NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = S.B.Duarte Found 45 matches. 2023CU03 Phys.Rev. C 107, 024613 (2023) E.Cupertino Gomes, U.B.RodrIguez, M.Goncalves, A.R.C.Pinheiro, B.M.Santos, C.R.R.Souza, L.R.Hirsch, S.B.Duarte Secondary particle predictions in quasifree proton scattering reactions in the 100-250 MeV energy range NUCLEAR REACTIONS 12C, 14N, 16O, 23Na, 31P, 32S, 36Cl, 39K, 40Ca, 56Fe, 64Cu, 65Zn, 79Se, 184W, 195Pt, 208Pb(p, X), E=100, 150, 200, 250 MeV; calculated proton and neutron yields. 12C(p, p'), (p, np), E=200 MeV; calculated σ(θ, E). C, O, Ca, Se, Pb(p, X), E=100, 250 MeV; calculated Ep (proton spectra), En (neutron spectra), σ(θ, E) for proton and neutron production. Al, Ti, Cu, Ag, Ta, Pb(p, π+), (p, π-), E=730 MeV; calculated pion multiplicity. Multicollisional Monte Carlo intranuclear cascade model. Determined the effects of the inclusion of an effective mass for bound baryons on yield, spectra, and angular distribution of secondary particles. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024613
2023DO10 Eur.Phys.J. A 59, 260 (2023) M.dos Santos, A.R.Samana, S.B.Duarte, C.A.Barbero Neutral-current neutrino-nucleus scattering within QRPA models
doi: 10.1140/epja/s10050-023-01171-9
2023MO06 Eur.Phys.J. A 59, 31 (2023) M.Mohammadzadeh, H.Khalili, A.R.Samana, M.dos Santos, C.A.Barbero, S.B.Duarte Neutrino and Antineutrino captures on 18O within QRPA models NUCLEAR REACTIONS 18O(ν, e-), (ν, e+), E<14 MeV; calculated σ within the Quasiparticle Random Phase Approximation (QRPA) and Projected QRPA (PQRPA) models. Comparison with available data.
doi: 10.1140/epja/s10050-023-00944-6
2022ME08 Phys.Rev. C 106, 024608 (2022) E.L.Medeiros, N.Teruya, S.B.Duarte, O.A.P.Tavares Nonlocality effect in α decay of heavy and superheavy nuclei RADIOACTIVITY 185mPt(α); calculated contribution of the nonlocal effect on tunneling calculations. Z=52-103(α); Z=104-118(α); calculated T1/2 for 239 heavy and 16 superheavy nuclei using α-cluster potential barrier penetration model with semiclassical WKB approach. Comparison of experimental results with new universal plot (NUP), and with universal decay law (UDL). 110Te, 155Tm, 157Lu, 161,163Ta, 161,167Re, 165Ir, 169,171Au, 183Tl, 220,236U, 224Pu, 232,250Cm, 242,244Fm, 258No, 257Lr, 260,264,266Rf, 257Db, 258,262,264,266Sg, 274,276Hs, 278,280,282Cn, 284Fl(α); calculated T1/2 and compared with experimental values.
doi: 10.1103/PhysRevC.106.024608
2019RO22 J.Phys.(London) G46, 115109 (2019) U.B.Rodriguez, C.Z.Vargas, M.Goncalves, S.B.Duarte, F.Guzman Alpha half-lives calculation of superheavy nuclei with Qα-value predictions based on the Bayesian neural network approach RADIOACTIVITY 259Sg, 269Hs, 273Ds, 272Rg, 289,290Mc, 294Og(α); analyzed available data; deduced Q-values. Comparison with available data.
doi: 10.1088/1361-6471/ab2c86
2017GO17 Phys.Lett. B 774, 14 (2017) M.Goncalves, N.Teruya, O.A.P.Tavares, S.B.Duarte Two-proton emission half-lives in the effective liquid drop model RADIOACTIVITY 16Ne, 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated Q-values and T1/2. Comparison with experimental data.
