NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = G.D.Adeev Found 62 matches. 2017MA17 Eur.Phys.J. A 53, 79 (2017); Erratum Eur.Phys.J. A 53, 144 (2017) K.Mazurek, P.N.Nadtochy, E.G.Ryabov, G.D.Adeev Fission fragment distributions within dynamical approach RADIOACTIVITY 224Th, 248,250Cf(SF); calculated fission, deformation, shapes, fission fragment mass distribution, charge distribution, angular distribution anisotropy. 224Th, 248Cf, 254Fm, 264Rf(SF); calculated angular distribution anisotropy. Langevin equations with statistical description of nuclear evaporation. Compared with available data. NUCLEAR REACTIONS 232Th(16O, f), E=128 MeV;238U(12C, f), E calculated fission fragment mass-energy distribution. 12C(93Nb, f), E=1060 MeV;144,154Sm(18O, f), E=158.8 MeV;197Au(18O, f), E=158.4 MeV;208Pb(16O, f), E=108 MeV;232Th(16O, f), E=128 MeV;238U(18O, f), E=159 MeV;240Pu(20Ne, f), E=174 MeV;246Cm(18O, f), E=102.5 MeV; calculated fission fragment mass distribution, variance of the distribution, neutron multiplicity, fragment kinetic energy. 27Al(86Kr, f), E=5.9, 10.6 MeV/nucleon;232Th(20Ne, f), E=1.25 MeV/nucleon;238U(22Ne, f), E=132, 162 MeV; calculated fission σ, mass and charge distribution. FRLDM (Finite-Range Liquid Drop Model), LSD (Lublin-Strasbourg Drop); compared with available data.
doi: 10.1140/epja/i2017-12262-1
2016NA46 Eur.Phys.J. A 52, 308 (2016) P.N.Nadtochy, E.G.Ryabov, A.V.Cheredov, G.D.Adeev Dissipation of the tilting degree of freedom in heavy-ion-induced fission from four-dimensional Langevin dynamics NUCLEAR STRUCTURE 248Cf; calculated fission barrier vs I, vs K using four-dimensional Langevin fission dynamics. NUCLEAR REACTIONS 183W, 232Th(16O, F), E=90-160 MeV; calculated fission fragment mass distribution, variance, neutron mean multiplicity, mean total kinetic energy, unnormalized σ(θ). 188Os(16O, F), E=84, 89, 94, 99 MeV; calculated fusion-fission σ(θ) using four-dimensional Langevin fission dynamics.
doi: 10.1140/epja/i2016-16308-6
2015RY03 Acta Phys.Pol. B46, 579 (2015) E.G.Ryabov, P.N.Nadtochy, G.D.Adeev Analysis of Experimental Data from Fusion-fission Reactions Within Four-dimensional Langevin Dynamics RADIOACTIVITY 224Th, 248Cf, 252Fm(SF); calculated deformation-dependent parameters, mean kinetic energy, fission fragment mass variance and fission fragment mean fragment total kinetic energy variance. 4-D model.
doi: 10.5506/APhysPolB.46.579
2014NA03 Phys.Rev. C 89, 014616 (2014) P.N.Nadtochy, E.G.Ryabov, A.E.Gegechkori, Yu.A.Anischenko, G.D.Adeev Incorporation of a tilting coordinate into the multidimensional Langevin dynamics of heavy-ion-induced fission: Analysis of experimental data from fusion-fission reactions NUCLEAR REACTIONS 93Nb(12C, X)105Ag*, E=1060 MeV; 144Sm(18O, X)162Yb*, E=158.8 MeV; 18O 154Sm(18O, X)172Yb*, E=158.8 MeV; 184W(16O, X)200Pb*, E=91.6, 97.7, 102.5, 107.9 MeV; 197Au(18O, X)215Fr*, E=158.4 MeV; 208Pb(16O, X)224Th*, E=108 MeV; 232Th(16O, X)248Cf*, E=128 MeV; 238U(16O, X)254Fm*, E=90, 96, 110, 114, 130, 140, 148, 215, 250 MeV; 248Cm(16O, X)264Rf*, E=110, 130, 148 MeV; 240Pu(20Ne, X)260Rf*, E=142, 174 MeV; 246Cm(18O, X)264Rf*, E=102.5 MeV; 238U(18O, X)256Fm*, E=159 MeV; calculated fission rates, fission time distributions, fission fragment charge and mass-energy distributions (MEDs), mean total kinetic energy, mean multiplicity of prescission neutrons, and anisotropy of fission fragment angular distributions. 4D dynamical model based on the 3D model with the inclusion of tilting degree of freedom into Langevin dynamics. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.014616
