NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = Z.Khan Found 23 matches. 2022NA41 Phys.Scr. 97, 125302 (2022) Investigation of β-decay properties of neutron-rich Cerium isotopes RADIOACTIVITY 120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137Ce(β+), 138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157Ce(β-); calculated centroid and total Gamow-Teller (GT) strength values of the GT strength within the proton-neutron quasiparticle random phase approximation (pn-QRPA) approach. Comparison with available data.
doi: 10.1088/1402-4896/ac9be7
2017AH03 Phys.Rev. C 95, 054601 (2017) S.Ahmad, A.A.Usmani, S.Ahmad, Z.A.Khan Interaction cross sections and matter radii of oxygen isotopes using the Glauber model NUCLEAR STRUCTURE 16,18,20,22,24,26O; calculated point proton and neutron density distributions, oscillator parameters, matter rms radii using Slater determinants consisting of the harmonic oscillator single-particle wave functions (SDHO) and relativistic mean-field approach (RMF). NUCLEAR REACTIONS 12C(16O, X), (18O, X), (20O, X), (22O, X), (24O, X), (26O, X), E=1.0 GeV/nucleon; calculated interaction σ. 16O(p, p), E=200, 300, 600, 1000 MeV; calculated σ(θ, E). 16O(p, X), E=40-1000 MeV; calculated reaction σ(E). Coulomb modified correlation expansion for Glauber model S matrix, and densities from the Slater determinants consisting of the harmonic oscillator single-particle wave functions (SDHO) and relativistic mean field (RMF) approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.054601
2017AH08 Phys.Rev. C 96, 064602 (2017) Matter radii of light proton-rich and neutron-rich nuclear isotopes NUCLEAR REACTIONS 1H(α, α), E=650, 850 MeV; 1H(16O, 16O'), E=1000 MeV; analyzed experimental differential σ(θ) data. 12C(α, X), (6He, X), (8He, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (14Be, X), (12B, X), (13B, X), (14B, X), (15B, X), E=790 MeV; 12C(10B, X), (13C, X), (16C, X), (19C, X), E=960 MeV; 12C(11B, X), (12C, X), (20Ne, X), (20O, X), (20F, X), (26F, X), (20Ne, X), (21Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (28Ne, X), (29Ne, X), (22Na, X), (23Na, X), (25Na, X), (26Na, X), (27Na, X), (28Na, X), (29Na, X), (30Na, X), (31Na, X), (32Na, X), (24Mg, X), (25Mg, X), (27Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), E=950 MeV; 12C(17B, X), (19B, X), E=800 MeV; 12C(14C, X), (17C, X), (14N, X), (22N, X), (22O, X), (24F, X), E=965 MeV; 12C(15C, X), (17N, X), E=740 MeV; 12C(18C, X), E=955 MeV; 12C(20C, X), E=905 MeV; 12C(15N, X), (18F, X), E=975 MeV; 12C(16N, X), (18N, X), (23F, X), E=1020 MeV; 12C(19N, X), (21N, X), (24F, X), E=1005 MeV; 12C(23N, X), E=920 MeV; 12C(16O, X), (17O, X), (19O, X), E=970 MeV; 12C(18O, X), E=1050 MeV; 12C(21O, X), E=980 MeV; 12C(19F, X), E=985 MeV; 12C(21F, X), E=1000 MeV; 12C(25F, X), E=1010 MeV; calculated oscillator constants, proton and neutron rms radii, proton and neutron density distributions; predicted experimental cross sections of stable and neutron-rich nuclei on 12C. 4,6,8He, 6,7,8,9,11Li, 9,10,11,12,13,14Be, 10,11,12,13,14,15,16,17,19B, 12,13,14,15,16,17,18,19,20C, 14,15,16,17,18,19,20,21,22,23N, 16,17,18,19,20,21,22,23,24O, 18,19,20,21,23,24,25,26F, 20,21,23,24,25,26,28,29Ne, 22,23,25,27,28,29,30,31,32Na, 24,25,27,29,30,31,32Mg; extracted matter rms radii of neutron-rich nuclei, and compared with other theoretical approaches. 3He, 7Be, 8B, 9,10,11C, 12,13N, 13,14,15O, 17F, 17,18,19Ne, 19,20,21Na, 20,22,23Mg; extracted matter rms radii of proton-rich nuclei, and compared with other calculations. Glauber model.