doi: 10.1016/j.physletb.2017.09.032
2016PI03 Phys.Rev. C 93, 034612 (2016) A.R.C.Pinheiro, L.P.G.De Assis, S.B.Duarte, B.M.Santos, M.Goncalves Multiparticle versus single sequential emission in nuclear evaporation processes NUCLEAR REACTIONS 208Pb, 200Hg(p, X), E=800, 1200, 1500 MeV; calculated neutron multiplicity versus excitation energy of the final nucleus using single sequential emission, and simultaneous multiparticle emission, charged-particle yields, channel branching ratios. Monte Carlo simulation for the effect of different emission channels on particle yield and fission process in compound nucleus modes of deexcitation. Comparison with experimental data. Relevance to acceleration driven system (ADS) reactors.
doi: 10.1103/PhysRevC.93.034612
2016SA06 Nucl.Phys. A948, 78 (2016) B.M.Santos, A.R.C.Pinheiro, M.Goncalves, S.B.Duarte, R.G.Cabral On the nucleon effective mass role to the high energy proton spallation reactions NUCLEAR REACTIONS Pb(p, x), E=0.8, 1.0, 1.2, 1.6, 1.8, 2.0 GeV; calculated time development of average E*, effective mass, neutron multiplicity, mass distribution during cascade and evaporation phases using TIERCE and INCL4 codes.
doi: 10.1016/j.nuclphysa.2016.01.048
2016TE03 Phys.Rev. C 93, 024606 (2016) N.Teruya, S.B.Duarte, M.M.N.Rodrigues Nonlocality effect in the tunneling of one-proton radioactivity RADIOACTIVITY 144,145,146,146m,147,147mTm, 150,150m,151,151mLu, 155,156,156m,157Ta, 159,160m,161,161mRe, 164,165,166,166m,167,167mIr, 170,170m,171,171mAu, 176,176Tl, 185Bi(p); calculated WKB barrier penetrability factor and half-lives with and without proton effective mass (EM) correction and using Becchetti and Greenlees nuclear shell model parametrization. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.024606
2012DU01 Phys.Rev. C 85, 017601 (2012) α-decay systematics for superheavy elements RADIOACTIVITY Z=51-103(α); calculated half-lives for 164 nuclides; deduced universal decay law (UDL) and new universal plot (NUP) fitting parameters. Z=104-118(α); calculated half-lives of 35 superheavy nuclides. Quantum-mechanical tunneling calculation with α-cluster potential description. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.017601
2011AN29 J.Phys.:Conf.Ser. 312, 082010 (2011) E.Andrade, II, J.C.M.Menezes, S.B.Duarte, F.Garcia, P.C.R.Rossi, O.A.P.Tavares, A.Deppman Fragment mass distributions for heavy nuclei fission induced by intermediate energy probes NUCLEAR REACTIONS 237Np, 241Am(p, F), E=660 MeV;238U(γ, F), E=0-50 MeV; calculated mass distribution from bremsstrahlung reaction using Monte Carlo for nuclear cascade followed by competition between fission and particle emission. Compared with data and other calculations.
doi: 10.1088/1742-6596/312/4/082010
2011GO29 J.Phys.(London) G38, 115105 (2011) I.Gonzalez, C.Barbero, A.Deppman, S.B.Duarte, F.Krmpotic, O.Rodriguez Many-body cascade calculation of final state interactions in 12ΛC nonmesonic weak decay RADIOACTIVITY 12C(nn), (np); calculated kinetic energy spectra for protons and neutrons, opening angle correlations between proton-neutron and neutron-neutron pairs, 12C hypernucleus. Comparison with experiment.
doi: 10.1088/0954-3899/38/11/115105
2010BA47 Phys.Rev. C 82, 067305 (2010) C.Barbero, A.Mariano, S.B.Duarte Role of the isovector nucleon-nucleus interaction potential in nonmesonic hypernuclear decay NUCLEAR STRUCTURE 5He, 12C; calculated hypernucleus decay observables using independent-particle shell model.
