NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Nasirov Found 89 matches. 2024NA02 Phys.Rev. C 109, 024613 (2024) Optimal colliding energy for the synthesis of a superheavy element with Z=119
doi: 10.1103/PhysRevC.109.024613
2023AT02 Phys.Rev. C 108, 034615 (2023) K.Atreya, A.Sen, T.K.Ghosh, A.K.Nasirov, D.Paul, M.M.Shaikh, K.Banerjee, C.Bhattacharya, S.Kundu, S.Manna, G.Mukherjee, S.Nandi, R.Pandey, T.K.Rana, P.Roy, S.Mukhopadhyay, R.K.Santra Exploring quasifission dynamics in reactions leading to the formation of 225Pa
doi: 10.1103/PhysRevC.108.034615
2023SH27 Eur.Phys.J. A 59, 238 (2023) Shruti, B.R.Behera, N.Saneesh, A.K.Nasirov, H.Arora, C.Sharma, Amit, Subodh, D.Arora, K.Chakraborty, A.Kaur, Raghav, M.Kumar, K.S.Golda, A.Jhingan, P.Sugathan, H.Singh, S.Mandal, H.J.Wollersheim, J.Gerl Probing binary fragmentation dynamics of 48Ti + 232Th reaction at an excitation energy of 63.5 MeV NUCLEAR REACTIONS 232Th(48Ti, X)280Cn, E=280 MeV; measured reaction and fission products; deduced mass distribution and mass-TKE correlation, fission Fragment mass distribution, mass-angle distribution, yields of binary fragments. Comparison with calculations. The 15UD Pelletron + LINAC accelerator at the Inter University Accelerator Centre (IUAC), New Delhi.
doi: 10.1140/epja/s10050-023-01135-z
2023TA09 Phys.Rev. C 107, 044611 (2023) R.B.Tashkhodjaev, A.K.Nasirov, Sh.A.Kalandarov, O.K.Ganiev Dynamical decay of a trinuclear system in the presence of friction forces in the spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated dynamics of the rupture of the ternary system 70Ni+50Ca+132Sn formed in spontaneous fission, trajectories and velocities of the trinuclear system fragments with different friction coefficients, final directions of the angular distribution of the final products. Dynamical calculations with microscopic friction forces.
doi: 10.1103/PhysRevC.107.044611
2022KA03 Phys.Rev. C 105, 014618 (2022) B.M.Kayumov, O.K.Ganiev, A.K.Nasirov, G.A.Yuldasheva Analysis of the fusion mechanism in the synthesis of superheavy element 119 via the 54Cr + 243Am reaction NUCLEAR REACTIONS 243Am(54Cr, 2n), (54Cr, 3n), (54Cr, 4n), E(cm)=261 MeV; calculated driving potential for the DNS, dependence of the quasifission barrier on the charge asymmetry of the DNS, charge distribution of the DNS fragments, partial and total σ for complete fusion, quasifission, fast fission, and evaporation residues formation for Z=119 super-heavy nuclei (SHN). 243Am(48Ca, xn), E(cm)=190-225 MeV; calculations for 243Am+54Cr reaction verified by comparison of theoretical and experimental σ(E). Combined dinuclear system (DNS) model and statistical model incorporated in KEWPIE2 code for SHEs.
doi: 10.1103/PhysRevC.105.014618
2022NA40 Phys.Atomic Nuclei 85, 776 (2022) A.K.Nasirov, B.M.Kayumov, O.K.Ganiev, G.A.Yuldasheva Interpretation of the Incomplete Fusion of Nucleus as Quasifission of Dinuclear System NUCLEAR REACTIONS 93Nb(16O, X), E<100 MeV; calculated σ, potential energy surfaces using the dinuclear system model. Comparison with experimental data.
