NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.I.Muminov Found 47 matches. 2015TA14 Phys.Rev. C 91, 054612 (2015) R.B.Tashkhodjaev, A.I.Muminov, A.K.Nasirov, W.von Oertzen, Y.Oh Theoretical study of the almost sequential mechanism of true ternary fission RADIOACTIVITY 252Cf(SF); calculated yield contours of massive clusters in ternary fission, potential-energy surface in (Z1, Z3) plane and collinear cluster tripartition (CCT), contour map of the calculated velocity of the middle fragment Z3. Collinear sequential ternary fission. Relevance to experiments by FOBOS group at FLNR-JINR facility.
doi: 10.1103/PhysRevC.91.054612
2014NA11 Phys.Scr. 89, 054022 (2014) A.K.Nasirov, W.von Oertzen, A.I.Muminov, R.B.Tashkhodjaev Peculiarities of cluster formation in true ternary fission of 252Cf and 236U* NUCLEAR REACTIONS 236U(n, F), E thermal; calculated ternary fission product distributions, potential energy surface; deduced nucleus-nucleus interaction potential. RADIOACTIVITY 252Cf(SF); calculated ternary fission product distributions, potential energy surface.
doi: 10.1088/0031-8949/89/5/054022
2011NA31 Phys.Rev. C 84, 044612 (2011) A.K.Nasirov, G.Mandaglio, G.Giardina, A.Sobiczewski, A.I.Muminov Effects of the entrance channel and fission barrier in the synthesis of superheavy element Z=120 NUCLEAR REACTIONS 249Bk(48Ca, X)297Ts, E(cm)=193-222 MeV; 249Cf(50Ti, X)299120, E(cm)=217-251 MeV; 248Cm(54Cr, X)302120, E(cm)=226-263 MeV; calculated cross sections for capture, quasifission, fast fission, complete fusion, evaporation residues. Comparison with experimental data for 3n- and 4n channels in 249Bk(48Ca, X). Dinuclear system and advanced statistical model calculations.
doi: 10.1103/PhysRevC.84.044612
2010NA09 Phys.Lett. B 686, 72 (2010) A.K.Nasirov, G.Mandaglio, M.Manganaro, A.I.Muminov, G.Fazio, G.Giardina Quasifission and difference in formation of evaporation residues in the 16O + 184W and 19F + 181Ta reactions NUCLEAR REACTIONS 181Ta(19F, X), 184W(16O, X), E(cm)=65-120 MeV; analyzed fusion, fission and evaporation residue σ, ratios and reaction mechanism features, L-dependence using statistical model for a dinuclear system.
doi: 10.1016/j.physletb.2010.02.018
2010NA27 J.Phys.:Conf.Ser. 205, 012018 (2010) A.K.Nasirov, A.I.Muminov, G.Giardina, G.Mandaglio, M.Manganaro Mixing of fusion-fission and quasifission products in reaction with massive nuclei NUCLEAR REACTIONS 154Sm(48Ca, X), E(cm)=140, 160 MeV; calculated mass distribution, σ, rotational angle time development. 238U(64Ni, 3n), (64Ni, 4n), (64Ni, 5n), (64Ni, X), E(cm)=265-285 MeV;244Pu(58Fe, 2n), (58Fe, 3n), (58Fe, 4n), (58Fe, 5n), (58Fe, X), E(cm)=245-270 MeV;248Cm(54Cr, 2n), (54Cr, 3n), (54Cr, 4n), (54Cr, 5n), (54Cr, X), E(cm)=230-285 MeV; calculated fusion σ, quasifission σ, fast fission σ, ER σ. Calculations based on dinuclear system and advanced statistical model.
