NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Asghar Found 89 matches. 2011YA18 Chin.Phys.C 35, 1013 (2011) Z.Yasin, W.Iram, M.Asghar, M.I.Shahzad Cascade-exciton model analysis of level density parameter dependence in proton induced fission cross sections of some sub-actinide nuclei NUCLEAR REACTIONS 182,183,184,186W, 206,207,208Pb, 209Bi(p, F), E<200 MeV/nucleon; calculated fission σ. CEM95 cascade exciton model code, comparison with experimental data.
doi: 10.1088/1674-1137/35/11/006
2003BE14 Nucl.Instrum.Methods Phys.Res. B201, 545 (2003) M.Belgaid, T.Segueni, F.Kadem, M.Asghar Semi-empirical systematics of (n, t) cross-sections for 14.5 MeV neutrons NUCLEAR REACTIONS 46Ti, 50Cr, 55Mn, 54,56Fe, 59Co, 58,60Ni, 64Zn, 70Ge, 86,88Sr, 90Zr, 93Nb, 92Mo, 103Rh, 102Pd, 106,114Cd, 112Sn, 141Pr, 170Er, 205Tl, 204Pb, 209Bi(n, t), E=14.5 MeV; analyzed σ; deduced parameters. Phenomenological formula.
doi: 10.1016/S0168-583X(02)02071-2
1999BE19 Nucl.Instrum.Methods Phys.Res. B149, 383 (1999) Semi-Empirical Systematics of (n, α) Cross Sections for 14.5 MeV Neutrons NUCLEAR STRUCTURE A=39-209; analyzed (n, α) reaction σ at 14.5 MeV energy; deduced parameters. Semi-empirical formula, evaporation model, droplet model.
doi: 10.1016/S0168-583X(98)00975-6
1999BE47 J.Radioanal.Nucl.Chem. 240, 991 (1999) Activation Cross Sections for Some Isotopes of Ti and Mo with 14.7 MeV Neutrons NUCLEAR REACTIONS 46Ti, 94Mo(n, 2n), 47,48,50Ti, 96,97Mo(n, p), E=14.7 MeV; measured activation σ. Comparison with previous results.
doi: 10.1007/BF02349889
1998BE45 Appl.Radiat.Isot. 49, 1497 (1998) Semi-Empirical Systematics of (n, p) Reaction Cross Sections for 14.5 MeV Neutrons
doi: 10.1016/S0969-8043(98)00054-2
1998BE46 Nucl.Instrum.Methods Phys.Res. B142, 463 (1998) Semi-Empirical Systematics of (n, p) Cross Sections for 14.5 MeV Neutrons
doi: 10.1016/S0168-583X(98)00333-4
1998BO12 J.Phys.(London) G24, 1029 (1998) B.Bouzid, M.Asghar, M.Djebara, G.Medkour The Nature of Dynamics of the Last Stages of the Fission Process NUCLEAR REACTIONS 230Th, 233,234,236U, 239,240Pu, 250Cf(n, F), E=thermal; analyzed fragments odd-even effect, ternary-to-binary fission ratio; deduced fission dynamics features.
doi: 10.1088/0954-3899/24/5/011
1998FA07 Phys.Rev. C58, 150 (1998) F.Farget, D.Santos, M.Asghar, C.Foin, J.Genevey, A.Gizon, J.Gizon, J.A.Pinston, C.W.Beausang, A.J.Boston, S.A.Forbes, D.T.Joss, P.J.Nolan, E.S.Paul, A.T.Semple, J.N.Wilson, R.M.Clark, K.Hauschild, N.J.O'Brien, C.Parry, R.Wadsworth, J.Simpson, B.M.Nyako, L.Zolnai Superdeformed Quasicontinuum Feeding of the Superdeformed Yrast Band in 132Ce NUCLEAR REACTIONS 100Mo(36S, 4n), E=155 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 132Ce deduced superdeformed quasicontiuum, weak rotational damping.
doi: 10.1103/PhysRevC.58.150
1998IS06 Eur.Phys.J. A 2, 173 (1998) S.Issmer, M.Fruneau, J.A.Pinston, M.Asghar, D.Barneoud, J.Genevey, Th.Kerscher, K.E.G.Lobner Direct Mass Measurements of A = 80 Isobars NUCLEAR REACTIONS 27Al(58Ni, X)80Rb/80Sr/80Y/80Zr, E=300 MeV; measured masses. Time-of-flight spectrometer. Comparison with previous results. ATOMIC MASSES 27Al(58Ni, X)80Rb/80Sr/80Y/80Zr, E=300 MeV; measured masses. Time-of-flight spectrometer. Comparison with previous results.
doi: 10.1007/s100500050106
1997ME04 J.Phys.(London) G23, 103 (1997) G.Medkour, M.Asghar, M.Djebara, B.Bouzid The Origin of the Proton Odd-Even Effect in Low-Energy Fission NUCLEAR REACTIONS 232U(n, F), E=thermal; measured light fission fragment mass, charge, kinetic energy correlated yield data; deduced proton odd-even effect related features. Cosi fan tutte spectrometer, other data included.
doi: 10.1088/0954-3899/23/1/008
1996AS03 J.Phys.(London) G22, 1643 (1996) M.Asghar, B.Bouzid, G.Medkour, M.Djebara Unification of Binary and LCP Fission Processes NUCLEAR REACTIONS 235U(n, F), E=thermal; analyzed fission fragments yield vs mass; deduced binary, ternary fission processes ambiguity removal. Adiabatic perturbation theory based model.
