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NSR database version of May 24, 2024.

Search: Author = Z.Khan

Found 23 matches.

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2022NA41      Phys.Scr. 97, 125302 (2022)

J.-U.Nabi, A.Ullah, Z.Khan

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
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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
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2017AH08      Phys.Rev. C 96, 064602 (2017)

S.Ahmad, A.A.Usmani, Z.A.Khan

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
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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
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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
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2013KH18      Int.J.Mod.Phys. E22, 1350082 (2013)

Z.A.Khan, D.Chauhan, M.Singh

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
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2012CH27      Phys.Rev. C 85, 067602 (2012)

D.Chauhan, Z.A.Khan

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
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2011CH11      Eur.Phys.J. A 47, 31 (2011)

D.Chauhan, Z.A.Khan

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
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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
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2009CH46      Int.J.Mod.Phys. E18, 1887 (2009)

D.Chauhan, Z.A.Khan

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
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2009CH58      Eur.Phys.J. A 41, 179 (2009)

D.Chauhan, Z.A.Khan

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
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2009CH60      Phys.Rev. C 80, 054601 (2009)

D.Chauhan, Z.A.Khan

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
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2007CH42      Phys.Rev. C 75, 054614 (2007)

D.Chauhan, Z.A.Khan

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
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2007KH12      Int.J.Mod.Phys. E16, 1741 (2007)

Z.A.Khan, M.Singh

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
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2005KH14      Int.J.Mod.Phys. E14, 787 (2005)

Z.A.Khan, M.Singh

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
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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
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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
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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
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1984KH01      J.Phys.(London) G10, 135 (1984)

Z.A.Khan, I.Ahmad

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
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1981KH07      Z.Phys. A303, 161 (1981)

Z.A.Khan

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
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1979AH04      Phys.Scr. 20, 26 (1979)

I.Ahmad, Z.A.Khan

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
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1977KH02      Pramana 8, 149 (1977)

Z.A.Khan, I.Ahmad

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
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1976AH09      Nucl.Phys. A274, 519 (1976)

I.Ahmad, Z.A.Khan

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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Note: The following list of authors and aliases matches the search parameter Z.Khan: , Z.A.KHAN, Z.U.KHAN