2012NA12 Phys.Rev. C 85, 064619 (2012) P.N.Nadtochy, E.G.Ryabov, A.E.Gegechkori, Yu.A.Anischenko, G.D.Adeev Four-dimensional Langevin dynamics of heavy-ion-induced fission NUCLEAR REACTIONS 208Pb(16O, X)224Th*, E=90, 110, 130, 148, 215 MeV; 232Th(16O, X)248Cf*, E=90, 95, 120, 140, 160 MeV; calculated Helmholtz free energy (F), second derivative of F with respect to the mass asymmetry coordinate (stiffness), saddle-point configuration quadrupole moments, fusion-fission cross section, evaporation residue cross section, prescission neutron multiplicity, fission fragment angular distributions. Four-dimensional Langevin dynamics of heavy-ion induced fission with dynamical evolution of orientation degree of freedom (K coordinate). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.064619
2011AN03 Acta Phys.Pol. B42, 493 (2011) Yu.A.Anischenko, A.E.Gegechkori, G.D.Adeev Fission Rate and Time of Highly Excited Nuclei in Multi-dimensional Stochastic Calculations NUCLEAR REACTIONS 208Pb(16O, X)224Th, E=90 MeV; calculated fission rate, T1/2. Four-dimensional stochastic approach.
doi: 10.5506/APhysPolB.42.493
2011AN05 Phys.Atomic Nuclei 74, 341 (2011); Yad.Fiz. 74, 361 (2011) Yu.A.Anischenko, A.E.Gegechkori, G.D.Adeev Effect of the orientation degree of freedom on the rate and time of fission of highly excited nuclei NUCLEAR REACTIONS 197Au(14N, X)211Rn, E=102, 110 MeV; 208Pb(16O, X)224Th, E=90, 110, 130, 148, 215 MeV; 232Th(16O, X)248Cf, E=90, 95, 120, 140, 160 MeV; 238U(16O, X)254Fm, E=90, 110, 130, 148, 215 MeV; calculated mean fission time and mean prescission-neutron multiplicity. Four-dimensional dynamical model.
doi: 10.1134/S1063778811030033
2008BO02 Nucl.Phys. A799, 56 (2008) M.V.Borunov, P.N.Nadtochy, G.D.Adeev Nuclear scission and fission-fragment kinetic-energy distribution: Study within three-dimensional Langevin dynamics NUCLEAR STRUCTURE 138Nd, 172Yb, 186Os, 187Ir, 210Tl, 201Bi, 210Po, 213At, 233Pa, 229Np, 237,240Pu, 244Cm, 248Cf, 256Fm, 260Rf; calculated fission fragment energy distribution parameters for different scission criteria.
doi: 10.1016/j.nuclphysa.2007.11.002
2008GE05 Phys.Atomic Nuclei 71, 2007 (2008); Yad.Fiz. 71, 2041 (2008) A.E.Gegechkori, Yu.A.Anischenko, P.N.Nadtochy, G.D.Adeev Impact of non-Markovian effects on the fission rate and time
doi: 10.1134/S1063778808120028
2008HI13 Phys.Atomic Nuclei 71, 1361 (2008); Yad.Fiz. 71, 1389 (2008) R.M.Hiryanov, A.V.Karpov, G.D.Adeev Stochastic model of angular distributions of fragments originating from the fission of excited compound nuclei NUCLEAR REACTIONS 208Pb, 209Bi, 232Th, 238U, 248Cm(16O, X), E=85-148 MeV; 224Th, 225Pa, 248Cm, 254Fm, 264Rf; calculated fusion σ, fission fragments angular aniostropy, pre-scission neutron multiplicities; stochastic model of fission; Langevin equation; Monte Carlo algorithm.
