NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = C.E.Bemis Found 64 matches. 1992ZH42 Rev.Mex.Fis. 38, 53 (1992) S.Zhu, X.Zhao, J.H.Hamilton, A.V.Ramayya, Q.Lu, W.-C.Ma, L.K.Peker, J.Kormicki, H.Xie, W.B.Gao, J.K.Deng, I.Y.Lee, N.R.Johnson, F.K.McGowan, C.E.Bemis, J.D.Cole, R.Aryaeinejad, G.M.Ter-Akopian, Yu.Ts.Oganessian Higher Spin States in Neutron Rich Nuclei
1988BE21 Phys.Rev. C38, 569 (1988) J.R.Beene, C.E.Bemis, Jr., M.L.Halbert Possibility of Pions Emitted in the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured fission fragment(γ)(γ)-coin; deduced π0 decay branching limit. 4π NaI(Tl) detectors, enriched source.
doi: 10.1103/PhysRevC.38.569
1988BE41 Phys.Scr. 38, 657 (1988) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson, G.A.Leander, C.W.Reich Coulomb Excitation of States in 229Th NUCLEAR REACTIONS 229Th(α, α), (α, α'), E=17 MeV; measured σ(Eα), σ(Eα') following Coulomb excitation. 229Th levels deduced excitation probability, B(E2), intrinsic quadrupole, hexadecapole moments, J, π, K, Nilsson assignments.
doi: 10.1088/0031-8949/38/5/004
1986ZU01 Phys.Lett. 167B, 383 (1986) J.D.Zumbro, R.A.Naumann, M.V.Hoehn, W.Reuter, E.B.Shera, C.E.Bemis, Jr., Y.Tanaka E2 and E4 Deformations in 232Th and 239,240,242Pu NUCLEAR MOMENTS 232Th, 239,240,242Pu; measured muonic X-ray data; deduced quadrupole, hexadecapole moments, charge parameters, rms radii. 239Pu deduced E2 martix elements. Adiabatic rotation model. ATOMIC PHYSICS, Mesic-Atoms 232Th, 239,240,242Pu; measured muonic X-ray data.
doi: 10.1016/0370-2693(86)91285-2
1985BE58 Hyperfine Interactions 24, 139 (1985) Laser Optical Pumping in Nuclear Physics: Fission isomers, oriented targets, and hyperfine pumping in single-electron atoms RADIOACTIVITY 240mAm(SF); measured optical isomer shift. Oriented targets, anisotropic fission decay from resonant laser optical pumping.
doi: 10.1007/BF02354808
1985JO04 Phys.Lett. 161B, 75 (1985) M.W.Johnson, E.B.Shera, M.V.Hoehn, R.A.Naumann, J.D.Zumbro, C.E.Bemis, Jr. 241Am and 243Am Charge Distributions from Muonic X-Ray Spectroscopy and the Quadrupole Moment of the 240Am Fission Isomer NUCLEAR REACTIONS 241,243Am(μ-, X), E at rest; measured muonic E X-ray, I X-ray. 241,243Am deduced intrinsic quadrupole moment, Barrett radii. 240Am deduced fission isomer quadrupole moment. Optical isotope shift data input. ATOMIC PHYSICS, Mesic-Atoms 241,243Am(μ, X), E at rest; measured muonic X-rays.
doi: 10.1016/0370-2693(85)90612-4
1984ZU02 Phys.Rev.Lett. 53, 1888 (1984) J.D.Zumbro, E.B.Shera, Y.Tanaka, C.E.Bemis, Jr., R.A.Naumann, M.V.Hoehn, W.Reuter, R.M.Steffen E2 and E4 Deformations in 233,234,235,238U NUCLEAR MOMENTS 233,234,235,238U; measured muonic X-rays. 234,238U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, rms radii. 233,235U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, B(E2). ATOMIC PHYSICS, Mesic-Atoms 233,234,235,238U; measured muonic X-rays.
doi: 10.1103/PhysRevLett.53.1888
1983DA06 Nucl.Sci.Eng. 84, 1 (1983); Corrigendum Nucl.Sci.Eng. 85, 81 (1983) J.W.T.Dabbs, C.E.Bemis, Jr., S.Raman, R.J.Dougan, R.W.Hoff Measurement of the 242mAm Neutron Fission Cross Section NUCLEAR REACTIONS 242mAm(n, F), E=0.000005-20 MeV; measured fission σ(E); deduced fission resonance integral. Tof.
