NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = H.Khan Found 30 matches. 2024AL10 Phys.Rev. D 109, 072002 (2024) A.Allega, M.R.Anderson, S.Andringa, J.Antunes, M.Askins, D.J.Auty, A.Bacon, J.Baker, N.Barros, F.Barao, R.Bayes, E.W.Beier, T.S.Bezerra, A.Bialek, S.D.Biller, E.Blucher, E.Caden, E.J.Callaghan, M.Chen, S.Cheng, B.Cleveland, D.Cookman, J.Corning, M.A.Cox, R.Dehghani, J.Deloye, M.M.Depatie, F.Di Lodovico, J.Dittmer, K.H.Dixon, E.Falk, N.Fatemighomi, R.Ford, A.Gaur, O.I.Gonzalez-Reina, D.Gooding, C.Grant, J.Grove, S.Hall, A.L.Hallin, W.J.Heintzelman, R.L.Helmer, C.Hewitt, B.Hreljac, V.Howard, J.Hu, R.Hunt-Stokes, S.M.A.Hussain, A.S.Inacio, C.J.Jillings, S.Kaluzienski, T.Kaptanoglu, P.Khaghani, H.Khan, J.R.Klein, L.L.Kormos, B.Krar, C.Kraus, C.B.Krauss, T.Kroupova, C.Lake, L.Lebanowski, J.Lee, C.Lefebvre, Y.H.Lin, V.Lozza, M.Luo, A.Maio, S.Manecki, J.Maneira, R.D.Martin, N.McCauley, A.B.McDonald, C.Mills, G.Milton, I.Morton-Blake, M.Mubasher, A.Molina Colina, D.Morris, S.Naugle, L.J.Nolan, H.M.O'Keeffe, G.D.Orebi Gann, J.Page, K.Paleshi, W.Parker, J.Paton, S.J.M.Peeters, L.Pickard, P.Ravi, A.Reichold, S.Riccetto, M.Rigan, J.Rose, R.Rosero, J.Rumleskie, I.Semenec, P.Skensved, M.Smiley, J.Smith, R.Svoboda, B.Tam, J.Tseng, S.Valder, E.Vazquez-Jauregui, C.J.Virtue, J.Wang, M.Ward, J.R.Wilson, J.D.Wilson, A.Wright, J.P.Yanez, S.Yang, M.Yeh, Z.Ye, S.Yu, Y.Zhang, K.Zuber, A.Zummo, for the SNO+ collaboration Event-by-event direction reconstruction of solar neutrinos in a high light-yield liquid scintillator
doi: 10.1103/PhysRevD.109.072002
2008BR03 Physics of Part.and Nuclei 39, 259 (2008) R.Brandt, V.A.Ditlov, K.K.Dwivedi, W.Ensinger, E.Ganssauge, S.-L.Guo, M.Haiduc, S.R.Hashemi-Nezhad, H.A.Khan, M.I.Krivopustov, R.Odoj, E.A.Pozharova, V.A.Smirnitzki, A.N.Sosnin, W.Westmeier, M.Zamani-Valasiadou Interactions of relativistic heavy ions in thick heavy element targets and some unresolved problems
doi: 10.1134/S1063779608020044
2007YA01 Nucl.Phys. A781, 296 (2007) Z.Yasin, M.I.Shahzad, R.J.Peterson, G.Sher, M.T.Javed, H.A.Khan Energy dependence of fission probabilities induced by negative pions in Sn, Au, and Bi NUCLEAR REACTIONS Sn, Au, Bi(π-, F), E=500, 672, 1068, 1665, 2300 MeV; measured fission probabilities, σ. Comparison with model predictions.
doi: 10.1016/j.nuclphysa.2006.10.081
2006RA15 Chin.Phys.Lett. 23, 1716 (2006) M.A.Rana, E.U.Khan, M.I.Shahzad, I.E.Qureshi, F.Malik, G.Sher, S.Manzoor, H.A.Khan Annihilation of Antiprotons in Light Nuclei NUCLEAR REACTIONS H, C, O(p-bar, X), E=5.9 MeV; measured light charged particle yields, angular distributions following antiproton annihilation in CR-39 detector.