doi: 10.1088/0954-3899/22/11/011
1993AS03 Nucl.Phys. A560, 677 (1993) M.Asghar, N.Boucheneb, G.Medkour, P.Geltenbort, B.Leroux Measurement of Cold Fission for 229Th(n(th), f), 232U(n(th), f) and 239Pu(n(th), f) with the Cosi Fan Tutte Spectrometer NUCLEAR REACTIONS 229Th, 232U, 239Pu(n, F), E=thermal; measured fission fragment mass-energy correlations for the light fragment group. 230Th, 233U, 240Pu deduced cold fission probability as a function of fragment mass.
doi: 10.1016/0375-9474(93)90040-5
1993BE52 Nucl.Phys. A565, 563 (1993) A.Benoufella, G.Barreau, M.Asghar, P.Audouard, F.Brisard, T.P.Doan, M.Hussonnois, B.Leroux, J.Trochon, M.S.Moore Measurement of Fragment Mass-Energy Correlations for 248Cm(s, f): Far-out asymmetric fission and cold fragmentations RADIOACTIVITY 248Cm(SF); measured fission fragment mass-energy correlations; deduced far-out asymmetric fission, cold fission features.
doi: 10.1016/0375-9474(93)90045-Y
1991BO36 Nucl.Phys. A535, 77 (1991) N.Boucheneb, M.Asghar, G.Barreau, T.P.Doan, B.Leroux, A.Sicre, P.Geltenbort, A.Oed A High-Resolution Multi-Parametric Study of 239Pu(n(th), f) with the Cosi-Fan-Tutte Spectrometer NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured light fragment mass-charge-energy correlations; deduced different mass, charge yields, proton, neutron yield odd-even effects, conditional charge variance.
doi: 10.1016/0375-9474(91)90516-9
1990BO05 Z.Phys. A335, 41 (1990) J.P.Bocquet, R.Brissot, H.R.Faust, M.Fowler, J.Wilhelmy, M.Asghar, M.Djebara Characteristics of Mass and Nuclear Charge Distributions of 229Th(n(th), F). Implications for Fission Dynamics NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured fission fragment yield vs mass, charge; deduced proton odd-even effect role in fission. Other data analyzed. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22143. 1990MA49 Nucl.Phys. A515, 433 (1990) G.Martinez, G.Barreau, A.Sicre, T.P.Doan, P.Audouard, B.Leroux, W.Arafa, R.Brissot, J.P.Bocquet, H.Faust, P.Koczon, M.Mutterer, F.Gonnenwein, M.Asghar, U.Quade, K.Rudolph, D.Engelhardt, E.Piasecki Mass and Nuclear Charge Yields for 237Np(2n(th), f) at Different Fission Fragment Kinetic Energies NUCLEAR REACTIONS 239Np(n, F), E=thermal; measured light fission product mass versus kinetic energies; deduced fractional independent fission yields, odd-even effects of elements, isotones. Double neutron capture on 237Np target.
doi: 10.1016/0375-9474(90)90593-B
1989BO37 Nucl.Phys. A502, 261c (1989) N.Boucheneb, P.Geltenbort, M.Asghar, G.Barreau, T.P.Doan, F.Gonnenwein, B.Leroux, A.Oed, A.Sicre High Resolution Measurements of Mass, Energy and Nuclear Charge Correlations for 229Th(n(th), F) with the COSI FAN TUTTE Spectrometer NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured fission fragment yield vs mass, kinetic energy; deduced conditional variance mass dependence.
doi: 10.1016/0375-9474(89)90666-0
1989DJ01 Nucl.Phys. A496, 346 (1989) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.
doi: 10.1016/0375-9474(89)90179-6
1989HA42 Radiochim.Acta 46, 23 (1989) M.Haddad, J.Crancon, G.Lhospice, M.Asghar Post-Neutron Mass Distribution for 232U(n(th), f) NUCLEAR REACTIONS 232U(n, F), E=thermal; measured fission yields for Kr, Sr, Y, Zr, Mo, Sb, I, Te, Xe, Cs, La, Ce isotopes. γ-spectroscopy. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22119. 1988HA17 Nucl.Phys. A481, 333 (1988) M.Haddad, J.Crancon, G.Lhospice, M.Asghar Post-Neutron Mass Distribution for 238Pu(n(th), f) NUCLEAR REACTIONS 238Pu(n, F), E=thermal; measured fission products mass distribution; deduced independent yields, proton odd-even effect.
doi: 10.1016/0375-9474(88)90500-3
1987HA43 Radiochim.Acta 42, 165 (1987) M.Haddad, J.Crancon, G.Lhospice, M.Asghar, J.Blachot Post-Neutron Mass Distribution of 229Th(n(th), f) NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured light, heavy fission product yield vs mass. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23702. 1986AS01 Radiat.Eff. 93, 69 (1986) M.Asghar, J.P.Bocquet, R.Brissot, M.Djebara, M.Maurel, H.Nifenecker, Ch.Ristori Quasi-Particle Excitations in Low Energy Fission NUCLEAR REACTIONS 229Th, 232U(n, F), E=thermal; measured fission fragment yield vs mass; deduced proton odd-even effect. 230Th, 233U deduced quasiparticle excitations.
doi: 10.1080/00337578608207432
1986BA24 Radiat.Eff. 93, 73 (1986) G.Barreau, A.Sicre, F.Caitucoli, M.Asghar, T.P.Doan, B.Leroux, G.Martinez, T.Benfoughal Fission Fragment Energy Correlation Measurements for Cf-252(SF) RADIOACTIVITY 252Cf(SF); measured fission fragment energy correlation; deduced fragment yield, total kinetic energy vs mass.