doi: 10.13182/NSE83-A17453
1983DA07 Nucl.Sci.Eng. 83, 22 (1983) J.W.T.Dabbs, C.H.Johnson, C.E.Bemis, Jr. Measurement of the 241Am Neutron Fission Cross Section NUCLEAR REACTIONS 241Am(n, F), E=0.00002-20 MeV; measured fission σ(E); deduced fission resonance integral.
doi: 10.13182/NSE83-A17986
1982BE12 Phys.Rev. C25, 1637 (1982) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of Ground Band Rotational States in 249Bk NUCLEAR REACTIONS 249Bk(α, α), (α, α'), E=17.06 MeV; measured σ(Eα, θ=150°). 249Bk levels deduced B(E2), B(M1), quadrupole moment, μ. Enriched target.
doi: 10.1103/PhysRevC.25.1637
1981BE03 Phys.Rev. C23, 555 (1981) C.E.Bemis, Jr., P.F.Dittner, R.L.Ferguson, D.C.Hensley, F.Plasil, F.Pleasonton Spontaneous-Fission Branching in the Decay of 259104 RADIOACTIVITY, Fission 259Rf(SF) [from 249Cf(13C, 3n), E=86.5 MeV]; measured T1/2(SF), Eα, Iα; deduced α-decay to SF-decay branching ratio. Enriched target. NUCLEAR REACTIONS 249Cf(13C, 3n), (13C, xnyp), E=86.5 MeV; measured production σ for 259Rf, 256No.
doi: 10.1103/PhysRevC.23.555
1981BE06 Phys.Lett. 99B, 213 (1981) F.E.Bertrand, J.R.Beene, C.E.Bemis, Jr., E.E.Gross, D.J.Horen, J.R.Wu, W.P.Jones Measurement of the Fission Decay of the Giant Quadrupole Resonance in 238U NUCLEAR REACTIONS, Fission 238U(α, α'F), E=152 MeV; measured σ(Eα', θ), α(fragment)-coin, fission probability vs excitation energy. 238U deduced Γf/Γ for GQR, possible K conservation.
doi: 10.1016/0370-2693(81)91110-2
1981BE48 Hyperfine Interactions 9, 143 (1981) J.R.Beene, C.E.Bemis, Jr., J.P.Young, S.D.Kramer Study of the Fission Isomer 240mAm(S.F.) using Laser-Induced Nuclear Polarization RADIOACTIVITY, Fission 240mAm(SF) [from 238U(7Li, 5n), E=49 MeV]; measured optical isomer shift; deduced quadrupole moment. Laser induced nuclear polarization, optical pumping.
doi: 10.1007/BF01020910
1981BE54 Phys.Rev. C24, 2723 (1981) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of Rotational States and Ground-State Quadrupole Moment for 243Am NUCLEAR REACTIONS 243Am(α, α'), E=17 MeV; measured σ(Eα', θ=150°), Coulomb excitation. 243Am levels deduced B(E2), B(E4), quadrupole moment. Enriched target.
doi: 10.1103/PhysRevC.24.2723
1981NI01 Nucl.Phys. A352, 138 (1981) J.M.Nitschke, M.Fowler, A.Ghiorso, R.E.Leber, M.E.Leino, M.J.Nurmia, L.P.Somerville, K.E.Williams, E.K.Hulet, J.H.Landrum, R.W.Lougheed, J.F.Wild, C.E.Bemis, Jr., R.J.Silva, P.Eskola Search for an 80 ms Spontaneous Fission Activity in Bombardments of 249Bk with 15N NUCLEAR REACTIONS, Fission 249Bk(15N, X), E=78, 82, 86, 88, 100 MeV; measured σ(E), spontaneous fission T1/2. 260Rf deduced no evidence for 80 ms spontaneous fission decay.