doi: 10.1088/0256-307X/23/7/017
2005QU02 Radiat.Meas. 40, 437 (2005) I.E.Qureshi, M.I.Shahzad, M.T.Javed, S.Manzoor, G.Sher, F.Aleem, H.A.Khan Study of projectile fragmentation in the reaction (158 A GeV) Pb + Pb using CR-39 NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; measured fragments charge and energy distributions; deduced total charge-changing σ. Plastic track detector.
doi: 10.1016/j.radmeas.2005.11.013
2005QU03 Radiat.Meas. 40, 464 (2005) I.E.Qureshi, M.I.Shahzad, E.U.Khan, G.Sher, H.A.Khan Study of the reaction step preceding sequential fission in the nuclear interaction (16.7 MeV/u) 238U+nat.Au NUCLEAR REACTIONS 197Au(238U, X), E=16.7 MeV/nucleon; measured fragments mass and angular distributions, multiplicity; deduced reaction mechanism features. Mica track detectors, sequential fission.
doi: 10.1016/j.radmeas.2005.03.013
2001KH12 Nucl.Phys. A690, 723 (2001) E.U.Khan, I.E.Qureshi, M.I.Shahzad, F.N.Khattak, H.A.Khan Emission of Intermediate Mass Fragments in the Heavy Ion Interaction of (14.0 MeV/u) Pb + Au NUCLEAR REACTIONS 197Au(208Pb, X), E=14.0 MeV/nucleon; measured reaction σ, σ(θ), intermediate mass fragments multiplicity distribution. Solid-state track detectors.
doi: 10.1016/S0375-9474(00)00697-7
2000MA85 Nucl.Instrum.Methods Phys.Res. A453, 525 (2000) S.Manzoor, I.E.Qureshi, M.A.Rana, M.I.Shahzad, G.Sher, M.Sajid, H.A.Khan, G.Giacomelli, M.Giorgini, G.Mandrioli, L.Patrizii, V.Popa, P.Serra, V.Togo Charge Identification in CR-39 Nuclear Track Detector using Relativistic Lead Ion Fragmentation NUCLEAR REACTIONS 27Al, Cu, Pb(207Pb, X), E=158 GeV/nucleon; measured heavy fragments charge distribution. CR-39 nuclear track detectors.
doi: 10.1016/S0168-9002(00)00470-8
1999SH01 Nucl.Phys. A645, 92 (1999) M.I.Shahzad, I.E.Qureshi, S.Manzoor, H.A.Khan Sequential Fission Process Observed in the Reaction (16.7 MeV/u) 238U + nat.Au using Mica as Dielectric Track Detector NUCLEAR REACTIONS 197Au(238U, X), E=16.7 MeV/nucleon; measured fragments mass, energy, angular distributions; deduced sequential fission process. Mica dielectric track detector.
doi: 10.1016/S0375-9474(98)00554-5
1996BB18 Nucl.Instrum.Methods Phys.Res. B111, 91 (1996) J.J.Baluch, E.U.Khan, M.S.Zafar, I.E.Qureshi, H.A.Khan Reproduction of Projectile and Target Masses from the Binary Data in the Heavy Ion Interaction of 17.0 MeV/N 132Xe with 238U NUCLEAR REACTIONS 238U(132Xe, 132Xe), E=17 MeV/nucleon; measured projectile, recoil tracks length, angle in mica detector; deduced projectile, target masses.
doi: 10.1016/0168-583X(95)01286-9
1996GO59 Fiz.Elem.Chastits At.Yadra 27, 377 (1996); Phys.Part.Nucl. 27, 154 (1996) P.A.Gottschalk, P.Vater, R.Brandt, I.E.Qureshi, H.A.Khan, G.Fiedler Kinematical Analysis of Heavy-Ion Induced Nuclear Reactions using Solid-State Nuclear Track Detectors: A review NUCLEAR REACTIONS U(84Kr, X), E=540, 806, 1050 MeV; U, Pb(208Pb, X), E=1535 MeV; 165Ho, 197Au, 209Bi(238U, X), E=2380 MeV; U(238U, X), E=1785, 2149, 2380, 3975 MeV; measured fragments mass, energy, multiplicity, angular distributions; deduced reaction σ, evidence for sequential fission. Solid state nuclear track detectors.