doi: 10.1134/S1063778823010398
2021WE07 Phys.Rev. C 103, 054601 (2021) P.W.Wen, C.J.Lin, R.G.Nazmitdinov, S.I.Vinitsky, O.Chuluunbaatar, A.A.Gusev, A.K.Nasirov, H.M.Jia, A.Gozdz Potential roots of the deep subbarrier heavy-ion fusion hindrance phenomenon within the sudden approximation approach NUCLEAR REACTIONS 100Mo(64Ni, X), E=120-160 MeV; 64Ni(64Ni, X), E=85-110 MeV; 64Ni(28Si, X), E=120-160 MeV; 12C(12C, X), E=1-6 MeV; calculated fusion cross sections σ(E) and astrophysical S(E) factors using improved coupled-channels (CC) by finite element method and incoming wave boundary conditions (IWBCs), with the Woods-Saxon potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.054601
2020GA35 J.Phys.(London) G47, 045115 (2020) Comparative analysis of the Coulomb barrier in heavy-ion collisions by the double-folding method NUCLEAR REACTIONS 58Ni(16O, X), 166Er(28Si, X), 78,86Kr(40Ca, X), 208Pb, 238U(36S, X), (48Ti, X), (64Ni, X), 40Ca(32S, X), (16O, X), 92Zr(12C, X), (16O, X), (35Cl, X), (28Si, X), 40,48Ca(40Ca, X), 204Pb(12C, X), 144,148Sm(16O, X), 144Sm(17O, X), (28S, X), 208Pb(16O, X), (19F, X), (28Si, X), (48Ti, X), (54Cr, X), (56Fe, X), (64Ni, X), (70Zn, X), 96Zr(36S, X), (86Kr, X), (40Ca, X), 89Y(34S, X), (32S, X), 90Zr(36S, X), (40Ca, X), 197Au(19F, X), 124Sn(40Ca, X), E not given; calculated fusion and capture σ using the double-folding method by the use of the expansion of the nuclear density in the Gaussian-type functions and polynomials. Comparison with experimental data.
doi: 10.1088/1361-6471/ab67ea
2020GU05 Phys.Lett. B 803, 135297 (2020) S.Gupta, K.Mahata, A.Shrivastava, K.Ramachandran, S.K.Pandit, P.C.Rout, V.V.Parkar, R.Tripathi, A.Kumar, B.K.Nayak, E.T.Mirgule, A.Saxena, S.Kailas, A.Jhingan, A.K.Nasirov, G.A.Yuldasheva, P.N.Nadtochy, C.Schmitt Competing asymmetric fusion-fission and quasifission in neutron-deficient sub-lead nuclei NUCLEAR REACTIONS 175Lu(16O, X)191Au, E=82.8 MeV; 154Sm(37Cl, X)191Au, E=166.4 MeV; measured reaction products, fission fragments; deduced mass fission yields, newly identified island of mass asymmetric fission in the sub-lead region near 191Au compound nucleus.
doi: 10.1016/j.physletb.2020.135297
2020LA12 Phys.Rev. C 102, 034613 (2020) P.V.Laveen, E.Prasad, N.Madhavan, A.K.Nasirov, J.Gehlot, S.Nath, G.Mandaglio, G.Giardina, A.M.Vinodkumar, M.Shareef, A.Shamlath, S.K.Duggi, P.Sandya Devi, T.Banerjee, M.M.Hosamani, Khushboo, P.Jisha, N.Kumar, P.Sharma, T.Varughese Fusion studies in 35, 37Cl + 181Ta reactions via evaporation residue cross section measurements NUCLEAR REACTIONS 181Ta(35Cl, X), (37Cl, X), E=169.7-236.6 MeV; measured evaporation residues (ERs) using HYbrid Recoil mass Analyzer (HYRA) and position sensitive multiwire proportional counter (MWPC) at the 15-UD Pelletron and superconducting linear accelerator (sc-LINAC) facility of IUAC-New Delhi; deduced σ(E), partial capture, fusion, fast fission and quasifission and total ER cross sections; calculated potential energy surface (PES) of populating 216Th compound nucleus as a function of the distance between the interacting nuclei and charge numbers (Z) of the fragments. Comparison with dinuclear system (DNS) model and statistical model calculations.
doi: 10.1103/PhysRevC.102.034613
2020VO16 Eur.Phys.J. A 56, 299 (2020) A new radioactive decay mode, true ternary fission, the decay of heavy nuclei into three comparable fragments NUCLEAR REACTIONS 235U, 249Cf(n, F), E thermal; analyzed available data. 132Sn, 42,43,44,45,46,47,48Ca, 68,69,70,71,72Ni, 236U, 250Cf; deduced mass distribution of ternary particle and binary fragments.
doi: 10.1140/epja/s10050-020-00286-7
2020WE03 Phys.Rev. C 101, 014618 (2020) P.W.Wen, O.Chuluunbaatar, A.A.Gusev, R.G.Nazmitdinov, A.K.Nasirov, S.I.Vinitsky, C.J.Lin, H.M.Jia Near-barrier heavy-ion fusion: Role of boundary conditions in coupling of channels NUCLEAR REACTIONS 144Sm(16O, X), E=55-75 MeV; 100Mo(64Ni, X), E=120-160 MeV; 48Ca(36S, X), E=36-65 MeV; calculated tunneling probability and fusion σ(E) using finite element method for numerically solving the coupled Schrodinger equations with boundary conditions corresponding to total absorption. Comparison with coupled-channels calculations with CCFULL and KANTBP codes, and with experimental data.
