NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Sandulescu Found 127 matches. Showing 1 to 100. [Next]2015AR05 Rom.J.Phys. 60, 147 (2015) Shell Effects in the Fragmentation Potential for Superheavy Elements NUCLEAR STRUCTURE 296Lv; calculated the best target/projectile combinations for formation of superheavy element.
2015AR09 Rom.J.Phys. 60, 1433 (2015) Fast Fission Yields in the Synthesis of the 296Lv Superheavy Element at E*=30 MeV NUCLEAR REACTIONS 248Cm(48Ca, X)296Lv, 200Pt(96Sr, X)296Lv, E not given; calculated production and fission yields; deduced isomeric minima for the adiabatic energy surface.
2014SA42 Eur.Phys.J. A 50, 110 (2014) Cold fission from isomeric states of superheavy nuclei NUCLEAR REACTIONS 238U, 244Pu, 248Lv(48Ca, F), E=low; calculated potential energy surface, deformation, fission probability from isomeric states using WKB.
doi: 10.1140/epja/i2014-14110-2
2013SA05 Europhys.Lett. 101, 62001 (2013) A.Sandulescu, M.Mirea, D.S.Delion Microscopic description of the alpha-decay of a superheavy element RADIOACTIVITY 296Lv(α) [from 248Cm(48Ca, X)296Lv, E not given]; calculated T1/2, Q-value. Woods-Saxon potential, comparison with available data.
doi: 10.1209/0295-5075/101/62001
2013SA51 Rom.J.Phys. 58, 1148 (2013) Cold fusion synthesis of a Z=116 superheavy element NUCLEAR REACTIONS 248Cm(48Ca, X)293Lv, E(cm)<220 MeV; calculated σ. Woods-Saxon superasymmetric two-center shell model.
2012MI17 Eur.Phys.J. A 48, 86 (2012) M.Mirea, A.Sandulescu, D.S.Delion 238Pu cluster decay in the macroscopic-microscopic approach RADIOACTIVITY 238Pu(32Si); calculated deformation evolution, fission, neutron, proton levels, J, π, T1/2. Half life compared with experiment.
doi: 10.1140/epja/i2012-12086-5
2011MI16 Nucl.Phys. A870-871, 23 (2011) M.Mirea, A.Sandulescu, D.S.Delion Predictions for 232U cluster-decays within the macroscopic-microscopic approximation RADIOACTIVITY 232U(SF); calculated energy surface, fission trajectory, mass asymmetry, Nilsson levels, T1/2 for the 24Ne cluster emission.
doi: 10.1016/j.nuclphysa.2011.09.007
2010MI07 Phys.Rev. C 81, 044317 (2010) M.Mirea, D.S.Delion, A.Sandulescu Microscopic cold fission yields of 252Cf RADIOACTIVITY 252Cf(SF); calculated deformation energy, fission barrier, cold-fission yields in the framework of two-center shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044317
2010MI09 Rom.J.Phys. 55, 309 (2010) M.Mirea, D.S.Delion, A.Sandulescu Microscopic description of 252Cf cold fission yields NUCLEAR STRUCTURE 252Cf; calculated fission yields, potential and deformation energies, fission barriers. Two center shell model.
2009MI03 Europhys.Lett. 85, 12001 (2009) M.Mirea, D.S.Delion, A.Sandulescu Cold valleys for fission/fusion superheavy elements beyond Z = 118
doi: 10.1209/0295-5075/85/12001
2007DE42 Rom.J.Phys. 52, 43 (2007) Synthesis of superheavy nuclei along cold fission paths NUCLEAR STRUCTURE Z > 117; calculated fission yields using a semiclassical approach. Analyzed best projectile target combinations for production of superheavy nuclei.
2005DE63 Rom.J.Phys. 50, 165 (2005) D.S.Delion, A.Sandulescu, W.Greiner Towards a selfconsistent cluster emission theory NUCLEAR STRUCTURE Z=84-112; analyzed α-decay widths; deduced α-clusterization effects.
2004DE18 Phys.Rev. C 69, 044318 (2004) D.S.Delion, A.Sandulescu, W.Greiner Evidence for α clustering in heavy and superheavy nuclei NUCLEAR STRUCTURE Z=90-118; analyzed α-decay data; deduced α clustering effects.
doi: 10.1103/PhysRevC.69.044318
2003DE02 J.Phys.(London) G29, 317 (2003) D.S.Delion, A.Sandulescu, W.Greiner Anisotropy in the ternary cold fission RADIOACTIVITY 252Cf(SF); calculated potentials and fragment angular distributions, deformation effects, related features for specific ternary cold fission channels. Stationary scattering formalism.
doi: 10.1088/0954-3899/29/2/309
2003DE31 Phys.Rev. C 68, 041303 (2003) D.S.Delion, A.Sandulescu, W.Greiner Probing mean field of neutron rich nuclei by cold fission RADIOACTIVITY 252Cf(SF); calculated cold fission fragment yields, sensitivity to fragments density distributions.
doi: 10.1103/PhysRevC.68.041303
2003DE42 Acta Phys.Hung.N.S. 18, 403 (2003) D.S.Delion, A.Sandulescu, W.Greiner Angular Distribution in Ternary Cold Fission RADIOACTIVITY 252Cf(SF); calculated ternary fission associated light charged particles energy and angular distributions.
doi: 10.1556/APH.18.2003.2-4.49
2002DE09 J.Phys.(London) G28, 289 (2002) D.S.Delion, A.Sandulescu, S.Misicu, F.Carstoiu, W.Greiner Double Fine Structure in Binary Cold Fission RADIOACTIVITY 252Cf(SF); calculated nuclear potential, wave functions, resonance decay widths, yields. 104Mo, 148Ba calculated yields as a function of excited state angular momentum. Stationary scattering theory. Comparison with data.
doi: 10.1088/0954-3899/28/2/308
2002DE20 J.Phys.(London) G28, 617 (2002) Towards a Self-Consistent Microscopic α-Decay Theory NUCLEAR STRUCTURE Os, Pt, Hg; calculated α-decay Q-values, cluster formation features, role of proton-neutron asymmetry.