doi: 10.1016/0375-9474(81)90564-9
1981RO09 Phys.Rev.Lett. 47, 635 (1981) R.M.Ronningen, R.C.Melin, J.A.Nolen, Jr., G.M.Crawley, C.E.Bemis, Jr. Higher-Order Deformations of 232Th and 234,236,238U NUCLEAR REACTIONS 232Th, 234,236,238U(p, p), (p, p'), E=35 MeV; measured σ(θ). 232Th, 234,236,238U deduced deformation parameters β2, β4, β6, multipole moments. Coupled-channels calculations, deformed spin-orbit interaction.
doi: 10.1103/PhysRevLett.47.635
1981WU02 Phys.Rev. C24, 500 (1981) J.R.Wu, J.R.Beene, C.E.Bemis, Jr., F.E.Bertrand, E.E.Gross, D.J.Horen, W.P.Jones Fission Probability of 239U at High Excitation Measured with the 238U(α, 3Hef) Reaction NUCLEAR REACTIONS, Fission 238U(α, 3HeF), E=152 MeV; measured σ(θ(3He), E(3He)), σ(θ(3He), E(3He), fragment θ), 3He(fragment)(fragment)-coin; deduced reaction mechanism. 239U deduced fission probability vs excitation energy.
doi: 10.1103/PhysRevC.24.500
1980HA28 Nucl.Sci.Eng. 75, 56 (1980) J.Halperin, C.E.Bemis, Jr., J.W.Dabbs, B.H.Ketelle, R.W.Stoughton Prompt Neutron Multiplicity Distribution in the Spontaneous Fission of Curium-242 RADIOACTIVITY, Fission 242Cm(SF) [from 242Am decay]; measured neutron multiplicity distribution. Hydrogen moderation, gas-filled proportional counter, hemispherical geometry.
doi: 10.13182/NSE80-A20317
1979BE46 Phys.Rev.Lett. 43, 1854 (1979); Erratum Phys.Rev.Lett. 44, 500 (1980) C.E.Bemis, Jr., J.R.Beene, J.P.Young, S.D.Kramer Optical Isomer Shift for the Spontaneous-Fission Isomer 240Am-m RADIOACTIVITY 240mAm; measured T1/2, optical isomer shift. 240mAm, 240Am deduced difference in rms radii. ATOMIC PHYSICS 240Am(SF); measured optical isomer shift. 240m,240Am deduced difference in rms radii.
doi: 10.1103/PhysRevLett.43.1854
1979MC04 Phys.Rev. C20, 2093 (1979) F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, D.Shapira, P.H.Stelson Coulomb Excitation of 183W NUCLEAR REACTIONS 183W(α, α'γ), E=15 MeV; 183W(α, α'), E=13 MeV; measured Eγ, Iγ, γ(θ), σ(Eα'; θ). 183W levels deduced B(E2), B(M1), J, π, δ. Enriched targets.
doi: 10.1103/PhysRevC.20.2093
1977BE09 Phys.Rev. C15, 705 (1977) C.E.Bemis, Jr., R.L.Ferguson, F.Plasil, R.J.Silva, F.Pleasonton, R.L.Hahn Fragment-Mass and Kinetic-Energy Distributions from the Spontaneous Fission of 252No RADIOACTIVITY, Fission 252No (SF); measured fragment-fragment coin, Eα, T1/2; deduced SF branching, α/SF, pre-neutron fragment masses, total kinetic energy distribution.
doi: 10.1103/PhysRevC.15.705
1977BE36 Phys.Rev. C16, 1146 (1977) C.E.Bemis, Jr., P.F.Dittner, R.J.Silva, R.L.Hahn, J.R.Tarrant, L.D.Hunt, D.C.Hensley Production, L X-Ray Identification, and Decay of the Nuclide 260105 RADIOACTIVITY 260Db [from 249Cf(15N, 4n)]; measured Eα, Iα, Eγ, Iγ, I(EC), xα-coin, xsf-coin, αα(t), T1/2; deduced SF branching, EC branching, Qα. 256Lr deduced levels, K, J, π, α-hindrance, SF hindrance. 256Lr; measured T1/2, Eα. 257,258Lr, 256No, 212At, 252,254Fm; measured Eα. Enriched target.
