NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Nix Found 63 matches. 2003YA13 Nucl.Phys. A721, 449c (2003) M.Yamaga, M.Dorochenko, T.Inagaki, N.Ishihara, G.Y.Lim, T.Morimoto, H.Okuno, K.Omata, T.Sato, M.Sekimoto, Y.Yoshimura, A.Ajimura, T.Ikei, Y.Ikemoto, M.Nomachi, T.Oba, K.Sakashita, Y.Sugaya, T.Yamanaka, M.Itaya, T.Iwata, T.Hariu, M.Moriya, Y.Tajima, M.Yamamoto, H.Yoshida, Y.Yoshida, A.Lednev, J.Nix, G.Perdue, E.Pod, M.Rawtajizak, Y.Wah, H.Watanabe, V.Baranov, N.Khomouov, A.Kurilin, G.Macharashvili, A.Moissenko, Z.Tsamalaidze, Y.Akune, Y.Fujioka, N.Kawakubo, S.Kobayashi, T.Kojima, J.K.Ahn, H.S.Lee, S.Y.Lee, T.Shinkawa, Y.B.Hsiung, T.Nakano KL → π0νν-bar experiment at KEK 12-GeV PS - E391a-
doi: 10.1016/S0375-9474(03)01096-0
1998NI13 Phys.Rev. C58, 2303 (1998) Low Freeze-Out Temperature and High Collective Velocities in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(Si, X), E at 14.6 GeV/c/nucleon; analyzed multiplicity distributions, two-particle correlations; deduced parameter dependences, source freeze-out temperature, related features. Nine-parameter expanding source model.
doi: 10.1103/PhysRevC.58.2303
1997MO25 At.Data Nucl.Data Tables 66, 131 (1997) Nuclear Properties for Astrophysical and Radioactive-Ion-Beam Applications NUCLEAR STRUCTURE Z=8-136; A=16-339; calculated, compiled total binding energy, one-, two-neutron, proton separation energies, pairing gaps, odd-nucleon parity, spin projection. Folded-Yukawa single particle potential, Lipkin-Nogami approximation. RADIOACTIVITY Z=8-136; A=16-339; calculated, compiled β-, α-decay Q, T1/2. Folded-Yukawa single particle potential, Lipkin-Nogami approximation.
doi: 10.1006/adnd.1997.0746
1997MO34 Z.Phys. A359, 251 (1997) P.Moller, J.R.Nix, P.Armbruster, S.Hofmann, G.Munzenberg Single-Particle Enhancement of Heavy-Element Production NUCLEAR REACTIONS 208Pb(50Ti, X), (68Zn, X), (70Zn, X), E not given; calculated fusion, fission potential barriers; deduced microscopic effects. Macroscopic-microscopic model, superheavy element production.
doi: 10.1007/s002180050399
1996CH20 Phys.Rev. C54, 866 (1996) Realistic Expanding Source Model for Invariant One-Particle Multiplicity Distributions and Two-Particle Correlations in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(Si, X), E=14.6 GeV/c/nucleon; analyzed invariant one-particle multiplicity distributions, two-particle correlations data, relativistic collisions. Realistic expanding source model.
doi: 10.1103/PhysRevC.54.866
1995CH48 Phys.Rev. C52, 2694 (1995) Extracting Source Parameters from Gaussian Fits to Two-Particle Correlations
doi: 10.1103/PhysRevC.52.2694
1995IW03 Nucl.Phys. A596, 329 (1995) A.Iwamoto, P.Moller, J.R.Nix, H.Sagawa Collisions of Deformed Nuclei: A path to the far side of the superheavy island NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E(cm) ≈ 55-70 MeV; calculated fusion σ(E), potential energy surface; deduced colliding nuclei deformation, orientation role. RADIOACTIVITY 288Og(α) [from 186W(104Ru, X), E=362.3 MeV]; 300122, 301122(α) [from 186W(116Cd, X), E=398 MeV]; 293Lv(α) [from 248Cm(48Ca, X), E=212.56 MeV]; 294120(α) [from 186W(110Pd, X), E=376.2 MeV]; calculated Q(α).
doi: 10.1016/0375-9474(95)00394-0
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
1994MO31 J.Phys.(London) G20, 1681 (1994) Stability of Heavy and Superheavy Elements NUCLEAR STRUCTURE 260Rf, 258No, 260,259Md, 258Fm; compiled, reviewed fission fragment mass, kinetic energy distribution data. Z=70-130; N=110-190; compiled, reviewed ground state microscopic corrections, α-decay T1/2, β-decay Gamow-Teller component information, Qα, Qβ, many other aspects, other nuclei; deduced heavy, superheavy elements stability features.
