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NSR database version of May 19, 2024.

Search: Author = S.A.Khan

Found 18 matches.

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2023KH04      Nucl.Phys. A1034, 122643 (2023)

S.A.Khan, M.Hasan, B.K.Patra

Heavy quarkonia in a baryon asymmetric strongly magnetized hot quark matter

doi: 10.1016/j.nuclphysa.2023.122643
Citations: PlumX Metrics

2020KH02      Nucl.Phys. A994, 121656 (2020)

S.A.Khan, J.A.Siddiqui, K.Ali

Modified projection operator methods and potential applied to light ions

doi: 10.1016/j.nuclphysa.2019.121656
Citations: PlumX Metrics

2017KH09      Int.J.Mod.Phys. E26, 1750029 (2017)

S.A.Khan, H.Rasheed, K.Ali

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2000KH15      Eur.Phys.J. A 7, 583 (2000)

S.A.Khan, M.Pusterla

Quantum-Like Approach to the Transversal and Longitudinal Beam Dynamics. The Halo Problem

doi: 10.1007/s100500050430
Citations: PlumX Metrics

1990KH05      Phys.Rev. C42, 1768 (1990)

S.A.Khan, W.P.Beres

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
Citations: PlumX Metrics

1989KH02      Phys.Rev. C39, 897 (1989)

S.A.Khan, W.P.Beres

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
Citations: PlumX Metrics

1988KH07      Phys.Rev. C37, 2515 (1988)

S.A.Khan, W.P.Beres

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
Citations: PlumX Metrics

1988KH09      Phys.Rev. C38, 1488 (1988)

S.A.Khan, W.P.Beres

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
Citations: PlumX Metrics

1986KH04      Phys.Rev. C33, 2028 (1986)

S.A.Khan, W.P.Beres

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
Citations: PlumX Metrics

1985KH05      Phys.Rev. C32, 871 (1985)

S.A.Khan, W.P.Beres

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
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1981SI03      Phys.Rev. C23, 1174 (1981)

S.K.Singh, S.A.Khan

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
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1981SI04      Z.Phys. A299, 337 (1981)

S.K.Singh, S.A.Khan

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
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1980SI11      Nucl.Phys. A340, 307 (1980)

S.K.Singh, S.A.Khan

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
Citations: PlumX Metrics

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