2002DE53 J.Phys.(London) G28, 2921 (2002) D.S.Delion, A.Sandulescu, W.Greiner Self-consistent description of the ternary cold fission: tri-rotor mode RADIOACTIVITY 252Cf(SF); calculated ternary fission fragments energies, angular distributions; deduced tri-rotor mode. Stationary scattering formalism.
doi: 10.1088/0954-3899/28/12/303
2002ST15 Int.J.Mod.Phys. E11, 119 (2002) Microscopic Coefficients for the Quantum Master Equation of a Fermi System
doi: 10.1142/S0218301302000739
2002ST32 Int.J.Mod.Phys. E11, 379 (2002) Dynamics of a Fermi System in a Blackbody Radiation Field
doi: 10.1142/S0218301302000910
2001DE08 Phys.Rev. C63, 044312 (2001) D.S.Delion, A.Florescu, A.Sandulescu Microscopic Description of the Cold α and 10Be Ternary Fission Yields of 252Cf in Spheroidal Coordinates RADIOACTIVITY 252Cf(SF); calculated fragment dynamics, yields for cold ternary fission. Spheroidal coordinate system.
doi: 10.1103/PhysRevC.63.044312
2001DE38 Phys.Rev. C64, 041303 (2001) D.S.Delion, A.Sandulescu, S.Misicu, F.Carstoiu, W.Greiner Quasimolecular Resonances in the Binary Cold Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated decay widths, fragments angular momentum distributions following cold binary fission. Quasimolecular resonant state.
doi: 10.1103/PhysRevC.64.041303
2001MI28 Phys.Rev. C64, 044610 (2001) S.Misicu, A.Sandulescu, W.Greiner Coupling between Fragment Radial Motion and the Transversal Degrees of Freedom in Cold Fission NUCLEAR STRUCTURE 252Cf; calculated penetrabilities for cold fission, role of collective transverse degrees of freedon.
doi: 10.1103/PhysRevC.64.044610
2001SI03 Nucl.Phys. A679, 317 (2001) I.Silisteanu, W.Scheid, A.Sandulescu Proton, Alpha and Cluster Decay Rates for Nuclei with 52 ≤ Z ≤ 56 and 52 ≤ N ≤ 60 RADIOACTIVITY 105Sb, 109I, 112,113Cs, 114Ba(p); 114Ba(2p); 106,107,108,109,110Te, 110,111,112,113I, 110,111,112,113Xe, 112,113,114,115Cs, 113,114,115,116Ba(α); 113,114,115,116,117,118Ba(12C); calculated T1/2. comparisons with data. NUCLEAR STRUCTURE Z=52-56; Z=84-88; analyzed decay energies, lifetimes; deduced systematic features.
doi: 10.1016/S0375-9474(00)00336-5
2000CA08 Phys.Rev. C61, 044606 (2000) F.Carstoiu, I.Bulboaca, A.Sandulescu, W.Greiner Half-Lives of Trinuclear Molecules RADIOACTIVITY 252Cf(SF); calculated cold ternary fission yields, fragment spectra, T1/2. Coplanar three-body cluster model.
doi: 10.1103/PhysRevC.61.044606
2000FL05 Phys.Rev. C61, 051602 (2000) A.Florescu, A.Sandulescu, D.S.Delion, J.H.Hamilton, A.V.Ramayya, W.Greiner Preformation Probabilities for Light Ternary Particles in the Cold (Neutronless) Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated light ternary particles preformation amplitudes in cold fission, geometric features.
doi: 10.1103/PhysRevC.61.051602
2000MI07 Phys.Rev. C61, 041602 (2000) S.Misicu, A.Sandulescu, W.Greiner Shift of the 21+ State of 10Be in Ternary Cold Fission of 252Cf NUCLEAR STRUCTURE 10Be; calculated level energy shift in ternary cold fission of 252Cf. Self-consistent Hartree-Fock approach, molecular scenario. RADIOACTIVITY 252Cf; calculated level energy shift of 10Be fragment in ternary cold fission. Self-consistent Hartree-Fock approach, molecular scenario.
doi: 10.1103/PhysRevC.61.041602
2000ST10 Int.J.Mod.Phys. E9, 17 (2000) E.Stefanescu, A.Sandulescu, W.Scheid The Collisional Decay of a Fermi System Interacting with a Many-Mode Electromagnetic Field
doi: 10.1016/S0218-3013(00)00003-9
1999HA10 Acta Phys.Slovaca 49, 31 (1999) J.H.Hamilton, A.V.Ramayya, J.K.Hwang, W.Greiner, S.J.Zhu, A.Sandulescu, A.Florescu, J.Kormicki, G.Ter-Akopian, Y.Oganesyan, A.V.Daniel, G.S.Popeko, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, M.W.Drigert, W.E.Collins, W.C.Ma, E.F.Jones, L.K.Peker, P.M.Gore, G.Drafta, B.R.S.Babu, G.Wang, J.K.Deng Cold Spontaneous Fission Processes of 252Cf and the Structure of Neutron Rich Ba and La Nuclei RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin; deduced cold binary, ternary fission yields. 143,144,146Ba, 145,147La deduced high-spin levels, J, π, stable octupole deformation. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13749. 1999KA48 Int.J.Mod.Phys. E8, 381 (1999) V.G.Kartavenko, A.Sandulescu, W.Greiner Ternary Configuration in the Framework of Inverse Mean-Field Method
doi: 10.1142/S0218301399000276
1999MI20 Nuovo Cim. 112A, 313 (1999) S.Misicu, A.Sandulescu, F.Carstoiu, M.Rizea, W.Greiner Long-Range Alpha Characteristics in the Ternary Cold Fission RADIOACTIVITY 252Cf(SF); calculated fragments kinetic energy in ternary cold fission. Deformed cluster model.