doi: 10.1103/PhysRevC.96.064602
2016AH01 Eur.Phys.J. A 52, 128 (2016) S.Ahmad, D.Chauhan, A.A.Usmani, Z.A.Khan Study of the neon interaction cross section using the Glauber model NUCLEAR REACTIONS 12C(17Ne, x), (18Ne, x), (19Ne, x), (20Ne, x), (21Ne, x), (22Ne, x), (23Ne, x), (24Ne, x), (25Ne, x), (26Ne, x), (27Ne, x), (28Ne, x), (29Ne, x), (30Ne, x), (31Ne, x), (32Ne, x), E=240 MeV/nucleon; calculated Ne harmonic oscillator parameters, neutron and proton rms radii, interaction σ, 1n removal σ using Glauber model S-matrix. Compared to available data. 31Ne deduced neutron halo.
doi: 10.1140/epja/i2016-16128-8
2014CH39 Phys.Rev. C 90, 024603 (2014) D.Chauhan, Z.A.Khan, A.A.Usmani Interaction cross sections for neon isotopes in the Glauber model and the halo structure of 31Ne NUCLEAR REACTIONS 12C(17Ne, X), (18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), E=240, 950 MeV/nucleon; calculated interaction cross sections with and without the two-body density term. Halo structure. Coulomb-modified correlation expansion for the Glauber model S matrix. Comparison with experimental data. NUCLEAR STRUCTURE 17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32Ne; calculated point-proton and neutron RMF density distributions, neutron, proton, and matter radii.
doi: 10.1103/PhysRevC.90.024603
2013KH18 Int.J.Mod.Phys. E22, 1350082 (2013) Analysis of p-4, 6, 8He and p-6, 9, 11Li scattering NUCLEAR REACTIONS 4,6,8He, 6,9,11Li(p, p), E=60, 72 MeV; analyzed available data; calculated σ(θ), polarization. Coulomb modified Glauber model, comparison with available data.
doi: 10.1142/S0218301313500821
2012CH27 Phys.Rev. C 85, 067602 (2012) K+-nucleus elastic scattering at intermediate energies NUCLEAR REACTIONS 12C, 40Ca(K+, K+), E at 635, 715, 800 MeV/c; analyzed K+N phase shifts; elastic σ(θ), reaction cross sections. Coulomb modified Glauber model.
doi: 10.1103/PhysRevC.85.067602
2011CH11 Eur.Phys.J. A 47, 31 (2011) Analysis of the 3He -nucleus total reaction cross-section NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(3He, X), E=96.4, 137.8, 167.3 MeV; calculated, analyzed total σ using realistic form factors and parameterization of basic NN amplitude; deduced parameters of NN interaction. 12C, 58Ni(α, α), E=172.5 MeV; 12C, 58Ni(3He, 3He), E=132 MeV; calculated σ(θ); deduced parameters of NN interaction. 1H(p, p), (n, n), E=43, 44 MeV; calculated σ(θ). Comparison with available data.
doi: 10.1140/epja/i2011-11031-6
2011SH10 Phys.Rev. C 83, 031601 (2011) M.Sharma, A.Bhagwat, Z.A.Khan, W.Haider, Y.K.Gambhir Neutron density distribution and the halo structure of 22C NUCLEAR REACTIONS 1H(19C, X), (20C, X), (22C, X), E=40 MeV/nucleon; calculated reaction cross sections, rms radii, neutron density distributions using the finite range Glauber model (FRGM) and the microscopic optical potential calculated within the Brueckner-Hartree-Fock formalism (BHF) formalism. Halo structure in 22C. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.031601
2009CH46 Int.J.Mod.Phys. E18, 1887 (2009) 16O-nucleus elastic scattering in the energy range 300 MeV-1.503 GeV NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca, 90Zr, 208Pb(16O, 16O), E=0.3-1.503 GeV; analyzed elastic angular distribution of 16O within the framework of the Coulomb modified correlation expansion for the Glauber amplitude.
doi: 10.1142/S0218301309013944
2009CH58 Eur.Phys.J. A 41, 179 (2009) α-nucleus elastic scattering in the energy range 25-70 MeV/nucleon NUCLEAR REACTIONS 1n, 1H(p, p), 4He(α, α), E=25, 30, 35, 40, 50, 70 MeV/nucleon; 58Ni, 116Sn, 197Au(α, α), E=60 MeV/nucleon; analyzed σ, σ(θ) within the Coulomb-modified Glauber model and effect of two scattering amplitude datasets.
