NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = W.Greiner Found 604 matches. Showing 1 to 100. [Next]2015GR17 JETP Lett. 102, 321 (2015) K.A.Gridnev, V.N.Tarasov, D.K.Gridnev, W.Greiner, J.Vinas Resonance capture of multineutrons by the 88Sr and 27Al nuclei NUCLEAR STRUCTURE 27Al, 88Sr, Mg; calculated neutron separation energies, rms radii, binding energies. Hartree-Fock method with the Skyrme forces (Ska) taking into account pairing in the Bardeen-Cooper-Schrieffer approximation.
doi: 10.1134/S002136401518006X
2015MI04 Nucl.Instrum.Methods Phys.Res. B349, 133 (2015) I.Mishustin, Y.Malyshkin, Ig.Pshenichnov, W.Greiner Synthesis of neutron-rich transuranic nuclei in fissile spallation targets NUCLEAR REACTIONS 232Th, 238U(d, F), E<10 GeV; Am(d, X)249Bk/249Cf/250Cm/252Cf/254Es/257Es/257Fm, E=1 GeV; calculated fission σ, abundances. Comparison with available data.
doi: 10.1016/j.nimb.2015.02.051
2015MI14 J.Phys.(London) G42, 075104 (2015) S.Misicu, I.N.Mishustin, W.Greiner Instability of α boson vacuum in highly compressed baryonic matter NUCLEAR STRUCTURE 4He; calculated Fermi baryon and antibaryon modes, boson modes for various compressions, particle and antiparticle lowest state, eigenvalues of bosons. Comparison with available data.
doi: 10.1088/0954-3899/42/7/075104
2015TA15 Int.J.Mod.Phys. E24, 1550057 (2015) V.N.Tarasov, K.A.Gridnev, S.Schramm, V.I.Kuprikov, D.K.Gridnev, D.V.Tarasov, K.S.Godbey, X.Vinas, W.Greiner Light exotic nuclei with extreme neutron excess and 2 ≤ Z ≤ 8 NUCLEAR STRUCTURE 18He, 40C; calculated neutron and proton rms radii, density distributions. HF + BCS method.
doi: 10.1142/S0218301315500573
2015TA19 Bull.Rus.Acad.Sci.Phys. 79, 819 (2015); Izv.Akad.Nauk RAS, Ser.Fiz 79, 910 (2015) V.N.Tarasov, K.A.Gridnev, W.Greiner, V.I.Kuprikov, D.K.Gridnev, D.V.Tarasov, X.Vinas, K.S.Godbey Investigating the properties of nuclei with extreme neutron excess and 2 ≤ Z ≤ 8 NUCLEAR STRUCTURE 18He, 40Ca; calculated neutron-separation energies; deduced neutron drip line. Hartree-Fock (HF) method with Skyrme forces (SkI2) and allowance for axial deformation and the Bardeen-Cooper-Schrieffer (BCS) pairing approximation.
doi: 10.3103/S1062873815070242
2015ZA05 Acta Phys.Pol. B46, 427 (2015) Production of Neutron-rich Nuclei in Low-energy Multinucleon Transfer Reactions NUCLEAR STRUCTURE N=126; analyzed available data; deduced nuclei parameters, production σ.
doi: 10.5506/APhysPolB.46.427
2015ZA11 Nucl.Phys. A944, 257 (2015) Cross sections for the production of superheavy nuclei NUCLEAR REACTIONS 208Pb(58Fe, x), E(cm)=210-250 MeV;236U(12C, x), E(cm)=55-90 MeV; calculated evaporation residues σ, survival probability. Compared with available data.
doi: 10.1016/j.nuclphysa.2015.02.010
2014GR09 Eur.Phys.J. A 50, 118 (2014) D.K.Gridnev, S.Schramm, K.A.Gridnev, W.Greiner Nuclear interactions with modern three-body forces lead to the instability of neutron matter and neutron stars
doi: 10.1140/epja/i2014-14118-6
2014MA42 Nucl.Data Sheets 118, 329 (2014) Yu.Malyshkin, I.Pshenichnov, I.Mishustin, W.Greiner Interaction of Fast Nucleons with Actinide Nuclei Studied with GEANT4 NUCLEAR REACTIONS 241Am(p, F), E=threshold-1000 MeV;calculated fission σ, mass distribution of products at 26.5 and 62.9 MeV. 241,243Am(n, F), E=0-20 MeV; calculated fission σ, neutron multiplicity from 0 to 15 MeV, neutron σ(En) at 2.9 MeV. 241,243Am(n, γ), E=0.2-20000 keV; calculated radiative capture σ. MCADS (Monte Carlo model for Accelerator Driven Systems) based on GEANT4; compared with data.
doi: 10.1016/j.nds.2014.04.072
2014TA23 Bull.Rus.Acad.Sci.Phys. 78, 569 (2014); Izv.Akad.Nauk RAS, Ser.Fiz 78, 782 (2014) V.N.Tarasov, K.A.Gridnev, W.Greiner, S.Schramm, D.K.Gridnev, D.V.Tarasov, X.Vinas Investigation of the properties of nuclei with extreme neutron excess in the vicinity of neutron magic numbers NUCLEAR STRUCTURE 240Ba, 248Gd, 250Dy, 266Pb; calculated single-particle spectra, J, π. Hartree-Fock method.
doi: 10.3103/S1062873814070235
2014ZA04 Acta Phys.Pol. B45, 291 (2014) V.Zagrebaev, A.Karpov, W.Greiner Synthesis of Superheavy Nuclei: Nearest and Distant Opportunities
doi: 10.5506/APhysPolB.45.291
2014ZA05 Phys.Rev. C 89, 054608 (2014) V.I.Zagrebaev, B.Fornal, S.Leoni, W.Greiner Formation of light exotic nuclei in low-energy multinucleon transfer reactions NUCLEAR REACTIONS 100Mo(20Ne, X), E=146 MeV; 89Y(19F, X), E=140 MeV; 159Tb(14N, X), E=92, 115 MeV; 238U(18O, X), E(cm)=125 MeV; 238U(26Mg, X), E(cm)=150 MeV; 238U(36S, X), E(cm)=180 MeV; calculated production σ(Z, A) of Z=5-20, A=6-60 projectile-like fragments (PLFs) using model based on coupled Langevin-type dynamical equations of motion for multinucleon transfers. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.054608
2013DY01 J.Phys.(London) G40, 085101 (2013) A.T.D'yachenko, K.A.Gridnev, W.Greiner Calculation of heavy ion collisions within the framework of the modified hydrodynamic approach NUCLEAR REACTIONS 12C, 108Ag, 197Au(12C, X), E<250 MeV; calculated σ(θ, E). Comparison with experimental data.