1999MI24 Phys.Rev. C60, 034613 (1999) S.Misicu, A.Sandulescu, G.M.Ter-Akopian, W.Greiner Angular Momenta of Even-Even Fragments in the Neutronless Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated fission fragments angular momenta; deduced Coulomb contribution. Molecular model, semiclassical coupled channels formalism.
doi: 10.1103/PhysRevC.60.034613
1999MI38 J.Phys.(London) G25, L147 (1999) S.Misicu, P.O.Hess, A.Sandulescu, W.Greiner Molecular Collective Vibrations in the Ternary Neutronless Fission of 252Cf NUCLEAR STRUCTURE 252Cf; calculated nuclear molecule collective excitations, related features. Three-cluster model.
doi: 10.1088/0954-3899/25/12/103
1999PO31 Bull.Rus.Acad.Sci.Phys. 63, 699 (1999) G.S.Popeko, G.M.Ter-Akopian, J.Hamilton, J.Kormicki, A.V.Daniel, Yu.Ts.Oganessian, A.V.Ramayya, J.K.Hwang, A.Sandulescu, A.Florescu, W.Greiner, J.Kliman, M.Morhac, J.Rasmussen, M.A.Stoyer, J.D.Cole Angular Momenta of Fragments and Dynamics of Spontaneous 252Cf Fission RADIOACTIVITY 252Cf(SF); measured Eγ, γγ-coin, fission fragments angular momenta vs neutron multiplicity and fragment mass. Gammasphere array. Comparison with calculations including flexural vibrations at the scission point.
1999SA33 Fiz.Elem.Chastits At.Yadra 30, 908 (1999); Phys.Part.Nucl. 30, 386 (1999) A.Sandulescu, S.Misicu, F.Carstoiu, W.Greiner Cold-Fission Modes in 252Cf RADIOACTIVITY 252Cf(SF); calculated binary, ternary fission modes potential energy, mass yields; deduced cold fragmentation mechanisms. Deformation-dependent cluster model.
1999SA43 Phys.Rev. C60, 044613 (1999) A.Sandulescu, F.Carstoiu, I.Bulboaca, W.Greiner Cluster Description of Cold (Neutronless) α Ternary Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated fission fragment isotopic yields for cold α ternary fission. Three body cluster model.
doi: 10.1103/PhysRevC.60.044613
1998KA45 Int.J.Mod.Phys. E7, 449 (1998) V.G.Kartavenko, A.Sandulescu, W.Greiner Nonlinear Waves of Nuclear Density
doi: 10.1142/S0218301398000233
1998RA09 Phys.Rev. C57, 2370 (1998) A.V.Ramayya, J.H.Hamilton, J.K.Hwang, L.K.Peker, J.Kormicki, B.R.S.Babu, T.N.Ginter, A.Sandulescu, A.Florescu, F.Carstoiu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, W.C.Ma, P.G.Varmette, J.O.Rasmussen, S.J.Asztalos, S.Y.Chu, K.E.Gregorich, A.O.Macchiavelli, R.W.Macleod, J.D.Cole, R.Aryaeinejad, K.Butler-Moore, M.W.Drigert, M.A.Stoyer, L.A.Bernstein, R.W.Lougheed, K.J.Moody, S.G.Prussin, S.J.Zhu, H.C.Griffin, R.Donangelo Cold (Neutronless) α Ternary Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin; deduced α-associated ternary fission isotopic yields.
doi: 10.1103/PhysRevC.57.2370
1998SA02 J.Phys.(London) G24, 181 (1998) A.Sandulescu, F.Carstoiu, S.Misicu, A.Florescu, A.V.Ramayya, J.H.Hamilton, W.Greiner Neutronless 10Be-Accompanied Ternary Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated 10Be-accompanied neutronless ternary fission isotopic yields. Cluster model, double-folding potential.
doi: 10.1088/0954-3899/24/1/022
1998SA16 Phys.Rev. C57, 2321 (1998) A.Sandulescu, S.Misicu, F.Carstoiu, A.Florescu, W.Greiner Role of the Higher Static Deformation of Fragments in the Cold Binary Fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated cold binary fission isotopic yields; deduced deformation dependence. Cluster model.
doi: 10.1103/PhysRevC.57.2321
1998SA57 Int.J.Mod.Phys. E7, 625 (1998) A.Sandulescu, A.Florescu, F.Carstoiu, A.V.Ramayya, J.H.Hamilton, J.K.Hwang, B.R.S.Babu, W.Greiner Cold (Neutronless) Alpha Ternary Fission of 252Cf: Theory and comparison with experiment RADIOACTIVITY 252Cf(SF); calculated neutronless alpha-associated ternary fission isotopic yields. Cluster model, double folding potential. Comparison with data.
doi: 10.1142/S021830139800035X
1998ST02 Phys.Rev. C57, 798 (1998) E.Stefanescu, R.J.Liotta, A.Sandulescu Giant Resonances as Collective States with Dissipative Coupling
doi: 10.1103/PhysRevC.57.798
1997HA64 Prog.Part.Nucl.Phys. 38, 273 (1997) J.H.Hamilton, A.V.Ramayya, J.K.Hwang, J.Kormicki, B.R.S.Babu, A.Sandulescu, A.Florescu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, S.J.Zhu, M.G.Wang, T.Ginter, J.K.Deng, W.C.Ma, G.S.Popeko, Q.H.Lu, E.Jones, R.Dodder, P.Gore, W.Nazarewicz, J.O.Rasmussen, S.Asztalos, I.Y.Lee, S.Y.Chu, K.E.Gregorich, A.O.Macchiavelli, M.F.Mohar, S.Prussin, M.A.Stoyer, R.W.Lougheed, K.J.Moody, J.F.Wild, L.A.Bernstein, J.A.Becker, J.D.Cole, R.Aryaeinejad, Y.X.Dardenne, M.W.Drigert, K.Butler-Moore, R.Donangelo, H.C.Griffin New Cold and Ultra Hot Binary and Cold Ternary Spontaneous Fission Modes for 252Cf and New Band Structures with Gammasphere RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-, (X-ray)γ-coin, prompt neutron multiplicity following binary, ternary fission; deduced fragments isotopic yields. 142,143,144,145,146,148Ba, 140Xe, 144Ce, 99,100,102Zr, 98,100Sr, 112,114,116Pd, 156,158,160Sm deduced high-spin levels, J, π, rotational bands features. 108,110,112Ru, 148,150,152Ce, 146,148,150,152,154Nd, 140Ba, 98Sr, 104Zr deduced rotational bands features. Gammasphere array.