doi: 10.1080/00337578608207433
1986CA14 Radiat.Eff. 92, 333 (1986) F.Caitucoli, M.Asghar, G.Barreau, B.Leroux, P.Perrin, M.Maurel, T.P.Doan, A.Sicre Fission Fragment Mass Energy Correlation for 13 Actinides ranging from Th to Cf RADIOACTIVITY 244Cm, 252Cf(SF); measured fission fragment yield vs mass, energy distribution; deduced potential energy surface role on cold fragmentation mass distributions. NUCLEAR REACTIONS 229Th, 231Pa, 232,233,235U, 237Np, 238,239,241Pu, 241,243Am(n, F), E=thermal; measured fission fragment yield vs mass, energy distribution; deduced potential energy surface role on cold fragmentation mass distributions. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23588. 1986HA15 Radiat.Eff. 93, 17 (1986) M.Haddad, J.Crancon, Ch.Hamelin, G.Lhospice, M.Asghar, J.Blachot Post-Neutron Mass Distribution for 232U(n(th), f) NUCLEAR REACTIONS 235U(n, F)85Kr/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/127Sb/129Sb/131I/132Te/133I/135Xe/138Cs/139Ba/140Ba/141Ce/142La/143Ce, E=thermal; measured fission fragment mass distribution, post-neutron residuals absolute mass yields.
doi: 10.1080/00337578608207419
1986SI10 Radiat.Eff. 93, 65 (1986) A.Sicre, G.Barreau, A.Boukellal, F.Caitucoli, T.P.Doan, B.Leroux, P.Geltenbort, F.Gonnenwein, A.Oed, M.Asghar High Resolution Study of U235(n(th), f) and Th229(n(th), f) with Cosi Fan Tutte Mass Spectrometer NUCLEAR REACTIONS 235U, 229Th(n, F), E=thermal; measured fission fragment correlated mass, kinetic energy, Z.
doi: 10.1080/00337578608207431
1985BA01 Nucl.Phys. A432, 411 (1985) G.Barreau, A.Sicre, F.Caitucoli, M.Asghar, T.P.Doan, B.Leroux, G.Martinez, T.Benfoughal Fission-Fragment Energy Correlation Measurements for 252Cf(sf) and Structures in Far-Out Asymmetric Fission RADIOACTIVITY 252Cf(SF); measured fission fragment energies; deduced fragment mass yield, kinetic energy, variances. Static macro-microscopic potential calculations.
doi: 10.1016/0375-9474(85)90251-9
1985SI22 Nucl.Phys. A445, 37 (1985) A.Sicre, T.Benfoughal, B.Bruneau, M.Asghar, G.Barreau, F.Caitucoli, T.P.Doan, G.D.James, B.Leroux Fission-Fragment Angular Distributions for 230Th(n, F) in the vicinity of the 715 keV Resonance NUCLEAR REACTIONS 230Th(n, F), E=692.5-740 keV; measured fission fragment σ(θ); deduced triple-humped fission barrier parameters. 231Th deduced levels, J, π, rotational bands, moment of inertia. Statistical model analysis.
doi: 10.1016/0375-9474(85)90359-8
1984DJ02 Nucl.Phys. A425, 120 (1984) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, M.Maurel, H.Nifenecker, Ch.Ristori Measurement of Charge Distributions for 229Th(n(th), f) and 232U(n(th), f) NUCLEAR REACTIONS 229Th, 232U(n, F), E=thermal; measured fission fragment charge yields, correlations with kinetic energy; deduced yields, most probable kinetic energies odd-even effect.
doi: 10.1016/0375-9474(84)90219-7
1984EM01 Z.Phys. A315, 201 (1984) A.Emsallem, M.Asghar, P.D'Hondt, C.Wagemans Thermal Neutron Induced α-Particle Reaction on 64, 65, 67Zn and 77Se NUCLEAR REACTIONS 64,65,67Zn, 77Se(n, α), E=thermal; measured σ(Eα). 65,66,68Zn, 78Se deduced resonances contributing to α-decay. 61,62,64Ni, 74Ge levels deduced α-branching. Natural, enriched, radioactive targets.
doi: 10.1007/BF01419380
1983CA02 Nucl.Phys. A394, 360 (1983) F.Caitucoli, M.Asghar, B.Leroux, G.Barreau, K.Hamadache, A.Sicre, T.P.Doan, M.Allab Fission-Fragment Energy Correlation Measurements for the Spontaneous Fission of 244Cm RADIOACTIVITY 244Cm(SF); measured complementary fission fragment kinetic energies, mass distribution yields; deduced mean values, rms widths, fission fragment mass vs energy correlations.
doi: 10.1016/0375-9474(83)90109-4
1983LE04 Nucl.Instrum.Methods 206, 235 (1983) B.Leroux, F.Caitucoli, P.Audouard, M.Asghar, G.Barreau, T.P.Doan, A.Sicre A Pile-Up Correction Method for Fission Work with Active Targets RADIOACTIVITY 244Cm(α), (SF); measured mean fission fragment kinetic energy vs heavy fragment provisional mass. Off-line pileup correction techniques.