doi: 10.1103/PhysRevC.101.014618
2019NA04 Eur.Phys.J. A 55, 29 (2019) A.K.Nasirov, B.M.Kayumov, G.Mandaglio, G.Giardina, K.Kim, Y.Kim The effect of the neutron and proton numbers ratio in colliding nuclei on the formation of the evaporation residues in the 34S + 208Pb and 36S + 206Pb reactions
doi: 10.1140/epja/i2019-12688-3
2018GI03 Nucl.Phys. A970, 169 (2018) G.Giardina, G.Mandaglio, A.K.Nasirov, A.Anastasi, F.Curciarello, G.Fazio Uncertainties and understanding of experimental and theoretical results regarding reactions forming heavy and superheavy nuclei COMPILATION Z=102-122; calculated fusion probability of colliding nuclei (target W to Cf, projectile Mg to Kr) to form given composite system and survival probability vs E(cm) and vs angular momentum. Compared with other results and with data. 240Pu(48Ca, n), E*=35.89 MeV; calculated neutron energy spectra σ(En) separately from 285,286,287,288Fl. 240Pu(48Ca, n), (48Ca, p), 240Pu(48Ca, α), E*=40.06 MeV; calculated first emitted n-spectra, p-spectra, α-spectra σ(out).
doi: 10.1016/j.nuclphysa.2017.11.010
2018MA60 Nucl.Phys. A979, 204 (2018) G.Mandaglio, A.K.Nasirov, A.Anastasi, F.Curciarello, G.Fazio, G.Giardina Role of charged particle emission on the evaporation residue formation in the 82Se+138Ba reaction leading to the 220Th compound nucleus NUCLEAR REACTIONS 138Ba(82Se, xnypzα)220Th, E*=12-70 MeV; calculated ER (Evaporation Residue) σ considering both quasifission of DNS (Double-Nuclear System) leading to ER, and the channel via creation of compound nucleus and its decay; deduced calculated total ER σ overpredict available experimental data at some cases.
doi: 10.1016/j.nuclphysa.2018.09.057
2018MA63 Phys.Rev. C 98, 044616 (2018) G.Mandaglio, A.Anastasi, F.Curciarello, G.Fazio, G.Giardina, A.K.Nasirov Effects of entrance channels on the deexcitation properties of the same compound nucleus formed by different pairs of collision partners NUCLEAR REACTIONS 204Pb(16O, X), 180Hf(40Ar, X), 138Ba(82Se, X), 124Sn(96Zr, X)220Th*/219Th*/218Th*/217Th*/216Th*, E*=35.5, 46, 61, 10-75 MeV; calculated partial fusion σ(E) as function of angular momentum effective fission barriers, neutron emission and fission probabilities for the excited 220Th* compound nucleus and isotopes formed after successive neutron evaporation up to emission of four neutron, ratio of evaporation residues with Z>90 and Z=90. 249Cf(48Ca, X)297Og*, E*=22.5-50 MeV; calculated evaporation residue σ(E) for one-neutron as well as charged particle emission.
doi: 10.1103/PhysRevC.98.044616
2017SH06 Phys.Rev. C 95, 034610 (2017) A.Shamlath, E.Prasad, N.Madhavan, P.V.Laveen, J.Gehlot, A.K.Nasirov, G.Giardina, G.Mandaglio, S.Nath, T.Banerjee, A.M.Vinodkumar, M.Shareef, A.Jhingan, T.Varughese, D.Kumar, P.Sandya Devi, Khushboo, P.Jisha, N.Kumar, M.M.Hosamani, S.Kailas Fusion and quasifission studies in reactions forming Rn via evaporation residue measurements NUCLEAR REACTIONS 180Hf(28Si, X)208Rn*, E=130.6, 135.0, 143.9, 149.4, 154.9, 164.2, 171.9, 193.7 MeV; 180Hf(30Si, X)210Rn*, E=130.6, 135.2, 139.6, 144.0, 149.5, 156.3, 160.7, 164.3, 171.8 MeV; measured evaporation residues (ERs) ERs, ΔE vs TOF plots, ER σ(Ε) using the Hybrid Recoil Mass Analyzer (HYRA) at the 15 UD Pelletron accelerator of IUAC-New Delhi. Comparison with theoretical cross sections, using dinuclear system and statistical models, and with the results of 194Pt(16O, X)210Rn* and 160Gd(50Ti, X)210Rn* compound nuclear reactions.
