompt Fission Neutron Spectrum of ²³⁵U(n, f) below 2.5 MeV for Incident Neutrons from 0.7 to 20 MeV

NUCLEAR REACTIONS ²³⁵U(n, F), E=0.7-20 MeV; measured reaction products, En, In, TOF; deduced prompt fission neutron spectrum, σ(E).

doi: 10.1016/j.nds.2018.02.008
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2018NE02      Nucl.Data Sheets 148, 293 (2018)

D.Neudecker, P.Talou, T.Kawano, A.C.Kahler, M.C.White, T.N.Taddeucci, R.C.Haight, B.Kiedrowski, J.M.O'Donnell, J.A.Gomez, K.J.Kelly, M.Devlin, M.E.Rising

Evaluations of Energy Spectra of Neutrons Emitted Promptly in Neutron-induced Fission of ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F)¹NN, E<20 MeV; analyzed available data; deduced σ(E), total kinetic energies.

doi: 10.1016/j.nds.2018.02.006
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2016NE02      Nucl.Data Sheets 131, 289 (2016)

D.Neudecker, T.N.Taddeucci, R.C.Haight, H.Y.Lee, M.C.White, M.E.Rising

The Need for Precise and Well-documented Experimental Data on Prompt Fission Neutron Spectra from Neutron-induced Fission of ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<20 MeV; calculated prompt fission En, In. Comparison with available data.

doi: 10.1016/j.nds.2015.12.005
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2015HA01      Nucl.Data Sheets 123, 130 (2015)

R.C.Haight, C.Y.Wu, H.Y.Lee, T.N.Taddeucci, B.A.Perdue, J.M.O'Donnell, N.Fotiades, M.Devlin, J.L.Ullmann, T.A.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, D.Neudecker, M.E.Rising, S.Mosby, S.Sjue, M.C.White, B.Bucher, R.Henderson

The LANL/LLNL Prompt Fission Neutron Spectrum Program at LANSCE and Approach to Uncertainties

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<15 MeV; analyzed available data; deduced possible prompt fission neutron spectra σ, yields, correlation matrices.

doi: 10.1016/j.nds.2014.12.023
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2015NE02      Nucl.Data Sheets 123, 146 (2015)

D.Neudecker, P.Talou, T.N.Taddeucci, R.C.Haight, T.Kawano, H.Y.Lee, D.L.Smith, R.Capote, M.E.Rising, M.C.White

Preliminary Evaluation and Uncertainty Quantification of the Prompt Fission Neutron Spectrum of ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, X), E<20 MeV; calculated σ correlation matrices, prompt fission neutron spectrum and associated covariances. ENDF/B-VII.1 evaluated nuclear data library.

doi: 10.1016/j.nds.2014.12.026
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2015TA03      Nucl.Data Sheets 123, 135 (2015)

T.N.Taddeucci, R.C.Haight, H.Y.Lee, D.Neudecker, J.M.O'Donnell, M.C.White, B.A.Perdue, M.Devlin, N.Fotiadis, J.L.Ullmann, R.O.Nelson, T.A.Bredeweg, M.E.Rising, S.K.Sjue, S.A.Wender, C.Y.Wu, R.Henderson

Multiple-scattering Corrections to Measurements of the Prompt Fission Neutron Spectrum

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<15 MeV; analyzed available data; deduced response functions, the shape of the prompt fission neutron spectrum.

doi: 10.1016/j.nds.2014.12.024
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2014AR09      Nucl.Data Sheets 119, 392 (2014)

C.W.Arnold, F.Tovesson, K.C.Meierbachtol, A.B.Laptev, T.A.Bredeweg, M.Jandel, R.O.Nelson, M.C.White

Precision Velocity Measurements of Fission Fragments Using the SPIDER Detector

doi: 10.1016/j.nds.2014.08.109
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2014HA27      Nucl.Data Sheets 119, 205 (2014)