doi: 10.1016/0167-5087(83)91264-4
1983RA11 Nucl.Phys. A398, 544 (1983) V.S.Ramamurthy, M.Asghar, S.K.Kataria Mean Distribution of Single-Particle Levels in Thin-Skinned Potential Wells and the Macroscopic Level Density Parameters of Nuclei NUCLEAR STRUCTURE A ≈ 27-220; calculated level density parameter. Thin skinned potential well single particle level densities, droplet model potential parameters.
doi: 10.1016/0375-9474(83)90301-9
1982AS02 Nucl.Phys. A373, 225 (1982) M.Asghar, F.Caitucoli, B.Leroux, M.Maurel, P.Perrin, G.Barreau Fission Fragment Energy Correlation Measurements for 229Th(n(th), f) NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; measured fragment kinetic energy vs mass, total fission fragment kinetic energy rms width vs heavy fragment mass; deduced mass 144 dominance.
doi: 10.1016/0375-9474(82)90148-8
1981AS08 Nucl.Phys. A368, 319 (1981) M.Asghar, F.Caitucoli, B.Leroux, M.Maurel, P.Perrin, G.Barreau Fission Fragment Energy Correlation Measurements for 238Pu(n(th), f) NUCLEAR REACTIONS, Fission 238Pu(n, F), E=thermal; measured E(fragment); deduced total kinetic energy, rms width vs heavy fragment mass.
doi: 10.1016/0375-9474(81)90687-4
1981AS09 Nucl.Phys. A368, 328 (1981) M.Asghar, F.Caitucoli, B.Leroux, P.Perrin, G.Barreau Fission-Fragment Energy Correlation Measurements for (n(th), f) of 232U and 233U NUCLEAR REACTIONS, Fission 232,233U(n, F), E=thermal; measured fragment mass, kinetic energy correlations; deduced total kinetic energy, rms width vs heavy fragment mass.
doi: 10.1016/0375-9474(81)90688-6
1981CA13 Nucl.Phys. A369, 15 (1981) F.Caitucoli, C.Wagemans, P.Perrin, E.Allaert, P.D'Hondt, M.Asghar Mass and Energy Characteristics of the 241Pu(n(th), f) Fragments NUCLEAR REACTIONS, Fission 241Pu(n, F), E=thermal; measured fragment kinetic energies; deduced energy, mass distributions, mass-energy correlations.
doi: 10.1016/0375-9474(81)90003-8
1981EM03 Nucl.Phys. A368, 108 (1981) A.Emsallem, M.Asghar, C.Wagemans, H.Weigmann Study of Neutron Induced Charged Particle Reactions on 40K. (I). Thermal Neutrons NUCLEAR REACTIONS 40K(n, α), (n, p), E=thermal; measured Eα, E(p), σ(Eα), σ(Ep); deduced Q(p), primary gamma-ray multipolarity.
doi: 10.1016/0375-9474(81)90733-8
1981WE12 Nucl.Phys. A368, 117 (1981) H.Weigmann, C.Wagemans, A.Emsallem, M.Asghar Study of Neutron Induced Charged Particle Reactions on 40K. (II). Resonance Neutrons NUCLEAR REACTIONS 40K(n, α), (n, p), E=0.00002-70 keV; measured σ(Eα), σ(Ep). 41K deduced resonances, L, J, π, < Γp >, < Γα >, level density spin cut-off parameter.
doi: 10.1016/0375-9474(81)90734-X
1980AS03 Nucl.Phys. A334, 327 (1980) M.Asghar, F.Caitucoli, P.Perrin, G.Barreau, B.Leroux Fission Fragment Energy Correlation Measurements for the Sub-Barrier (n(th), f) of 241Am and 243Am NUCLEAR REACTIONS 241,243Am(n, F), E=thermal; measured complementary fragment kinetic energies; deduced average total kinetic energy, rms width vs fragment A.
doi: 10.1016/0375-9474(80)90072-X
1980AS05 Nucl.Phys. A341, 388 (1980) M.Asghar, F.Caitucoli, P.Perrin, T.P.Doan, G.Barreau, B.Leroux Structures in Far-Out Asymmetric Mass Distributions in Low Energy Fission RADIOACTIVITY 252Cf (SF); measured fragment energies; deduced fragment mass yields. NUCLEAR REACTIONS 235U, 239Pu, 243Am(n, F), E=th; measured fragment energies; deduced fragment mass yields.
doi: 10.1016/0375-9474(80)90372-3
1980CA25 Z.Phys. A298, 219 (1980) F.Caitucoli, B.Leroux, G.Barreau, N.Carjan, T.Benfoughal, T.P.Doan, F.El Hage, A.Sicre, M.Asghar, P.Perrin, G.Siegert The Thermal-Neutron-Induced Alpha-Accompanied Fission of 235U Investigation of the Low Energy Part of the Alpha Spectrum NUCLEAR REACTIONS, Fission 235U(n, αF), E=thermal; measured σ(Eα); deduced asymmetry at low energies, multiplicative factor relative to binary fission.