1995PE11 Z.Phys. A352, 181 (1995) R.J.Peterson, S.de Barros, I.O.de Souza, M.B.Gaspar, H.A.Khan, S.Manzoor Mass and Energy Dependence of Pion-Induced Fission NUCLEAR REACTIONS Fe, Cu, 93Nb, Ag, Cd(π+, F), E=80, 100 MeV; measured binary, ternary fission σ; deduced fission probability. Data on other nuclei, other (π-, F) reactions analyzed.
doi: 10.1007/BF01298906
1993KH01 Phys.Lett. 298B, 181 (1993) Shadowing of Deuteron Spin Structure Functions NUCLEAR STRUCTURE 2H; calculated low x-behavior twist-two structure function.
doi: 10.1016/0370-2693(93)91727-5
1991KH01 Phys.Rev. C43, 250 (1991) H.A.Khan, N.A.Khan, R.J.Peterson Mass Dependence of Positive Pion-Induced Fission NUCLEAR REACTIONS 238U, 232Th, 209Bi, 207Pb, 197Au, 184W, 179Hf, 165Ho(π+, F), E=80, 100 MeV; measured fission σ; deduced fission probabilities.
doi: 10.1103/PhysRevC.43.250
1991KH07 Phys.Rev. C44, 1219 (1991) Convenient Parametrization for Deep Inelastic Structure Functions of the Deuteron NUCLEAR STRUCTURE 2H; calculated deep inelastic structure functions. Convolution model.
doi: 10.1103/PhysRevC.44.1219
1990KH07 Nucl.Instrum.Methods Phys.Res. B51, 421 (1990) H.A.Khan, N.A.Khan, R.J.Peterson Pion Induced Interactions in Tantalum, Europium, Antimony and Zirconium NUCLEAR REACTIONS Ta, Eu, Sb, Zr(π+, X), (π+, F), E=80, 100 MeV; measured fission, light reaction fragment σ(θ, E(fragment)); deduced binary, ternary fission σ. Muscovite mica, CR-39 solid state track detectors.
doi: 10.1016/0168-583X(90)90562-9
1988KH06 J.Phys.(London) G14, 701 (1988) Application of Threshold Track Detectors in Studying the Interaction of Intermediate-Energy 18O Ions with Light and Heavy Targets NUCLEAR REACTIONS 232Th, 209Bi, 93Nb, 180Hf(18O, X), (18O, F), E=86 MeV/nucleon; measured σ(fragment θ), σ vs multiplicity, fission fragment σ(θ1, θ2); deduced reaction mechanism.
doi: 10.1088/0305-4616/14/6/009
1988QU01 Phys.Rev. C37, 393 (1988) I.E.Qureshi, H.A.Khan, K.Rashid, P.A.Gottschalk, P.Vater, R.Brandt Four-Fragment Exit Channel in the Interaction of 1050 MeV 84Kr with U Studied with Mica Detectors NUCLEAR REACTIONS U(84Kr, X), E=1050 MeV; measured fragment mass yield, relative velocity distributions.
doi: 10.1103/PhysRevC.37.393
1988QU02 Nucl.Phys. A477, 510 (1988) I.E.Qureshi, H.A.Khan, K.Rashid, P.Vater, R.Brandt, P.A.Gottschalk Kinematical Analysis of 2-, 3- and 4-Body Channels in the Reaction (12.5 MeV/u) 84Kr + (nat)U Observed with Mica Track Detectors NUCLEAR REACTIONS 238U(84Kr, nX), E=12.5 MeV/nucleon; measured multiplicities event number; deduced reaction σ, generalized Fresnel model parameters, fragment mass yield curves, energy, angular distribution.