doi: 10.1103/PhysRevC.82.067305
2009LE22 Phys.Rev. C 80, 014606 (2009) T.N.Leite, N.Teruya, A.Dimarco, S.B.Duarte, O.A.P.Tavares, M.Goncalves 12O resonant structure evaluated by the two-proton emission process RADIOACTIVITY 12O(2p); analyzed characteristics of resonant ground state, decay energy distribution, channel distribution ratios, and widths using statistical model for the sequential and simultaneous two-proton emission decay modes. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.014606
2008PO02 Eur.Phys.J. D 48, 145 (2008) D.Portes, Jr., H.Rodrigues, S.B.Duarte, B.Baseia Quantum states transfer between coupled fields
doi: 10.1140/epjd/e2008-00088-0
2007ME28 Eur.Phys.J. A 34, 417 (2007) E.L.Medeiros, M.M.N.Rodrigues, S.B.Duarte, O.A.P.Tavares Systematics of half-lives for proton radioactivity NUCLEAR STRUCTURE A=30-186; analyzed proton-decay partial T1/2. RADIOACTIVITY 30Cl, 53Co, 58Ge, 68Br, 89Rh, 105Sb, 108,109I, 112,113Cs, 117La, 121Pr, 130,131Eu, 135Tb, 140,141Ho, 145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171,173Au, 176,177Tl, 184,185,186Bi(p); calculated proton-decay partial T1/2. Semi-empirical model including effect of deformation.
doi: 10.1140/epja/i2007-10513-4
2006DE27 Phys.Rev. C 73, 064607 (2006) A.Deppman, G.Silva, S.Anefalos, S.B.Duarte, F.Garcia, F.H.Hisamoto, O.A.P.Tavares Photofission and total photoabsorption cross sections in the energy range of shadowing effects NUCLEAR REACTIONS 12C, 27Al, 63Cu, 118Sn, 207Pb(γ, X), E=1000-3000 MeV; calculated total photoabsorption σ. 207Pb, 232Th, 233,235,238U, 237Np(γ, F), E=900-3400 MeV; calculated photofission σ. Comparison with data.
doi: 10.1103/PhysRevC.73.064607
2006ME15 J.Phys.(London) G32, B23 (2006) E.L.Medeiros, M.M.N.Rodrigues, S.B.Duarte, O.A.P.Tavares Systematics of alpha-decay half-life: new evaluations for alpha-emitter nuclides NUCLEAR STRUCTURE A=100-300; analyzed α-decay T1/2; deduced parameters. RADIOACTIVITY 110Te, 113I, 151Gd, 174Hf, 163Ta, 180W, 184Os, 210Po, 200,206,208,211,218At, 203,228Ra, 231Pa, 250Cm, 266Sg, 272Rg(α); calculated α-decay partial T1/2. Semiempirical model.
doi: 10.1088/0954-3899/32/8/B01
2006ME20 J.Phys.(London) G32, 2345 (2006) E.L.Medeiros, M.M.N.Rodrigues, S.B.Duarte, O.A.P.Tavares Comments on the rarest alpha activity observed in nature RADIOACTIVITY 180W(α); compiled, analyzed T1/2.
doi: 10.1088/0954-3899/32/11/N01
2005TA37 Braz.J.Phys. 35, 915 (2005) O.A.P.Tavares, S.B.Duarte, V.Morcelle, A.Deppman Photofissility at 1 GeV for Nuclei Throughout the Periodic Table NUCLEAR REACTIONS 48Ti, 56Fe, 59Ni, 63Cu, 65Zn, 93Nb, 96Mo, 108Ag, 112Cd, 115In, 119Sn, 122Sb, 128Te, 139La, 140Ce, 144Nd, 150Sm, 157Gd, 159Tb, 163Dy, 165Ho, 169Tm, 173,174Yb, 175Lu, 178Hf, 181Ta, 184W, 186Re, 190Os, 195Pt, 197Au, 201Hg, 204Tl, 207,208Pb, 209Bi, 232Th, 233,235,238U, 237Np(γ, F), E=1 GeV; calculated first-chance fission probability.
doi: 10.1590/S0103-97332005000500054
2004DU23 J.Phys.(London) G30, 1487 (2004) S.B.Duarte, O.A.P.Tavares, M.Goncalves, O.Rodriguez, F.Guzman, T.N.Barbosa, F.Garcia, A.Dimarco Half-life predictions for decay modes of superheavy nuclei NUCLEAR STRUCTURE Z=110-135; calculated α-decay, cluster-decay, and cold fission T1/2. Effective liquid-drop model. RADIOACTIVITY 287,288Mc, 283,284Nh, 279,280Rg(α); calculated T1/2, Qα. Effective liquid-drop model, comparison with data.
doi: 10.1088/0954-3899/30/10/014
2004GO61 Braz.J.Phys. 34, 919 (2004) M.Goncalves, E.C.de Oliveira, E.L.Medeiros, S.de Pina, S.B.Duarte Hot Hypernucleus Formation in High-Energy Photonuclear Reactions NUCLEAR REACTIONS C, Al, Ni(γ, X), E=1.2 GeV; calculated fragment charge and mass distributions, hypernucleus yields.
