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NSR database version of May 6, 2024.

Search: Author = S.Manzoor

Found 12 matches.

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2011RA23      Int.J.Mod.Phys. E20, 1709 (2011)

M.A.Rana, G.Sher, S.Manzoor, M.I.Shehzad

Pion-Induced Fission of 209Bi and 119Sn: Measurements, Calculations, Analyses, and Comparison

NUCLEAR REACTIONS 209Bi, 119Sn(π-, F), E=500-1665 MeV; analyzed experimental and theoretical data; deduced energy dependence, collective nuclear excitations, fission cross sections, spontaneous fission.

doi: 10.1142/S0218301311019593
Citations: PlumX Metrics


2011RA25      Chin.Phys.Lett. 28, 092501 (2011)

M.A.Rana, G.Sher, S.Manzoor, M.I.Shahzad

Fission of Weakly Prolate 119Sn and Weakly Oblate 209Bi Nuclei Induced by 500 and 672 MeV Negative Pions

NUCLEAR REACTIONS 209Bi, 119Sn(π-, F), E=500, 672 MeV; analyzed experimental and theoretical data; deduced energy dependence, collective nuclear excitations, logarithmic dependence of fission cross sections.

doi: 10.1088/0256-307X/28/9/092501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1891.


2011SH02      Chin.Phys.Lett. 28, 012501 (2011)

G.Sher, M.A.Rana, S.Manzoor, M.I.Shahzad

Negative Pion Induced Fission with Heavy Target Nuclei

NUCLEAR REACTIONS Bi, Cu(π-, F), E=500-2500 MeV; calculated fission σ. Comparison with experimental data, CEM95 code.

doi: 10.1088/0256-307X/28/1/012501
Citations: PlumX Metrics


2008CE03      Nucl.Phys. A807, 206 (2008)

S.Cecchini, T.Chiarusi, G.Giacomelli, M.Giorgini, A.Kumar, G.Mandrioli, S.Manzoor, A.R.Margiotta, E.Medinaceli, L.patrizii, V.Popa, I.E.Qureshi, G.sirri, M.Spurio, V.Togo

Fragmentation cross sections of Fe26+, Si14+ and C6+ ions of 0.3-10 A GeV on polyethylene, CR39 and aluminum targets

NUCLEAR REACTIONS 1H, 12C, 27Al(12C, X), (28Si, X), (56Fe, X), E=0.3?10 GeV/nucleon; measured total fragmentation σ. Comparison with semi-empirical formula. Polyethylene targets and CR39 track detectors.

doi: 10.1016/j.nuclphysa.2008.03.017
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0946.


2008RA18      Chin.Phys.Lett. 25, 3208 (2008)

M.A.Rana, S.Manzoor

Total Fragmentation Cross Section of 158A GeV Lead Projectiles in Cu Target

NUCLEAR REACTIONS Cu(Pb, X), E=158 GeV/nucleon; measured total fragmentation cross section.

doi: 10.1088/0256-307X/25/9/031
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2000DE02      Nucl.Phys. A662, 207 (2000)

H.Dekhissi, G.Giacomelli, M.Giorgini, G.Mandrioli, S.Manzoor, L.Patrizii, V.Popa, P.Serra, V.Togo

Fragmentation Studies of 158 A GeV Pb Ions using CR39 Nuclear Track Detectors

NUCLEAR REACTIONS H, C, O, 27Al, Cu, Pb(208Pb, X), E=158 GeV/nucleon; measured total, break-up, pick-up charge changing σ. CR39 nuclear track detectors.

doi: 10.1016/S0375-9474(99)00414-5
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1998GI12      Nucl.Instrum.Methods Phys.Res. A411, 41 (1998)

G.Giacomelli, M.Giorgini, G.Mandrioli, S.Manzoor, L.Patrizii, V.Popa, P.Serra, V.Togo, E.C.Vilela

Extended Calibration of a CR39 Nuclear Track Detector with 158 A GeV 207Pb Ions

NUCLEAR REACTIONS Pb(207Pb, X), E=158 GeV/nucleon; measured fragments charge distribution; deduced track detector characteristics.

doi: 10.1016/S0168-9002(98)00270-8
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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