NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Nerlo-Pomorska Found 100 matches. 2023PO07 Phys.Rev. C 107, 054616 (2023) K.Pomorski, B.Nerlo-Pomorska, C.Schmitt, Z.G.Xiao, Y.J.Chen, L.L.Liu Fourier-over-spheroid shape parametrization applied to nuclear fission dynamics NUCLEAR REACTIONS 235U(n, F), E = thermal; calculated fission fragments mass and charge yields, total kinetic energy (TKE) of fission fragments, post-fission neutron multiplicities, fission fragment excitation energy. 3D Langevin code, based on the Fourier-over-spheroid (FoS) shape parametrization, the LSD+Yukawa folded macroscopic-microscopic potential energy landscape, a procedure to account for charge equilibration at scission, and a method to compute the excitation energy available in the primary fragments. Comparison to experimental data. RADIOACTIVITY 246,248,250,252,254,256,258,260,262Fm(SF); calculated fission fragment mass yields distribution, total kinetic energy (TKE) of fission fragments, post-fission neutron multiplicities. Comparison to experimental data. NUCLEAR STRUCTURE 236U, 252,254,256,258,260,262Fm; calculated potential energy surfaces. 240Pu; calculated energy at scission as a function of the heavy fragment charge number, Wigner distribution probability of the fission fragment charge number.
doi: 10.1103/PhysRevC.107.054616
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
2023WA08 Phys.Rev. C 107, L041601 (2023) Y.Wang, F.Guan, X.Diao, M.Wan, Y.Qin, Z.Qin, Q.Wu, D.Guo, D.Si, S.Xiao, B.Zhang, Y.Zhang, B.Tian, X.Wei, H.Yang, P.Ma, R.J.Hu, L.Duan, F.Duan, Q.Hu, J.Ma, S.Xu, Z.Bai, Y.Yang, J.Wang, W.Liu, W.Su, X.Wei, C.-W.Ma, X.Li, H.Wang, F.Wang, Y.Zhang, M.Warda, A.Dobrowolski, B.Nerlo-Pomorska, K.Pomorski, L.Ou, Z.Xiao Observing the ping-pong modality of the isospin degree of freedom in cluster emission from heavy-ion reactions NUCLEAR REACTIONS 208Pb(86Kr, X), E=25 MeV/nucleon; measured reaction products, A=3 isobars in coincidence with the intermediate mass fragments of A=6-11; deduced velocity spectra of 3H and 3He, yields ratios of 3H/3He correlate reversely to the neutron-to-proton ratio N/Z of the intermediate mass fragments. Comparison with ImQMD transport model. Yield ratio 3H/3He exhibits evident anticorrelation with the N/Z of the latter, suggesting the ping-pong modality of the N/Z of the emitted particles. Anti-correlation shows dependence on the slope of the symmetry energy at saturation density. Compact Spectrometer for Heavy IoN Experiment (CSHINE) at the final focal plane of the Radioactive Ion Beam Line at Lanzhou (RIBLL-I).
doi: 10.1103/PhysRevC.107.L041601
2022PO03 Eur.Phys.J. A 58, 77 (2022) K.Pomorski, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, J.Bartel, Z.Xiao, Y.Chen, L.Liu, J.-L.Tian, X.Diao On the stability of superheavy nuclei
doi: 10.1140/epja/s10050-022-00737-3
2021KO43 Chin.Phys.C 45, 124108 (2021) P.V.Kostryukov, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, Z.Xia, Y.Chen, L.Liu, J.-L.Tian, K.Pomorski Potential energy surfaces and fission fragment mass yields of even-even superheavy nuclei NUCLEAR STRUCTURE 254,256,258,260,262Rf, 258,260,262,264,266Sg, 264,266,268,270,272Hs, 276,278,280,282,284Ds, 278,280,282,284,286Cn, 282,284,286,288,290Fl, 286,288,290,292,294Lv, 290,292,294,296,298Og, 294,296,298,300,302120; calculated potential energy surfaces. The Lublin-Strasbourg Drop (LSD) model.
doi: 10.1088/1674-1137/ac29a3
2021PO06 Chin.Phys.C 45, 054109 (2021) K.Pomorski, J.M.Blanco, P.V.Kostryukov, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, Z.-G.Xiao, Y.-J.Chen Fission fragment mass yields of Th to Rf even-even nuclei NUCLEAR STRUCTURE 216,218,220,222,224,226,228,230,232,234,236,238,240Th, 220,222,224,226,228,230,232,234,236,238,240,242,244,246U, 222,224,226,228,230,232,234,236,238,240,242,244,246,248,250Pu, 224,226,228,230,232,234,236,238,240,242,244,246,248,250,252Cm, 238,240,242,244,246,248,250,252,254,256,258,260Cf, 240,242,244,246,248,250,252,254,256,258,260,262Fm, 242,244,246,248,250,252,254,256,258,260,262,264No, 250,252,254,256,258,260,262,264,266,268,270,272,274,276Rf; calculated potential energy surfaces, fission barrier heights, fragment mass yields.
doi: 10.1088/1674-1137/abec69
2020PO06 Eur.Phys.J. A 56, 107 (2020) K.Pomorski, B.Nerlo-Pomorska, A.Dobrowolski, J.Bartel, C.M.Petrache Shape isomers in Pt, Hg and Pb isotopes with N ≤ 126
doi: 10.1140/epja/s10050-020-00115-x
2020PO09 Phys.Rev. C 101, 064602 (2020) K.Pomorski, A.Dobrowolski, R.Han, B.Nerlo-Pomorska, M.Warda, Z.Xiao, Y.Chen, L.Liu, J.-L.Tian Mass yields of fission fragments of Pt to Ra isotopes RADIOACTIVITY 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202Hg, 174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204Pb, 176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206Po, 196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226Rn, 198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228Ra, 236,238,240,242,244,246Pu(SF); calculated fission fragment mass distributions using collective three-dimensional model with Fourier nuclear shape parametrization and coupling fission, neck and mass asymmetry modes. 184Hg; calculated potential energy surfaces in (q2, q3) and (q3, q4) planes by macroscopic-microscopic model based on the Lublin-Strasbourg drop macroscopic energy and Yukawa-folded single-particle potential. Comparison with experimental fission fragment mass yields for 180,182,184Hg, 194,196Po, 202,204,206,208Rn, and 210,212,214,216,218Ra.