doi: 10.1134/S106377880808005X
2008RY05 Phys.Rev. C 78, 044614 (2008) E.G.Ryabov, A.V.Karpov, P.N.Nadtochy, G.D.Adeev Application of a temperature-dependent liquid-drop model to dynamical Langevin calculations of fission-fragment distributions of excited nuclei NUCLEAR STRUCTURE 156,159,162Yb, 184,185Pt, 195Hg, 224Th, 244Cm, 248Cf, 254Fm, 264Rf; calculated potential energy surfaces, σ, fission fragment distributions using stochastic approach.
doi: 10.1103/PhysRevC.78.044614
2007KA01 J.Phys.(London) G34, 255 (2007) A.V.Karpov, R.M.Hiryanov, A.V.Sagdeev, G.D.Adeev Dynamical treatment of fission fragment angular distribution NUCLEAR REACTIONS 232Th, 238U, 248Cf(16O, F), E=90-160 MeV; calculated fission fragment angular distributions. Dynamical approach.
doi: 10.1088/0954-3899/34/2/007
2007RU16 Phys.Atomic Nuclei 70, 1679 (2007); Yad.Fiz. 70, 1724 (2007) A.Ya.Rusanov, G.D.Adeev, M.G.Itkis, A.V.Karpov, P.N.Nadtochy, V.V.Pashkevich, I.V.Pokrovsky, V.S.Salamatin, G.G.Chubarian Investigation of the reaction 208Pb(18O, f): Fragment spins and phenomenological analysis of the angular anisotropy of fission fragments NUCLEAR REACTIONS 208Pb(18O, F), E=78.0-198.5 MeV; measured Eγ, Iγ, average multiplicity from fission fragments. Deduced total spins of fission fragments.
doi: 10.1134/S106377880710002X
2007RY01 Phys.Part. and Nucl.Lett. 4, 29 (2007); Pisma Zh.Fiz.Elem.Chast.Atom.Yadra No.1 [137], 54 (2007) E.G.Ryabov, A.V.Karpov, G.D.Adeev Analysis of Angular Momentum Dependence of Fission Fragment Mass-Energy Distribution Within Langevin Dynamics NUCLEAR STRUCTURE 162Yb, 184Pt, 244Cm; calculated fission fragments mass-energy distributions vs excitation energy. Three-dimensional Langevin calculations.
doi: 10.1134/S1547477107010062
2006RY01 Nucl.Phys. A765, 39 (2006) E.G.Ryabov, A.V.Karpov, G.D.Adeev Influence of angular momentum on fission fragment mass distribution: Interpretation within Langevin dynamics NUCLEAR STRUCTURE 244Cm, 184Pt, 162Yb; calculated fission fragment mass distributions, angular momentum dependence, fission barriers, neutron binding energies, prescission neutron multiplicities, fission and neutron widths. Finite-range liquid-drop model, three-dimensional Langevin dynamics, comparisons with data.
doi: 10.1016/j.nuclphysa.2005.10.005
2005AD38 Fiz.Elem.Chastits At.Yadra 36, 712 (2005); Physics of Part.and Nuclei 36, 378 (2005) G.D.Adeev, A.V.Karpov, P.N.Nadtochy, D.V.Vanin Multidimensional Stochastic Approach to the Fission Dynamics of Excited Nuclei
2005NA39 Phys.Rev. C 72, 054608 (2005) Dynamical interpretation of average fission-fragment kinetic energy systematics and nuclear scission NUCLEAR STRUCTURE 142Ce, 224Th, 256Fm; calculated fission trajectories in deformation space. A=119-256; calculated average fission fragment energy, scission deformation parameters. Dynamical approach.
doi: 10.1103/PhysRevC.72.054608
2005RY04 Yad.Fiz. 68, 1583 (2005); Phys.Atomic Nuclei 68, 1525 (2005) Static and Statistical Properties of Hot Rotating Nuclei in a Macroscopic Temperature-Dependent Finite-Range Model NUCLEAR STRUCTURE 109Ag, 224Th, 306Lv; Z=50-112; calculated level density parameters. 220Fr, 240Pu; A=60-300; calculated fission barrier parameters. Other properties of hot rotating nuclei discussed.
doi: 10.1134/1.2053335
2004KA29 Nucl.Phys. A734, E37 (2004) A.V.Karpov, P.N.Nadtochy, E.G.Ryabov, D.V.Vanin, G.D.Adeev Level-density parameter of hot rotating fissioning nuclei within the finite-range liquid-drop model NUCLEAR STRUCTURE Z=47-116; 109Ag, 306Lv; calculated level density parameters. Finite-range liquid-drop model.
