NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = J.E.Gindler Found 53 matches. 1994AH03 Nucl.Phys. A576, 246 (1994) I.Ahmad, J.E.Gindler, M.P.Carpenter, D.J.Henderson, E.F.Moore, R.V.F.Janssens, I.G.Bearden, C.C.Foster Level Structure of the Odd-Odd Nucleus 22489Ac RADIOACTIVITY 228Pa(α) [from 232Th(p, 5n)]; measured Eα, Iα, Eγ, Iγ, I(ce), αγ-, αγγ-, α(ce)-coin. 224Ac deduced levels, J, π, ICC, γ-multipolarity.
doi: 10.1016/0375-9474(94)90259-3
1987AH05 Nucl.Phys. A472, 285 (1987) I.Ahmad, J.E.Gindler, A.M.Friedman, R.R.Chasman, T.Ishii Level Structure of 225Ac RADIOACTIVITY 229Pa(α) [from 229Th(d, 2n), 230Th(d, 3n)]; measured Eγ, Iγ, I(ce), αγ-, γγ-coin. 225Ra(β-) [from 229Th α-decay]; measured Eγ, Iγ. 225Ac deduced levels, J, π.
doi: 10.1016/0375-9474(87)90211-9
1985BA29 Phys.Rev. C32, 195 (1985); Erratum Phys.Rev. C33, 385 (1986) B.B.Back, R.R.Betts, J.E.Gindler, B.D.Wilkins, S.Saini, M.B.Tsang, C.K.Gelbke, W.G.Lynch, M.A.McMahan, P.A.Baisden Angular Distributions in Heavy-Ion-Induced Fission NUCLEAR REACTIONS, ICPND 208Pb, 232Th, 238U, 248Cm(16O, F), E=85-148 MeV; 208Pb(19F, F), E=110-190 MeV; 208Pb(24Mg, F), E=140-210 MeV; 208Pb(28Si, F), E=160-260 MeV; 197Au(32S, F), E=185-255 MeV; 208Pb(32S, F), E=180-266 MeV; measured total fission σ(E), σ(θ) vs E. Standard fission theory analysis.
doi: 10.1103/PhysRevC.32.195
1985IS03 Nucl.Phys. A444, 237 (1985) T.Ishii, I.Ahmad, J.E.Gindler, A.M.Friedman, R.R.Chasman, S.B.Kaufman Measurement of Rates of Fast E1 Transitions in Ac-Ra Nuclei RADIOACTIVITY 225Ra(β-); 229Th, 231Pa(α); measured γγ(t), αγ(t). 225Ra levels deduced T1/2, quadrupole moment, B(λ), α-branching ratio. 225,227Ac deduced T1/2, B(λ).
doi: 10.1016/0375-9474(85)90348-3
1985KU24 Phys.Rev. C32, 2036 (1985) W.Kutschera, I.Ahmad, S.G.Armato III, A.M.Friedman, J.E.Gindler, W.Henning, T.Ishii, M.Paul, K.E.Rehm Spontaneous 14C Emission from 223Ra RADIOACTIVITY 223Ra(14C), (α) [from 227Th decay]; measured 14C(SF-decay), (14C)/α branching ratio. Enge split-pole magnetic spectrograph.
doi: 10.1103/PhysRevC.32.2036
1984AH01 Phys.Rev.Lett. 52, 503 (1984) I.Ahmad, R.R.Chasman, J.E.Gindler, A.M.Friedman Enhanced E1 Transition Rates and Octupole Deformation in 225Ac RADIOACTIVITY 229Pa(α); 225Ra(β-); measured I(K X-ray), Iγ, ratio. 225Ra level deduced J, π. 225Ac levels deduced J, π, γ-branching, γ-multipolarity, enhanced B(E1), parity doublet rotational band characteristics.
doi: 10.1103/PhysRevLett.52.503
1984BA01 Phys.Rev.Lett. 52, 397 (1984) B.B.Back, R.R.Betts, K.Cassidy, B.G.Glagola, J.E.Gindler, L.E.Glendenin, B.D.Wilkins Fission Anisotropies and Sequential Fission: A Response NUCLEAR REACTIONS 208Pb, 238U(16O, X), E=80-180 MeV; calculated fission σ(E); deduced sharp cut-off model validity.