doi: 10.1103/PhysRevC.101.064602
2019PO10 Acta Phys.Pol. B50, 535 (2019) K.Pomorski, B.Nerlo-Pomorska, J.Bartel, C.Schmitt On the Properies of Super-heavy Even-Even Nuclei Around 294Og NUCLEAR STRUCTURE 288,290,292Lv, 290,292,294Og, 296,298,300120; calculated potential energy surfaces. Four-dimensional Fourier parametrization of nuclear shapes, combined with the macroscopic-microscopic approach of the potential energy based on the Lublin-Strasbourg drop and microscopic shell and pairing corrections.
doi: 10.5506/aphyspolb.50.535
2018PO05 Phys.Rev. C 97, 034319 (2018) K.Pomorski, B.Nerlo-Pomorska, J.Bartel, C.Schmitt Stability of superheavy nuclei NUCLEAR STRUCTURE 280Ds, 276Cn, 268,270,272Hs, 264,266,268Sg, 258,260,262,264Rf, 254,256,258Fm, 252Cf; calculated deformation energy surfaces in (q2, q3), (q3, q4), (q2, η) and (q4, η) planes. Z=94-126, N-Z=42-72; calculated values of the collective coordinates η, q2, q3 and q4 at equilibrium deformation, ground-state microscopic contribution to the potential energy, fission barrier heights. Comparison to available experimental data. Four-dimensional Fourier parametrization of nuclear shapes, combined with the macroscopic-microscopic approach of the potential energy based on the Lublin-Strasbourg drop and microscopic shell and pairing corrections. RADIOACTIVITY 230,232,234,236,238,240,242,244,246,248,250,252,254,256,258Pu, 232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262Cm, 238,240,242,244,246,248,250,252,254,256,258,260,262,264,266Cf, 242,244,246,248,250,252,254,256,258,260,262,264,266,268,270Fm, 246,248,250,252,254,256,258,260,262,264,266,268,270,272,274No, 250,252,254,256,258,260,262,264,266,268,270,272,274,276,278Rf, 254,256,258,260,262,264,266,268,270,272,274,276,278,280,282Sg, 258,260,262,264,266,268,270,272,274,276,278,280,282,284,286Hs, 262,264,266,268,270,272,274,276,278,280,282,284,286,288,290Ds, 266,268,270,272,274,276,278,280,282,284,286,288,290,292,294Cn, 270,272,274,276,278,280,282,284,286,288,290,292,294,296,298Fl, 274,276,278,280,282,284,286,288,290,292,294,296,298,300,302Lv, 278,280,282,284,286,288,290,292,294,296,298,300,302,304,306Og, 282,284,286,288,290,292,294,296,298,300,302,304,306,308,310120, 286,288,290,292,294,296,298,300,302,304,306,308,310,312,314122, 290,292,294,296,298,300,302,304,306,308,310,312,314,316,318124(α); calculated Q(α) and α-decay half-lives using Gamow-type WKB approach, and compared with available experimental data.
doi: 10.1103/PhysRevC.97.034319
2017NE02 Acta Phys.Pol. B48, 451 (2017) B.Nerlo-Pomorska, K.Pomorski, J.Bartel, C.Schmitt Potential Energy Surfaces of Thorium Isotopes in the 4D Fourier Parametrisation NUCLEAR STRUCTURE 218,220,222,224,226,230Th; calculated potential energy surface, deformation. 210,212,214,216,218,220,222,224,226,230,232,234,236,238Th; calculated gs and superdeformed quadrupole moment. Fourier shape parameterization. Detailed studies in progress. Quadrupole moments compared with available data.
doi: 10.5506/APhysPolB.48.451
2017NE03 Eur.Phys.J. A 53, 67 (2017) B.Nerlo-Pomorska, K.Pomorski, J.Bartel, C.Schmitt On possible shape isomers in the Pt-Ra region of nuclei NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192Pt, 178,180,182,184,186,188,190,192,194Hg, 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208Pb, 194,196,198,200,202,204,206,208,210Po, 196,198,200,202,204,206,208,210,212Rn, 208,210,212,214,216,218,220,222,224,226,228,230,232,234,236Ra; calculated deformation, potential surface, gs energy, shape isomeric minima, electric quadrupole moment using macroscopic-microscopic model based on Lublin-Strasbourg Drop model; deduced possibility of isomers, rapidly converging shape parameterization. Compared with available data.
doi: 10.1140/epja/i2017-12259-8
2017PO05 Acta Phys.Pol. B48, 541 (2017) K.Pomorski, J.Bartel, B.Nerlo-Pomorska On Jacobi and Poincare Shape Transitions in Rotating Nuclei NUCLEAR STRUCTURE 46Ti, 120Cd; calculated potential energy surface, mass excess, deformation for different angular momenta of rotating nuclei using LSD (Lublin-Strasbourg Drop) model iwith two additional deformation degrees of freedom of higher multipolarity and without microscopic corrections; deduced no sign of Poincare shape transition.
doi: 10.5506/APhysPolB.48.541
2017PO06 Eur.Phys.J. A 53, 59 (2017) K.Pomorski, F.A.Ivanyuk, B.Nerlo-Pomorska Mass distribution of fission fragments within the Born-Oppenheimer approximation NUCLEAR STRUCTURE 236U; calculated potential energy surface, deformation of fissioning nucleus, neck radius, fission probability using approximate solution of collective Hamiltonian describing the fission process. Compared to data. NUCLEAR REACTIONS 235U(n, f), E=thermal; calculated fission fragment yields using approximate solution of collective Hamiltonian describing the fission process. Compared to data.
doi: 10.1140/epja/i2017-12250-5
2017PO08 Phys.Scr. 92, 064006 (2017) K.Pomorski, B.Nerlo-Pomorska, J.Bartel Fourier expansion of deformed nuclear shapes expressed as the deviation from a spheroid NUCLEAR STRUCTURE 238U; analyzed available data; deduced a Fourier decomposition of nuclear shapes to cover a very wide range of nuclear deformations up to the scission point.
