NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = D.Delion Found 138 matches. Showing 1 to 100. [Next]2023DE26 Eur.Phys.J. A 59, 210 (2023) Alpha-clustering and related phenomena in medium and heavy nuclei NUCLEAR STRUCTURE 164Dy, 168Er, 172Yb, 176Hf, 180W, 184Os, 188Pt, 192Hg, 196Pb, 200Po, 204Rn; analyzed available data; deduced even–odd staggering in pair binding energies along α-lines in terms of the so-called isospin pairing.
doi: 10.1140/epja/s10050-023-01105-5
2023DU02 Phys.Rev. C 107, 024302 (2023) Cluster mean-field description of α emission RADIOACTIVITY 242Pu, 266Sg, 264,270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α); calculated α-decay width Hartree-Fock-Bogoliubov (HFB) method with including a residual nucleon-nucleon surface Gaussian interaction (SGI) in order to describe the α-clustering in even-even nuclei. Comparison to experimental values. NUCLEAR STRUCTURE A=150-250; analyzed experimental data on superfluid even-even α emitters ranging from rare earths to actinides and superheavy nuclei; deduced pairing strength systematics.
doi: 10.1103/PhysRevC.107.024302
2022DE06 Phys.Rev. C 105, L031301 (2022) Two-proton emission systematics RADIOACTIVITY 6Be, 8C, 10N, 12O, 19Mg, 28Cl, 32K, 45Fe, 48Ni, 52Cu, 54Zn, 57Ga, 67Kr(2p); analyzed available theoretical and experimental data on 2p-decay, Q-values, decay widths, Coulomb parameter, reduced radius, fragmentation potential; deduced correlations between decay parameters, linear correlation between the logarithm of the reduced width and pairing gap, influence of the quadrupole deformation on the decay probability.
doi: 10.1103/PhysRevC.105.L031301
2022DU04 At.Data Nucl.Data Tables 145, 101501 (2022) The phenomenology of particle and cluster emission RADIOACTIVITY 109I, 112,113Cs, 117La, 130,131Eu, 135Tb, 140,141Ho, 144,145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 165,166,167Ir, 170,171Au, 176,177Tl, 185Bi(p), 106,108Te, 110Xe, 144Nd, 146,148Sm, 148,150,152Gd, 150Dy, 154Dy, 154,156Yb, 156,158Hf, 158,160,162,164W, 162Os, 166,168,170,172Os, 186Os, 166,168,170,172,174,176,178Pt, 190Pt, 172,174,176,178,180,182,184Hg, 180Pb, 186,188Pb, 188,190,192,194,196,198,200,202Po, 206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 218U, 224,226,228,230,232,234,236,238U, 232,234,236,238,240,242,244Pu, 238,240,242,244,246,248Cm, 240,242,244,246,248,250,252Cf, 246,248,250,252,254,256Fm, 252,254,256No, 258Rf, 260Sg, 266Sg, 264,266Hs, 270Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α), 222,224,226Ra(14C), 226Th(18O), 228Th(20O), 230Th(24Ne), 230U(22Ne), 232Th(24Ne), 232Th(26Ne), 232U(24Ne), 232,234U(28Mg), 234U(24Ne), (26Ne), 236Pu(28Mg), 238Pu(30Mg), 238Pu(28Mg), 238Pu(30Mg), 240Pu, 242Cm(34Si); analyzed available data; calculated T1/2; deduced impact of centrifugal and deformation effects within the Froman approach.
doi: 10.1016/j.adt.2022.101501
2022GH06 Phys.Rev. C 106, 034602 (2022) Semimicroscopic model of two-proton emission RADIOACTIVITY 19Mg, 45Fe, 54Zn(2p); calculated potential matrix as function of the hyper-radius, Sommerfeld parameters as function of the hyper-radius, wave function components, decay widths as functions of proton-proton interaction strength, hyper-sphere radius and Q values, partial decay widths. Semimicroscopic model in hyperspherical coordinates for the two-proton emission process, with assumed emission of protons from a paired state, and between the ground states of the parent and daughter nuclei. Relevance to investigation of proton-proton potential inside the nuclear medium as well as far away from it.
doi: 10.1103/PhysRevC.106.034602
2021DE12 Phys.Rev. C 103, 054325 (2021) Universal proton emission systematics RADIOACTIVITY 109I, 112,113Cs, 117La, 130,131Eu, 135Tb, 140,141,141m,144,145,145m,146,146m,147,147mHo, 150,150m,151,151mLu, 155,156,156m,157Ta, 159,160,161,161mRe, 164,165,166,166m,167,167mIr, 170,170m,171,171mAu, 176,177,177mTl, 185Bi; compiled experimental data for J, π, l-transfers, Q values, T1/2, β2 and β4 deformation parameters; analyzed proton systematics in terms of the barrier penetration and formation probability by approximating the realistic proton-core interaction by a parabolic dependence describing the nuclear part, and analytic WKB solutions for the wave functions in the regions of nuclear and Coulomb barriers; deduced nuclear centrifugal and deformation terms as much smaller than the corresponding Coulomb terms, and the Coulomb action one order of magnitude larger than the nuclear action term.
doi: 10.1103/PhysRevC.103.054325
2021GH08 J.Phys.(London) G48, 105108 (2021) Semiclassical propagator approach for emission processes from deformed nuclei NUCLEAR STRUCTURE 234Th, 238U; calculated realistic alpha-daughter double-folding potential radius, wave functions; deduced α-decay systematics and fine structure, deformation and spectroscopic factors.
