NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.B.Malik Found 65 matches. 2015HO06 Phys.Rev. C 91, 064613 (2015) S.Hossain, A.S.B.Tariq, A.Nilima, M.S.Islam, R.Majumder, M.A.Sayed, M.M.Billah, M.M.B.Azad, M.A.Uddin, I.Reichstein, F.B.Malik, A.K.Basak Dependence of the 16O+16O nuclear potential on nuclear incompressibility NUCLEAR REACTIONS 16O(16O, 16O), E=31.0, 41.0, 49.0, 59.0, 75.0, 80.6, 87.2, 92.4, 94.8, 98.6, 103.1, 115.9, 124.0, 145.0, 250.0, 350.0 MeV; analyzed σ(E, θ) data in the optical model using Nonmonotonic (NM) nucleus-nucleus potentials from energy-density functional (EDF) theory, and for nuclear incompressibility in K=188-266 MeV range.
doi: 10.1103/PhysRevC.91.064613
2013HO02 Phys.Scr. 87, 015201 (2013) S.Hossain, M.N.A.Abdullah, Md.Zulfiker Rahman, A.K.Basak, F.B.Malik Non-monotonic potentials for 6Li elastic scattering at 88 MeV NUCLEAR REACTIONS 24,25,26Mg, 27Al, 40,44Ca, 59Co, 60Ni, 197Au, 206,208Pb(6Li, 6Li), E=88 MeV; analyzed available data, performance of the traditional phenomenological Woods-Saxon (WS) and squared WS potentials with that of a non-monotonic potential; deduced energy density functional, σ(θ). Comparison with available data.
doi: 10.1088/0031-8949/87/01/015201
2013HO16 J.Phys.(London) G40, 105109 (2013) S.Hossain, M.Billah, M.M.B.Azad, F.Parvin, M.N.A.Abdullah, K.M.Hasan, M.A.Uddin, A.S.B.Tariq, A.K.Basak, I.Reichstein, F.B.Malik Non-monotonic potential description of alpha-Zr refractive elastic scattering NUCLEAR REACTIONS 90Zr(α, α), E=15-141.7 MeV; analyzed available data; deduced scattering parameters, σ. Optical model framework using non-monotonic potentials.
doi: 10.1088/0954-3899/40/10/105109
2013UD01 Eur.Phys.J. D 67, 214 (2013) M.A.Uddin, A.K.F.Haque, T.I.Talukder, A.K.Basak, B.C.Saha, F.B.Malik Semi-empirical model for stopping cross sections of p, α and Li ions NUCLEAR REACTIONS Mo, Au(α, X), (p, X), (Li, X), E<100 MeV; calculated stopping σ for Z=2-100; Comparison with available data.
doi: 10.1140/epjd/e2013-40164-8
2012SU04 Int.J.Mod.Phys. E21, 1250003 (2012) The expressions for the super-allowed beta-decay rates in the Coriolis coupling model: Application to the 1d5/2 shell nuclei NUCLEAR STRUCTURE 21Na, 21Ne, 23Mg, 23Na, 25Al, 25Mg, 27Si, 27Al; calculated magnetic dipole and quadrupole moments, energy levels, J, π. Comparison with experimental data. RADIOACTIVITY 21Na, 23Mg, 25Al, 27Si(IT); calculated transition rates, log ft. Coriolis coupling model.
doi: 10.1142/S0218301312500036
2011BA23 Europhys.Lett. 94, 62002 (2011) A.K.Basak, M.M.Billah, M.J.Kobra, M.K.Sarkar, M.Mizanur Rahman, Pretam K.Das, S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, S.Bhattacharjee, I.Reichstein, F.B.Malik Non-monotonic potentials and vector analyzing powers of 6, 7Li scattering by 12C, 26Mg, 58Ni, and 120Sn NUCLEAR REACTIONS 12C, 26Mg, 58Ni(6Li, 6Li), (7Li, 7Li), E=20 MeV; 120Sn(6Li, 6Li), (7Li, 7Li), E=44 MeV; calculated σ, vector analyzing power. Optical model potential, comparison with experimental data.