doi: 10.1016/S0146-6410(97)00037-9
1997LU01 J.Phys.(London) G23, 343 (1997) A.Ludu, A.Sandulescu, W.Greiner Nonlinear Liquid Drop Model. Cnoidal Waves
doi: 10.1088/0954-3899/23/3/005
1997RA39 Nuovo Cim. 110A, 1073 (1997) A.V.Ramayya, J.H.Hamilton, J.K.Hwang, L.K.Peker, J.Kormicki, B.R.S.Babu, T.N.Ginter, A.Sandulescu, A.Florescu, F.Carstoiu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, A.V.Daniel, W.C.Ma, P.G.Varmette, J.O.Rasmussen, S.J.Asztalos, S.Y.Chu, K.E.Gregorich, A.O.Macchiavelli, R.W.MacLeod, J.D.Cole, R.Aryaeinejad, K.Butler-Moore, M.W.Drigert, M.A.Stoyer, L.A.Bernstein, R.W.Lougheed, K.J.Moody, S.G.Prussin, S.J.Zhu, H.C.Griffin, R.Donangelo Cold Binary and Ternary Fragmentations in Spontaneous Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin; deduced fragment isotopic yields, binary, α-associated ternary events features.
doi: 10.1007/BF03035948
1997SA10 J.Phys.(London) G23, L7 (1997) A.Sandulescu, A.Florescu, F.Carstoiu, W.Greiner Cold Alpha-Accompanied Fission of 248Cm RADIOACTIVITY 248Cm(SF); calculated spontaneous cold ternary α-accompanied fission fragment isotopic yields. Double folding potential, Coulomb plus M3Y nucleon-nucleon forces, realistic fragment deformations.
doi: 10.1088/0954-3899/23/3/001
1997SA72 Nuovo Cim. 110A, 1079 (1997) A.Sandulescu, A.Florescu, F.Carstoiu, A.V.Ramayya, J.H.Hamilton, J.K.Hwang, B.R.S.Babu, W.Greiner Binary and Ternary Cold Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin; deduced fragment isotopic yields, 10Be-, 14C-associated ternary events features.
doi: 10.1007/BF03035949
1996AV03 Roum.J.Phys. 41, 7 (1996) V.Avrigeanu, A.Florescu, T.Glodariu, A.Sandulescu Level Density Effect on Cold-Fission Yields of 234U NUCLEAR REACTIONS 233U(n, F), E=thermal; analyzed cold fission yields data; deduced level density effects role.
1996HA27 Phys.Rep. 264, 215 (1996) J.H.Hamilton, G.M.Ter-Akopian, Yu.Ts.Oganessian, J.Kormicki, S.J.Zhu, M.G.Wang, Q.Lu, K.Butler-Moore, A.V.Ramayya, W.C.Ma, B.R.S.Babu, D.Shi, J.K.Deng, G.S.Popeko, A.V.Daniel, W.Greiner, A.Sandulescu, J.D.Cole, R.Aryaeinejad, J.Kliman, V.Polhorsky, M.Morhac, N.R.Johnson, I.Y.Lee, F.K.McGowan, L.K.Peker Structure of Neutron-Rich Nuclei and Neutron Multiplicities in Spontaneous Fission RADIOACTIVITY 252Cf(SF); compiled, reviewed γγ-, γγγ-coin data. 140,143,145,147Ba, 136Te, 138Xe deduced high-spin levels. Other nuclei included.
doi: 10.1016/0370-1573(95)00039-9
1996KA22 Int.J.Mod.Phys. E5, 329 (1996) V.G.Kartavenko, A.Ludu, A.Sandulescu, W.Greiner Nonlinear Approach of Alpha and Cluster Decays in the Reaction Channel NUCLEAR REACTIONS 208Pb(α, X), (28Mg, X), E not given; calculated density distribution vs θ. Nonlinear approach to α-, cluster decay.
doi: 10.1142/S0218301396000153
1996SA13 Phys.Rev. C54, 258 (1996) A.Sandulescu, A.Florescu, F.Carstoiu, W.Greiner, J.H.Hamilton, A.V.Ramayya, B.R.S.Babu Isotopic Yields for the Cold Fission of 252Cf RADIOACTIVITY 252Cf(SF); analyzed cold SF fission isotopic yields data.
doi: 10.1103/PhysRevC.54.258
1996SA18 J.Phys.(London) G22, L87 (1996) A.Sandulescu, A.Florescu, F.Carstoiu, W.Greiner The Cold Fission of 248Cm RADIOACTIVITY 248Cm(SF); calculated cold fission associated fragment yields, probable charge fragmentation vs mass fragmentation; deduced barrier penetration. Heavy cluster radioactivity approach.
doi: 10.1088/0954-3899/22/7/003
1996ST10 Phys.Rev. C53, 3014 (1996) E.Stefanescu, W.Scheid, A.Sandulescu, W.Greiner Cold Fission as Cluster Decay with Dissipation NUCLEAR STRUCTURE 252Cf; calculated cold fission modes fine structure for 148Ba+104Mo, 146Ba+160Mo channels. Analytical model of quantum tunneling.
doi: 10.1103/PhysRevC.53.3014
1995AV05 Phys.Rev. C52, R1755 (1995) V.Avrigeanu, A.Florescu, A.Sandulescu, W.Greiner Cold-Fission Yields at Effective Excitation Energies NUCLEAR REACTIONS 233U(n, F), E=thermal; analyzed cold fission fragment yields vs total excitation energy. Ground state potential barrier penetrabilities, WKB approximation. NUCLEAR STRUCTURE 90Y, 90Zr, 90Nb, 92Zr; calculated nuclear level density parameters. Back-shifted Fermi gas model.
doi: 10.1103/PhysRevC.52.R1755
1995LU11 J.Phys.(London) G21, L41 (1995) A.Ludu, A.Sandulescu, W.Greiner, K.M.Kallman, M.Brenner, T.Lonnroth, P.Manngard Alpha + 28Si Cluster Structure as Solitons on the Nuclear Surface NUCLEAR REACTIONS 28Si(α, α), E=6.5-13 MeV; measured σ(θ) vs E. 32S deduced α-cluster states, J. Nonlinear Lagrangian associated with system dynamics.
doi: 10.1088/0954-3899/21/6/002
1995LU18 J.Phys.(London) G21, 1715 (1995) A.Ludu, A.Sandulescu, W.Greiner Quasimolecular Resonances in the α + 20Ne System NUCLEAR REACTIONS 20Ne(α, α), E not given; analyzed data; deduced composite system spectra.
