NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.G.Thompson Found 82 matches. 1976BA08 Nucl.Phys. A258, 172 (1976) R.Babinet, L.G.Moretto, J.Galin, R.Jared, J.Moulton, S.G.Thompson Diffusion Processes in the Relaxed Cross Section for the Reaction 107,109Ag + 20Ne NUCLEAR REACTIONS 107,109Ag(20Ne, X), E=175, 252 MeV; measured σ(E, Z, θ), Z ≤ 32.
doi: 10.1016/0375-9474(76)90538-8
1976MO05 Nucl.Phys. A259, 173 (1976) L.G.Moretto, J.Galin, R.Babinet, Z.Fraenkel, R.Schmitt, R.Jared, S.G.Thompson Potential Energy Effects and Diffusion in the Relaxed Components of the Reaction 197Au + 40Ar at 288 and 340 MeV Bombarding Energies NUCLEAR REACTIONS 197Au(40Ar, X), E=288, 340 MeV; measured σ(E(fragment Z), θ), Z ≤ 32.
doi: 10.1016/0375-9474(76)90502-9
1975GA21 Nucl.Phys. A255, 472 (1975) J.Galin, L.G.Moretto, R.Babinet, R.Schmitt, R.Jared, S.G.Thompson Evidence of Incomplete Relaxation in the Reaction Ag+40Ar at 288 and 340 MeV Bombarding Energies NUCLEAR REACTIONS 107,109Ag(40Ar, X), E=288, 340 MeV; measured σ(E(fragment mass), θ), Z ≤ 30.
doi: 10.1016/0375-9474(75)90694-6
1975MO25 Phys.Lett. 58B, 31 (1975) L.G.Moretto, R.P.Babinet, J.Galin, S.G.Thompson Experimental Evidence of a Diffusion Process Associated with the Mass Asymmetry Degree of Freedom in Heavy Ion Reactions NUCLEAR REACTIONS 107,109Ag(14N, X), E=160 MeV; 107,109Ag(20Ne, X), E=252 MeV; 107,109Ag(40Ar, X), E=228 MeV; measured σ(fragment mass, θ).
doi: 10.1016/0370-2693(75)90719-4
1975MO30 Nucl.Phys. A255, 491 (1975) L.G.Moretto, S.K.Kataria, R.C.Jared, R.Schmitt, S.G.Thompson Intermediate Mass Fragments Emitted in the Reaction Ag+14N at 100, 160 and 250 MeV Bombarding Energy NUCLEAR REACTIONS 107,109Ag(14N, X), E=100, 160, 250 MeV; measured σ(E(fragment mass), θ), Z ≤ 17.
doi: 10.1016/0375-9474(75)90695-8
1975NA03 Nucl.Phys. A237, 419 (1975) E.Nardi, L.G.Moretto, S.G.Thompson Statistical Decay of Gamma Rays in (n(th), γ) Reactions NUCLEAR STRUCTURE Z=69-197; calculated isomer production ratios for thermal neutron capture.
doi: 10.1016/0375-9474(75)90408-X
1973NA02 Phys.Lett. 43B, 259 (1973) E.Nardi, L.G.Moretto, S.G.Thompson Calculations of Neutron Evaporation from 252Cf Fission Fragments Based On the Shell Model NUCLEAR STRUCTURE 252Cf; calculated neutron evaporation.
doi: 10.1016/0370-2693(73)90434-6
1972CH39 Phys.Rev. C6, 1348 (1972) E.Cheifetz, R.C.Jared, E.R.Giusti, S.G.Thompson Search for Superheavy Elements in Nature
doi: 10.1103/PhysRevC.6.1348
1972MO10 Phys.Lett. 38B, 471 (1972) L.G.Moretto, S.G.Thompson, J.Routti, R.C.Gatti Influence of Shells and Pairing on the Fission Probabilities of Nuclei Below Radium NUCLEAR STRUCTURE, Fission 213At, 212Po, 211Po, 209Bi, 207Bi, 201Tl, 198Hg, 191Ir, 189Ir, 186,187,188Os, 185Re, 179Ta, 173Lu; analyzed fission probabilities; deduced fission barriers.