doi: 10.1209/0295-5075/94/62002
2011SA43 Nucl.Instrum.Methods Phys.Res. B269, 2463 (2011) M.S.Sabra, M.A.Clemens, R.A.Weller, M.H.Mendenhall, A.F.Barghouty, F.B.Malik Validation of nuclear reaction models of 180 MeV proton-induced fragmentation of 27Al NUCLEAR REACTIONS 27Al(p, n), (p, p), (p, α), E=180 MeV; calculated reaction fragments, σ(θ, E), σ(θ), isobaric σ. Binary cascade and cascade exciton models, comparison with experimental data.
doi: 10.1016/j.nimb.2011.07.098
2009HO11 Eur.Phys.J. A 41, 215 (2009) S.Hossain, M.N.A.Abdullah, A.K.Basak, S.K.Das, M.A.Uddin, A.S.B.Tariq, I.Reichstein, K.M.Rusek, F.B.Malik Potential description of 6Li elastic scattering by 28Si NUCLEAR REACTIONS 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 22.8, 25.0, 27.0, 30.0, 34.0, 46.0, 75.6, 99.0, 135.0, 154.0, 210.0, 318.0 MeV; calculated σ(θ) using the energy-density functional formalism with different potentials; deduced parameters for the various potentials.
doi: 10.1140/epja/i2009-10813-7
2008HO15 Europhys.Lett. 84, 52001 (2008) S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, A.K.Basak, K.M.Rusek, I.Reichstein, F.B.Malik Microscopic 6Li-28Si potential from the energy-density functional theory NUCLEAR REACTIONS 28Si(7Li, 7Li), E=7.5-99.0 MeV; analyzed σ(θ).
doi: 10.1209/0295-5075/84/52001
2006AB32 Nucl.Phys. A775, 1 (2006) M.N.A.Abdullah, M.S.Sabra, M.M.Rashid, Z.Shehadeh, M.M.Billah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-alpha potential up to 47.3 MeV bombarding energy NUCLEAR REACTIONS 4He(α, α), E=2.0-47.3 MeV; analysed σ, σ(θ); deduced parameters. 8Be deduced decay width. Various non-monotonic and Woods-Saxon α-nucleus potentials compared, phase shift effects discussed.
doi: 10.1016/j.nuclphysa.2006.06.007
2006HO04 Phys.Lett. B 636, 248 (2006) S.Hossain, M.N.A.Abdullah, K.M.Hasan, M.Asaduzzaman, M.A.R.Akanda, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, F.B.Malik Shallow folding potential for 16O + 12C elastic scattering NUCLEAR REACTIONS 16O(α, α), E=23.2-172.5 MeV; 12C(16O, 16O), E=132.0-260.0 MeV; calculated σ(θ). 12C deduced radius, α-cluster structure. Folding model, comparisons with data.
doi: 10.1016/j.physletb.2006.03.071
2006SA11 Eur.Phys.J. A 27, 167 (2006) M.S.Sabra, Z.F.Shehadeh, F.B.Malik Alpha-induced fragmentation of 28Si in a statistical model NUCLEAR REACTIONS 28Si(α, X), E(cm)=102.7, 173.7, 300, 500, 1000 MeV; calculated fragment-pair spectra, isotopic yields and branching ratios, excitation energies, σ(θ), total reaction σ. Statistical model calculations, comparison with data.
doi: 10.1140/epja/i2005-10253-5
2005AB24 Nucl.Phys. A760, 40 (2005) M.N.A.Abdullah, A.B.Idris, A.S.B.Tariq, M.S.Islam, S.K.Das, M.A.Uddin, A.S.Mondal, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Potentials for the α- 40, 44, 48Ca elastic scattering NUCLEAR REACTIONS 40,44,48Ca(α, α), E=10-180 MeV; analyzed σ(θ); deduced parameters. Non-monotonic and Squared Woods-Saxon α-nucleus potentials compared, dispersion effects discussed.
doi: 10.1016/j.nuclphysa.2005.05.149
2005BI23 Nucl.Phys. A762, 50 (2005) M.M.Billah, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-Ni optical model potentials NUCLEAR REACTIONS 58,60,62,64Ni(α, α), E ≈ 15-166 MeV; calculated σ(θ). Four optical potentials compared with data.