doi: 10.1088/0954-3899/21/12/008
1994HA31 J.Phys.(London) G20, L85 (1994) J.H.Hamilton, A.V.Ramayya, J.Kormicki, W.-C.Ma, Q.Lu, D.Shi, J.K.Deng, S.J.Zhu, A.Sandulescu, W.Greiner, G.M.Ter-Akopian, Yu.Ts.Oganessian, G.S.Popeko, A.V.Daniel, J.Kliman, V.Polhorsky, M.Morhac, J.D.Cole, R.Aryaeinejad, I.Y.Lee, N.R.Johnson, F.K.McGowan Zero Neutron Emission in Spontaneous Fission of 252Cf: A form of cluster radioactivity RADIOACTIVITY 252Cf(SF); measured γγγ-coin; deduced neutronless spontaneous fission evidence, 106Mo+146Ba, 108Mo+144Ba, 104Zr+148Ce cluster production.
doi: 10.1088/0954-3899/20/8/003
1994ST09 J.Phys.(London) G20, 811 (1994) E.Stefanescu, A.Sandulescu, W.Greiner Analytical Model for Quantum Tunnelling with Dissipation through a Fission-Like Barrier NUCLEAR STRUCTURE 236U; calculated cold fission tunnelling rate vs barrier characteristics, dissipation parameters. Analytical model.
doi: 10.1088/0954-3899/20/5/014
1993FL01 J.Phys.(London) G19, 669 (1993) A.Florescu, A.Sandulescu, C.Cioaca, W.Greiner Mass and Charge Yield Calculations for Cold Fragmentation of Actinide Nuclei NUCLEAR STRUCTURE 230Th, 234,236U; calculated fragment yield vs mass, charge. Dynamical model, cold fragmentation. NUCLEAR REACTIONS 232,233,235U(n, F), E=thermal; calculated fragment yield vs mass, charge. Dynamical model, cold fragmentation.
doi: 10.1088/0954-3899/19/4/020
1993FL08 J.Phys.(London) G19, 1947 (1993) A.Florescu, A.Sandulescu, W.Greiner Isotopic Yields for the Cold Fission of Actinides as a Function of the Fragment Excitation Energies NUCLEAR REACTIONS 233,235U(n, F), E=thermal; calculated light fission fragment relative mass, isotopic yields for fixed fragments total excitation energy. Dynamical model, cold fission.
doi: 10.1088/0954-3899/19/11/021
1993GR06 Phys.Rev. C48, 940 (1993) Coherent States Description of α Decay
doi: 10.1103/PhysRevC.48.940
1993GU11 J.Phys.(London) G19, 2063 (1993) R.K.Gupta, M.Horoi, A.Sandulescu, M.Greiner, W.Scheid Cluster Preformation Probabilities and Fine-Structure Effects in Heavy-Cluster Decays using Folding Potentials RADIOACTIVITY 221Fr, 225Ac, 221,222,223,224,226Ra(14C); calculated cluster decay width, Q, cluster preformation probability, other features. Double-folding potentials.
doi: 10.1088/0954-3899/19/12/011
1993SC38 Roum.J.Phys. 38, 331 (1993) W.Scheid, I.Silisteanu, A.Sandulescu Lifetimes of Cluster Radioactivity of Neutron Deficient Trans-Tin Isotopes RADIOACTIVITY A=114-241; analyzed cluster decay T1/2 vs Q data. 114Ba deduced 12C-decay T1/2, branching ratio relative to α-decay.
1992GU10 J.Phys.(London) G18, 1533 (1992) R.J.Gupta, S.Singh, R.K.Puri, A.Sandulescu, W.Greiner, W.Scheid Influence of the Nuclear Surface Diffuseness on Exotic Cluster Decay Half-Life Times RADIOACTIVITY 224,222Ra(14C), 234U(24Ne), 234U, 238Pu(28Mg), 238Pu(34Si); calculated preformation, WKB penetration probabilities, decay constant, log T1/2, branching ratio relative to α-decay. 223,221Ra, 221Fr(14C), 236,232,234U(24Ne), (26Ne), (28Mg), 236U, 237Np, 238Pu(30Mg), 238Pu(32Si), (34Si), 241Am(34Si), 252Cf(46Ar), (48Ca), (50Ca); calculated branching ratio, preformation probability relative to α-decay; deduced nuclear surface diffuseness role. Preformed cluster model.
doi: 10.1088/0954-3899/18/9/014
1992LU07 Int.J.Mod.Phys. E1, 169 (1992) A.Ludu, A.Sandulescu, W.Greiner A New Large Amplitude Collective Motion in Nuclei. Clusters as Solitons on the Nuclear Surface RADIOACTIVITY 212Po(α); calculated α-decay characteristics, soliton potential barriers. 222,224,226Ra(14C); 228Th(20O); 232,234U, 236Pu(24Ne); 234U, 236Pu(28Mg); calculated soliton potential barriers. Liguid drop model, large amplitude collective motion.
doi: 10.1142/S0218301392000084
1992SA29 Rep.Prog.Phys. 55, 1423 (1992) Cluster Decays NUCLEAR STRUCTURE A=222-298; compiled reviewed cluster decay, other data. Alpha-decay, fission-decay like theories.
doi: 10.1088/0034-4885/55/9/002
1992SA30 Int.J.Mod.Phys. E1, 379 (1992) A.Sandulescu, R.K.Gupta, W.Greiner, F.Carstoiu, M.Horoi Role of Cluster Deformations on Their Preformation Probabilities in Radioactive Cluster-Decay Studies RADIOACTIVITY 230Th, 234,232U(24Ne); 222,224,226Ra(14C); 228Th(20O); 236Pu, 234U(28Mg); calculated cluster preformation probability, Gamow factors, WKB pentrabilities. Folded Michigan-3-Yukawa potential.
doi: 10.1142/S0218301392000199
1991GR20 J.Phys.(London) G17, S429 (1991) Cold Valleys; Cluster Decay, Cold Fusion, Cold Fission - A Unifying Theory of Related Phenomena - RADIOACTIVITY 234U(α), (24Ne); calculated potential energy surface contours, potential barriers. 262Md(SF); calculated fission event number vs total kinetic energy. Unified model for cluster decay, cold fusion, cold fission. NUCLEAR STRUCTURE Z=107-109; calculated potential energy vs target mass. Unified model for cluster decay, cold fusion, cold fission, heavy-ion reactions.