1979GU02 Nucl.Phys. A314, 1 (1979) C.Guet, C.Signarbieux, P.Perrin, H.Nifenecker, M.Asghar, F.Caitucolli, B.Leroux A Detailed Investigation of the Thermal Neutron Induced Ternary Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured ternary fission, Eα, σ(θα), fragment energy, mass; deduced correlations.
doi: 10.1016/0375-9474(79)90551-7
1978AN14 Phys.Scr. 18, 165 (1978) G.Andersson, M.Asghar, A.Emsallem, E.Hagberg, B.Jonson, P.Tidemand-Petersson Study of the Reaction 76Br(n(th), p)76Se NUCLEAR REACTIONS 76Br(n, p), E=th; measured σ; deduced Q. 77Br level deduced proton decay.
doi: 10.1088/0031-8949/18/3/002
1978AS01 Nucl.Phys. A298, 13 (1978) Fission Fragment Yield Distributions as a Function of their Excitation Energies for 235U(n(th), f) NUCLEAR REACTIONS 235U(n, F), E=th; measured fragment energies; deduced fragment mass versus energy correlations.
doi: 10.1016/0375-9474(78)90003-9
1978AS02 Z.Phys. A286, 299 (1978) The Sub-Barrier Photo-Fission and the 232Th Fission Barrier Profile NUCLEAR REACTIONS 232Th(γ, F), E=sub-barrier MeV; analyzed data.
doi: 10.1007/BF01408260
1978AS06 Z.Phys. A288, 45 (1978) M.Asghar, A.Emsallem, E.Hagberg, B.Jonson, P.Tidemand-Petersson Thermal Neutron Induced Charged Particle Reactions in Radioactive Targets of 37Ar, 109Cd, 125Xe, 127Xe, and 132Cs NUCLEAR REACTIONS 37Ar(n, p), 37Ar, 109Cd, 125,127Xe, 132Cs(n, α), E=thermal; measured Q, Γα/Γp; deduced σ. Isotopically pure targets. Si surface barrier detector.
doi: 10.1007/BF01408200
1978AS08 Nucl.Phys. A311, 205 (1978) M.Asghar, F.Caitucoli, P.Perrin, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Fission of 239Pu and 235U NUCLEAR REACTIONS 239Pu, 235U(n, F), E=thermal; measured reaction products; deduced complementary fragment kinetic energies, fragment mass-versus energy correlations.
doi: 10.1016/0375-9474(78)90510-9
1978AS09 Nucl.Phys. A311, 413 (1978) M.Asghar, F.Caitucoli, P.Perrin, C.Guet, P.D'Hondt, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Sub-Barrier Fission of 231Pa NUCLEAR REACTIONS 235U, 231Pa(n, F), E=th; measured complementary fragment kinetic energies; deduced fragment mass-versus-energy correlations.
doi: 10.1016/0375-9474(78)90522-5
1978CR03 Z.Phys. A287, 45 (1978) J.Crancon, C.Ristori, H.Ohm, W.Rudolph, K.-L.Kratz, M.Asghar Half-Lives and P(n) Values of Delayed-Neutron Precursors in the Mass Chains 85-87, 92, 135, 136 and 145 RADIOACTIVITY 85,86,87As, 92Br, 135,136Sb, 136Te, 145Cs; measured T1/2, neutron emission probability. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23352. 1978DH01 Nucl.Phys. A303, 275 (1978) P.D'Hondt, A.De Clercq, A.J.Deruytter, C.Wagemans, M.Asghar, A.Emsallem Study of α-Particles Produced in Thermal Neutron Induced Reactions on 235U NUCLEAR REACTIONS 235U(n, F), 235U(n, α), E=thermal; measured fission α-distribution, σ(n, α).
doi: 10.1016/0375-9474(78)90358-5
1978EM01 Z.Phys. A286, 411 (1978) A.Emsallem, M.Asghar, C.Wagemans, P.D'hondt Search for the (n(th), α) Reaction on 180Hf, 181Ta and 209Bi NUCLEAR REACTIONS 180Hf, 181Ta, 209Bi(n, α), E=th; measured σ(Eα).
doi: 10.1007/BF01408899
1978GU22 J.Phys.(Paris), Lett. 39, L-213 (1978) C.Guet, C.Signarbieux, P.Perrin, H.Nifenecker, B.Leroux, M.Asghar Evidence for Quasi-Static Scission Configurations Obtained from Long Range Particle Accompanied Fission Distributions NUCLEAR REACTIONS 236U(n, F), E=th; measured σ(θα), widths. Comparison with 252Cf(SF). Semi-equilibrium model for scission.
doi: 10.1051/jphyslet:019780039013021300
1978ST02 Z.Phys. A284, 95 (1978) R.Stippler, F.Munnich, H.Schrader, J.P.Bocquet, M.Asghar, G.Siegert, R.Decker, B.Pfeiffer, H.Wollnik, E.Monnand, F.Schussler Experimental Beta-Decay Energies of Short-Lived Light Fission Products RADIOACTIVITY 88Br, 90,92Kr, 90,92,93Rb, 93,95,96,97,98Sr, 96,97,97m,98,98mY, 98,100,101,102Nb, 99,100Zr; measured Eβ; deduced Qβ.
doi: 10.1007/BF01433881
1978WA15 Ann.Nucl.Energy 5, 267 (1978) C.Wagemans, M.Asghar, F.Caitucoli, P.Perrin, P.D'Hondt, A.J.Deruytter Measurement of the Thermal Neutron-Induced Fission Cross-Section of 231Pa NUCLEAR REACTIONS 231Pa(n, F), E=thermal; measured σ.
doi: 10.1016/0306-4549(78)90079-8
1977AS02 Z.Phys. A282, 375 (1977) M.Asghar, A.Emsallem, N.G.Sjostrand Thermal Neutron Induced Charged Particle Reactions on 58,59,61Ni NUCLEAR REACTIONS 58,59,61Ni(n, α), 59Ni(n, p), E=th; measured σ. 60Ni levels deduced α-, p-branching, nature of low energy primary transitions. Enriched targets.