doi: 10.1016/j.nuclphysa.2005.07.020
2005HO12 J.Phys.(London) G31, 309 (2005) S.Hossain, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, I.J.Thompson, F.B.Malik Band mixing in 29Si and 29P NUCLEAR REACTIONS 28Si(α, t), (α, 3He), E=45 MeV; analyzed σ(E, θ). 29P, 29Si deduced configurations, band-mixing effects. Coupled channels approach, finite-range transfer theory, Nilsson model.
doi: 10.1088/0954-3899/31/5/003
2003AB11 J.Phys.(London) G29, 1259 (2003) M.N.A.Abdullah, S.K.Das, A.S.B.Tariq, M.S.Mahbub, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Molecular versus squared Woods-Saxon α-nucleus potentials in the 27Al(α, t)28Si reaction NUCLEAR REACTIONS 27Al(α, t), (α, α), E=64.5 MeV; calculated σ(θ), σ(E, θ). Comparison of Woods-Saxon and molecular potentials, comparison with data.
doi: 10.1088/0954-3899/29/6/323
2003AB22 Phys.Lett. B 571, 45 (2003) M.N.A.Abdullah, M.S.I.Sarker, S.Hossain, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 40, 44, 48Ca NUCLEAR REACTIONS 40,44,48Ca(α, α), E=22-166 MeV; analyzed σ(θ); deduced parameters. 40,44,48Ca deduced α-cluster structure. Folded potential.
doi: 10.1016/j.physletb.2003.08.014
2003AB24 Eur.Phys.J. A 18, 65 (2003) M.N.A.Abdullah, S.Hossain, M.S.I.Sarker, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 16O NUCLEAR REACTIONS 16O(α, α), E=25.4-146.0 MeV; calculated σ(θ). 16O deduced radius. Folding model, α-cluster configurations, comparisons with data.
doi: 10.1140/epja/i2003-10068-7
2002AB22 Eur.Phys.J. A 15, 477 (2002) M.N.A.Abdullah, M.S.Mahbub, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Investigation of α-nucleus interaction in the 27Al(α, α)27Al scattering and 27Al(α, d)29Si reaction NUCLEAR REACTIONS 27Al(α, α), E=22.3-64.5 MeV; analyzed σ(θ); deduced potential parameters. 27Al(α, d), E=26.5, 27.2 MeV; calculated spectroscopic factors, σ(θ). Molecular and Michel potentials, DWBA.
doi: 10.1140/epja/i2002-10066-0
2001BB08 Eur.Phys.J. A 12, 387 (2001) A.K.Basak, M.N.A.Abdullah, A.S.B.Tariq, S.K.Das, A.F.M.M.Rahman, A.S.Mondal, H.M.Sen Gupta, F.B.Malik Investigation of Inelastic α-Scattering on 24Mg and 28Si NUCLEAR REACTIONS 24Mg(α, α'), E=54 MeV; 28Si(α, α'), E=26 MeV; measured σ(E, θ); deduced potential parameters. Coupled channels analysis.
doi: 10.1007/s10050-001-8662-4
2001DA19 Phys.Rev. C64, 034605 (2001) S.K.Das, A.S.B.Tariq, A.F.M.M.Rahman, S.Hossain, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Interaction on the 29, 30Si(α, d)31, 32P Reaction NUCLEAR REACTIONS 29,30Si(α, d), E=25 MeV; calculated σ(E, θ), spectroscopic factors. Microscopic and macroscopic DWBA calculations, comparison of molecular, standard and squared Woods-Saxon α-nucleus potentials.