doi: 10.1016/0370-2693(72)90519-9
1972WI15 Phys.Rev. C5, 2041 (1972) J.B.Wilhelmy, E.Cheifetz, R.C.Jared, S.G.Thompson, H.R.Bowman, J.O.Rasmussen Angular Momentum of Primary Products Formed in the Spontaneous Fission Of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(fragment)(γ)-, (fragment)(fragment)(γ)(γ)-, (fragment)(fragment)(X)(γ)-coin, γγ-coin, Iγ(θ); deduced angular momentum of primary products. 100,102Zr, 104,106Mo, 108,110,112Ru, 112,114,116Pd, 118Cd, 138,140Xe, 142,144,146Ba, 146,148,150Ce, 152,154Nd, 158Sm; measured Iγ.
doi: 10.1103/PhysRevC.5.2041
1971CH14 Phys.Rev. C3, 2017 (1971) E.Cheifetz, H.R.Bowman, J.B.Hunter, S.G.Thompson Prompt Neutrons from Spontaneous Fission of 257Fm RADIOACTIVITY, Fission 257Fm(SF); measured average prompt neutron number.
doi: 10.1103/PhysRevC.3.2017
1971CH44 Phys.Rev. C4, 1913 (1971) E.Cheifetz, J.B.Wilhelmy, R.C.Jared, S.G.Thompson Determination of the Charge and Mass Distribution in the Fission of 252Cf RADIOACTIVITY, Fission 252Cf; measured mass, charge distributions.
doi: 10.1103/PhysRevC.4.1913
1970CH11 Phys.Rev.Lett. 25, 38 (1970) E.Cheifetz, R.C.Jared, S.G.Thompson, J.B.Wilhelmy Experimental Information Concerning Deformation of Neutron Rich Nuclei In the A Approx. 100 Region RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(fragment)(X)-, (fragment)(fragment)(γ)-, γγ-, X(K)γ-coin. 96Sr, 100,102Zr, 102,104,106Mo, 108,110,112Ru, 112,114,116Pd; measured Eγ, Iγ; deduced levels, T1/2, B(E2).
doi: 10.1103/PhysRevLett.25.38
1970WA05 Nucl.Phys. A141, 449 (1970) R.L.Watson, J.B.Wilhelmy, R.C.Jared, C.Rugge, H.R.Bowman, S.G.Thompson, J.O.Rasmussen A Study of the Low-Energy Transitions Arising from the Prompt de-Excitation of Fission Fragments RADIOACTIVITY, Fission 252Cf(SF); measured E(ce), I(ce), E(X-ray), I(X-ray), I(ce)(t), (fragment)(fragment)(ce)(X)-coin. 102Zr, 106Mo, 108,109Tc, 110Ru, 116Rh, 140Cs, 144Ba, 146La, 148Ce, 149,150Pr; measured E(ce), I(ce); deduced Eγ, K/L, T1/2 (level). Detector - Si(Li), Si(P) fragment detectors.
doi: 10.1016/0375-9474(70)90982-6
1970WA12 Phys.Rev. C1, 1866 (1970) R.L.Watson, R.C.Jared, S.G.Thompson Distribution of K X-Rays as a Function of Mass and Atomic Number in the Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured (fission fragment)(K X-ray)-coin; deduced I(K X-ray)(A, Z).
doi: 10.1103/PhysRevC.1.1866
1970WI16 Phys.Rev.Lett. 25, 1122 (1970) J.B.Wilhelmy, S.G.Thompson, R.C.Jared, E.Cheifetz Ground-State Bands in Neutron-Rich Even Te, Xe, Ba, Ce, Nd, and Sm Isotopes Produced in the Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(fragment)(X)-, (fragment)(fragment)(X)(γ)-coin. 132,134Te, 138,140Xe, 140,142,144,146Ba, 144,146,148,150Ce, 152,154Nd, 156,158Sm; measured Eγ, Iγ; deduced levels, T1/2, B(E2).
doi: 10.1103/PhysRevLett.25.1122
1969MO39 Phys.Rev. 179, 1176 (1969) L.G.Moretto, R.C.Gatti, S.G.Thompson, J.T.Routti, J.H.Heisenberg, L.M.Middleman, M.R.Yearian, R.Hofstadter Electron- and Bremsstrahlung-Induced Fission of Heavy and Medium-Heavy Nuclei NUCLEAR REACTIONS 154Sm(γ, f), 209Bi(γ, f), E=49.8-421 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry L0090.
doi: 10.1103/PhysRev.179.1176
1966AS06 Priv.Comm., quoted by 1967LE24, unpublshed (1966) F.Asaro, M.C.Michel, S.G.Thompson, I.Perlman
1966WA01 Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.423 (1966) R.L.Watson, H.R.Bowman, S.G.Thompson, J.O.Rasmussen Internal Conversion Electrons from Primary Fission Fragments NUCLEAR STRUCTURE 252Cf; measured not abstracted; deduced nuclear properties.