doi: 10.1088/0954-3899/20/11/003
1994MO52 J.Alloys and Compounds 213/214, 43 (1994) Applications of a global nuclear structure model to studies of the heaviest elements NUCLEAR STRUCTURE 272,288Ds; calculated mass excess, Coulomb redistribution effects, α-decay and fission T1/2. 254,255Fm, 255,256Md, 256,257No, 257,258Lr, 258,259Rf, 259,260Db, 260,261Sg, 261,262Bh; calculated Qα. 258Fm; calculated potential energy surface for fission. Finite-range droplet model.
doi: 10.1016/0925-8388(94)90879-6
1992MO01 Nucl.Phys. A536, 20 (1992) Nuclear Pairing Models NUCLEAR STRUCTURE Z ≤ 100; N ≤ 160; calculated proton, neutron pairing gap energies. 94Sr; calculated proton pairing gap summation interval dependence. BCS, Lipkin-Nogami pairing models.
doi: 10.1016/0375-9474(92)90244-E
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
1992MO22 Nucl.Phys. A549, 84 (1992) Stability and Decay of Nuclei at the End of the Periodic System NUCLEAR STRUCTURE Z=80-120; N=120-190; calculated α-, β+, β-decay T1/2, EC-, Gamow-Teller β-decay Q-values. 252Fm, 272Ds; calculated proton, single particle states. 258Fm; calculated fission path potential energy surface. Mass model with Coulomb redistribution effects.
doi: 10.1016/0375-9474(92)90068-U
1990MO30 Nucl.Phys. A520, 369c (1990) Global Nuclear-Structure Calculations NUCLEAR STRUCTURE N ≤ 160; calculated β-decay T1/2, ground state masses, pairing gaps. Macroscopic, microscopic approach.
doi: 10.1016/0375-9474(90)91161-J
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
1988MA04 Nucl.Phys. A476, 1 (1988) New Model of the Average Neutron and Proton Pairing Gaps NUCLEAR STRUCTURE 250Cf, 150Sm, 50Cr; N ≤ 160; calculated neutron, proton pairing gaps. 150Eu; calculated residual interaction vs finite difference order.
doi: 10.1016/0375-9474(88)90370-3
1988MO19 At.Data Nucl.Data Tables 39, 213 (1988) Nuclear Masses from a Unified Macroscopic-Microscopic Model NUCLEAR STRUCTURE A=16-318; calculated masses. Macroscopic-microscopic model. ATOMIC MASSES A=16-318; calculated masses. Macroscopic-microscopic model.
doi: 10.1016/0092-640X(88)90022-8
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
1986CA04 Nucl.Phys. A452, 381 (1986) Effect of Dissipation on Ternary Fission in very Heavy Nuclear Systems NUCLEAR STRUCTURE A=100-300; calculated ternary fission fragment translational kinetic energy vs mass, dissipation dependence. Macroscopic dynamical model.
doi: 10.1016/0375-9474(86)90204-6
1986GA12 Phys.Lett. 176B, 312 (1986) A.Gavron, A.Gayer, J.Boissevain, H.C.Britt, J.R.Nix, A.J.Sierk, P.Grange, S.Hassani, H.A.Weidenmuller, J.R.Beene, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, G.A.Petitt, C.Butler Neutron Emission Prior to Fission NUCLEAR REACTIONS 142Nd(16O, F), E=207 MeV; measured fission(fragment)n-coin, σ(En, θn); deduced post, prior fission neutron multiplicity relationship. 158Er deduced fission barrier, other parameters, reduced nuclear dissipation coefficient limit.
doi: 10.1016/0370-2693(86)90170-X
1986GR09 Phys.Rev. C34, 209 (1986) P.Grange, S.Hassani, H.A.Weidenmuller, A.Gavron, J.R.Nix, A.J.Sierk Effect of Nuclear Dissipation on Neutron Emission Prior to Fission NUCLEAR REACTIONS 142Nd(16O, F), E=207 MeV; calculated neutron emission multiplicity prior to fission. 158Er deduced saddle to scission time vs reduced dissipation coefficient, Γf vs t. Bohr-Wheeler statistical model.
doi: 10.1103/PhysRevC.34.209
1986MA67 Radiat.Eff. 96, 103 (1986) D.G.Madland, R.J.Labauve, J.R.Nix Comparisons of Four Representations of the Prompt Neutron Spectrum for the Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); analyzed prompt neutron spectra following fission; calculated threshold integral σ.
doi: 10.1080/00337578608211722
1986MO03 Z.Phys. A323, 41 (1986) P.Moller, G.A.Leander, J.R.Nix On the Stability of the Transeinsteinium Elements NUCLEAR STRUCTURE Z>100; calculated Q(α), fission T1/2, ground state property microscopic corrections; deduced 288100, 299100 superheavy high stability.
