NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Anwar Found 24 matches. 2024AA04 Eur.Phys.J. A 60, (2024) G.Aarts, Ch.Allton, M.N.Anwar, R.Bignell, T.J.Burns, B.Jager, J.-I.Skullerud Non-zero temperature study of spin 1/2 charmed baryons using lattice gauge theory
doi: 10.1140/epja/s10050-024-01261-2
2023AN01 J.Phys.(London) G50, 025105 (2023) Cluster folding model analysis of the 7Be+28Si elastic scattering in the near-barrier NUCLEAR REACTIONS 28Si(7Be, 7Be), E=13-22 MeV; analyzed available data; deduced σ, best-fit parameters of the generated potentials. Comparison with experimental data.
doi: 10.1088/1361-6471/acb0e8
2021BE08 Chin.Phys.C 45, 024101 (2021) K.O.Behairy, M.El-Azab Farid, A.A.Ibraheem, O.Ramadan, M.Anwar Analysis of strong refractive effect within 11Li projectile structure NUCLEAR REACTIONS 12C, 28Si(11Li, 11Li), E=29, 50, 60 MeV/nucleon; analyzed available data. 11Li; deduced rms proton, neutron and mass radii, volume integrals, σ(θ) with the WS potential model, σ, fitting parameters.
doi: 10.1088/1674-1137/abca1b
2021HE26 Phys.Rev. C 104, 044604 (2021) A.Hemmdan, M.A.Hassanain, M.Anwar, K.O.Behairy Analysis of elastic and inelastic scattering of 20Ne on 76Ge at 306 MeV NUCLEAR REACTIONS 76Ge(20Ne, 20Ne), (20Ne, 20Ne'), E=306 MeV; analyzed experimental σ(θ) data using coupled channels analysis and through two optical potentials, the two-cluster CP1 and phenomenological Woods-Saxon potential (WSP) and the double folding model by taking into account the effect of the low-lying states of 20Ne and 76Ge; deduced best-fit parameters for the WSP potential.
doi: 10.1103/PhysRevC.104.044604
2020AN08 Phys.Rev. C 101, 064617 (2020) Semimicroscopic analysis of 6Li elastic scattering at 40 MeV/nucleon NUCLEAR REACTIONS 24Mg, 28Si, 40,48Ca, 58Ni, 90Zr, 116Sn(6Li, 6Li), (6Li, X), E=40 MeV/nucleon; analyzed experimental data for elastic σ(θ) and total σ using double folding optical models with phenomenological effective nucleon-nucleon interaction and density-independent single Yukawa term, density-independent M3Y effective interaction, and Woods-Saxon-type optical model potentials; deduced radial sensitivity of elastic differential σ(θ), optical model parameters.
doi: 10.1103/PhysRevC.101.064617
2019HA35 Phys.Atomic Nuclei 82, 615 (2019) M.A.Hassanain, H.F.A.Alshrani, A.A.Ibraheem, M.Anwar, K.O.Behairy, Z.M.M.Mahmoud, E.M.Darwish Analysis of Elastic 16O + 40Ca Refractive Scattering at 214 MeV
doi: 10.1134/S1063778819060073
2018HA17 Phys.Rev. C 97, 044610 (2018) M.A.Hassanain, M.Anwar, K.O.Behairy Semimicroscopic analysis of 6Li + 28Si elastic scattering at 76 to 318 MeV NUCLEAR REACTIONS 28Si(6Li, 6Li), E=76-318 MeV; calculated microscopic nuclear potentials, best-fit parameters, and differential σ(E, θ) using α-cluster analysis with DFC1 and CDM3Y6 interactions for the real potential, and Woods-Saxon form for the imaginary potential; deduced volume integral per interacting nucleon pair for different optical potentials, impact of addition of the surface (DWS) imaginary potential term. Comparison with experimental results.
doi: 10.1103/PhysRevC.97.044610
2018HA27 Phys.Rev. C 98, 014621 (2018) M.A.Hassanain, F.M.Z.Alqahtani, A.A.Ibraheem, M.Anwar, K.O.Behary, Z.M.Mahmoud, M.El-Azab Farid Elastic and inelastic 16O + 12C rainbow scattering within the coupled-channels mechanism NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E=181, 200, 260, 281, 608, 1503 MeV; analyzed experimental data for elastic and inelastic differential σ(θ, E) in the framework of Woods-Saxon (WS) and full cluster folded (DFC1) optical model potentials, and using the coupled-channel (CC) formalism; deduced best-fit parameters for WS potentials, and energy dependence of real and imaginary volume integrals of WS and DFC1 potentials, and that of the total reaction σ(E).
