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NSR database version of May 24, 2024.

Search: Author = F.B.Malik

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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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2012SU04      Int.J.Mod.Phys. E21, 1250003 (2012)

M.Sultan Parvez, F.B.Malik

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
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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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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1991AL03      Nucl.Phys. A524, 88 (1991)

M.M.Alam, F.B.Malik

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
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1990AL05      Phys.Lett. 237B, 14 (1990)

M.M.Alam, F.B.Malik

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
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1990SU11      Can.J.Phys. 68, 227 (1990)

M.Sultan Parvez, F.B.Malik

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0653.

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
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1987RE08      Phys.Lett. 192B, 35 (1987)

I.Reichstein, F.B.Malik

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
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1987WA01      J.Phys.(London) G13, 37 (1987)

Y.Wang, F.B.Malik

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
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1986HA13      J.Phys.(London) G12, 537 (1986)

Q.Haider, F.B.Malik

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
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1984HA53      At.Data Nucl.Data Tables 31, 185 (1984)

Q.Haider, F.B.Malik

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
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1983HA39      Phys.Rev. C28, 2328 (1983)

Q.Haider, F.B.Malik

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
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1982CO17      J.Phys.(London) G8, 1447 (1982)

B.Compani-Tabrizi, F.B.Malik

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
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1982HA29      Phys.Rev. C26, 162 (1982)

Q.Haider, F.B.Malik

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
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1982HA42      Phys.Rev. C26, 989 (1982)

Q.Haider, F.B.Malik

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
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1981HA47      J.Phys.(London) G7, 1661 (1981)

Q.Haider, F.B.Malik

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
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1976RE09      Ann.Phys. (New York) 98, 322 (1976)

I.Reichstein, F.B.Malik

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
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1975HO04      Phys.Lett. 55B, 144 (1975)

M.A.Hooshyar, F.B.Malik

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
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1974HO04      Helv.Phys.Acta 46, 720 (1974)

M.A.Hooshyar, F.B.Malik

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)

M.A.Hooshyar, F.B.Malik

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)

D.R.Alexander, F.B.Malik

A Microscopic Calculation of the Imaginary Potential in Heavy-Nucleus Scattering

doi: 10.1016/0370-2693(72)90094-9
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1972HI12      Helv.Phys.Acta 45, 738 (1972)

M.D.High, R.Malmin, F.B.Malik

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)

M.A.Hooshyar, F.B.Malik

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
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1972HO48      Helv.Phys.Acta 45, 567 (1972)

M.A.Hooshyar, F.B.Malik

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

1971RE21      Phys.Lett. 37B, 344 (1971)

I.Reichstein, F.B.Malik

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
Citations: PlumX Metrics

1971WA01      Nucl.Phys. A160, 113 (1971)

P.Wasielewski, F.B.Malik

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
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1970MU20      Phys.Rev. C2, 2068 (1970)

M.G.Mustafa, F.B.Malik

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
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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
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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
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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
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1968SC20      Phys.Rev. 176, 1355(1968)

W.Scholz, F.B.Malik

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
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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
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1967SC06      Phys.Rev. 153, 1071 (1967)

W.Scholz, F.B.Malik

Coriolis-Coupling Model Prediction of Moments and Transition Rates for Deformed Odd Nuclei in the 1f7/2 Shell

doi: 10.1103/PhysRev.153.1071
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1966MA32      Phys.Rev. 150, 919 (1966)

F.B.Malik, W.Scholz

Level Spectra of Odd-Even 1f7/2-Shell Nuclei in the Coriolis Coupling Model

doi: 10.1103/PhysRev.150.919
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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)

W.Scholz, F.B.Malik

Evidence of Deformation in V51

NUCLEAR STRUCTURE 51V; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.147.836
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