1986NI06 Radiat.Eff. 92, 263 (1986) J.R.Nix, D.G.Madland, A.J.Sierk Effect of Fission Dynamics on the Spectra and Multiplicities of Prompt Fission Neutrons NUCLEAR REACTIONS 235U(n, F), E=0.53 MeV; calculated prompt fission neutron spectra vs E; deduced multiple-chance fission role. Unified macroscopic-microscopic method. NUCLEAR STRUCTURE 240Pu; calculated beyond fission saddle point dynamical evolution; deduced surface plus window dissipation role. Unified macroscopic-microscopic model.
doi: 10.1080/00337578608208336
1985KU15 Z.Phys. A321, 455 (1985) Calculation of the Nuclear Inertia in a Generalized Cranking Model NUCLEAR STRUCTURE 240Pu; calculated spheroidal deformation inertia. Generalized cranking model.
doi: 10.1007/BF01411980
1984BE27 Phys.Scr. 29, 402 (1984) R.Bengtsson, P.Moller, J.R.Nix, Jing-ye Zhang Nuclear Shapes and Shape Transitions NUCLEAR STRUCTURE A=16-279; calculated potential energy surfaces, ground state masses, shapes. Macroscopic Yukawa plus exponential model.
doi: 10.1088/0031-8949/29/5/002
1984HA19 J.Phys.(London) G10, L87 (1984) J.H.Hamilton, A.V.Ramayya, C.F.Maguire, R.B.Piercey, R.Bengtsson, P.Moller, J.R.Nix, Jing-ye Zhang, R.L.Robinson, S.Frauendorf Effects of Reinforcing Shell Gaps on the Competition between Spherical and Highly Deformed Shapes NUCLEAR STRUCTURE A=70-80, 100; analyzed data systematics; deduced neutron, proton shell gap reinforcement, nuclear shape coexistence in the A=75 region.
doi: 10.1088/0305-4616/10/5/001
1984KU17 Nucl.Phys. A426, 353 (1984) Generalized Cranking Model for Collective Nuclear Motion NUCLEAR STRUCTURE 240Pu; calculated translational, rotational moment of inertia vs pairing gap. Collective motion, generalized cranking model.
doi: 10.1016/0375-9474(84)90112-X
1984LE12 Phys.Rev. C30, 416 (1984) G.A.Leander, J.Dudek, W.Nazarewicz, J.R.Nix, Ph.Quentin Single-Particle Levels in the Doubly Magic 132Sn and 100Sn Nuclei NUCLEAR STRUCTURE 56Ni, 100,132Sn, 208Pb; calculated single particle binding energies. Woods-Saxon, folded Yukawa, Skyrme interaction models.
doi: 10.1103/PhysRevC.30.416
1984NI09 Nucl.Phys. A424, 239 (1984) J.R.Nix, A.J.Sierk, H.Hofmann, F.Scheuter, D.Vautherin Stationary Fokker-Planck Equation Applied to Fission Dynamics NUCLEAR STRUCTURE 158Yb, 213At; calculated fission barrier height, excitation energy. Stationary Fokker-Planck fission dynamics treatment. NUCLEAR REACTIONS 209Bi(α, F), E=120 MeV; calculated mean kinetic energy at scission point vs dissipation strength following fission. 150Nd(20Ne, 2n), E=176, 239 MeV; calculated saddle to scission time vs dissipation strength following residual nucleus fission. Stationary Fokker-Planck fission dynamics treatment.
doi: 10.1016/0375-9474(84)90184-2
1984NI15 Nucl.Phys. A428, 161c (1984) Dynamics of Fission and Heavy Ion Reactions NUCLEAR REACTIONS 208Pb(58Fe, X), E(cm)=238-363 MeV; calculated mass transfer vs angular momentum, capture σ vs E. 142Nd(16O, F), E=208 MeV; calculated mean saddle to scission time vs dissipation strength for fission. Unified macroscopic, microscopic description.