doi: 10.1590/s0103-97332004000500057
2004LI78 Braz.J.Phys. 34, 753 (2004) V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, H.Dias, S.B.Duarte, W.R.Carvalho, Jr., M.S.Hussein, A.C.S.Lima, L.F.R.Macedo, J.Mesa, S.A.Pashchuk, T.E.Rodrigues, G.Silva, H.R.Schelin, O.A.P.Tavares Residual Nucleus Excitation Energy in (e, e'p)- Reaction
doi: 10.1590/S0103-97332004000500012
2004RO22 Phys.Rev. C 69, 064611 (2004) T.E.Rodrigues, J.D.T.Arruda-Neto, A.Deppman, V.P.Likhachev, J.Mesa, C.Garcia, K.Shtejer, G.Silva, S.B.Duarte, O.A.P.Tavares Photonuclear reactions at intermediate energies investigated via the Monte Carlo multicollisional intranuclear cascade model NUCLEAR REACTIONS Sn, Ce, Ta, Pb(γ, X), E=20-140 MeV; calculated total photoabsorption σ, neutron multiplicities. Monte Carlo multicollisional intranuclear cascade model, comparison with data.
doi: 10.1103/PhysRevC.69.064611
2004TA04 J.Phys.(London) G30, 377 (2004) O.A.P.Tavares, S.B.Duarte, A.Deppman, V.P.Likhachev Nuclear photofissility of natPb and 232Th at energies above the pion photoproduction threshold NUCLEAR REACTIONS Pb, 232Th(γ, F), E=0.2-6 GeV; calculated fissility, fragment production probabilities. Intranuclear cascade and evaporation-fission competition mechanisms, comparison with data.
doi: 10.1088/0954-3899/30/4/001
2004TA48 Braz.J.Phys. 34, 924 (2004) O.A.P.Tavares, S.B.Duarte, A.Deppman, V.P.Likhachev New Approach to Nuclear Photofission Reactions above 0.15 GeV NUCLEAR REACTIONS Pb(γ, F), E ≈ 0.1-7 GeV; analyzed fission probability. Two-step model.
doi: 10.1590/S0103-97332004000500058
2003DE20 Nucl.Instrum.Methods Phys.Res. B211, 15 (2003) A.Deppman, O.A.P.Tavares, S.B.Duarte, J.D.T.Arruda-Neto, M.Goncalves, V.P.Likhachev, J.Mesa, E.C.de Oliveira, S.R.de Pina, O.Rodriguez A Monte Carlo method for nuclear evaporation and fission at intermediate energies NUCLEAR STRUCTURE 237Np, 238U, 232Th; calculated fissility vs excitation energy, competition with evaporation channels. Monte Carlo approach.
doi: 10.1016/S0168-583X(03)01265-5
2002DE35 J.Phys.(London) G28, 2259 (2002) S.R.de Pina, J.Mesa, A.Deppman, J.D.T.Arruda-Neto, S.B.Duarte, E.C.de Oliveira, O.A.P.Tavares, E.L.Medeiros, M.Goncalves, E.de Paiva Nucleon Effective Mass Effects on the Pauli-Blocking Function
doi: 10.1088/0954-3899/28/8/311
2002DE60 Phys.Rev. C 66, 067601 (2002) A.Deppman, O.A.P.Tavares, S.B.Duarte, J.D.T.Arruda-Neto, M.Goncalves, V.P.Likhachev, E. C.de Oliveira Photofissility of heavy nuclei at intermediate energies NUCLEAR REACTIONS 209Bi, 232Th, 238U, 237Np, 243Am(γ, F), E=200-1000 MeV; calculated fissility. 209Bi, 243Am(γ, F), E=200-1000 MeV; calculated photofission σ. Monte Carlo approach.