doi: 10.1103/PhysRevC.64.034605
2000DA28 Phys.Rev. C62, 054605 (2000) S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, K.M.Rashid, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 28Si(α, d)30P Reaction NUCLEAR REACTIONS 28Si(α, d), E=26 MeV; analyzed σ(E, θ). 30P level deduced J, π. DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054605
2000DA29 Phys.Rev. C62, 054606 (2000) S.K.Das, A.K.Basak, K.Banu, A.S.Mondal, A.S.B.Tariq, A.F.M.M.Rahman, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Potential on the 28Si(α, p)31P Reaction NUCLEAR REACTIONS 28Si(α, α), (α, p), E=26 MeV; analyzed σ(E, θ). DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054606
1999DA20 Phys.Rev. C60, 044617 (1999); Comment Phys.Rev. C62, 049801 (2000) S.K.Das, A.S.B.Tariq, A.F.M.Rahman, R.K.Roy, M.N.Huda, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 27Al(α, t)28Si Reaction NUCLEAR REACTIONS 27Al(α, α), E=64.5 MeV; analyzed σ(θ); deduced parameters. 27Al(α, t), E=64.5 MeV; calculated σ(E, θ). 28Si deduced spectroscopic factors. Finite-range DWBA, molecular and Michel optical potentials. Comparisons with data.
doi: 10.1103/PhysRevC.60.044617
1999SH09 Phys.Rev. C59, 826 (1999) Z.F.Shehadeh, M.M.Alam, F.B.Malik Inverse-Scattering Theory at a Fixed Energy for the Klein-Gordon Equation
doi: 10.1103/PhysRevC.59.826
1999TA13 Phys.Rev. C59, 2558 (1999) A.S.B.Tariq, A.F.M.M.Rahman, S.K.Das, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Potential Description of Anomalous Large Angle Scattering of α Particles NUCLEAR REACTIONS 28Si(α, α), E=14.47-45 MeV; 30Si(α, α), E=26.6 MeV; 24Mg(α, α), E=22-120 MeV; analyzed σ(θ); deduced potential parameters. Michel, molecular potentials, anomalous large angle scattering.
doi: 10.1103/PhysRevC.59.2558
1991AL03 Nucl.Phys. A524, 88 (1991) An Inverse Scattering Method for Identical Particles NUCLEAR REACTIONS 12C(12C, 12C), E=40 MeV; 16O(16O, 16O), E=20 MeV; analyzed data; deduced model parameters. Inverse scattering method.
doi: 10.1016/0375-9474(91)90017-Z
1990AL05 Phys.Lett. 237B, 14 (1990) Nature of the α-12C Potential at Low Energy Using an Inverse Scattering Method NUCLEAR REACTIONS 12C(α, α), E=4.86-6.46 MeV; calculated σ(θ), phase shifts; deduced model parameters. Inverse scattering method.
doi: 10.1016/0370-2693(90)90452-C
1990SU11 Can.J.Phys. 68, 227 (1990) A Note on the Determination of the Nuclear Charge Density Radius from the β Decay between Mirror Nuclei RADIOACTIVITY A ≤ 45; analyzed maxium Eβ+, β+-decay; deduced nuclear charge density radius, surface thickness. Trapezoidal distribution.
doi: 10.1139/p90-033
1989BR29 Nucl.Phys. A504, 49 (1989) A.Bredbacka, M.Brenner, F.B.Malik Level Spectra, Electromagnetic Moments and Transition Rates and Spectroscopic Factors for Odd Rhodium Isotopes in the Coriolis Coupling Model NUCLEAR STRUCTURE 97,99,101,103,105,107,109Rh; calculated levels, μ, quadrupole moments, B(λ). Coriolis coupling model.
doi: 10.1016/0375-9474(89)90282-0
1989GR29 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2220 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.11, 168 (1989) K.A.Gridnev, P.B.Danilov, V.B.Subbotin, F.B.Malik Internuclear Potentials in the Method of the Energy-Density Functional NUCLEAR STRUCTURE 40Ca; calculated proton density, binding energy, rms radius vs density. Energy density functional method, Thomas-Fermi model. NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E not given; calculated ion-ion potential vs internuclear distance. Energy density functional method, Thomas-Fermi model.
