NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.J.Dougan Found 21 matches. 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.
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
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
1986BL10 Radiat.Eff. 92, 305 (1986) R.C.Block, D.R.Harris, H.T.Maguire, Jr., C.R.S.Stopa, R.E.Slovacek, J.W.T.Dabbs, R.J.Dougan, R.W.Hoff, R.W.Lougheed Intermediate Structure in the Fission Cross Sections of the Even Curium Isotopes NUCLEAR REACTIONS 244,246,248Cm(n, F), E ≤ 100 keV; analyzed fission σ(E); deduced structure. 245,247,249Cm deduced barrier parameter differences.
doi: 10.1080/00337578608208340
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
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
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
1985MA14 Nucl.Sci.Eng. 89, 293 (1985); see 1985Ma28 H.T.Maguire, Jr., C.R.S.Stopa, R.C.Block, D.R.Harris, R.E.Slovacek, J.W.T.Dabbs, R.J.Dougan, R.W.Hoff, R.W.Lougheed Neutron-Induced Fission Cross-Section Measurements of 244Cm, 246Cm, and 248Cm
doi: 10.13182/NSE85-A18621
1985MA28 Nucl.Sci.Eng. 89, 293 (1985) H.T.Maguire, Jr., C.R.S.Stopa, R.C.Block, D.R.Harris, R.E.Slovacek, J.W.T.Dabbs, R.J.Dougan, R.W.Hoff, R.W.Lougheed Neutron-Induced Fission Cross-Section Measurements of 244Cm, 246Cm, and 248Cm NUCLEAR REACTIONS 244,246,248Cm(n, F), E=0.1 eV-80 keV; measured fission σ(E). 245,247,249Cm deduced intermediate structure evidence.
doi: 10.13182/NSE85-A18621
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
1984BR10 Phys.Rev. C29, 2188 (1984) J.C.Browne, R.M.White, R.E.Howe, J.H.Landrum, R.J.Dougan, R.J.Dupzyk 242mAm Fission Cross Section NUCLEAR REACTIONS 242mAm(n, F), E ≈ 0.001 eV-20 MeV; measured fission σ(E). 243Am deduced resonaces, Γn, ΓF, average level spacing, s-wave strength function. Breit-Wigner single level sum analysis.
doi: 10.1103/PhysRevC.29.2188
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
1983HO21 Nucl.Phys. A407, 193 (1983) R.E.Howe, R.M.White, J.C.Browne, J.H.Landrum, R.J.Dougan, R.W.Lougheed, R.J.Dupzyk Measurement of the Prompt Fission Neutron Multiplicity from the 245Cm(n, f) and 242mAm(n, f) Reactions NUCLEAR REACTIONS 245Cm(n, F), E=0.00005-14000 keV; 242mAm(n, F), E=14 MeV; measured prompt fission neutron multiplicity.
doi: 10.1016/0375-9474(83)90314-7
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
1981HO08 Nucl.Sci.Eng. 77, 454 (1981) R.E.Howe, J.C.Browne, R.J.Dougan, R.J.Dupzyk, J.H.Landrum Fission Neutron Multiplicity for the 242mAm(n, f) Reaction NUCLEAR REACTIONS, Fission 242mAm(n, F), E=0.037-30 MeV; measured neutron multiplicity vs E. Semiempirical model. Liquid benzene scintillator, tof.
doi: 10.13182/NSE81-A18958
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
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