doi: 10.1088/1742-6596/205/1/012018
2009NA01 Phys.Rev. C 79, 024606 (2009) A.K.Nasirov, G.Giardina, G.Mandaglio, M.Manganaro, F.Hanappe, S.Heinz, S.Hofmann, A.I.Muminov, W.Scheid Quasifission and fusion-fission in reactions with massive nuclei: Comparison of reactions leading to the Z = 120 element NUCLEAR REACTIONS 144Sm(48Ca, xn), E=130-180 MeV; 154Sm(48Ca, xn), $E=125-190 MeV; 186W(16O, xn), E not given; 238U(64Ni, xn), E=262-284 MeV; 244Pu(58Fe, xn), E=246-271 MeV; 248Cm(54Cr, xn), E=230-260 MeV; 249Cf(48Ca, xn), E=190-230 MeV; calculated excitation functions, cross sections and yields for evaporation residues, fusion-fission and quasifission fragments using dinuclear system and advanced statistical model. Comparison with experimental data. Discussed suitable reactions for the formation of Z=120 element.
doi: 10.1103/PhysRevC.79.024606
2009NA38 Bull.Rus.Acad.Sci.Phys. 73, 1476 (2009); Izv.Akad.Nauk RAS, Ser.Fiz. 73, 1571 (2009) A.K.Nasirov, G.Fazio, S.Hofmann, G.Giardina, A.I.Muminov, G.Mandaglio, M.Manganaro, W.Scheid Comparison of the characteristics of the fusion-fission and quasifission products in reactions with heavy ions NUCLEAR REACTIONS 154Sm(48Ca, X), 248Cm(54Cr, X), 244Pu(58Fe, X), 238U(64Ni, X) E(cm)<280 MeV; analyzed fusion-fission product mass distribution, yields, σ for heavy ion reactions;calculated σ; deduced large value of σ of evaporation residues in the 248Cm + 54Cr reaction.
doi: 10.3103/S1062873809110112
2007NA24 J.Nucl.Radiochem.Sci. 8, 63 (2007) A.K.Nasirov, G.Giardina, A.I.Muminov, G.Mandaglio, R.K.Utamuratov Peculiarities of Nuclear Fusion in Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(70Zn, X), 238U(48Ca, X), E not given; calculated fusion cross sections, compared results to data. Studied the role of entrance channel.
doi: 10.14494/jnrs2000.8.63
2007NA34 Eur.Phys.J. A 34, 325 (2007) A.K.Nasirov, A.I.Muminov, R.K.Utamuratov, G.Fazio, G.Giardina, F.Hanappe, G.Mandaglio, M.Manganaro, W.Scheid Angular anisotropy of the fusion-fission and quasifission fragments NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 208Pb(19F, X), E(cm)=70-180 MeV; 208Pb(32S, X), E=160-280 MeV; analyzed capture, fusion and quasi-fission σ, angular anisotropy of fission fragments and charge distribution. Reaction mechanism discussed.
doi: 10.1140/epja/i2007-10504-5
2007UT01 Phys.Atomic Nuclei 70, 1485 (2007) R.K.Utamuratov, A.I.Muminov, A.K.Nasirov Eligibility of spherical-well approximation for calculations of nucleon-transfer matrix elements
doi: 10.1134/S1063778807090025
2005FA01 J.Phys.Soc.Jpn. 74, 307 (2005) G.Fazio, G.Giardina, A.Lamberto, C.Sacca, R.Palamara, A.I.Muminov, A.K.Nasirov, K.V.Pavliy, F.Hanappe, T.Materna, L.Stuttge Effect of the Entrance Channel on the Fission of the Compound Nucleus NUCLEAR REACTIONS 204Pb(16O, X), 124Sn(96Zr, X), 234U(20Ne, X), 176Yb(78Ge, X), 232U(24Mg, X), 192Os(64Ni, X), E* ≈ 10-100 MeV; calculated fusion σ, evaporation residue production, compound nucleus fission probability; deduced entrance channel effects.
