NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = W.J.Swiatecki Found 59 matches. 2010SW01 Phys.Rev. C 81, 019804 (2010) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Reply to "Comment on 'Ratios of disintegration rates for distinct decay modes of an excited nucleus'"
doi: 10.1103/PhysRevC.81.019804
2009SW01 Int.J.Mod.Phys. E18, 747 (2009) Some fission problems CIRCA 1950 AND 2008
doi: 10.1142/S0218301309012835
2008SW01 Phys.Rev. C 78, 054604 (2008) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Ratios of disintegration rates for distinct decay modes of an excited nucleus NUCLEAR REACTIONS 208Pb(58Fe, X); 249Cf(48Ca, X), E<50 MeV; calculated ratios of breakup widths of compound nuclei.
doi: 10.1103/PhysRevC.78.054604
2007SW01 Acta Phys.Pol. B38, 1565 (2007) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Effect of Shell Structure on Saddle Point Masses NUCLEAR STRUCTURE Z=71-120; calculated deviations of experimental and theoretical ground state and fission saddle point masses from their respective macroscopic approximations.
2005SW01 Phys.Rev. C 71, 014602 (2005) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Fusion by diffusion. II. Synthesis of transfermium elements in cold fusion reactions NUCLEAR REACTIONS 208Pb(58Fe, n), (50Ti, n), (54Cr, n), (64Ni, n), (70Zn, n), (65Cu, n), E(cm) ≈ 175-270 MeV; 209Bi(50Ti, n), (64Ni, n), E(cm) ≈ 175-260 MeV; calculated excitation functions. 238U, 244Pu, 243Am, 245,248Cm, 249Cf(48Ca, X), E*=25, 35, 45 MeV; 208Pb(70Zn, X), (76Ge, X), (82Se, X), (86Kr, X), 209Bi(76Ge, X), E*=13-14 MeV; calculated fusion hindrance factors. Comparisons with data.
doi: 10.1103/PhysRevC.71.014602
2005SW02 Phys.Rev. C 71, 047301 (2005) W.J.Swiatecki, A.Trzcinska, J.Jastrzebski Difference of the root-mean-square sizes of neutron and proton distributions in nuclei: Comparison of theory with data NUCLEAR STRUCTURE 40,48Ca, 54,56,57Fe, 58,60,64Ni, 59Co, 90,96Zr, 106,116Cd, 112,116,120,124Sn, 122,124,126,128Te, 208Pb, 209Bi, 232Th, 238U; calculated neutron-proton radius difference. Droplet model, comparison with data.
doi: 10.1103/PhysRevC.71.047301
2004SW01 Int.J.Mod.Phys. E13, 261 (2004) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Calculations of cross sections for the synthesis of super-heavy nuclei in cold fusion reactions NUCLEAR REACTIONS 208Pb, 209Bi(48Ca, X), (50Ti, X), (54Cr, X), (58Fe, X), (62Ni, X), (64Ni, X), (70Zn, X), (76Ge, X), (82Se, X), (86Kr, X), E not given; calculate compound nucleus survival probability. Comparisons with data.
doi: 10.1142/S021830130400203X
2003SW01 Acta Phys.Pol. B34, 2049 (2003) W.J.Swiatecki, K.Siwek-Wilczynska, J.Wilczynski Fusion by diffusion NUCLEAR REACTIONS 208Pb(48Ca, n), (50Ti, n), (54Cr, n), (58Fe, n), (62Ni, n), (64Ni, n), (70Zn, n), (86Kr, n), E* ≈ 12-15 MeV; calculated σ. Statistical diffusion. Comparisons with data.
2003SW02 Acta Phys.Pol. B34, 1901 (2003) On nuclear molecules built up from 132Sn components NUCLEAR STRUCTURE 264Fm; calculated quasi-molecular states features.