1989MA50 Nucl.Phys. A504, 130 (1989) P.Manngard, M.Brenner, M.M.Alam, I.Reichstein, F.B.Malik Molecular Potential and Elastic Scattering of Alpha Particles by 28Si from 14 to 28 MeV NUCLEAR REACTIONS 28Si(α, α), E=14.47 MeV; measured σ(θ). Energy density formalism, molecular potential, other data analyzed.
doi: 10.1016/0375-9474(89)90286-8
1987OH02 Nucl.Phys. A465, 550 (1987) N.Ohtsuka, R.Linden, A.Faessler, F.B.Malik Real and Imaginary Parts of the Microscopic Optical Potential between Nuclei in the Sudden and Adiabatic Approximation and Its Application to Medium Energy 12C - 12C Scattering NUCLEAR REACTIONS 12C(12C, 12C), 16O(16O, 16O), 40Ca(40Ca, 40Ca), 208Pb(208Pb, 208Pb), E=0.0, ≤4.313 GeV; calculated potential parameter internucleus distance dependence. 12C(12C, 12C), (12C, 12C'), (12C, X), E=300, 306, 1016 MeV; calculated σ(θ), reaction, inelastic σ(E). Sudden, adiabatic approximations. NUCLEAR STRUCTURE 12C, 16O, 40Ca, 208Pb; calculated rms radius, binding energy per nucleon. Realistic two-nucleon interactions.
doi: 10.1016/0375-9474(87)90364-2
1987RE08 Phys.Lett. 192B, 35 (1987) On the Pocket in the 238U-238U and 238U-248Cm Potential-Energy Surfaces NUCLEAR REACTIONS 238U, 248Cm(238U, 238U), E not given; calculated potential energy surfaces. Sudden approximation.
doi: 10.1016/0370-2693(87)91137-3
1987WA01 J.Phys.(London) G13, 37 (1987) Level Spectrum of 50Ti in the Rotational-Particle Coupling Model NUCLEAR STRUCTURE 50Ti; calculated levels. Rotational particle coupling model.
doi: 10.1088/0305-4616/13/1/007
1986HA13 J.Phys.(London) G12, 537 (1986) Barrier Penetration Calculation of Heavy-Ion Fusion Cross Sections in the Above- and Sub-Barrier Regions NUCLEAR REACTIONS, ICPND 9Be, 11B, 12,13C, 14,15N, 16,17,18O, 19F, 20Ne, 24Mg(12C, X), E=10-30 MeV; 24Mg(18O, X), 27Al, 28,30Si(19F, X), 40Ca(16O, X), E ≈ 20-40 MeV; calculated fusion σ(E); deduced model parameters. Barrier penetration model.
doi: 10.1088/0305-4616/12/6/012
1984HA53 At.Data Nucl.Data Tables 31, 185 (1984) Heavy-Ion Fusion Cross-Section Data for Systems with Compound Atomic Mass between 18 and 80 COMPILATION A=18-80; compiled fusion reaction data leading to compound nuclei in mass range.
doi: 10.1016/0092-640X(84)90022-6
1983HA39 Phys.Rev. C28, 2328 (1983) Theory for Structures in the Fusion Cross Sections and an Application to 12C + 28,29,30Si NUCLEAR REACTIONS, ICPND 28,29,30Si(12C, X), E(cm)=15-35 MeV; calculated fusion σ(E). 40,41,42Ca deduced resonance parameters. Bound states embedded in continuum, S-matrix approach.
doi: 10.1103/PhysRevC.28.2328
1982CO17 J.Phys.(London) G8, 1447 (1982) A Statistical-Model Calculation of Proton-Induced Binary Fragmentation of 16O NUCLEAR REACTIONS, ICPND 16O(p, n), (p, 8Be), (p, 3He), (p, α), (p, 5Li), (p, 8B), (p, 6Be), (p, 6Li), (p, 7Be), (p, 7Li), E=33.7, 37.9, 41.9 MeV; calculated fragmentation σ(θ), total σ, compound nuclear decay widths. Statistical model.
doi: 10.1088/0305-4616/8/10/014
1982HA29 Phys.Rev. C26, 162 (1982) Heavy-Ion Fusion using a Parabolic Barrier with Coulomb Interaction NUCLEAR REACTIONS, ICPND 16O, 24,26Mg, 28,29,30Si(16O, X), E(cm)=15-40 MeV; 28,29,30Si(12C, X), E(cm)=15-40 MeV; 40Ca(40Ca, X), E(cm)=50-100 MeV; calculated fusion σ vs E. Coulomb, parabolic barriers, appropriate boundary conditions.