doi: 10.1088/0954-3899/40/8/085101
2013PA14 Phys.Rev. C 87, 054905 (2013) Production of antinuclei and hypernuclei in a relativistic Hagedorn resonance gas model
doi: 10.1103/PhysRevC.87.054905
2013PO06 J.Phys.(London) G40, 105105 (2013) D.N.Poenaru, R.A.Gherghescu, W.Greiner Nuclear inertia and the decay modes of superheavy nuclei RADIOACTIVITY 284Cn(SF); calculated potential barriers. 132Sn, 152Sm, 130Cd, 154Gd, 138,142,146Ba, 140Ce, 144Xe;deduced mass and charge asymmetry, fission fragment parameters, T1/2. Comparison AME 2012 and other data.
doi: 10.1088/0954-3899/40/10/105105
2013PO07 Rom.J.Phys. 58, 1157 (2013) D.N.Poenaru, R.A.Gherghescu, W.Greiner Alpha- Cluster-and Fission Decay of Superheavy Nuclei NUCLEAR STRUCTURE Z=118-124; calculated T1/2 for α-cluster decay and fission. Analytical superasymmetric fission model.
2013SA37 Phys.Rev. C 88, 024908 (2013) L.M.Satarov, I.N.Mishustin, W.Greiner Evolution of antibaryon abundances in the early universe and in heavy-ion collisions
doi: 10.1103/PhysRevC.88.024908
2013TA10 Int.J.Mod.Phys. E22, 1350009 (2013) V.N.Tarasov, K.A.Gridnev, D.K.Gridnev, D.V.Tarasov, S.Schramm, X.Vinas, W.Greiner Stability peninsulas on the neutron drip line NUCLEAR STRUCTURE 40O, 74S, 108Fe, 166Zr, 238Xe, 240Ba, 42Ne, 80Ti, 112Zn, 170Ru, 172Pd, 248Gd, 266Pb; calculated binding energy, quadrupole deformation parameter, neutron and proton rms radii; deduced existence of stability peninsula. HF+BCS method with Skyrme forces.
doi: 10.1142/S0218301313500092
2013TA24 Bull.Rus.Acad.Sci.Phys. 77, 842 (2013); Izv.Akad.Nauk RAS, Ser.Fiz 77, 927 (2013) V.N.Tarasov, K.A.Gridnev, W.Greiner, S.Schramm, D.K.Gridnev, D.V.Tarasov, X.Vinas Peninsula of neutron stability of nuclei in the neighborhood of neutron magic number N = 126 NUCLEAR STRUCTURE 164Sr, 166Zr, 168Mo, 170Ru, 172Pd, 178Te, 180Xe, 186Nd, 190Gd; calculated neutron separation energy, quadrupole deformation parameters, neutron and proton rms radii. Hartree-Fock method with Skyrme forces.
doi: 10.3103/S1062873813070241
2013ZA02 Phys.Rev. C 87, 034608 (2013) Production of heavy trans-target nuclei in multinucleon transfer reactions NUCLEAR REACTIONS 248Cm(48Ca, X), E(cm)=220 MeV; 248Cm(238U, X), E(cm)=770 MeV; 186W(160Gd, X), E(cm)=460 MeV; 208Pb(136Xe, X), E(cm)=526 MeV; 166Er(86Kr, X), E(cm)=464 MeV; 180Hf(86Kr, X), E(cm)=300 MeV; 197Au(192Os, X), E(cm)=610 MeV; 248Cm, 244Pu, 238U(232Th, X), E(cm)=715, 730, 750 MeV; 238U(198Pt, X), E(cm)=700 MeV; 207Pb(64Ni, X), E(cm)=244 MeV; 248Cm(136Xe, X), (238U, X), E(cm)=500 MeV; calculated mass distributions, primary fission fragment cross section. Multi-nucleon transfers. Calculations based on two-center shell model and the adiabatic potential energy. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.034608
2012DE17 Phys.Rev. C 86, 024606 (2012) J.N.De, S.K.Samaddar, X.Vinas, M.Centelles, I.N.Mishustin, W.Greiner Effects of medium on nuclear properties in multifragmentation
doi: 10.1103/PhysRevC.86.024606
2012GR14 J.Phys.:Conf.Ser. 337, 012002 (2012) Superheavy nuclei and beyond: hypermatter and antimatter
doi: 10.1088/1742-6596/337/1/012002
2012GR15 Bull.Rus.Acad.Sci.Phys. 76, 871 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 971 (2012) K.A.Gridnev, W.Greiner, V.N.Tarasov, S.Schramm, D.K.Gridnev, D.V.Tarasov, X.Vinas Investigating the neutron and proton density distributions in extremely neutron-rich nuclei NUCLEAR STRUCTURE 16,40O, 90,166Zr, 146,248Gd, 240Ba, 266Pb, 344Rn; calculated neutron and proton density distributions, neutron and proton rms radii. Hartree-Fock method using the Skyrme forces.
doi: 10.3103/S1062873812080138
2012KA03 Int.J.Mod.Phys. E21, 1250013 (2012) A.V.Karpov, V.I.Zagrebaev, Y.Martinez Palenzuela, L.F.Ruiz, W.Greiner Decay propertes and stability of heaviest elements NUCLEAR STRUCTURE Z<132; calculated T1/2. 291,293Cn; deduced island of stability.
doi: 10.1142/S0218301312500139
2012MA60 Bull.Rus.Acad.Sci.Phys. 76, 1165 (2012) Y.Martinez Palenzuela, L.F.Ruiz, A.Karpov, W.Greiner Systematic study of decay properties of heaviest elements RADIOACTIVITY 291,293Cn(β-); calculated T1/2; deduced island of stability. Comparison with available data.
doi: 10.3103/S1062873812110172
2012PO01 J.Phys.(London) G39, 015105 (2012) D.N.Poenaru, R.A.Gherghescu, W.Greiner Simple relationships for α-decay half-lives RADIOACTIVITY 108,109,110Te, 112I, 109,110Xe, 112,113,114Ba, 164,165Re, 173,175Ir, 169Pt, 179Au, 175Hg, 186Tl, 203Bi, 194At, 221Rn, 203,210Fr, 228Ac, 232Am, 238,239Cm, 247Es, 247,249Fm, 247,251Md, 251,255,257No, 253,254,255,258Lr, 257,258Rf, 256,257,258,260Db, 260,261,263,265,271Sg, 261,262,266,272Bh, 265,267,270Hs, 270,276,278Mt, 267,269,279,281Ds, 279,280Rg, 283,284,285Cn, 272,282,283,284,285,286Nh, 286,287,288,289Fl, 287,288,289Mc, 290,291,292,293Lv, 293,294Ts, 294,295Og(α); calculated T1/2; deduced universal decay law using α-like R-matrix theory.