doi: 10.1007/BF01434292
1977AS08 Nucl.Phys. A292, 225 (1977) M.Asghar, P.D'Hondt, C.Guet, P.Perrin, C.Wagemans Fission Fragment Energy Correlation Measurements for the Thermal Neutron Sub-Barrier Fission of 237Np and Above-the-Barrier Fission of 235U NUCLEAR REACTIONS 237Np, 235U(n, F), E=th; measured complementary fragment kinetic energies; deduced average kinetic energies, σ, fragment mass versus energy correlations.
doi: 10.1016/0375-9474(77)90370-0
1977PF01 J.Phys.(Paris) 38, 9 (1977) B.Pfeiffer, J.P.Bocquet, J.A.Pinston, R.Roussille, M.Asghar, G.Bailleul, R.Decker, J.Greif, H.Schrader, G.Siegert, H.Wollnik, J.Blachot, E.Monnand, F.Schussler Gamma Spectroscopy of Some Short-Lived Fission Products with the Isotope Separator Lohengrin RADIOACTIVITY 100Y, 100Zr, 149,150Ce, 150Pr, 136Te, 87Se; measured Eγ, Iγ, T1/2. 149Pr, 135,137Te, 86Se; measured Eγ, Iγ. 88Se; measured Eγ, Iγ; deduced ground state β-branching. 85Se; measured Eγ, Iγ, T1/2; deduced ground state β-branching.
doi: 10.1051/jphys:019770038010900
1977WA09 Nucl.Phys. A285, 32 (1977) C.Wagemans, M.Asghar, P.D'Hondt, A.J.Deruytter, A.Emsallem Study of Some Characteristics of the Thermal-Neutron-Induced Sub-Barrier Fission of 231Pa, 232Th and 237Np NUCLEAR REACTIONS 231Pa, 232Th, 237Np(n, F), E=th; measured σ, average kinetic energy, long range alphas/binary fission.
doi: 10.1016/0375-9474(77)90144-0
1976AN05 Phys.Lett. 61B, 234 (1976) G.Andersson, M.Asghar, A.Emsallem, E.Hagberg, B.Jonson Observation of Proton Emission Following Thermal Neutron Capture in 34.5 d 84Rb NUCLEAR REACTIONS 84Rb(n, p), E=th; measured Ep, Ip; deduced Q. 85Rb deduced proton branching. 84Kr deduced levels, Γp.
doi: 10.1016/0370-2693(76)90137-4
1976AN22 Phys.Lett. B 61, 234 (1976) G.Anderson, M.Asghar, A.Emsallem, E.Hagberg, B.Jonson Observation of Proton Emission Following Thermal Neutron Capture in 3 4.5-D 84Rb NUCLEAR REACTIONS 84Rb(n, p), E=0.0253 eV; measured products, Ep, Ip; deduced σ, σ(E). Data were imported from EXFOR entry 22600.
doi: 10.1016/0370-2693(76)90137-4
1976AS02 Nucl.Phys. A259, 429 (1976) M.Asghar, A.Emsallem, R.Chery, C.Wagemans, P.D'Hondt, A.J.Deruytter The 238U(n, α)235Th Reaction with Thermal Neutrons NUCLEAR REACTIONS 238U(n, α), E=thermal; measured σ(Eα); deduced Q. 235Th deduced mass, Qβ.
doi: 10.1016/0375-9474(76)90078-6
1976KR18 Phys.Lett. 65B, 231 (1976) K.-L.Kratz, W.Rudolph, H.Ohm, H.Franz, G.Herrmann, C.Ristori, J.Crancon, M.Asghar, G.I.Crawford, F.M.Nuh, S.G.Prussin Decay of Individual Levels in Delayed Neutron Emitters to Excited States in the Final Nuclei RADIOACTIVITY 85As, 135Sb, 94Rb; measured β-delayed neutrons, γ spectra. 135Te levels deduced delayed neutron branching. 134Te deduced levels.
doi: 10.1016/0370-2693(76)90170-2
1976RI06 Z.Phys. A277, 71 (1976) C.Ristori, M.Asghar, J.Crancon, J.P.Gautheron Nuclear Charge Distributions from 4π-β Measurements on Mass Separated Fragments from 235U(n(th), f) NUCLEAR REACTIONS 235U(n, F), E=th; measured β-activity of A=91, 93, 94, 95, 137, 139; deduced nuclear charge distributions, σ(Z).
doi: 10.1007/BF01547504
1976RI12 Z.Phys. A 277, 71 (1976) C.Ristori, M.Asghar, J.Crancon, J.P.Gautheron Nuclear Charge Distributions From 4π-β Measurements On Mass Separated Fragments From 235U (nth, f) NUCLEAR REACTIONS 235U(n, f), E=0.0253 eV; measured products, 139Cs, 139Xe, 137Xe, 139I, 137Te, 137I, 95Y, 95Sr, 94Sr, 93Sr, 95Rb, 94Rb, 93Rb, 91Rb, 94Kr, 93Kr, 91Kr, 91Br; deduced yields. Data were imported from EXFOR entry 21556.
doi: 10.1007/BF01547504
1976WA04 Nucl.Phys. A259, 423 (1976) C.Wagemans, P.D'Hondt, A.J.Deruytter, A.Emsallem, M.Asghar The Thermal Neutron Induced Fission Cross Section of 232Th NUCLEAR REACTIONS 232Th(n, F), E=thermal; measured, calculated σ(n, F).