doi: 10.1103/PhysRevLett.52.397
1984WI13 Phys.Rev. C30, 1228 (1984) B.D.Wilkins, B.B.Back, J.E.Gindler, B.G.Glagola, K.Kwiatkowski, S.H.Zhou, V.E.Viola, Jr. Mass and Kinetic Energy Distributions in Near-Barrier Fission of 182W NUCLEAR REACTIONS, ICPND 178Hf(α, F), E=49.2 MeV; measured fission fragment yields, total kinetic energy release vs fragment mass; deduced no shell effects. 182W deduced fission characteristics.
doi: 10.1103/PhysRevC.30.1228
1983AH02 Phys.Rev. C27, 2239 (1983) Electron Capture Decay of 237Pu, 235Np and 236Np RADIOACTIVITY 237Pu(EC), (α) [from 235U(α, 2n), E=31 MeV]; 235Np(EC), (α) [from 235U(d, 2n), E=18 MeV]; 236Np(EC), (β-) [from 238U(d, 4n), E=21 MeV]; measured Eγ, Iγ, I(ce), I X-ray; deduced log ft(EC), log ft(β-). 237Np, 236U, 236Pu deduced levels, J, π, γ-multipolarity. Cooled Si(Li) electron spectrometer, mass separated 237Pu.
doi: 10.1103/PhysRevC.27.2239
1983BA07 Phys.Rev.Lett. 50, 818 (1983) B.B.Back, R.R.Betts, K.Cassidy, B.G.Glagola, J.E.Gindler, L.E.Glendenin, B.D.Wilkins Experimental Signatures of Quasifission Reactions NUCLEAR REACTIONS 238U(16O, F), E=90, 110, 130, 148 MeV; 208Pb(32S, F), E=185, 198, 205, 219, 225 MeV; measured fission fragment σ(θ), absolute total fission σ; deduced quasifission mechanism, rigid to effective moment of inertia ratio. Optical, extra push model analyses.
doi: 10.1103/PhysRevLett.50.818
1983GI05 Phys.Rev. C27, 2058 (1983) J.E.Gindler, L.E.Glendenin, D.J.Henderson, J.W.Meadows Mass Distributions in Monoenergetic-Neutron-Induced Fission of 239Pu NUCLEAR REACTIONS 239Pu(n, F)87Kr/88Kr/91Sr/92Sr/93Y/97Zr/99Mo/103Ru/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb/129Sb/132Te/134Te/133I/134I/135I/135Xe/140Ba/142La/143Ce, E=0.17-7.9 MeV; measured fission fragment yield vs mass, σ(fission) vs E. Activation technique.
doi: 10.1103/PhysRevC.27.2058
1982AH08 Phys.Rev.Lett. 49, 1758 (1982) I.Ahmad, J.E.Gindler, R.R.Betts, R.R.Chasman, A.M.Friedman Possible Ground-State Octupole Deformation in 229Pa RADIOACTIVITY 229Pa(EC), 229U(EC) [from mass separation]; measured I(ce), Eγ, Iγ, γγ-, γ(X-ray)-, (ce)(X-ray)-coin. 229Pa deduced levels, J, π, K, γ-multipolarity, ground state doublet splitting, Nilsson assignment. NUCLEAR REACTIONS 231Pa(p, t), E=16.5 MeV; measured σ(Et). 229Pa deduced levels, J, π, possible octupole deformation, Nilsson assignment, K.
doi: 10.1103/PhysRevLett.49.1758
1981GI02 J.Inorg.Nucl.Chem. 43, 895 (1981) J.E.Gindler, D.J.Henderson, L.E.Glendenin Spontaneous Fission Yields for 246Cm RADIOACTIVITY, Fission 246Cm(SF); measured Eγ, Iγ; deduced cumulative yields for 95,97Zr, 99Mo, 103,105Ru, 111,112Ag, 131,133,135I, 132Te, 140Ba, 141,143,144Ce, 142La, 147Nd.