doi: 10.1088/1402-4896/aa7002
2017SC05 Phys.Rev. C 95, 034612 (2017) C.Schmitt, K.Pomorski, B.Nerlo-Pomorska, J.Bartel Performance of the Fourier shape parametrization for the fission process RADIOACTIVITY Z=78-94(SF); 178,180,184,192Hg, 194,196,202,210Po, 228Ra, 218,222,226,228,230,232,234,236Th, 238,240,242,246Pu(SF); calculated potential energy contours and fission paths, fission valleys, and exotic ground and metastable states for 100 even-even nuclei from Pt to Pu. Macroscopic-microscopic approach, employing a four-dimensional (4D) nuclear shape parametrization based on Fourier expansion, and realistic potential-energy prescription.
doi: 10.1103/PhysRevC.95.034612
2016NE05 Acta Phys.Pol. B47, 943 (2016) B.Nerlo-Pomorska, K.Pomorski, J.Bartel On the Possibility to Observe New Shape Isomers in the Po-Th Region NUCLEAR STRUCTURE 188,192,196,200,204,208,212,216,220Po; calculated deformation-energy landscapes, rotational energies, charge quadrupole moments.
doi: 10.5506/APhysPolB.47.943
2016PO04 52, 144 (2016) Remarks on the nuclear shell-correction method NUCLEAR STRUCTURE 88Sr; calculated smoothed single-particle level density for neutrons and protons using 3D harmonic oscillator and HFB with Gogny force, shell energy corrections using traditional Strutinsky approach and using smoothing over the particle number. Z=36-42; calculated neutron and proton sp levels, J using HFB with Gogny force.
doi: 10.1140/epja/i2016-16144-8
2015BA48 Phys.Scr. 90, 114004 (2015) J.Bartel, K.Pomorski, B.Nerlo-Pomorska, C.Schmitt Fission properties of Po isotopes in different macroscopic-microscopic models RADIOACTIVITY 212Po, Po(SF); calculated fission-barrier heights of nuclei in the Po isotopic chain. Yukawa-folded single-particle potential, the Lublin-Strasbourg drop (LSD) model.
doi: 10.1088/0031-8949/90/11/114004
2015NE15 Phys.Scr. 90, 114010 (2015) B.Nerlo-Pomorska, K.Pomorski, C.Schmitt, J.Bartel Potential energy surfaces of Polonium isotopes NUCLEAR STRUCTURE 188,192,196,200,204,208,212,216,220Po; calculated total deformation energy, potential energy surfaces. Lublin-Strasbourg drop model and the Yukawa-folded single-particle energies.
doi: 10.1088/0031-8949/90/11/114010
2015PO05 Phys.Rev. C 91, 054605 (2015) K.Pomorski, B.Nerlo-Pomorska, P.Quentin b decay of 252Cf in the transition from the exit point to scission RADIOACTIVITY 252Cf(SF), (β-); calculated branching ratio for rare Fermi β- decay for 252Cf during the spontaneous fission process up to the scission point, nuclear dissipation. Classical dynamical approach. NUCLEAR STRUCTURE 252Cf; calculated potential energy surface contours, Proton and neutron single-particle levels in the ground state and at the scission point. Macroscopic-microscopic calculations.
doi: 10.1103/PhysRevC.91.054605
2014BA10 Phys.Scr. 89, 054003 (2014) J.Bartel, B.Nerlo-Pomorska, K.Pomorski, C.Schmitt The potential energy surface of 240Pu around scission NUCLEAR STRUCTURE 240Pu; analyzed potential energy surface within the macroscopic-microscopic approach; deduced effect of strong neutron shell corrections on mass distributions.
doi: 10.1088/0031-8949/89/5/054003
2014NE03 Phys.Scr. 89, 054004 (2014) B.Nerlo-Pomorska, K.Pomorski, P.Quentin, J.Bartel Rotational bands in well deformed heavy nuclei NUCLEAR STRUCTURE 230,232Th, 234,236,238U, 240,242Pu, 246Cm, 252No; calculated energy levels, J, π, rotational bands. Comparison with experimental data.
doi: 10.1088/0031-8949/89/5/054004
2014NE17 Phys.Scr. 89, 054031 (2014) B.Nerlo-Pomorska, K.Pomorski, C.Schmitt, J.Bartel Low-energy fission within the Lublin-Strasbourg drop and Yukawa folded model NUCLEAR STRUCTURE 180,198Hg, 234U, 240Pu, 260Fm; calculated fission potential energy surface. 222,228Th; calculated potential energy for symmetric and asymmetric fission paths. Macroscopic (Lublin-Strasbourg drop) - microscopic (BCS with Yukawa force) method.
doi: 10.1088/0031-8949/89/5/054031
2013NE05 Phys.Scr. T154, 014026 (2013) B.Nerlo-Pomorska, K.Pomorski, C.Schmitt Potential energy landscapes of Th isotopes within the Lublin Strasbourg drop + Yukawa-folded model NUCLEAR STRUCTURE 220,226Th, 208Pb; calculated potential energy surfaces in a four-dimensional deformation space. Lublin Strasbourg drop model, Yukawa-folded potential.
doi: 10.1088/0031-8949/2013/T154/014026
2013NE06 Phys.Scr. T154, 014028 (2013) Masses and rotational energies of the heaviest nuclei NUCLEAR STRUCTURE Z=88-112; calculated ground-state masses of even-even nuclei, pairing strengths, 226Ra, 248Cm, 278Cn. Lublin Strasbourg drop mass formula for the macroscopic part and the Yukawa-folded single-particle potential.
doi: 10.1088/0031-8949/2013/T154/014028
2012BA22 Int.J.Mod.Phys. E21, 1250023 (2012) J.Bartel, K.Pomorski, B.Nerlo-Pomorska Light-Particle Emission From Fissioning Hot Rotating Nuclei RADIOACTIVITY 160Yb(n), (p), (α); calculated energy spectra of neutrons, protons and alpha particles, En, In, Ep, Ip, Eα, Iα. 208Pb; deduced nuclear potential.
doi: 10.1142/S0218301312500231
2012NE04 Int.J.Mod.Phys. E21, 1250050 (2012) B.Nerlo-Pomorska, K.Pomorski, J.Bartel Dynamical coupling of rotation with the pairing field in heavy nuclei NUCLEAR STRUCTURE 230,232,234,236,238,240U, 242,246,248Cm, 248,250,252,254No; calculated level energies, J, π, rotational bands. Macroscopic-macroscopic model with the Lublin-Strasbourg Drop, the Yukawa-folded single-particle potential, comparison with available data.