2002NI10 Phys.Rev.Lett. 89, 039901 (2002); see also 1999Ni03 V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk Editorial Note: Observation of Superheavy Nuclei Produced in the Reaction of 86Kr with 208Pb
doi: 10.1103/PhysRevLett.89.039901
2002WA24 Phys.Rev. C66, 024317 (2002) D.Ward, R.M.Diamond, W.J.Swiatecki, R.M.Clark, M.Cromaz, M.A.Deleplanque, P.Fallon, A.Goergen, G.J.Lane, I.Y.Lee, A.O.Macchiavelli, W.Myers, F.S.Stephens, C.E.Svensson, K.Vetter Search for the Jacobi shape transition in rapidly rotating nuclei NUCLEAR REACTIONS 50Ti, 64Ni, 96Zr, 124Sn(48Ca, xnypzα), E=195-215 MeV; measured Eγ, Iγ, γγ-coin, multiplicities; deduced quasicontinuum spectrum features, moment of inertia vs angular momentum, possible Jacobi shape transition. 91Nb, 108Cd, 140Nd, 168Yb; deduced collective E2 bump centroids. Gammasphere and 8PI arrays.
doi: 10.1103/PhysRevC.66.024317
2001MY01 Phys.Rev. C63, 034318 (2001) Isospin Dependence of the Nuclear Surface Tension
doi: 10.1103/PhysRevC.63.034318
2001MY02 Acta Phys.Pol. B32, 1033 (2001) At the Extremes of Nuclear Charge and Spin NUCLEAR STRUCTURE 94Mo, 108Cd, 140Nd, 168Yb; calculated γ energy vs angular momentum, deformation features. Thomas-Fermi approach. NUCLEAR REACTIONS 208Pb(50Ti, X), (70Zn, X), (86Kr, X), E*=13 MeV; calculated fusion barrier features.
2001NI02 Nucl.Phys. A682, 98c (2001) V.Ninov, K.E.Gregorich, T.N.Ginter, F.P.Hessberger, R.Krucken, D.M.Lee, W.Loveland, W.D.Myers, J.Patin, M.W.Rowe, N.K.Seward, W.J.Swiatecki, A.Turler, P.A.Wilk Production and Structure of the Heaviest Elements
doi: 10.1016/S0375-9474(00)00627-8
2000ME21 Acta Phys.Pol. B31, 1471 (2000) The Dragon Guarding the Island of Superheavy Nuclei has Dropped His Shield
2000MY01 Phys.Rev. C62, 044610 (2000) Nucleus-Nucleus Proximity Potential and Superheavy Nuclei NUCLEAR REACTIONS 208Pb(50Ti, X), (70Zn, X), (86Kr, X), 142Ce(136Xe, X), E* ≈ 13 MeV; calculated potential energy vs separation, fusion barrier features. Proximity potential, application to superheavy element production.
doi: 10.1103/PhysRevC.62.044610
1999MY01 Phys.Rev. C60, 014606 (1999) Thomas-Fermi Fission Barriers NUCLEAR STRUCTURE Z=70-100; calculated fission barriers. Self-consistent Thomas-Fermi model. Comparison with data.
doi: 10.1103/PhysRevC.60.014606
1999MY02 Phys.Rev. C60, 054313 (1999) Nuclear Diffuseness as a Degree of Freedom. II. An Improved Approach NUCLEAR STRUCTURE 20Ne, 200Hg; calculated neutron, proton densities. A=20-340; calculated surface diffuseness, related features. Thomas-Fermi approach.
doi: 10.1103/PhysRevC.60.054313
1999NI03 Phys.Rev.Lett. 83, 1104 (1999); Erratum Phys.Rev.Lett. 89, 039901 (2002); see also 2002GrZZ V.Ninov, K.E.Gregorich, W.Loveland, A.Ghiorso, D.C.Hoffman, D.M.Lee, H.Nitsche, W.J.Swiatecki, U.W.Kirbach, C.A.Laue, J.L.Adams, J.B.Patin, D.A.Shaughnessy, D.A.Strellis, P.A.Wilk Observation of Superheavy Nuclei Produced in the Reaction of 86Kr with 208Pb NUCLEAR REACTIONS 208Pb(86Kr, n), E=449 MeV; measured α-spectra, (recoil)α-, αα-coin following residual nucleus decay, production σ; deduced evidence for 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg. Gas-filled separator. RADIOACTIVITY 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs(α) [from 208Pb(86Kr, n) and subsequent α-decay]; measured Eα, T1/2.