doi: 10.1016/0022-1902(81)80145-5
1981GI05 J.Inorg.Nucl.Chem. 43, 1433 (1981) J.E.Gindler, L.E.Glendenin, D.J.Henderson Mass Distribution for Thermal-Neutron-Induced Fission of 229Th NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; measured yields for 77,78As, 83Se, 85m,87,88Kr, 84Br, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 115Cd, 111Ag, 121,125Sn, 127,129Sb, 132,134Te, 131,133,135I, 140Ba, 141,143,144Ce, 142La, 147,149Nd. Activation technique.
doi: 10.1016/0022-1902(81)80313-2
1981GI06 J.Inorg.Nucl.Chem. 43, 1743 (1981) J.E.Gindler, L.E.Glendenin, D.J.Henderson Mass Distributions for the Fission of 250Cf NUCLEAR REACTIONS, Fission 249Cf(n, F), E=thermal; measured yields for 85m,88Kr, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 111Ag, 115,115m,117Cd, 121,123,125Sn, 127,129Sb, 131,133,134,135I, 132,134Te, 135Xe, 136,137Cs, 139,140Ba, 141,143,144Ce, 142La, 147,149Nd, 151Pm, 153,155,156Sm, 157Eu; deduced mass distribution characteristics. Activation technique. RADIOACTIVITY, Fission 250Cf(SF); measured yields for 101,104Tc, 105Ru, 107Rh, 133I, 139Ba, 142La; deduced heavy, light fragment mean mass.
doi: 10.1016/0022-1902(81)80376-4
1981GI18 J.Inorg.Nucl.Chem. 43, 445 (1981) J.E.Gindler, L.E.Glendenin, E.L.Krapp, S.J.Fernandez, K.F.Flynn, D.J.Henderson Mass distribution in thermal-neutron-induced fission of long-lived 236Np NUCLEAR REACTIONS 236Np(n, F)84Br/85Kr/87Kr/88Kr/91Sr/92Sr/93Y/95Zr/97Zr/99Mo/103Ru/104Tc/105Ru/104Tc/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb, E thermal; measured fission products, Eγ, Iγ; deduced fission yields.
doi: 10.1016/0022-1902(81)80481-2
1981GI19 Trans.Amer.Nucl.Soc. 39, 877 (1981) J.E.Gindler, L.E.Glendenin, D.J.Henderson, J.W.Meadows Neutron-Induced Fission Yields of 235U from 0.17 to 8.1 MeV NUCLEAR REACTIONS 235U(n, F)84Br/85Kr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/103Ru/105Ru/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/127Sb/129Sb/131I/132Te/133I/134Te/134I/135Xe/138Xe/139Ba/140Ba/141Ce/142La/143Ce/144Ce/147Nd/149Pm/151Pm, E=0.17-8.1 MeV; measured fission products, Eγ, Iγ, Eβ, Iβ; deduced yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12729. 1981GL04 Phys.Rev. C24, 2600 (1981) L.E.Glendenin, J.E.Gindler, D.J.Henderson, J.W.Meadows Mass Distributions for Monoenergetic-Neutron-Induced Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=0.17, 0.55, 1, 2, 4, 5.5, 6.3, 7.1, 8.1 MeV; measured yields vs E for 84Br, 85m,87,88Kr, 89Rb, 91,92Sr, 93,94Y, 95,97Zr, 99Mo, 103,105Ru, 109,112Pd, 111Ag, 115Cd, 121,125Sn, 127,129Sb, 131,133,134,135I, 135,138Xe, 139,140Ba, 141,143,144Ce, 142La, 141,143,144Ce, 147Nd, 149,151Pm; deduced second-chance fission characteristics. Activation techniques.
doi: 10.1103/PhysRevC.24.2600
1980GL05 Phys.Rev. C22, 152 (1980) L.E.Glendenin, J.E.Gindler, I.Ahmad, D.J.Henderson, J.W.Meadows Mass Distributions in Monoenergetic-Neutron-Induced Fission of 232Th NUCLEAR REACTIONS 232Th(n, F), E=2, 3, 4, 5.9, 6.4, 6.9, 7.6, 8 MeV; measured Eγ, Iγ, Iβ; deduced production σ for 77,78Se, 84Br, 85,87,88Kr, 88,89Rb, 91,92,93Sr, 91,93,94Y, 97Zr, 97Nb, 99Mo, 99,101Tc, 103,105Ru, 109,112Pd, 111Ag, 115Cd, 121Sn, 127,129Sb, 131,133,135I, 132,134Te, 135,138Xe, 138Cs, 139,140,141Ba, 140,142La, 141,143,146Ce, 147,149Nd.