doi: 10.1103/PhysRevC.66.067601
2002DU16 At.Data Nucl.Data Tables 80, 235 (2002) S.B.Duarte, O.A.P.Tavares, F.Guzman, A.Dimarco, F.Garcia, O.Rodriguez, M.Goncalves Half-Lives for Proton Emission, Alpha Decay, Cluster Radioactivity, and Cold Fission Processes Calculated in a Unified Theoretical Framework RADIOACTIVITY 105Sb, 109I, 112,113Cs, 117La, 131Eu, 140,141Ho, 145,146,147Tm, 150,151Lu, 156,157Ta, 160,161Re, 165,166,167Ir, 171Au, 185Bi(p); calculated proton emission T1/2. 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 228Th(20O); 230Th, 231Pa, 232,233,234U(24Ne); 234U(26Ne); 234U, 236,238Pu(28Mg); 238Pu(30Mg), (32Si); 242Cm(34Si); calculated cluster emission T1/2. 258,259Fm, 259,260Md, 258,262No(SF); calculated fission fragment mass distributions. Z=27-111; A=50-273; calculated T1/2, Q for p-decay, α-decay, cluster emission. Z=82-111; A=180-272; calculated cold fission T1/2. Effective liquid drop model, comparisons with data.
doi: 10.1006/adnd.2002.0881
2001DE41 Phys.Rev.Lett. 87, 182701 (2001) A.Deppman, O.A.P.Tavares, S.B.Duarte, E.C.de Oliveira, J.D.T.Arruda-Neto, S.R.de Pina, V.P.Likhachev, O.Rodriguez, J.Mesa, M.Goncalves Photofissility of Actinide Nuclei at Intermediate Energies NUCLEAR REACTIONS 237Np, 238U, 232Th(γ, F), E ≈ 200-1000 MeV; analyzed fissility; deduced role of proton and α evaporation. Monte Carlo approach.
doi: 10.1103/PhysRevLett.87.182701
2000DI17 Int.J.Mod.Phys. E9, 205 (2000) A.Dimarco, S.B.Duarte, O.A.P.Tavares, M.Goncalves, F.Garcia, O.Rodriguez, F.Guzman Effect of Nuclear Deformation on the Alpha-Decay Half-Life of Even-Even Alpha Emitters NUCLEAR STRUCTURE Z=52-108; calculated α-decay T1/2, deformation effects. Comparison with data.
doi: 10.1016/S0218-3013(00)00014-3
2000GA25 J.Phys.(London) G26, 755 (2000) F.Garcia, O.Rodriguez, M.Goncalves, S.B.Duarte, O.A.P.Tavares, F.Guzman Alpha Decay and Nuclear Deformation: The case for favoured alpha transitions of even-even emitters RADIOACTIVITY A=106-264(α); calculated T1/2 including quadrupole deformation effects. Comparison with experimental values.
doi: 10.1088/0954-3899/26/6/301
2000GO11 Eur.Phys.J. A 7, 435 (2000) M.Goncalves, M.Chiapparini, L.Castro, E.C.de Oliveira, S.B.Duarte, E.L.Medeiros Multiparticle Correlations in Resonance-Matter Formation NUCLEAR REACTIONS 12C(12C, X), 20Ne(20Ne, X), 40Ca(40Ca, X), 58Ni(58Ni, X), E=1-2 GeV/nucleon; calculated maximum number of resonances, particle population, pion multiplicity, density time evolution. Intranuclear cascade model with particle correlations, comparison with data.
doi: 10.1007/s100500050414
1999GU08 Phys.Rev. C59, R2339 (1999) F.Guzman, M.Goncalves, O.A.P.Tavares, S.B.Duarte, F.Garcia, O.Rodriguez Proton Radioactivity from Proton-Rich Nuclei RADIOACTIVITY 55Cu, 58Ge, 105Sb, 109I, 112,113Cs, 142Ho, 146,147Tm, 150,151Lu, 156,157Ta, 160,161Re, 165,166,167Ir, 171Au, 177,178,179Tl, 185,187Bi(p); calculated proton decay T1/2. Effective liquid drop model. Comparison with data.
doi: 10.1103/PhysRevC.59.R2339
1999RO01 Phys.Rev. C59, 253 (1999) O.Rodriguez, F.Guzman, S.B.Duarte, O.A.P.Tavares, F.Garcia, M.Goncalves New Valleys of Cold Fission and Cluster Radioactivity Processes from Nuclei Far from the β-Stability Line RADIOACTIVITY Rn, Po, Pb; calculated α-decay T1/2. Ba, Sn, Po, Bi; calculated cluster decay T1/2 in neutron-deficient isotopes; deduced shell effects. Geiger-Nutall systematics.