doi: 10.1142/S0218301312500504
2011NE05 Int.J.Mod.Phys. E20, 539 (2011) B.Nerlo-Pomorska, K.Pomorski, A.Dobrowolski Rotational states in heaviest isotopes NUCLEAR STRUCTURE 248,252,254,256Fm, 254No; calculated deformation energy, pairing strength, rotational energies, masses. Comparison with experimental data.
doi: 10.1142/S0218301311017971
2011NE09 Phys.Rev. C 84, 044310 (2011) B.Nerlo-Pomorska, K.Pomorski, J.Bartel Rotational states and masses of heavy and superheavy nuclei NUCLEAR STRUCTURE Z=88-112, N=136-170; calculated nuclear masses, rotational bands, single particle levels, potential energy surfaces, deformation energies. 238Cm; calculated energy and moment of inertia contour plots on c, h plane. 238Cm, 236U; calculated Cross section of the potential energies as function of the mass-asymmetry deformation parameter. 230,232U, 236,244Pu, 242,246,248Cm, 248,250Fm, 252,254No; calculated rotational bands. Lublin-Strasbourg drop (LSD), Strutinsky shell-correction method, Yukawa-folded (YF) mean-field potential, BCS approach for pairing correlations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.044310
2011PO05 Int.J.Mod.Phys. E20, 316 (2011) K.Pomorski, B.Nerlo-Pomorska, J.Bartel Microscopic energy corrections at the scission configuration RADIOACTIVITY 236U(SF); calculated shell energy, single-particle potential, fission fragments, microscopic fission barrier.
doi: 10.1142/S0218301311017673
2010DO07 Int.J.Mod.Phys. E19, 699 (2010) A.Dobrowolski, B.Nerlo-Pomorska, K.Pomorski, J.Bartel Rotational bands in heavy and superheavy nuclei within the Lublin Strasbourg Drop + Yukawa folded Model NUCLEAR STRUCTURE 254No; calculated deformation energy, shell correction, moment of inertia, rotational energies.
doi: 10.1142/S0218301310015126
2009BA33 Int.J.Mod.Phys. E18, 986 (2009) J.Bartel, B.Nerlo-Pomorska, K.Pomorski Jacobi bifurcation in hot rotating nuclei with a LSD + Yukawa folded approach NUCLEAR STRUCTURE 88Mo; calculated deformation energy surfaces for excited nuclei.
doi: 10.1142/S0218301309013130
2009DO07 Acta Phys.Pol. B40, 705 (2009) A.Dobrowolski, B.Nerlo-Pomorska, K.Pomorski, J.Bartel Fission Barrier Heights of Medium Heavy and Heavy Nuclei
2009NE01 Int.J.Mod.Phys. E18, 123 (2009) B.Nerlo-Pomorska, K.Pomorski, F.Ivanyuk Remarks on the nuclear shell-correction method NUCLEAR STRUCTURE 40Ca, 132Sn; calculated single particle energies, shell corrections.
doi: 10.1142/S0218301309012070
2009NE08 Int.J.Mod.Phys. E18, 1099 (2009) Simple tool to search quasi-magic structures in deformed nuclei NUCLEAR STRUCTURE 264Hs; calculated level energies, deformation, quasi-magic structures.
doi: 10.1142/S0218301309013324
2008NE02 Acta Phys.Pol. B39, 417 (2008) B.Nerlo-Pomorska, K.Pomorski, J.Bartel, A.Dobrowolski Nuclear Level Density Parameter
2007NE02 Int.J.Mod.Phys. E16, 328 (2007) On the average pairing energy in nuclei NUCLEAR STRUCTURE 232,234Th, 240,246Pu, 236U, 246Cm; calculated pairing energy vs deformation.
doi: 10.1142/S0218301307005764
2007NE03 Int.J.Mod.Phys. E16, 474 (2007) B.Nerlo-Pomorska, K.Pomorski, M.Zwierzchowska Predictions of nuclear masses in different models ATOMIC MASSES Z=8-112; analyzed masses. Comparison of Lublin-Strasbourg drop and Thomas-Fermi approaches.
doi: 10.1142/S0218301307005909
2007PO02 Int.J.Mod.Phys. E16, 566 (2007) K.Pomorski, B.Nerlo-Pomorska, J.Bartel Nuclear level density parameter with Yukawa folded potential NUCLEAR STRUCTURE O, Ca, Sr, Sn, Sm, Pb, Th; calculated level density parameters. 40Ca, 50Cr, 100Ru, 150Sm, 200Hg, 250Cf; calculated level density parameters vs deformation. Yukawa folded potential.
doi: 10.1142/S0218301307006009
2006BA12 Int.J.Mod.Phys. E15, 478 (2006) J.Bartel, K.Pomorski, B.Nerlo-Pomorska Nuclear level density at finite temperatures NUCLEAR STRUCTURE Z=8-82; A=16-224; calculated single-particle level densities vs temperature. Selfconsistent mean-field approach.
doi: 10.1142/S0218301306004399
2006NE02 Int.J.Mod.Phys. E15, 471 (2006) Pairing energy obtained by folding in the nucleon number space
doi: 10.1142/S0218301306004387
2006NE07 Phys.Rev. C 74, 034327 (2006) B.Nerlo-Pomorska, K.Pomorski, J.Bartel Shell energy and the level-density parameter of hot nuclei NUCLEAR STRUCTURE 40Ca, 50Cr, 100Ru, 150Sm, 200Hg, 250Cf; calculated level density parameters, shell-correction energy vs temperature. Macroscopic-microscopic approach.
doi: 10.1103/PhysRevC.74.034327
2006NE09 Phys.Scr. T125, 210 (2006) Macroscopic part of nuclear energy in different self-consistent models
doi: 10.1088/0031-8949/2006/T125/055
2006PO17 Phys.Scr. T125, 21 (2006) Shell and pairing energies obtained by folding in N space NUCLEAR STRUCTURE 208Pb; N=20-200; calculated shell and pairing energies vs deformation. Modified Strutinsky method.
doi: 10.1088/0031-8949/2006/T125/005
2005DU11 Int.J.Mod.Phys. E14, 383 (2005) J.Dudek, K.Mazurek, B.Nerlo-Pomorska Search for the tri-axial hexadecapole-deformation effects in trans-actinide nuclei NUCLEAR STRUCTURE 238U, 250,252Cf, 256,258Fm; calculated energy vs deformation, tri-axial hexadecapole-deformation effects. Macroscopic-microscopic method, comparison with Hartree-Fock-Bogoliubov approach.
doi: 10.1142/S0218301305003168
2005MA30 Acta Phys.Pol. B36, 1355 (2005) K.Mazurek, J.Dudek, B.Nerlo-Pomorska Non-axial quadrupole and hexadecapole deformations in Cf-Ds nuclear region NUCLEAR STRUCTURE 254,256,258Fm, 256,258,260No, 258,260,262Rf; calculated deformation energy along fission path. Lublin-Strasbourg drop model.
