NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = N.Carjan Found 60 matches. 2023OK02 Phys.Rev. C 107, 034608 (2023) K.Okada, T.Wada, R.Capote, N.Carjan Cassini-oval description of the multidimensional potential energy surface for 236U: Role of octupole deformation and calculation of the most probable fission path NUCLEAR STRUCTURE 236U; calculated potential energy surfaces, static fission path, influence of octupole deformation parameter, total deformation energy. Calculations in the frame of the microscopic-macroscopic model with a Cassini-oval description of the nuclear shapes. Established existence of a triple-humped barrier with a shallow third minimum.
doi: 10.1103/PhysRevC.107.034608
2019CA11 Phys.Rev. C 99, 034613 (2019) Structures in the energy distribution of the scission neutrons: Finite neutron-number effect NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated Fourier transforms of neutron wave packets during scission, scission neutron kinetic energy distributions at different intervals of time after scission. Dynamical scission model with bidimensional time-dependent Schrodinger equation. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.034613
2019CA15 Phys.Rev. C 99, 064606 (2019) N.Carjan, F.A.Ivanyuk, Yu.Ts.Oganessian Fission of superheavy nuclei: Fragment mass distributions and their dependence on excitation energy RADIOACTIVITY 252,254,256,258,260,262,264,266,268,270No, 264,266,268,270,272,274,276,278Hs, 276,278,280,282,284,286Cn, 290,291,292,293Lv, 268,270,272,274,276,278,280,282,284,288,292Ds, 254,256,258,260,262,264,266,268,270Rf, 272,274,276,280,284,285,286,287,288,292,296,298,300,304Fl, 276,280,284,288,292,294,296,300,304Og(SF); calculated average mass of light and heavy fission fragments, fission fragment mass distribution, average total kinetic energy of fission fragments, second moments of the total kinetic energy distribution of fission using a prescission point model.
doi: 10.1103/PhysRevC.99.064606
2019CA31 Int.J.Mod.Phys. E28, 1950103 (2019) Time-dependent decay rate and angular distribution of the scission neutrons by a dynamical approach NUCLEAR REACTIONS 235U(n, F), E thermal; calculated equipotentials before and after scission, scission neutrons decay rates, neutron survival probabilities, scission neutrons σ(θ).
doi: 10.1142/S0218301319501039
2017CA29 Nucl.Phys. A968, 453 (2017) N.Carjan, F.A.Ivanyuk, Yu.Ts.Oganessian Pre-scission model predictions of fission fragment mass distributions for super-heavy elements RADIOACTIVITY 279,280,281Ds, 281Rg, 282,283,284Cn, 284,285,286Fl[from superheavies produced in 48Ca impacting neutron-rich transuranium targets and sequentiual α-decays]; calculated relative yields from 279,281Ds, 281Rg, 282,284Cn vs mass number and vs TKE, potential energy surfaces, deformation of 280Ds and 284Cn. Fl, Lv, Og, Z=126(SF); calculated fragment mass distribution. 284,304Fl, 308,328126; calculated potential energy surface, deformation vs fragment mass. 274,276,278,280,282Fl; calculated yields vs fragment mass, potential energy surface, deformation. 252,254,256,258,262No; calculated fragment mass distribution, yield vs TKER; compared with data; deduced effect of octupole deformation on TKE and mass distribution. Calculations done using Strutinsky prescription, nuclear shapes prior to fission descibed using Cassinian ovals. Deformation described using α1, α3, α4 and α6 parameters.
doi: 10.1016/j.nuclphysa.2017.06.048
2016CA07 Phys.Rev. C 93, 024609 (2016) Scission neutrons for U, Pu, Cm, and Cf isotopes: Relative multiplicities calculated in the sudden limit RADIOACTIVITY 232,234,236,238,240U, 236,238,240,242,244Pu, 242,244,246,248,250Cm, 246,248,250,252,254Cf(SF); calculated scission-neutron (SN) multiplicity in the sudden limit as a function of mass asymmetry and as function of neutron number of fissioning nucleus, scission-neutron multiplicities averaged over all mass ratios. Fission yields calculated using GEF code. Scission-neutron (SN) multiplicity calculated also for the 235U(n, F), E=thermal reaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.024609
2016RI05 Eur.Phys.J. A 52, 368 (2016) Fourier transforms of single-particle wave functions in cylindrical coordinates
doi: 10.1140/epja/i2016-16368-6
2015CA19 Nucl.Phys. A942, 97 (2015) N.Carjan, F.A.Ivanyuk, Yu.Oganessian, G.Ter-Akopian Fission of transactinide elements described in terms of generalized Cassinian ovals: Fragment mass and total kinetic energy distributions NUCLEAR STRUCTURE 254,264Fm, 254,264Rf; calculated potential energy surface vs mass asymmetry and elongation, scission shapes at fission. 246,248,250,252,254,256,258,260,262,264Fm, 254,256,258,260,262,264,266,268Rf; calculated mass distribution and total kinetic energy distribution. 252,254,256,258,260,262,264No, 258,260,262,264,266,268Sg; calculated mass distribution. Generalized Cassinian ovals.