doi: 10.1103/PhysRevC.22.152
1979GI06 Nucl.Sci.Eng. 70, 101 (1979) J.E.Gindler, L.E.Glendenin, J.W.Meadows, Jr., K.F.Flynn Fission Yields for Fast-Neutron Fission of Uranium-238 NUCLEAR REACTIONS 238U(n, F), E=1.5-7.7 MeV; measured nothing; calculated fission yields in 238U exposed to watt neutron spectrum. Results compared with available compilations for fast fission yields.
doi: 10.13182/NSE79-A18933
1978NA01 Phys.Rev. C17, 163 (1978) S.Nagy, K.F.Flynn, J.E.Gindler, J.W.Meadows, L.E.Glendenin Mass Distributions in Monoenergetic-Neutron-Induced Fission of 238U NUCLEAR REACTIONS 238U(n, F), E=1.5, 2.0, 3.9, 5.5, 6.9, 7.7 MeV; measured mass yields.
doi: 10.1103/PhysRevC.17.163
1977FL07 J.Inorg.Nucl.Chem. 39, 759 (1977) K.F.Flynn, J.E.Gindler, L.E.Glendenin Mass Distributions for the Spontaneous Fission of 248Cm and 250Cf RADIOACTIVITY, Fission 248Cm(SF), 250Cf(SF); measured mass distribution fission yield.
doi: 10.1016/0022-1902(77)80149-8
1977GI11 Inorg.Nucl.Chem.Lett. 13, 95 (1977) The Half-Lives of 109Pd and 112Pd RADIOACTIVITY 109,112Pd; measured T1/2.
doi: 10.1016/0020-1650(77)80061-5
1977GI15 Phys.Rev. C16, 1483 (1977) J.E.Gindler, K.F.Flynn, L.E.Glendenin, R.K.Sjoblom Distribution of Mass, Kinetic Energy, and Neutron Yield in the Spontaneous Fission of 254Fm RADIOACTIVITY, Fission 254Fm(SF); measured radiochemical mass yields, fragment energy; deduced neutron yields, σ(A, E(fragment)).
doi: 10.1103/PhysRevC.16.1483
1976FL03 J.Inorg.Nucl.Chem. 38, 661 (1976) K.F.Flynn, J.E.Gindler, L.E.Glendenin, R.K.Sjoblom Mass Distributions for the Spontaneous Fission of 253Es and the Thermal-Neutron-Induced Fission of 254Es RADIOACTIVITY, Fission 253Es(SF); measured mass yield. NUCLEAR REACTIONS 254Es(n, F), E=thermal; measured mass yield.
doi: 10.1016/0022-1902(76)80333-8
1976GI14 Inorg.Nucl.Chem.Lett. 12, 931 (1976) The Half-Lives of 83Rb and 84Rb RADIOACTIVITY 83,84Rb; measured T1/2.
doi: 10.1016/0020-1650(76)80011-6
1975FL04 J.Inorg.Nucl.Chem. 37, 881 (1975) K.F.Flynn, J.E.Gindler, L.E.Glendenin The Mass Distribution for Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured fission yields for 35 mass chains.
doi: 10.1016/0022-1902(75)80666-X
1975FL06 Phys.Rev. C11, 1676 (1975) K.F.Flynn, J.E.Gindler, R.K.Sjoblom, L.E.Glendenin Mass Distributions for Thermal-Neutron-Induced Fission of 255Fm and 251Cf NUCLEAR REACTIONS 251Cf, 255Fm(n, F), E=0.025 eV; measured radiochemical mass yields, σ.
doi: 10.1103/PhysRevC.11.1676
1975FL09 Phys.Rev. C12, 1478 (1975) K.F.Flynn, J.E.Gindler, L.E.Glendenin Distribution of Mass in Thermal-Neutron-Induced Fission of 257Fm NUCLEAR REACTIONS 257Fm(n, F), E=0.025 eV; measured radiochemical mass yields.