R.C.Haight, H.Y.Lee, T.N.Taddeucci, J.M.O'Donnell, B.A.Perdue, N.Fotiades, M.Devlin, J.L.Ullmann, A.Laptev, T.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, M.C.White, C.Y.Wu, E.Kwan, A.Chyzh, R.Henderson, J.Gostic

The Prompt Fission Neutron Spectrum (PFNS) Measurement Program at LANSCE

doi: 10.1016/j.nds.2014.08.057
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2014ME10      Nucl.Data Sheets 119, 389 (2014)

K.Meierbachtol, F.Tovesson, C.W.Arnold, A.B.Laptev, T.A.Bredeweg, M.Jandel, R.O.Nelson, M.C.White

Development of an Ionization Chamber for the SPIDER Fission Fragment Detector

doi: 10.1016/j.nds.2014.08.108
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2014PA29      Phys.Lett. B 735, 387 (2014)

D.Patel, U.Garg, M.Itoh, H.Akimune, G.P.A.Berg, M.Fujiwara, M.N.Harakeh, C.Iwamoto, T.Kawabata, K.Kawase, J.T.Matta, T.Murakami, A.Okamoto, T.Sako, K.W.Schlax, F.Takahashi, M.White, M.Yosoi

Excitation of giant monopole resonance in ²⁰⁸Pb and ¹¹⁶Sn using inelastic deuteron scattering

NUCLEAR REACTIONS ²⁰⁸Pb, ¹¹⁶Sn(d, d'), (d, d), E=196 MeV; measured reaction products; deduced σ(θ), σ(θ, E), isoscalar giant monopole resonance strength. Comparison with available data.

doi: 10.1016/j.physletb.2014.06.073
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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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2010TA15      Nucl.Sci.Eng. 166, 254 (2010)

P.Talou, T.Kawano, D.G.Madland, A.C.Kahler, D.K.Parsons, M.C.White, R.C.Little, M.B.Chadwick

Uncertainty Quantification of Prompt Fission Neutron Spectrum for n(0.5 MeV) + ²³⁹Pu

NUCLEAR REACTIONS ²³⁹Pu(n, F), E<0.5 MeV; calculated fission spectrum uncertainties, probability distribution functions; deduced correlation matrix. Madland-Nix model.

doi: 10.13182/NSE09-10
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2009CH04      Ann.Nucl.Energy 36, 258 (2009)

M.B.Chadwick, R.C.Little, T.Kawano, P.Talou, D.Viera, M.Jandel, T.A.Bredeweg, M.C.White, A.P.Tonchev, J.A.Becker

Actinide ENDF/B-VII cross-section evaluations and validation testing

NUCLEAR REACTIONS ²⁴¹Am(n, γ), E < 1000 MeV; ²⁴¹Am(n, 2n), E < 20 MeV; analyzed cross sections. ²³⁹Pu(n, X), E=1.0 MeV; ²³⁸U(n, γ), E < 1.0 MeV; calculated cross sections.

doi: 10.1016/j.anucene.2008.11.011
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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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2003CH80      Nucl.Sci.Eng. 144, 157 (2003)

M.B.Chadwick, P.G.Young, R.E.MacFarlane, M.C.White, R.C.Little

Photonuclear Physics in Radiation Transport - I: Cross Sections and Spectra

NUCLEAR REACTIONS ^206,207,208Pb, ¹⁸⁴W, ¹⁸¹Ta, ⁶³Cu, ⁴⁰Ca, ²⁸Si, ²⁷Al, ¹⁶O, ¹²C(γ, X), (γ, nX), E < 150 MeV; calculated absorption, photoneutron production σ. Comparison with data.

doi: 10.13182/NSE144-157
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2003WH01      Nucl.Sci.Eng. 144, 174 (2003)