doi: 10.1016/j.nuclphysa.2004.03.014
2003AD09 Yad.Fiz. 66, 647 (2003); Phys.Atomic Nuclei 66, 618 (2003) Probabilistic Scission of a Fissile Nucleus into Fragments NUCLEAR REACTIONS 194Pt(12C, X), E=99 MeV; 197Au(18O, X), E=158.8 MeV; 232Th(12C, X), E=97 MeV; 240Pu(20Ne, X), E=142 MeV; calculated fragment mass distributions, neutron multiplicity following compound nucleus fission. Probabilistic scission mechanism, Strutinsky criterion. Comparison with data. NUCLEAR STRUCTURE 206Po, 215Fr, 244Cm, 260Rf; calculated fission fragment mass distributions, neutron multiplicity following compound nucleus formation. 244Cm; calculated energy of fission fragment interaction vs distance and neck radius. Probabilistic scission mechanism, Strutinsky criterion.
doi: 10.1134/1.1568813
2003KA44 J.Phys.(London) G29, 2365 (2003) A.V.Karpov, P.N.Nadtochy, E.G.Ryabov, G.D.Adeev Consistent application of the finite-range liquid-drop model to Langevin fission dynamics of hot rotating nuclei NUCLEAR STRUCTURE 109Ag, 224Th, 306Lv; calculated level density parameters vs deformation. 186Os; calculated fission barrier heights vs temperature and angular momentum. Generalized finite-range liquid drop model. NUCLEAR REACTIONS 181Ta(19F, X), 208Pb(16O, X), E ≈ 20-200 MeV; calculated prescission neutron multiplicity, fission probability. Generalized finite-range liquid drop model.
doi: 10.1088/0954-3899/29/10/305
2003NA11 Yad.Fiz. 66, 1240 (2003); Phys.Atomic Nuclei 66, 1203 (2003) P.N.Nadtochy, A.V.Karpov, D.V.Vanin, G.D.Adeev Reduction Coefficient in Surface-Plus-Window Dissipation: Analysis of Experimental Data from Fusion-Fission Reactions within a Stochastic Approach NUCLEAR REACTIONS 209Bi(α, X), 194Pt, 232Th(12C, X), 170Er, 182W, 208Pb, 232Th(16O, X), 144,154Sm, 197Au, 238U(18O, X), 232Th, 240Pu(20Ne, X), 169Tm(36Ar, X), E ≈ 80-215 MeV; calculated fission probabilities, fragment angular and mass distributions, neutron multiplicities. Three-dimensional stochastic approach.
doi: 10.1134/1.1586438
2002KA36 Eur.Phys.J. A 14, 169 (2002) Langevin Description of Charge Fluctuations in Fission of Highly Excited Nuclei NUCLEAR REACTIONS 232Th(α, F), E not given; calculated fission fragments charge variance distribution as function of nuclear viscosity. Stochastical approach.
doi: 10.1140/epja/i2002-10004-2
2002KA54 Yad.Fiz. 65, 1637 (2002); Phys.Atomic Nuclei 65, 1596 (2002) Langevin Description of the Charge Distribution of Fragments Originating from the Fission of Excited Nuclei NUCLEAR REACTIONS 232U(α, F), E*=110 MeV; calculated fission fragment charge distribution. Stochastic approach, Langevin equations.
doi: 10.1134/1.1508691
2002NA15 Yad.Fiz. 65, 832 (2002); Phys.Atomic Nuclei 65, 799 (2002) P.N.Nadtochy, A.V.Karpov, G.D.Adeev Langevin Fission Dynamics of Hot Rotating Nuclei: Systematic application to Z2/A = 34-42 heavy nuclei NUCLEAR REACTIONS 194Pt, 232Th(12C, F), E ≈ 99 MeV; 197Au, 238U(18O, F), E=159 MeV; 208Pb(16O, F), E=108 MeV; 209Bi, 240Pu(20Ne, F), E ≈ 150 MeV; calculated fission fragment energy and mass distributions, prescission neutron yields. Langevin dynamics.