doi: 10.1088/0954-3899/17/S/044
1991IS02 J.Phys.(London) G17, 385 (1991) A.Isar, A.Sandulescu, W.Scheid Use of a Characteristic Function in Open Quantum Systems and Charge Equilibration in Deep Inelastic Reactions NUCLEAR REACTIONS 209Bi(56Fe, X), E=465 MeV; analyzed fragment charge centroid vs time. Lindbald theory, characteristic function.
doi: 10.1088/0954-3899/17/3/015
1991SA08 J.Phys.(London) G17, L83 (1991) A.Sandulescu, A.Florescu, W.Greiner On the Charge Distribution in Very Asymmetric Thermal Neutron Fission of 233,235U and 229Th NUCLEAR REACTIONS 233,235U, 229Th(n, F), E=thermal; analyzed fission data. 234,236U, 230Th deduced charge order features. Cold fission, analogy to SF-decay by light fragment emission.
doi: 10.1088/0954-3899/17/5/005
1989SA45 J.Phys.(London) G15, 1815 (1989) A.Sandulescu, A.Florescu, W.Greiner Cold Fission as Emission of Fragments NUCLEAR REACTIONS 233,235U, 239Pu, 245Cm(n, F), E=thermal; analyzed fission fragment distributions. 234,236U, 240Pu, 246Cm deduced cold fission, exotic decay identity. RADIOACTIVITY 252Cf(SF); analyzed fission fragment distributions; deduced cold fission, exotic decay identity.
doi: 10.1088/0954-3899/15/12/008
1988DE25 J.Phys.(London) G14, 891 (1988) K.Depta, Hou-ji Wang, J.A.Maruhn, W.Greiner, A.Sandulescu Charge Equilibration in Cold Fragmentation NUCLEAR STRUCTURE 234,236U; calculated cold fission product distribution, yields.
doi: 10.1088/0305-4616/14/7/009
1988SA35 Phys.Scr. T23, 43 (1988) Magic Radioactivity RADIOACTIVITY 242,244,246,248,250,252,254,256,258Fm; calculated α-decay, SF-decay, Sn-decay T1/2; deduced systematics. Unified model.
doi: 10.1088/0031-8949/1988/T23/006
1988SA39 Few-Body Systems 5, 107 (1988) A.Sandulescu, E.W.Schmid, G.Spitz Formation of Clusters in the Nuclear Surface NUCLEAR STRUCTURE 8Be; calculated surface α-cluster formation. One-particle density plots, shell, resonating group models.
1987IV01 Rev.Roum.Phys. 32, 549 (1987) M.Ivascu, A.Sandulescu, I.Silisteanu On the Rates of Radioactive Decays by Emission of Heavy Clusters RADIOACTIVITY 222,223,224,226Ra(14C), 231Pa, 232,233U(24Ne); calculated T1/2, branching ratios, one-body resonance widths, cluster spectroscopic factors. Microscopic-macroscopic method.
1987MA45 J.Phys.(London) G13, L127 (1987) M.T.Magda, A.Pop, A.Sandulescu A Model for Large Cluster Transfer in Reactions Leading to Heavy Actinides NUCLEAR REACTIONS 254Es(18O, X)254Fm/255Fm/256Fm/257Fm/258Fm/254Md/255Md/256Md/257Md/258Md/259Md/260Md/256No/257No/258No/259No/260No/258Lr/259Lr/260Lr/261Lr/262Lr/263Lr, E=97 MeV; 249Cf(18O, X)248Es/249Es/250Es/251Es/252Es/253Es/254Es/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm, E=97 MeV; 248Cm(18O, X)246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/251Es/252Es/253Es/254Es/255Es/256Es/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm, E=98 MeV; 248Cm(238U, X)244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/252Es/253Es/254Es/255Es/256Es/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/254Md/255Md/256Md/257Md/258Md, E=7.4 MeV/nucleon; calculated residuals production σ(E); deduced cluster transfer mechanism.
doi: 10.1088/0305-4616/13/7/003
1987MA50 Rev.Roum.Phys. 32, 597 (1987) M.T.Magda, A.Pop, A.Sandulescu Fragmentation Processes in Multinucleon Transfer Reactions NUCLEAR REACTIONS, ICPND 254Es(18O, X)258Lr/259Lr/260Lr/257No/259No/252Fm/254Fm/256Fm/257Fm/255Md/256Md/257Md/258Md/259Md/260Md, E=98 MeV; 254Es(22Ne, X)252Fm/254Fm/255Fm/256Fm/257Fm/254Md/255Md/256Md/257Md/258Md/259Md/260Md/254No/255No/256No/257No/259No/256Lr/258Lr/259Lr, E=126 MeV; 254Es(48Ca, X)253Fm/254Fm/255Fm/256Fm/257Fm/254Md/255Md/256Md/257Md/258Md/259No, E=266 MeV; calculated residuals production σ. Projectile fragmentation model.
1986MA34 Yad.Fiz. 43, 1176 (1986) M.T.Magda, A.Pop, A.Sandulescu Breakup of Projectile Ion and Emission of 2 ≤ Z ≤ 4 Clusters in Heavy-Ion Reactions at Low Energy NUCLEAR REACTIONS 181Ta(20Ne, X)6He/3He/8He/7Li/9Be/10Be, E=178 MeV; 181Ta(22Ne, X)6He/7Li/9Be, E=141 MeV; 232Th(22Ne, X)6He/8Li, E=176 MeV; 232Th(11B, X)8He/6He, E=89 MeV; measured σ(fragment θ, E); deduced cluster production mechanism. Serber model.