doi: 10.1088/0954-3899/39/1/015105
2012PO04 Rom.J.Phys. 57, 431 (2012) D.N.Poenaru, R.A.Gherghescu, W.Greiner Metallic Atomic Clusters
2012PO05 Phys.Rev. C 85, 034615 (2012) D.N.Poenaru, R.A.Gherghescu, W.Greiner Cluster decay of superheavy nuclei NUCLEAR STRUCTURE Z=104-124; calculated half-lives and branching ratios for α decay, and competing cluster decay with spontaneous emission of Be, C, Ar, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Sr, Y, Zr, Nb, and Mo isotopes. Analytical superasymmetric fission (ASAF) model with Q values from AME-11, and three different theoretical mass calculations. Discussed unexpected dominance of cluster decay over α decay for some of the heaviest superheavy isotopes, and need for better accuracy of calculated masses in the region of heaviest SHE for reliable half-life predictions. RADIOACTIVITY 302,303,304122(α), (96Zr); 304124(α), (95Zr), (96Zr), (98Mo); 305,306124(α), (100Mo); 307124(α), (102Mo); calculated Q values, half-lives for α and cluster decay, branching ratios. Analytical superasymmetric fission (ASAF) model with Q values from three different theoretical mass calculations.
doi: 10.1103/PhysRevC.85.034615
2012PO09 Int.J.Mod.Phys. E21, 1250022 (2012) D.N.Poenaru, R.A.Gherghescu, W.Greiner Competition of α decay and heavy particle decay in superheavy nuclei NUCLEAR STRUCTURE Z=104-126; calculated T1/2 for heavy cluster emission; deduced large half-lives for Z=124. AME11 mass table.
doi: 10.1142/S021830131250022X
2012SC07 Int.J.Mod.Phys. E21, 1250047 (2012) S.Schramm, D.Gridnev, D.V.Tarasov, V.N.Tarasov, W.Greiner The quest for the heaviest uranium isotope NUCLEAR STRUCTURE 320,340,354Cf, 350U, 344Rn; calculated quadrupole deformation parameters, proton and neutron density distributions, one- and two-neutron separation energies. Relativistic mean field and Skyrme-type approaches.
doi: 10.1142/S0218301312500474
2012TA05 Phys.Atomic Nuclei 75, 17 (2012); Yad.Fiz. 75, 19 (2012) V.N.Tarasov, K.A.Gridnev, W.Greiner, D.K.Gridnev, V.I.Kuprikov, D.V.Tarasov, X.Vinas Peninsulas of the neutron stability of nuclei in the vicinity of neutron magic numbers NUCLEAR STRUCTURE 16,40O, 146,248Gd, 238Xe, 240Ba, 266Pb; calculated chemical potentials, neutron separation energies, quadrupole deformation parameters, neutron and proton density distributions; deduced peninsulas of stable of neutron emission nuclei. Hartee-Fock method.
doi: 10.1134/S1063778812010139
2012TA14 Bull.Rus.Acad.Sci.Phys. 76, 876 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 976 (2012) V.N.Tarasov, K.A.Gridnev, W.Greiner, S.Schramm, D.K.Gridnev, D.V.Tarasov, X.Vinas The peninsula of neutron nuclear stability in the vicinity of N = 258 NUCLEAR STRUCTURE 344,346Rn, 348Th, 350U; calculated one- and two-neutron separation energies, quadrupole deformation parameters; deduced peninsula of stable nuclei.
doi: 10.3103/S1062873812080266
2012ZA01 Phys.Rev. C 85, 014608 (2012) V.I.Zagrebaev, A.V.Karpov, W.Greiner Possibilities for synthesis of new isotopes of superheavy elements in fusion reactions NUCLEAR REACTIONS 250Cm, 251Cf, 254Es, 239Pu, 243Cm, 241Am(48Ca, X), 251Cf(40Ar, X), 243Am(44Ca, X), E*=25-55 MeV; calculated superheavy (SH) nuclei production cross sections, survival probability. Extension of production of SHE region. Empirical channel coupling model for Coulomb barrier and two-center shell model for energy surface calculations. RADIOACTIVITY 285Mc, 286,287,288Lv, 299119(α); suggested decay chains, including possible EC decay of some of the intermediate nuclides in the decay chain.
doi: 10.1103/PhysRevC.85.014608
2011PO02 Phys.Rev. C 83, 014601 (2011) D.N.Poenaru, R.A.Gherghescu, W.Greiner Single universal curve for cluster radioactivities and α decay NUCLEAR STRUCTURE Z=87-96; calculated half-lives of cluster decay modes of 37 heavy nuclei with the emission of 14C, 20O, 23F, 22,24,25,26Ne, 28,30Mg, 32,34Si clusters. Z=52-118; calculated half-lives of α decay for 163 even-even nuclei. A new single line of universal curve (UNIV) for alpha decay and cluster radioactivities based on fission theory. Comparison with the universal decay law (UDL) derived using α-like R-matrix theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014601
2011PO08 Phys.Rev.Lett. 107, 062503 (2011) D.N.Poenaru, R.A.Gherghescu, W.Greiner Heavy-Particle Radioactivity of Superheavy Nuclei RADIOACTIVITY 222Ra, 288Fl(14C), (80Ge); calculated T1/2, spontaneous emission of heavy particles. KTUY05 and FRDM95 mass models.
doi: 10.1103/PhysRevLett.107.062503
2011SH14 J.Phys.(London) G38, 055104 (2011) M.K.Sharma, S.Kanwar, G.Sawhney, R.K.Gupta, W.Greiner Fusion excitation functions of 64Ni+112-132Sn reactions studied on the dynamical cluster-decay model NUCLEAR REACTIONS 112,118,124Sn(64Ni, X)176Pt/182Pt/188Pt/196Pt, 64Ni(132Sn, X)196Pt, E(cm)<200 MeV; calculated fusion σ, fragmentation potentials. Dynamical cluster-decay model.
doi: 10.1088/0954-3899/38/5/055104
2011SH27 J.Phys.(London) G38, 105101 (2011) M.K.Sharma, G.Sawhney, R.K.Gupta, W.Greiner The decay of the compound nucleus 215Fr* formed in the 11B+204Pb and 18O+197Au reaction channels using the dynamical cluster-decay model NUCLEAR REACTIONS 204Pb(11B, X)215Fr, 197Au(18O, X)215Fr, E(cm)=60.24 MeV; calculated cross sections, compound nucleus decay barrier for fusion-fission mode. Dynamical cluster-decay model.
