NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = E.K.Hulet Found 71 matches. 1995LA20 Phys.Rev.Lett. 75, 1903 (1995) Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, Yu.S.Tsyganov, V.K.Utyonkov, F.Sh.Abdullin, S.Iliev, A.N.Polyakov, J.Rigol, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, G.V.Buklanov, B.N.Gikal, V.B.Kutner, A.N.Mezentsev, I.M.Sedykh, D.V.Vakatov, R.W.Lougheed, J.F.Wild, K.J.Moody, E.K.Hulet New Nuclide 267108 Produced by the 238U + 34S Reaction NUCLEAR REACTIONS, ICPND 238U(34S, X)267Hs, E=186 MeV; measured Eα, Iα; deduced residual production σ. RADIOACTIVITY 267Hs(α) [from 238U(34S, X), E=186 MeV]; measured Eα, Iα, T1/2.
doi: 10.1103/PhysRevLett.75.1903
1995SC53 Radiochim.Acta 68, 7 (1995) M.Schadel, E.Jager, W.Bruchle, K.Summerer, E.K.Hulet, J.F.Wild, R.W.Lougheed, R.J.Dougan, K.J.Moody Radiochemical Search for Neutron-Rich Isotopes of Nielsbohrium in the 16O + 254Es Reaction NUCLEAR REACTIONS, ICPND 254Es(16O, xn)E=113, 116 MeV; measured α-spectra following residual decay; deduced production σ for 265,266,267107 vs assumed T1/2. On-line gas chromatography.
1994HU18 Yad.Fiz. 57, No 7, 1165 (1994); Phys.Atomic Nuclei 57, 1099 (1994) Role of the Second Barrier Upon Mass Division in the Spontaneous Fission of the Heaviest Elements RADIOACTIVITY 252,254No, 256Rf, 258Rf(SF); measured fission fragment mass, total kinetic energy distributions; deduced sharp asymmetrical to symmetrical mass division transition, second barrier role. Data on other nuclei included. Sources from (heavy ion, xn) reactions.
1994LA22 Phys.Rev.Lett. 73, 624 (1994) Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, V.K.Utyonkov, F.Sh.Abdullin, G.V.Buklanov, B.N.Gikal, S.Iliev, A.N.Mezentsev, A.N.Polyakov, I.M.Sedykh, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, Yu.S.Tsyganov, V.E.Zhuchko, R.W.Lougheed, K.J.Moody, J.F.Wild, E.K.Hulet, J.H.McQuaid Discovery of Enhanced Nuclear Stability Near the Deformed Shells N = 162 and Z = 108 NUCLEAR REACTIONS 248Cm(22Ne, X), E=116, 121 MeV; measured Eα, Iα; deduced evidence for 265Sg, 266Sg. RADIOACTIVITY 265Sg, 266Sg(α); measured Eα, Iα; deduced T1/2, SF-decay upper limits. 262Rf [from 266Sg(α-decay)]; measured T1/2.
doi: 10.1103/PhysRevLett.73.624
1994LO27 J.Alloys and Compounds 213/214, 61 (1994) R.W.Lougheed, K.J.Moody, J.FD.Wild, E.K.Hulet, J.H.McQuaid, Yu.A.Lazarev, Yu.V.Lobanov, Yu.Ts.Oganessian, V.K.Utyonkov, F.Sh.Abdullin, G.V.Buklanov, B.N.Gikal, S.Iliev, A.N.Mezentsev, A.N.Polyakov, I.M.Sedykh, I.V.Shirokovsky, V.G.Subbotin, A.M.Sukhov, Yu.S.Tsyganov, V.E.Zhuchko Observation of enhanced nuclear stability near the 162 neutron shell RADIOACTIVITY 265,266Sg(α) [from 248Cm(22Ne, xn)]; measured Eα, T1/2. 262Rf(SF) [from 266Sg decay]; measured T1/2. Comparison with model predictions.
doi: 10.1016/0925-8388(94)90881-8
1994WI17 J.Alloys and Compounds 213/214, 86 (1994) J.F.Wild, E.K.Hulet, R.W.Lougheed, K.J.Moody, B.B.Bandong, R.J.Dougan, A.Veeck Spontaneous fission properties of 252, 254No and 256, 258[104] and the disappearance of the outer fission barrier RADIOACTIVITY 252,254No(SF) [from 244,246Cm(12C, 4n)]; 256,258Rf(SF) [from 244Cm(16O, 4n) and 249Cf(12C, 3n)]; measured fission fragment kinetic energy and mass distributions; deduced fission barrier features.
