NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = M.Iqbal Found 31 matches. 2012PA31 Eur.Phys.J. A 48, 119 (2012) T.M.Partanen, J.A.Niskanen, M.J.Iqbal Parity nonconserving proton-proton elastic scattering NUCLEAR REACTIONS 1H(p, p), E=1-350 MeV; calculated longitudinal analyzing power using DDH potential with short-range ρ and ω and longer-ranged 2π exchanges as parity nonconserving interactions.
doi: 10.1140/epja/i2012-12119-1
2011MA71 J.Korean Phys.Soc. 59, 1503s (2011) Depletion and Decay Analysis of Pakistan Research Reactor-2 (PARR-2) with HEU and LEU Fuel
doi: 10.3938/jkps.59.1503
2008AB22 Nucl.Data Sheets 109, 2785 (2008) H.Abdel-Khalik, P.Turinsky, M.Jessee, J.Elkins, T.Stover, M.Iqbal Uncertainty Quantification, Sensitivity Analysis, and Data Assimilation for Nuclear Systems Simulation
doi: 10.1016/j.nds.2008.11.010
2008NI08 Eur.Phys.J. A 36, 295 (2008) J.A.Niskanen, T.M.Partanen, M.J.Iqbal Parity nonconserving two-pion exchange in elastic proton-proton scattering NUCLEAR REACTIONS 1H(polarized p, p), E=10-1000 MeV; calculated analyzing power using various models. Comparison with data.
doi: 10.1140/epja/i2007-10595-x
1996AR25 Radiochim.Acta 73, 45 (1996) M.Arif, J.H.Zaidi, I.H.Qureshi, M.Z.Iqbal Fission Neutron Spectrum Averaged Cross Sections of some Threshold Reactions on Tellurium: Estimation of radioactive impurities in (n, γ)-produced 131Te-131I NUCLEAR REACTIONS 120,122,124,125,126Te(n, p), 126Te(n, α), 120Te(n, 2n), E=fission spectrum; measured fission spectrum averaged residuals, isomer production σ. Activation technique, radiochemical separations, high-resolution γ-spectroscopy, discussed radioactive impurities estimation in (n, γ)-produced 131Te-131I. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31563. 1996AR33 Radiochim.Acta 75, 175 (1996) M.Arif, J.H.Zaidi, I.H.Qureshi, M.Z.Iqbal Fission Neutron Spectrum Averaged Cross Sections of Some Threshold Reactions on Tin: Small scale production of 111In in a nuclear reactor NUCLEAR REACTIONS 112Sn(n, 2n), (n, n'p), E=reactor; 114,115,116,117Sn(n, p), E=reactor; 118,120Sn(n, α), E=reactor; measured residuals production σ. Activation method. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31562. 1996IQ01 Phys.Lett. 386B, 55 (1996) M.J.Iqbal, X.Jin, D.B.Leinweber ρ-ω Mixing Via QCD Sum Rules with Finite Mesonic Widths
doi: 10.1016/0370-2693(96)00914-8
1996IQ02 Phys.Lett. 367B, 45 (1996) M.J.Iqbal, X.Jin, D.B.Leinweber Mesonic Width Effects on the Momentum Dependence of the ρ-ω Mixing Matrix Element
doi: 10.1016/0370-2693(95)01447-0
1994IQ01 Phys.Rev. C49, 355 (1994) Isobar Excitation in Parity Nonconserving Proton-Proton Scattering NUCLEAR REACTIONS 1H(polarized p, p), E=10-1000 MeV; calculated parity violating average longitudinal analyzing power. Meson exchange model, isobar excitation.
doi: 10.1103/PhysRevC.49.355
1994IQ02 Phys.Lett. 322B, 7 (1994) The Effect of Off-Shell Variations of (ρ(Omega)) Meson Mixing on Charged Symmetry Breaking Neutron-Proton Scattering NUCLEAR REACTIONS 1n(polarized p, p), E=183-800 MeV; calculated charge symmetry breaking observable vs θ; deduced ρ(omega)-mixing matrix off-shell variations implications.
doi: 10.1016/0370-2693(94)90482-0
1993VU02 Phys.Rev. D48, 1009 (1993) J.-C.Vuilleumier, J.Busto, J.Farine, V.Jorgens, L.W.Mitchell, M.Treichel, J.-L.Vuilleumier, H.T.Wong, F.Boehm, P.Fisher, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, B.M.O'Callaghan-Hay, J.Thomas, K.Gabathuler Search for Neutrinoless Double-β Decay in 136Xe with a Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured 0ν-, 2ν-accompanied 2β-decay T1/2 lower limits. Xenon time projection chamber, underground measurement.
doi: 10.1103/PhysRevD.48.1009
1992SO16 Nucl.Phys. A548, 562 (1992) V.Sossi, M.J.Iqbal, R.R.Johnson, G.Jones, M.Pavan, F.M.Rozon, M.Sevior, D.Vetterli, P.Weber, G.Sheffer, G.R.Smith, P.Camerini, N.Grion, R.Rui, N.R.Stevenson, M.J.Vicente-Vacas Pion-Induced Pion Production on Deuterium: A quasifree process NUCLEAR REACTIONS 2H(π+, π-), E=280 MeV; measured σ(θ(π+), θ(π-), E(π+), E(π-)). Comparison with isobar model with Fermi motion.