doi: 10.1088/0954-3899/38/10/105101
2011ZA01 Phys.Rev. C 83, 044618 (2011) Production of heavy and superheavy neutron-rich nuclei in transfer reactions NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; calculated production σ for N=126 nuclei, energy-mass distribution, isotopic yields, angular distribution of Pt isotopes. 9Be(208Pb, X), E(cm)=1 GeV/nucleon; calculated cross section for proton removal process. 208Pb(136Xe, X), E(cm)=430-550 MeV; 86Kr, 132Sn, 136Xe, 192Os(208Pb, X), E(cm)=330-620 MeV; 136Xe(198Pt, X), E(cm)=435 MeV; calculated production cross section of Pt nuclei. 248Cm(238U, X), E(cm)=730-830 MeV; 248Cm(136Xe, X), E(cm)=500 MeV; 248Cm(48Ca, X), E(cm)=220, 800 MeV; calculated cross sections of production of Z=72-113, A=200-290 nuclei. Multi-particle transfer reactions for production of heavy and superheavy neutron-rich nuclei. Langevin equations of motion. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044618
2011ZA07 Phys.Rev. C 84, 044617 (2011) V.I.Zagrebaev, A.V.Karpov, I.N.Mishustin, W.Greiner Production of heavy and superheavy neutron-rich nuclei in neutron capture processes NUCLEAR STRUCTURE Z=100-126, N=140-190; calculated decay modes and T1/2 of superheavy nuclei. A=238-265; calculated yields of heavy nuclei and compared with experimental values. Z=92-103; calculated yields of superheavy elements in reactors. 291,293Cn; discussed formation of long-lived SHE in astrophysical r processes.
doi: 10.1103/PhysRevC.84.044617
2010GR01 Int.J.Mod.Phys. E19, 449 (2010) K.A.Gridnev, V.N.Tarasov, D.V.Tarasov, D.K.Gridnev, V.V.Pilipenko, W.Greiner Theoretical prediction of extremely neutron rich Zr and Pb NUCLEAR STRUCTURE 150,152Zr, 224,226,230,232,266,268,270,272,274,276,278,280,282,284,286,288Pb;calculated one-neutron separation energies, neutron and proton parameters of quadrupole deformation; deduced existence of island of stability around 152Zr; Deformed HF calculations with Skyrme forces.
doi: 10.1142/S0218301310014868
2010GR08 Nucl.Phys. A834, 323c (2010) Extension of the Periodic System: Superheavy, Superneutronic, Superstrange, Antimatter Nuclei
doi: 10.1016/j.nuclphysa.2010.01.033
2010LA08 Phys.Rev. C 82, 024602 (2010) A.B.Larionov, I.N.Mishustin, L.M.Satarov, W.Greiner Possibility of cold nuclear compression in antiproton-nucleus collisions NUCLEAR REACTIONS 16O(p-bar, X), E at 0.3-10 GeV/c; calculated nucleon and antiproton densities, antiproton survival probability, probability of antiproton annihilation in compressed zone (ACZ), radial and momentum distributions of annihilation points, antiproton annihilation cross section, and other dynamical properties using Giessen Boltzmann-Uehling-Uhlenbeck microscopic transport model with relativistic mean fields.
doi: 10.1103/PhysRevC.82.024602
2010NI16 J.Phys.(London) G37, 115103 (2010) Establishing the island of stability for superheavy nuclei via the dynamical cluster-decay model applied to a hot fusion reaction 48Ca + 238U → 286112* NUCLEAR REACTIONS 238U(48Ca, X)286Cn, E(cm)=200.6 MeV; calculated scattering potentials, preformation probability for compound system, neck-length parameter, fusion ER σ. Dynamical cluster model (DCM).
doi: 10.1088/0954-3899/37/11/115103
2010PO07 Nucl.Phys. A834, 163c (2010) Extension of superasymmetric fission theory from cluster decay to nanophysics RADIOACTIVITY Z=87-96(α), (14C), (20O), (24Ne), (25Ne), (28Mg), (30Mg), (32Si), (34Si); analyzed T1/2 for cluster decay. Discussed cluster emission from metallic clusters.
doi: 10.1016/j.nuclphysa.2009.12.029
2010TA25 Bull.Rus.Acad.Sci.Phys. 74, 1559 (2010); Izv.Akad.Nauk RAS, Ser.Fiz 74, 1624 (2010) V.N.Tarasov, K.A.Gridnev, D.K.Gridnev, V.I.Kuprikov, D.V.Tarasov, W.Greiner, X.Vinyes Investigating the neutron stability of neutron-rich O, Ar, Kr, and Rn isotopes NUCLEAR STRUCTURE 40,42O, 38,58,76Ar, 118,120,126,132,134,136,138Kr, 254,256,270,274,282,304,306,308,314Rn; calculated single-particle levels, two-, one-neutron separation energies, quadrupole deformation. Hartee-Fock method with Skyrme forces.
doi: 10.3103/S1062873810110158
2010ZA04 Phys.Rev. C 81, 044608 (2010) V.I.Zagrebaev, A.V.Karpov, W.Greiner True ternary fission of superheavy nuclei RADIOACTIVITY 292Lv(SF) [from 248Cm(48Ca, X), E not given]; 476184(SF)[from 238U(238U, X), E not given]; calculated adiabatic potential energies for ternary fission using liquid drop model (LDM) plus shell corrections within the formalism of two-center shell-model (TCSM).
doi: 10.1103/PhysRevC.81.044608
2010ZA08 Nucl.Phys. A834, 366c (2010) New ideas on the production of heavy and superheavy neutron rich nuclei NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; calculated σ. 248Cm(238U, X), E(cm)=800 MeV; calculated superheavy element production σ. Langevin-type dynamical equations of motion model.
doi: 10.1016/j.nuclphysa.2010.01.041
2009GU06 Int.J.Mod.Phys. E18, 601 (2009) R.K.Gupta, Niyti, M.Manhas, S.Hofmann, W.Greiner Role of static deformation and compact orientation of target nucleus in measured fusion, fusion-fission and capture cross-sections of 244Pu + 48Ca reaction NUCLEAR REACTIONS 244Pu(48Ca, X), E≈ 31-53 MeV; calculated the fusion evaporation, fusion-fusion and quasi-fission excitation functions, neutron evaporation σ. Dynamical cluster decay model.
doi: 10.1142/S0218301309012744
2009GU09 J.Phys.(London) G36, 075104 (2009) R.K.Gupta, D.Singh, R.Kumar, W.Greiner Universal functions of nuclear proximity potential for Skyrme nucleus-nucleus interaction in a semiclassical approach NUCLEAR REACTIONS 32S(40Ca, X), 64Ni(64Ni, X), E(cm)=109 MeV;Calculated nuclear proximity potential. Thomas-Fermi approach.
doi: 10.1088/0954-3899/36/7/075104
2009GU25 J.Phys.(London) G36, 115105 (2009) R.K.Gupta, Niyti, M.Manhas, W.Greiner Island of stability for superheavy elements and the dynamical cluster-decay model for fusion evaporation residue cross sections: 48Ca+238U → 286112* as an example NUCLEAR REACTIONS 238U(48Ca, X)286Cn, E(cm)=200.6 MeV; calculated fusion evaporation residue σ for 3- and 4-neutron emission; deduced island of stability around Z=126 and N=184.