2005NE08 Acta Phys.Pol. B36, 1377 (2005) B.Nerlo-Pomorska, J.Sykut, J.Bartel Temperature dependence of the nuclear shell energies NUCLEAR STRUCTURE 216Th; calculated shell correction energies. Ca, Sr, Sn, Sm, Pb, Th; calculated level-density parameters.
2005NE09 Int.J.Mod.Phys. E14, 505 (2005) B.Nerlo-Pomorska, K.Pomorski, J.Sykut, J.Bartel Temperature dependence of the nuclear energy in relativistic mean-field theory NUCLEAR STRUCTURE A=16-224; analyzed level densities, temperature-dependent shell corrections.
doi: 10.1142/S021830130500334X
2004DU04 Int.J.Mod.Phys. E13, 117 (2004) J.Dudek, K.Mazurek, B.Nerlo-Pomorska Competition between axial and non-axial octupole deformations in heavy nuclei NUCLEAR STRUCTURE 224Rn, 226Ra; calculated energy vs deformation. Macroscopic-microscopic method.
doi: 10.1142/S0218301304001825
2004DU15 Acta Phys.Pol. B35, 1263 (2004) J.Dudek, K.Mazurek, B.Nerlo-Pomorska Potential Energy Surfaces Calculated Using Macroscopic-Microscopic Method with the LSD Model NUCLEAR STRUCTURE 250Cf; calculated potential energy surfaces, fission barrier features. Lubin Strasbourg Drop model.
2004NE01 Int.J.Mod.Phys. E13, 75 (2004) A new parameter set for the relativistic mean field theory NUCLEAR STRUCTURE 40,42,44,48Ca, 46,48,50Ti, 52Cr, 58Ni, 90Zr, 116,124Sn, 208Pb; calculated radii. Ca, Sr, Sn, Sm, Pb, Th; calculated radii, masses for even-even isotopes. Relativistic mean-field theory, comparison with data.
doi: 10.1142/S0218301304001758
2004NE05 Acta Phys.Pol. B35, 1299 (2004) Macroscopic Properties of Nuclei within Self-Consistent and Liquid Drop Models NUCLEAR STRUCTURE A=40-220; analyzed binding energies; deduced parameters. Lublin-Strasbourg Drop model.
2004NE14 Int.J.Mod.Phys. E13, 1147 (2004) B.Nerlo-Pomorska, K.Pomorski, J.Sykut, J.Bartel Temperature dependence of nuclear structure in the relativistic mean-field theory with a new parameter set NUCLEAR STRUCTURE A=16-220; calculated masses, binding energies, level density vs temperature. Relativistic mean-field theory.
doi: 10.1142/S0218301304002636
2003DU24 Acta Phys.Pol. B34, 2247 (2003) J.Dudek, K.Mazurek, B.Nerlo-Pomorska Interaction strengths for the Fock-space formulation of the nuclear pairing problem NUCLEAR STRUCTURE Z=20-100; analyzed data; deduced pairing strength parameters.
2003NE18 Acta Phys.Pol. B34, 1777 (2003) B.Nerlo-Pomorska, K.Mazurek, M.Kleban Limits of nuclear stability NUCLEAR STRUCTURE Ca, Sr, Sn, Sm, Pb, Th; calculated binding energies, shell corrections, related features; deduced stability limits. Comparison of liquid-drop model, HFB approach.
2002KL03 Phys.Rev. C65, 024309 (2002) M.Kleban, B.Nerlo-Pomorska, J.F.Berger, J.Decharge, M.Girod, S.Hilaire Global Properties of Spherical Nuclei Obtained from Hartree-Fock-Bogoliubov Calculations with the Gogny Force NUCLEAR STRUCTURE Z=30-100; A=50-240; calculated single-particle levels, shell corrections, radii. 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb, 154Hf, 156W, 158Os, 160Pt, 162Hg, 164Pb; calculated neutron and proton shell corrections. Self-consistent HFB calculations, Gogny force.
doi: 10.1103/PhysRevC.65.024309
2002KL04 Acta Phys.Pol. B33, 383 (2002) M.Kleban, B.Nerlo-Pomorska, K.Pomorski, J.F.Berger, J.Decharge The Ground State Properties of Spherical Nuclei Calculated by Hartree-Fock-Bogoliubov Procedure with the Gogny D1S Force NUCLEAR STRUCTURE A=40-220; calculated binding energies, neutron and charge radii. HFB method, Gogny force.
2002NE17 Phys.Rev. C 66, 051302 (2002) B.Nerlo-Pomorska, K.Pomorski, J.Bartel, K.Dietrich Nuclear level densities within the relativistic mean-field theory NUCLEAR STRUCTURE A=30-210; calculated level density parameters. 118Sn; calculated mean-field energy vs temperature. Relativistic mean-field approach.
doi: 10.1103/PhysRevC.66.051302
2002NE21 Phys.Rev. C 66, 064305 (2002) Macroscopic properties of nuclei according to relativistic mean field theory NUCLEAR STRUCTURE 40,42,44,48Ca, 46,48,50Ti, 52Cr, 58,64Ni, 90Zr, 118,124Sn, 208Pb; calculated neutron radii. Z=20-90; calculated binding energies, radii. Relativistic mean field, self-consistent approach.
doi: 10.1103/PhysRevC.66.064305
2001KL06 Acta Phys.Pol. B32, 1119 (2001) M.Kleban, B.Nerlo-Pomorska, K.Pomorski, J.F.Berger, J.Decharge Shell Corrections of Spherical Nuclei Calculated by Hartree-Fock Procedure with the Gogny Force NUCLEAR STRUCTURE Ca, Sr, Sn, Sm; calculated Gogny shell corrections, radii.