doi: 10.1134/1.1481471
2002NA16 Phys.Rev. C65, 064615 (2002) P.N.Nadtochy, G.D.Adeev, A.V.Karpov More Detailed Study of Fission Dynamics in Fusion-Fission Reactions within a Stochastic Approach NUCLEAR REACTIONS 154Sm, 197Au, 238U(18O, X), E=159 MeV; 169Tm(36Ar, X), E=205 MeV; 232Th(20Ne, X), E=215 MeV; calculated fission fragments average kinetic energy, prescission neutron multiplicity, fragment mass distributions following compound nucleus fission. Three-dimensional stochastic approach.
doi: 10.1103/PhysRevC.65.064615
2001KA30 Phys.Rev. C63, 054610 (2001) A.V.Karpov, P.N.Nadtochy, D.V.Vanin, G.D.Adeev Three-Dimensional Langevin Calculations of Fission Fragment Mass-Energy Distribution from Excited Compound Nuclei NUCLEAR REACTIONS 194Pt(12C, F), E=99 MeV; 208Pb(16O, F), E=108 MeV; 232Th(12C, F), E=97 MeV; 240Pu(20Ne, F), E=142, 174 MeV; calculated fission fragments energy, mass distributions, prescission neutron multiplicities. Three-dimensional Langevin dynamics, comparisons with data.
doi: 10.1103/PhysRevC.63.054610
2001NA26 Yad.Fiz. 64, No 5, 926 (2001); Phys.Atomic Nuclei 64, 861 (2001) P.N.Nadtochy, A.V.Karpov, D.V.Vanin, G.D.Adeev Mass-Energy Distribution of Fragments from the Fission of Excited Nuclei within Three-Dimenstional Langevin Dynamics NUCLEAR REACTIONS 194Pt(12C, F), E=99 MeV; calculated fission fragments kinetic energy and mass distributions. Three-dimensional Langevin dynamics.
doi: 10.1134/1.1378876
2000KU37 Yad.Fiz. 63, No 11, 1978 (2000); Phys.Atomic Nuclei 63, 1885 (2000) R.S.Kurmanov, G.I.Kosenko, G.D.Adeev New Formula for Calculating Coulomb Energies in the Liquid-Drop Model
doi: 10.1134/1.1326978
2000VA27 Yad.Fiz. 63, No 11, 1957 (2000); Phys.Atomic Nuclei 63, 1865 (2000) D.V.Vanin, P.N.Nadtochy, G.I.Kosenko, G.D.Adeev Langevin Description of Mass Distributions of Fragments Originating from the Fission of Excited Nuclei NUCLEAR REACTIONS 232Th(12C, F), E=97 MeV; 249Cf(16O, F), E=145 MeV; calculated fission fragment mass distributions, neutron yields following compound nucleus decay. Liquid drop model.
doi: 10.1134/1.1326976
1999VA06 Phys.Rev. C59, 2114 (1999) D.V.Vanin, G.I.Kosenko, G.D.Adeev Langevin Calculations of Fission Fragment Mass Distribution in Fission of Excited Nuclei NUCLEAR STRUCTURE 105Ag, 117I, 124Ba, 210Po, 244Cm, 249Fm; calculated potential energy surfaces, fission fragment mass distributions, variances vs fissility parameter. Two-dimensional stochastic approach, two liquid drop models compared. NUCLEAR REACTIONS 165Ho(40Ar, F), E=180-280 MeV; calculated fission fragment mass distributions. Two-dimensional stochastic approach, two liquid drop models compared. Comparison with data.
doi: 10.1103/PhysRevC.59.2114
1998KO12 Yad.Fiz. 61, No 3, 416 (1998); Phys.Atomic Nuclei 61, 356 (1998) G.I.Kosenko, D.V.Vanin, G.D.Adeev Multiplicity of Postscission Neutrons Produced in the Fission of Excited Nuclei
1998KO68 Yad.Fiz. 61, No 12, 2142 (1998); Phys.Atomic Nuclei 61, 2031 (1998) G.I.Kosenko, D.V.Vanin, G.D.Adeev Application of the Combined Dynamics-Evaporation Model to the Fission of Excited Nuclei NUCLEAR REACTIONS 232Th, 238U(α, F), E=47-220 MeV; calculated neutron, proton, alpha multiplicities, fission fragments mean kinetic energy; deduced charged particle emission role in fragment deexcitation. Comparisons with data. Combined dynamics-evaporation model.