doi: 10.1016/0925-8388(94)90885-0
1993MO18 Nucl.Phys. A563, 21 (1993) K.J.Moody, R.W.Lougheed, J.F.Wild, R.J.Dougan, E.K.Hulet, R.W.Hoff, C.M.Henderson, R.J.Dupzyk, R.L.Hahn, K.Summerer, G.D.O'Kelley, G.R.Bethune Decay Properties of Heavy Mendelevium Isotopes NUCLEAR REACTIONS, ICPND 254Es(18O, X)256Md/255Md/257Md/258Md/258mMd/259Md/260Md, E=105 MeV; 254Es(22Ne, X)256Md/255Md/257Md/258Md/258mMd/259Md/260Md, E=126 MeV; measured Eα, Iα; deduced residual nuclei production σ. RADIOACTIVITY 256Md(EC), (α); 257Md(EC), (α), (SF); 258Md(α), (SF), (EC), (β-); 258mMd(EC), (α), (SF), (β-); 259Md(SF), (α); measured Eα, Iα, γ-spectra, SF-decay; deduced T1/2, branching ratio. 256,257,258Md deduced mass excess. 259Md deduced SF-decay hindrance factor. 252,253,254Es deduced levels, J, π, γ transitions.
doi: 10.1016/0375-9474(93)90010-U
1992MO03 Phys.Rev. C45, 1392 (1992) K.J.Moody, E.K.Hulet, P.B.Price Search for Cluster Radioactivity of 237Np RADIOACTIVITY 237Np; measured cluster emission T1/2 lower limit; deduced 30Mg, 32Si as most likely clusters.
doi: 10.1103/PhysRevC.45.1392
1992MO25 Phys.Rev. C46, 2624 (1992) K.J.Moody, R.W.Lougheed, E.K.Hulet Search for the Double Beta Decay of 244Pu RADIOACTIVITY 244Pu(2β-); measured ingrowth of 244Cm, alpha activity; deduced T1/2 limit.
doi: 10.1103/PhysRevC.46.2624
1991PR02 Phys.Rev. C43, 1781 (1991) P.B.Price, K.J.Moody, E.K.Hulet, R.Bonetti, C.Migliorino High-Statistics Study of Cluster Radioactivity from 233U RADIOACTIVITY 233U(α), (24Ne), (25Ne), (28Mg); measured T1/2; deduced relative branching ratios. Track recording phosphate glass detector.
doi: 10.1103/PhysRevC.43.1781
1990MO01 Phys.Rev. C41, 152 (1990) K.J.Moody, R.W.Lougheed, R.J.Dougan, E.K.Hulet, J.F.Wild, K.Summerer, R.L.Hahn, J.van Aarle, G.R.Bethune Actinide Cross Sections from the Reaction of 13C with 254gEs NUCLEAR REACTIONS 254Es(13C, X), E=72 MeV; measured production σ for 252-256Es, 253-257Fm, 255-260Md, 256,257,259No, 259-262Lr, 261104, 262105; deduced reaction σ, production mechanism.
doi: 10.1103/PhysRevC.41.152
1990WI01 Phys.Rev. C41, 640 (1990) J.F.Wild, J.van Aarle, W.Westmeier, R.W.Lougheed, E.K.Hulet, K.J.Moody, R.J.Dougan, E.-A.Koop, R.E.Glaser, R.Brandt, P.Patzelt Prompt Neutron Emission from the Spontaneous Fission of 260Md NUCLEAR REACTIONS 254Es(22Ne, X), E=126 MeV; measured (neutron)(fragment)-coin; deduced 260Md production evidence. RADIOACTIVITY 260Md(SF) [from 254Es(22Ne, X), E=126 MeV]; measured fission neutron multiplicity distribution, emission probabilities.
doi: 10.1103/PhysRevC.41.640
1989HU09 Phys.Rev. C40, 770 (1989) E.K.Hulet, J.F.Wild, R.J.Dougan, R.W.Lougheed, J.H.Landrum, A.D.Dougan, P.A.Baisden, C.M.Henderson, R.J.Dupzyk, R.L.Hahn, M.Schadel, K.Summerer, G.R.Bethune Spontaneous Fission Properties of 258Fm, 259Md, 260Md, 258No, and 260[104]: Bimodal fission RADIOACTIVITY 258Fm, 258No, 259,260Md, 260Rf(SF); measured fission fragment mass, kinetic energy distributions; deduced fission features.