doi: 10.1016/0375-9474(92)90642-W
1991HA01 Phys.Rev. C43, 230 (1991) O.Hausser, M.C.Vetterli, R.W.Fergerson, C.Glashausser, R.C.Jeppesen, R.D.Smith, R.Abegg, F.T.Baker, A.Celler, R.L.Helmer, R.Henderson, K.Hicks, M.J.Iqbal, K.P.Jackson, K.W.Jones, J.Lisantti, J.Mildenberger, C.A.Miller, R.S.Sawafta, S.Yen Nuclear Response in the 54Fe(p(pol), p(pol)') Reaction at 290 MeV NUCLEAR REACTIONS 54Fe(polarized p, p'), E=290 MeV; measured σ(θ), spin observables, analyzing power, spin-flip probabilities. 54Fe(n, p), E=298 MeV; analyzed data. 54Fe deduced isovector giant dipole, isoscalar giant quadrupole resonance. 54Mn deduced Gamow-Teller transition strength, quenching. Surface RPA model.
doi: 10.1103/PhysRevC.43.230
1991WO03 Phys.Rev.Lett. 67, 1218 (1991) H.T.Wong, F.Boehm, P.Fisher, K.Gabathuler, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, V.Jorgens, L.W.Mitchell, B.M.O'Callaghan-Hay, J.Thomas, M.Treichel, J.-C.Vuilleumier, J.-L.Vuilleumier New Limit on Neutrinoless Double β Decay in 136Xe with a Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured neutrinoless double β-decay T1/2 lower limit; deduced Majorana neutrino mass parameter upper limit. Xenon time projection chamber.
doi: 10.1103/PhysRevLett.67.1218
1991WO06 J.Phys.(London) G17, S165 (1991) H.T.Wong, F.Boehm, P.Fisher, K.Gabathuler, H.E.Henrikson, D.A.Imel, M.Z.Iqbal, V.Jorgens, L.W.Mitchell, B.M.O'Callaghan-Hay, J.Thomas, M.Treichel, J.-C.Vuilleumier, J.-L.Vuilleumier First 0ν Half-Life Limit from the Gotthard Xenon Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured 0ν-mode 2β-decay T1/2 lower limit. Xenon time projection chamber, Gotthard Tunnel underground laboratory.
doi: 10.1088/0954-3899/17/S/017
1990IQ01 Phys.Rev. C42, 1872 (1990) Parity Violating Nuclear Force by Meson Mixing NUCLEAR REACTIONS 1H(polarized p, p), E=10-1000 MeV; calculated average longitudinal analyzing power; deduced form factors, correlations role. Meson mixing, parity violating interaction.
doi: 10.1103/PhysRevC.42.1872
1990MA76 Radiochim.Acta 51, 49 (1990) A.Mannan, I.H.Qureshi, M.Z.Iqbal, R.Wolfle, S.M.Qaim Integral Tests of Differential Cross Sections for (n, α) and (n, 2n) Reactions on Niobium NUCLEAR REACTIONS 93Nb(n, α), (n, 2n), E ≤ 30 MeV; measured σ; deduced 90Y isomer σ ratio. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30977. 1989CH39 Nucl.Phys. A505, 670 (1989) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Xu, Z.Tang, D.M.Drake, I.Bergqvist, A.Brockstedt, J.Lisantti, F.Bertrand, D.J.Horen, K.Hicks, M.Vetterli, M.J.Iqbal Analyzing Powers and Cross Sections of Inclusive Polarized Proton Scattering on 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290, 500 MeV; measured σ(θ), analyzing power vs θ. DWBA, relativistic impulse approximation analyses.
doi: 10.1016/0375-9474(89)90037-7
1989NI01 Phys.Lett. 218B, 272 (1989) ρ(Omega) Meson Mixing in the Reaction np → dπ0 NUCLEAR REACTIONS 1n(p, π0), E=580, 800 MeV; calculated pion production σ asymmetry; deduced ρ(omega) mixing role.
doi: 10.1016/0370-2693(89)91579-7
1989SW01 Phys.Rev. C40, 246 (1989) L.W.Swenson, X.Y.Chen, J.Lisantti, D.K.McDaniels, I.Bergqvist, F.E.Bertrand, D.J.Horen, E.E.Gross, C.Glover, R.O.Sayer, B.L.Burks, O.Hausser, K.Hicks, M.J.Iqbal Different Continuum Approaches to Giant Resonances in 208Pb with 400-MeV Protons NUCLEAR REACTIONS 208Pb(p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200 MeV; measured σ(θ). 208Pb deduced giant resonance L, Γ, EWSR. DWBA analysis, continuum models comparison.
