NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.S.Moore Found 41 matches. 1996DA42 Nucl.Sci.Eng. 124, 482 (1996) Y.Danon, M.S.Moore, P.E.Koehler, P.E.Littleton, G.G.Miller, M.A.Ott, L.J.Rowton, W.A.Taylor, J.B.Wilhelmy, M.A.Yates, A.D.Carlson, N.W.Hill, R.Harper, R.Hilko Fission Cross-Section Measurements of the Odd-Odd Isotopes 232Pa, 238Np, and 236Np NUCLEAR REACTIONS, ICPND 232Th(p, n), (p, 3n), E=threshold-20 MeV; 232Th(d, n), (d, 2n), E=threshold-20 MeV; measured residuals production σ(E). 232Pa, 238,236Np(n, F), E < 100 keV; measured fission σ(E). 237Np deduced resonances, fission width, 2gΓn.
doi: 10.13182/NSE96-A17926
1994DA41 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.245 (1994) Y.Danon, M.S.Moore, P.E.Koehler, R.W.Lougheed, R.W.Hoff, N.W.Hill Measurement and analysis of the neutron-induced fission cross section s of 247Cm, 250Cf and 254Es NUCLEAR REACTIONS 247Cm(n, n), 247Cm(n, f), 250Cf(n, f), 254Es(n, f), E=-8.8E-4 eV-9.8 keV; measured products; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 13646. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13646. 1993BE52 Nucl.Phys. A565, 563 (1993) A.Benoufella, G.Barreau, M.Asghar, P.Audouard, F.Brisard, T.P.Doan, M.Hussonnois, B.Leroux, J.Trochon, M.S.Moore Measurement of Fragment Mass-Energy Correlations for 248Cm(s, f): Far-out asymmetric fission and cold fragmentations RADIOACTIVITY 248Cm(SF); measured fission fragment mass-energy correlations; deduced far-out asymmetric fission, cold fission features.
doi: 10.1016/0375-9474(93)90045-Y
1991DA19 Nucl.Sci.Eng. 109, 341 (1991) Y.Danon, R.E.Slovacek, R.C.Block, R.W.Lougheed, R.W.Hoff, M.S.Moore Fission Cross-Section Measurements of 247Cm, 254Es, and 250Cf from 0.1 eV to 80 keV NUCLEAR REACTIONS 247Cm, 254Es, 250Cf(n, F), E ≤ 80 keV; measured fission σ(E). 248Cm deduced resonance widths.
doi: 10.13182/NSE91-A23859
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
1988DE33 Phys.Rev. C38, 1270 (1988) A.D'Eer, C.Wagemans, M.Neve de Mevergnies, F.Gonnenwein, P.Geltenbort, M.S.Moore, J.Pauwels Neutron-Induced Fission of the 26 min 235U Isomer NUCLEAR REACTIONS 235,235mU(n, F), E=cold, thermal; measured isomer to ground state fission σ ratio. Target production from 239Pu decay.
doi: 10.1103/PhysRevC.38.1270
1988SC04 Phys.Lett. 203B, 22 (1988) R.L.Schutt, R.E.Shamu, P.W.Lisowski, M.S.Moore, G.L.Morgan Nucleon Scattering from 208Pb at Low and Intermediate Energies NUCLEAR REACTIONS 208Pb(n, n), E=2-250 MeV; analyzed σ(E). 208Pb(n, n), E=13.5-40 MeV; analyzed σ(θ); deduced model parameters. Phenomenological optical model.
doi: 10.1016/0370-2693(88)91562-6
1987KO17 Phys.Lett. 191B, 249 (1987) P.Koczon, M.Mutterer, J.P.Theobald, P.Geltenbort, F.Gonnenwein, A.Oed, M.S.Moore Cold and ' Hot ' Fragmentation in Thermal Neutron Induced Fission of 245Cm NUCLEAR REACTIONS 245Cm(n, F), E=thermal; measured fission fragment energy, mass distributions; deduced fragmentation mechanism. Tof spectrometer.