doi: 10.1103/PhysRevC.40.770
1989MO07 Phys.Rev. C39, 2445 (1989) K.J.Moody, E.K.Hulet, S.Wang, P.B.Price Heavy-Fragment Radioactivity of 234U RADIOACTIVITY 234U(24Ne), (26Ne), (28Mg); measured T1/2, branching ratios, fragment energies.
doi: 10.1103/PhysRevC.39.2445
1989WA10 Phys.Rev. C39, 1647 (1989) S.Wang, D.Snowden-Ifft, P.B.Price, K.J.Moody, E.K.Hulet Heavy-Fragment Radioactivity of 238Pu: Si and Mg emission RADIOACTIVITY 238Pu(28Mg), (30Mg), (32Si); measured decay T1/2, branching ratio relative to α-decay.
doi: 10.1103/PhysRevC.39.1647
1987MO28 Phys.Rev. C36, 2710 (1987) K.J.Moody, E.K.Hulet, Shicheng Wang, P.B.Price, S.W.Barwick Search for Heavy-Ion Radioactivity from 241Am RADIOACTIVITY 241Am(34Si), (α); measured (34Si)/α branching upper limit. Track detectors. Cluster model, super asymmetric fission predictions comparisons.
doi: 10.1103/PhysRevC.36.2710
1987SH27 Phys.Rev. C36, 2717 (1987) Shicheng Wang, P.B.Price, S.W.Barwick, K.J.Moody, E.K.Hulet Radioactive Decay of 234U via Ne and Mg Emission RADIOACTIVITY 234U(24Ne), (26Ne), (28Mg), (SF), (α); measured T1/2, Ne, Mg, SF-decay fragment charges, ranges; deduced branching ratio relative to alpha decay. Track recording phosphate glass detector.
doi: 10.1103/PhysRevC.36.2717
1986CZ02 Nucl.Phys. A458, 123 (1986) T.Czosnyka, D.Cline, L.Hasselgren, C.Y.Wu, R.M.Diamond, H.Kluge, C.Roulet, E.K.Hulet, R.W.Lougheed, C.Baktash E2 Properties of the Ground State Band in 248Cm NUCLEAR REACTIONS 248Cm(136Xe, 136Xe'), E=641 MeV; 248Cm(58Ni, 58Ni'), E=260 MeV; measured Eγ, Iγ following Coulomb excitation. 248Cm levels deduced J, π, E2 transition matrix elements.
doi: 10.1016/0375-9474(86)90286-1
1986HU01 Phys.Rev.Lett. 56, 313 (1986) E.K.Hulet, J.F.Wild, R.J.Dougan, R.W.Lougheed, J.H.Landrum, A.D.Dougan, M.Schadel, R.L.Hahn, P.A.Baisden, C.M.Henderson, R.J.Dupzyk, K.Summerer, G.R.Bethune Bimodal Symmetric Fission Observed in the Heaviest Elements RADIOACTIVITY 258Fm(SF); 258m,259,260Md(SF) [from 254Es(18O, X), E=105 MeV; 254Es(22Ne, X), E=16 MeV]; 258No(SF) [from 248Cm(13C, X), E=81 MeV]; 260Rf(SF) [from 249Bk(15N, X), E=81 MeV]; measured fission fragment mass, kinetic energy partitioning; deduced bimodal symmetric fission evidence.
doi: 10.1103/PhysRevLett.56.313
1986HU05 Phys.Rev. C34, 1394 (1986) E.K.Hulet, R.W.Lougheed, J.F.Wild, R.J.Dougan, K.J.Moody, R.L.Hahn, C.M.Henderson, R.J.Dupzyk, G.R.Bethune Z and A Identification of 370-μs 258Fm RADIOACTIVITY 258mFm(SF) [from 258mMd(EC-decay)]; measured fission (fragment)(X-ray) time correlation; deduced T1/2, charge, mass. Ge and Si-Au detectors.
doi: 10.1103/PhysRevC.34.1394
1986KR02 Phys.Rev. C33, 504 (1986) J.V.Kratz, W.Bruchle, H.Folger, H.Gaggeler, M.Schadel, K.Summerer, G.Wirth, N.Greulich, G.Herrmann, U.Hickmann, P.Peuser, N.Trautmann, E.K.Hulet, R.W.Lougheed, J.M.Nitschke, R.L.Ferguson, R.L.Hahn Search for Superheavy Elements in Damped Collisions between 238U and 248Cm NUCLEAR REACTIONS 248Cm(238U, X), E=6.2-7.3 MeV/nucleon; measured SF-fission fragment kinetic energies, neutron multiplicities; deduced superheavy nuclei production σ upper limit. Chemical separation, spontaneous fission counting.