doi: 10.1103/PhysRevC.95.034610
2017TH04 Eur.Phys.J. A 53, 133 (2017) M.Thakur, B.R.Behera, R.Mahajan, N.Saneesh, G.Kaur, P.Sharma, R.Dubey, K.Kapoor, A.Yadav, N.Kumar, S.Kumar, K.Rani, P.Sugathan, A.Jhingan, A.Chatterjee, M.B.Chatterjee, S.Mandal, A.Saxena, S.Pal, S.Kailas, A.Nasirov, B.Kayumov Binary fragmentation based studies for the near super-heavy compound nucleus 256Rf NUCLEAR REACTIONS 208Pb(48Ti, x), E=275 MeV; measured fission fragments using MWPCs; deduced intermediate mass fragments mass distribution, TKE; calculated QF (QuasiFission), FF (Fast Fission), DNS (Double Nuclear System) yields separately, especially close to near superheavy 256Rf. Compared to data.
doi: 10.1140/epja/i2017-12323-5
2016NA01 Nucl.Phys. A946, 89 (2016) Peculiarities of quasifission reactions in heavy ion collisions
doi: 10.1016/j.nuclphysa.2015.11.013
2016NA18 Eur.Phys.J. A 52, 135 (2016) A.K.Nasirov, R.B.Tashkhodjaev, W.von Oertzen Pre-scission configuration of the tri-nuclear system at spontaneous ternary fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated tri-nuclear system potential in spontaneous ternary fission, deformation, energy for different combinations of fragments.
doi: 10.1140/epja/i2016-16135-9
2016SH01 Nucl.Phys. A945, 67 (2016) A.Shamlath, M.Shareef, E.Prasad, P.Sugathan, R.G.Thomas, A.Jhingan, S.Appannababu, A.K.Nasirov, A.M.Vinodkumar, K.M.Varier, C.Yadav, B.R.S.Babu, S.Nath, G.Mohanto, Ish Mukul, D.Singh, S.Kailas Fission fragment mass distribution studies in 30Si + 180Hf reaction NUCLEAR REACTIONS 180Hf(30Si, F), E=128-148 MeV;194Pt(16O, F), E not given; measured fission fragments using two large area position-sensitive MWPCs; deduced fragment mass distribution; calculated fragment mass distribution, potential energy surface using CCFULL code, ratio quasifission σ to capture σ using DNS (Double Nuclear System) model.
doi: 10.1016/j.nuclphysa.2015.09.011
2016TA21 Phys.Rev. C 94, 054614 (2016) R.B.Tashkhodjaev, A.K.Nasirov, E.Kh.Alpomeshev Dynamics of the tri-nuclear system at spontaneous fission of 252Cf RADIOACTIVITY 252Cf(SF); calculated total interaction potential contours for ternary fission involving 70Ni+50Ca+132Sn system as a function of relative distance between Ni and Sn nuclei. Tri-nuclear system (TNS) model in the framework of classical Lagrange formalism.
doi: 10.1103/PhysRevC.94.054614
2015KI05 Phys.Rev. C 91, 064608 (2015) K.Kim, Y.Kim, A.K.Nasirov, G.Mandaglio, G.Giardina Effects of entrance channels on the evaporation residue yields in reactions leading to the 220Th compound nucleus NUCLEAR REACTIONS 138Ba(82Se, X)220Th*, E(cm)=235, 245 MeV; 96Zr(124Sn, X), 138Ba(82Se, X), 180Hf(40Ar, X), 204Pb(16O, X)220Th*, E(*) at 10-80 MeV; calculated capture, fusion, and evaporation residue cross sections, potential energy surface as a function of relative distance between the interacting nuclei and charge number of a fragment, driving potential for the dinuclear system (DNS), dependence of quasifission barrier on angular momentum, charge distribution of DNS fragments, survival probability. Entrance channel effects. Combined dinuclear system (DNS) and advanced statistical models. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.064608
2015NA15 Pramana 85, 367 (2015) A.K.Nasirov, W.Von Oertzen, R.B.Tashkhodjaev Nuclear shell effect and collinear tripartition of nuclei RADIOACTIVITY 252Cf, 236U(SF); analyzed available data; calculated contour plots of the total interaction potential, potential energy surfaces for the pre-scission state of the collinear ternary system.