2001LO24 Acta Phys.Pol. B32, 2981 (2001) Z.Lojewski, B.Nerlo-Pomorska, J.Dudek Microscopic Calculation of the Nucleonic Levels and Mean Square Radii of Atomic Nuclei with the New Woods-Saxon Potential Parameters NUCLEAR STRUCTURE 40,48Ca, 56Ni, 90Zr, 132Sn, 208Pb; calculated single-particle level energies. Z=36-88; calculated radii. Woods-Saxon potential, new parameters.
2001MA23 Acta Phys.Pol. B32, 783 (2001) Nilsson Single Particle Potential Parameters Reproducing the Ground State and K-Isomers Radii
2001NE05 Acta Phys.Pol. B32, 925 (2001) B.Nerlo-Pomorska, K.Pomorski, J.F.Berger The Neutron and Proton Density Distributions within the HFB Calculation with the Gogny Force NUCLEAR STRUCTURE 232Th; calculated neutron, proton densities, deformations. Hartree-Fock-Bogoliubov calculations.
2000NE05 Eur.Phys.J. A 8, 19 (2000) B.Nerlo-Pomorska, K.Pomorski, J.F.Berger, J.Decharge The Neutron Halo in Heavy Nuclei Calculated with the Gogny Force NUCLEAR STRUCTURE 48Ca, 58Ni, 96Zr, 96,104Ru, 100Mo, 106,116Cd, 112,124Sn, 128,130Te, 144,154Sm, 148Nd, 160Gd, 176Yb, 232Th, 238U; calculated binding energies, one- and two-neutron separation energies, deformation, halo features, density distributions. Hartree-Fock-Bogoliubov method, Gogny force. Comparisons with data.
doi: 10.1007/s100530050004
2000PO23 Nucl.Phys. A679, 25 (2000) K.Pomorski, B.Nerlo-Pomorska, A.Surowiec, M.Kowal, J.Bartel, K.Dietrich, J.Richert, C.Schmitt, B.Benoit, E.de Goes Brennand, L.Donadille, C.Badimon Light-Particle Emission from the Fissioning Nuclei 126Ba, 188Pt and 266, 272, 278110: Theoretical predictions and experimental results NUCLEAR REACTIONS 98Mo(28Si, X), E=166, 187, 204 MeV; 107Ag(19F, X), E=128, 148 MeV; 154Sm(34S, X), E=160, 203 MeV; 172Yb(16O, X), E=138 MeV; 208Pb(58Ni, X), (64Ni, X), 232Th(40Ca, X), 238U(40Ar, X), E=66-186 MeV; calculated fusion, fission σ(L), prefission particle multiplicities; deduced entrance channel effects. Comparisons with data.
doi: 10.1016/S0375-9474(00)00327-4
1998WA17 Nucl.Phys. A635, 484 (1998) M.Warda, B.Nerlo-Pomorska, K.Pomorski Isospin Dependence of Proton and Neutron Radii within Relativistic Mean Field Theory NUCLEAR STRUCTURE A=40-208; analyzed neutron, proton radii of beta-stable even-even nuclei; deduced phenomenological formula. Several isotope, isotone chains also discussed. Relativistic mean-field theory.
doi: 10.1016/S0375-9474(98)00188-2
1997PO10 Acta Phys.Pol. B28, 413 (1997) Light Particles Emission from Hot, Rotating, Compound Nuclei NUCLEAR STRUCTURE 150,160Yb, 144,154Gd; calculated neutron, proton, alpha emission widths, prescission multiplicities; deduced deformation dependence. Hot, rotating nuclei.
1997PO13 Nucl.Phys. A624, 349 (1997) K.Pomorski, P.Ring, G.A.Lalazissis, A.Baran, Z.Lojewski, B.Nerlo-Pomorska, M.Warda Ground State Properties of the β Stable Nuclei in Various Mean Field Theories NUCLEAR STRUCTURE A=16-256; calculated even-even stable nucleus proton, neutron separation energies, charge radii, other ground state properties. Several models compared. Comparisons with data.
doi: 10.1016/S0375-9474(97)00367-9
1996NE03 Acta Phys.Pol. B27, 537 (1996) B.Nerlo-Pomorska, K.Pomorski, J.Puszyk The Isotopic Shifts of the Mean Square Radii of Odd Nuclei NUCLEAR STRUCTURE N=36-74; N=46-80; N=50-80; calculated charge mean square vs neutron number for Rb, Ag, Sn isotopes. BCS theory, Nilsson single particle potential.
1995BA45 J.Phys.(London) G21, 657 (1995) A.Baran, J.L.Egido, B.Nerlo-Pomorska, K.Pomorski, P.Ring, L.M.Robledo Mean-Field Calculations of Proton and Neutron Distributions in Sr, Xe and Ba Isotopes NUCLEAR STRUCTURE 78,80,82,84,86,88,90,92,94,96,98,100,102Sr, 114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146Xe, 120,122,124,126,130,132,134,136,138,140,142,144,146,148Ba; calculated rms radii, n-, p- radii, quadrupole deformations differences, electric quadrupole moments. Mean field approach.
doi: 10.1088/0954-3899/21/5/010
1995LO01 Phys.Rev. C51, 601 (1995) Z.Lojewski, B.Nerlo-Pomorska, K.Pomorski, J.Dudek Mean Square Radii of Nuclei Calculated with the Woods-Saxon Potential NUCLEAR STRUCTURE Z=46-60; Z=60-70; calculated mean square charge radii. Woods-Saxon potential.
doi: 10.1103/PhysRevC.51.601
1995NE12 At.Data Nucl.Data Tables 60, 287 (1995) Nuclear Charge Radii and Electric Quadrupole Moments of Even-Even Isotopes NUCLEAR STRUCTURE Z=20-98; calculated isotope shifts, charge mean-square radii, electric quadrupole moments. Dynamical microscopic model, even-even nuclei.
doi: 10.1006/adnd.1995.1008
1994LO12 Acta Phys.Pol. B25, 1147 (1994) Z.Lojewski, B.Nerlo-Pomorska, K.Pomorski Influence of the Quadrupole Pairing Interaction on the Mean-Square Radii of Nuclei NUCLEAR STRUCTURE 76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112Sr; calculated equilibrium deformations, rms charge radii isotope shifts; deduced quadrupole pairing forces role. Microscopic static calculations, Ba, Xe, Nd, Pt isotopes studied.