doi: 10.1016/j.nuclphysa.2015.07.019
2014CA17 Nucl.Data Sheets 118, 199 (2014) Current Density and Angular Distribution of Neutrons Emitted During Scission NUCLEAR REACTIONS 235U(n, F), E not given; calculated spatial distribution of neutron emission direction from scission, neutron multiplicity angular distribution.
doi: 10.1016/j.nds.2014.04.036
2013RI04 Nucl.Phys. A909, 50 (2013) Dynamical scission model RADIOACTIVITY 236U(SF); calculated scission fragment yields, energy partitions, spatial distribution of unbound neutrons, scission-neutron multiplicity, using time-dependent microscopic approach to scission.
doi: 10.1016/j.nuclphysa.2013.04.014
2012CA11 Rom.J.Phys. 57, 92 (2012) Dynamic Single-Particle Excitations in Low-Energy Fission RADIOACTIVITY 236U(SF); calculated emission points, partitions, excitation energy, pre-scission neutron multiplicity. Time-dependent Schrodinger equation.
2012CA17 Phys.Rev. C 85, 044601 (2012) N.Carjan, F.-J.Hambsch, M.Rizea, O.Serot Partition between the fission fragments of the excitation energy and of the neutron multiplicity at scission in low-energy fission
doi: 10.1103/PhysRevC.85.044601
2012CA22 Int.J.Mod.Phys. E21, 1250031 (2012) Nonadiabatic transition of the fissioning nucleus at scission: The time scale RADIOACTIVITY 236U(SF); calculated scission process using time-dependent approach, neutron multiplicities, time scale for adiabatic limit.
doi: 10.1142/S0218301312500310
2010CA21 Phys.Rev. C 82, 014617 (2010) Scission neutrons and other scission properties as function of mass asymmetry in 235U(nth, f) NUCLEAR REACTIONS 235U(n, X), E=thermal; calculated excitation energies of fragments, pairing gap and yield at scission, and scission neutron multiplicity for fragments of A=70-118. Renormalized BCS theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.014617
2009GH02 J.Phys.(London) G36, 025106 (2009) Two and three fragment decay from Z = 120 isotopes NUCLEAR STRUCTURE 294,288,282120; calculated fission barriers for binary fission channels.
doi: 10.1088/0954-3899/36/2/025106
2008CA09 Int.J.Mod.Phys. E17, 53 (2008) N.Carjan, K.Siwek-Wilczynska, I.Skwira-Chalot, J.Wilczynski Macroscopic dynamical description of rotating Au + Au system NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; analyzed surface instability of fissioning system in the framework of Los Alamos finite-range macroscopic dynamical model.
doi: 10.1142/S0218301308009549
2008GH01 Phys.Rev. C 77, 044607 (2008) R.A.Gherghescu, D.N.Poenaru, N.Carjan Neck influence on fission paths RADIOACTIVITY 236Pu (SF); calculated potential energy surfaces.
doi: 10.1103/PhysRevC.77.044607
2007CA37 Nucl.Phys. A792, 102 (2007) Emission of scission neutrons in the sudden approximation NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated scission neutron multiplicities, primary fission fragments excitation energies, reaction mechanism features.
doi: 10.1016/j.nuclphysa.2007.05.006
2007CA39 Phys.Atomic Nuclei 70, 1640 (2007) Isospin dependence of scission-neutron multiplicities in Pu isotopes NUCLEAR STRUCTURE 236,256Pu; calculated scission neutron multiplicities using the framework of sudden approximation.