doi: 10.1088/1361-6471/ac22f5
2020BA57 Phys.Rev. C 102, 061301 (2020) V.V.Baran, D.R.Nichita, D.Negrea, D.S.Delion, N.Sandulescu, P.Schuck Bridging the quartet and pair pictures of isovector proton-neutron pairing
doi: 10.1103/PhysRevC.102.061301
2020DE25 Phys.Rev. C 102, 014327 (2020) Realistic analytical approach for α decay and clustering RADIOACTIVITY Z=50-82, N=50-82(α); Z=50-82, N=82-126(α); Z=82-100, N=82-126(α); Z=82-100, N>126(α); Z>100, N>126(α); calculated radial parameters versus mass number, Coulomb parameters and fragmentation potentials versus neutron number, reduced widths versus number of α clusters, harmonic oscillator frequencies and length parameters versus mass number, lowest quartet number versus magic asymmetry for even-even and odd-A α emitters. Double folding procedure with parabolic dependence to derive the realistic α-core nuclear interaction between the inner turning point and the Coulomb barrier, and by including in the analysis α-decay experimental data for Q values and widths for 149 even-even α emitters.
doi: 10.1103/PhysRevC.102.014327
2020GH03 Phys.Rev. C 101, 044304 (2020) Coupled-channels analysis of the α decay in strong electromagnetic fields RADIOACTIVITY 212Po(α); calculated radial components of the Fourier transform, quadrupole deformation of the nuclear barrier, angular distributions of emitted particles and decay widths, α-clustering under the influence of monochromatic strong laser electromagnetic field. Coupled-channel formalism, by analyzing the Fourier components of the time-dependent α-core realistic potential in the Henneberger representation.
doi: 10.1103/PhysRevC.101.044304
2020PE13 Phys.Rev. C 102, 044317 (2020) P.Petkov, D.-S.Delion, C.Muller-Gatermann Collectivity of the 2+1 state in Z ≤ 82 even-even nuclei probed by a ratio involving dynamic and static electromagnetic E2 moments: Evolution of the quadrupole degrees of freedom and a new signature for shape coexistence NUCLEAR STRUCTURE 16O, 20,22Ne, 24,26Mg, 28Si, 32S, 42Ca, 46,48Ti, 50,52,54Cr, 56,58Fe, 60Ni, 70Zn, 72,74,76Ge, 74,76,78,80,82Se, 96,98,100Mo, 98,100,102,104Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116Sn, 122,124,126,128,130Te, 134,136,138,142Ba, 144,146,148,150Nd, 148,150,152,154Sm, 154,156,158,160Gd, 164Dy, 166,170Er, 170,172,174,176Yb, 176,178,180Hf, 180,182,184,186W, 184,186,188,190,182Os, 192,194,196,198Pt, 198,200,202Hg, 204Pb; analyzed ratios of experimental and deduced B(E2) values for the first 2+ states in even-even nuclei, the latter from experimental static quadrupole moments for the first 2+ states; deduced collective excitations and sensitivity to shell- and subshell closures, and a new signature for shape coexistence.
doi: 10.1103/PhysRevC.102.044317
2019BA12 Phys.Rev. C 99, 031303 (2019) Analytical approach for the quartet condensation model
doi: 10.1103/PhysRevC.99.031303
2019BA29 Phys.Rev. C 99, 064311 (2019) Unified description of pairing and quarteting correlations within the particle-hole-boson approach NUCLEAR STRUCTURE 104Te, 108Xe, 112Ba, 116Ce; calculated average level occupation fractions, and correlation energies corresponding to the exact quartet condensation model (QCM) and to the renormalized bosonic quartet condensation model (rbQCM) for nuclei above the 100Sn core. Projected BCS and the quartet condensation model, with new bosonic approximation for pair and quartet condensates, corresponding to the standard pairing and isovector pairing scenarios.
doi: 10.1103/PhysRevC.99.064311
2019BA38 Phys.Rev. C 100, 034326 (2019) V.V.Baran, D.S.Delion, S.Dolteanu Disentangling the pair and quartet condensates NUCLEAR STRUCTURE 110Te, 112Xe, 118Ba; calculated average neutron and proton level occupations using Bonn A isovector pairing interaction within the QCM and ADC approaches. 108,110,116Te, 112,114Xe, 118Ba, 130Sm; calculated correlation energies, quartet-pair correlation energies with the Bonn interaction. 48,50,56Ti, 52Cr, 58Fe, 70Ge; calculated correlation energies, quartet-pair correlation energies with the KB3G interaction. 108Xe, 112Ba, 116Ce, 120Nd, 124Sm; calculated correlation energies for N=Z systems. Quartet condensate model (QCM) and analytical disentangled condensate model (ADC) model.
doi: 10.1103/PhysRevC.100.034326
2019DE23 Phys.Rev. C 100, 024331 (2019) D.S.Delion, A.Dumitrescu, J.Suhonen Effective axial-vector strength within proton-neutron deformed quasiparticle random-phase approximation NUCLEAR STRUCTURE N=10-200; A=20-200; 78Ge; analyzed experimental data for Gamow-Teller β transition strengths versus neutron number, ratios of transition amplitudes β-/β-(Fermi) and β+/β+(Fermi) versus mass number, and half-lives of 2β emitters; deduced effective axial-vector strength versus the particle-particle strength in 78Ge, and versus mass number in even-even and odd-odd A=20-200 emitters for β- and β+ transitions using pn-QRPA equations of motion, with projected angular momentum, and a schematic quadrupole-quadrupole residual interaction.