doi: 10.1103/PhysRevC.16.1146
1977BE43 Phys.Rev.Lett. 39, 1246 (1977) C.E.Bemis, Jr., R.L.Ferguson, F.Plasil, R.J.Silva, G.D.O'Kelley, M.L.Klefer, R.L.Hahn, D.C.Hensley, E.K.Hulet, R.W.Lougheed Mass Asymmetry and Total-Kinetic-Energy Release in the Spontaneous Fission of 262[105] RADIOACTIVITY, Fission 262Db, 256Fm(SF); measured σ(A), total kinetic energy distributions.
doi: 10.1103/PhysRevLett.39.1246
1977BE58 Nucl.Sci.Eng. 63, 413 (1977) C.E.Bemis, Jr., J.H.Oliver, R.Eby, J.Halperin Thermal-Neutron Capture and Fission Cross Sections and Resonance Integrals for Curium-243 NUCLEAR REACTIONS 243Cm(n, γ), (n, F), E=th; measured σ, resonance integrals.
doi: 10.13182/NSE77-A27058
1977MI11 Phys.Rev. C16, 1686 (1977) W.T.Milner, C.E.Bemis, Jr., F.K.McGowan Quadrupole and Hexadecapole Deformations in the Actinide Nuclei NUCLEAR STRUCTURE 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm; calculated model dependent β.
doi: 10.1103/PhysRevC.16.1686
1974BE52 Phys.Rev. C10, 1590 (1974) C.E.Bemis, Jr., F.Plasil, R.L.Ferguson, E.E.Gross, A.Zucker Attempted Coulomb Excitation of the Spontaneous-Fission Isomeric State In 239Pu NUCLEAR REACTIONS 239Pu(20Ne, 20Ne'), E=100, 117 MeV; measured fission fragments. 239mPu deduced upper limit on yield.
doi: 10.1103/PhysRevC.10.1590
1974MC15 Phys.Rev. C10, 1146 (1974) F.K.McGowan, C.E.Bemis, Jr., W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson Coulomb Excitation of Vibrational-Like States in the Even-A Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 236,238U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα'). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm levels deduced B(E2), B(E3). Enriched targets.
doi: 10.1103/PhysRevC.10.1146
1973BE33 Phys.Rev.Lett. 31, 647 (1973) C.E.Bemis, Jr., R.J.Silva, D.C.Hensley, O.L.Keller, Jr., J.R.Tarrant, L.D.Hunt, P.F.Dittner, R.L.Hahn, C.D.Goodman X-Ray Identification of Element 104 RADIOACTIVITY 257Rf [from 249Cf(12C, 4n), E=73.0 MeV]; measured αx-coin, Eα. 214Ra measured T1/2. 253No levels deduced transitions, T1/2.
doi: 10.1103/PhysRevLett.31.647
1973BE40 Phys.Rev. C8, 1934 (1973) C.E.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle Interference between Direct Nuclear Reactions and Coulomb Excitation with Alpha Particles on 154Sm, 166Er, and 182W NUCLEAR REACTIONS 154Sm, 166Er, 182W(α, α), (α, α'), E=11-21 MeV; measured σ(E;Eα'). 154Sm, 166Er levels deduced E2, E4 matrix elements.
doi: 10.1103/PhysRevC.8.1934
1973BE44 Phys.Rev. C8, 1466 (1973) C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, P.H.Stelson, R.L.Robinson E2 and E4 Transition Moments and Equilibrium Deformations in the Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 236U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-19 MeV; 238U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα', θ). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm deduced B(E2), B(E4), β.
doi: 10.1103/PhysRevC.8.1466
1973BO27 Nucl.Phys. A209, 125 (1973) J.S.Boyno, J.R.Huizenga, T.W.Elze, C.E.Bemis, Jr. Levels of 234U and 236U Excited by the (d, d') Reaction NUCLEAR REACTIONS 234,236U(d, d'), E=16 MeV; measured σ(Ed', θ=90°, 125°). 234,236U deduced levels, J, π, B(E2), B(E3). Enriched targets.
doi: 10.1016/0375-9474(73)90056-0
1973FE07 Phys.Rev. C8, 1104 (1973) R.L.Ferguson, F.Plasil, H.Freiesleben, C.E.Bemis, Jr., H.W.Schmitt Fragment Kinetic Energy in 18O-Induced Fission of 232Th and 246Cm NUCLEAR REACTIONS, Fission 232Th, 246Cm(18O, F), E=93.7-125.6 MeV; measured E(fragment). Deduced fragment, kinetic energy.