doi: 10.1134/S1063778807090244
2007PO03 Europhys.Lett. 77, 62001 (2007) D.N.Poenaru, R.A.Gherghescu, N.Carjan Alpha-decay lifetimes semiempirical relationship including shell effects NUCLEAR STRUCTURE Z=52-118; analyzed α-decay T1/2; deduced parameters.
doi: 10.1209/0295-5075/77/62001
2005CA46 Comput.Phys.Commun. 173, 41 (2005) N.Carjan, M.Rizea, D.Strottman Improved boundary conditions for the decay of low lying metastable proton states in a time-dependent approach RADIOACTIVITY 109mIn, 147mTm, 166mIr, 171mAu(p); calculated T1/2 for proton emission from excited states. Time-dependent Schrodinger equation, improved boundary conditions, comparison with data.
doi: 10.1016/j.cpc.2005.07.005
2005GH03 Phys.Rev. C 71, 054612 (2005) Macroscopic-microscopic deformation energy in fusion isobaric reactions NUCLEAR REACTIONS 60Fe(44Ca, X), 60Ni(44Ar, X), 64Zn(46Ca, X), 64Ni(46Ar, X), 110Pd(182Hf, X), 110Cd(182Yb, X), 110Sn(182Er, X), 110Te(182Dy, X), E not given; calculated fusion barrier distributions, shell corrections, related features.
doi: 10.1103/PhysRevC.71.054612
2004PE04 Nucl.Phys. A735, 345 (2004) M.Petit, M.Aiche, G.Barreau, S.Boyer, N.Carjan, S.Czajkowski, D.Dassie, C.Grosjean, A.Guiral, B.Haas, D.Karamanis, S.Misicu, C.Rizea, F.Saintamon, S.Andriamonje, E.Bouchez, F.Gunsing, A.Hurstel, Y.Lecoz, R.Lucas, Ch.Theisen, A.Billebaud, L.Perrot, E.Bauge Determination of the 233Pa(n, f) reaction cross section from 0.5 to 10 MeV neutron energy using the transfer reaction 232Th(3He, p)234Pa NUCLEAR REACTIONS 232Th(3He, pF), (3He, dF), (3He, tF), (3He, αF), E=24-30 MeV; measured particle spectra, fission fragment anisotropies, fission probabilities. 231,233Pa, 230Th(n, F), E=0.5-10 MeV; deduced fission σ. 232,234Pa deduced fission barrier parameters. Comparison with previous work, model predictions.
doi: 10.1016/j.nuclphysa.2004.02.017
2002BR36 Phys.Rev. C66, 014608 (2002) T.A.Bredeweg, R.Yanez, B.P.Davin, K.Kwiatkowski, R.T.de Souza, R.Lemmon, R.Popescu, R.J.Charity, L.G.Sobotka, D.Hofman, N.Carjan Near-Scission Emission of Intermediate Mass Fragments in 12C + 232Th at E/A = 16 and 22 MeV NUCLEAR REACTIONS 232Th(12C, X), E=16, 22 MeV/nucleon; measured intermediate mass fragment yields, energy, angular distribution in coincidence with fission fragments following incomplete fusion; deduced statistical emission mechanism, other reaction mechanism features. Comparison with ternary fission data. NUCLEAR STRUCTURE 216,236U; calculated saddle-to-scission shapes vs angular momentum. Dynamical model.
doi: 10.1103/PhysRevC.66.014608
2000SE09 Eur.Phys.J. A 8, 187 (2000) Description of Long-Range Alpha Emission using the Sudden Approximation RADIOACTIVITY 238,240,242,244Pu(SF); calculated long-range alpha emission probabilities, angular distributions. Comparison with data.
doi: 10.1007/s100500070105
2000ST22 Phys.Scr. T88, 148 (2000) D.Strottman, N.Carjan, P.Talou New Aspects in the Decay of Quasi-Stationary Proton States by Mutidimensional Tunneling
doi: 10.1238/Physica.Topical.088a00148
2000TA23 Phys.Rev. C62, 014609 (2000) P.Talou, N.Carjan, C.Negrevergne, D.Strottman Exact Dynamical Approach to Spherical Ground-State Proton Emitters RADIOACTIVITY 105Sb, 113Cs, 147Tm, 151Lu, 157Ta, 185Bi(p); calculated T1/2. Time-dependent Schroedinger equation, comparison with data.