1997KO14 Yad.Fiz. 60, No 3, 404 (1997); Phys.Atomic Nuclei 60, 334 (1997) G.I.Kosenko, I.G.Cagliari, G.D.Adeev Using the Combined Dynamical Evaporation Approach to Describe Fission Induced by Heavy Ions NUCLEAR REACTIONS 184W(16O, F), E=288 MeV; 181Ta(19F, F), E=124 MeV; 197Au(18O, F), E=159 MeV; calculated fission fragment mean kinetic energy, variance prescission n-, α-, p-multiplicities, postscission n-multiplicities. Combined dynamical evaporation approach.
1989AD06 Nucl.Phys. A502, 405c (1989) Theory of Macroscopic Fission Dynamics NUCLEAR STRUCTURE 205At, 252Fm; calculated fission trajectories. Macroscopic fission dynamics.
doi: 10.1016/0375-9474(89)90679-9
1989AD08 Yad.Fiz. 50, 1242 (1989) G.D.Adeev, I.I.Gonchar, V.V.Pashkevich, O.I.Serdyuk Relaxation Times of Collective Modes in Fission of Excited Nuclei NUCLEAR STRUCTURE 235U; calculated different fission mode relaxation times.
1988AD10 Fiz.Elem.Chastits At.Yadra 19, 1229 (1988); Sov.J.Part.Nucl 19, 529 (1988) G.D.Adeev, I.I.Gonchar, V.V.Pashkevich, N.I.Pischasov, O.I.Serdyuk Diffusion Model of the Formation of Fission-Fragment Distributions NUCLEAR STRUCTURE 252Fm, 205At, 235U; calculated dynamical trajectories at fission. 198Pb, 240U; calculated fission fragment energy, mass distributions. 200Hg, 230Th, 252Cf, 212At; calculated fission fragment energy excess, distribution asymmetry coefficient. Other fission characteristics discussed.
1988SA28 Yad.Fiz. 48, 42 (1988) G.Saupe, O.I.Serdyuk, G.D.Adeev, V.V.Pashkevich Adiabatic Description of Mass and Energy Distributions of Fission Fragments NUCLEAR REACTIONS 232Th(40Ar, F), E=301 MeV; 249Cf(22Ne, F), E=174 MeV; calculated fission fragment mass distribution. Adiabatic distribution.
1987SE16 Yad.Fiz. 46, 710 (1987); Sov.J.Nucl.Phys. 46, 399 (1987) O.I.Serdyuk, G.D.Adeev, I.I.Gonchar, V.V.Pashkevich, N.I.Pischasov Mass-Energy Distribution of Fission Fragments in the Diffusion Model NUCLEAR STRUCTURE 234Pu, 209Po, 200Tl; calculated fission fragment kinetic energy vs dispersion. 206Pb, 223Ra, 252Cf, 212At, 198Hg; calculated fission fragment kinetic energy excess, asymmetry coefficient.
1986AD03 Yad.Fiz. 43, 1137 (1986) G.D.Adeev, I.I.Gonchar, L.A.Marchenko, N.I.Pischasov Fluctuative-Dissipative Dynamics of Formation of Mass Distribution of Fission Fragments NUCLEAR STRUCTURE 248Fm, 205At, 221Pa; calculated fission fragment mass distribution variances; deduced mass dispersion angular momentum dependence. Fokker-Planck equation.
1986AD09 Yad.Fiz. 44, 897 (1986); Sov.J.Nucl.Phys. 44, No.4, 579 (1986) On the Passage of a fissioning Nucleus through the Barrier to Scission in a Multidimensional Diffusion Model NUCLEAR STRUCTURE 205At; calculated fission saddle point distribution function dispersions, energy surface dynamical trajectories. Multi-dimensional diffusion model.
1985AD02 Z.Phys. A320, 451 (1985) The Dynamical Description of the Mass Distribution of Fission Fragments NUCLEAR STRUCTURE 248Cf; calculated potential energy dependence on parameters. 252Fm, 248Cf, 236U, 212At, 196Pt; calculated fission stiffness coefficient vs elongation parameters. Pt, Tl, Pb, Bi, Rn, Ra, At, Ac, Th, U, Pu, Cm, Cf, Fm; calculated fission stiffness coefficient vs fissility parameter. 238U; calculated fission fragment mass distribution variance vs friction parameter. Fokker-Planck equation.
doi: 10.1007/BF01415722
1985AD07 Yad.Fiz. 42, 42 (1985) G.D.Adeev, I.I.Gonchar, L.A.Marchenko Fluctuation-Dissipation Dynamics of Formation of Charge Distribution of Fission Fragments NUCLEAR STRUCTURE 236U; calculated fission fragment charge distribution parameters. Fokker-Planck equation.