doi: 10.1103/PhysRevC.33.504
1986LO16 J.Less-Common Met. 122, 461 (1986) R.W.Lougheed, E.K.Hulet, R.J.Dougan, J.F.Wild, R.J.Dupzyk, C.M.Henderson, K.J.Moody, R.L.Hahn, K.Summerer, G.Bethune The Discovery of 260Md and the Decay Properties of 258Fm, 258m,258gMd and 259Md NUCLEAR REACTIONS 254Es(18O, xnyp), E=105 MeV; 254Es(22Ne, xnyp), E=126 MeV; measured Fm, Md isotope production σ. RADIOACTIVITY 260Md(SF) [from 254Es(18O, xnyp), E=105 MeV; 254Es(22Ne, xnyp), E=126 MeV]; measured T1/2. 258mMd(EC), 258,259Md, 258Fm(SF) [from 254Es(18O, xnyp), E=105 MeV; 254Es(22Ne, xnyp), E=126 MeV]; measured decay characteristics, T1/2.
doi: 10.1016/0022-5088(86)90442-X
1986MO06 Phys.Rev. C33, 1315 (1986) K.J.Moody, D.Lee, R.B.Welch, K.E.Gregorich, G.T.Seaborg, R.W.Lougheed, E.K.Hulet Actinide Production in Reactions of Heavy Ions with 248Cm NUCLEAR REACTIONS 248Cm(16O, X), E=96.5 MeV; 248Cm(136Xe, X), E=699-790 MeV; 248Cm(86Kr, X), E=493-546 MeV; measured actinide (232Pa-256Fm) yields; deduced optimum reactions.
doi: 10.1103/PhysRevC.33.1315
1986SC10 Phys.Rev. C33, 1547 (1986) M.Schadel, W.Bruchle, M.Brugger, H.Gaggeler, K.J.Moody, D.Schardt, K.Summerer, E.K.Hulet, A.D.Dougan, R.J.Dougan, J.H.Landrum, R.W.Lougheed, J.F.Wild, G.D.O'Kelley Transfer Cross Sections from Reactions with 254Es as a Target NUCLEAR REACTIONS, ICPND 254Es(16O, X), E=98 MeV; measured production σ for No, Lr isotopes. 254Es(18O, X)260Md/261Md/260No/261No/262No/261Lr/262Lr/263Lr, E=98 MeV; 254Es(22Ne, X)260Md/261Md/260No/261No/262No/261Lr/262Lr/263Lr, E=127 MeV; measured residual production σ. Activation technique.
doi: 10.1103/PhysRevC.33.1547
1985LO13 Phys.Rev. C32, 1760 (1985) R.W.Lougheed, J.H.Landrum, E.K.Hulet, J.F.Wild, R.J.Dougan, A.D.Dougan, H.Gaggeler, M.Schadel, K.J.Moody, K.E.Gregorich, G.T.Seaborg Search for Superheavy Elements using the 48Ca + 254gEs Reaction NUCLEAR REACTIONS 254Es(48Ca, X)211At/209At/212Pb, E=240, 249 MeV; measured residuals, superheavy production σ. Aqueous, gas phase separation technique.
doi: 10.1103/PhysRevC.32.1760
1985SO03 Phys.Rev. C31, 1801 (1985) L.P.Somerville, M.J.Nurmia, J.M.Nitschke, A.Ghiorso, E.K.Hulet, R.W.Lougheed Spontaneous Fission of Rutherfordium Isotopes RADIOACTIVITY 256Rf(SF) [from 249Cf(12C, 5n), E=85 MeV]; 257Rf(SF) [from 249Cf(12C, 4n), E=75 MeV]; 258Rf(SF) [from 246Cm(16O, 4n), E=95 MeV]; 259Rf(SF) [from 245Cm(18O, 4n), E=93 MeV]; 260Rf(SF) [from 249Bk(15N, 4n), E=80 MeV; 248Cm(16O, 4n), E=92 MeV; 249Cf(16O, 3nα), E=96 MeV]; 262Rf(SF) [from 248Cm(18O, 4n), E=89 MeV; 244Pu(22Ne, 4n), E=113 MeV]; measured T1/2(SF), fission branching. Fast tape system. NUCLEAR REACTIONS, ICPND 244Pu(22Ne, 4n), E=113 MeV; 248Cm(18O, 4n), E=89 MeV; 249Cf(18O, 3nα), E=96 MeV; 248Cm(16O, 4n), E=92 MeV; 249Bk(15N, 4n), E=80 MeV; 245Cm(18O, 4n), E=93 MeV; 246Cm(16O, 4n), E=95 MeV; 249Cf(12C, 4n), E=75 MeV; 249Cf(12C, 5n), E=85 MeV; measured residual production σ, T1/2(SF), fission branch estimate. Fast tape system.