1964AS08 Compt.Rend.Congr.Intern.Phys.Nucl., Paris, P.Gugenberger, Ed., Centre National de la Recherche Scientifique, Paris, Vol.II, p.564(1964) F.Asaro, M.C.Michel, S.G.Thompson, I.Perlman Coriolis Interactions in Odd-Odd Nuclei: Am242m Alpha Decay NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
1964BU15 Phys.Rev. 134, B952 (1964) D.S.Burnett, R.C.Gatti, F.Plasil, P.B.Price, W.J.Swiatecki, S.G.Thompson Fission Barrier of Thallium-201 NUCLEAR REACTIONS, Fission 197Au(α, F), E=25-40 MeV; measured σ(E;E(fragment)). 201Tl deduced fission barrier.
doi: 10.1103/PhysRev.134.B952
1964CO15 UCRL-11213, p. 20 (1964) J.A.Cooper, R.Gatti, J.O.Rasmussen, S.G.Thompson Antimony-131 Gamma Spectrum NUCLEAR STRUCTURE 131Sb; measured not abstracted; deduced nuclear properties.
1964CO30 J.Inorg.Nucl.Chem. 26, 2041 (1964) J.A.Cooper, R.C.Gatti, J.O.Rasmussen, S.G.Thompson γ-Ray Spectrum of Sb131 NUCLEAR STRUCTURE 131Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(64)80147-0
1964FR10 Phys.Rev.Lett. 13, 438 (1964) Properties of the Alpha Particles Emitted in the Spontaneous Fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products, Eα, Iα; deduced α particles kinetic energy, angular distributions.
doi: 10.1103/PhysRevLett.13.438
1963BO45 Phys.Rev. 129, 2133 (1963) H.R.Bowman, J.C.D.Milton, S.G.Thompson, W.J.Swiatecki Further Studies of the Prompt Neutrons from the Spontaneous Fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products, neutron and fission fragments TOF; deduced neutron density distributions, number of neutrons per fragment as a fragment mass, the average c.m. neutron and fragment kinetic energies, nuclear temperature. Comparison with available data and calculations.
doi: 10.1103/PhysRev.129.2133
1963BR35 Phys.Rev. 131, 2617 (1963) R.Brandt, S.G.Thompson, R.C.Gatti, L.Phillips Mass and Energy Distributions in the Spontaneous Fission of Some Heavy Isotopes RADIOACTIVITY 248Cm, 250,252,254Cf, 253Es, 254Fm(SF); measured decay products; deduced energy and mass distributions, fission-energy spectra, mass yields, total kinetic-energy distributions. Comparison with available data.
doi: 10.1103/PhysRev.131.2617
1963FR16 Can.J.Phys. 41, 2080 (1963) J.S.Fraser, J.C.D.Milton, H.R.Bowman, S.G.Thompson Precise kinetic energy measurements and fine structure in the spontaneous fission of Cf252 RADIOACTIVITY 252Cf(SF); measured decay products; deduced fission fragment kinetic energy spectra, energy, velocity, mass, mass ratio distributions, mass yields, mass-energy contours.
doi: 10.1139/p63-205
1963GA08 J.Inorg.Nucl.Chem. 25, 1089 (1963) R.C.Gatti, R.Brandt, L.Phillips, S.G.Thompson Discovery of a New Fermium Isotope NUCLEAR STRUCTURE 257Fm, 258Fm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(63)80126-8
1963PH01 J.Inorg.Nucl.Chem. 25, 1085 (1963) L.Phillips, R.C.Gatti, R.Brandt, S.G.Thompson Spontaneous Fission Half Lives of Cf254, Fm255, and Cf250 NUCLEAR STRUCTURE, Fission 250Cf, 255Fm, 254Cf, 254Es; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(63)80125-6
1962GA24 UCRL-18456 (1962); Nuclear Sci.Abstr. 17, 3200, Abstr.24404 (1963) R.C.Gatti, R.Brandt, L.Phillips, S.G.Thompson The Discovery of a New Fermium Isotope NUCLEAR STRUCTURE 257Fm, 258Fm; measured not abstracted; deduced nuclear properties.