1985AD13 Z.Phys. A322, 479 (1985) A Simplified Two-Dimensional Diffusion Model for Calculating the Fission-Fragment Kinetic-Energy Distribution NUCLEAR STRUCTURE 200Tl, 206Bi, 212At, 230Th, 236U, 240Pu, 244Cm, 248Cf, 252Fm; calculated fission fragment kinetic energy distribution, stiffness coefficient, fissility parameter. Two-dimensional diffusion model.
doi: 10.1007/BF01412083
1984AD08 Yad.Fiz. 40, 869 (1984) Fluctuation-Dissipation Dynamics of Formation of the Energy Distribution of Fission Fragments NUCLEAR STRUCTURE 230Th, 236U, 240Pu, 244Cm, 248Cf, 252Fm; analyzed fission fragment kinetic energy variance dependence on inertia, friction parameters; deduced fissility parameter, nonequilibrium fission roles. Fokker-Planck equation.
1983AD04 Yad.Fiz. 37, 1113 (1983) Dynamical Description of Variances in Kinetic Energy of Fission Fragments NUCLEAR STRUCTURE 236U; analyzed fission fragment energy distribution; deduced nonequilibrium effects in fission. Dynamical variances description.
1982AD01 Yad.Fiz. 35, 27 (1982) Influence of Diffused Distribution of the Nucleon Density on Effective Moments of Inertia of Fissionable Nuclei NUCLEAR STRUCTURE 173Lu, 179Ta, 182W, 186,187,188,190Os, 192,193,194,196Pt, 197Au, 196,198,199,200Hg, 201Tl, 209Bi, 212,211,210,208Po, 213At; calculated effective moment of inertia. Droplet model, nuclear surface diffuseness.
1981AD06 Yad.Fiz. 33, 90 (1981) G.D.Adeev, L.A.Phylipenko, P.A.Cherdantsev Analysis of Isotopic and Charge Distributions in Reactions with Heavy Ions NUCLEAR REACTIONS 238U(11B, X), (22Ne, X), (40Ca, X), (40Ar, X), E not given; analyzed σ(fragment A, Z); deduced fission mechanism dominance. Total fusion, fission following deep inelastic transfer models.
1979AD07 Yad.Fiz. 30, 933 (1979); Sov.J.Nucl.Phys. 30, 485 (1979) G.D.Adeev, L.A.Filipenko, P.A.Cherdantsev Description of the Fission Barriers of Pre-Actinide Nuclei in the Droplet Model NUCLEAR STRUCTURE 213At, 208,210,211,212Po, 209Bi, 201Tl, 200,199,198,196Hg, 197Au, 196,194,193,192Pt, 190,188,187,186Os, 182W, 179Ta, 172Lu; calculated fission barriers. Droplet model.
1979AD09 Izv.Akad.Nauk SSSR, Ser.Fiz. 43, 2417 (1979); Bull.Acad.Sci.USSR, Phys.Ser. 43, No.11, 149 (1979) G.D.Adeev, L.A.Filipenko, P.A.Cherdantsev Isotopic Distribution of Products in Reactions with Heavy Ions NUCLEAR REACTIONS 238U(22Ne, F), E not given; 238U(40Ca, F), E=218-306 MeV; calculated fragment yield. Rb, Au deduced isotopic distribution. Complete fusion, deep inelastic transfer mechanism.