1994NE06 Z.Phys. A348, 169 (1994) Simple Formula for Nuclear Charge Radius NUCLEAR STRUCTURE A ≤ 250; analyzed mean square radii, isotope shifts data, even-even nuclei. Mass, neutron excess dependent charge radius formula.
doi: 10.1007/BF01291913
1994NE09 Acta Phys.Pol. B25, 725 (1994) Nuclear Radius NUCLEAR STRUCTURE N=36-154; calculated even-even Sr, Ce, actinide, other isotopes rms charge radii. Isotope shifts data comparison.
1993NE02 Z.Phys. A344, 359 (1993) Isospin Dependence of Nuclear Radius NUCLEAR STRUCTURE Z=38-78; N=36-92; N=68-124; calculated mean square radii; deduced isotopic dependence.
doi: 10.1007/BF01283190
1993NE03 Acta Phys.Pol. B24, 441 (1993) B.Nerlo-Pomorska, K.Pomorski, B.Mach The Mean Square Radii and Quadrupole Moments of Even-Even Isotopes with 38 ≤ Z ≤ 74, N ≤ 74 NUCLEAR STRUCTURE Z=38-74; Z ≤ N ≤ 74; calculated deformation energies, mean square radii, quadrupole moments. Generator coordinate method, Sr-W nuclei.
1993NE06 Nucl.Phys. A562, 180 (1993) B.Nerlo-Pomorska, K.Pomorski, B.S.Mach Mean Square Radii and Quadrupole Moments of Even-Even Isotopes with 38 ≤ Z ≤ 60, N ≤ 74 NUCLEAR STRUCTURE Z=38-60; N ≤ 74; calculated rms radii, quadrupole moments, deformation energies. Microscopic model, even-even Sr-Nd isotopes.
doi: 10.1016/0375-9474(93)90194-3
1988RO02 Phys.Lett. 201B, 409 (1988) L.M.Robledo, J.L.Egido, B.Nerlo-Pomorska, K.Pomorski A Quantum Parity-Conserving Study on Octupole Deformation in the Light-Actinide Region NUCLEAR STRUCTURE 222Ra; calculated mass parameters, B(λ), moments of inertia. Hartree-Fock plus BCS.
doi: 10.1016/0370-2693(88)90592-8
1987BO12 Acta Phys.Pol. B18, 47 (1987) K.Boning, Z.Patyk, A.Sobiczewski, B.Nerlo-Pomorska, K.Pomorski Role of a Consistency Condition in Macroscopic-Microscopic Calculations of the Collective Potential Energy NUCLEAR STRUCTURE 224Ra; calculated oscillator energies, density, potential deformation difference, ratio, microscopic, macroscopic multipole moments ratio, scaled, nonscaled energies.
1987NE03 Nucl.Phys. A462, 252 (1987) B.Nerlo-Pomorska, K.Pomorski, M.Brack, E.Werner Multipole Moments of Rare-Earth Nuclei in the Generator Coordinate Method NUCLEAR STRUCTURE 166Er; calculated potential energy surface, charge monopole, electric quadrupole, hexadecapole moments, overlap width mass parameters; 148,150,152,154,156,158,160,162,164,166Nd, 150,152,154,156,158,160,162,164,166,168Sm, 152,154,156,158,160,162,164,166,168,170Gd, 160,162,164,166,168,170,172,174,176,178Hf, 158,160,162,164,166,168,170,172,174,176Yb, 156,158,160,162,164,166,168,170,172,174Er, 154,156,158,160,162,164,168,170,172Dy; calculated charge rms radii, hexadecapole electric moments. Generator coordinate method, gaussian overlap approximation.
doi: 10.1016/0375-9474(87)90547-1
1987NE07 Z.Phys. A328, 11 (1987) Deformation Energies of Rare-Earth Nuclei in Generator Coordinate Method NUCLEAR STRUCTURE 144,146,148,150,152,154,156,158,160,162,164Ce, 144,146,148,152,154,156,158,160,162,164,166Nd, 148,150,152,154,156,158,160,162,164,166,168Sm, 150,152,154,156,158,160,162,164,166,168Gd, 152,154,156,158,160,162,164,166,168,170,172Dy, 154,156,158,160,162,164,166,168,170,172,174,176Er, 156,158,160,162,164,166,168,170,172,174,176Yb, 158,160,162,164,166,168,170,172,174,176,178Hf; calculated deformation. Mean field Nilsson hamiltonian.
1985BO43 Phys.Lett. 161B, 231 (1985) K.Boning, A.Sobiczewski, B.Nerlo-Pomorska, K.Pomorski Coupled Octupole and Quadrupole Vibrations of Nuclei around Radium NUCLEAR STRUCTURE 226Th; calculated levels, potential energy vs quadrupole, octupole deformations, B(λ); deduced octupole instability.
doi: 10.1016/0370-2693(85)90751-8
1983NE02 Z.Phys. A309, 341 (1983) The Dynamical Effects in the Ground State of Nuclei NUCLEAR STRUCTURE 228,230,232,234,236,238,240,242,244U, 150Nd; calculated potential energy surfaces. 150Nd, 152,154Sm; calculated quadrupole, hexadecapole moments. Dynamical effects, shell correction, collective model.
doi: 10.1007/BF01413837
1983RO14 Nucl.Phys. A405, 252 (1983) P.Rozmej, B.Nerlo-Pomorska, K.Pomorski Equilibrium Deformations for the Ra-Th Region of Nuclei NUCLEAR STRUCTURE 220,222,224Rn, 220,222,224Ra, 222,224,236Th, 224,236,238U, 226,240Pu; calculated potential equilibrium deformation. 220,222,224,226,228,230,232Rn, 220,222,224,226,228,230,232Ra, 222,224,226,228,230,232,234,236Th, 224,226,228,230,232,234,236,238U, 226,228,230,232,234,236,240Pu; calculated deformation energies, electric, static quadrupole, hexadecapole moments. Density-dependent shell correction method.
doi: 10.1016/0375-9474(83)90571-7
1981GY03 Phys.Lett. 105B, 95 (1981) A.Gyurkovich, A.Sobiczewski, B.Nerlo-Pomorska, K.Pomorski On the Stable Octupole Deformation of Nuclei NUCLEAR STRUCTURE 218,220,222Rn, 220,222,224Ra, 224,226,228Th, 228,230,232U, 234,236,238Pu; calculated potential energy; deduced quadrupole, octupole equilibrium deformations. Macroscopic-Microscopic method.