doi: 10.1103/PhysRevC.98.014621
2017BE01 Nucl.Phys. A957, 332 (2017) K.O.Behairy, Z.M.M.Mahmoud, M.Anwar α-particle elastic scattering from 12C, 16O, 24Mg, and 28Si NUCLEAR REACTIONS 12C(α, α), E=104-172.2 MeV;16O(α, α), E=48.7-146 MeV;24Mg(α, α), E=50-119 MeV;28Si(α, α), E=104, 120, 166, 240 MeV; calculated nuclear rms radius, σ(θ), σ using single folding model with optical model potential and density dependent α-nucleon interaction; deduced model parameters. Compared with available data.
doi: 10.1016/j.nuclphysa.2016.09.008
1987GU10 Nucl.Instrum.Methods Phys.Res. B24/25, 496 (1987) K.Gul, M.Anwar, S.M.Saleem, M.Ahmad Neutron Emission Cross Section Measurements with a 14 MeV Neutron Generator NUCLEAR REACTIONS 27Al, Cu, Pb(n, xn), E=14 MeV; measured σ(En, θn), σ. Liquid scintillator.
doi: 10.1016/0168-583X(87)90692-6
1986GU09 Radiat.Eff. 92, 187 (1986) K.Gul, M.Anwar, S.M.Saleem, M.Ahmad Measurements of Neutron Emission Cross Sections for Al, Cu and Pb at 14.6 MeV Neutron Energy NUCLEAR REACTIONS 27Al, Cu, Pb(n, n), (n, xn), E=3-14 MeV; measured σ(θ). 27Al deduced total, level excitation σ.
doi: 10.1080/00337578608208318
1986GU13 Nucl.Sci.Eng. 94, 42 (1986) K.Gul, M.Ahmad, M.Anwar, S.M.Saleem Measurements of Neutron Fission Cross Sections of 237Np, 240Pu, 241Pu, 242Pu, 244Pu, and 241Am at 14.7 MeV NUCLEAR REACTIONS 237Np, 240,241,242,244Pu, 241Am(n, F), E=14.7 MeV; measured fission σ. Ge(Li), Si detectors.
doi: 10.13182/NSE86-A17115
1985GU01 Phys.Rev. C31, 69 (1985) K.Gul, M.Anwar, M.Ahmad, S.M.Saleem, N.A.Khan Scattering of 14.6 MeV Neutrons from Fe: Investigation of structure in neutron emission spectra NUCLEAR REACTIONS Fe(n, n'), E=14.6 MeV; measured σ(En), σ(θ). 56Fe deduced levels, possible M1 giant resonance. Natural target.
doi: 10.1103/PhysRevC.31.69
1985GU02 Phys.Rev. C31, 74 (1985) K.Gul, M.Anwar, M.Ahmad, S.M.Saleem, N.A.Khan Scattering of 14.6 MeV Neutron from Fe: Neutron emission cross measurements NUCLEAR REACTIONS Fe(n, n'), E=14.6 MeV; measured σ(E, θ), σ(θ), σ. Natural target.
doi: 10.1103/PhysRevC.31.74
1985GU05 J.Phys.(London) G11, 393 (1985) K.Gul, M.Anwar, M.Ahmad, S.M.Saleem, N.A.Khan, R.J.Peterson Excitation of M1 States in 56Fe through Inelastic Scattering of 14.6 MeV Neutrons NUCLEAR REACTIONS 56Fe(n, n'), E=14.6 MeV; measured σ(θ). 56Fe deduced isovector M1 transition strength, triplet J, π.
doi: 10.1088/0305-4616/11/3/017
1985GU21 Nucl.Instrum.Methods Phys.Res. B10/11, 401 (1985) K.Gul, M.Anwar, M.Ahmad, S.M.Saleem 14 MeV Neutron Scattering Experiments at PINSTECH NUCLEAR REACTIONS 56Fe(n, n'), E=14.6 MeV; measured σ(En).