doi: 10.1103/PhysRevLett.83.1104
1998MY01 Phys.Rev. C57, 3020 (1998); Erratum Phys.Rev. C 74, 029902 (2006) Nuclear Equation of State
doi: 10.1103/PhysRevC.57.3020
1998MY03 Nucl.Phys. A641, 203 (1998) A Model of Nuclear Rotation NUCLEAR STRUCTURE 152,154,156Dy, 160Er, 172Hf, 178Os, 232Th, 236,238U, 240,244Pu, 194Hg, 194Pb, 132Ce; calculated rotational bands transition energies. 135Nd, 126Xe; calculated binding energy vs spin. Phenomenological model.
doi: 10.1016/S0375-9474(98)00463-1
1998MY04 Phys.Rev. C58, 3368 (1998) Nuclear Diffuseness as a Degree of Freedom
doi: 10.1103/PhysRevC.58.3368
1997BL05 Nucl.Phys. A618, 1 (1997) J.Blocki, J.Skalski, W.J.Swiatecki The Excitation of an Independent-Particle Gas by a Time-Dependent Potential Well: Part II
doi: 10.1016/S0375-9474(97)00017-1
1997MY01 Nucl.Phys. A612, 249 (1997) The Congruence Energy: A contribution to nuclear masses, deformation energies and fission barriers NUCLEAR STRUCTURE A=173-252; calculated congruence energy related corrections to saddle point energies, masses, fission barriers.
doi: 10.1016/S0375-9474(96)00328-4
1997MY02 Acta Phys.Pol. B28, 9 (1997) The Nuclear Thomas-Fermi Model with Angular Momentum: Fission barriers, superdeformations, moments of inertia NUCLEAR STRUCTURE 135Nd, 184Hg; calculated binding energy vs angular momentum, deformation; deduced fission barriers angular momentum dependence. 238U, 172Hf, 194Hg, 152Dy; calculated rotational bands moments of inertia. Thomas-Fermi model.
1996BL08 Nucl.Phys. A599, 486 (1996) J.Blocki, C.Jarzynski, W.J.Swiatecki Effect of Dynamical Correlations in a Slowly Pumped Knudsen Gas
doi: 10.1016/0375-9474(95)00498-X
1996BL13 Acta Phys.Pol. B27, 555 (1996) J.Blocki, J.Skalski, Z.Sujkowski, W.J.Swiatecki Giant Monopole Resonances and the Compressibility of Nuclear Matter NUCLEAR STRUCTURE A=20-240; analyzed giant monopole resonance energy data. Two-mode coupling model of isoscalar density oscillations.
1996MY01 Nucl.Phys. A601, 141 (1996) Nuclear Properties According to the Thomas-Fermi Model NUCLEAR STRUCTURE 56Fe, 124Sn, 209Bi; calculated Thomas-Fermi charge distributions. 83,120,167Sn; calculated nucleon density distributions. Z=47-66; calculated Thomas-Fermi mass excess with, without shell corrections. A=8-252; calculated fission barriers. Thomas-Fermi model.
doi: 10.1016/0375-9474(95)00509-9
1996MY02 Acta Phys.Pol. B27, 99 (1996) The Rotating Nuclear Thomas-Fermi Model NUCLEAR STRUCTURE 152Dy, 83Sr; calculated fission barrier vs angular momentum, superdeformed nuclei.
1995BL17 Nucl.Phys. A594, 137 (1995) J.Blocki, J.Skalski, W.J.Swiatecki The Excitation of an Independent-Particle Gas - Classical or Quantal-by a Time-Dependent Potential Well
doi: 10.1016/0375-9474(95)00341-W
1995GH04 Nucl.Phys. A583, 861c (1995) A.Ghiorso, D.Lee, L.P.Somerville, W.Loveland, J.M.Nitschke, W.Ghiorso, G.T.Seaborg, P.Wilmarth, R.Leres, A.Wydler, M.Nurmia, K.Gregorich, R.Gaylord, T.Hamilton, N.J.Hannink, D.C.Hoffman, C.Jarzynski, C.Kacher, B.Kadkhodayan, S.Kreek, M.Lane, A.Lyon, M.A.McMahan, M.Neu, T.Sikkeland, W.J.Swiatecki, A.Turler, J.T.Walton, S.Yashita Evidence for the Synthesis of 267110 Produced by the 59Co + 209Bi Reaction NUCLEAR REACTIONS 209Bi(59Co, n), E ≈ 5.1 MeV/nucleon; measured Eα, production σ; deduced evidence for 267Ds.