doi: 10.1103/PhysRevC.12.1478
1975FL10 Trans.Amer.Nucl.Soc. 22, 677 (1975) K.F.Flynn, S.Nagy, L.E.Glendenin, J.E.Gindler, J.W.Meadows Monoenergetic Neutron Fission of 238U NUCLEAR REACTIONS 238U(n, F)83Br/85Kr/87Kr/88Kr/89Rb/89Sr/91Y/92Sr/93Y/94Y/95Zr/97Zr/99Mo/101Mo/103Ru/105Ru/106Ru/107Rh/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/131I/132Te/133I/135I/138Xe/139Ba/140Ba/141Ce/142La/143Ce/144Ce/146Ce/147Nd/149Nd/149Pm/151Pm/153Sm/156Eu, E=2, 8 MeV; measured reaction products, Eγ, Iγ; deduced fission product yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10798. 1974GE06 J.Phys.(Paris) 35, 483 (1974) S.Gerstenkorn, P.Luc, J.Verges, D.W.Engelkemeir, J.E.Gindler, F.S.Tomkins Structures Hyperfines du Spectre d'Etincelle, Moment Magnetique et Quadrupolaire de l'Isotope 229 du Thorium NUCLEAR MOMENTS 229Th; measured μ, quadrupole moment. Optical spectroscopy.
doi: 10.1051/jphys:01974003506048300
1973GI06 J.Inorg.Nucl.Chem. 35, 2617 (1973) J.E.Gindler, K.F.Flynn, L.E.Glendenin The Half-Life of 132Cs RADIOACTIVITY 132Cs; measured T1/2.
doi: 10.1016/0022-1902(73)80490-7
1972EN06 J.Inorg.Nucl.Chem. 34, 1799 (1972) The Negatron Half-Life of the Long-Lived 236Np Isomer RADIOACTIVITY 236mNp; measured T1/2.
doi: 10.1016/0022-1902(72)80525-6
1970AU01 J.Inorg.Nucl.Chem. 32, 731 (1970) The Ratio of 111Pd Isomers Formed in Charged-Particle and Photon-Induced Fission of Several Heavy Nuclides NUCLEAR REACTIONS, Fission 230,232Th, 236U(α, F), E=24-45 MeV; 232Th, 233,234,235,236,238U(γ, F), E < 17 MeV; measured 110Ag activity. 111Pd deduced isomeric σ ratio.
doi: 10.1016/0022-1902(70)80055-0
1969AU02 J.Inorg.Nucl.Chem. 31, 1935 (1969) D.C.Aumann, K.F.Flynn, J.E.Gindler, L.E.Glendenin Formation of 111Pd isomers in neutron fission of several heavy nuclides NUCLEAR REACTIONS, Fission 232Th, 233,235,238U(n, F), E= thermal; measured 111Pd isomer yield ratios. 111Rh deduced β-branching.
doi: 10.1016/0022-1902(69)90008-6
1968CO28 Phys.Rev. 176, 1421(1968) R.E.Cote, H.Diamond, J.E.Gindler, H.Shwe Neutron Resonances of Th230 NUCLEAR REACTIONS 230Th(n, X), E = 0.05-500 eV; measured σ(E). 230Th deduced T1/2. 231Th deduced resonances, level-width.
doi: 10.1103/PhysRev.176.1421
1966CO21 WASH-1068, p.17 (1966); and Priv.Comm. (1966) R.E.Cote, H.Diamond, J.E.Gindler The Neutron Resonances of Th230 NUCLEAR STRUCTURE 231Th; measured not abstracted; deduced nuclear properties.
1964GI07 Phys.Rev. 136, B1333 (1964) J.E.Gindler, G.L.Bate, J.R.Huizenga Fission Fragment Angular Distributions in Charged- Particle-Induced Fission of Ra226 NUCLEAR REACTIONS 226Ra(α, f), 226Ra(d, f), 226Ra(p, f), E=-1.0 eV-43 MeV; measured products; deduced σ(θ), σ, σ(E). Data were imported from EXFOR entry C0714.
doi: 10.1103/PhysRev.136.B1333
1963DI05 J.Inorg.Nucl.Chem. 25, 143 (1963) Alpha Half-Lives of 216Po, 217At and 218Rn NUCLEAR STRUCTURE 217At, 218Rn, 216Po; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(63)80001-9
1963GI17 Radiochim.Acta 2, 58 (1963) Half-Life Determination of 220Rn NUCLEAR STRUCTURE 220Rn; measured not abstracted; deduced nuclear properties.