doi: 10.1088/0954-3899/36/11/115105
2009KA23 Int.J.Mod.Phys. E18, 1453 (2009) S.Kanwar, M.K.Sharma, B.Singh, R.K.Gupta, W.Greiner Decay of 202Pb formed in 48Ca+154Sm reaction using the dynamical cluster-decay model NUCLEAR REACTIONS 154Sm(48Ca, X)202Pb, E(cm)=140.4, 156.36 MeV; 144Sm(48Ca, X)192Pb, E(cm)=143.6 MeV;calculated scattering and fragmentation potentials for decay of 202Pb, fusion-evaporation residue, compound nucleus fission, fusion-fission, and quasi-fission σ, mass distribution yields. Dynamical cluster-decay model.
doi: 10.1142/S0218301309013725
2009LA16 Phys.Rev. C 80, 021601 (2009) A.B.Larionov, I.A.Pshenichnov, I.N.Mishustin, W.Greiner Antiproton-nucleus collisions simulation within a kinetic approach with relativistic mean fields
doi: 10.1103/PhysRevC.80.021601
2009PO13 J.Phys.(London) G36, 125101 (2009) D.N.Poenaru, R.A.Gherghescu, W.Greiner Special properties of 264Fm and of atomic clusters emitting singly charged trimers NUCLEAR STRUCTURE 264Fm; calculated potential energy surfaces, deformation energies.Comparison with superheavy nucleus 294118.
doi: 10.1088/0954-3899/36/12/125101
2008BA50 Phys.Rev. C 78, 065804 (2008) S.Banik, W.Greiner, D.Bandyopadhyay Critical temperature of antikaon condensation in nuclear matter
doi: 10.1103/PhysRevC.78.065804
2008BU02 J.Phys.(London) G35, 025103 (2008) T.J.Burvenich, L.Guo, P.Klupfel, P.-G.Reinhard, W.Greiner Proton-neutron deformations in 16C and their consequences NUCLEAR STRUCTURE 16C; calculated deformation parameters and rms radii mean field models.
doi: 10.1088/0954-3899/35/2/025103
2008GH03 Phys.Rev. C 78, 024604 (2008) R.A.Gherghescu, D.N.Poenaru, W.Greiner Proton gap due to the necking potential NUCLEAR REACTIONS 144Nd(92Se, F)E not given; calculated deformation energy, penetrabilities of 144Nd+92Se fission channel.
doi: 10.1103/PhysRevC.78.024604
2008GH05 Int.J.Mod.Phys. E17, 2221 (2008) R.A.Gherghescu, D.N.Poenaru, W.Greiner Binary and ternary emission from superheavy nuclei RADIOACTIVITY 282,288,294120(SF); calculated dynamical barriers for the main and ternary fission channels.
doi: 10.1142/S0218301308011379
2008GU11 J.Phys.(London) G35, 075106 (2008) R.K.Gupta, S.K.Patra, P.D.Stevenson, C.Beck, W.Greiner Fission of hyper-hyperdeformed 56Ni: a clustering analysis within mean-field approaches NUCLEAR STRUCTURE 56Ni; calculated binding energy, radii, matter density distributions; deduced alpha-clustering effect. Compared two models.
doi: 10.1088/0954-3899/35/7/075106
2008LA10 Phys.Rev. C 78, 014604 (2008) A.B.Larionov, I.N.Mishustin, L.M.Satarov, W.Greiner Dynamical simulation of bound antiproton-nuclear systems and observable signals of cold nuclear compression NUCLEAR REACTIONS 16O, 40Ca, 208Pb(p-bar, X), E not given; calculated nucleon density, emitted nucleon spectra, pion multiplicity distributions. Self-consistent relativistic mean field approach, bound anti-proton nuclear systems. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.014604
2008MI19 Phys.Rev. C 78, 024901 (2008) A.Mishra, S.Schramm, W.Greiner Kaons and antikaons in asymmetric nuclear matter
doi: 10.1103/PhysRevC.78.024901
2008PO07 Int.J.Mod.Phys. E17, 2255 (2008) Cluster radioactivities - past, present and future
doi: 10.1142/S0218301308011446
2008TA20 Phys.Atomic Nuclei 71, 1255 (2008); Yad.Fiz. 71, 1283 (2008) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, W.Greiner, V.G.Kartavenko, V.V.Pilipenko Properties of lead isotopes in the vicinity of the neutron drip line NUCLEAR STRUCTURE 266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288Pb; calculated S(1n), S(2n), quadrupole deformation parameters, root mean square radii; HF+BCS, HFB approximation; Skyrme forces.
doi: 10.1134/S1063778808070193
2008TA22 Bull.Rus.Acad.Sci.Phys. 72, 842 (2008) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, W.Greiner, V.G.Kartavenko, V.I.Kuprikov Properties of Zr isotopes near the neutron drip line and beyond it NUCLEAR STRUCTURE Zr; calculated neutron and two-neutron separation energies, mean-square radii, neutron and proton quadrupole deformation parameters of neutron-rich Zr isotopes. Hartree-Fock method with Skyrme forces.
doi: 10.3103/S1062873808060270
2008TA25 Int.J.Mod.Phys. E17, 1273 (2008) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, V.G.Kartavenko, W.Greiner Properties of Fe, Ni and Zn isotopes near the drip-lines NUCLEAR STRUCTURE Fe, Ni, Zn, O; calculated single particle energies, S(1n), S(1p), S(2n), quadrupole deformation parameters, βn, βp, pairing gaps, rms radii; deformed Hartree-Fock method with Skyrme forces; comparison with experimental data and other calculations.
doi: 10.1142/S021830130801043X
2008TO19 Int.J.Mod.Phys. E17, 2150 (2008) S.Yu.Torilov, K.A.Gridnev, W.Greiner New insight on the chain states and Bose-Einstein condensate in light nuclei
doi: 10.1142/S0218301308011252
2008ZA06 Phys.Rev.Lett. 101, 122701 (2008) Production of New Heavy Isotopes in Low-Energy Multinucleon Transfer Reactions NUCLEAR REACTIONS 208Pb(58Ni, X), E=328.4 MeV; calculated proton and neutron stripping and pickup cross sections. Compared results to data. 208Pb(136Xe, X), E(cm)=450 MeV; calculated production cross sections for neutron rich nuclei.