doi: 10.1103/PhysRevC.31.1801
1985WI10 Phys.Rev. C32, 488 (1985) J.F.Wild, P.A.Baisden, R.J.Dougan, E.K.Hulet, R.W.Lougheed, J.H.Landrum Light-Charged-Particle Emission in the Spontaneous Fission of 250Cf, 256Fm, and 257Fm RADIOACTIVITY 250Cf, 256Fm, 257Fm(SF); measured σ(Eα) following fission; deduced α-, t-, p-, total light particle emission probabilities.
doi: 10.1103/PhysRevC.32.488
1982SC05 Phys.Rev.Lett. 48, 852 (1982) M.Schadel, W.Bruchle, H.Gaggeler, J.V.Kratz, K.Summerer, G.Wirth, G.Herrmann, R.Stakemann, G.Tittel, N.Trautmann, J.M.Nitschke, E.K.Hulet, R.W.Lougheed, R.L.Hahn, R.L.Ferguson Actinide Production in Collisions of 238U with 248Cm NUCLEAR REACTIONS 248Cm(238U, X), E=7.4 MeV/nucleon; measured production σ for 244,246,248,250,251Bk, 246,248,250,251,252,253,254Cf, 252,253,254,255,256Es, 252,253,254,255,256Fm, 255,256,257,258Md; deduced dominant transfer reaction deexcitation channel.
doi: 10.1103/PhysRevLett.48.852
1982WI08 Phys.Rev. C26, 1531 (1982) J.F.Wild, E.K.Hulet, R.W.Lougheed, P.A.Baisden, J.H.Landrum, R.J.Dougan, M.G.Mustafa Unusually Low Fragment Energies in the Symmetric Fission of 259Md RADIOACTIVITY 259No(EC), (α) [from 248Cm(18O, 3nα)]; measured α-decay T1/2. 259Md(SF) [from 259No(EC-decay)]; measured T1/2, (fragment)(fragment)-coin; deduced SF-decay upper limit, fragment mass, total kinetic energy distributions.
doi: 10.1103/PhysRevC.26.1531
1981LO15 J.Inorg.Nucl.Chem. 43, 2239 (1981) R.W.Lougheed, E.K.Hulet, J.F.Wild, B.J.Qualheim, J.E.Evans, R.J.Dupzyk Two New Isotopes with N = 157: 256Es and 255Cf RADIOACTIVITY 256Es, 255Cf [from neutron irradiation of 255Es, 254Cf]; measured β-decay T1/2. NUCLEAR REACTIONS 255Es, 254Cf(n, γ), E=reactor; measured σ(effective); deduced evidence for 256Es, 255Cf. Enriched targets.
doi: 10.1016/0022-1902(81)80239-4
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
1980HO04 Phys.Rev. C21, 972 (1980) D.C.Hoffman, J.B.Wilhelmy, J.Weber, W.R.Daniels, E.K.Hulet, R.W.Lougheed, J.H.Landrum, J.F.Wild, R.J.Dupzyk 12.3-min 256Cf and 43-min 258Md and Systematics of the Spontaneous Fission Properties of Heavy Nuclides RADIOACTIVITY 256Cf(SF) [from 254Cf(t, p), E=16 MeV]; measured T1/2, (fragment)(fragment)-coin; deduced total kinetic energy, mass distribution. 258Md[from 255Es(α, n), E=26.3 MeV]; measured T1/2. 258Fm (SF) [from ϵ decay of 258Md]; measured (fragment)(fragment)-coin; deduced total kinetic energy, mass distribution.
doi: 10.1103/PhysRevC.21.972
1980HU03 Phys.Rev. C21, 966 (1980) E.K.Hulet, R.W.Lougheed, J.H.Landrum, J.F.Wild, D.C.Hoffman, J.Weber, J.B.Wilhelmy Spontaneous Fission of 259Fm NUCLEAR REACTIONS 257Fm(t, p), E=16 MeV; measured σ, (fragment)(fragment)-coin. 259Fm deduced SF isomer, T1/2, fragment mass distribution.