doi: 10.1016/0168-583X(85)90278-2
1983KH05 Nucl.Instrum.Methods 215, 193 (1983) N.A.Khan, H.A.Khan, M.Ahmad, K.Jamil, M.Anwar, S.M.Saleem, K.Gul Calibration of Homalite Cr-39 Plastic Track Detector for Light Particle Spectrometry and Its Application in Studying the (n, α) and (n, p) Reaction on 51V NUCLEAR REACTIONS 51V(n, p), (n, α), E=14.7 MeV; measured σ, σ(Eα). 48Sc deduced level density, nuclear temperature.
doi: 10.1016/0167-5087(83)91308-X
1981GU12 Phys.Rev. C24, 2458 (1981) K.Gul, M.Anwar, M.Ahmad, S.M.Saleem, N.A.Khan Scattering of 14.7 MeV Neutrons from 12C and Evidence for a New Reaction Channel NUCLEAR REACTIONS 12C(n, n), (n, n'), (n, nα), E=14.7 MeV; measured σ(En, θ), integrated σ. 9Be level deduced neutron emission probability. Natural target.
doi: 10.1103/PhysRevC.24.2458
1980KH04 Nucl.Instrum.Methods 173, 137 (1980) N.A.Khan, H.A.Khan, K.Gul, R.A.Akbar, M.Anwar, A.Waheed, G.Hussain, M.S.Shaikh A New Approach to Measure Reaction Parameters in the 14.8 MeV Neutron Induced Fission of 240Pu and 241Pu NUCLEAR REACTIONS, Fission 240,241Pu(n, F), E=14.8 MeV; measured σ, σ(fragment θ). Solid state nuclear track detectors, 2π-geometry.
doi: 10.1016/0029-554X(80)90578-9
1980KH05 Nucl.Instrum.Methods 173, 163 (1980) N.A.Khan, H.A.Khan, K.Gul, M.Anwar, G.Hussain, R.A.Akbar, A.Waheed, M.S.Shaikh 14.8 MeV Neutron Induced Fission Studies of 239Pu, 242Pu, 244Pu and 241Am NUCLEAR REACTIONS, Fission 239,242,244Pu, 241Am(n, F), E=14.8 MeV; measured σ, σ(fragment θ). Muscovite mica track detector, 2π-geometry.
doi: 10.1016/0029-554X(80)90583-2
1980LI08 Nucl.Phys. A339, 205 (1980) A.Lindholm, L.Nilsson, M.Ahmad, M.Anwar, I.Bergqvist, S.Joly Direct-Semidirect and Compound Contributions to Radiative Neutron Capture Cross Sections NUCLEAR REACTIONS 40Ca, 58Ni, 89Y, 206Pb(n, γ), E=0.5-11 MeV; measured Eγ, Iγ. 41Ca, 59Ni, 90Y, 207Pb levels deduced production σ(E). Compound nucleus, direct-semidirect model analysis.
doi: 10.1016/0375-9474(80)90087-1
1976MI19 Nucl.Phys. A272, 133 (1976) J.A.Mirza, A.M.Khan, M.Irshad, H.A.Schmidt, A.F.M.Ishaq, M.Anwar-Ul-Islam The 142Nd(n, γ)143Nd Reaction with Thermal Neutrons NUCLEAR REACTIONS 142Nd(n, γ), E=th; measured Eγ, Iγ, γγ-coin; deduced Q. 143Nd deduced levels, J, π. Enriched, natural targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(76)90322-5
1974IS06 Nucl.Instrum.Methods 121, 193 (1974) A.F.M.Ishaq, A.M.Khan, M.Anwar-Ul-Islam, M.R.Najam Precise Energies of Gamma Rays from Thermal Neutron Capture in Nitrogen NUCLEAR REACTIONS 14N(n, γ), E=thermal; measured Eγ. 15N deduced transitions, neutron binding energy.
doi: 10.1016/0029-554X(74)90157-8
1974MU04 Nucl.Instrum.Methods 115, 345 (1974) S.Mubarakmand, M.Ahmad, M.Anwar, M.S.Chaudhry Cross-Section Measurements with a Neutron Generator NUCLEAR REACTIONS 12C, 27Al, 238U(n, X), E=1.7-14.7 MeV; measured σ(E).
doi: 10.1016/0029-554X(74)90230-4
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