doi: 10.1103/PhysRevC.100.024331
2018BA05 J.Phys.(London) G45, 035106 (2018) Alpha-like resonances in nuclei NUCLEAR STRUCTURE 100Sn; calculated energy weighted sum rule (EWSR), dipole oscillations in a system of protons, neutrons and α-particles within the Brink approach.
doi: 10.1088/1361-6471/aa98c7
2018DE15 J.Phys.(London) G45, 053001 (2018) D.S.Delion, Z.Ren, A.Dumitrescu, D.Ni Coupled channels description of the α-decay fine structure RADIOACTIVITY 246Cf, 242Cm, 253Fm, 251Cf(α); calculated branching ratios, J, π, deformation parameters. Comparison with available data.
doi: 10.1088/1361-6471/aaac52
2018DE21 Phys.Rev. C 97, 064303 (2018) D.S.Delion, A.Dumitrescu, V.V.Baran Theoretical investigation of α-like quasimolecules in heavy nuclei NUCLEAR STRUCTURE 144Nd; calculated vibrational resonant states and rotational bands built on them in the α+140Ce molecular potential. Z>50, N=50-155; calculated monopole length parameter of g.s. channel, spectroscopic factors and absorption energy-integrated cross section of 162 even-even α emitters. Discussed experimental methods for determining α-like quasimolecular structure in heavy nuclei.
doi: 10.1103/PhysRevC.97.064303
2017DE09 Phys.Rev. C 95, 034330 (2017) Two-neutrino ββ decays and low-lying Gamow-Teller β- strength functions in the mass range A=70-176 RADIOACTIVITY 70Zn, 76Ge, 80,82Se, 86Kr, 94,96Zr, 100Mo, 104Ru, 110Pd, 128,130Te, 134,136Xe, 142Ce, 148,150Nd, 154Sm, 160Gd, 176Yb(2β-); calculated 2νββ decay half-lives, and Gamow-Teller strengths up to 6 MeV excitation energy summed in bins of 0.5 MeV. Comparison with available experimental data and other theoretical calculations. Proton-neutron deformed quasiparticle random-phase approximation (pn-dQRPA) calculations.
doi: 10.1103/PhysRevC.95.034330
2017DE33 Phys.Rev.Lett. 119, 202501 (2017) Geiger-Nuttall Law for Nuclei in Strong Electromagnetic Fields NUCLEAR STRUCTURE 232Pu; calculated logarithm of penetrability for various quadrupole deformations.
doi: 10.1103/PhysRevLett.119.202501
2016BA45 Phys.Rev. C 94, 034319 (2016) Proton-neutron versus α-like correlations above 100Sn NUCLEAR STRUCTURE Z=52, N=52; Z=54, N=54; Z=56, N=56; Z=58, N=58; calculated neutron densities by BCS calculations and by diagonalization, α-formation amplitude in the pn-BCS approach. Z=52, 54, 88; calculated strength of α-clustering additional part of the mean-field potential versus the reduced width. Discussed α-like dipole pigmy resonance in the region above 100Sn.
doi: 10.1103/PhysRevC.94.034319
2016DE11 Phys.Rev. C 93, 044321 (2016) D.S.Delion, A.Dumitrescu, V.V.Baran Even-odd staggering of the spectroscopic factor as new evidence for α clustering NUCLEAR STRUCTURE N=80-160, Z=70-100; calculated α spectroscopic factors for even Z nuclides of Ra, Th, U, Pu, Cm, Cf and Fm, and odd Z nuclides of Au, Bi, At, Fr, Ac, Pa, ratios between experimental and BCS spectroscopic factors, QQ coupling strength versus reduced width; deduced even-odd staggering in α spectroscopic factors, α clustering. Standard Bardeen-Cooper-Schrieffer (BCS) approach.
doi: 10.1103/PhysRevC.93.044321
2016DE19 J.Phys.(London) G43, 095109 (2016) D.S.Delion, M.Patial, R.J.Liotta, R.Wyss A simple approach to α-decay fine structure NUCLEAR STRUCTURE N=80-170; calculated hindrance and spectroscopic factors, partial α-decay widths. Standard spherical semiclassical approach where the action integrals have close analytical forms.
doi: 10.1088/0954-3899/43/9/095109
2016DU03 Phys.Rev. C 93, 024313 (2016) Description of electromagnetic and favored α transitions in heavy odd-mass nuclei NUCLEAR STRUCTURE 225Ra, 223,225Ac, 229,231Th, 231,233Pa, 237U, 235,237,239Np, 239,241Pu, 241,243,245Am, 243,245,249Cm, 241,247,249,251Bk, 247,251,253Cf; calculated levels, J, π, bands, B(E2) using particle coupled to coherent state core model. Comparison with experimental values. RADIOACTIVITY 225Ra, 223,225Ac, 229,231Th, 231,233Pa, 237U, 235,237,239Np, 239,241Pu, 241,243,245Am, 243,245,249Cm, 241,247,249,251Bk, 247,251,253Cf(α); calculated half-lives and fine structure of favored α-transitions to first three members of rotational bands using coupled channels method and QQ interaction. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.024313
2015BA22 Rom.J.Phys. 60, 722 (2015) Pairing Coherence Length in Nuclei NUCLEAR STRUCTURE 52Fe, 48Cr, 220Ra; calculated paring gap versus sp energy, proton coherence length. HF+BCS formalism.