doi: 10.1103/PhysRevC.21.966
1978IL01 Phys.Lett. 78B, 209 (1978) J.D.Illige, E.K.Hulet, J.M.Nitschke, R.J.Dougan, R.W.Lougheed, A.Ghiorso, J.H.Landrum Search for Volatile Superheavy Elements from the Reaction 248Cm + 48Ca NUCLEAR REACTIONS 248Cm(48Ca, X), E=267 MeV; measured σ for α-, SF-decay fragments; deduced no volatile superheavy elements with T1/2=1 sec-4.17 days.
doi: 10.1016/0370-2693(78)90007-2
1978LO13 J.Inorg.Nucl.Chem. 40, 1865 (1978) R.W.Lougheed, J.F.Wild, E.K.Hulet, R.W.Hoff, J.H.Landrum A New Isotope of Curium and its Decay Properties: 251Cm RADIOACTIVITY 251Cm [from 250Cm(n, γ)]; measured T1/2, Eγ, Iγ, Qβ-, Eβ. 251Bk deduced levels, J, K, π.
doi: 10.1016/0022-1902(78)80244-9
1978WI12 S.Afr.J.Phys. 1, 116 (1978) J.B.Wilhelmy, H.C.Britt, D.C.Hoffman, W.R.Daniels, E.Cheifetz, A.Gavron, J.Weber, E.K.Hulet, J.H.Landrum, R.W.Lougheed, J.F.Wild Fission Properties of the Heavy Actinides NUCLEAR REACTIONS 254Es(d, pF), (t, pF), E not given; measured fission barriers. RADIOACTIVITY, Fission 256Cf(SF) [from 254Cf(t, p)]; 258Fm(SF) [from 255Es(α, n)258Md+electron capture]; 259Fm(SF) [from 257Fm(t, p)]; measured fragment mass distribution, average kinetic energy release.
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
1977BU14 Phys.Lett. 68B, 122 (1977) P.A.Butler, I.Y.Lee, J.O.Newton, Y.El-Masri, M.M.Aleonard, P.Colombani, R.M.Diamond, F.S.Stephens, R.W.Lougheed, E.K.Hulet Fission of 232Th, 238U, 244Pu, 248Cm Induced by Xe and Kr Ions at Coulomb Barrier Energies NUCLEAR REACTIONS 232Th, 238U, 244Pu, 248Cm(86Kr, F), (136Xe, F), E ≈ Coulomb barrier; measured σ(θ).
doi: 10.1016/0370-2693(77)90181-2
1977HU04 Phys.Rev.Lett. 39, 385 (1977) E.K.Hulet, R.W.Lougheed, J.F.Wild, J.H.Landrum, P.C.Stevenson, A.Ghiorso, J.M.Nitschke, R.J.Otto, D.J.Morrissey, P.A.Baisden, B.F.Gavin, D.Lee, R.J.Silva, M.M.Fowler, G.T.Seaborg Search for Superheavy Elements in the Bombardment of 248Cm with 48Ca NUCLEAR REACTIONS 248Cm(48Ca, X), E=267 MeV; measured σ for formation of superheavy elements.
doi: 10.1103/PhysRevLett.39.385
1976BO13 J.Inorg.Nucl.Chem. 38, 1291 (1976) Mossbauer Studies of Americium Compounds NUCLEAR MOMENTS 243Am; measured isomer shift, quadrupole moment ratio. Mossbauer studies in Am compounds.
doi: 10.1016/0022-1902(76)80138-8
1974GH04 Phys.Rev.Lett. 33, 1490 (1974) A.Ghiorso, J.M.Nitschke, J.R.Alonso, C.T.Alonso, M.Nurmia, G.T.Seaborg, E.K.Hulet, R.W.Lougheed Element 106 NUCLEAR REACTIONS 249Cf(18O, X)263Sg, E=95 MeV; measured reaction products, Eα, Iα; deduced σ. RADIOACTIVITY 263Sg(α); measured decay products, Eα, Iα; deduced T1/2.
doi: 10.1103/PhysRevLett.33.1490
1974RA02 Phys.Rev. C9, 399 (1974) R.C.Ragaini, E.K.Hulet, R.W.Lougheed, J.Wild Symmetric Fission in the Neutron-Induced Fission of 255Fm NUCLEAR REACTIONS 251Cf, 255Fm(n, F), E=thermal; measured E(fragment), deduced fragment mass distribution.
doi: 10.1103/PhysRevC.9.399
1973HU01 Radiochim.Radioanal.Lett. 13, 217 (1973) Decay of Californium-248 RADIOACTIVITY 248Cf; measured T1/2, α/SF-ratio, xα-coin.