doi: 10.1103/PhysRevC.62.014609
1999TA06 Nucl.Phys. A647, 21 (1999) P.Talou, N.Carjan, D.Strottman Time-Dependent Approach to Bidimensional Quantum Tunneling: Application to the proton emission from deformed nuclei NUCLEAR STRUCTURE 208Pb; calculated decay rates, tunneling probability for proton emission from deformed, excited states. Time-dependent two-dimensional Schrodinger equation.
doi: 10.1016/S0375-9474(99)00005-6
1999TA30 Phys.Rev. C60, 054318 (1999) P.Talou, D.Strottman, N.Carjan Exact Calculation of Proton Decay Rates from Excited States in Spherical Nuclei RADIOACTIVITY 109I(p); calculated proton decay rates, T1/2 vs level energy. One-dimensional time-dependent Schrodinger equation.
doi: 10.1103/PhysRevC.60.054318
1998MI24 J.Phys.(London) G24, 1745 (1998) Proton Decay from Excited States in Spherical Nuclei NUCLEAR STRUCTURE 208Pb; calculated proton decay rates from excited states. Single-particle model, dynamical approach.
doi: 10.1088/0954-3899/24/9/008
1998TA25 Phys.Rev. C58, 3280 (1998) P.Talou, N.Carjan, D.Strottman Time-Dependent Properties of Proton Decay from Crossing Single-Particle Metastable States in Deformed Nuclei
doi: 10.1103/PhysRevC.58.3280
1996GR09 Phys.Rev. C54, 706 (1996) Dissipative Shape Dynamics in the sd Shell NUCLEAR STRUCTURE 28Si; calculated quadrupole shape dynamics; deduced pairing effects, dissipation, temperature roles, decay time scales, thermalization, configuration transitions related features. Time-dependent HFB Langevin formalism.
doi: 10.1103/PhysRevC.54.706
1996GR22 Roum.J.Phys. 41, 55 (1996) Dissipative Decay of Isomeric States
1995ER01 Nucl.Phys. A583, 395c (1995) B.Erazmus, R.Lednicky, V.L.Lyuboshitz, L.Martin, D.Nouais, J.Pluta, N.Carjan, B.Jakobsson, and the CHIC Collaboration Influence of the Emitting Nucleus on the Light-Particle Correlation Function NUCLEAR REACTIONS 197Au(Ar, X), E=30 MeV/nucleon; measured nn-, np-, pp-correlation function; deduced emitting nucleus role.
doi: 10.1016/0375-9474(94)00693-H
1995MA14 Nucl.Phys. A583, 407c (1995) L.Martin, B.Erazmus, J.Pluta, D.Nouais, D.Ardouin, P.Eudes, F.Guilbault, P.Lautridou, C.Lebrun, R.Lednicky, A.Rahmani, T.Reposeur, D.Roy, L.Sezac, M.Lewitowicz, W.Mittig, P.Roussel-Chomaz, N.Carjan, P.Aguer, W.Burzynski, W.Peryt, H.Dabrowski, P.Stefanski Two-Proton Correlation Function Measured at Very Small Relative Momenta NUCLEAR REACTIONS 48Ti(129Xe, X), E=45 MeV/nucleon; measured pp-coin; deduced emission mechanism, source velocity.
doi: 10.1016/0375-9474(94)00695-J
1994CA36 Z.Phys. A349, 353 (1994) N.Carjan, O.Serot, D.Strottman Time-Dependent Schrodinger Approach to Sub-Barrier Fission NUCLEAR STRUCTURE 213At; calculated fission rates at saddle, scission points. Time-dependent Schrodinger approach.
doi: 10.1007/BF01288994
1994ER01 Phys.Rev. C49, 349 (1994) B.Erazmus, L.Martin, R.Lednicky, N.Carjan Classical and Quantum Approach to Light-Particle Correlations in Intermediate-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 108Ag(40Ar, X), E=44 MeV/nucleon; calculated proton spectra, pp-, pd-correlation functions. Classical, quantum mechanical models.
doi: 10.1103/PhysRevC.49.349
1994SE02 Nucl.Phys. A569, 562 (1994) O.Serot, N.Carjan, D.Strottman Transient Behaviour in Quantum Tunneling: Time-dependent approach to alpha decay
doi: 10.1016/0375-9474(94)90319-0
1993WA10 Phys.Rev.Lett. 70, 3538 (1993) One-Body Dissipation in Agreement with Prescission Neutrons and Fragment Kinetic Energies NUCLEAR REACTIONS 181Ta(19F, F), 184W(16O, X), E not given; calculated fission width, emitted neutron, proton, α-particle numbers, time dependence, fusion-fission σ(E). 200Pb deduced fission dynamics. Two-dimensional Langevin equation.