doi: 10.1103/PhysRevLett.101.122701
2008ZA07 Phys.Rev. C 78, 034610 (2008) Synthesis of superheavy nuclei: A search for new production reactions NUCLEAR REACTIONS 208Pb(48Ca, X)256No; 208Pb(50Ti, X)258Rf; 208Pb(54Cr, X)262Sg; 248Cm(48Ca, X), E(cm)=210 MeV; 208Pb(48Ca, n), (48Ca, 2n), (48Ca, 3n), (50Ti, n), (50Ti, 2n), (50Ti, 3n), (54Cr, n), (54Cr, 2n), (54Cr, 3n), (58Fe, n), E=10-40 MeV; 208Pb(48Ca, n), (50Ti, n), (54Cr, n), (58Fe, n), (64Ni, n), (70Zn, n), (76Ge, n), (82Se, n), (86Kr, n), E=15 MeV; 208Pb, 210Po, 222Rn, 226Ra, 232Th, 238U, 244Pu, 248Cm, 249Cf(48Ca, 3n), E=35 MeV; 238U(48Ca, X)286Cn; E=25-55 MeV; 248Cm(44S, X)292Cn, E=25-55 MeV; 248Cm(22O, 5n), (22O, 5n), E=80-115 MeV; 136Xe(136Xe, n), (136Xe, 2n), (136Xe, 3n), (136Xe, 4n), E<50 MeV; 244Pu, 243Am, 249Bk, 249Cf(50Ti, 4n), (50Ti, 2n), (50Ti, 3n), (50Ti, 5n), E=30-55 MeV; 226Ra, 249Bk, 249Cf(48Ca, 2n), (48Ca, 4n), (48Ca, 5n), E=30-55 MeV; 238U(248Cm, X), E not given; calculated survival, fusion and compound nucleus formation probabilities, absorption and production σ.
doi: 10.1103/PhysRevC.78.034610
2008ZA09 J.Phys.(London) G35, 125103 (2008) New way for the production of heavy neutron-rich nuclei NUCLEAR REACTIONS 208Pb(58Ni, X), E=328.4 MeV; calculated proton stripping, neutron pickup, proton and neutron transfer cross sections. 238U(82Se, X), E=500 MeV; calculated fragmentation cross sections. 248Cm(238U, X), E(cm)=500 MeV; 208Pb(48Ca, X), E(cm)=185 MeV; 208Pb(136Xe, X), E(cm)=450 MeV; 248Cm(48Ca, X), E(cm)=210 MeV; calculated cross sections. Comparisons to experimental data.
doi: 10.1088/0954-3899/35/12/125103
2008ZA12 Int.J.Mod.Phys. E17, 2199 (2008) Clustering phenomena in superheavy nuclear systems NUCLEAR REACTIONS 248Cm(48Ca, X), E(cm)=203 MeV; 243Am, 249Bk, 249Cf(50Ti, X)293Ts/299119/299120, E=30-55 MeV; 248Cm(238U, X), E(cm)=800 MeV;calculated TKE-mass distributions of reaction products, excitation functions of 50Ti, isotope yields.
doi: 10.1142/S0218301308011343
2007BR11 Int.J.Mod.Phys. E16, 777 (2007) L.Bravina, I.Arsene, M.S.Nilsson, K.Tywoniuk, E.Zabrodin, M.Bleicher, H.Stocker, W.Greiner Equilibration of matter in relativistic heavy-ion collisions
doi: 10.1142/S0218301307006277
2007BU26 Phys.Rev. C 76, 034310 (2007) T.J.Burvenich, I.N.Mishustin, W.Greiner Nuclei embedded in an electron gas
doi: 10.1103/PhysRevC.76.034310
2007GR15 Int.J.Mod.Phys. E16, 1059 (2007) K.A.Gridnev, S.Yu.Torilov, V.G.Kartavenko, W.Greiner Model of binding alpha-particles and structure of the light nuclei
doi: 10.1142/S0218301307006502
2007GU04 Phys.Rev. C 75, 024603 (2007) Semiclassical and microscopic calculations of the spin-orbit density part of the Skyrme nucleus-nucleus interaction potential with temperature effects included NUCLEAR REACTIONS 28Si(28Si, X), 24Mg(24Mg, X), 26Mg(26Mg, X), E not given; calculated spin-orbit interaction potential for transfer reactions. Comparison of semiclassical and microscopic shell model approaches.
doi: 10.1103/PhysRevC.75.024603
2007GU20 Int.J.Mod.Phys. E16, 1721 (2007) R.K.Gupta, S.K.Patra, P.D.Stevenson, W.Greiner A highly neutron-rich cluster and/or a superheavy nucleus in the compound nucleus 238U+238U: A Mean field study NUCLEAR REACTIONS 238U(238U, X), E not given; calculated neutron and proton matter density distributions, resonance state properties, clustering structures in the superheavy nucleus using a relativistic mean field and non-relativistic Hartree-Fock approach.
doi: 10.1142/S0218301307006137
2007PA30 J.Phys.(London) G34, 2073 (2007) S.K.Patra, R.K.Gupta, B.K.Sharma, P.D.Stevenson, W.Greiner Exotic clustering in heavy and superheavy nuclei within the relativistic and non-relativistic mean field formalisms NUCLEAR STRUCTURE 222Ra, 232U, 236Pu, 242Cm; Z=114; calculated binding energies, deformation parameters, and rms charge radii within the relativistic mean field approach and the non-relativistic Skyrme-Hartree-Fock formalism.
doi: 10.1088/0954-3899/34/9/016
2007PO08 Int.J.Mod.Phys. E16, 995 (2007) D.N.Poenaru, R.A.Gherghescu, I.H.Plonski, W.Greiner Heavy particle radioactivities NUCLEAR STRUCTURE 228Th; calculated potential energy surface for binary decay modes using macroscopic-microscopic model.
doi: 10.1142/S0218301307006459
2007TA19 Bull.Rus.Acad.Sci.Phys. 71, 747 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 774 (2007) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, V.G.Kartavenko, W.Greiner, V.E.Mitroshin Neutron-deficient and neutron-rich Fe and Ni isotopes near the drip line NUCLEAR STRUCTURE Fe, Ni; calculated proton and neutron separation energies using the Hartree-Fock method with Skyrme forces.
doi: 10.3103/S1062873807060019
2007TO19 Int.J.Mod.Phys. E16, 1757 (2007) S.Yu.Torilov, K.A.Gridnev, W.Greiner Chain configurations in light nuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg; calculated level, J, π for the rotational bands of the chain configurations. Compared results to available data.
doi: 10.1142/S0218301307006927
2007ZA04 Phys.Rev. C 75, 035809 (2007) V.I.Zagrebaev, V.V.Samarin, W.Greiner Sub-barrier fusion of neutron-rich nuclei and its astrophysical consequences NUCLEAR REACTIONS 58Ni(18O, X), 60Ni(16O, X), E(cm) ≈ 25-40 MeV; 48Ca(40Ca, X), (48Ca, X), 90,96Zr(40Ca, X), E(cm) ≈ 80-110 MeV; 132,134Sn(64Ni, X), E(cm) ≈ 130-160 MeV; 68Zn(11Li, X), 70Zn(9Li, X), E(cm) ≈ 8-16 MeV; calculated fusion σ. 206Pb(6He, 2n), (6He, 3n), 208Pb(α, γ), (α, n), (α, 2n), E(cm) ≈ 10-30 MeV; calculated σ. Semiempirical channel coupling model.