2015DE02 Phys.Rev. C 91, 024312 (2015) Pairing versus quarteting coherence length NUCLEAR STRUCTURE 48Cr, 220Ra; calculated pairing, and quartet coherence lengths between proton and neutron pairs in the spin-singlet channel using effective density-dependent delta (DDD) and Gaussian interactions, by considering bound states and narrow resonances. Evidence for the role of proton-neutron correlations by estimating α coherence length.
doi: 10.1103/PhysRevC.91.024312
2015DE15 Phys.Rev. C 91, 054329 (2015) Double-β decay within a consistent deformed approach RADIOACTIVITY 150Nd(2β-); calculated B(GT) strength versus excitation energy in the intermediate nucleus 150Pm, Gamow-Teller 2νββ matrix element. 82Se, 96Zr, 100Mo, 128,130Te, 150Nd, 238U(2β-); calculated half-lives. Calculations based on proton-neutron deformed quasiparticle random-phase approximation (pn-dQRPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.91.054329
2015DE25 Phys.Rev. C 92, 021303 (2015) Systematics of α-decay transitions to excited states
doi: 10.1103/PhysRevC.92.021303
2015DE27 Rom.J.Phys. 60, 993 (2015) Systematics of the Pairing Coherence Length NUCLEAR STRUCTURE 48Cr; analyzed available data; calculated resonance energies and widths, pairing gap, proton coherence length, strength parameters. Comparison with available data.
2015DE35 Phys.Rev. C 92, 051301 (2015) D.S.Delion, R.J.Liotta, R.Wyss Exact estimate of the α-decay rate and semiclassical approach in deformed nuclei RADIOACTIVITY 230U, 236Pu, 244Cm(α); calculated fragmentation potential, partial decay widths and total half-life in the laboratory system and from "angular momentum WKB" approach. New semiclassical "angular momentum WKB" procedure to evaluate the total α-decay widths in deformed nuclei.
doi: 10.1103/PhysRevC.92.051301
2015DU08 Rom.J.Phys. 60, 767 (2015) Coherent State Description of the α-Emission Spectrum
2014DE29 Europhys.Lett. 107, 52001 (2014) Effective axial-vector strength and β-decay systematics RADIOACTIVITY 70Ga, 78Br, 100Tc, 104Rh, 106,110Ag, 116In, 128I, 130Cs(β-), (EC); calculated Gamow-Teller decay rates, matrix elements, T1/2. Proton-neutron quasiparticle random-phase approximation (pnQRPA), comparison with experimental data.
doi: 10.1209/0295-5075/107/52001
2014DE43 At.Data Nucl.Data Tables 101, 1 (2014) Systematics of the α-decay fine structure in even-even nuclei RADIOACTIVITY 154Er, 156,158Yb, 158,160,162,164Hf, 164,166,168,170W, 164,166,168,170,172,174,176,178,180,182Os, 168,170,172,174,176,178,180,182,184Pt, 176,178,180,182,184,186,188,190Hg, 206,208Pb, 214Pb, 192,194,196,198,200Po, 202Po, 208Po, 198,200Rn, 206Rn, 216,218,220,222Rn, 208Ra, 218,220,222,224,226,228Ra, 220,222,224,226,228,230,232,234Th, 226,228,230,232,234,236,238,240U, 234,236,238,240,242,244Pu, 236,238,240,242,244,246,248Cm, 242,244,246,248,250,252Cf, 248,250,252Fm, 252,254No, 256Rf, 262Rf, 260,262Sg, 266Sg, 266Hs, 280Ds, 284Cn, 288Fl, 290Lv(α);calculated energy levels, J, π, deformation parameters, B(E2), T1/2. Comparison with available data, Coherent State Model (CSM).
doi: 10.1016/j.adt.2014.09.001
2014DE48 Phys.Rev. C 90, 061303 (2014) D.S.Delion, R.J.Liotta, C.Qi, R.Wyss Probing shape coexistence by α decays to 0+ states RADIOACTIVITY 180,182,184Hg, 202Rn(α); analyzed fine structure of α decays to first excited 0+ states, hindrance factors, spectroscopic factors. Shape coexistence. Two-level model using microscopic description of the α-particle formation amplitude.
doi: 10.1103/PhysRevC.90.061303
2013DE05 Phys.Rev. C 87, 024309 (2013) Unified description of 21+ states within the deformed quasiparticle random-phase approximation NUCLEAR STRUCTURE 130Te, 240Pu; calculated energy-weighted strength functions S(E) for spherical and vibrational nucleus. Z=50-100; calculated B(E2) for first 2+ states, 2+ level energies. deformed quasiparticle random phase approximation (dQRPA) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.024309
2013DE08 Phys.Rev. C 87, 034328 (2013) D.S.Delion, R.J.Liotta, R.Wyss Simple approach to two-proton emission RADIOACTIVITY 45Fe, 48Ni(2p); calculated two-proton radial wave function, proton pairing gap, two-proton decay width, T1/2. Scattering theory with a realistic proton-proton interaction, BCS equations.