doi: 10.1016/0375-9474(84)90249-5
1984SC43 Phys.Lett. 149B, 303 (1984) F.Scheuter, C.Gregoire, H.Hofmann, J.R.Nix Fission-Fragment Kinetic-Energy Distributions from a Two-Dimensional Fokker-Planck Equation NUCLEAR REACTIONS 209Bi(α, F), E not given; calculated fission fragment kinetic energy distribution, variance vs temperature. Two-dimensional Fokker-Planck equation.
doi: 10.1016/0370-2693(84)90411-8
1983DA13 Phys.Rev. C28, 679 (1983) K.T.R.Davies, A.J.Sierk, J.R.Nix Dynamical Thresholds for Compound-Nucleus Formation in Symmetric Heavy-Ion Reactions NUCLEAR REACTIONS 110Pd(110Pd, X), E not given; calculated compound nucleus formation dynamical thresholds.
doi: 10.1103/PhysRevC.28.679
1982MA06 Phys.Rev. C25, 918 (1982) Excitation Energy at Scission in Thermal-Neutron-Induced Fission NUCLEAR REACTIONS, Fission 233,235U(n, F), E=thermal; analyzed γ-, neutron yields, fission fragment mass distribution odd-even effect; deduced scission point internal excitation energy. One-body dissipation, two-body viscosity models.
doi: 10.1103/PhysRevC.25.918
1982MA14 Nucl.Sci.Eng. 81, 213 (1982) New Calculation of Prompt Fission Neutron Spectra and Average Prompt Neutron Multiplicities NUCLEAR REACTIONS, Fission 235U(n, F), E=0.53-15 MeV; 229Th, 239Pu, 249Cf(n, F), E=thermal; calculated prompt fission σ(En), average neutron multiplicities. Evaporation theory.
doi: 10.13182/NSE82-5
1981LA18 Nucl.Phys. A368, 352 (1981) Two-Dimensional Calculation of Sub-Barrier Heavy-Ion Fusion Cross Sections NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=95-109 MeV; calculated σ(fusion, E). Two-dimensional potential energy surface, monopole, quadrupole Coulomb interaction energies, exponential Yukawa interaction.
doi: 10.1016/0375-9474(81)90690-4
1981MO24 At.Data Nucl.Data Tables 26, 165 (1981) Atomic Masses and Nuclear Ground-State Deformations Calculated with a New Macroscopic Model COMPILATION A=16-279; calculated atomic masses, ground state deformation. Macroscopic-microscopic model.
doi: 10.1016/0092-640X(81)90003-6
1981ST26 Phys.Rev.Lett. 47, 1807 (1981) H.Stocker, C.Riedel, Y.Yariv, L.P.Csernai, G.Buchwald, G.Graebner, J.A.Maruhn, W.Greiner, K.Frankel, M.Gyulassy, B.Schurmann, G.Westfall, J.D.Stevenson, J.R.Nix, D.Strottman Nuclear Fluid Dynamics Versus Intranuclear Cascade- Possible Evidence for Collective Flow in Central High-Energy Nuclear Collisions NUCLEAR REACTIONS 238U(20Ne, p), E=393 MeV/nucleon; calculated σ(θ, Ep); deduced collective flow effects. Different collision models.
doi: 10.1103/PhysRevLett.47.1807
1980NI01 Phys.Rev. C21, 396 (1980) Macroscopic Description of Isoscalar Giant Multipole Resonances NUCLEAR STRUCTURE 208Pb; calculated energy, Γ of T=0, GMR. Distorted-Fermi-surface macroscopic model.
doi: 10.1103/PhysRevC.21.396
1980SC29 Z.Phys. A297, 289 (1980) G.Schutte, P.Moller, J.R.Nix, A.J.Sierk Fission with Microscopic Energy Dissipation RADIOACTIVITY, Fission 236U; calculated neutron, proton single particle energies, excitation of pair states, microscopic energy dissipation. Nonadiabatic BCS formalism.