doi: 10.1103/PhysRevC.26.162
1982HA42 Phys.Rev. C26, 989 (1982) Fusion between Heavy Ions at Sub-Barrier Energies NUCLEAR REACTIONS 16O, 14N, 12C(16O, X), 14N(14N, X), 14N, 10,11B(12C, X), E=sub-barrier; calculated capture process S-factor. Continuous potential surface, proper boundary conditions, asymptotic wave functions.
doi: 10.1103/PhysRevC.26.989
1981HA47 J.Phys.(London) G7, 1661 (1981) An Ananlysis of 12C + 12C Elastic Scattering Data using a Molecular Potential NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=13-62 MeV; analyzed σ(E, θ=90°). Complex molecular potential.
doi: 10.1088/0305-4616/7/12/015
1976RE09 Ann.Phys. (New York) 98, 322 (1976) Potential Energy Surfaces and Lifetimes for Spontaneous Fission of Heavy and Superheavy Elements from a Variable Density Dependent Mass Formula NUCLEAR STRUCTURE, Fission 234,236U, 240Pu, 244Cm, 248,252Cf(SF); calculated potential energy, T1/2.
doi: 10.1016/0003-4916(76)90157-3
1975HO04 Phys.Lett. 55B, 144 (1975) Charge Distribution and Average Masses in the Spontaneous and Isomeric Fission of 234U, 236U and 240Pu RADIOACTIVITY, Fission 234,236U(SF), 240Pu(SF); calculated fission yields.
doi: 10.1016/0370-2693(75)90427-X
1974HO04 Helv.Phys.Acta 46, 720 (1974) Total Spontaneous Fission Half-Life, Mass and Charge Distribution of 252Cf RADIOACTIVITY, Fission 252Cf(SF); calculated T1/2, mass, charge distribution.
1974HO05 Helv.Phys.Acta 46, 724 (1974) Total Spontaneous Fission Half-Lives, Kinetic Energy and Mass Yield Spectra of 250Cm, 254Cf and 258Fm RADIOACTIVITY, Fission 250Cm, 254Cf, 258Fm(SF); calculated T1/2, kinetic energy, mass yield.
1972AL46 Phys.Lett. 42B, 412 (1972) A Microscopic Calculation of the Imaginary Potential in Heavy-Nucleus Scattering
doi: 10.1016/0370-2693(72)90094-9
1972HI12 Helv.Phys.Acta 45, 738 (1972) A Note on the Alpha-Decay Half-Lives of Heavy and Superheavy Elements RADIOACTIVITY Z=112, 114, 126; calculated T1/2(α).
1972HO11 Phys.Lett. 38B, 495 (1972) Total Spontaneous and Isomer Fission Half-Lives of 234U, 236U and 240Pu NUCLEAR STRUCTURE, Fission 234,236U, 240Pu(SF); calculated total T1/2, T1/2(SF), average fragment kinetic energies. Coupled-channel decay theory.
doi: 10.1016/0370-2693(72)90525-4
1972HO48 Helv.Phys.Acta 45, 567 (1972) A Coupled Channel Approach to the Isomer Fission State
1971CO03 Nucl.Phys. A160, 385 (1971) J.R.Comfort, P.Wasielewski, F.B.Malik, W.Scholz Properties of 55Mn, 56Mn and 57Fe in the Unified Rotational Model NUCLEAR STRUCTURE 55,56Mn, 57Fe; calculated levels, T1/2, μ, quadrupole moment, γ-mixing, B(λ). Unified rotational model.
doi: 10.1016/0375-9474(71)90139-4
1971LU12 Nucl.Phys. A175, 289 (1971) C.C.Lu, F.B.Malik, T.A.Carlson Calculation of the K X-Ray Intensities for Elements from Z = 92 to 126 ATOMIC PHYSICS Z=92-126; calculated I(K X-ray).
doi: 10.1016/0375-9474(71)90283-1
1971LU14 At.Data 3, 1 (1971) C.C.Lu, T.A.Carlson, F.B.Malik, T.C.Tucker, C.W.Nestor, Jr. Relativistic Hartree-Fock-Slater Eigenvalues, Radial Expectation Values, and Potentials for Atoms, 2 < Z < 126
doi: 10.1016/S0092-640X(71)80002-5
1971RE21 Phys.Lett. 37B, 344 (1971) Dependence of 16O-16O Potential on the Density Ansatz NUCLEAR REACTIONS 16O(16O, X), E not given; analyzed 16O-16O interaction potential.