M.C.White, R.C.Little, M.B.Chadwick, P.G.Young, R.E.MacFarlane

Photonuclear Physics in Radiation Transport - II: Implementation

doi: 10.13182/NSE144-174
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1965SC13      Phys.Rev. 138, B306 (1965)

R.G.Schlecht, M.B.White, D.W.McColm

Hyperfine Structures of Re¹⁸⁶ and Re¹⁸⁸

NUCLEAR STRUCTURE ¹⁸⁶Re, ¹⁸⁸Re; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.306
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1965WH03      Phys.Rev. 137, B477 (1965)

M.B.White, S.S.Alpert, S.Penselin, T.I.Moran, V.W.Cohen, E.Lipworth

Hyperfine Structure of Lu^176m by the Method of Atomic Beams

NUCLEAR STRUCTURE ¹⁷⁶Lu; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.477
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1964WH05      Phys.Rev. 136, B584 (1964)

M.B.White, E.Lipworth, S.Alpert

Hyperfine Structure and Nuclear Moments of Br⁸⁰ and Br^80m

NUCLEAR STRUCTURE ⁸⁰Br; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.136.B584
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1963CO26      Bull.Am.Phys.Soc. 8, No.8, 619, S7 (1963)

V.W.Cohen, T.I.Moran, S.Penselin, S.Alpert, M.W.White

Hyperfine Structure of Lu^176m by Atomic Beams

NUCLEAR STRUCTURE ¹⁷⁶Lu; measured not abstracted; deduced nuclear properties.

1963SC16      Bull.Am.Phys.Soc. 8, No.6, 464, C3 (1963)

R.G.Schlecht, M.B.White, D.McColm

Hyperfine Structure of Re¹⁸⁶ and Re¹⁸⁸

NUCLEAR STRUCTURE ¹⁸⁸Re, ¹⁸⁶Re; measured not abstracted; deduced nuclear properties.

1963WH05      UCRL-11013 (1963)

M.B.White, E.Lipworth, S.Alpert

NUCLEAR STRUCTURE ⁸⁰Br; measured not abstracted; deduced nuclear properties.

1962AL02      Phys.Rev. 125, 256 (1962)

S.S.Alpert, E.Lipworth, M.B.White, K.F.Smith

Hyperfine Structure and Nuclear Moments of RaE (Bi²¹⁰)

NUCLEAR STRUCTURE ²¹⁰Bi; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.125.256
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1962WH10      Bull.Am.Phys.Soc. 7, No.7, 476, MA11 (1962)

M.B.White, S.S.Alpert, E.Lipworth

Nuclear Moments of Br⁸⁰ and Br^80m

NUCLEAR STRUCTURE ⁸⁰Br; measured not abstracted; deduced nuclear properties.

1962WH11      Thesis, Univ.California (1962); UCRL-10321; Priv.Comm. (April 1963)

M.B.White

Hyperfine Structure and Nuclear Moments of Lu^176m, Br⁸⁰, Br⁸⁰m, and I¹³²

NUCLEAR STRUCTURE ⁸⁰Br, ¹⁷⁶Lu, ¹³²I; measured not abstracted; deduced nuclear properties.

1961AL03      Bull.Am.Phys.Soc. 6, No.1, 74, Y9 (1961); Oral Report

S.S.Alpert, E.Lipworth, M.B.White, K.F.Smith

Magnetic Dipole and Electric Quadrupole Interaction COnstants of Bi²¹⁰

NUCLEAR STRUCTURE ²¹⁰Bi; measured not abstracted; deduced nuclear properties.

1960AL01      Bull.Am.Phys.Soc. 5, No.4, 273, R3 (1960)

S.S.Alpert, E.Lipworth, M.B.White

Nuclear Moments of I¹³³

NUCLEAR STRUCTURE ¹³³I; measured not abstracted; deduced nuclear properties.

1960WH01      Bull.Am.Phys.Soc. 5, No.4, 273, R6 (1960)

M.B.White, S.S.Alpert, E.Lipworth

Nuclear Spin of Lu^176m

NUCLEAR STRUCTURE ¹⁷⁶Lu; measured not abstracted; deduced nuclear properties.