doi: 10.1103/PhysRevC.87.034328
2013DE11 Phys.Rev. C 87, 041302 (2013) Shell-model representation to describe α emission RADIOACTIVITY Z<82, N=82-126(α); Z>82, N=82-126(α); Z>82, N>126(α); calculated proton clustering strength, reduced α widths, Qα-Coulomb barrier for even-even nuclei. 220Rn(α); calculated proton and neutron pairing formation probabilities, decay width and compared with experimental data. Woods-Saxon mean field plus spin-orbit potential of shell model, with an additional attractive Gaussian pocket potential.
doi: 10.1103/PhysRevC.87.041302
2013DE12 Phys.Rev. C 87, 044314 (2013) Unified description of electromagnetic and α transitions in even-even nuclei RADIOACTIVITY 172,174Os, 176,178,180Pt, 196,198,216,218Po, 216,218,220,222Rn, 218,220,222,224Ra, 222,224,226,228,230,232,234Th, 230,232,234,236,238U, 236,238,240,242,244Pu, 242,244,246,248Cm, 248,250Cf(α); calculated β2 and d deformation parameters, CSM parameter A1, α-core QQ coupling parameter C, Iα to 2+, 4+ and 6+ states in daughter nuclei, rigidity parameter, E4/E2 and E6/E4 ratios, effective charge, hindrance factors using the coherent state model (CSM). Comparison with experimental data.
doi: 10.1103/PhysRevC.87.044314
2013DE35 Rom.J.Phys. 58, 1167 (2013) Coherent State Description of α-Transitions to Excited States in Even-Even Nuclei NUCLEAR STRUCTURE N=126; calculated alpha-branching ratios to 2+ states, deformation parameters. Coherent state model.
2013IX01 Rom.J.Phys. 58, 1396 (2013) Two-Proton Emission: A Numerical Approach
2013JE05 Phys.Rev. C 88, 044004 (2013) Self-consistent random-phase approximation from a coupled-cluster wave function perspective
doi: 10.1103/PhysRevC.88.044004
2013MA66 Phys.Rev. C 88, 044301 (2013) P.J.R.Mason, Zs.Podolyak, N.Marginean, P.H.Regan, P.D.Stevenson, V.Werner, T.Alexander, A.Algora, T.Alharbi, M.Bowry, R.Britton, A.M.Bruce, D.Bucurescu, M.Bunce, G.Cata-Danil, I.Cata-Danil, N.Cooper, D.Deleanu, D.Delion, D.Filipescu, W.Gelletly, D.Ghita, I.Gheorghe, T.Glodariu, G.Ilie, D.Ivanova, S.Kisyov, S.Lalkovski, R.Lica, S.N.Liddick, R.Marginean, C.Mihai, K.Mulholland, C.R.Nita, A.Negret, S.Pascu, S.Rice, O.J.Roberts, T.Sava, J.F.Smith, P.-A.Soderstrom, L.Stroe, G.Suliman, R.Suvaila, S.Toma, C.Townsley, E.Wilson, R.T.Wood, M.Zhekova, C.Zhou Half-life of the yrast 2+ state in 188W: Evolution of deformation and collectivity in neutron-rich tungsten isotopes NUCLEAR REACTIONS 186W(7Li, pα), E=35 MeV; measured Eγ, γγ-coin, T1/2 of first 2+ state by γγ(t) at IFIN-HH, Bucharest facility. 188W; deduced level, B(E2) for first 2+ state, enhanced γ softness in 188W. Systematics of energies of low-lying 0+, 2+ and 4+ states and B(E2) values for first 2+ states in even-even Hf, W, Os and Pt nuclei with N=102-120. NUCLEAR STRUCTURE 184,186,188,190,192,194W; calculated Woods-Saxon potential energy surface (PES) contours in (β, γ) plane; deduced prolate to oblate shape transition.
doi: 10.1103/PhysRevC.88.044301
2013MA74 Phys.Rev. C 88, 044301 (2013) P.J.R.Mason, Zs.Podolyak, N.Marginean, P.H.Regan, P.D.Stevenson, V.Werner, T.Alexander, A.Algora, T.Alharbi, M.Bowry, R.Britton, A.M.Bruce, D.Bucurescu, M.Bunce, G.Cata-Danil, I.Cata-Danil, N.Cooper, D.Deleanu, D.Delion, D.Filipescu, W.Gelletly, D.Ghita, I.Gheorghe, T.Glodariu, G.Ilie, D.Ivanova, S.Kisyov, S.Lalkovski, R.Lica, S.N.Liddick, R.Marginean, C.Mihai, K.Mulholland, C.R.Nita, A.Negret, S.Pascu, S.Rice, O.J.Roberts, T.Sava, J.F.Smith, P.-A.Soderstrom, L.Stroe, G.Suliman, R.Suvaila, S.Toma, C.Townsley, E.Wilson, R.T.Wood, M.Zhekova, C.Zhou Half-life of the yrast 2+ state in 188W: Evolution of deformation and collectivity in neutron-rich tungsten isotopes
doi: 10.1103/PhysRevC.88.044301
2013RO07 Acta Phys.Pol. B44, 403 (2013) O.J.Roberts, A.M.Bruce, F.Browne, N.Marginean, T.Alexander, T.Alharbi, D.Bucurescu, D.Deleanu, D.Delion, D.Filipescu, L.Fraile, I.Gheorghe, D.Ghita, T.Glodariu, D.Ivanova, S.Kisyov, R.Marginean, P.J.R.Mason, C.Mihai, K.Mulholland, A.Negret, C.Nita, B.Olaizola, S.Pascu, P.-A.Soderstrom, P.H.Regan, T.Sava, L.Stroe, S.Toma, C.Townsley Half-life Measurements of Excited States in 132Te, 134Xe NUCLEAR REACTIONS 130Te(7Li, X)132Te/134Xe, E=31.5 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced energy levels, J, π, B(E2). Comparison with systematics.
