NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Zdeb Found 14 matches. 2023BL04 Phys.Rev. C 108, 044618 (2023) J.M.Blanco, A.Dobrowolski, A.Zdeb, J.Bartel Spontaneous fission half-lives of actinides and superheavy elements
doi: 10.1103/PhysRevC.108.044618
2023PO11 Acta Phys.Pol. B54, 9-A2 (2023) K.Pomorski, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, A.Zdeb, J.Bartel, H.Molique, C.Schmitt, Z.G.Xiao, Y.J.Chen, L.L.Liu Fission Fragment Mass and Kinetic Energy Yields of Fermium Isotopes NUCLEAR STRUCTURE 246,248,250,252,254,256,258,260,262Fm; analyzed available data; deduced the post-fission neutron multiplicities, potential energy surfaces.
doi: 10.5506/APhysPolB.54.9-A2
2021HA45 Phys.Rev. C 104, 064602 (2021) R.Han, M.Warda, A.Zdeb, L.M.Robledo Scission configuration in self-consistent calculations with neck constraints RADIOACTIVITY 258No(SF); calculated nuclear density distribution contours for different neck configurations and in scission regions, potential energy surface (PES) and neck contour in quadrupole-octupole (Q20, Q30) planes; deduced roles of constraint on the neck parameter and nuclear density distributions, scission configurations, potential energy surfaces, pre-scission line and configuration of the asymmetric fission mode in self-consistent mean-field calculations, including pairing, such as Hartree-Fock-Bogoliubov (HFB) approximation.
doi: 10.1103/PhysRevC.104.064602
2021ZD01 Phys.Rev. C 104, 014610 (2021) Description of the multidimensional potential-energy surface in fission of 252Cf and 258No RADIOACTIVITY 252Cf, 258No(SF); calculated potential energy surfaces (PES) in (Q20, Q30), (Q20, Q22) and (Q30, Q40)planes, density distributions, fission barriers, fission fragments and cross sections; deduced multiple solutions for given constraints and transitions between various overlapping potential-energy surfaces. Self-consistent Hartree-Fock-Bogoliubov approach with the D1S parametrization of the Gogny nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.104.014610
2018WA29 Phys.Rev. C 98, 041602 (2018) Cluster radioactivity in superheavy nuclei NUCLEAR STRUCTURE 234U, 258No, 284Cn; calculated potential energy surfaces (PEC) in (Q2, Q3) plane, pre- and post-scission configurations. 224Ra, 228Th, 234U, 238Pu, 244Cm, 248Cf, 254Fm, 258No, 264Rf, 268Sg, 274Hs, 278Ds, 284Cn, 290Fl, 294Lv; calculated cluster radioactivity (CR) fission paths as function of Q2 and Q3, and half-lives using microscopic theory. Comparison with available experimental data. Relevance to cluster decay mode in superheavy nuclei (SHN).
doi: 10.1103/PhysRevC.98.041602
2017ZD01 Phys.Rev. C 95, 054608 (2017) A.Zdeb, A.Dobrowolski, M.Warda Fission dynamics of 252Cf RADIOACTIVITY 252Cf(SF); calculated potential energy surface of 252Cf, tunneling probability, fission fragment mass distributions, mass yields from ground state to excited states, statistical mixing of eigenstates and fission fragment mass distributions. Time-dependent generator coordinate method with the gaussian overlap approximation (TDGCM+GOA) approach.
doi: 10.1103/PhysRevC.95.054608
2016ZD01 Eur.Phys.J. A 52, 323 (2016) A.Zdeb, M.Warda, C.M.Petrache, K.Pomorski Proton emission half-lives within a Gamow-like model RADIOACTIVITY 109I, 113Cs, 131Eu, 145,146,147Tm, 155,156,157Ta, 160,161Re, 166,167Ir, 170,171Au, 177Tl, 141Ho, 146,147Tm, 150,151Lu, 156Ta, 161Re, 166Ir, 177Tl(p); calculated proton emission T1/2 using simple phenomenological Gamow-like formalism; deduced nuclear radius constant parameter. Compared with other formalisms and with data. NUCLEAR STRUCTURE 109I, 131Eu, 177Tl; calculated levels, J, π.
doi: 10.1140/epja/i2016-16323-7
2015PO08 Phys.Scr. 90, 114013 (2015) On spontaneous fission and α-decay half-lives of atomic nuclei RADIOACTIVITY Te, I, Xe, Sm, Gd, Lu, Hf, Ta, W, Re, Os, Ir, Pt, Au, Hg, Dy, Ho, Er, Tm, Yb, Tl, Rn, Pb, Fr, Bi, Ra, Po, Ac, At, Th, Pa, U, Np, Pu, Am, Cm, Bk, Cf, Fm, Md, No, Lr, Rf, Db, Sg, Bh, Hs, Ds, Mt(α), (SF); calculated T1/2. Comparison with experimental data.