1980SI06 Phys.Rev. C21, 982 (1980) Fission in a Wall-and-Window One-Body-Dissipation Model RADIOACTIVITY 236U (SF); calculated most probable fission-fragment kinetic E. Wall, window one-body dissipation model.
doi: 10.1103/PhysRevC.21.982
1979KR08 Phys.Rev. C20, 992 (1979) H.J.Krappe, J.R.Nix, A.J.Sierk Unified Nuclear Potential for Heavy-Ion Elastic Scattering, Fusion, Fission, and Ground-State Masses and Deformations NUCLEAR REACTIONS 12C(α, X), 28Si(16O, X), 208Pb(84Kr, X), E not given; calculated HI interaction potential. 28Si(16O, 16O), E=37.7, 81.0, 215.2 MeV; calculated σ(θ). 27Al(32S, X), 62Ni(35Cl, X), 208Pb(16O, X); calculated compound nuclear σ, fission barrier heights, ground-state masses. Unified nuclear potential model.
doi: 10.1103/PhysRevC.20.992
1978KO02 Phys.Rev. C17, 111 (1978) T.Kodama, R.A.M.S.Nazareth, P.Moller, J.R.Nix Exact Calculation of the Penetrability for a Simple Two-Dimensional Heavy-Ion Fusion Barrier NUCLEAR REACTIONS 100Mo(100Mo, X); calculated fusion σ, penetrability for simple two-dimensional fusion barrier.
doi: 10.1103/PhysRevC.17.111
1977AM01 Phys.Rev.Lett. 38, 1055 (1977) A.A.Amsden, J.N.Ginocchio, F.H.Harlow, J.R.Nix, M.Danos, E.C.Halbert, R.K.Smith, Jr. Comparison of Macroscopic and Microscopic Calculations of High-Energy 20Ne + 238U Collisions NUCLEAR REACTIONS 238U(20Ne, X), E=250 MeV/nucleon; calculated σ(θ) for outgoing protons.
doi: 10.1103/PhysRevLett.38.1055
1977AM02 Phys.Rev. C15, 2059 (1977) A.A.Amsden, F.H.Harlow, J.R.Nix Relativistic Nuclear Fluid Dynamics NUCLEAR REACTIONS 238U(20Ne, X), E=0.25, 2.1 GeV/nucleon; calculated σ, time evolution of matter distribution. Hydrodynamic model.
doi: 10.1103/PhysRevC.15.2059
1977DA16 Phys.Rev. C16, 1890 (1977) K.T.R.Davies, R.A.Managan, J.R.Nix, A.J.Sierk Rupture of the Neck in Nuclear Fission NUCLEAR STRUCTURE 252Cf, 236U; calculated fission parameters.
doi: 10.1103/PhysRevC.16.1890
1977MO03 Nucl.Phys. A281, 354 (1977) Potential-Energy Surfaces for Asymmetric Heavy-Ion Reactors NUCLEAR STRUCTURE 8Be, 32S, 80Kr, 108Cd, 140Nd, 172Hf, 200Po, 220U, 248Fm; calculated potential energy surfaces.
doi: 10.1016/0375-9474(77)90031-8
1977NI02 Phys.Rev. C15, 2072 (1977) Calculation of Compound-Nucleus Cross Sections for Symmetric Very-Heavy-Ion Reactions NUCLEAR REACTIONS 100Mo(100Mo, X), 110Pd(110Pd, X), 124Sn(124Sn, X); calculated compound nucleus σ. Liquid-drop model, hydrodynamical model.
doi: 10.1103/PhysRevC.15.2072
1977SI13 Phys.Rev. C16, 1048 (1977) Effect of the Finite Range of the Nuclear Force on the Dynamics of Fission and Heavy-Ion Collisions NUCLEAR REACTIONS 150Nd(150Nd, X); calculated fission dynamics for 236U, superheavy systems.
doi: 10.1103/PhysRevC.16.1048
1976DA08 Phys. Rev. C13, 2385 (1976) K.T.R.Davies, A.J.Sierk, J.R.Nix Effect of Viscosity on the Dynamics of Fission NUCLEAR STRUCTURE 236U, 252Cf; calculated effect of viscosity on fission dynamics.
doi: 10.1103/PhysRevC.13.2385
1976KO01 Phys.Rev. C13, 209 (1976) Microscopic Calculation of Nuclear Dissipation NUCLEAR STRUCTURE 236U fission; calculated microscopically energy dissipated between saddle point, scission. Monopole pairing force, time dependent wave function of BCS form, correspondence with Landau-Zener formula, nuclear viscosity, axially symmetric, reflection-asymmetric deformations.
doi: 10.1103/PhysRevC.13.209
1976ME02 Phys.Rev. C13, 182 (1976) H.W.Meldner, G.A.Cowan, J.R.Nix, R.W.Stoughton How to Detect the Heaviest Man-Made Isotopes NUCLEAR STRUCTURE A > 200; calculated allowed β-decay T1/2.