doi: 10.5506/APhysPolB.44.403
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
2012DE04 Rom.J.Phys. 57, 149 (2012) Decay Theory Beyond the Gamow Picture RADIOACTIVITY 210,212Po(α); calculated B(E2), α formation probability, reduced widths.
2012DE10 Phys.Rev. C 85, 064306 (2012) D.S.Delion, R.J.Liotta, P.Schuck, A.Astier, M.-G.Porquet Shell model plus cluster description of negative parity states in 212Po NUCLEAR STRUCTURE 212Po; calculated negative-parity levels, J, π, B(E1), B(E2), octupole TDA amplitudes, α-decay widths. 208,210Pb, 210Po; calculated interaction energies, B(E2). Shell-model with α cluster approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.064306
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
2012QI03 Phys.Rev. C 85, 011303 (2012) C.Qi, D.S.Delion, R.J.Liotta, R.Wyss Effects of formation properties in one-proton radioactivity RADIOACTIVITY 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141,141mHo, 144,145,146,146m,147,147mTm, 150,150m,151,151mLu, 155,156,156m,157Ta, 159m,160,161,161mRe, 164,165m,166,166m,167,167mIr, 170,170m,171,171mAu, 176,177,177mTl, 185Bi(p); calculated T1/2, proton formation probabilities. Fitting parameter from microscopic description of the decay process. Deformation property of the parent nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.011303
2011AS06 Int.J.Mod.Phys. E20, 785 (2011) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Pure α-208Pb states in 212Po revealed by their enhanced E1 decays, A novel α clustering NUCLEAR REACTIONS 208Pb(18O, 14C)212Po, E=85 MeV; measured reaction products, Eγ, Iγ, γ-γ-γ-coin.; deduced energies, states, J, π, yrast states, B(E1), α-208Pb states.
doi: 10.1142/S0218301311018678
2011AS09 J.Phys.:Conf.Ser. 312, 092014 (2011) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck A novel manifestation of α clustering in 212Po: Pure α-208Pb states revealed by their enhanced E1 decays NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured Eγ, Iγ(θ), γγ-coin using Eurobal array of Ge crystals. 212Po deduced γ yrast transitions angular distribution, T1/2 using Doppler shift, B(E1), α-core.
doi: 10.1088/1742-6596/312/9/092014
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
2010AS01 Phys.Rev.Lett. 104, 042701 (2010) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Novel Manifestation of α-Clustering Structures: New "α+ 208Pb" States in 212Po Revealed by Their Enhanced E1 Decays NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured Eγ, Iγ; deduced 212Po level scheme, yrast state, lifetimes, B(E1). Doppler-shift attenuation method.
doi: 10.1103/PhysRevLett.104.042701
2010AS03 Eur.Phys.J. A 46, 165 (2010) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Coexistence of "a + 208Pb" cluster structures and single-particle excitations in 21284Po128 NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin. 212Po; deduced level scheme, transition energies, γ-ray intensities, J, π, angular-distribution coefficients, internal conversion coefficients, yrast states, lifetimes, B(E1), B(E2), B(E3). EUROBALL project, DSAM method, comparison with low-lying cluster structure models. RADIOACTIVITY 212Po(α); measured decay products, Eγ, Iγ, alpha spectrum; deduced branching ratios, partial T1/2 for yrast states.
doi: 10.1140/epja/i2010-11053-6
2010DE27 Phys.Rev. C 82, 024307 (2010) D.S.Delion, R.Wyss, R.J.Liotta, B.Cederwall, A.Johnson, M.Sandzelius Investigations of proton-neutron correlations close to the drip line NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116,118,120,122,124,126Sn, 106,108,110,112,114,116,118,120,122,124,126,128Te, 108,110,112,114,116,118,120,122,124,126,128,130Xe, 210,212,214Pb, 210,212,214,216,218Po, 212,214,216,218,220,222Rn, 214,216,218,220,222,224,226Ra; calculated lowest QRPA 2+ eigenvalues, B(E2), proton-neutron coupling strength, proton-neutron pairing gap, proton pairing gap, and neutron pairing gap using proton-neutron pairing plus quadrupole Hamiltonian approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.024307
2010DE33 Phys.Rev. C 82, 031302 (2010) Systematics of 2+1 states in semimagic nuclei NUCLEAR STRUCTURE Z=28, 50, 82; N=28, 50, 82, 126; calculated energies and B(E2) for the first 2+ states in even-even semi-magic nuclei using two-level pairing plus quadrupole Hamiltonian, within the spherical quasiparticle random phase approximation (QRPA).
doi: 10.1103/PhysRevC.82.031302
2010KO01 J.Phys.(London) G37, 015101 (2010) J.Kotila, J.Suhonen, D.S.Delion Description of the two-neutrino ββ decay of 100Mo by pnMAVA NUCLEAR STRUCTURE 100Mo; calculated Gamow-Teller strength functions, nuclear matrix elements for two-neutrino 2β-decay, T1/2. Microscopic anharmonic vibrator approach (MAVA), comparison with available data.
doi: 10.1088/0954-3899/37/1/015101
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.