doi: 10.1016/0375-9474(76)90077-4
1975AS03 J.Inorg.Nucl.Chem. 37, 1563 (1975) M.Asghar, J.Crancon, J.P.Gautheron, C.Ristori Delayed Neutron Emission Probabilities of 92,93Kr, 92,93Rb, 141,142Xe and 141,142Cs Precursors RADIOACTIVITY 92,93Kr, 92,93Rb, 141,142Xe, 141,142Cs; measured delayed neutrons, β-activity; deduced probability of neutron emission.
doi: 10.1016/0022-1902(75)80277-6
1975AS04 Nucl.Phys. A247, 359 (1975) M.Asghar, J.P.Gautheron, G.Bailleul, J.P.Bocquet, J.Greif, H.Schrader, G.Siegert, C.Ristori, J.Crancon, G.I.Crawford The p(n) Values of the 235U(n(th), f) Produced Precursors in the Mass Chains 90, 91, 93-95, 99, 134 and 137-139 RADIOACTIVITY 90,91Br, 91Se, 93,94Kr, 93,94,95Rb, 99Y, 99Sr, 134Sn, 137,138Te, 137,138,139I [from 235U(n, F), E=thermal]; measured delayed neutrons, β-activity, T1/2; deduced delayed neutron probability.
doi: 10.1016/0375-9474(75)90642-9
1975AS05 J.Inorg.Nucl.Chem. 37, 2229 (1975) M.Asghar, J.Crancon, J.P.Gautheron, C.Ristori Delayed Neutron Emission Probabilities of 92,93Kr, 92,93Rb, 141,142Xe and 141,142Cs Precursors RADIOACTIVITY 92,93Kr, 92,93Rb, 141,142Xe, 141,142Cs; measured delayed neutron emission probabilities.
doi: 10.1016/0022-1902(75)80715-9
1975BA36 Z.Phys. A273, 283 (1975) G.Bailleul, J.P.Bocquet, H.Schrader, R.Stippler, B.Pfeiffer, M.Asghar, C.Chauvin, J.P.Gautheron, J.Greif, G.Siegert, P.Armbruster, H.Ewald, J.Blachot, E.Monnand, F.Schussler Gamma-Ray Spectroscopy of Short-Lived Fission Products Using the Recoil Separator 'Lohengrin' RADIOACTIVITY 90Br, 95,96Rb, 96Sr, 96Y, 132Sb, 132Sn; measured T1/2, Eγ, Iγ. 96Sr; measured Eβ; deduced Qβ. 90Kr, 95,96Sr, 96Y deduced levels.
doi: 10.1007/BF01410011
1975CL02 Nucl.Phys. A247, 74 (1975) H.-G.Clerc, K.-H.Schmidt, H.Wohlfarth, W.Lang, H.Schrader, K.E.Pferdekamper, R.Jungmann, M.Asghar, J.P.Bocquet, G.Siegert Nuclear Charge Distribution of Mass-Separated Isobars from Thermal-Neutron-Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured nuclear charge distributions of fission products; deduced nuclear charge distribution widths; on-line mass separation.
doi: 10.1016/0375-9474(75)90278-X
1975EM04 Z.Phys. A275, 157 (1975) The (n(th), α)-Reaction on 95Mo, 123Te and 145Nd NUCLEAR REACTIONS 95Mo, 123Te, 145Nd(n, α), E=thermal; measured σ(Eα). 96Mo, 124Te, 146Nd levels deduced α-branching ratios, Γα.
doi: 10.1007/BF01409591
1975EM05 Z.Phys. A 275, 157 (1975) The (n th, α)-Reaction On 95Mo, 123Te, and 145Nd NUCLEAR REACTIONS 95Mo(n, α), 123Te(n, α), 145Nd(n, α), E=0.0253 eV; measured products, 92Zr, 2-HE-4, 120Sn, 142Ce. Data were imported from EXFOR entry 20612.
doi: 10.1007/BF01409591
1975SI04 Phys.Rev.Lett. 34, 1034 (1975) G.Siegert, J.Greif, H.Wollnik, G.Fiedler, R.Decker, M.Asghar, G.Bailleul, J.P.Bocquet, J.P.Gautheron, H.Schrader, P.Armbruster, H.Ewald Nuclear Charge Distributions in the Isobars 92 to 100 Resulting from Thermal Neutron Fission of Uranium-235 NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fractional yields; deduced nuclear charge distribution in isobars A=92-100.
doi: 10.1103/PhysRevLett.34.1034
1974CR06 J.Phys.(London) A7, L141 (1974) G.I.Crawford, S.J.Hall, J.D.Kellie, M.Asghar, G.Bailleul, J.P.Bocquet, C.Chauvin, J.P.Gautheron, H.Schrader, G.Siegert, J.Crancon, C.Ristori Population of Excited States in Delayed Neutron Emission RADIOACTIVITY 85As, 90Br, 95Rb; measured nγ-coin. 94Sr, 89Kr deduced levels.
doi: 10.1088/0305-4470/7/12/001
1974EM01 Nucl.Phys. A231, 437 (1974) A.Emsallem, Do Huu Phuoc, R.Chery, M.Asghar The (n, α) Reaction on 147Sm, 151,153Eu and Yb Isotopes NUCLEAR REACTIONS 147Sm, 151,153Eu, 168,170,171,172,173,176Yb(n, α), E=thermal; measured σ(Eα). 148Sm, 152Eu levels deduced α-branching ratios. Enriched, natural targets.