1986PO06 At.Data Nucl.Data Tables 34, 423 (1986) D.N.Poenaru, W.Greiner, K.Depta, M.Ivascu, D.Mazilu, A.Sandulescu Calculated Half-Lives and Kinetic Energies for Spontaneous Emission of Heavy Ions from Nuclei NUCLEAR STRUCTURE Z=47-106; calculated, evaluated heavy-ion SF decay characteristics, T1/2, branching ratio relative to α-decay, Q, kinetic energies. Analytical superasymmetric fission model.
doi: 10.1016/0092-640X(86)90013-6
1985DE31 J.Phys.(London) G11, 1087 (1985) K.Depta, R.Herrmann, W.Greiner, W.Scheid, A.Sandulescu Fission Mass Yields of Excited Medium-Heavy Nuclei Studied within the Fragmentation Theory - The 172Yb System as an Example NUCLEAR REACTIONS, ICPND 154Sm(18O, X)172Yb, 150Nd(20Ne, X)172Yb, E not given; calculated fission fragment yields. Fragmentation theory. NUCLEAR STRUCTURE 172Yb; calculated fission potential, mass yield, nuclear shape, fragment deformation parameters. Fragmentation theory.
doi: 10.1088/0305-4616/11/9/015
1985GR01 Z.Phys. A320, 347 (1985) W.Greiner, M.Ivascu, D.N.Poenaru, A.Sandulescu On Exotic Nuclear Decay of 223Ra by Emission of 14C Nuclei RADIOACTIVITY 238U; calculated α, Ne, Mg, S, 34Si, Ar, Ca, Ti, Cr, Fe penetrability, T1/2. Even-even cluster emission, superasymmetric fission mechanism.
doi: 10.1007/BF01881286
1985MA13 J.Phys.(London) G11, L75 (1985) M.T.Magda, A.Pop, A.Sandulescu Projectile Break-Up and Cluster Emission in Heavy-Ion Reactions at Low Energy NUCLEAR REACTIONS 181Ta(22Ne, 6He), (22Ne, 3He), (22Ne, 8He), (22Ne, X), E=178 MeV; 181Ta(22Ne, X), E=141 MeV; analyzed σ(fragment θ, E) for light fragments; deduced reaction mechanism. Serber model, sequential projectile breakup.
doi: 10.1088/0305-4616/11/5/002
1985PO11 Phys.Rev. C32, 572 (1985) D.N.Poenaru, M.Ivascu, A.Sandulescu, W.Greiner Atomic Nuclei Decay Modes by Spontaneous Emission of Heavy Ions RADIOACTIVITY 222Fr, 222,223,224,226Ra(14C); 223,224Ac, 231Th, 232U(15N); 233,235U(24Ne); 233,235U(25Ne); 233U, 236Np, 236Pu(28Mg); 235U, 236Np(29Mg); 239Cm(32Si); 251Cf(46Ar); 253Fm, 254Md, 255No(48Ca); 258Md, 259No(50Ca); calculated decay T1/2, (heavy ion/α) branching ratio.
doi: 10.1103/PhysRevC.32.572
1985PO12 Rev.Roum.Phys. 30, 173 (1985) D.N.Poenaru, M.Ivascu, A.Sandulescu, W.Greiner New Natural Radioactivities by Emission of Heavy Ions RADIOACTIVITY 222Fr, 225,226Ra, 223,224,225,227Ac, 227,228,229,230,232Th, 231Pa, 232,233,234,235,238U, 236,237Np, 236,239,240,242Pu, 243Am, 239,251,252Cf; calculated heavy ion emission T1/2, branching ratio relative to α-decay.
1985PO20 Phys.Rev. C32, 2198 (1985) D.N.Poenaru, W.Greiner, M.Ivascu, A.Sandulescu Heavy Cluster Decay of Trans-Zirconium ' Stable ' Nuclides RADIOACTIVITY 150Sm(12C), (α); 151Eu, 156Dy, 181Ta, 180,182,183,184W, 184Os(α); 154Gd(16O), (α); 169Tm, 170Yb(32Si), (α); 168Yb(30Si), (α); 180Hf, 185Re(48Ca), (α); 186W(50Ca), (α); 187Os(49Ca), (α); 188Os(52Ti), (α); 189Os(53Ti), (α); 192Os(58Cr), (α); 191Ir, 192Pt(56Cr), (α); 198Pt(58Ni), (α); 197Au(62Fe), (α); 196Hg(60Fe), (α); 202Hg(68Ni), (α); calculated heavy cluster decay, Q, T1/2. Analytical superasymmetric fission model.
doi: 10.1103/PhysRevC.32.2198
1985SA02 Phys.Rev.Lett. 54, 490 (1985) A.Sandulescu, D.N.Poenaru, W.Greiner, J.H.Hamilton Comment on ' Exotic Nuclear Decay of 223Ra by Emission of 14C Nuclei ' NUCLEAR STRUCTURE 223,226Ra, 232Th, 233U, 237Np; analyzed decay by 14C, 24,25,26Ne, 30Mg emission.
doi: 10.1103/PhysRevLett.54.490
1985SA40 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2104 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 20 (1985) A.Sandulescu, Yu.S.Zamyatnin, I.A.Lebedev, B.F.Myasoedov, S.P.Tretyakova, D.Hasegan Spontaneous Decay of 231Pa with the Emission of Neon Nuclei RADIOACTIVITY 231Pa(SF), (24Ne); measured decay products distributions; deduced half life. Lavsan detector.
1984GU03 J.Phys.(London) G10, 209 (1984) R.K.Gupta, M.Munchow, A.Sandulescu, W.Scheid A Quantum-Mechanical Model of Coupled Proton and Neutron Asymmetries and the Fast Charge Equilibration Process in Deep-Inelastic Collisions NUCLEAR REACTIONS 116,124Sn(129Xe, X), E=780 MeV; calculated fragment N, Z distribution variances vs energy loss. Deep inelastic reactions, quantum mechanical model of coupled harmonic oscillators.
doi: 10.1088/0305-4616/10/2/012
1984PO08 J.Phys.(London) G10, L183 (1984) D.N.Poenaru, M.Ivascu, A.Sandulescu, W.Greiner Spontaneous Emission of Heavy Clusters RADIOACTIVITY 223,226Ra, 227Ac, 230,232Th, 232,233,234,235,238U, 237Np, 252Cf(SF); calculated cluster SF decay T1/2, (T1/2(SF)/T1/2(α)); deduced decay probability dependence on magic, near magic nature of daughter nucleus. Two-center spherical shape parametrization.
doi: 10.1088/0305-4616/10/8/004
1983SA04 Lett.Nuovo Cim. 36, 321 (1983) A.Sandulescu, R.Y.Cusson, W.Greiner Time-Dependent Hartree-Fock Study of Alpha Decay NUCLEAR REACTIONS 208Pb(α, α), E not given; calculated compound nuclear shapes during, after α-capture. TDHF.