doi: 10.1143/JPSJ.74.307
2005FA17 Phys.Rev. C 72, 064614 (2005) G.Fazio, G.Giardina, G.Mandaglio, R.Ruggeri, A.I.Muminov, A.K.Nasirov, Yu.Ts.Oganessian, A.G.Popeko, R.N.Sagaidak, A.V.Yeremin, S.Hofmann, F.Hanappe, C.Stodel Strong influence of the entrance channel on the formation of compound nuclei 216, 222Th* and their evaporation residues NUCLEAR REACTIONS 176Hf(40Ar, X), 130,136Xe(86Kr, X), 92Zr(124Sn, X), 174Yb(48Ca, X), E* ≈ 10-100 MeV; calculated capture and complete fusion σ; analyzed evaporation residue σ, related data; deduced entrance channel effects.
doi: 10.1103/PhysRevC.72.064614
2005PI04 Yad.Fiz. 68, 201 (2005); Phys.Atomic Nuclei 68, 177 (2005) V.P.Pikul, U.Yu.Jovliev, Yu.N.Koblik, A.V.Khugaev, A.I.Muminov, A.K.Nasirov, K.V.Pavliy, B.S.Yuldashev Analysis of Fragment Mass Distribution in Asymmetric Area at Fission of 235U Induced by Thermal Neutrons NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment mass yields, kinetic energy spectra; deduced shell effects. Dinuclear system model analysis.
doi: 10.1134/1.1866373
2004FA03 Eur.Phys.J. A 19, 89 (2004) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, C.Sacca, R.Palamara, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, F.Hanappe, T.Materna, L.Stuttge Formation of heavy and superheavy elements by reactions with massive nuclei NUCLEAR REACTIONS 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), E* ≈ 30-110 MeV; 181Ta(40Ar, X), E* ≈ 160-220 MeV; 248Cm(48Ca, X), E* ≈ 220-280 MeV; analyzed capture, fusion, evaporation residue σ; deduced entrance channel and shell structure effects. 248Cm, 243Am, 249Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E=220-270 MeV; calculated excitation functions.
doi: 10.1140/epja/i2003-10103-6
2004FA29 Eur.Phys.J. A 22, 75 (2004) G.Fazio, G.Giardina, A.Lamberto, A.I.Muminov, A.K.Nasirov, F.Hanappe, L.Stuttge The influence of the entrance channel dynamics on the evaporation residue formation NUCLEAR REACTIONS 204Pb(16O, X), 124Sn(96Zr, X), E* ≈ 10-100 MeV; calculated fusion, fission, evaporation residue σ; deduced entrance channel effects.
doi: 10.1140/epja/i2004-10030-0
2004GI11 Acta Phys.Hung.N.S. 19, 101 (2004) G.Giardina, G.Fazio, A.Lamberto, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, R.Palamara, R.Ruggeri Reactions of Massive Nuclei for the Synthesis of Heavy and Superheavy Nuclei NUCLEAR REACTIONS 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 20-130 MeV; analyzed fusion, evaporation residue σ, entrance channel effects.
doi: 10.1556/APH.19.2004.1-2.15
2004NA29 Acta Phys.Hung.N.S. 19, 109 (2004) A.K.Nasirov, G.Giardina, A.I.Muminov, W.Scheid, U.T.Yakhshiev Dynamics of Capture and Fusion in Heavy Ion Collisions NUCLEAR REACTIONS 244Pu(58Fe, X), E=330 MeV; calculated quasifission products mass distribution, driving potential, shell effects.
doi: 10.1556/APH.19.2004.1-2.16
2003FA08 Yad.Fiz. 66, 1107 (2003); Phys.Atomic Nuclei 66, 1071 (2003) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, F.Bonsignore, R.Palamara, A.I.Muminov, A.K.Nasirov, B.Benoit, F.Hanappe, T.Materna, L.Stuttge Synthesis of Heavy and Superheavy Elements by Reactions of Massive Nuclei NUCLEAR REACTIONS 176Hf(40Ar, X), 92Zr(124Sn, X), 130Xe(86Kr, X), 182W(32S, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 20-100 MeV; analyzed capture, fusion, and evaporation residue σ; deduced entrance channel effects. Dinuclear system approach.