1962GI05 Phys.Rev. 128, 2276 (1962) J.Gillmore, S.G.Thompson, I.Perlman Investigation of the Influence of Angular Momentum on Fission Probability
doi: 10.1103/PhysRev.128.2276
1962GI06 Phys.Rev. 128, 2276 (1962) J.Gillmore, S.G.Thompson, I.Perlman Investigation of the Influence of Angular Momentum on Fission Probability NUCLEAR REACTIONS 165Ho(20Ne, f), 165Ho(16O, f), 169Tm(12C, f), 169Tm(16O, f), 181Ta(20Ne, f), 181Ta(16O, f), 185Re(12C, f), 185Re(16O, f), 187Re(12C, f), 187Re(16O, f), E=79-211 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry C0725.
doi: 10.1103/PhysRev.128.2276
1962PH02 UCRL-10464 (1962); Nuclear Sci.Abstr. 17, 3201, Abstr.24405 (1963) L.Phillips, R.C.Gatti, R.Brandt, S.G.Thompson Spontaneous-Fission Half Lives of Cf254, Fm255, and Cf250 NUCLEAR STRUCTURE, Fission 250Cf, 255Fm, 254Cf, 254Es; measured not abstracted; deduced nuclear properties.
1961AS03 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press, Inc., New York, p.311 (1961) F.Asaro, M.C.Michel, S.G.Thompson, I.Perlman The Alpha Decay Scheme of 152 Year Am242m NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
1961AS04 UCRL-10023, p.22 (1961) F.Asaro, M.C.Michel, S.G.Thompson, I.Perlman NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
1961BR40 UCRL-10023, p.66 (1961) R.Brandt, R.C.Gatti, L.Phillips, S.G.Thompson Spontaneous Fission of Certain Californium, Einsteinium, and Fermium Isotopes NUCLEAR STRUCTURE 254Es, 255Fm; measured not abstracted; deduced nuclear properties.
1960AS05 Phys.Rev. 120, 934 (1960) F.Asaro, I.Perlman, J.O.Rasmussen, S.G.Thompson Isomers of Am242 NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.934
1960AS06 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Eds., Univ. Toronto Press, p. 581 (1960) F.Asaro, S.G.Thompson, F.S.Stephens, I.Perlman Decay Scheme of E253 NUCLEAR STRUCTURE 253Es; measured not abstracted; deduced nuclear properties.
1960AS08 UCRL-9382 (1960) F.Asaro, S.G.Thompson, F.S.Stephens, I.Perlman Decay Scheme of E253 NUCLEAR STRUCTURE 253Es; measured not abstracted; deduced nuclear properties.
1960DI03 Phys.Rev. 119, 2000 (1960) H.Diamond, P.R.Fields, C.S.Stevens, M.H.Studier, S.M.Fried, M.G.Inghram, D.C.Hess, G.L.Pyle, J.F.Mech, W.M.Manning, A.Ghiorso, S.G.Thompson, G.H.Higgins, G.T.Seaborg, C.I.Browne, H.L.Smith, and R.W.Spence Heavy Isotope Abundances in Mike Thermonuclear Device NUCLEAR REACTIONS 235,238U(n, γ)239U/240U/241U/242U/243U/244U/245U/246U/247U/248U/249U/250U/251U/252U/253U/254U/255U, E fast; measured reaction products mass spectrometrically and radiometrically; deduced isotopic abundances.