doi: 10.1007/s12043-015-1051-3
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
2015VO07 Phys.Lett. B 746, 223 (2015), Erratum Phys.Lett. B 762, 550 (2016), Corrigendum to "Multi-modal Fission in Collinear Ternary Cluster decay of 252Cf(sf, fff)" [Phys. Lett. B 746 (2015) 223] W.von Oertzen, A.K.Nasirov, R.B.Tashkhodjaev Multi-modal fission in collinear ternary cluster decay of 252Cf(sf, fff) RADIOACTIVITY 252Cf(SF); calculated fission fragment masses, kinetic energies, potential energy surfaces, barriers. Comparison with experimental data.
doi: 10.1016/j.physletb.2015.05.00
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
2014VO03 Phys.Lett. B 734, 234 (2014) True ternary fission, the collinear decay into fragments of similar size in the 252Cf(sf) and 235U(nth, f) reactions RADIOACTIVITY 252Cf(SF), (2n), 236U(2n); calculated ternary fission yields, potential energy surfaces. Comparison with experimental data.
doi: 10.1016/j.physletb.2014.05.067
2013NA36 Eur.Phys.J. A 49, 147 (2013) A.Nasirov, K.Kim, G.Mandaglio, G.Giardina, A.Muminov, Y.Kim Main restrictions in the synthesis of new superheavy elements: Quasifission and/or fusion fission NUCLEAR REACTIONS 232Th(58Fe, X), E(cm)=237-290 MeV;232Th(64Ni, X), E(cm)=263-283 MeV;248Cm(48Ca, X), E(cm)=197-235 MeV; calculated DNS (double nuclear system) potential energy surface, deformation, driving potential, fusion, fast fission, quasifission, evaporation residue σ. Evaporation residue σ compared with available data.
doi: 10.1140/epja/i2013-13147-y
2012MA55 Phys.Rev. C 86, 064607 (2012) G.Mandaglio, G.Giardina, A.K.Nasirov, A.Sobiczewski Investigation of the 48Ca+249-252Cf reactions synthesizing isotopes of the superheavy element 118 NUCLEAR REACTIONS 249,250,251,252Cf(48Ca, X), (48Ca, xn), E(cm)=197-235 MeV; calculated capture, quasifission, fusion, evaporation residue σ. Formation of evaporation residue nuclei from 297,298,299,300118 superheavy compound nuclei. Comparison with experimental data for 294118.
doi: 10.1103/PhysRevC.86.064607
2012NA11 Bull.Rus.Acad.Sci.Phys. 76, 467 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 525 (2012) A.K.Nasirov, R.B.Tahkhodzhaev, O.O.Abdurazakov True ternary fission of 236U: A sequential mechanism? RADIOACTIVITY 236U(SF); calculated fragment yields; deduced new sequential mechanism. Comparison with available data.
doi: 10.3103/S1062873812040259
2011NA12 Int.J.Mod.Phys. E20, 406 (2011) A.Nasirov, G.Fazio, G.Giardina, G.Mandaglio, M.Manganaro, A.Muminov Appearance of nuclear shell effects and initial charge (mass) asymmetry in the formation of products of heavy ion collisions NUCLEAR REACTIONS 249Cf(50Ti, X), 248Cm(54Cr, X), E(cm)<260 MeV; calculated σ, fission barrier. Comparison with experimental data.
doi: 10.1142/S021830131101779X
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
2011TA27 Eur.Phys.J. A 47, 136 (2011) R.B.Tashkhodjaev, A.K.Nasirov, W.Scheid Collinear cluster tripartition as sequential binary fission in the 235U(nth, f) reaction NUCLEAR REACTIONS 235U(n, F), E=thermal; calculated fission isotope yields; deduced possible sequential fission assuming collinear cluster tripartition.
doi: 10.1140/epja/i2011-11136-x
2010GI04 Int.J.Mod.Phys. E19, 882 (2010) G.Giardina, G.Fazio, G.Mandaglio, M.Manganaro, A.K.Nasirov, M.V.Romaniuk, C.Sacca Expectations and limits to synthesize nuclei with Z ≥ 120 NUCLEAR REACTIONS 124,132Sn(96Zr, X), 136Xe(86Kr, X), (136Xe, X), 174Yb(48Ca, X), (132Sn, X), 182W(32S, X), 181Ta(40Ar, X), 208Pb(32S, X), (48Ca, X), (50Ti, X), (58Fe, X), (86Kr, X), 238U(16O, X), (64Ni, X), 226Ra(48Ca, X), 248Cm(26Mg, X), (48Ca, X), (54Cr, X), 243Am(48Ca, X), 248Bk(48Ca, X), 249Cf(48Ca, X), (54Cr, X), (64Ni, X), 244Pu(58Fe, X), 176Hf(132Sn, X), 186W(132Sn, X), 232Th(84Kr, X), E not given; calculated evaporation residue σ, fusion probabilities; deduced projectile restrictions for synthesis of super-heavy elements.