doi: 10.1088/0031-8949/90/11/114013
2015WA33 Phys.Scr. 90, 114003 (2015) Fission fragment mass yield deduced from density distribution in the pre-scission configuration RADIOACTIVITY 256,258Fm, 252Cf, 180Hg(SF); calculated potential energy surfaces as well as nuclear shapes; deduced fission fragment mass distributions. Hartree-Fock-Bogoliubov model with the effective Gogny D1S density-dependent interaction.
doi: 10.1088/0031-8949/90/11/114003
2015ZD01 Acta Phys.Pol. B46, 423 (2015) On Systematics of Spontaneous Fission Half-lives RADIOACTIVITY Th, U, Pu, Cm, Cf, Fm, No(SF); analyzed available data; deduced T1/2 systematics.
doi: 10.5506/APhysPolB.46.423
2014ZD01 Acta Phys.Pol. B45, 303 (2014) Alpha Decay Half-lives for Super-heavy Nuclei Within a Gamow-like Model NUCLEAR STRUCTURE Z=100-122; calculated T1/2. Comparison with available data.
doi: 10.5506/APhysPolB.45.303
2014ZD02 Phys.Scr. 89, 054015 (2014) Half-lives of heavy nuclei within simple phenomenological models COMPILATION Th, Pa, U, Np, Pu, Am, Cm, Bk, Cf, Es, Fm, Md, No, Lr(SF), (α); compiled, analyzed T1/2; deduced simple formula for T1/2.Compared with available data.
doi: 10.1088/0031-8949/89/5/054015
2013ZD01 Phys.Rev. C 87, 024308 (2013) Half-lives for α and cluster radioactivity within a Gamow-like model RADIOACTIVITY 188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,206,208,209,210,211,212,213,214,215,216,217,218Po, 193,194,195,196,197,198,199,200,201,202,203,204,205,207,209,211,212,213,214,215,216,217,218,219,220At, 195,196,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222Rn, 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221Fr, 202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,226Ra, 206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225Ac, 209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,232Th, 212,213,214,215,216,217,218,219,220,221,223,224,225,226,227,231Pa, 217,218,219,223,225,226,227,228,229,230,232,233,234,235,236,238U, 226,227,229,230,231,237Np, 229,230,232,234,236,237,238,239,240,242,244Pu, 241,243Am, 234,238,240,242,243,244,245,246,247,248Cm, 247Bk, 240,242,243,244,245,246,248,249,250,251,252Cf, 243,245,247,252,253,254Es, 243,246,247,248,250,251,252,253,254,255,256,257Fm, 246,248,249,255,256,257,258Md, 252,253,254,255,256,257,259No, 253,255,257,258Lr, 255,257,259,261Rf, 257,259,260,262Db, 260,265Sg, 261,262Bh, 265,266Hs, 266Mt, 269,270,271,273,281Ds(α); 221Fr, 221,222,223,224,226Ra, 223,225Ac(14C); 223Ac(15N), 226Th(18O); 228Th(20O); 230U(22Ne); 231Pa(23F); 230,232Th, 231Pa, 232,233,234,235,236U(24Ne); 233,235U(25Ne); 232Th, 234,236U(26Ne); 233,234,236U, 236,238Pu(28Mg); 236U, 237Np, 238Pu(30Mg); 238Pu(32Si); 240Pu, 241Am, 242Cm(34Si); calculated T1/2 for α decay and cluster emissions. Phenomenological model based on Gamow theory with WKB approximation for the penetration of Coulomb barrier. Comparison with experimental values of half-lives.
doi: 10.1103/PhysRevC.87.024308
2013ZD02 Phys.Scr. T154, 014029 (2013) Half-lives for α and cluster radioactivity in a simple model RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C), 226Th(18O), 228Th(20O), 230Th(24Ne), 230U(22Ne), 231Pa(23F), (24Ne), 232Th(24Ne), (25Ne), 232U(24Ne), 233U(24Ne), (25Ne), (28Mg), 234U(24Ne), (25Ne), (28Mg), 235U(24Ne), (25Ne), 236U(24Ne), (25Ne), (28Mg), (30Mg), 236Pu(28Mg), 237Np(30Mg), 238Pu(28Mg), (30Mg), (32Si), 240Pu(34Si), 241Am(34Si), 242Cm(34Si); calculated cluster radioactivity T1/2. Simple phenomenological model based on the WKB theory, comparison with available data.
doi: 10.1088/0031-8949/2013/T154/014029
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