doi: 10.1103/PhysRev.119.2000
1959SI88 J.Inorg.Nuclear Chem. 11, 261 (1959) T.Sikkeland, S.Amiel, S.G.Thompson Spallation Reactions of Californium-252 with Helium Ions
doi: 10.1016/0022-1902(59)80039-7
1958AS64 UCRL-8369, p.27 (1958) F.Asaro, S.G.Thompson, F.S.Stephens, Jr., I.Perlman New Alpha Groups of Californium-250 and Californium-252
1958CH38 J.Inorg.Nucl.Chem. 7, 197 (1958) Electron Capture Half-Life of 243Cm
doi: 10.1016/0022-1902(58)80069-X
1957AM47 Phys.Rev. 106, 553 (1957) S.Amiel, A.Chetham-Strode, Jr., G.R.Choppin, A.Ghiorso, B.G.Harvey, L.W.Holm, S.G.Thompson Production and Properties of the Nuclides Fermium-250, 251, and 252
doi: 10.1103/PhysRev.106.553
1957AS70 Bull.Am.Phys.Soc. 2, No.8, 393 R1 (1957) F.Asaro, S.G.Thompson, F.S.Stephens, Jr., I.Perlman Alpha and Gamma Spectra of Cm243
1957AS83 Priv.Comm., quoted by 1964HY02 (1964) F.Asaro, S.G.Thompson, F.S.Stephens, Jr., I.Perlman
1957ST70 Bull.Am.Phys.Soc. 2, No.8, 394 R2 (1957) F.S.Stephens, Jr., F.Asaro, S.G.Thompson, I.Perlman Decay Scheme of Cf249
1956AS60 Priv.Comm., quoted by 1964HY02, unpublshed (1956) F.Asaro, F.S.Stephens, Jr., S.G.Thompson RADIOACTIVITY 250Bk; measured Eγ, Iγ, βγ-, γ(X-ray)-coin. 250Cf level deduced γ-decay characteristics, multipolarity.
1956FI11 Phys.Rev. 102, 180 (1956) P.R.Fields, M.H.Studier, H.Diamond, J.F.Mech, M.G.Inghram, G.L.Pyle, C.M.Stevens, S.Fried, W.M.Manning, A.Ghiorso, S.G.Thompson, G.H.Higgins, G.T.Seaborg Transplutonium Elements in Thermonuclear Test Debris
doi: 10.1103/PhysRev.102.180
1956HA80 Phys.Rev. 104, 1315 (1956) B.G.Harvey, A.Chetham-Strode, A.Ghiorso, G.R.Choppin, S.G.Thompson New Isotopes of Einsteinium
doi: 10.1103/PhysRev.104.1315
1955AS08 Phys.Rev. 98, 19 (1955) F.Asaro, F.S.Stephens, Jr., S.G.Thompson, I.Perlman Gamma Rays of 100254
doi: 10.1103/PhysRev.98.19
1955CH30 Phys.Rev. 98, 1519 (1955) G.R.Choppin, B.G.Harvey, S.G.Thompson, A.Ghiorso Nuclear Properties of 100256
doi: 10.1103/PhysRev.98.1519
1955GH01 Phys.Rev. 99, 1048 (1955) A.Ghiorso, S.G.Thompson, G.H.Higgins, G.T.Seaborg, M.H.Studier, P.R.Fields, S.M.Fried, H.Diamond, J.F.Mech, G.L.Pyle, J.R.Huizenga, A.Hirsch, W.M.Manning, C.I.Browne, H.L.Smith, R.W.Spence New Elements Einsteinium and Fermium, Atomic Numbers 99 and 100 RADIOACTIVITY 253Cf, 255Es(β-); measured decay products, Eα, Iα; deduced T1/2, element names.
doi: 10..1103/PhysRev.99.1048
1955GH02 Phys.Rev. 98, 1518 (1955) A.Ghiorso, B.G.Harvey, G.R.Choppin, S.G.Thompson, G.T.Seaborg New Element Mendelevium, Atomic Number 101 NUCLEAR REACTIONS 253Es(He, X)256Md, E=48 MeV; measured reaction products, Eα, Iα; deduced a new Z=101 element in recognition of the pioneering role of the great Russian chemist, Dmitri Mendeleev, who was the first to use the periodic system of the elements to predict the chemical properties of undiscovered elements, a principle which has been the key to the discovery of the last seven transuranium (actinide) elements. RADIOACTIVITY 256Md(α); measured decay products, Eα, Iα; deduced T1/2.