doi: 10.1142/S0218301310015333
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
2010ZH06 Phys.Rev. C 81, 034611 (2010) H.Q.Zhang, C.L.Zhang, C.J.Lin, Z.H.Liu, F.Yang, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina Competition between fusion-fission and quasifission processes in the 32S+184W reaction NUCLEAR REACTIONS 184W(32S, X), E=140, 145, 150, 155, 160, 165, 170 MeV; measured capture σ, σ(θ) of fission fragments, fission excitation functions. 182,184(32S, X), E(cm)=120-220 MeV; analyzed fission excitation functions, comparison with previous experimental data and theoretical cross sections using dinuclear system (DNS) model for capture, complete fusion, quasifission, fast fission, and total evaporation residues.
doi: 10.1103/PhysRevC.81.034611
2010ZH29 Nucl.Phys. A834, 201c (2010) C.L.Zhang, H.Q.Zhang, C.J.Lin, A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina Competition between fusion-fission and quasifission processes in 32S+184W reaction NUCLEAR REACTIONS 184W(32S, F), E(cm)=118.8, 123.1, 127.3, 131.5, 135.8, 141.4, 144.4 MeV; measured fission fragment angular distributions; deduced fission, fusion σ, σ(θ), reaction mechanism features. Comparison with dinuclear system model.
doi: 10.1016/j.nuclphysa.2009.12.040
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
2009NA14 Int.J.Mod.Phys. E18, 841 (2009) A.Nasirov, G.Fazio, G.Giardina, G.Mandaglio, M.Manganaro, F.Hanappe, A.Muminov, W.Scheid Comparison of the fusion-fission and quasifission mechanism in heavy-ion collisions
doi: 10.1142/S021830130901294X
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
2006NA06 Int.J.Mod.Phys. E15, 311 (2006) A.K.Nasirov, Y.Aritomo, A.Fukushima, M.Ohta, T.Wada, G.Giardina, G.Mandaglio, A.Muminov, R.K.Utamuratov Role of the nuclear shell structure and orientation angles of deformed reactants in complete fusion NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 154Sm(60Ni, X), E=240-330 MeV; calculated fusion and evaporation residue σ; deduced shell structure and orientation effects. Dinuclear system concept, Langevin calculations, comparison with data.
doi: 10.1142/S0218301306004144
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
2005NA29 Nucl.Phys. A759, 342 (2005) A.Nasirov, A.Fukushima, Y.Toyoshima, Y.Aritomo, A.Muminov, S.Kalandarov, R.Utamuratov The role of orientation of nucleus symmetry axis in fusion dynamics NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 154Sm(60Ni, X), E=250-320 MeV; calculated capture, quasi-fission and fusion σ, entrance channel effects.Dinuclear system model analysis.
doi: 10.1016/j.nuclphysa.2005.05.152
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
1999GI16 Pramana 53, 409 (1999) G.Giardina, P.D'Agostino, G.Fazio, M.Herman, A.I.Muninov, A.Nasirov, G.Oliva, R.Palamara, R.Ruggeri Fusion-Fission Dynamics in the Superheavy Nucleus Production NUCLEAR REACTIONS 208Pb(64Ni, X), E=300-320 MeV; 238U, 244Pu(48Ca, X), E=220-280 MeV; calculated fusion, quasifission σ. 238U, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E=220-260 MeV; 208Pb(64Ni, n), E ≈ 310 MeV; calculated excitation functions. Comparisons with data.
doi: 10.1007/s12043-999-0007-x
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
1998AN07 Phys.Rev. C57, 1832 (1998) N.V.Antonenko, A.K.Nasirov, T.M.Shneidman, V.D.Toneev Towards Exotic Nuclei Via Binary Reaction Mechanism NUCLEAR REACTIONS 106Cd(58Ni, X), (54Fe, X), (56Fe, X), (40Ca, X), (64Zn, X), E not given; calculated yields; deduced light Sn isotopes production features. Microscopic transport model.
doi: 10.1103/PhysRevC.57.1832
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.