1981HA15 J.Phys.(London) G7, 785 (1981) J.Hahn, J.A.Maruhn, A.Sandulescu, W.Greiner Collective Mass Transfer in Heavy-Ion Collisions NUCLEAR REACTIONS 120Sn(132Xe, X), E=5.9 MeV/nucleon; 166Er(86Kr, X), E=6, 8.2, 12.1 MeV/nucleon; calculated σ(fragment Z); deduced shell effects on mass transfer. Time-dependent Schrodinger equation.
doi: 10.1088/0305-4616/7/6/012
1981MA05 J.Phys.(London) G7, 359 (1981) M.T.Magda, A.Pop, D.Poenaru, A.Sandulescu, W.Greiner Synthesis of Superheavy Elements in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 206Pb(59Co, xn), E=310-340 MeV; 209Bi(56Fe, xn), E=290-325 MeV; 203Tl(62Ni, xn), E=320-355 MeV; 181Ta(84Kr, xn), E=410-455 MeV; 202Hg(63Cu, xn), E=325-355 MeV; 225Ac(48Ca, xn), E=230-250 MeV; 232Th(48Ca, xn), E=230-255 MeV; 231Pa(48Ca, xn), E=235-250 MeV; 226Ra(48Ca, xn), E=220-260 MeV; 208Pb(58Fe, xn), E=290-320 MeV; 233U(48Ca, xn), E=245-260 MeV; 240Pu(48Ca, xn), E=240-265 MeV; 238U(50Ti, xn), E=260-280 MeV; 242,244Pu(48Ca, xn), E=237.5-260 MeV; 248Cm(48Ca, xn), E=240-275 MeV; 237Np(51V, xn), E=280-300 MeV; 238Pu(50Ti, xn), E=270-290 MeV; 234U(54Cr, xn), E=290-315 MeV; 232Th(56Fe, xn), E=315-335 MeV; calculated production σ(E) for 266108, 274108, 265109, 273109, 280110, 279111, 281112, 288114, 290114, 292114, 288116, 296116. Statistical model, fusion reaction, Krappe-Nix-Sierk interaction barriers.
doi: 10.1088/0305-4616/7/3/011
1980MA01 J.Phys.(London) G6, 221 (1980) M.T.Magda, A.Sandulescu, D.G.Popescu, W.Greiner Heavy-Ion Fusion and the Production of Elements 103, 105 and 107 NUCLEAR REACTIONS 203Tl(50Ti, X), 206Pb(51V, X), 209Bi(54Cr, X), E not given; calculated production σ for 253Lr, 257105, 263107. Fragmentation theory, statistical model.
doi: 10.1088/0305-4616/6/2/012
1980PO02 Rev.Roum.Phys. 25, 55 (1980) D.N.Poenaru, M.Ivascu, D.Mazilu, A.Sandulescu On the Charge Density Asymmetry of Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 109Ag(40Ar, X), 138Ce(57Fe, X), 144Nd(61Ni, X), E not given; calculated interaction barriers, fusion Q, potential energy surfaces. Generalized liquid drop model.
1980SA36 Fiz.Elem.Chastits At.Yadra 11, 1334; Sov.J.Part.Nucl. 11, 528 (1980) A.Sandulescu, D.N.Poenaru, W.Greiner New Type of Decay of Heavy Nuclei Intermediate between Fission and α decay RADIOACTIVITY, Fission 252No(SF); calculated fission product yields; 252,254No, 248,250Cm, 250,252Cf, 254,252Fm, 244,246Pu, 238,236U(SF); calculated two-body fragmentation penetrability vs mass; deduced decay mechanism intermediate between fission, α-decay. Fragmentation theory.
1979MA23 J.Phys.(London) G5, 961 (1979) M.T.Magda, M.Duma, A.Sandulescu Cross Sections for Production of Transfermium Elements NUCLEAR REACTIONS 238U(40Ca, X), E=218-306 MeV; 238U(44Ca, X), E=274 MeV; 238U(48Ca, X), E=245 MeV; 232Th(48Ca, X), E=245-300 MeV; 208Pb(48Ca, X), E=255 MeV; calculated fusion σ, production σ for transfermium elements. 252No deduced best target projectile combination.
doi: 10.1088/0305-4616/5/7/010
1979MA40 Rev.Roum.Phys. 24, 911 (1979) Critical Angular Momentum Dependence of the Fission Barriers and the Stability of Superheavy Nuclei NUCLEAR REACTIONS 238U(40Ar, X), E=212-340 MeV; 207,208Pb(48Ca, xn), E=235 MeV; 238U(40Ca, X), (48Ca, X), E not given; 203,205Tl(50Ti, X), E=260 MeV; 209Bi(50Ti, X), 207,208Pb(51V, X), E=270 MeV; 209Bi(54Cr, X), 208Pb(55Mn, X), E=290 MeV; 248Cm(40Ar, X), E not given; 248Cm(48Ca, X), E=267 MeV; 243Am(66Zn, X), E=360-400 MeV; analyzed evaporation σ data; deduced critical L, stability against fission for superheavies.
1979PO18 J.Phys.(London) G5, L169 (1979) D.N.Poenaru, M.Ivascu, A.Sandulescu Alpha Decay as a Fission-Like Process RADIOACTIVITY Ra, Th, U, Pu, Cm, Cf, Fm, No; calculated Q, T1/2 for α-decay. Liquid drop model, two-center parametrization, folded Yukawa plus exponential potential.
doi: 10.1088/0305-4616/5/10/005
1979PO23 J.Phys.(Paris), Lett. 40, L-465 (1979) D.N.Poenaru, M.Ivascu, A.Sandulescu La Radioactivite Alpha Etudiee par les Methodes de la Fission RADIOACTIVITY, Fission 222,224,226Ra, 224,226,228,230,232Th, 226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 194,196,198,200,202,204,206,208,210,212,214,216,218Po; calculated α-decay T1/2, Q; deduced plausible SF. Liquid drop model, phenomenological shell correction.
doi: 10.1051/jphyslet:019790040018046500
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