doi: 10.1103/PhysRevC.75.035809
2007ZA12 Physics of Part.and Nuclei 38, 469 (2007) V.Zagrebaev, A.Karpov, Y.Aritomo, M.Naumenko, W.Greiner Potential energy of a heavy nuclear system in fusion-fission processes
doi: 10.1134/S106377960704003X
2007ZA14 Int.J.Mod.Phys. E16, 696 (2007) Collisions of transactinides: Superheavy nuclei and giant nuclear molecules NUCLEAR REACTIONS 238U(238U, X), (248Cm, X), 232Th(250Cf, X), E not given; calculated fragment mass distributions, yields and cross sections within a realistic dynamic model.
doi: 10.1142/S0218301307006435
2007ZA15 Nucl.Phys. A787, 363c (2007) Superheavy nuclei and giant quasi-atoms NUCLEAR REACTIONS 209Bi(136Xe, X), E(cm)=569 MeV; calculated σ, σ(θ, E), fragment yields. 136Xe(136Xe, 2n), (136Xe, 3n), (136Xe, 4n), E*=10-50 MeV; 248Cm(48Ca, 3n), (48Ca, 4n), (54Cr, 3n), (54Cr, 4n), E*=25-50 MeV; calculated σ. 250Cf(232Th, X), E(cm)=800 MeV; 238U, 248Cm(238U, F), E(cm)=800 MeV; calculated fission fragment yields. 248Cm(238U, F), E(cm)=700-875 MeV; calculated fission σ. Semi-empirical two-core model with dynamic Langevin type equations. Discussed reaction mechanism features, time dependence. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.12.057
2007ZA16 J.Phys.(London) G34, 2265 (2007) Shell effects in damped collisions: a new way to superheavies NUCLEAR REACTIONS 186W(160Gd, X), E(cm)=460 MeV; calculated potential energy surfaces, fragment yields and mass distributions.
doi: 10.1088/0954-3899/34/11/004
2006GH06 J.Phys.(London) G32, L73 (2006) R.A.Gherghescu, D.N.Poenaru, W.Greiner, Y.Nagame Synthesis of 286114 and 290114 using low-energy fusion channels NUCLEAR REACTIONS 172Er(114Pd, X), (118Pd, X), 170Er(116Pd, X), (120Pd, X), 168Er(118Pd, X), (122Pd, X), 144Ba(142Ce, X), 144Ce(142Ba, X), 146Ce(140Ba, X), 148Ce(138Ba, X), 162Gd(124Sn, X), 160Gd(126Sn, X), 158Gd(128Sn, X), 156Gd(130Sn, X), 156Sm(130Te, X), 154Sm(132Te, X), 152Sm(134Te, X), 168Dy(118Cd, X), (122Cd, X), 166Dy(120Cd, X), 164Dy(122Cd, X), 150Nd(136Xe, X), 148Nd(138Xe, X), 170Yb(120Ru, X), 172Yb(118Ru, X), 174Yb(116Ru, X), 176Yb(114Ru, X), 178Yb(112Ru, X), 180Yb(110Ru, X), 174Hf(116Mo, X), 176Hf(114Mo, X), 178Hf(112Mo, X), 180Hf(110Mo, X), 182Hf(108Mo, X), 184Hf(106Mo, X), 186Hf(104Mo, X), 178W(112Zr, X), 182W(108Zr, X), 184W(106Zr, X), 186W(104Zr, X), 188W(102Zr, X), 190W(100Zr, X), 182Os(108Sr, X), 186Os(104Sr, X), 188Os(102Sr, X), 190Os(100Sr, X), 186Pt(104Kr, X), 188Pt(102Kr, X), 190Pt(100Kr, X), E not given; calculated fusion barrier distributions, potential energy. Macroscopic-microscopic approach, dynamic minimization.
doi: 10.1088/0954-3899/32/11/L03
2006GR03 Phys.Atomic Nuclei 69, 1 (2006); Yad.Fiz. 69, 3 (2006) K.A.Gridnev, D.K.Gridnev, V.G.Kartavenko, V.E.Mitroshin, V.N.Tarasov, D.V.Tarasov, W.Greiner Specific Features of the Nuclear Drip Line in the Region of Light Nuclei NUCLEAR STRUCTURE 14,16,18,20,22,24,26,28,30O; calculated one- and two-neutron separation energies, one-proton separation energies. 20,40O; calculated proton and neutron density distributions. 38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80Ca; calculated one- and two-neutron separation energies. Skyrme-Hartree-Fock approach.
doi: 10.1134/S1063778806010017
2006GR07 Int.J.Mod.Phys. E15, 673 (2006) K.A.Gridnev, D.K.Gridnev, V.G.Kartavenko, V.E.Mitroshin, V.N.Tarasov, D.V.Tarasov, W.Greiner On stability of the neutron-rich oxygen isotopes NUCLEAR STRUCTURE 14,16,18,20,22,24,26,28,30,32,34,36,38,40,42,44O; calculated proton, neutron, and two-neutron separation energies. 20,40O; calculated proton and neutron distributions. 38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80Ca; calculated one and two neutron separation energies. Hartree-Fock approach, Skyrme forces.
doi: 10.1142/S0218301306004053
2006GR11 J.Nucl.Radiochem.Sci. 7, R1 (2006) Long-Lived Superheavy Nuclear and Giant Quasi-Atoms Produced in Damped Collisions of Transactinides NUCLEAR REACTIONS 238U, 248Cm(238U, X), 250Cf(232Th, X), E=800 MeV; calculated fragment isotopic yields; deduced possible superheavy nucleus production. Multidimensional transport equations.
doi: 10.14494/jnrs2000.7.R1
2006GU05 J.Phys.(London) G32, 345 (2006) R.K.Gupta, M.Balasubramaniam, R.Kumar, D.Singh, S.K.Arun, W.Greiner The dynamical cluster-decay model of preformed clusters for a hot rotating 116Ba* nucleus produced in the low-energy 58Ni + 58Ni reaction NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=100-400 MeV; calculated fragment mass distributions, light charged particle and intermediate mass fragment production σ, preformation probability, angular momentum effects. Dynamical cluster-decay model.
doi: 10.1088/0954-3899/32/3/009
2006GU07 J.Phys.(London) G32, 565 (2006) R.K.Gupta, M.Balasubramaniam, S.Kumar, S.K.Patra, G.Munzenberg, W.Greiner Magic numbers in exotic light nuclei near drip lines NUCLEAR STRUCTURE 12,14Be, 18Ne, 29F; calculated cluster configurations potential energies; deduced shell closure features.