doi: 10.1103/PhysRevC.8.1104
1973PL04 Phys.Rev. C8, 1018 (1973) F.Pleasonton, R.L.Ferguson, F.Plasil, C.E.Bemis, Jr. Fragment-Mass and Kinetic-Energy Distributions from the Spontaneous Fission of 246Cm RADIOACTIVITY, Fission 246Cm(SF); measured fragment(E).
doi: 10.1103/PhysRevC.8.1018
1973ST04 Nucl.Sci.Eng. 50, 169 (1973) R.W.Stoughton, J.Halperin, C.E.Bemis, H.W.Schmitt Neutron Multiplicity Distributions in the Spontaneous Fission of 246Cm, 248Cm, and 252Cf RADIOACTIVITY, Fission 246,248Cm, 252Cf(SF); measured (n)(fragment)-coin, deduced neutron multiplicity distribution.
doi: 10.13182/NSE73-A23241
1973ST15 J.Inorg.Nucl.Chem. 35, 3369 (1973) J.R.Stokely, C.E.Bemis, Jr., R.D.Baybarz, R.Eby The Absolute Specific Activity and Half Life for 249Cf RADIOACTIVITY 249Cf; measured T1/2.
doi: 10.1016/0022-1902(73)80046-6
1972BE09 Nucl.Sci.Eng. 47, 371 (1972) C.E.Bemis, Jr., R.E.Druschel, J.Halperin, J.R.Walton Thermal-Neutron Capture Cross Section and Resonance Integral for 10.7-Year Krypton-85 NUCLEAR REACTIONS 85Kr(n, γ), E=thermal; measured σ; deduced resonance integral.
doi: 10.13182/NSE72-A22423
1972CH01 Phys.Rev. A5, 67 (1972) Y.Y.Chu, M.L.Perlman, P.F.Dittner, C.E.Bemis, Jr. Electron Binding Energies, X-Ray Spectra, and L-Shell Fluorescence Yields in Curium (Z = 96) RADIOACTIVITY 249Cf; measured E(K X-ray), I(K X-ray). 250Cf; measured E(L X-ray), I(L X-ray), I(ce), Eγ, Iγ. Cm deduced electron binding energies, L-shell fluorescence yields. ATOMIC PHYSICS Cm; measured E(L X-ray), I(L X-ray), E(K X-ray);I(K X-ray); deduced electron binding energies, L-shell fluorescence yields.
doi: 10.1103/PhysRevA.5.67
1972DI02 Phys.Rev. A5, 481 (1972) K-Series X-Ray Energies and Intensities for Curium, Berkelium, Californium, and Einsteinium RADIOACTIVITY 249Cf, 254Es, 250Bk, 251Fm; measured E(K X-ray). Cm, Bk, Cf, Es deduced K-shell binding energies, relative transition probabilities. ATOMIC PHYSICS Cm, Bk, Cf, Es; measured E(K X-ray); deduced K-shell binding energies, relative transition probabilities.
doi: 10.1103/PhysRevA.5.481
1972SC01 Nucl.Phys. A178, 410 (1972) M.Schmorak, C.E.Bemis, Jr., M.J.Zender, N.B.Gove, P.F.Dittner Ground State Rotational Bands in Doubly Even Actinide Nuclei RADIOACTIVITY 234U, 236U, 238Pu, 240Pu, 242Pu, 244,246Cm, 250Cf(α); measured Eγ, Iγ. 230Th, 232Th, 234U, 236U, 238U, 240Pu, 242Pu, 246Cm deduced levels. Ge(Li) detector.
doi: 10.1016/0375-9474(72)90468-X
1971CH24 Nucl.Phys. A168, 250 (1971) E.T.Chulick, P.L.Reeder, C.E.Bemis, Jr., E.Eichler Energy Spectrum of Delayed Neutrons from the Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf(SF); measured En delayed neutrons. Time of flight spectrometer.
doi: 10.1016/0375-9474(71)90791-3
1971CH51 Radiochim.Acta 16, 8 (1971) E.T.Chulick, P.L.Reeder, C.E.Bemis, E.Eichler Analysis of Delayed-Neutron Yields from 252Cf NUCLEAR STRUCTURE, Fission 252Cf(SF); calculated delayed neutron yields.