doi: 10.1016/0370-2693(71)90197-3
1971WA01 Nucl.Phys. A160, 113 (1971) Application of the Unified Model with Coriolis Coupling to 22Na, 26Al and 30P NUCLEAR STRUCTURE 22Na, 26Al, 30P; calculated levels, μ, quadrupole moment, B(λ), γ-mixing. Unified model, Coriolis coupling.
doi: 10.1016/0375-9474(70)90177-6
1970MU20 Phys.Rev. C2, 2068 (1970) Evidence of E2 and M1 Transitions in High-Energy Photonuclear Reactions in O16 NUCLEAR REACTIONS 16O(γ, n), (γ, p), E=20-50 MeV; calculated σ(E;θ), P; deduced E2, M1 transition interference.
doi: 10.1103/PhysRevC.2.2068
1969CA10 Nucl.Phys. A135, 57 (1969) T.A.Carlson, C.W.Nestor, Jr., F.B.Malik, T.C.Tucker Calculation of K, L, M and N Binding Energies and K X-Rays for Elements From Z = 96-120
doi: 10.1016/0375-9474(69)90147-X
1969TU02 Phys.Rev. 178, 998 (1969) T.C.Tucker, L.D.Roberts, C.W.Nestor, Jr., T.A.Carlson, F.B.Malik Relativistic Self-Consistent-Field Calculation of the Wave Functions, Eigenvalues, Isotope Shifts, and the 6S Hyperfine-Structure Coupling Constant as a Function of Pressure for Metallic Gold in the Wigner-Seitz Model ATOMIC PHYSICS Au; calculated wave functions, eigenvalues, isotope shift , hfs coupling constant.
doi: 10.1103/PhysRev.178.998
1968CA29 Phys.Rev. 169, 27 (1968) T.A.Carlson, C.W.Nestor, Jr., T.C.Tucker, F.B.Malik Calculation of Electron Shake-Off for Elements from Z = 2 to 92 with the Use of Self-Consistent-Field Wave Functions ATOMIC PHYSICS Z=2-92; calculated electron shake-off.
doi: 10.1103/PhysRev.169.27
1968SC20 Phys.Rev. 176, 1355(1968) Level Spectra of Odd Isotopes of Ga, As, Br, and Rb in the Coriolis Coupling Model with a Residual Interaction of the Pairing Type NUCLEAR STRUCTURE Ga, As, Br, Rb. calculated levels of odd isotopes. Coriolis coupling model.
doi: 10.1103/PhysRev.176.1355
1968TU03 Phys.Rev. 174, 118 (1968) T.C.Tucker, L.D.Roberts, C.W.Nestor, Jr., T.A.Carlson, F.B.Malik Calculation of the Electron Binding Energies and X-Ray Energies for the Superheavy Elements 114, 126, and 140 Using Relativistic Self-Consistent-Field Atomic Wave Functions ATOMIC PHYSICS Au, U; Z=114, 116, 140; calculated electron binding energies, X-ray energies.
doi: 10.1103/PhysRev.174.118
1967SC06 Phys.Rev. 153, 1071 (1967) Coriolis-Coupling Model Prediction of Moments and Transition Rates for Deformed Odd Nuclei in the 1f7/2 Shell
doi: 10.1103/PhysRev.153.1071
1966MA32 Phys.Rev. 150, 919 (1966) Level Spectra of Odd-Even 1f7/2-Shell Nuclei in the Coriolis Coupling Model
doi: 10.1103/PhysRev.150.919
1966NE10 ORNL-4027 (1966) C.W.Nestor, T.C.Tucker, T.A.Carlson, L.D.Roberts, F.B.Malik, C.Froese Relativistic and Non-Relativistic scf Wave Functions for Atoms and Ions from Z = 2 to 80, Together with Calculations of Binding Energies, Mean Radii, Screening Constants, Charge Distributions, and Electron Shake-Off Probabilities
1966SC10 Phys.Rev. 147, 836 (1966) Evidence of Deformation in V51 NUCLEAR STRUCTURE 51V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.147.836
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