1962DI08 TID-16202 (1962); Nucl.Sci.Abstr. 17, 1511, Abstr.11632 (1963) Alpha Half-Lives of Po216, At217 and Rn218 NUCLEAR STRUCTURE 218Rn, 217At, 216Po; measured not abstracted; deduced nuclear properties.
1962HU14 Nucl.Phys. 34, 439 (1962) J.R.Huizenga, K.M.Clarke, J.E.Gindler, R.Vandenbosch Photofission Cross Sections Of Several Nuclei With Mono-Energetic Gamma Rays NUCLEAR REACTIONS 232Th(γ, f), 233U(γ, f), 234U(γ, f), 235U(γ, f), 236U(γ, f), 238U(γ, f), 237Np(γ, f), E=6.1-7 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry M0505.
doi: 10.1016/0029-5582(62)90231-6
1961CO16 Bull.Am.Phys.Soc. 6, No.5, 417, C1 (1961) R.E.Cote, H.Diamond, J.E.Gindler Total Neutron Cross Section of Th229 NUCLEAR STRUCTURE 229Th; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12298. 1960GI03 Phys.Rev. 119, 1645 (1960) Alpha Decay of Np235 NUCLEAR STRUCTURE 235Np; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.119.1645
1960GI04 J.Inorg.Nuclear Chem. 15, 1 (1960) J.E.Gindler, K.F.Flynn, J.Gray, Jr. Thermal Neutron Fission Cross-Section of 229Th NUCLEAR STRUCTURE 229Th; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(60)80002-4
1959GI54 Phys.Rev. 115, 1271 (1959) J.E.Gindler, J.Gray, Jr., J.R.Huizenga Neutron Fission Cross Sections of Pu236 and Pu237
doi: 10.1103/PhysRev.115.1271
1959GI58 J.Inorg.Nuclear Chem. 12, 8 (1959) Electron-Capture/Negatron-Emission Branching Ratio of 236Np (22 hr)
doi: 10.1016/0022-1902(59)80086-5
1958GI05 Phys.Rev. 109, 1263 (1958) J.E.Gindler, J.R.Huizenga, D.W.Engelkemeir Neptunium Isotopes: 234, 235, 236
doi: 10.1103/PhysRev.109.1263
1956FR07 Phys.Rev. 102, 585 (1956) A.M.Friedman, J.E.Gindler, R.F.Barnes, R.Sjoblom, P.R.Fields Properties of Fm252
doi: 10.1103/PhysRev.102.585
1956HU28 Bull.Am.Phys.Soc. 1, No.4, 171, E7 (1956) J.R.Huizenga, D.W.Engelkemeir, M.S.Freedman, F.T.Porter, J.E.Gindler Radiations of Np234
1955BE99 Proc.Int.Conf.Peaceful Uses Atomic Energy, Geneva (1955), United Nations Publ., Vol.7, p.261 (1956) W.C.Bentley, H.Diamond, P.R.Fields, A.M.Friedman, J.E.Gindler, D.C.Hess, J.R.Huizenga, M.G.Inghram, A.H.Jaffey, L.B.Magnusson, W.M.Manning, J.F.Mech, G.L.Pyle, R.Sjoblom, C.M.Stevens, M.H.Studier The Formation of Higher Isotopes and Higher Elements by Reactor Irradiation of Pu239; Some Nuclear Properties of the Heavier Isotopes
1955FI36 Phys.Rev. 100, 172 (1955) P.R.Fields, J.E.Gindler, A.L.Harkness, M.H.Studier, J.R.Huizenga, A.M.Friedman Electron Capture Decay of Am244 and the Spontaneous Fission Half-Life Of Pu244
doi: 10.1103/PhysRev.100.172
1955ST10 Phys.Rev. 97, 88 (1955) M.H.Studier, J.E.Gindler, C.M.Stevens Long-Lived Isomer of Np236
doi: 10.1103/PhysRev.97.88
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