doi: 10.1134/1.1586420
2003FA12 J.Phys.Soc.Jpn. 72, 2509 (2003) G.Fazio, G.Giardina, A.Lamberto, R.Ruggeri, C.Sacca, R.Palmara, A.I.Muminov, A.K.Nasirov, U.T.Yakhshiev, F.Hanappe, T.Materna, L.Stuttge Entrance Channel Effect on the Formation of Heavy and Superheavy Nuclei NUCLEAR REACTIONS 176Hf, 181Ta(40Ar, X), 92Zr(124Sn, X), 130Xe(86Kr, X), 182W(32S, X), 166Er(48Ti, X), 154Sm(60Ni, X), 248Cm(48Ca, X), E* ≈ 15-140 MeV; calculated fusion, capture, and evaporation residue σ; deduced entrance channel and shell structure effects.
doi: 10.1143/JPSJ.72.2509
2000GI09 Nucl.Phys. A671, 165 (2000) G.Giardina, F.Hanappe, A.I.Muminov, A.K.Nasirov, L.Stuttge Capture and Fusion Dynamics in Heavy-Ion Collisions NUCLEAR REACTIONS 107Ag(19F, X), 98Mo(28Si, X), E(cm)=40-210 MeV; calculated capture, fusion σ, spin distributions. Ag(40Ar, X)148Tb, E not given; calculated potential energy surface. Dynamical and statistical model, comparison with data.
doi: 10.1016/S0375-9474(99)00838-6
2000GI13 Eur.Phys.J. A 8, 205 (2000) G.Giardina, S.Hofmann, A.I.Muminov, A.K.Nasirov Effect of the Entrance Channel on the Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(50Ti, X), E=220-255 MeV; 208Pb(58Fe, X), E=275-292 MeV; 208Pb(64Ni, X), E=305-315 MeV; 209Bi(64Ni, X), E=310-320 MeV; 208Pb(70Zn, X), E=337-345 MeV; 209Bi(70Zn, X), E=338-355 MeV; 208Pb(76Ge, X), E=366-395 MeV; 208Pb(86Kr, X), E not given; calculated quasifission, fusion and evaporation residues σ, excitation energy; deduced entrance channel effects. Comparison with data, cold nuclear reactions. Dinuclear system approach.
doi: 10.1007/s100530050028
2000GI18 Bull.Rus.Acad.Sci.Phys. 64, 689 (2000) G.Giardina, P.D'Agostino, A.I.Muminov, A.K.Nasirov, G.Oliva, R.Palamara, R.Ruggeri, A.Taccone, G.Fazio, M.Herman Formation of Evaporation Residues in Synthesis of Superheavy Elements NUCLEAR REACTIONS 232Th, 238U, 244Pu(48Ca, F), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=215-255 MeV; calculated fusion, quasi-fission, evaporation residue σ, compound nucleus fission barrier vs bombarding energy. Dinuclear system concept, comparison with data.
2000JO13 Eur.Phys.J. A 8, 115 (2000) R.V.Jolos, A.K.Nasirov, G.G.Adamian, A.I.Muminov Effect of Shell Structure on Energy Dissipation in Heavy-Ion Collisions NUCLEAR REACTIONS 248Cm(40Ca, X), (48Ca, X), E not given; calculated light, heavy fragments excitation energies; deduced shell structure effects. Microscopic approach.
doi: 10.1007/s100500070125
1999GI17 Bull.Rus.Acad.Sci.Phys. 63, 745 (1999) G.Giardina, A.I.Muminov, A.K.Nasirov, F.Hanappe Competition between Quasifission and Fusion in Nucleus-Nucleus Collisions NUCLEAR REACTIONS Ag(40Ar, X), E=50-350 MeV; calculated capture, fusion and recoil nucleus formation σ. Quasifission, dinuclear system concept, comparison with data.