2009DE24 Rom.J.Phys. 54, 587 (2009) Reduced Width in Cluster Emission Processes
2009DE26 Phys.Rev. C 80, 024310 (2009) Universal decay rule for reduced widths RADIOACTIVITY Z<82, N=50-126(α); Z>82, N>82(α); Z>68(p)(2p); Z<68(p), (2p); calculated half-lives, reduced widths and hindrance factors for α decays of even-even nuclides, cluster decay, proton, and di-proton emissions using shifted harmonic oscillator plus Coulomb cluster-daughter interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024310
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
2008DE34 Rom.J.Phys. 53, 1089 (2008) α-clustering in Nuclei
2008DE37 Int.J.Mod.Phys. E17, 2283 (2008) Alpha-decay versus alpha-clustering
doi: 10.1142/S0218301308011483
2008PE25 Phys.Rev. C 78, 034608 (2008) S.Peltonen, D.S.Delion, J.Suhonen α-decay spectroscopy of deformed nuclei reexamined NUCLEAR STRUCTURE Z=74-104, A=168-256; calculated α-decay half-lives, hindrance factors, spectroscopic factors for deformed even-even nuclei.
doi: 10.1103/PhysRevC.78.034608
2007DE01 Nucl.Phys. A781, 88 (2007) Microscopic anharmonic vibrator approach for beta decays RADIOACTIVITY 106,108Ag(β+); 106,108Rh(β-); calculated matrix elements for β transitions to one- and two-phonon states. Microscopic anharmonic vibrator approach.
doi: 10.1016/j.nuclphysa.2006.10.079
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.
2007DE53 Phys.Rev. C 76, 044301 (2007) D.S.Delion, R.J.Liotta, R.Wyss α decay of high-spin isomers in superheavy nuclei RADIOACTIVITY 250,252,254,256,258Fm, 252,254,256,258,260No, 258,260,262,264,266,268,270,272Rf, 258,260,262,264,266,268,270,272Sg, 262,264,266,268,270,272Hs, 264,266,268,270,272,274Ds, 280,282,284,286,288Cn, 282,284,286,288,290Fl, 284,286,288,290,292Lv, 286,288,290,292,294Og, 288,290,292,294,296120(α); calculated α-decay hindrance factors, deformation parameters, spectroscopic factors for low- and high-spin states.
doi: 10.1103/PhysRevC.76.044301
2007DE57 Rom.J.Phys. 52, 771 (2007) Acad. Aureliu Sandulescu's Contribution to Physics: from Magic Radioactivity to Superheavy Nuclei
2007PE12 Phys.Rev. C 75, 054301 (2007) S.Peltonen, D.S.Delion, J.Suhonen Folding description of the fine structure of α decay to 2+ vibrational and transitional states NUCLEAR STRUCTURE A=166-222; calculated fine structure, hindrance and spectroscopic factors for α-decay to ground and 2+ vibrational states in even-even nuclei using a coupled channel formalism.
doi: 10.1103/PhysRevC.75.054301
2006DE04 Phys.Rep. 424, 113 (2006) D.S.Delion, R.J.Liotta, R.Wyss Theories of proton emission
doi: 10.1016/j.physrep.2005.11.001
2006DE05 Phys.Rev. C 73, 014315 (2006) D.S.Delion, S.Peltonen, J.Suhonen Systematics of the α-decay to rotational states RADIOACTIVITY 226,228,230,232,234Th, 230,232,234,236,238U, 236,238,240,242,244Pu, 242,244,246,248Cm, 248,250Cf(α); analyzed T1/2, decay widths for α-decay to rotational states; deduced parameters. Stationary coupled channels approach.
doi: 10.1103/PhysRevC.73.014315
2006DE07 Phys.Rev.Lett. 96, 072501 (2006) D.S.Delion, R.J.Liotta, R.Wyss Systematics of Proton Emission RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 160,161Re, 164,165,167Ir, 171Au, 177Tl, 185Bi(p); analyzed proton decay T1/2, Q; deduced systematic trends.
doi: 10.1103/PhysRevLett.96.072501
2006KO01 Nucl.Phys. A765, 354 (2006) J.Kotila, J.Suhonen, D.S.Delion Study of the low-lying collective states in 94-100Mo isotopes using the MAVA NUCLEAR STRUCTURE 94,96,98,100Mo; calculated two-phonon states energies, configurations, transitions B(E2). Microscopic anharmonic vibrator approach, comparison with data.
doi: 10.1016/j.nuclphysa.2005.11.009
2006KO21 Czech.J.Phys. 56, 473 (2006) J.Kotila, J.Suhonen, D.S.Delion Study of low-lying collective states using a Microscopic Anharmonic Vibrator Approach NUCLEAR STRUCTURE 98,100,102,104,106Ru; calculated two-phonon states energies, B(E2) ratios. Microscopic anharmonic vibrator approach.
doi: 10.1007/s10582-006-0111-9
2005DE61 Phys.Rev. C 72, 064305 (2005) D.S.Delion, P.Schuck, J.Dukelsky Self-consistent random phase approximation and the restoration of symmetries within the three-level Lipkin model
doi: 10.1103/PhysRevC.72.064305
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.