doi: 10.2172/914464
1955HA35 Phys.Rev. 99, 337 (1955) B.G.Harvey, S.G.Thompson, G.R.Choppin, A.Ghiorso Nuclide 99254
doi: 10.1103/PhysRev.99.337
1955HO67 Phys.Rev. 100, 1403 (1955) R.W.Hoff, H.Jaffe, T.O.Passell, F.S.Stephens, E.K.Hulet, S.G.Thompson Radioactive Decay of the Isomers of Americium-242
doi: 10.1103/PhysRev.100.1403
1954CH23 Phys.Rev. 94, 1080 (1954) G.R.Choppin, S.G.Thompson, A.Ghiorso, B.G.Harvey Nuclear Properties of Some Isotopes of Californium, Elements 99 and 100
doi: 10.1103/PhysRev.94.1080
1954GH12 Phys.Rev. 93, 257 (1954) A.Ghiorso, G.B.Rossi, B.G.Harvey, S.G.Thompson Reactions of U238 with Cyclotron-Produced Nitrogen Ions
doi: 10.1103/PhysRev.93.257
1954GH24 Phys.Rev. 94 1081 (1954) A.Ghiorso, S.G.Thompson, G.R.Choppin, B.G.Harvey New Isotopes of Americium, Berkelium and Californium
doi: 10.1103/PhysRev.94.1081
1954GH25 Phys.Rev. 95, 293 (1954) A.Ghiorso, S.G.Thompson, G.H.Higgins, B.G.Harvey, G.T.Seaborg Evidence for Subshell at N = 152 RADIOACTIVITY 244,246,248,249,250,252Cf, Pu, Am, Cm, Bk, Es, Fm(α); analyzed available data; deduced α-particle energy vs. mass number systematics, N=152 subshell.
doi: 10.1103/PhysRev.95.293
1954HA69 Phys.Rev. 95, 581 (1954) B.G.Harvey, H.P.Robinson, S.G.Thompson, A.Ghiorso, G.R.Choppin Some pile neutron cross sections of isotopes of americium, berkelium, californium, and element 99 NUCLEAR REACTIONS 243Am(n, γ), 249Bk, 249Cf(n, X), 249Cf(n, f), 249Cf(n, γ), 252Cf(n, γ), 254Cf(n, γ), 253Es(n, γ), 254Es(n, γ), E=0.0253 eV; measured products, 244Am, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12567.
doi: 10.1103/PhysRev.95.581
1954HA73 Phys.Rev. 93, 1129 (1954) B.G.Harvey, S.G.Thompson, A.Ghiorso, G.R.Choppin Further Production of Transcurium Nuclides by Neutron Irradiation RADIOACTIVITY 254Es, 253Cf(β-) [from 252Cf, 254Es(n, γ), E thermal]; measured decay products. 254Fm; deduced element 100. The Materials Testing Reactor (MTR).
doi: 10.1103/PhysRev.93.1129
1954HO72 Phys.Rev. 96, 1350 (1954) Orbital Electron Capture in the Heaviest Elements
doi: 10.1103/PhysRev.96.1350
1954HU50 Phys.Rev. 95, 1703 (1954) E.K.Hulet, S.G.Thompson, A.Ghiorso Isotopes of Curium, Berkelium, and Californium
doi: 10.1103/PhysRev.95.1703
1954HU58 Phys.Rev. 95, 1703 (1954) E.K.Hulet, S.G.Thompson, A.Ghiorso Isotopes of Curium, Berkelium, and Californium
doi: 10.1103/PhysRev.95.1703
1954TH01 Phys.Rev. 93, 908 (1954) S.G.Thompson, A.Ghiorso, B.G.Harvey, G.R.Choppin Transcurium Isotopes Produced in the Neutron Irradiation of Plutonium
doi: 10.1103/PhysRev.93.908
1953AS14 Phys.Rev. 92, 694 (1953) F.Asaro, S.G.Thompson, I.Perlman The Alpha Spectra of Cm242, Cm243, and Cm244
doi: 10.1103/PhysRev.92.694
1953HU85 Phys.Rev. 89, 878 (1953) E.K.Hulet, S.G.Thompson, A.Ghiorso Spontaneous Fission Rate of Cf246
doi: 10.1103/PhysRev.89.878
1953RA02 Phys.Rev. 89, 33 (1953) J.O.Rasmussen, Jr., S.G.Thompson, A.Ghiorso Alpha-Radioactivity in the 82-Neutron Region
doi: 10.1103/PhysRev.89.33
1952GH27 Phys.Rev. 87, 163 (1952) A.Ghiorso, G.H.Higgins, A.E.Larsh, G.T.Seaborg, S.G.Thompson Spontaneous Fission of U234, Pu236, Cm240, and Cm244
doi: 10.1103/PhysRev.87.163
1952ST70 Phys.Rev. 85, 135 (1952) K.Street Jr, A.Ghiorso, S.G.Thompson Slow Neutron Fission of Am242, Am242m, and Am243 NUCLEAR REACTIONS 241Am(n, γ), 242Am(n, f), 242Am(n, X), 242Am(n, γ), 243Am(n, f), E=0.0253 eV; measured products, 242Am, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12583.
