NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.A.Khan Found 18 matches. 2023KH04 Nucl.Phys. A1034, 122643 (2023) Heavy quarkonia in a baryon asymmetric strongly magnetized hot quark matter
doi: 10.1016/j.nuclphysa.2023.122643
2020KH02 Nucl.Phys. A994, 121656 (2020) Modified projection operator methods and potential applied to light ions
doi: 10.1016/j.nuclphysa.2019.121656
2017KH09 Int.J.Mod.Phys. E26, 1750029 (2017) Quasimolecular nuclear potential and its application to 12C+16O reaction near and above the Coulomb barrier NUCLEAR REACTIONS 16O(12C, X), E(cm)=12-20 MeV; calculated σ, resonance energies, S-factor.
doi: 10.1142/S021830131750029X
2011JA11 J.Korean Phys.Soc. 59, 1361s (2011) V.Jagannathan, U.Pal, R.Karthikeyan, A.Srivastava, S.A.Khan Sensitivity to Nuclear Data Libraries in the Physics Core Characteristics of Conceptual Thorium Breeders
doi: 10.3938/jkps.59.1361
2011KH09 J.Korean Phys.Soc. 59, 1073s (2011) S.A.Khan, V.Jagannathan, U.Pal, R.Karthikeyan, A.Srivastava Need for High Temperature Nuclear Data Library for LWR Design Computations
doi: 10.3938/jkps.59.1073
2010KH01 Chin.J.Phys.(Taiwan) 48, 186 (2010) S.A.Khan, M.Z.M.Jafri, K.L.Low α Decay of Superheavy Nuclei Using the Projection Operator Method NUCLEAR STRUCTURE 271Sg, 275Hs, 279Ds, 283,285Cn, 286,287,288,289Fl, 290,291,292,293Lv, 294Og; calculated spectroscopic factors, lifetimes, reduced widths; deduced density distributions in superheavy nuclei. Comparison with experimental data.
2005KH11 Int.J.Mod.Phys. E14, 269 (2005) IWBC analysis with quasimolecular optical potentials NUCLEAR REACTIONS 12C(12C, X), E=1-9 MeV; 16O(16O, X), E=5-12 MeV; calculated fusion σ.12C(12C, 12C), E=8-28 MeV; 16O(16O, 16O), E=17-35 MeV; calculated elastic σ(θ=90°). Quasimolecular potentials, incoming wave boundary condition method.
doi: 10.1142/S0218301305003028
2004KH17 Int.J.Mod.Phys. E13, 1217 (2004) Projection operator treatment for sub-Coulomb widths RADIOACTIVITY 144Nd, 148Sm, 152Gd, 208Pb, 212Po, 232Th, 238U(α); calculated reduced widths, spectroscopic factors. Comparison with data.
doi: 10.1142/S0218301304002624
2000KH15 Eur.Phys.J. A 7, 583 (2000) Quantum-Like Approach to the Transversal and Longitudinal Beam Dynamics. The Halo Problem
doi: 10.1007/s100500050430
1990KH05 Phys.Rev. C42, 1768 (1990) Semistatistical Model for 12C + 12C Reaction Cross Sections Below the Coulomb Barrier NUCLEAR REACTIONS, ICPND 12C(12C, α), (12C, p), (12C, n), E < Coulomb barrier; calculated σ(E). Semi-statistical model.
doi: 10.1103/PhysRevC.42.1768
1989KH02 Phys.Rev. C39, 897 (1989) 12C + 12C Structure Factor at Sub-Coulomb Energies NUCLEAR REACTIONS 12C(12C, X), E < 6 MeV; calculated modified structure factor.
doi: 10.1103/PhysRevC.39.897
1988KH07 Phys.Rev. C37, 2515 (1988) Projection Operator Model for Heavy-Ion Resonance Parameters below the Coulomb Barrier and Its Application to 12C + 12C NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=2.91-6 MeV; calculated intermediate resonances, Γ. Generalized doorway formalism.
doi: 10.1103/PhysRevC.37.2515
1988KH09 Phys.Rev. C38, 1488 (1988) Perturbative Treatment of Imaginary Potential in 12C + 12C NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=3.8-6 MeV; calculated L=2 phase shifts; deduced exact, approximate estimates comparison. Perturbative treatment.
doi: 10.1103/PhysRevC.38.1488
1986KH04 Phys.Rev. C33, 2028 (1986) Projection Operator Method for Resonances in Repulsive Core Potentials NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=5.8-7 MeV; calculated l=0-8 resonance energies, widths. 24Mg deduced resonances, Γ. Projection operators, comparison to phase shift analysis.
doi: 10.1103/PhysRevC.33.2028
1985KH05 Phys.Rev. C32, 871 (1985) 28Si + 28Si Elastic Scattering in the Doorway Model NUCLEAR REACTIONS 28Si(28Si, 28Si), E=100-200 MeV; analyzed σ(θ). 56Ni deduced doorway structure. Projection operator method, projectile, target excitation, sudden approximation.
doi: 10.1103/PhysRevC.32.871
1981SI03 Phys.Rev. C23, 1174 (1981) ν(ν-bar) + d → ν(ν-bar) + n + p at Intermediate Energies NUCLEAR REACTIONS 2H(ν, ν), (ν-bar, ν-bar), E=50-500 MeV; calculated deuteron disintegration σ(E). Helicity conserving, helicity flipping theories, neutral currents, closure approximation.
doi: 10.1103/PhysRevC.23.1174
1981SI04 Z.Phys. A299, 337 (1981) ν(bar)(e)+d → ν(bar)(e)+n+p at Reactor Energies NUCLEAR REACTIONS 2H(ν-bar, nν-bar), E=2.5-12 MeV; calculated σ(E). Helicity conserving, flipping, final state interaction.
doi: 10.1007/BF01441276
1980SI11 Nucl.Phys. A340, 307 (1980) Asymmetry in Polarized e-d Inelastic Scattering NUCLEAR REACTIONS 2H(polarized e, e'), E=200, 400, 600, 800, 1000 MeV; calculated asymmetry vs θ. Impulse approximation, parity violating effects.
doi: 10.1016/0375-9474(80)90277-8
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