1999JO02 Eur.Phys.J. A 4, 245 (1999) R.V.Jolos, A.I.Muminov, A.K.Nasirov The Role of the Entrance Channel in the Fusion of Massive Nuclei NUCLEAR REACTIONS 244Pu(48Ca, X), E(cm)=190-220 MeV; 208Pb(74Ge, X), (76Ge, X), E(cm)=260-270 MeV; calculated capture σ, dinuclear system excitation energy. 282,284,292Fl; calculated driving potential for fusion, fusion barrier. Implications for superheavy element formation discussed.
doi: 10.1007/s100500050227
1997AD09 Phys.Rev. C56, 373 (1997) G.G.Adamian, R.V.Jolos, A.K.Nasirov, A.I.Muminov Friction Coefficient for Deep-Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 196Pt(64Zn, X), E=440 MeV; 208Pb(56Fe, X), E=480 MeV; 208Pb(64Ni, X), E=320 MeV; calculated nucleus-nucleus interaction potential, radial friction coefficients; deduced total kinetic energy losses vs time. Microscopic calculations, deep inelastic collisions.
doi: 10.1103/PhysRevC.56.373
1997AD16 Bull.Rus.Acad.Sci.Phys. 61, 155 (1997) G.G.Adamian, R.V.Jolos, A.I.Muminov, A.K.Nasirov Dynamics of Deep Inelastic Nuclear Collisions: Self-consistent calculation of kinetic coefficients NUCLEAR REACTIONS 196Pt(64Zn, X), E=440 MeV; calculated radial friction coefficient vs internuclear distance, total kinetic energy loss vs interaction time. 208Pb(56Fe, X), E=480 MeV; calculated radial friction coefficient vs internuclear distance. Microscopic approach.
1997AM10 Bull.Rus.Acad.Sci.Phys. 61, 614 (1997) I.P.Amankulov, B.K.Kuldzhanov, I.K.Kuldzhanov, A.I.Muminov, Sh.A.Shayusupov Angular Distributions of Prompt γ-Radiation in the Reaction 93Nb(α, 2n)95Tc NUCLEAR REACTIONS 93Nb(α, 2n), E=36 MeV; measured Eγ, Iγ(θ). 95Tc deduced levels, J, π, angular distribution coefficients.
1996AD01 Phys.Rev. C53, 871 (1996) G.G.Adamian, R.V.Jolos, A.K.Nasirov, A.I.Muminov Effects of Shell Structure and N/Z Ratio of a Projectile on the Excitation Energy Distribution between Interacting Nuclei in Deep-Inelastic Collisions NUCLEAR REACTIONS 248Cm(34Ar, X), (40Ar, X), (46Ar, X), E=280 MeV; 248Cm(40Ca, X), (44Ca, X), (48Ca, X), (54Ca, X), E=285 MeV; 40,48Ca(20Ne, X), (22Ne, X), E=150 MeV; 238U(40Ca, X), (48Ca, X), E=8 MeV/nucleon; calculated fragment excitation energy distribution vs energy loss, charge, mass distributions variances; deduced N/Z, shell effects role. Deep inelastic collisions.
doi: 10.1103/PhysRevC.53.871
1996AD05 Yad.Fiz. 59, No 1, 89 (1996); Phys.Atomic Nuclei 59, 82 (1996) G.G.Adamian, R.V.Jolos, A.I.Muminov, A.K.Nasirov Effect of the Ratio N/Z in a Projectile on the Distribution of Excitation Energy Among the Products of Deep-Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 248Cm(34Ar, X), (40Ar, X), (46Ar, X), (40Ca, X), (44Ca, X), (48Ca, X), (54Ca, X), 238U(40Ca, X), (48Ca, X), E not given; calculated products excitation energy, charge, mass distribution, deep inelastic collision; deduced projectile N/Z dependence related features.
1994AD15 Bull.Rus.Acad.Sci.Phys. 58, 60 (1994) G.G.Adamian, R.V.Jolos, A.I.Muminov, A.K.Nasirov Excitation Energy Distribution Over Heavy Ion Collision Products NUCLEAR REACTIONS 124Sn(238U, X), E=1.468 GeV; 110Pd(238U, X), E=1.398 GeV; 165Ho(56Fe, X), E=505 MeV; 165Ho(74Ge, X), E=629 MeV; 197Au(58Ni, X), E=880 MeV; calculated incident nucleus to composite system excitation energy ratio. Microscopic model.