1960WH06      Bull.Am.Phys.Soc. 5, No.7, 504, L9 (1960)

M.B.White, S.S.Alpert, H.L.Garvin, E.Lipworth

Nuclear Moments of I¹³²

NUCLEAR STRUCTURE ¹³²I; measured not abstracted; deduced nuclear properties.

1952YN01      Phys.Rev. 87, 223 UA8 (1952)

J.L.Yntema, M.G.White

p-p Scattering at 18.3 Mev

NUCLEAR REACTIONS ¹H(p, p), E=18.3 MeV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with available data.

doi: 10.1103/PhysRev.87.179
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1949SH25      Phys.Rev. 75, 282 (1949)

R.Sherr, H.R.Muether, M.G.White

Radioactivity of C¹⁰ and O¹⁴

doi: 10.1103/PhysRev.75.282
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1941WH02      Phys.Rev. 59, 63 (1941)

M.G.White, E.C.Creutz, L.A.Delsasso, R.R.Wilson

Positrons from Light Nuclei

doi: 10.1103/PhysRev.59.63
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1940CR06      Phys.Rev. 58, 481 (1940)

E.C.Creutz, L.A.Delsasso, R.B.Sutton, M.G.White, W.H.Barkas

Radioactivity Produced by Proton Bombardment of Br and Iodine

doi: 10.1103/PhysRev.58.481
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1940DE01      Phys.Rev. 58, 586 (1940)

L.A.Delsasso, M.G.White, W.Barkas, E.C.Creutz

The Carbon Isotopes of Mass Ten and Eleven

NUCLEAR REACTIONS ¹¹B(p, n), ¹⁴N(p, α), ¹⁰B(p, n), E=6.4 MeV; measured reaction products, Eβ, Iβ; deduced T_1/2, Q-values. Cloud chamber, Princeton cyclotron.

doi: 10.1103/PhysRev.58.586
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1939DE01      Phys.Rev. 55, 113 (1939)

L.A.Delsasso, L.N.Ridenour, R.Sherr, M.G.White

Artificial Radioactivity Produced by Protons

doi: 10.1103/PhysRev.55.113
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1939FO01      Phys.Rev. 55, 1106 (1939)

J.G.Fox, E.C.Creutz, M.G.White, L.A.Delsasso

The Difference in Coulomb Energy of Light, Isobaric Nuclei

NUCLEAR REACTIONS ¹⁹F, ²³Na, ²¹Ne(p, n), E not given; measured reaction products; deduced Q-values, T_1/2. Comparison with available data.

doi: 10.1103/PhysRev.55.1106
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1939WH02      Phys.Rev. 56, 512 (1939)

M.G.White, L.A.Delsasso, J.G.Fox, E.C.Creutz

Short-Lived Radioactivities Induced in Fluorine, Sodium and Magnesium by High Energy Protons

doi: 10.1103/PhysRev.56.512
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1938RI01      Phys.Rev. 53, 770 (1938)

L.N.Ridenour, L.A.Delsasso, M.G.White, R.Sherr

Artificial Radioactivity Produced by Protons

NUCLEAR REACTIONS Ni(p, X)⁶¹Cu/⁶⁴Cu/⁶²Cu/⁵⁸Cu, Cu(p, X)⁶³Zn, Mg(p, X)²⁶Al/²⁴Al/²⁵Al, Ag(p, X)¹⁰⁷Cd/¹⁰⁹Cd, E=3.8 MeV; measured reaction products. ^58,60Ni, ^107,109In; deduced new isotopes T_1/2, relative radiation intensities.

doi: 10.1103/PhysRev.53.770
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Note: The following list of authors and aliases matches the search parameter M.White: , M.B.WHITE, M.C.WHITE, M.G.WHITE, M.W.WHITE