doi: 10.1016/0370-2693(87)90249-8
1986KO14 Radiat.Eff. 93, 49 (1986) P.Koczon, M.Mutterer, J.P.Theobald, M.S.Moore, F.Goennenwein, P.Geltenbort, A.Oed, J.Pannicke Mass and Energy Distribution of Fragments from the 245Cm(n(th), f) Reaction NUCLEAR REACTIONS 245Cm(n, F), E=thermal; measured fission fragment mass yield vs fragment kinetic energy, long range Eα, σ(θα).
doi: 10.1080/00337578608207427
1984AU01 Phys.Rev. C29, 174 (1984) G.F.Auchampaugh, M.S.Moore, J.D.Moses, R.O.Nelson, R.C.Extermann, C.E.Olsen, N.W.Hill, J.A.Harvey Nature of the Coupling in Subthreshold Fission of 238Np NUCLEAR REACTIONS 237Np(n, F), (n, X), E-1-600 eV; measured fission, total σ(E). 238Np deduced fission strength function, sharp, broad levels, Γ, subthreshold fission characteristics. Multi-level R-matrix fits.
doi: 10.1103/PhysRevC.29.174
1984MO12 Phys.Rev. C30, 214 (1984) M.S.Moore, L.Calabretta, F.Corvi, H.Weigmann Analysis of Intermediate Structure in the Fission and Capture Cross Sections of (235U+n) NUCLEAR REACTIONS 235U(n, F), (n, γ), E=2-32 keV; analyzed fission to capture σ(E) ratio; deduced intermediate structure role.
doi: 10.1103/PhysRevC.30.214
1983MO02 Nucl.Phys. A393, 1 (1983) M.S.Moore, J.A.Wartena, H.Weigmann, C.Budtz-Jorgensen, H.-H.Knitter, C.E.Olsen Neutron Induced Fission Cross Section of 244Pu NUCLEAR REACTIONS 244Pu(n, F), E=0.001-8 MeV; measured fission σ(E). Gridded ionization chamber, 235U data standard.
doi: 10.1016/0375-9474(83)90061-1
1983SP03 Phys.Rev.Lett. 51, 1522 (1983) W.Spreng, F.Azgui, H.Emling, E.Grosse, R.Kulessa, Ch.Michel, D.Schwalm, R.S.Simon, H.J.Wollersheim, M.Mutterer, J.P.Theobald, M.S.Moore, N.Trautmann, J.L.Egido, P.Ring First Observation of Backbending in an Actinide Nucleus NUCLEAR REACTIONS 242,244Pu(208Pb, 208Pb'), E=5.1, 5.3 MeV/nucleon; measured Coulomb excitation, Doppler shifted γ-spectra, Eγ. 242,244Pu deduced levels, J, π, yrast transitions, backbending, proton shell alignment effects. Microscopic calculations.
doi: 10.1103/PhysRevLett.51.1522
1982LI23 Phys.Rev.Lett. 49, 255 (1982) P.W.Lisowski, R.E.Shamu, G.F.Auchampaugh, N.S.P.King, M.S.Moore, G.L.Morgan, T.S.Singleton Search For Resonance Structure In The np Total Cross Section Below 800 Mev NUCLEAR REACTIONS 1H(n, x), E=39-793 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12761.
doi: 10.1103/PhysRevLett.49.255
1978MO16 Phys.Rev. C18, 1328 (1978) M.S.Moore, J.D.Moses, G.A.Keyworth, J.W.T.Dabbs, N.W.Hill Spin Determination of Resonance Structure in (238U + n) below 25 keV NUCLEAR REACTIONS 235U(n, F), E=1 eV-25 keV; measured J dependence of σ(E). 236U deduced resonance parameters, J, average fission width.