doi: 10.1088/0954-3899/32/4/012
2006GU12 Phys.Rev. C 73, 054307 (2006) R.K.Gupta, M.Manhas, W.Greiner Compactness of the 48Ca induced hot fusion reactions and the magnitudes of quadrupole and hexadecapole deformations NUCLEAR REACTIONS 232Th, 238U, 244Pu, 248Cm(48Ca, X), 236U, 242Pu, 246Cm(50Ca, X), 226Ra, 232Th, 238U, 242Pu(54Ti, X), 220Rn, 226Ra, 232Th, 236U(60Cr, X), 220Rn(66Fe, X), 222Rn(70Ni, X), 208Pb, 220Rn(72Ni, X), 206Hg(74Zn, X), (80Ge, X), 208Pb(78Zn, X), (88Se, X), 210Pb(82Ge, X), (86Se, X), 195Os(85Se, X), 206Pb(90Se, X), 194Os, 206Hg, 210Pb(86Se, X), 194Os(92Kr, X), (98Sr, X), (102Zr, X), 192W(100Zr, X), 180Yb, 190W(106Mo, X), 178Yb, 184Hf(108Mo, X), 172Dy(108Ru, X), 146Ce, 152Nd, 158Sm, 162Gd(134Te, X), E not given; calculated scattering and fragmentation potentials, role of quadrupole and hexadecapole deformation, orientation effects. Fragmentation theory.
doi: 10.1103/PhysRevC.73.054307
2006MA61 Phys.Rev. C 74, 034603 (2006) M.Manhas, R.K.Gupta, Q.Li, S.K.Patra, W.Greiner Higher-multipole deformations and compactness of hot fusion reactions NUCLEAR REACTIONS 226Ra(54Ti, X), (60Cr, X), 184W, 238U, 244Pu(48Ca, X), 198Os(92Kr, X), 232Th(60Cr, X), E not given; calculated fusion barrier energies, effects of high-multipole deformations.
doi: 10.1103/PhysRevC.74.034603
2006ME12 Int.J.Mod.Phys. E15, 1149 (2006) M.S.Mehta, B.K.Sharma, S.K.Patra, R.K.Gupta, W.Greiner Decrease of the spin-orbit interaction in drip-line nuclei, using relativistic mean field models NUCLEAR STRUCTURE F, Mg, Sb, Pb, Bi; calculated spin-orbit splitting energy vs neutron excess. 120,130,140,150,160,170,180,190Nd; calculated radial dependence of spin-orbit potential.
doi: 10.1142/S0218301306004740
2006MI17 J.Phys.(London) G32, L59 (2006) I.N.Mishustin, L.M.Satarov, W.Greiner Possible glueball production in relativistic heavy-ion collisions NUCLEAR REACTIONS Au(Au, X), E(cm)=30-5000 GeV/nucleon; calculated φ-meson and glueball multiplicities. Thermal model.
doi: 10.1088/0954-3899/32/9/L01
2006PO02 Phys.Rev. C 73, 014608 (2006) D.N.Poenaru, R.A.Gherghescu, W.Greiner Potential energy surfaces for cluster emitting nuclei RADIOACTIVITY 222Ra(14C); 232U(24Ne); 236Pu(28Mg); 242Cm(34Si); calculated potential energy surfaces, cluster emission and fission barrier features, shell effects. Asymmetric two-center shell model.
doi: 10.1103/PhysRevC.73.014608
2006PO08 Phys.Rev. C 74, 014312 (2006) D.N.Poenaru, I.-H.Plonski, W.Greiner α-decay half-lives of superheavy nuclei NUCLEAR STRUCTURE Z=93-118; calculated α-decay T1/2. Several models compared with data.
doi: 10.1103/PhysRevC.74.014312
2006PO11 J.Phys.(London) G32, 1223 (2006) D.N.Poenaru, I.H.Plonski, R.A.Gherghescu, W.Greiner Valleys due to Pb and Sn on the potential energy surface of superheavy and lighter α-emitting nuclei NUCLEAR STRUCTURE 106Te, 212Po, 294Og; calculated potential energy surfaces; deduced shell effects. Two-center shell model. Systematics of α-decay half-lives discussed.
doi: 10.1088/0954-3899/32/9/002
2006SH01 J.Phys.(London) G32, L1 (2006) B.K.Sharma, P.Arumugam, S.K.Patra, P.D.Stevenson, R.K.Gupta, W.Greiner Clustering in superheavy nuclei within the relativistic mean field approach NUCLEAR STRUCTURE 292,296,300,304120; calculated binding energies, deformation parameters, radii, matter density distributions; deduced cluster configurations. Relativistic mean field approach.
doi: 10.1088/0954-3899/32/1/L01
2006SH20 J.Phys.(London) G32, 2089 (2006) B.K.Sharma, S.K.Patra, R.K.Gupta, A.Shukla, P.Arumugam, P.D.Stevenson, W.Greiner Reaction cross-sections for light nuclei on 12C using relativistic mean field formalism NUCLEAR REACTIONS 12C(8B, X), (9B, X), (10B, X), (11B, X), (12B, X), (13B, X), (14B, X), (15B, X), (16B, X), (17B, X), (18B, X), (19B, X), (7Be, X), (8Be, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (13Be, X), (14Be, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (10Li, X), (11Li, X), E ≈ 800 MeV/nucleon; calculated reaction σ. Relativistic mean field approach. NUCLEAR STRUCTURE 6,7,8,9,10,11Li, 10,11,12,13,14Be, 15,16,17B; calculated binding energies, deformation. Relativistic mean field approach.
doi: 10.1088/0954-3899/32/11/004
2006SI09 Int.J.Mod.Phys. E15, 699 (2006) B.Singh, M.K.Sharma, R.K.Gupta, W.Greiner Entrance-channel effects in the dynamical cluster-decay model for the decay of hot and rotating compound nucleus 48Cr at E8CN ≈ 60 MeV NUCLEAR REACTIONS 24Mg(24Mg, X), E(cm)=44.4 MeV; 12C(36Ar, X), E(cm)=47 MeV; calculated fragment mass, kinetic energy, and angular distributions; deduced entrance channel effects. Dynamical cluster-decay model.
doi: 10.1142/S0218301306004521
2006ZA03 Phys.Rev. C 73, 031602 (2006) V.I.Zagrebaev, Yu.Ts.Oganessian, M.G.Itkis, W.Greiner Superheavy nuclei and quasi-atoms produced in collisions of transuranium ions NUCLEAR REACTIONS 250Cf(232Th, X), (248Cm, X), E(cm)=800 MeV; calculated fragment mass distributions. 238U, 248Cm(238U, X), E ≈ 800 MeV/nucleon; calculated fragments isotopic yields. Realistic dynamical model, production of superheavy nuclei discussed.
doi: 10.1103/PhysRevC.73.031602
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