1971DI03 Phys.Rev.Lett. 26, 1037 (1971) P.F.Dittner, C.E.Bemis, Jr., D.C.Hensley, R.J.Silva, C.D.Goodman Identification of the Atomic Number of Nobelium by an X-Ray Technique RADIOACTIVITY 255No; measured αX-coin, αX-delay, Eα. 251Fm level deduced T1/2.
doi: 10.1103/PhysRevLett.26.1037
1971FO17 Phys.Rev.Lett. 27, 1232 (1971) J.L.C.Ford, Jr., P.H.Stelson, C.E.Bemis, Jr., F.K.McGowan, R.L.Robinson, W.T.Milner Precise Coulomb Excitation B(E2) Values for First 2+ States of the Actinide Nuclei NUCLEAR REACTIONS 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf(α, α'), E=17, 18 MeV; measured B(E2). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf deduced B(E2). 252Cf deduced level.
doi: 10.1103/PhysRevLett.27.1232
1971MC19 J.Inorg.Nucl.Chem. 33, 3251 (1971) J.E.McCracken, J.R.Stokely, R.D.Baybarz, C.E.Bemis, Jr., R.Eby Determination of the Half-Lives of 246Cm and 248Cm by Absolute Specific Activity Techniques RADIOACTIVITY 246,248Cm; measured T1/2(α). 248Cm; measured T1/2(SF).
doi: 10.1016/0022-1902(71)80645-0
1971MC21 Phys.Rev.Lett. 27, 1741 (1971) F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson Equilibrium Quadrupole and Hexadecapole Deformations in 230Th and 238U NUCLEAR REACTIONS 230Th, 238U(α, α), (α, α'), E=17, 18 MeV; measured σ(Eα'). 230Th, 238U deduced B(EL), equilibrium deformation parameters.
doi: 10.1103/PhysRevLett.27.1741
1970BE44 Inorg.Nucl.Chem.Lett. 6, 747 (1970); ORNL-4581, p.36 (1970) C.E.Bemis, Jr., R.J.Silva, J.E.Bigelow, A.M.Friedman Search for a Long-Lived Spontaneous Fission Isomer of 241Pu NUCLEAR REACTIONS 240Pu(n, γ), E=thermal, > 1 MeV; 242Pu(n, 2n), E > 6.2 MeV; 238U(α, n), E=40 MeV; measured σ. 241Pu deduced no 0.3-yr SF-isomer.
doi: 10.1016/0020-1650(70)80091-5
1970SC12 Phys.Rev.Lett. 24, 1507 (1970) M.R.Schmorak, C.E.Bemis, Jr., M.Zender, F.E.Coffman, A.V.Ramayya, J.H.Hamilton Evidence for a Two-Phonon Octupole Vibrational Band in 240Pu RADIOACTIVITY 240Np; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft. 240Pu deduced levels, ICC, γ-multipolarity, J, π, K. Ge(Li), NaI(Tl) detector.
doi: 10.1103/PhysRevLett.24.1507
1970SI19 Phys.Rev. C2, 1948 (1970) R.J.Silva, R.L.Hahn, K.S.Toth, M.L.Mallory, C.E.Bemis, Jr., P.F.Dittner, O.L.Keller New Isotopes 241Cf and 240Cf RADIOACTIVITY 240,241Cf; measured T1/2, Eα, Iα. 242Cf; measured Eα. NUCLEAR REACTIONS 233,234,235U(12C, X), E=60-90 MeV; measured σ(E) for 240,241,242Cf production.
doi: 10.1103/PhysRevC.2.1948
1970TO04 J.Inorg.Nucl.Chem. 32, 1051 (1970) K.S.Toth, R.L.Hahn, C.E.Bemis, Jr., T.H.Handley, M.F.Roche Search for 172Hf Alpha Decay RADIOACTIVITY 172Hf[from 175Lu(p, 4n)]; measured α-activity; deduced α-branching, T1/2.