1973WI03 J.Inorg.Nucl.Chem. 35, 1063 (1973) J.F.Wild, E.K.Hulet, R.W.Lougheed Some Nuclear Properties of Fermium-257 RADIOACTIVITY 257Fm; measured T1/2, α/SF ratio.
doi: 10.1016/0022-1902(73)80176-9
1971HO16 Nucl.Phys. A169, 641 (1971) R.W.Hoff, E.K.Hulet, R.J.Dupzyk, R.W.Lougheed, J.E.Evans Alpha Decay of 255Md, 256Md and 257Md RADIOACTIVITY 255,256,257Md [from 253,254Es(α, xn)]; measured T1/2, Eα, Iα; deduced hindrance factors, α/(α+EC) ratios, lower limit T1/2(SF). 253Es(α, n), (α, 2n), 254Es(α, n), E = 38 MeV; measured relative σ.
doi: 10.1016/0375-9474(71)90708-1
1971HU03 Phys.Rev. Lett. 26, 523 (1971) E.K.Hulet, J.F.Wild, R.W.Lougheed, J.E.Evans, B.J.Qualheim, M.Nurmia, A.Ghiorso Spontaneous-Fission Half-Life of 258Fm and Nuclear Instability RADIOACTIVITY, Fission 258Fm(SF)[from 257Fm(d, p)]; measured T1/2.
doi: 10.1103/PhysRevLett.26.523
1971JO13 Phys.Rev.Lett. 27, 45 (1971) W.John, E.K.Hulet, R.W.Lougheed, J.J.Wesolowski Symmetric Fission Observed in Thermal-Neutron-Induced and Spontaneous Fission of 257Fm RADIOACTIVITY, Fission 257Fm(SF); measured (fragment)(fragment)-coin; deduced mass distributions. NUCLEAR REACTIONS, Fission 257Fm(n, F), E=thermal; measured (fragment)(fragment)-coin; deduced mass distributions.
doi: 10.1103/PhysRevLett.27.45
1970HU17 UCRL-72858 (1970) E.K.Hulet, J.F.Wild, R.W.Lougheed, J.E.Evans, B.J.Qualheim, M.Nurmia, A.Ghiorso Spontaneous-Fission Half-Life of 258Fm and Nuclear Instability
1968HO13 Nucl.Phys. A115, 225 (1968) R.W.Hoff, J.E.Evans, E.K.Hulet, R.J.Dupzyk, B.J.Qualheim Nuclear Decay Properties of 256Fm RADIOACTIVITY 256Fm [from 253Es(α, p), 253Es(α, n)256Md EC]; measured T1/2, Eα, Iα. Reactor-produced target. Isotopically enriched 256Fm. NUCLEAR REACTIONS 255Fm(n, γ), E = reactor spectrum; measured σ. Reactor-produced target.
doi: 10.1016/0375-9474(68)90657-X
1968HO15 Bull.Am.Phys.Soc. 13, No.4, 604, DF6 (1968); Oral Report R.W.Hoff, E.K.Hulet, R.J.Dupzyk, R.W.Lougheed, J.E.Evans Alpha Decay of 255Md, 256Md, and 257Md NUCLEAR STRUCTURE 256Md, 257Md, 255Md; measured not abstracted; deduced nuclear properties.
1968HU06 Bull.Am.Phys.Soc. 13, No.4, 604, DF7 (1968); Oral Report E.K.Hulet, A.Ghiorso, R.W.Lougheed, J.E.Evans, J.D.Brady, R.W.Hoff, R.E.Stone, B.J.Qualheim Discovery of 258Md NUCLEAR STRUCTURE 258Md; measured not abstracted; deduced nuclear properties.
1968ST02 J.Inorg.Nucl.Chem. 30, 2003 (1968) Radiochemical Determination of the Alpha Half-Life of 241Am NUCLEAR STRUCTURE 241Am; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(68)80190-3
1967HU04 UCRL-70636 (1967); Priv.Comm. (September 1967) Nuclear Decay Properties of Separated Isotopes of Mendelevium and Fermium NUCLEAR STRUCTURE Fm, Md; measured not abstracted; deduced nuclear properties.