doi: 10.1103/PhysRevLett.70.3538
1992CA09 Phys.Rev. C45, 2185 (1992) Asymmetric Fission of 149Tb(*) from the Finite-Range, Rotating-Liquid-Drop Model: Mean total kinetic energies for binary fragmentation NUCLEAR STRUCTURE 149Tb; calculated fission fragment total kinetic energies vs charge, mass; deduced dissipative path motion features. Finite range rotating liquid drop model.
doi: 10.1103/PhysRevC.45.2185
1992OB05 Z.Phys. A344, 59 (1992) Information on Nuclear Shapes Near the Scission Point from Internal Trajectory Calculations NUCLEAR REACTIONS 235U(n, F), E not given; calculated Eα, α-yield vs θ in α-accompanied fission; deduced α-emission process, nuclear shapes. Trajectory calculations, α-particle inside, outside 236U.
doi: 10.1007/BF01291021
1991ER05 Phys.Rev. C44, 2663 (1991) B.Erazmus, N.Carjan, D.Ardouin Classical Model for Two-Proton Correlations in Intermediate-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 108Ag(40Ar, X), E=44 MeV/nucleon; calculated pp-correlation function. Three-body trajectories, Coulomb, nuclear forces.
doi: 10.1103/PhysRevC.44.2663
1988CA18 Phys.Rev. C38, 1692 (1988) Predictions of the Macroscopic Model of Nuclei: Barriers to fusion and to light fragment emission NUCLEAR STRUCTURE 149Tb, 194Hg; calculated fission, fusion barriers. Macroscopic model.
doi: 10.1103/PhysRevC.38.1692
1986CA04 Nucl.Phys. A452, 381 (1986) Effect of Dissipation on Ternary Fission in very Heavy Nuclear Systems NUCLEAR STRUCTURE A=100-300; calculated ternary fission fragment translational kinetic energy vs mass, dissipation dependence. Macroscopic dynamical model.
doi: 10.1016/0375-9474(86)90204-6
1986VA20 Z.Phys. A324, 331 (1986) L.C.Vaz, J.M.Alexander, N.Carjan Comparison of Semiclassical and Quantum Mechanical Angular Distributions for Nuclear Fission and Evaporation NUCLEAR REACTIONS 56Fe(α, αX), E=17 MeV; 159Tb(22Ne, αX), E=60, 176 MeV; calculated evaporation α-anisotropy. 248Cm(32S, F), E=218 MeV; calculated fission fragment anisotropy. Semi-classical, quantum mechanical methods.
1982SC26 Z.Phys. A308, 215 (1982) K.-H.Schmidt, H.Delagrange, J.P.Dufour, N.Carjan, A.Fleury Influence of Shell Structure and Pairing Correlations on the Nuclear State Density NUCLEAR STRUCTURE 194Hg, 212Th, 208Pb; calculated ground state energy corrections. 216Th, 252Fm; calculated entropy fluctuation vs excitation. 208Pb; calculated level density parameter vs deformation. Microscopic model.
doi: 10.1007/BF01418283
1980CA22 Phys.Rev. C22, 2008 (1980) Finite-Size Effects in Trajectory Calculations for α Particles Emitted During Nuclear Fission NUCLEAR REACTIONS, Fission 235U(n, αF), E not given; calculated α-particle trajectories. Fissioning nucleus time evolution, fission fragment finite size effects.
doi: 10.1103/PhysRevC.22.2008
1980CA25 Z.Phys. A298, 219 (1980) F.Caitucoli, B.Leroux, G.Barreau, N.Carjan, T.Benfoughal, T.P.Doan, F.El Hage, A.Sicre, M.Asghar, P.Perrin, G.Siegert The Thermal-Neutron-Induced Alpha-Accompanied Fission of 235U Investigation of the Low Energy Part of the Alpha Spectrum NUCLEAR REACTIONS, Fission 235U(n, αF), E=thermal; measured σ(Eα); deduced asymmetry at low energies, multiplicative factor relative to binary fission.