doi: 10.1103/PhysRevC.18.1328
1972MO21 Phys.Rev.Lett. 29, 504 (1972) M.S.Moore, L.G.Miller, G.E.Stokes Correlation between Fission-Channel Effects and Fragment Kinetic Energies NUCLEAR REACTIONS, Fission 235U(n, F), E < 60 eV; measured relative yield of high-energy fission fragments.
doi: 10.1103/PhysRevLett.29.504
1971MO11 Phys.Rev. C3, 1656 (1971) Analysis of the Fission and Capture Cross Sections of the Curium Isotopes NUCLEAR REACTIONS 244,245,246,247,248Cm(n, F), 244,246Cm(n, γ), E=20 eV-3 MeV; measured σ(E). 245,246,247,248,249Cm deduced resonances, level-width.
doi: 10.1103/PhysRevC.3.1656
1971MO21 Phys.Rev. C4, 273 (1971) M.S.Moore, J.H.McNally, R.D.Baybarz Neutron-Induced Fission Cross Section of 252Cf NUCLEAR REACTIONS, Fission 252Cf(n, F), E=20 eV - 5 MeV; measured σ(E). 253Cf deduced resonance parameters, subbarrier fission structure.
doi: 10.1103/PhysRevC.4.273
1971SI06 Nucl.Phys. A164, 34 (1971) F.B.Simpson, L.G.Miller, M.S.Moore, R.W.Hockenbury, T.J.King Neutron Scattering Cross Sections of 233U, 235U and 239Pu NUCLEAR STRUCTURE 240Pu deduced resonance spins below 75 eV. NUCLEAR REACTIONS 233U(n, n), E=0.5 to 190 eV; measured σ(ns)(E). 235U(n, n), E=0.5 to 190 eV; measured σ(ns)(E). 236U deduced resonance spins below 20 eV. 239Pu(n, n), E=2 to 450 eV; measured σ(ns)(E). 240Pu deduced resonance spins below 75 eV.
doi: 10.1016/0375-9474(71)90841-4
1967SI21 Nucl.Sci.Eng. 29, 415 (1967) O.D.Simpson, M.S.Moore, J.R.Berreth Total Neutron Cross Section of 232U NUCLEAR REACTIONS 232U(n, X), E=0.01-10000 eV; measured reaction products, En, In; deduced σ. The Materials Testing Reactor (MTR) fast chopper.
doi: 10.13182/NSE67-A17289
1964MO10 IDO-16932, p.14 (1964) M.S.Moore, O.D.Simpson, T.Watanabe Pu-241 Fission Cross Section NUCLEAR STRUCTURE, Fission 242Pu; measured not abstracted; deduced nuclear properties.
1964MO22 Phys.Rev. 135, B945 (1964) M.S.Moore, O.D.Simpson, T.Watanabe, J.E.Russell, R.W.Hockenbury Fission Cross Section of Pu241 NUCLEAR STRUCTURE, Fission 242Pu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B945
1964MO27 WASH-1046, p.95 (1964); Priv.Comm. (1966) M.S.Moore, O.D.Simpson, T.Watanabe Pu241 Fission Cross Section
1964SI28 Nucl.Instrum.Methods 30, 293 (1964) O.D.Simpson, R.G.Fluharty, M.S.Moore, N.H.Marshall, F.B.Simpson, G.E.Stokes, T.Watanabe, T.E.Young The Determination Of Backgrounds For Neutron Time-Of-Flight Spectrometers NUCLEAR REACTIONS H(n, x), C(n, x), E=0.4222 eV-1.7 keV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 11020.