1967WO01 J.Opt.Soc.Am. 57, 550 (1967) E.F.Worden, E.K.Hulet, R.Lougheed, J.G.Conway Nuclear Spin of 249Bk from the Hyperfine Structure in its Emission Spectrum NUCLEAR STRUCTURE 249Bk; measured not abstracted; deduced nuclear properties.
doi: 10.1364/JOSA.57.000550
1966HO01 Phys.Rev. 148, 1192 (1966); See keynumber 1966RG01 R.W.Hoff, C.P.Bailey, G.W.Barton, G.H.Coleman, M.S.Coops, J.E.Evans, B.A.Hannon, W.N.Hayes, R.A.Heckman, E.K.Hulet, R.W.Lougheed, R.J.Morrow, R.S.Newbury, B.J.Qualheim, R.Quong, E.H.Stearns, H.D.Wilson, J.P.Balagna, J.W.Barnes, G.A.Cowan, W.R.Daniels, B.J.Dropesky, G.P.Ford, J.S.Gilmore, S.B.Helmick, D.C.Hoffman, J.D.Knight, G.W.Knobeloch, C.J.Orth, T.T.Shull, H.L.Smith, W.G.Warren, K.Wolfsberg, F.Asaro, J.Burnett, B.B.Cunningham, S.M.Fried, J.T.Haley, A.Ghiorso, J.Green, R.Latimer, F.T.McCarthy, H.V.Michel, M.C.Michel, D.F.Mosier, T.C.Parsons, I.Perlman, J.E.Rees, J.C.Wallmann, R.F.Barnes, L.J.Basile, H.Diamond, P.R.Fields, A.M.Friedman, E.P.Horowitz, J.K.Lerner, D.N.Metta, J.Milsted, R.K.Sjoblom, C.M.Stevens Nuclear Decay Properties of Heavy Nuclides Produced in Thermonuclear Explosions - Par and Barbel Events RADIOACTIVITY 251,252,253,254Cf, 255Es, 257,258Fm(α), 250Cm(SF), 251Bk, 252Cm(β-) [from U(n, F), U(n, X), E ∼ 2 MeV]; measured decay products, Eα, Iα; deduced α-particles energies, α-decay branchings, T1/2. Two low-yield thermonuclear explosions, the Par and Barbel events, chemical separation of products. NUCLEAR REACTIONS Cm(n, X)249Cf/250Cf/252Cf/252Cf/253Cf/254Cf/253Es/254Es/255Es, E thermal; measured reaction products, Eα, Iα, Eβ, Iβ; deduced isotopic abundances. Cm irradions, reactor.
doi: 10.1103/PhysRev.148.1192
1964AS11 Priv.Comm., quoted by 1964Hy02 unpublished (1964) F.Asaro, F.S.Stephens, Jr., J.M.Hollander, E.K.Hulet, R.W.Hoff, I.Perlman
1964HU02 Phys.Rev.Letters 13, 343 (1964) E.K.Hulet, R.W.Hoff, J.E.Evans, R.W.Lougheed 79-Day Fermium Isotope of Mass 257 NUCLEAR STRUCTURE 257Fm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.13.343
1961HU18 Priv.Comm., quoted by 1964Hy02, unpublished (1961) RADIOACTIVITY 248Cm; measured Eα, Iα. Magnetic spectrograph.
1959HO02 J.Nuclear Energy 8, 224 (1959) R.W.Hoff, E.K.Hulet, M.C.Michel Branching Ratio of 242mAm Decay
1958HO98 J.Nuclear Energy 8, 224 (1958) R.W.Hoff, E.K.Hulet, M.C.Michel Branching Ratio of 242mAm Decay Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12578. 1957HU06 Priv.Comm., quoted by 1958ST50, unpublished (1957)
1957HU70 Phys.Rev. 107, 1294 (1957) E.K.Hulet, R.W.Hoff, H.R.Bowman, M.C.Michel Thermal-Neutron Fission Cross Sections for Isotopes of Plutonium, Americium, and Curium
doi: 10.1103/PhysRev.107.1294
1956HU27 Phys.Rev. 102, 182 (1956) New Isotope of Berkelium
doi: 10.1103/PhysRev.102.182
1956HU97 Phys.Rev. 102, 1621 (1956) E.K.Hulet, H.R.Bowman, M.C.Michel, R.W.Hoff Thermal-Neutron Fission Cross Section Of Pu240 NUCLEAR REACTIONS 240Pu(n, f), E=0.0253 eV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 13466.
doi: 10.1103/PhysRev.102.1621
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
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
1953HU60 Thesis, Univ.California (1953); UCRL-2283 (1953) An Investigation of the Isotopes of Berkelium and Californium
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
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
1950RE55 Phys.Rev. 80, 467 (1950) F.L.Reynolds, E.K.Hulet, K.Street, Jr. Mass-Spectrographic Identification of Cm243 and Cm244
doi: 10.1103/PhysRev.80.467
Back to query form |