1997CH54 Bull.Rus.Acad.Sci.Phys. 61, 1740 (1997) E.A.Cherepanov, G.G.Adamyan, N.V.Antonenko, V.V.Volkov, A.K.Nasirov Concept of a Double Nuclear System in Conditions for Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(62Ni, X), (70Zn, X), (82Se, X), 244Pu(48Ca, X), 136Xe(136Xe, X), E not given; calculated entrance potential, double-nuclear-system potential energy; deduced superheavy element formation features.
1997VO18 Nuovo Cim. 110A, 1127 (1997) V.V.Volkov, G.G.Adamian, N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov Process of Complete Fusion of Nuclei within the Framework of Dinuclear System Concept
doi: 10.1007/BF03035954
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.
1996AN20 Bull.Rus.Acad.Sci.Phys. 60, 85 (1996) N.V.Antonenko, V.V.Volkov, A.K.Nasirov, E.A.Cherepanov Fusion of Massive Nuclei within a Concept of Double Nuclear System and Macroscopic Dynamic Model NUCLEAR REACTIONS, ICPND 110Pd(110Pd, X), E(cm) ≈ 240-300 MeV; calculated evaporation residue production, compound nucleus formation σ vs E. 180Hf(40Ar, X), 96Zr(124Sn, X), E(cm) ≈ 205-250 MeV; calculated fusion probability vs E. 208Pb(62Ni, X), E not given; calculated dinuclear system potential vs Z. Macroscopic dynamical model, double nuclear systems concepts.
1995AN12 Phys.Rev. C51, 2635 (1995) N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov, V.P.Permyakov, V.V.Volkov Compound Nucleus Formation in Reactions between Massive Nuclei: Fusion barrier NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), 110Pd(110Pd, X), E(cm)=180-300 MeV; measured evaporation, compound nucleus formation σ(E), fusion barrier dependence on the angular momentum. 180Hf(40Ar, X), 96Zr(124Sn, X), E(cm)=200-250 MeV; calculated compound nucleus formation probability vs E.
doi: 10.1103/PhysRevC.51.2635
1995CH15 Nucl.Phys. A583, 165c (1995) E.A.Cherepanov, V.V.Volkov, N.V.Antonenko, V.P.Permyakov, A.K.Nasirov Model of Competition between Complete Fusion and Quasi-Fission in Reactions with Massive Nuclei NUCLEAR REACTIONS, ICPND 110Pd(110Pd, X), E(cm)=220-300 MeV; 100Mo(100Mo, X), E(cm)=180-260 MeV; calculated fusion σ(E), fusion, quasifission barrier vs angular momentum. Massive symmetric dinuclear system.
doi: 10.1016/0375-9474(94)00654-6
1994AD03 Z.Phys. A347, 203 (1994) G.G.Adamian, R.V.Jolos, A.K.Nasirov Partition of Excitation Energy between Reaction Products in Heavy Ion Collisions NUCLEAR REACTIONS 165Ho(56Fe, X), E=505 MeV; 110Pd(238U, X), E=1.398 GeV; 165Ho(74Ge, X), E=629 MeV; 124Sn(238U, X), E=1.468 GeV; 197Au(58Ni, X), E=880 MeV; calculated projectile-like fragment to total excitation energy ratio vs total energy loss. Single-particle approach, p-h excitations, nucleon exchange included.
doi: 10.1007/BF01292377
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.
1994AD22 Fiz.Elem.Chastits At.Yadra 25, 1379 (1994); Sov.J.Part.Nucl 25, 583 (1994) G.G.Adamyan, A.K.Nasirov, N.V.Antonenko, R.V.Jolos Influence of Shell Effects on the Dynamics of Deep Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(56Fe, X), E=505 MeV; 165Ho(74Ge, X), E=629 MeV; 124Sn(238U, X), E=1468 MeV; 110Pd(238U, X), E=1398 MeV; 197Au(58Ni, X), E=880 MeV; calculated fragment, projectile excitation energy ratio vs energy loss. 165Ho(56Fe, X), E=505, 403 MeV; 165Ho(74Ge, X), E=629 MeV; 197Au(58Ni, X), E=880 MeV; calculated fragment charge, mass distributions, variances vs energy loss. 181Ta(52Cr, X), E=378 MeV; 197Au(51V, X), E=447 MeV; 197Au(20Ne, X), E=175 MeV; calculated fragment charge distributions. Microscopic model, other aspects, other reactions discussed.
1994AN26 Bull.Rus.Acad.Sci.Phys. 58, 55 (1994) N.V.Antonenko, V.V.Volkov, A.K.Nasirov, V.P.Permyakov, E.A.Cherepanov Reactions with Complete Fusion of Massive Nuclei: Competition between complete fusion and quasifission NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm)=180-240 MeV; 110Pd(110Pd, X), E(cm)=220-300 MeV; calculated fusion, evaporation residue production σ(E). Double nuclear system approach.
