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NSR database version of May 21, 2024.

Search: Author = W.Greiner

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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
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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
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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
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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
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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
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2015ZA05      Acta Phys.Pol. B46, 427 (2015)

V.Zagrebaev, W.Greiner

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
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2015ZA11      Nucl.Phys. A944, 257 (2015)

V.I.Zagrebaev, W.Greiner

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
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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
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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
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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
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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
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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
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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
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2013PA14      Phys.Rev. C 87, 054905 (2013)

S.Pal, W.Greiner

Production of antinuclei and hypernuclei in a relativistic Hagedorn resonance gas model

doi: 10.1103/PhysRevC.87.054905
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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
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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
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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
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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
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2013ZA02      Phys.Rev. C 87, 034608 (2013)

V.I.Zagrebaev, W.Greiner

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
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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
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2012GR14      J.Phys.:Conf.Ser. 337, 012002 (2012)

W.Greiner

Superheavy nuclei and beyond: hypermatter and antimatter

doi: 10.1088/1742-6596/337/1/012002
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2011ZA01      Phys.Rev. C 83, 044618 (2011)

V.I.Zagrebaev, W.Greiner

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
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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
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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
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2010GR08      Nucl.Phys. A834, 323c (2010)

W.Greiner, V.Zagrebaev

Extension of the Periodic System: Superheavy, Superneutronic, Superstrange, Antimatter Nuclei

doi: 10.1016/j.nuclphysa.2010.01.033
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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
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2010NI16      J.Phys.(London) G37, 115103 (2010)

Niyti, R.K.Gupta, W.Greiner

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
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2010PO07      Nucl.Phys. A834, 163c (2010)

D.N.Poenaru, W.Greiner

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
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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
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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
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2010ZA08      Nucl.Phys. A834, 366c (2010)

V.Zagrebaev, W.Greiner

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2008PO07      Int.J.Mod.Phys. E17, 2255 (2008)

D.N.Poenaru, W.Greiner

Cluster radioactivities - past, present and future

doi: 10.1142/S0218301308011446
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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
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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
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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
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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
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2008ZA06      Phys.Rev.Lett. 101, 122701 (2008)

V.Zagrebaev, W.Greiner

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
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2008ZA07      Phys.Rev. C 78, 034610 (2008)

V.Zagrebaev, W.Greiner

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
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2008ZA09      J.Phys.(London) G35, 125103 (2008)

V.Zagrebaev, W.Greiner

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
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2008ZA12      Int.J.Mod.Phys. E17, 2199 (2008)

V.Zagrebaev, W.Greiner

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
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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
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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
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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
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2007GU04      Phys.Rev. C 75, 024603 (2007)

R.K.Gupta, D.Singh, W.Greiner

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
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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
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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
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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
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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
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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
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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
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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
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2007ZA14      Int.J.Mod.Phys. E16, 696 (2007)

V.Zagrebaev, W.Greiner

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
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2007ZA15      Nucl.Phys. A787, 363c (2007)

V.Zagrebaev, W.Greiner

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
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2007ZA16      J.Phys.(London) G34, 2265 (2007)

V.Zagrebaev, W.Greiner

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
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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
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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
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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
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2006GR11      J.Nucl.Radiochem.Sci. 7, R1 (2006)

W.Greiner, V.Zagrebaev

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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