2005PE08 Phys.Rev. C 71, 044315 (2005) S.Peltonen, D.S.Delion, J.Suhonen Systematics of the α decay to vibrational 2+ states RADIOACTIVITY 144Nd, 146,148Sm, 148,150Gd, 150Dy, 152,154Er, 154,156,158Yb, 156,158,160,162Hf, 162,164,166W, 166,168,170,172Os, 172,174,176Pt, 194,196,200,202,204,206,212,214,216,218Po, 202,204,206,208,214,216,218,220Rn, 208,210,216,218Ra, 218,220Th(α); calculated hindrance factors for decay to 2+ states, daughter nucleus transition B(E2). Quasiparticle RPA, comparisons with data.
doi: 10.1103/PhysRevC.71.044315
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
2004DE54 Phys.Rev. C 70, 061301 (2004) D.S.Delion, R.Wyss, D.Karlgren, R.J.Liotta Proton emission from triaxial nuclei RADIOACTIVITY 161Re, 185Bi(p); calculated proton emission T1/2, angular distribution, sensitivity to triaxial deformation.
doi: 10.1103/PhysRevC.70.061301
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
2003DE08 Phys.Rev. C 67, 034301 (2003) Microscopic description of low-lying two-phonon states: Electromagnetic transitions NUCLEAR STRUCTURE 106,108Pd; calculated multiphonon states energies, J, π, B(E2). Quasiparticle RPA, comparison with data.
doi: 10.1103/PhysRevC.67.034301
2003DE17 Phys.Rev. C 67, 054317 (2003) D.S.Delion, A.Insolia, R.J.Liotta Anisotropic α decay in Am, Es, and Fm isotopes RADIOACTIVITY 241,243Am, 253,255Es, 255,257Fm(α); calculated α-decay anisotropy. Microscopic approach.
doi: 10.1103/PhysRevC.67.054317
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
2003DE35 Phys.Rev. C 68, 054603 (2003) D.S.Delion, R.J.Liotta, R.Wyss High-spin proton emitters in odd-odd nuclei and shape changes RADIOACTIVITY 58Cu(p); calculated T1/2; deduced hindrance due to change in deformation, other structure effects.
doi: 10.1103/PhysRevC.68.054603
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
2003KO36 Phys.Rev. C 68, 014307 (2003) J.Kotila, J.Suhonen, D.S.Delion Microscopic calculation of the electric decay properties of low-energy vibrational states in even 110-120Cd isotopes NUCLEAR STRUCTURE 110,112,114,116,118,120Cd; calculated two-phonon states energies, configurations, transitions B(E2). Microscopic formalism, comparison with data.
doi: 10.1103/PhysRevC.68.014307
2003KO70 Phys.Rev. C 68, 054322 (2003) J.Kotila, J.Suhonen, D.S.Delion Low-lying collective states in 98-106Ru isotopes studied using a microscopic anharmonic vibrator approach NUCLEAR STRUCTURE 98,100,102,104,106Ru; calculated levels, J, π, collective states features. Microscopic anharmonic vibrator approach, comparisons with data.
doi: 10.1103/PhysRevC.68.054322
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.
2002DE23 Yad.Fiz. 65, 653 (2002); Phys.Atomic Nuclei 65, 621 (2002) Influence of a Continuum on Cluster-Decay Processes NUCLEAR STRUCTURE 212Po; calculated α-like levels, J, π, continuum effects in α-decay. Microscopic approach.
doi: 10.1134/1.1471262
2002DE24 Yad.Fiz. 65, 685 (2002); Phys.Atomic Nuclei 65, 653 (2002) D.S.Delion, A.Insolia, R.J.Liotta Anisotropic α Decay RADIOACTIVITY 241Am, 199,201,203,205,207,209,211,217At, 221Fr, 227,229Pa(α); calculated α-decay anisotropy, deformation effects. Microscopic approach.
doi: 10.1134/1.1471268
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
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
2001DE21 Phys.Rev. C63, 061306 (2001) Microscopic Description of α + 40Ca Quasimolecular Resonances NUCLEAR STRUCTURE 44Ti; calculated α-like resonance features. Multistep microscopic approach, comparison with data.
doi: 10.1103/PhysRevC.63.061306
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
2001DE47 Phys.Rev. C64, 064302 (2001) Microscopic Description of the α-Decay Fine Structure in Spherical Nuclei RADIOACTIVITY 198,200,202,204Rn(α); calculated hindrance factors. Microscopic approach, quasiparticle RPA.
doi: 10.1103/PhysRevC.64.064302
2000DE04 Phys.Rev. C61, 024304 (2000) Microscopic Description of α-like Resonances NUCLEAR STRUCTURE 210Po, 210Pb, 210Bi; calculated two-particle states excitation energies, configurations. 212Po; calculated α-like resonances energy, J, π.
doi: 10.1103/PhysRevC.61.024304
2000DE47 Phys.Rev. C62, 044311 (2000) D.S.Delion, J.Dukelsky, P.Schuck, E.J.V.de Passos, F.Krmpotic Proton-Neutron Self-Consistent Quasiparticle Random Phase Approximation within the O(5) Model
doi: 10.1103/PhysRevC.62.044311
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
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