1986JO13 Yad.Fiz. 44, 357 (1986) R.V.Jolos, A.I.Muminov, A.K.Nasirov Nuclear Structure Effect on Multinucleon-Transfer Reactions NUCLEAR REACTIONS 196Au(56Fe, X), E=460 MeV; 168Er(86Kr, X), E=515 MeV; 120Sn(132Xe, X), E=778 MeV; calculated product mass, charge distributions; deduced structure effects.
1985MU13 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 900 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.5, 60 (1985) A.I.Muminov, A.Akbarov, B.Ibragimov, O.I.Kochetov, I.K.Kuldzhanov, R.Razhabbaev γγ-Angular Correlations in 108Cd NUCLEAR STRUCTURE 108,106,110,112,114,116Cd; measured levels, B(E2). Quasiparticle-phonon model. RADIOACTIVITY 108In(β+), (EC); measured Eγ, Iγ, γγ(θ). 108Cd deduced levels, J, π, γ-multipolarity, δ, B(E2). Quasiparticle-phonon model.
1985ZH09 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2096 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 13 (1985) U.I.Zhovliev, V.G.Kiptilyi, M.F.Kudoyarov, I.Kh.Lemberg, A.I.Muminov, A.A.Pasternak, L.A.Rassadin Life Times and Structure of 83Rb Levels NUCLEAR REACTIONS 76Ge(10B, 3nγ), E=30 MeV; measured Eγ, Iγ, DSA. 83Rb deduced levels, T1/2, δ.
1984AK02 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 945 (1984); Bull.Acad.Sci.USSR, Phys..Ser. 48, 105 (1984) A.Akbarov, B.Ibragimov, I.K.Kuldzhanov, A.I.Muminov, R.Razhabbaev Study of γγ-Angular Correlation for Even-Even Sr Isotopes RADIOACTIVITY 84,86Y(EC), (β+); 88Rb(β-); measured γγ(θ). 84,86,88Sr levels deduced γ-multipolarity, B(E2).
1984BE59 Yad.Fiz. 40, 1131 (1984) A.D.Belyaev, Z.S.Bikbova, V.I.Kogan, A.I.Muminov, V.P.Pikul, A.M.Usmandiyar Structure of Product Mass Distributions from Thermal Neutron Induced Fission of 235U and 239Pu Nuclei at Fixed Energies of the Fission Products NUCLEAR REACTIONS 235U, 239Pu(n, F), E=thermal; measured fission fragment relative mass yields, total kinetic energy distribution. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31798. 1984VY02 Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 1809 (1984) Ts.Vylov, V.B.Brudanin, V.M.Grorozhankin, K.Ya.Gromov, A.Marinov, A.Minkova, A.I.Muminov, V.N.Pokrovsky Measurement of Neutrino Helicity in the Decay of 152mEu with the Aid of Ge(Li)-Detector RADIOACTIVITY 152mEu(β-), (β+), (EC) [from 151Eu(n, γ), E=reactor]; measured Eγ, Iγ; deduced neutrino helicity.
1983MU20 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2125 (1983) A.I.Muminov, R.Kh.Safarov, F.N.Usmanov, E.Kh.Yuldashbaeva Quantitative Characteristics of the Anomalous Behavior of the Yrast-Band Levels of Er Isotopes NUCLEAR STRUCTURE 156,158,160,162,164,166Er; analyzed yrast band levels, back bending characteristics; deduced ground, s-band interaction potential vs chemical potential. Self-consistent model, constrained rotation.
1982BA64 Yad.Fiz. 36, 1360 (1982) I.I.Bakhromi, A.D.Belyaev, M.S.Vakher, V.I.Kogan, A.I.Muminov, V.P.Pikul, A.M.Usmandiyarov Mass-Separator Measurment of Mass and Energy Distributions for Products of Fission of 235U Induced by Thermal Neutrons NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment yield vs mass, total kinetic energy. Mass separator measurement. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31797. 1980BU26 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 1831 (1980) M.Budzynski, E.P.Grigorev, K.Ya.Gromov, O.I.Kochetov, G.Lizurei, Kh.Nezgoda, A.I.Muminov, M.Subotovich, T.Khazratov, Yu.V.Yushkevich Angular Correlation of 166Er γ-Rays RADIOACTIVITY 166Tm [from Ta spallation]; measured γγ(θ). 166Er deduced γ-multipolarity, δ(E2/M1).