doi: 10.1016/0375-9474(94)00775-I
1995GH05 Phys.Rev. C51, R2293 (1995) A.Ghiorso, D.Lee, L.P.Somerville, W.Loveland, J.M.Nitschke, W.Ghiorso, G.T.Seaborg, P.Wilmarth, R.Leres, A.Wydler, M.Nurmia, K.Gregorich, K.Czerwinski, R.Gaylord, T.Hamilton, N.J.Hannink, D.C.Hoffman, C.Jarzynski, C.Kacher, B.Kadkhodayan, S.Kreek, M.Lane, A.Lyon, M.A.McMahan, M.Neu, T.Sikkeland, W.J.Swiatecki, A.Turler, J.T.Walton, S.Yashita Evidence for the Possible Synthesis of Element 110 Produced by the 59Co + 209Bi Reaction NUCLEAR REACTIONS 209Bi(59Co, n), E=5.1 MeV/nucleon; measured implanted recoil Bρ, dE/dx, recoil energy; deduced 267Ds synthesis evidence, production σ.
doi: 10.1103/PhysRevC.51.R2293
1995MO29 At.Data Nucl.Data Tables 59, 185 (1995) P.Moller, J.R.Nix, W.D.Myers, W.J.Swiatecki Nuclear Ground-State Masses and Deformations NUCLEAR STRUCTURE A=16-339; calculated mass excess, ground state deformations. Finite-range droplet macroscopic, folded-Yukawa single particle microscopic models.
doi: 10.1006/adnd.1995.1002
1995MY01 Nucl.Phys. A587, 92 (1995) The Compressibility of Finite Nuclei NUCLEAR STRUCTURE A=10-260; calculated compressibilities for N=Z nuclei. Universal scaling dependence approach.
doi: 10.1016/0375-9474(94)00793-M
1995MY02 Acta Phys.Pol. B26, 111 (1995) The Nuclear Thomas-Fermi Model NUCLEAR STRUCTURE Z=70-108; N=96-156; calculated deformation energies vs constraint parameter. Z=71-98; calculated fission barrier heights. 82,120,170Sn; calculated nucleon density distributions. Statistical Thomas-Fermi model, other nuclei, other aspects studied.
1994BL09 Acta Phys.Pol. B25, 637 (1994) J.Blocki, F.Brut, W.J.Swiatecki Excitation of Quantal Gas in a Time-Dependent Potential
1994SW02 Nucl.Phys. A574, 233c (1994) Nuclear Physics: Macroscopic aspects
doi: 10.1016/0375-9474(94)90048-5
1992MO02 Nucl.Phys. A536, 61 (1992) P.Moller, J.R.Nix, W.D.Myers, W.J.Swiatecki The Coulomb Redistribution Energy as Revealed by a Refined Study of Nuclear Masses NUCLEAR STRUCTURE 16O, 48Ca, 132Sn, 208Pb, 266Mt; calculated Coulomb volume, surface redistribution energies. N ≤ 200; Z ≤ 140; calculated ground state mass vs shape degrees of freedom; deduced Coulomb redistribution energy terms role. Macroscopic, microscopic approach.
doi: 10.1016/0375-9474(92)90245-F
1991MY01 Ann.Phys.(New York) 211, 292 (1991) A Thomas-Fermi Model of Nuclei. II. Fission Barriers and Charge Distributions NUCLEAR STRUCTURE Z=70-108; N=96-156; calculated deformation energies, fission barriers. 56Fe, 124Sn, 208Bi; calculated charge distributions. Thomas-Fermi model.
doi: 10.1016/0003-4916(91)90207-O
1990MY01 Ann.Phys.(New York) 204, 401 (1990) A Thomas-Fermi Model of Nuclei. Part I. Formulation and First Results NUCLEAR STRUCTURE 40Ar, 124Sn, 209Bi; calculated Thomas-Fermi charge distributions. Generalized Seyler-Blanchard effective interaction.