doi: 10.1140/epja/i2009-10818-2
2009CH60 Phys.Rev. C 80, 054601 (2009) Glauber model for α-nucleus total reaction cross section NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 58,60Ni, 112,116,120,124Sn, 208Pb(α, X), E=69.6, 117.2, 163.9, 192.4 MeV; calculated total reaction σ using Coulomb-modified Glauber model. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.054601
2007CH42 Phys.Rev. C 75, 054614 (2007) 12C-12C elastic scattering at 1.016, 1.449, and 2.4 GeV and the NN amplitude NUCLEAR REACTIONS 12C(12C, 12C), E=1.016, 1.449, 2.400 GeV/nucleon; analyzed elastic scattering angular distributions and reaction cross sections witin the framework of Coulomb modified Glauber model.
doi: 10.1103/PhysRevC.75.054614
2007KH12 Int.J.Mod.Phys. E16, 1741 (2007) Proton-nucleus elastic scattering at ∼ 1 GeV and the NN amplitude NUCLEAR REACTIONS 4He, 12C, 16O, 40Ca(p, p), E=1 GeV; analyzed σ, angular distributions and polarization data using the Glauber formalism.
doi: 10.1142/S0218301307006915
2005KH14 Int.J.Mod.Phys. E14, 787 (2005) Proton-4He elastic scattering at ∼ 1 GeV NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 1 GeV; analyzed σ(θ), polarization observables; deduced parameters. 4He(p, p), E ≈ 1 GeV; calculated σ(θ), polarization observables. Glauber model.
doi: 10.1142/S0218301305003557
2005SU30 Pramana 65, 1027 (2005) M.A.Suhail, N.Neelofer, Z.A.Khan Relativistic analysis of nuclear ground state densities at 135 to 200 MeV NUCLEAR REACTIONS 40Ca(p, p), E=135-200 MeV; analyzed elastic σ(θ), analyzing powers; deduced ground state densities, related features. Relativistic analysis.
doi: 10.1007/BF02705278
1994AH05 Nuovo Cim. 107A, 1203 (1994) I.Ahmad, Z.A.Khan, S.Ali, G.M.Bhuiyan α-12C Elastic Scattering at 1.37 GeV in the α-Particle Model NUCLEAR REACTIONS 12C(α, α), E=1.37 GeV; calculated σ(θ). Glauber multiple scattering theory.
doi: 10.1007/BF02775760
1993AL10 Nuovo Cim. 106A 491 (1993) M.A.Alvi, I.Ahmad, Z.A.Khan, S.M.Saliem Inelastic Scattering of 1.37 GeV Alpha-Particle and the Semi-Phenomenological N-Alpha Amplitude NUCLEAR REACTIONS 12C, 40,42,44Ca(α, α'), E=1.37 GeV; analyzed σ(θ). Semi-phenomenological N-alpha amplitude.
doi: 10.1007/BF02782702
1984KH01 J.Phys.(London) G10, 135 (1984) d- and α - 12C Inelastic Scattering at Intermediate Energies NUCLEAR REACTIONS 12C(d, d'), E=0.698 GeV; 12C(α, α'), E=1.37 GeV; analyzed σ(θ). Glauber model S-matrix, effective profile expansion method.
doi: 10.1088/0305-4616/10/2/006
1981KH07 Z.Phys. A303, 161 (1981) Elastic Scattering of Intermediate Energy Protons on 4He and 12C NUCLEAR REACTIONS 4He, 12C(p, p), (polarized p, p), E ≈ 1 GeV; calculated σ(θ), P(θ). Glauber amplitude correlation expansion, Coulomb, spin effects.
doi: 10.1007/BF01420274
1979AH04 Phys.Scr. 20, 26 (1979) Scattering of Intermediate Energy Protons on 6Li and the α-d Cluster Model NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=0.6, 1.04 GeV; calculated σ(θ). Glauber multiple scattering theory, α-d cluster description of 6Li.
doi: 10.1088/0031-8949/20/1/005
1977KH02 Pramana 8, 149 (1977) Elastic and the 2+ Inelastic Scattering of High Energy Protons on 12C And the Alpha-Particle Model NUCLEAR REACTIONS 12C(p, p), (p, p'), E=1 GeV; calculated σ. Glauber multiple scattering theory.
doi: 10.1007/BF02868065
1976AH09 Nucl.Phys. A274, 519 (1976) The Proton Total Cross Section on 12C and the α-Particle Model NUCLEAR REACTIONS 12C(p, X), E=0.15-1 GeV; calculated σ. α-model, Glauber multiple scattering theory.
doi: 10.1016/0375-9474(76)90218-9
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