1980BU27 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 1791 (1980) M.Budzynski, O.I.Kochetov, N.A.Lebedev, G.Lizurei, A.I.Muminov, Kh.Nezgoda, M.Subotovich, T.Khazratov Perturbed Angular Correlation of the 180-86 keV Cascade in 155Gd RADIOACTIVITY 155Tb [from Ta(p, X), E=660 MeV]; measured Eγ, Iγ, γγ(θ, t, T). 155Gd deduced γ-branching, γ-multipolarity, δ.
1980VY01 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 67 (1980); Bull.Acad.Sci.USSR, Phys.Ser. 44, No.1, 56 (1980) Ts.Vylov, Sh.Omanov, V.S.Aleksandrov, N.B.Badalov, A.Budzyak, V.V.Kuznetsov, A.I.Muminov, Khan Khen Mo Investigation of the Radioactive Decay 147Gd → 147Eu RADIOACTIVITY 147Gd [from Ta(p, X), E=660 MeV]; measured Eγ, Iγ, I(ce), ceγ-coin, Eβ+, Iβ+; deduced Q(β+). 147Eu deduced levels, J, π, γ multipolarity, log ft.
1972BE94 Dokl.Akad.Nauk Uzb.SSR No.1, 32 (1972) R.B.Begzhanov, A.I.Muminov, N.A.Ilkhamdzhanov, U.Y.Yuldashev, A.T.Salikhbaev Magnetic Properties of 159Tb, 172Yb and 182W RADIOACTIVITY 159Gd, 182Ta, 172Lu; measured γγ(θ), γγ(θ, H). 159Tb, 172Yb, 182W deduced level, g, μ.
1971BE71 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 2295 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 2083 (1972) R.B.Begzhanov, D.G.Gaffarov, A.I.Muminov, P.S.Radzhapov Magentic Properties of 153Eu, 155Eu and 189Os RADIOACTIVITY 153,155Sm, 189Ir[from Sm(n, γ), Ir(p, X)]; measured γγ(θ), integral attenuation, γγ-delay. 153,155Eu, 189Os levels deduced g, μ, T1/2. Enriched 154Sm target.
1970BE67 Izv.Akad.Nauk Uzb.SSR, Ser.Fiz.-Mat.Nauk, No.2, 65 (1970) R.B.Begzhanov, D.G.Gaffarov, N.Ilkhamdzhanov, A.I.Muminov Properties of the Excited States of 147Sm and 149Pm RADIOACTIVITY 147Eu, 149Nd; measured γγ(θ), γγ-coin. 147Sm, 149Pm levels deduced J, π, γ-mixing, μ.
1970BE76 Dokl.Akad.Nauk Uzv.SSR. No. 1, 18 (1970) R.B.Begzhanov, D.G.Gaffarov, N.Ilkhamdzhanov, A.I.Muminov, K.T.Salikhbaev Properties of Excited States of 151Sm RADIOACTIVITY 151Pm; measured γγ(θ), γγ(θ, H, t), γγ-coin. 151Sm deduced γ-multipolarities, γ-mixing, levels, J, π, g.
1970GA37 Izv.Akad.Nauk Uzb.SSR, Ser.Fiz.-Mat.Nauk No.5, 81 (1970) D.G.Gaffarov, N.A.Ilkhamdzhanov, A.I.Muminov External Magnetic Field (Fe + Gd) and Magnetic Moments of Some Excited States (155Gd, 156Gd) RADIOACTIVITY 155,156Tb; measured γγ(θ) in Fe; deduced internal field. 155,156Gd levels deduced g.
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