doi: 10.1103/PhysRev.85.135.2
1951GH23 Phys.Rev. 81, 154 (1951) A.Ghiorso, S.G.Thompson, K.Street, Jr., G.T.Seaborg Californium Isotopes from Bombardment of Uranium with Carbon Ions NUCLEAR REACTIONS 238U(12C, 6n)244Cf, 238U(12C, 4n)246Cf, E not given; measured reaction products, Eα, Iα; deduced α-particles energies, T1/2, evidence for element Z=98 isotopes. Comparison with theoretical calculations.
doi: 10.1103/PhysRev.81.154
1951HO30 Phys.Rev. 83, 1068 (1951) R.W.Hoff, J.O.Rasmussen, S.G.Thompson Neutron Deficient Europium and Gadolinium Isotopes
doi: 10.1103/PhysRev.83.1068
1951HU39 Phys.Rev. 84, 366 (1951) E.K.Hulet, S.G.Thompson, A.Ghiorso, K.Street, Jr. New Isotopes of Berkelium and Californium RADIOACTIVITY 243,245Bk(EC), (α), 243,245Cm, 246Cf(α) [from 242,243,244Cm(d, X), E=16 MeV; 242,243,244Cm(3He, X), E=35 MeV]; measured decay products, Eβ, Iβ, Eα, Iα; deduced new isotopes T1/2. Comparison with available data. The pile facilities of the Atomic Energy Project, National Research Council of Canada, Chalk River, Ontario, Canada. The 60-inch cyclotron of the Crocker Laboratory.
doi: 10.1103/PhysRev.84.366.2
1951TH20 Phys.Rev. 84, 165 (1951) S.G.Thompson, K.Street, Jr., A.Ghiorso, F.L.Reynolds Properties of the Isotope Pu243
doi: 10.1103/PhysRev.84.165
1950MA14 Phys.Rev. 78, 363 (1950) L.B.Magnusson, S.G.Thompson, G.T.Seaborg New Isotope of Neptunium
doi: 10.1103/PhysRev.78.363
1950RA56 Phys.Rev. 80, 475 (1950) J.O.Rasmussen, F.L.Reynolds, S.G.Thompson, A.Ghiorso Mass Assignments of Alpha-Active Isotopes in the Rare Earth Region
doi: 10.1103/PhysRev.80.475
1950TH52 Phys.Rev. 80, 781 (1950) S.G.Thompson, A.Ghiorso, G.T.Seaborg The New Element Berkelium (Atomic Number 97)
doi: 10.1103/PhysRev.80.781
1950TH54 Phys.Rev. 80, 1108 (1950) S.G.Thompson, K.Street, Jr., A.Ghiorso, F.L.Reynolds The New Isotope Pu242 and Additional Information on Other Plutonium Isotopes
doi: 10.1103/PhysRev.80.1108
1950TH55 Phys.Rev. 77, 838 (1950) S.G.Thompson, A.Ghiorso, G.T.Seaborg Element 97 NUCLEAR REACTIONS 241Am(α, X)243Bk/244Bk, E not given; measured reaction products, Eα, Iα; deduced α-particles energies, evidence for element Z=97.
doi: 10.1103/PhysRev.77.838.2
1950TH56 Phys.Rev. 78, 298 (1950) S.G.Thompson, K.Street, Jr., A.Ghiorso, G.T.Seaborg Element 98 NUCLEAR REACTIONS 242Cm(α, X)244Cf, E=35 MeV; measured reaction products, Eα, Iα; deduced α-particles energies, evidence for element Z=98.
doi: 10.1103/PhysRev.78.298.2
1950TH57 Phys.Rev. 80, 790 (1950) S.G.Thompson, K.Street, Jr., A.Ghiorso, G.T.Seaborg The New Element Californium (Atomic Number 98) NUCLEAR REACTIONS 242Cm(α, X)244Cf, E=35 MeV; measured reaction products, Eα, Iα; deduced α-particles energies, T1/2, evidence for element Z=98.
doi: 10.1103/PhysRev.80.790
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