1978AD01 Izv.Akad.Nauk SSSR, Ser.Fiz. 42, 208 (1978); Bull.Acad.Sci.USSR, Phys.Ser. 42, No.1, 181 (1978) G.D.Adeev, A.M.Kazantseva, V.A.Matusevich, I.P.Chernov Inelastic Scattering of 3He Ions on 12C Nuclei NUCLEAR REACTIONS 12C(3He, 3He'), E=18, 20, 24.5 MeV; measured σ(E, θ). 12C levels deduced deformation parameter. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1161. 1977AD01 Phys.Lett. 66B, 11 (1977) Statistical Calculations of the Charge Distribution in Fission NUCLEAR STRUCTURE 236U, 240Pu; calculated fission fragment yield.
doi: 10.1016/0370-2693(77)90600-1
1977AD06 Phys.Lett. 72B, 30 (1977) Droplet Model Description of the Division of Charge in Fission NUCLEAR STRUCTURE 238U; calculated charge division in fission. Droplet model.
doi: 10.1016/0370-2693(77)90055-7
1977AD07 Yad.Fiz. 26, 683 (1977); Sov.J.Nucl.Phys. 26, 361 (1977) G.D.Adeev, A.M.Kazantseva, V.V.Kozyr, V.A.Matusevich, I.P.Chernov The (3He, 4He) Reaction in the Carbon Isotopes NUCLEAR REACTIONS 12C(3He, α), E=18, 20, 24.5 MeV; 13C(3He, α), E=18, 20 MeV; measured σ(θ). Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1139. 1976AD01 Yad.Fiz. 23, 30 (1976); Sov.J.Nucl.Phys. 23, 15 (1976) G.D.Adeev, L.A.Filipenko, P.A.Cherdantsev Polarizability of Nuclear Matter in a Fissioning Nucleus and Charge Distribution of Fission Fragments NUCLEAR STRUCTURE 236,238U, 252Cf; calculated potential energy. Strutinsky method.
1975AD06 Yad.Fiz. 21, 491 (1975); Sov.J.Nucl.Phys. 21, 258 (1975) Application of the Strutinskii Method to the Investigation of Shell Effects in the Density of Excited Nuclear States NUCLEAR STRUCTURE 48,50Ti, 50,52Cr, 56,58Fe, 56,58,60,62,64Ni, 144,146Nd, 148,150Sm, 158,156Gd, 162,164Dy, 168,170Er, 172,174Yb, 178,180Hf, 184W, 188Os, 208Pb, 238U, 242Pu, 246Cm, 252Cf; calculated level density.
1972AD06 Phys.Lett. 39B, 485 (1972) Dependence of Mass Fission Asymmetry on the Compound Excitation Energy NUCLEAR STRUCTURE 238U; calculated potential energy surface vs nuclear temperature.
doi: 10.1016/0370-2693(72)90325-5
1972AD16 Yad.Fiz. 16, 919 (1972); Sov.J.Nucl.Phys. 16, 507 (1973) Fission Barriers of Odd Nuclei NUCLEAR STRUCTURE 239U, 241Pu, 242Am, 245Bk, 257Fm; calculated fission barriers using Strutinsky method.
1971AD02 Phys.Lett. 35B, 125 (1971) G.D.Adeev, P.A.Cherdantsev, I.A.Gamalya Energy Surfaces of 238U in Parametrization of Cassinian Ovaloids NUCLEAR STRUCTURE 238U; calculated 3-dimensional energy surface. Strutinsky method.
doi: 10.1016/0370-2693(71)90235-8
1971AD04 Yad.Fiz. 13, 1180 (1971); Sov.J.Nucl.Phys. 13, 679 (1971) G.D.Adeev, I.A.Gamalya, P.A.Cherdantsev Potential Energy of U238 at Asymmetrical Fission in Parametrization of The Nuclear Shape by Means of the Cassini Ovaloid-Type Figures NUCLEAR REACTIONS, Fission 238U(n, F); calculated 3-dimensional potential energy surface. Strutinsky method.
1971AD08 Yad.Fiz. 14, 1144 (1971); Sov.J.Nucl.Phys. 14, 637 (1972) G.D.Adeev, I.A.Gamalya, P.A.Cherdantsev Potential Energy of Heavy Nuclei in Asymmetrical Fission NUCLEAR STRUCTURE, Fission 226Ra, 232Th, 252Cf, 254Cf; calculated fission barriers, potential energy surfaces.
1970AD08 Yad.Fiz. 12, 272 (1970); Sov.J.Nucl.Phys. 12, 148 (1971) G.D.Adeev, I.A.Gamalya, P.A.Cherdantsev Single-Nucleon States and Energy Surfaces of U238 in the Fission Process NUCLEAR STRUCTURE 238U; calculated single-particle states, energy surfaces.
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