doi: 10.1016/0375-9474(88)90354-5
1987KH01 Phys.Rev. C35, 645 (1987) H.A.Khan, N.A.Khan, R.J.Peterson Fission Induced in (nat)U, (nat)Pb, 197Au, and 165Ho by 80 and 100 MeV π+ and π- NUCLEAR REACTIONS U, Pb, 165Ho, 197Au(π+, F), (π-, F), E=80, 100 MeV; measured fission fragment σ(θ), mass yields, σ(θ1, θ2); deduced binary, tenary fission yields. Solid state track detectors.
doi: 10.1103/PhysRevC.35.645
1987KH03 Nucl.Instrum.Methods Phys.Res. B22, 541 (1987) H.A.Khan, F.R.Khan, N.A.Khan, M.Ahmed, M.A.Baig Elastic and Inelastic Scattering of 8.5 MeV/Nucleon 132Xe Ions By Uranium Atoms NUCLEAR REACTIONS U(132Xe, 132Xe), (132Xe, 132Xe'), E=8.5 MeV/nucleon; measured σ; deduced grazing angular momentum, interaction radius, reaction σ. Track detectors.
doi: 10.1016/0168-583X(87)90158-3
1987KH04 Nucl.Instrum.Methods Phys.Res. B22, 546 (1987) Measurement of Cross-Sections and Angular Distributions of Reaction Products formed in the Interaction of 86 MeV/Nucleon 18O with 184W NUCLEAR REACTIONS 184W(18O, X), (18O, F), E=86 MeV/nucleon; measured fission, σ, σ(θ), fragment σ(θ1, θ2). Threshold track detectors, thin target.
doi: 10.1016/0168-583X(87)90159-5
1985KH06 Phys.Rev. C32, 1551 (1985) H.A.Khan, I.E.Qureshi, W.Westmeier, R.Brandt, P.A.Gottschalk Elastic and Inelastic Scattering of Uranium Ions by Holmium, Gold, and Bismuth Targets NUCLEAR REACTIONS 165Ho, 197Au, 209Bi(238U, 238U), E=10 MeV/nucleon; measured σ(θ); deduced reaction parameters, σ. Optical, sharp cutoff model analysis. Solid state track detectors, 2π geometry.
doi: 10.1103/PhysRevC.32.1551
1984KH03 Phys.Rev. C29, 2199 (1984) Fission and Spallation Induced by 7-GeV Protons on U, Bi, Pb, Au, W, Ho and Ag NUCLEAR REACTIONS U, 209Bi, Pb, 197Au, W, 165Ho, Ag(p, F), (p, X), E=7 GeV; measured fission, spallation σ; deduced fissility parameter, spallation process target mass dependences. Muscovite mica, Makrofol, Daicel detectors, 4π, 2π geometries.
doi: 10.1103/PhysRevC.29.2199
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
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
1977MU09 Nucl.Instrum.Methods 147, 279 (1977) S.Mubarakmand, K.Rashid, P.Chaudhry, H.A.Khan Application of Glass Solid State Nuclear Track Detectors in the Measurement of the Charged Particle Fission Cross Section of Uranium NUCLEAR REACTIONS U, 238U(3he, f), E=25.1-30 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry B0150.
doi: 10.1016/0029-554X(77)90493-1
1973KH10 Radiat.Eff. 17, 133 (1973) Measurement of Spontaneous-Fission Decay Constant of 238U with a Mica Solid State Track Detector RADIOACTIVITY, Fission 238U(SF); measured T1/2.
doi: 10.1080/00337577308232607
1971KH10 Nucleus (Lahore) 8, 63 (1971) The Determination of Fission Rate, Decay Constant, Profiles and Distributions of Cf252, Pu239, and U235 Fission Sources by Solid State Track Detectors RADIOACTIVITY, Fission 252Cf(SF); measured T1/2, fission rate. Mica, Lexan track detectors.
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