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NSR database version of May 24, 2024.

Search: Author = A.I.Muminov

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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset41465.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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