doi: 10.1016/0003-4916(90)90395-5
1989MO03 Nucl.Phys. A492, 349 (1989) P.Moller, J.R.Nix, W.J.Swiatecki New Developments in the Calculation of Heavy-Element Fission Barriers NUCLEAR STRUCTURE 252,256,260,264Fm, 240Pu, 272,290Ds, 259,260Md, 262Db, 272Mt, 258,260Cf, 258,262No, 264Sg, 262Rf; calculated potential energy surfaces. Z=98-109; calculated fission T1/2.
doi: 10.1016/0375-9474(89)90403-X
1989SH37 Chin.J.Nucl.Phys. 11, No. 4, 31 (1989) Theoretical Estimates of Spontaneous Radioactive Decay by Emission of Heavy Ion-Branching Ratios to α-Decay Larger than 10-16 RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 230Th, 231Pa, 232U(24Ne); 232Th(26Ne); 233U(25Ne); 237Np(30Mg); 240Pu, 241Am(34Si); calculated α to heavy-ion branching ratios.
1988MO20 At.Data Nucl.Data Tables 39, 225 (1988) P.Moller, W.D.Myers, W.J.Swiatecki, J.Treiner Nuclear Mass Formula with a Finite-Range Droplet Model and a Folded-Yukawa Single-Particle Potential NUCLEAR STRUCTURE A=16-318; calculated masses. Macroscopic-microscopic model. ATOMIC PHYSICS A=16-318; calculated masses. Macroscopic-microscopic model.
doi: 10.1016/0092-640X(88)90023-X
1987MO16 Nucl.Phys. A469, 1 (1987) P.Moller, J.R.Nix, W.J.Swiatecki Calculated Fission Properties of the Heaviest Elements RADIOACTIVITY 252,254,256,258,260,264Fm, 252,254,256,258,260,262Cf, 250,256,258Cm, 256,254,260,262,264,266No, 256Rf, 258Rf, 260Rf, 262Rf, 264Rf, 268Rf, 260Sg, 264Sg, 266Sg, 270Sg, 264Hs, 270Hs, 272Hs(SF); calculated fission fragment elongation σ, fission T1/2. Macroscopic-microscopic model.
doi: 10.1016/0375-9474(87)90083-2
1987SH04 Nucl.Phys. A464, 205 (1987) Estimates of the Influence of Nuclear Deformations and Shell Effects on the Lifetimes of Exotic Radioactivities RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(α), (14C); 230Th, 231Pa, 232U(α), (24Ne); 237Np(α), (30Mg); 240Pu, 241Am(α), (34Si); 233U(α), (25Ne); 232Th(α), (26Ne); calculated exotic decay T1/2, penetrability integrals, parent deformations, exotic to α-decay branching ratios; deduced deformations, shell effects.
doi: 10.1016/0375-9474(87)90335-6
1987SW01 Phys.Rev.Lett. 58, 1184 (1987) Superdeformed Band in 152Dy as Evidence for the Centrifugal Solidification of a Rotating Nucleus NUCLEAR STRUCTURE 152Dy; analyzed superdeformed rotational spectrum; deduced centrifugal solidification evidence. Macroscopic model.
doi: 10.1103/PhysRevLett.58.1184
1986DO03 Nucl.Phys. A451, 189 (1986) C.O.Dorso, W.D.Myers, W.J.Swiatecki Droplet-Model Electric Dipole Moments NUCLEAR STRUCTURE 222Th, 226Ra; calculated electric dipole moment, proton charge units. Deformed nucleus, droplet model.
doi: 10.1016/0375-9474(86)90410-0
1985BL18 Nucl.Phys. A445, 367 (1985) J.Blocki, K.Grotowski, R.Planeta, W.J.Swiatecki Symmetric Splitting of very Light Systems in the Coalescence and Reseparation Model NUCLEAR REACTIONS 40Ca(12C, X), E=132, 162, 186 MeV; 40Ca(9Be, X), (6Li, X), E not given; calculated trajectories; deduced fusion-fission mechanism. 56Fe, 49Cr, 46V deduced compound states, fission saddle points. Coalescence, reseparation models.