doi: 10.1016/0375-9474(74)90507-7
1974SI23 Phys.Lett. 53B, 45 (1974) G.Siegert, H.Wollnik, J.Greif, G.Fiedler, M.Asghar, G.Bailleul, J.P.Bocquet, J.P.Gautheron, H.Schrader, H.Ewald, P.Armbruster Direct Determination of the Nuclear Charge Distribution of Mass Separated Fission Products from 235U(n(th), f) NUCLEAR REACTIONS 235U(n, F), E=thermal; measured charge distribution of A=90-91 isobaric chains.
doi: 10.1016/0370-2693(74)90339-6
1970AS03 Nucl.Phys. A145, 549 (1970) M.Asghar, P.Ribon, E.Silver, J.Trochon The Spins of Low-Energy Neutron Resonances of 155Gd and 157Gd NUCLEAR REACTIONS 155Gd(n, n), E < 70 eV; 157Gd(n, n), E < 240 eV; 155,157Gd(n, γ), E<90 eV; measured σ(E). 156,158Gd deduced resonances, J. Enriched 157Gd target.
doi: 10.1016/0375-9474(70)90440-9
1970AS04 Nucl.Phys. A145, 657 (1970) M.Asghar, C.Carles, R.Chastel, T.P.Doan, M.Ribrag, C.Signarbieux A Multi-Parameter Study of LRA Fission and Binary Fission of 235U with Thermal Neutrons NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured fragment energy, mass distributions for binary, long-range-α ternary fission; deduced α-emission probability.
doi: 10.1016/0375-9474(70)90446-X
1970DO12 J.Phys.(Paris) 31, 929 (1970) T.P.Doan, M.Asghar, C.Carles, R.Chastel Probabilite d'Emission de Particules Alpha au Cours de la Fission NUCLEAR STRUCTURE 236U, 252Cf; calculated α-emission probability.
doi: 10.1051/jphys:019700031011-12092900
1969IR01 Nucl.Phys. A136, 631 (1969) J.L.Irigaray, M.Asghar, J.Dalmas, G.Y.Petit, J.Roturier The 89Y(p, γ)90Zr, 88Sr(p, γ)89Y and 86Sr(p, γ)87Y Reactions with 4 MeV Protons NUCLEAR REACTIONS 86,88Sr, 89Y(p, γ), E = 3930 keV; measured σ(Eγ); deduced Q. 87,89Y, 90Zr deduced levels, proton separation energy.
doi: 10.1016/0375-9474(69)90134-1
1969TR10 Nucl.Instr.Methods 72, 307 (1969) J.Trochon, M.Asghar, B.Lucas, P.Ribon Etude d'un Detecteur pour des Mesures de Diffusion Elastique de Neutrons de Resonances NUCLEAR REACTIONS 103Rh, 197Au(n, n), E < 2300 eV; measured σ(E).
doi: 10.1016/0029-554X(69)90517-5
1968AS02 Nucl.Phys. A108, 535(1968) M.Asghar, C.M.Chaffey, M.C.Moxon The Neutron Resonance Parameters and Average Capture Cross Section of 165Ho NUCLEAR REACTIONS 165Ho(n, γ), E = 2.5 to 105 eV; 165Ho(n, n), E = 35 to 750 eV; measured σ(E). 166Ho deduced resonance parameters.
doi: 10.1016/0375-9474(68)90322-9
1968AS04 Phys.Letters 26B, 664 (1968) An Attempt to Determine the Spins of 235U Slow Neutron Resonances NUCLEAR STRUCTURE 235U; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90383-3
1967AS01 Nucl.Phys. A98, 33(1967) Spin Assignments of Low-Energy Resonances in 239Pu NUCLEAR REACTIONS 239Pu(n, n), E = 14.7 to 300 eV; measured σ(ns)(E). 240Pu deduced resonance spins.
doi: 10.1016/0375-9474(67)90896-2
1966AS07 Nucl.Phys. 76, 196(1966) M.Asghar, C.M.Chaffey, M.C.Moxon, N.J.Pattenden, E.R.Rae, C.A.Uttley The Neutron Cross Sections of Thorium and the Analysis of the Resonances up to 1 keV NUCLEAR REACTIONS Th(n, γ), Th(n, n), E = 15 eV - 1 keV; measured σ(nt), σ(nn), σ(nγ); n-width, γ-width.
doi: 10.1016/0029-5582(66)90969-2
1966AS09 Nucl.Phys. 85, 305(1966) M.Asghar, C.M.Chaffey, M.C.Moxon Low-Energy Neutron Resonance Parameters of 238U NUCLEAR REACTIONS 238U(n, γ), (n, n), E = 5 to 1000 eV; measured σ(nγ)(E), σ(nn)(E). 239U deduced resonance parameters.
doi: 10.1016/0029-5582(66)90626-2
1966AS13 Proc.Intern.Conf.Study of Nucl.Struct.with Neutrons, Antwerp, Belgium (1965), M.N.De Mevergnies, P.Van Assche, J.Vervier, Eds., North-Holland Publishing Co., Amsterdam, p.522 (1966); EANDC-50-S, Paper 65 M.Asghar, M.C.Moxon, C.M.Chaffey The Low Energy Neutron Resonance Parameters of 107,109Ag, 169Tm, 197Au, 159Tb and 165Ho NUCLEAR STRUCTURE 198Au, 166Ho, 170Tm, 160Tb, 110Ag, 108Ag; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21492. 1962BR31 Conf.Low Energy Nuclear Phys., Harwell, AERE-R-4131, p.25, 8a.1 (September 1962) NUCLEAR STRUCTURE 198Au, 169Tm; measured not abstracted; deduced nuclear properties.
Back to query form |