doi: 10.1016/0370-2693(81)90997-7
1979NE08 Z.Phys. A293, 9 (1979) Microscopic Quadrupole and Hexadecapole Moments of Rare Earth Nuclei NUCLEAR STRUCTURE 168,170,172,174,176,178,180,182,184Yb, 168,170,172,174,176,178,180,182,184,186Hf, 166,168,170,172,174,176,178,180,182,184,186,188,190W, 170,172,174,176,178,180,182,184,186,188,190,192,194Os, 176,178,180,182,184,186,188,190,192,194,196Pt, 180,182,184,186,188,190Hg; calculated multipole moments, stiffness parameters, deformation energies. Microscopic model, self-consistency condition.
doi: 10.1007/BF01414779
1978IG01 Phys.Lett. 76B, 543 (1978) A.V.Ignatiuk, I.N.Mikhailov, R.G.Nazmitdinov, B.Nerlo-Pomorska, E.Pomorski Equilibrium Properties of Fast-Rotating Heated Nuclei NUCLEAR STRUCTURE 128Ba, 166Er, 208Pb; calculated equilibrium deformation in excited, heated rotating nuclei.
doi: 10.1016/0370-2693(78)90849-3
1978JA18 Phys.Lett. 79B, 347 (1978) D.Janssen, I.N.Mikhailov, R.G.Nazmitdinov, B.Nerlo-Pomorska, K.Pomorski, R.K.Safarov Calculations of Low-Lying Collective Excitation Energies in 168Yb at High Angular Momenta NUCLEAR STRUCTURE 168Yb; calculated energies of low-lying collective states using microscopic model; deduced relationship of lowest I-odd states to γ-vibration states, to one-phonon precessional excitation for large I.
doi: 10.1016/0370-2693(78)90379-9
1978NE05 Z.Phys. A287, 337 (1978) B.Nerlo-Pomorska, J.Ludziejewski The Deformation of the Ground and Excited States in the Ag and Sn Nuclei NUCLEAR STRUCTURE 102,104,106Cd, 110,112,114,116,118,120Sn, 100,102Pd, 101,103,105Ag; calculated potential energy.
doi: 10.1007/BF01481714
1978NE13 Nukleonika 23, 119 (1978) Effect of a Simple Consistency Condition on the Multipole Moments of Actinides NUCLEAR MOMENTS 230,232,234,236,238,240U, 234,236,238,240,242,244,246Pu, 240,242,244,246,248,252Cm, 250,252,254Cf; calculated static electric quadrupole, hexadecapole moments. Strutinsky shell-correction method, macroscopic, microscopic density distribution equality condition.
1977NE15 Nukleonika 22, 289 (1977) Effect of a Simple Consistency Condition in the Fission Barrier Calculations NUCLEAR STRUCTURE 240Pu; calculated density parameters, liquid drop, total energies, shell, pairing correction energies; deduced effect on fission barriers. Macroscopic, microscopic method, self-consistency condition.
1977PO12 Z.Phys. A283, 383 (1977) High Spin Behavior of Nuclei with Proton Number 40-60 NUCLEAR STRUCTURE 114,116,118,120,122,134Te, 126Ba, 116,118,120,122,124,126Xe, 90Zr, 94Mo, 100Ru, 108Cd, 112,116Sn, 124,126,130Ce, 128,134,140Nd; calculated potential energy surfaces.
doi: 10.1007/BF01409519
1977RO30 Nucl.Phys. A292, 66 (1977) S.G.Rohozinski, J.Dobaczewski, B.Nerlo-Pomorska, K.Pomorski, J.Srebrny Microscopic Dynamic Calculations of Collective States in Xenon and Barium Isotopes NUCLEAR STRUCTURE 118,120,122,124,126,128,130Xe, 122,124,126,128,130,132,134Ba; calculated levels, shape parameters, μ, quadrupole moment.
doi: 10.1016/0375-9474(77)90358-X
1977RO31 Nukleonika 22, 293 (1977) S.G.Rohozinski, J.Dobaczewski, J.Srebrny, B.Nerlo-Pomorska, K.Pomorski Solution of the Schrodinger Equation with the Bohr Hamiltonian for the Even-Even Barium and Xenon Nuclei NUCLEAR STRUCTURE 122Xe; calculated energy levels, potential energy surfaces, B(E2). Schrodinger equation, generalized Bohr Hamiltonian.
1976AN10 Nucl.Phys. A268, 205 (1976) G.Andersson, S.E.Larsson, G.Leander, P.Moller, S.G.Nilsson, I.Ragnarsson, S.Aberg, R.Bengtsson, J.Dudek, B.Nerlo-Pomorska, K.Pomorski, Z.Szymanski Nuclear Shell Structure at Very High Angular Momentum NUCLEAR STRUCTURE 24Mg, 114,116,118Te, 122,124,126Xe, 122,124,126,128,130,138Ba, 150Gd, 150,154Sm, 158,160,164,166,168Yb, 178W, 182,178,186,190Os, 204Pb, 160Er, 298Fl; calculated potential energy surfaces, shell structure.
doi: 10.1016/0375-9474(76)90461-9
1976NE02 Nucl.Phys. A259, 481 (1976) Static Electric Quadrupole and Hexadecapole Moments of Nuclei NUCLEAR STRUCTURE A=148-244; calculated quadrupole moment.
doi: 10.1016/0375-9474(76)90083-X
1974RA24 Nucl.Phys. A233, 329 (1974) I.Ragnarsson, A.Sobiczewski, R.K.Sheline, S.E.Larsson, B.Nerlo-Pomorska Comparison of Potential-Energy Surfaces and Moments of Inertia with Experimental Spectroscopic Trends for Non-Spherical Z = 50-82 Nuclei NUCLEAR STRUCTURE Z=50-82; calculated ground state potential energy surfaces.
doi: 10.1016/0375-9474(74)90460-6
1973PO06 Nucl.Phys. A205, 433 (1973) K.Pomorski, B.Nerlo-Pomorska, I.Ragnarsson, R.K.Sheline, A.Sobiczewski Ground State Moments of Inertia of Deformed Nuclei Around Barium NUCLEAR STRUCTURE A=116-144; calculated deformation energies, moments of inertia using cranking model.
doi: 10.1016/0375-9474(73)90698-2
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