1980LE10 Nucl.Phys. A342, 37 (1980) H.-D.Lemke, B.Ziegler, M.Mutterer, J.P.Theobald, N.Carjan Absolute Photofission Cross Section of 209Bi in the Energy Range from 40 to 65 MeV NUCLEAR REACTIONS 209Bi(γ, F), E=40-65 MeV; measured σ; deduced total photoabsorption σ for compound nucleus formation. Statistical model.
doi: 10.1016/0375-9474(80)90505-9
1979CA07 Phys.Rev. C19, 2267 (1979) N.Carjan, H.Delagrange, A.Fleury Excitation Energy Dependence of the Level Density for Fissionable Nuclei NUCLEAR STRUCTURE 194Hg, 210Po, 240Pu; calculated nuclear level densities; deduced dependence on excitation energy, deformation, nuclear parameters. Microscopic model, shell, pairing effect.
doi: 10.1103/PhysRevC.19.2267
1975CA02 Phys.Rev. C11, 782 (1975) N.Carjan, A.Sandulescu, V.V.Pashkevich Shell and Pairing Effects in Alpha-Accompanied Fission RADIOACTIVITY, Fission 252Cf(SF); calculated preformation probability of α particles for different shapes. NUCLEAR REACTIONS 235U(n, F); calculated preformation probability of α particles for different shapes.
doi: 10.1103/PhysRevC.11.782
1973CA12 Rev.Roum.Phys. 18, 151 (1973) N.Carjan, V.V.Pashkevich, A.Sandulescu Nuclear Structure Effects in Alpha-Accompanied Fission NUCLEAR STRUCTURE, Fission 235U(n, F), 252Cf(SF); calculated X-emission probability.
1971BO60 Rev.Roum.Phys. 16, 397 (1971) On the Calculation of the Beta Decay Observables for the 1- → 0+ Transition RADIOACTIVITY 210Bi; calculated log ft, β-shape factor, longitudinal polarization.
1971CA33 Rev.Roum.Phys. 16, 811 (1971) N.Carjan, S.Holan, A.Sandulescu, C.Sabac Alpha Reduced Widths for Superheavy Nuclei RADIOACTIVITY Sg, Hs, Ds; Z=112, 114, 116; calculated reduced α-widths.
1971CA37 Z.Naturforsch. 26a, 1389 (1971) Estimating the Alpha-Particles Transmission Through a Barrier RADIOACTIVITY 194,196,198,200,202,204,206,208,210,212,214,216,218Po; analyzed α-decay data. 208,210,212Po calculated barrier penetrabilities JWKB method.
1971CA43 Rev.Roum.Phys. 16, 1175 (1971) N.Carjan, S.Holan, A.Sandulescu, C.Sabac Theoretical Alpha Decay Rates of Platinum, Gold and Mercury Isotopes RADIOACTIVITY 173,174,175,176,177,178,179,180,181,182,183,184,186,188,190Pt, 177,179,181,183,185,187Au, 179,180,181,182,183,184,185,186,187Hg; calculated reduced α-widths, penetrabilities.
1970BO04 Phys.Lett. 31B, 280 (1970) The Isobaric Analogue State of the 199Au Ground State and the β Decay of the Latter RADIOACTIVITY 199Au; calculated log ft, β-shape factors, linear polarization.
doi: 10.1016/0370-2693(70)90170-X
1970BO14 Rev.Roum.Phys. 15, 355 (1970) D.Bogdan, N.Carjan, I.Piticu, C.Protop, I.Vata On the Calculation of Beta Decay Observables RADIOACTIVITY 166Dy, 186,188Re, 198,199Au; calculated log ft, β-shape factors, βγ(θ) coefficients, βγ-CP coefficients, P(W) for first-forbidden transitions.
1970BO38 Yad.Fiz. 12, 700 (1970); Sov.J.Nucl.Phys. 12, 379 (1971) D.Bogdan, N.Carjan, C.Protop, I.Vata Effects of Correction Matrix Elements for the First Forbidden β- Transition in Au198 RADIOACTIVITY 198Au; calculated log ft, βγ correlation coefficients.
1970BO42 Z.Phys. 240, 233 (1970) A Theoretical Study of the Beta Decay Transitions 0- → 2+ and 0- → 0+ of the Ho166 Nucleus RADIOACTIVITY 166Ho; calculated log ft, shape factors, βγ(θ) coefficients.
doi: 10.1007/BF01395560
Back to query form |