doi: 10.1016/0375-9474(85)90075-2
1985MO12 Nucl.Phys. A440, 89 (1985) K.Mohring, W.J.Swiatecki, M.Zielinska-Pfabe Simple Estimates for Fermi Jets NUCLEAR REACTIONS 158Gd(12C, xn), E=152 MeV; 93Nb(16O, xn), E=204 MeV; calculated jetted neutron σ(En). Fermi jets, two colliding potential wells.
doi: 10.1016/0375-9474(85)90044-2
1985SH01 Phys.Rev.Lett. 54, 300 (1985) Theoretical Estimates of the Rates of Radioactive Decay of Radium Isotopes by 14C Emission RADIOACTIVITY 222,223,224Ra(α), (14C); analyzed α-, 14C-decay branching ratio data. Fragment Coulomb repulsion, nuclear proximity attraction.
doi: 10.1103/PhysRevLett.54.300
1985SH07 Nucl.Phys. A438, 450 (1985) Estimates of Radioactive Decay by the Emission of Nuclei Heavier than α-Particles RADIOACTIVITY 222,223,224Ra(14C), (α); calculated T1/2, penetrability factor ratios.
doi: 10.1016/0375-9474(85)90385-9
1982BJ03 Nucl.Phys. A391, 471 (1982) Dynamical Aspects of Nucleus-Nucleus Collisions NUCLEAR REACTIONS 116Sn, 141Pr(35Cl, X), 109Ag(40Ar, X), 208Pb(26Mg, X), (27Al, X), (48Ca, X), (50Ti, X), (52Cr, X), (58Fe, X), (64Ni, X), E(cm) ≈ 100-250 MeV; calculated σ(evaporation), fast, delayed fission, quasielastic σ vs E. 248Cm, 254Es, 252Cf(48Ca, X), E(cm) ≈ 200-300 MeV; calculated superheavy formation characteristics. Macroscopic theory, touching, conditional, unconditional saddle point configurations.
doi: 10.1016/0375-9474(82)90621-2
1982SW01 Nucl.Phys. A376, 275 (1982) The Dynamics of the Fusion of Two Nuclei NUCLEAR REACTIONS 26Mg, 27Al(208Pb, X), E ≈ 100-200 MeV; 48Ca, 50Ti, 52Cr(208Pb, X), E ≈ 200-300 MeV; 64Ni, 58Fe(208Pb, X), E ≈ 250-400 MeV; calculated σ(fusion) vs E. Schematic one-body dissipation model.
doi: 10.1016/0375-9474(82)90065-3
1980MY01 Nucl.Phys. A336, 267 (1980) Droplet-Model Theory of the Neutron Skin NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,124Sn, 208Pb; calculatged n, p rms radii differences. Droplet model.
doi: 10.1016/0375-9474(80)90623-5
1974CO41 Ann.Phys.(New York) 82, 557 (1974) S.Cohen, F.Plasil, W.J.Swiatecki Equilibrium Configurations of Rotating Charged or Gravitating Liquid Masses with Surface Tensor. II. NUCLEAR REACTIONS 107Ag(20Ne, X), E(cm)=25-205 MeV; calculated impact parameter. 85Rb(20Ne, X), 65Cu(40Ar, X), 48Ti(18O, X), 27Al(16O, X), 12C(12C, X), E not given; calculated fission barrier, neutron binding energy, excitation energy. 105Ag, 66Zn, 43Sc, 24Mg; deduced possible superdeformation. Rotating liquid masses. NUCLEAR STRUCTURE A=1-300; calculated angular momentum where fission barrier would vanish. A=1-200; calculated fission barrier. Rotating liquid masses.
doi: 10.1016/0003-4916(74)90126-2
1966MY02 Nucl.Phys. 81, 1 (1966) Nuclear Masses and Deformations
doi: 10.1016/0029-5582(66)90639-0
1965DI10 Izv.Akad.Nauk SSSR, Ser.Fiz. 29, 1070 (1965); Bull.Acad.Sci.USSR, Phys.Ser. 29, 1073 (1966) R.M.Diamond, N.L.Lark, F.S.Stephens, W.J.Swiatecki High-Spin Rotational States in Some Nuclei
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
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
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