doi: 10.1103/PhysRevC.40.246
1988CH13 Phys.Lett. 205B, 436 (1988) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Tang, Z.Xu, D.M.Drake, I.Bergqvist, A.Brockstedt, F.E.Bertrand, D.J.Horen, J.Lisantti, K.Hicks, M.Vetterli, M.J.Iqbal Relativistic Medium Effects for 208Pb(p(pol), p') at Intermediate Energies NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290 MeV; measured σ(θp', Ep'), analyzing power vs θ; deduced relativistic medium effects.
doi: 10.1016/0370-2693(88)90973-2
1988HA27 Phys.Rev.Lett. 61, 822 (1988) O.Hausser, R.Abegg, R.G.Jeppesen, R.Sawafta, A.Celler, A.Green, R.L.Helmer, R.Henderson, K.Hicks, K.P.Jackson, J.Mildenberger, C.A.Miller, M.C.Vetterli, S.Yen, M.J.Iqbal, R.D.Smith Complete Spin Observables for Quasielastic Proton Scattering from 54Fe at 290 MeV NUCLEAR REACTIONS 54Fe(polarized p, p'X), E=290 MeV; measured σ(θ, Ep'), spin-transfer σ(θ, Ep'), analyzing power, spin observables; deduced Fermi motion, nuclear response function, nucleon-nucleon interaction role. Relativistic, non-relativistic models, impulse approximation.
doi: 10.1103/PhysRevLett.61.822
1988IQ01 Phys.Rev. C38, 2259 (1988) Charge Symmetry Breaking in Neutron-Proton Scattering Including Arbitrary Mesons NUCLEAR REACTIONS 1n(polarized p, p), 1H(polarized n, n), E=100 MeV; analyzed polarization asymmetry data; deduced charge symmetry breaking sensitivity to meson-nucleon form factors.
doi: 10.1103/PhysRevC.38.2259
1988IQ02 Nucl.Phys. A487, 626 (1988) M.J.Iqbal, J.I.Johansson, S.Hama, H.S.Sherif Isovector Dirac Optical Potentials and Nucleon Charge Exchange Reactions NUCLEAR REACTIONS 90Zr(polarized p, n), E=160 MeV; 48Ca(polarized p, n), E=134 MeV; calculated σ(θ), analyzing power. 208Pb(polarized p, n), E=134 MeV; calculated σ(θ), spin rotation parameter vs θ; deduced model parameters. Dirac optical potentials.
doi: 10.1016/0375-9474(88)90030-9
1987BL20 Phys.Lett. 196B, 295 (1987) Relativistic Hartree-Fock Calculations for Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated charge, matter densities, binding energy, rms charge radii. Relativistic Hartree-Fock.
doi: 10.1016/0370-2693(87)90734-9
1987BL22 Phys.Lett. 198B, 14 (1987) Contribution of Charge Symmetry Breaking Forces to Energy differences in Mirror Nuclei NUCLEAR REACTIONS 1H(p, p), 1n(n, n), E=low; calculated scattering length differences, charge symmetry breaking potentials. NUCLEAR STRUCTURE A=11-41; calculated odd mirror nuclei energy, differences. Charge symmetry breaking potentials.
doi: 10.1016/0370-2693(87)90148-1
1987IQ01 Nucl.Instrum.Methods Phys.Res. A259, 459 (1987) M.Z.Iqbal, H.E.Henrikson, L.W.Mitchell, B.M.G.O'Callaghan, J.Thomas, H.T.-k.Wong Design and Construction of a High Pressure Xenon Time Projection Chamber RADIOACTIVITY 136Xe(2β); measured double beta decay, T1/2. High pressure time projection chamber.
doi: 10.1016/0168-9002(87)90827-8
1987IQ02 Phys.Rev. C36, 2442 (1987) M.J.Iqbal, J.Thaler, R.M.Woloshyn Effect of Neutron-Proton Mass Difference on Charge Symmetry Breaking in Neutron-Proton Elastic Scattering NUCLEAR REACTIONS 1H(n, n), E not given; calculated n-p mass difference contribution to charge symmetry breaking.
doi: 10.1103/PhysRevC.36.2442
1986HO10 Phys.Rev. C33, 2059 (1986); Erratum Phys.Rev. C34, 2012 (1986) Relativistic Effects on Spin Observables in Quasielastic Proton Scattering NUCLEAR REACTIONS 12C, 40Ca, 208Pb(polarized p, p'), E=0.2-1 GeV; calculated polarization, analyzing powers, other spin observables vs θ. Relativistic DWBA analysis.
doi: 10.1103/PhysRevC.33.2059
1985IQ01 Phys.Rev. C32, 556 (1985) Intermediate Isobar Effects in a Two-Nucleon Mechanism for (p, π) NUCLEAR REACTIONS 12C(p, π+), E=250, 265, 200 MeV; calculated σ(θ). Two-nucleon model, intermediate isobar effects.
doi: 10.1103/PhysRevC.32.556
1976IQ01 Int.J.Appl.Radiat.Isotop. 27, 258 (1976) Production of Manganese-54 in a Nuclear Reactor NUCLEAR REACTIONS Fe(n, γ), E=reactor; measured 54Mn yields.
doi: 10.1016/0020-708X(76)90008-9
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