doi: 10.1103/PhysRevC.59.253
1998DE38 Phys.Lett. 434B, 1 (1998) S.de Pina, E.C.de Oliveira, E.L.Medeiros, S.B.Duarte, M.Goncalves Photonuclear K+ Production Calculation Near Threshold NUCLEAR REACTIONS 1H, 12C, 64Cu, 208Pb(γ, K+X), E=0.85-1.2 GeV; calculated pion, kaon multiplicities. 12C(γ, K+X), E=0.8-1.1 GeV; calculated σ(θ). Comparison with data.
doi: 10.1016/S0370-2693(98)00726-6
1998DU05 Phys.Rev. C57, 2516 (1998) S.B.Duarte, O.Rodriguez, O.A.P.Tavares, M.Goncalves, F.Garcia, F.Guzman Cold Fission Description with Constant and Varying Mass Asymmetries RADIOACTIVITY 234U(SF); calculated T1/2, fragments mass distributions. Comparison of constant, variable mass asymmetry descriptions. Alpha, cluster radioactivity also discussed.
doi: 10.1103/PhysRevC.57.2516
1998TA21 J.Phys.(London) G24, 1757 (1998) O.A.P.Tavares, S.B.Duarte, O.Rodriguez, F.Guzman, M.Goncalves, F.Garcia Effective Liquid Drop Description for Alpha Decay of Atomic Nuclei NUCLEAR STRUCTURE Z=52-111; calculated α-decay T1/2. Effective liquid drop model. Comparison with data.
doi: 10.1088/0954-3899/24/9/009
1997DU14 Phys.Rev. C56, 3414 (1997) S.B.Duarte, O.A.P.Tavares, M.Goncalves Importance of the Inner Potential Barrier in Nuclear Spontaneous Cold Fission Processes RADIOACTIVITY 234U, 242Pu, 248Cf, 252Cf(SF); calculated potential barrier for several decay modes; deduced inner barrier role.
doi: 10.1103/PhysRevC.56.3414
1997GO05 Phys.Rev. C55, 2625 (1997) M.G.Goncalves, E.L.Medeiros, S.B.Duarte Effect of Multiparticle Collisions on Pion Production in Relativistic Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ca, X), E=2 GeV/nucleon; calculated N-body collisions frequency time evolution. 40Ca(40Ca, X), E ≤ 2 GeV/nucleon; analyzed pion multiplicity data, other aspects; deduced multi-baryonic collisions role.
doi: 10.1103/PhysRevC.55.2625
1997GO11 Phys.Lett. 406B, 1 (1997) M.Goncalves, S.de Pina, D.A.Lima, W.Milomem, E.L.Medeiros, S.B.Duarte Many-Body Cascade Calculation for Photonuclear Reactions NUCLEAR REACTIONS 27Al, 100Ru(γ, X), E=0.5-1.5 GeV; calculated Δ resonance population, pion multiplicity, residual nucleus excitation energy, multiplicity of emitted nucleons, proton spectra. Many-body cascade approach, comparison with one-body cascade model.
doi: 10.1016/S0370-2693(97)00662-X
1996CH21 Phys.Rev. C54, 936 (1996) M.Chiapparini, H.Rodrigues, S.B.Duarte Neutrino Trapping in Nonstrange Dense Stellar Matter
doi: 10.1103/PhysRevC.54.936
1996DU04 Phys.Rev. C53, 2309 (1996) Effective Inertial Coefficient for the Dinuclear Regime of the Exotic Decay of Nuclei RADIOACTIVITY A ≈ 120-243; calculated α-, exotic decay T1/2; deduced effective inertial coefficient role. Geometric, incompressibility constraint relations used.
doi: 10.1103/PhysRevC.53.2309
1993GO18 Phys.Rev. C48, 2409 (1993) Effective Liquid Drop Description for the Exotic Decay of Nuclei RADIOACTIVITY 221Fr, 226,221,222,223,224Ra(14C); 228Th(20O); 231Pa(23F); 230Th, 231Pa, 232,234U(24Ne); 233U(25Ne); 234U, 236,238Pu(28Mg); 237Np(30Mg); 238Pu(32Si); 241Am, 242Cm(34Si); calculated exotic decay T1/2. Effective liquid drop model, shell corrections.
doi: 10.1103/PhysRevC.48.2409
Back to query form |