doi: 10.1016/0029-554X(64)90289-7
1963BE32 IDO-16898, p. 9 (1963) J.R.Berreth, M.S.Moore, O.D.Simpson Total Cross Section of U232 NUCLEAR STRUCTURE 233U; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12375. 1963BE58 WASH-1044, p.74 (1963); Priv.Comm. To K.K.Seth (1964) J.R.Berreth, M.S.Moore, O.D.Simpson, R.P.Schuman Total Neutron Cross Section of U232
1963BE61 Trans.Amer.Nucl.Soc. 6, 44 (1963) J.R.Berreth, M.S.Moore, O.D.Simpson Total Neutron Cross Section of U-232 NUCLEAR REACTIONS 232U(n, X), E=0.01-1000 eV; measured reaction products; deduced σ. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12375. 1962MO05 Nuclear Sci.And Eng. 13, 18 (1962) The Neutron Elastic Scattering Cross Section of U233 below 2 eV NUCLEAR STRUCTURE 233U; measured not abstracted; deduced nuclear properties.
doi: 10.13182/NSE62-A26123
1961RE02 Nuclear Phys. 22, 104 (1961) D.H.Rester, M.S.Moore, F.E.Durham, C.M.Class Internal Conversion Electrons from Coulomb Excitation of Heavy Elements NUCLEAR STRUCTURE 232Th, 236U, 234U, 230Th, 192Os, 188Os, 189Os, 190Os, 186Os, 197Au, 238U; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90367-4
1961SI02 Bull.Am.Phys.Soc. 6, No.3, 275, P8 (1961) Analysis of the Pu241 Total Neutron Cross Section NUCLEAR STRUCTURE 242Pu; measured not abstracted; deduced nuclear properties.
1961SI05 Phys.Rev. 123, 559 (1961) Multilevel Analysis of the Total Neutron Cross Section of Pu241 below 12 eV
doi: 10.1103/PhysRev.123.559
1960MO06 Phys.Rev. 118, 714 (1960) M.S.Moore, L.G.Miller, O.D.Simpson Slow Neutron Total and Fission Cross Sections of U233 NUCLEAR STRUCTURE 234U, 233U; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.118.714
1960MO23 Phys.Rev. 118, 718 (1960) Multilevel Analysis Of Slow Neutron Cross Sections Of U233 NUCLEAR REACTIONS 233U, 233U(n, n), 233U(n, f), 233U(n, γ), E=0.15-10.5 eV; measured products, Eγ, Iγ; deduced resonance parameters. Data were imported from EXFOR entry 12342.
doi: 10.1103/PhysRev.118.718
1958FL41 Proc.U.N.Intern.Conf.Peaceful Uses At. Energy, 2nd, Geneva 15, 111 (1958) R.G.Fluharty, M.S.Moore, J.E.Evans
1958MI90 IDO-16505, p.58 (1958) L.G.Miller, M.K.Brice, M.S.Moore Measurements to Determine the Half-Life of Tantalum180
1958RE05 Bull.Am.Phys.Soc. 3, No.1, 6, A5 (1958) R.B.Regier, W.H.Burgus, J.R.Smith, M.S.Moore Neutron Energy Dependent Mass Distribution in U233 Fission
1956MO08 Bull.Am.Phys.Soc. 1, No.2, 88, H2 (1956) M.S.Moore, C.M.Class, F.W.Prosser, Jr., J.P.Schiffer Conversion Spectra of Coulomb-Excited Th232 and Au197
1956MO95 Bull.Am.Phys.Soc. 1, 327, G10 (1956) M.S.Moore, L.G.Miller, C.W.Reich Uranium-233 resonance parameters for neutron energies below 4 eV NUCLEAR REACTIONS 233U(n, X), (n, F), (n, γ), E<4 eV; measured reaction products, En, In; deduced resonance parameters. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12342. 1956PR12 Bull.Am.Phys.Soc. 1, No.4, 163, B7 (1956); Oral Report F.W.Prosser, Jr., M.S.Moore, J.P.Schiffer Positron Decay of Cu59
1956SC09 Phys.Rev. 104, 1661 (1956) J.P.Schiffer, M.S.Moore, C.M.Class Compound States of the System Ni58 + p
doi: 10.1103/PhysRev.104.1661
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