doi: 10.1103/PhysRevC.13.182
1976MO25 Phys.Rev.Lett. 37, 1461 (1976) Calculated Half-Lives of Superheavy Nuclei Near 354126 RADIOACTIVITY, Fission 354126; calculated Eα, Eβ, T1/2, fission barrier, T1/2(SF).
doi: 10.1103/PhysRevLett.37.1461
1976MO31 Nucl.Phys. A272, 502 (1976) Macroscopic Potential-Energy Surfaces for Symmetric Fission and Heavy-Ion Reactions NUCLEAR STRUCTURE 8Be, 32S, 80Kr, 108Cd, 140Nd, 172Hf, 200Po, 220U, 248Fm; calculated potential energy surfaces.
doi: 10.1016/0375-9474(76)90345-6
1974MO17 Nucl.Phys. A229, 269 (1974) Calculation of Fission Barriers with the Droplet Model and Folded Yukawa Single-Particle Potential NUCLEAR STRUCTURE 240Pu, 250Cm; calculated single particle energies. A=88-108; calculated fission barrier equilibrium points. Fm, Cf, Cm, Pu, U, Th, 212,210Po, 198Hg, 188,186Os calculated fission barrier heights.
doi: 10.1016/0375-9474(74)90788-X
1974MO18 Nucl.Phys. A229, 292 (1974) P.Moller, S.G.Nilsson, J.R.Nix Calculated Ground-State Properties of Heavy Nuclei NUCLEAR STRUCTURE 208Pb, 231Th, 233Pa, 240Pu, 245Cm, 249Bk; calculated single particle energies. A=68-108 calculated ground state deformations, single particle corrections.
doi: 10.1016/0375-9474(74)90789-1
1974NI04 Nucl.Phys. A222, 221 (1974) S.G.Nilsson, J.R.Nix, P.Moller, I.Ragnarsson How Much of a Bubble Is There in 184Hg (Question) NUCLEAR STRUCTURE 184Hg; calculated shape.
doi: 10.1016/0375-9474(74)90389-3
1973BR04 Phys.Rev. C7, 801 (1973) H.C.Britt, M.Bolsterli, J.R.Nix, J.L.Norton Fission Barriers Deduced from the Analysis of Fission Isomer Results
doi: 10.1103/PhysRevC.7.801
1972BO10 Phys.Rev. C5, 1050 (1972) M.Bolsterli, E.O.Fiset, J.R.Nix, J.L.Norton New Calculation of Fission Barriers for Heavy and Superheavy Nuclei NUCLEAR STRUCTURE, Fission 208Pb, 240Pu; calculated single-particle energies. 188Os, 210Po, 240Pu; calculated fission barrier heights. 240Pu, 236,244,248Pu, 232,236,240,244Th, 240,244,248,252Cf, 244,248,252,256No, Element-110, Element-114, Element-118, Element-122; calculated potential energy vs symmetric-deformation coordinate.
doi: 10.1103/PhysRevC.5.1050
1972FI18 Nucl.Phys. A193, 647 (1972) Calculation of Half-Lives for Superheavy Nuclei RADIOACTIVITY, Fission A > 200; calculated T1/2(SF), T1/2(α), T1/2(β), fission barriers.
doi: 10.1016/0375-9474(72)90346-6
1971BO32 Phys.Rev.Lett. 27, 681 (1971) M.Bolsterli, E.O.Fiset, J.R.Nix, J.L.Norton Shape of the Island of Superheavy Nuclei NUCLEAR STRUCTURE, Fission Ds; Z=114, 118, 122; calculated fission barriers.
doi: 10.1103/PhysRevLett.27.681
1969NI06 Nucl.Phys. A132, 60 (1969) A Discussion of the Secondary-Minimum Hypothesis for Spontaneously Fissioning Isomers
doi: 10.1016/0375-9474(69)90612-5
1969WY02 Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1263 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1169 (1970) S.Wycech, A.Sobiczewski, Z.Szymanski, S.G.Nilsson, J.R.Nix, H.F.Tsang, C.Gustafson, P.Moller, B.Nilsson Microscopic Values for the Mass Parameter of Heavy and Superheavy Nuclei NUCLEAR STRUCTURE 228,230,232,234Th, 230,232,234,236,238,240U, 234,236,238,240,242,244,246Pu, 238,240,242,244,246,248,250,252Cm, 244,246,248,250,252,254,256Cf, 248,250,252,254,256,258,260Fm, 250,252,254,256,258No, 258,260,262Rf; calculated mass parameter.
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