doi: 10.1016/0022-1902(70)80094-X
1969BE06 J.Inorg.Nucl.Chem. 31, 599 (1969) C.E.Bemis, Jr., J.Halperin, R.Eby The Alpha Decay Half Lives of 242Pu and 244Pu RADIOACTIVITY 242Pu; measured T1/2. 244Pu [from 242Pu(n)]; measured T1/2, Eα, Iα; deduced Qα. 240U deduced levels.
doi: 10.1016/0022-1902(69)80004-7
1969BR03 Nucl.Phys. A125, 217 (1969) S.M.Brahmavar, J.H.Hamilton, A.V.Ramayya, E.F.Zganjar, C.E.Bemis, Jr. The Decay of 110mAg: Gamma-Ray Energy and Intensity Standardization RADIOACTIVITY 110mAg [from 109Ag(n, γ)]; 108mAg [from 107Ag(n, γ)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 108Pd, 110Cd deduced levels. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90840-9
1969CH37 Radiochim.Acta 12, 164 (1969) E.T.Chulick, P.L.Reeder, E.Eichler, C.E.Bemis, Jr. Redetermination of Delayed Neutrons from 252Cf RADIOACTIVITY, Fission 252Cf; measured delayed neutron yields, T1/2.
1968BE21 Nucl.Phys. A121, 433 (1968) The Alpha Decay of 253Cf and 254Cf RADIOACTIVITY 253,254Cf; measured T1/2, Eα, Iα; deduced Q, SF/α branch. 249,250Cm deduced levels, J, π.
doi: 10.1016/0375-9474(68)90431-4
1968BE49 Priv.Comm.(1968)
1968BE63 Arkiv Fysik 37, 203 (1968) The Decay of 134Te RADIOACTIVITY 134Te; measured T1/2, Eγ, Iγ, I(ce) ICC, γγ-coin; deduced log ft. 134I deduced levels, J, π, γ-mixing, ICC. Ge(Li) detector.
1968BE64 Arkiv Fysik 37, 213 (1968) Decay Properties of the 133Te Isomers RADIOACTIVITY 133Te; measured Eγ, Iγ, I(ce). 133I deduced levels, γ-mixing, ICC. Ge(Li) detector.
1968WA06 Priv.Comm. (1968) NUCLEAR STRUCTURE 245Pu; measured not abstracted; deduced nuclear properties.
1967BE63 Priv.Comm. (1967) NUCLEAR STRUCTURE 246Am; measured not abstracted; deduced nuclear properties.
1966FR02 Nucl.Phys. 78, 207 (1966) The Decay of 132Te and Levels in Odd 132I RADIOACTIVITY 132Te [from fission]; measured Eγ, E(ce), Iγ, I(ce), ICC; deduced γ-mixing(E2/M1), B(λ). 132I deduced levels, J, π. Separated source.
doi: 10.1016/0029-5582(66)91000-5
1965BE04 Bull.Am.Phys.Soc. 10, No.1, 82, GC5 (1965) Decay of 37-min Sb130 NUCLEAR STRUCTURE 130Sb, 131Sb, 131Te; measured not abstracted; deduced nuclear properties.
1965BE26 Phys.Letters 19, 567 (1965) On the Properties of the 27.78 keV Level in 129I NUCLEAR STRUCTURE 129Te; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90780-8
1965WA05 Bull.Am.Phys.Soc. 10, No.3, 377, KF3 (1965) W.B.Walters, C.E.Bemis, Jr., G.E.Gordon Decay Scheme of Te131g NUCLEAR STRUCTURE 131Te; measured not abstracted; deduced nuclear properties.
1965WA11 Phys.Rev. 140, B268 (1965) W.B.Walters, C.E.Bemis, Jr., G.E.Gordon Decay Scheme of 25-Minute Te131g NUCLEAR STRUCTURE 131Te; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B268
1964BE06 J.Inorg.Nucl.Chem. 26, 213 (1964) C.E.Bemis, G.E.Gordon, C.D.Coryell Half-Life of Sb135 and Evidence on the Half-Life of Sb134 NUCLEAR STRUCTURE 135Sb, 134Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(64)80060-9
Back to query form |