1993AD01 Nucl.Phys. A551, 321 (1993) G.G.Adamian, N.V.Antonenko, R.V.Jolos, A.K.Nasirov Microscopic Driving Potential for a Dinuclear Systm NUCLEAR REACTIONS 232Th(40Ar, 40Ar), E=200 MeV; 238U(32S, 32S), E=192 MeV; 197Au(63Cu, 63Cu), E not given; calculated microscopic driving potential.
doi: 10.1016/0375-9474(93)90484-F
1993AN20 Phys.Lett. 319B, 425 (1993) N.V.Antonenko, E.A.Cherepanov, A.K.Nasirov, V.P.Permjakov, V.V.Volkov Competition between Complete Fusion and Quasi-Fission in Reactions between Massive Nuclei. The Fusion Barrier NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm) ≈ 180-250 MeV; 110Pd(110Pd, X), E(cm)=220-300 MeV; calculated compound nucleus formation, evaporation residue production σ vs E; deduced new type of fusion barrier. Complete, quasifusion channels competition model.
doi: 10.1016/0370-2693(93)91746-A
1993AN21 Bull.Rus.Acad.Sci.Phys. 57, 1261 (1993) N.V.Antonenko, V.V.Volkov, A.K.Nasirov, V.P.Permyakov, E.A.Cherepanov Compound Nucleus Formation and Analysis of Complete Fusion of Massive Nuclei. Fusion Barrier NUCLEAR REACTIONS, ICPND 100Mo(100Mo, X), E(cm)=190-250 MeV; 110Pd(110Pd, X), E(cm) ≈ 230-300 MeV; analyzed compound nucleus, evaporation residue production σ(E); deduced reaction mechanism. Conventional models.
1992AD07 Yad.Fiz. 55, 660 (1992); Sov.J.Nucl.Phys. 55, 366 (1992) G.G.Adamyan, R.V.Dzholos, A.K.Nasirov Shell Effects in the Nucleon-Transfer Matrix Elements and the Process of Multinucleon Transfer NUCLEAR REACTIONS 165Ho(56Fe, X), 100Mo(40Ar, X), 120Sn(132Xe, X), E not given; calculated fragment charge distribution variance vs interaction time.
1992AD10 Bull.Rus.Acad.Sci.Phys. 56, 1799 (1992) G.G.Adamyan, A.K.Nasirov, V.P.Permyakov Influence of Particle-Hole Excitation and Multinucleon Transfer on Interaction Potential of Complex Nuclei NUCLEAR REACTIONS 92Zr(58Ni, X), 181Ta(52Cr, X), E not given; calculated transferred nucleon number mean square value, interaction potential vs temperature. Semi-microscopic model.
1989JO03 Yad.Fiz. 50, 382 (1989) R.V.Jolos, S.M.Lukyanov, A.K.Nasirov, V.P.Permyakov, V.S.Salamatin, G.G.Chubarian Nuclear Shell-Structure Effect on Mass Distribution in Multinucleon-Transfer Reactions NUCLEAR REACTIONS 124Sn, 108Ag, 139La(40Ar, X), E=220 MeV; 122Sn, 108Ag, 139La(64Zn, X), E=315 MeV; measured σ(fragment θ) vs mass; deduced shell structure role.
1988DZ02 Yad.Fiz. 48, 1304 (1988) R.V.Dzholos, A.K.Nasirov, V.P.Permyakov On Total Kinetic Energies of Heavy-Ion Deep Inelastic Collisions and Quasifissions NUCLEAR REACTIONS 232Th(40Ar, X), (40Ar, F), E=220 MeV; 197Au, 238U, 232Th(22Ne, X), (22Ne, F), E=179 MeV; 238U(32S, X), E=192 MeV; 122Sn(64Zn, X), (64Zn, F), E=315 MeV; calculated deep inelastic, fission fragment dynamical deformation, nucleon exchange, neck formation.
1987DZ01 Yad.Fiz. 45, 1298 (1987) Effects of Nucleon Transfers in Nucleus-Nucleus Interaction Potential NUCLEAR REACTIONS 208Pb(208Pb, X), E=1643.2 MeV; 209Bi(132Xe, X), E=963.6 MeV; 196Au(132Xe, X), E=996.6 MeV; 208Pb(40Ar, X), E=340 MeV; calculated interaction potential energies. Multi-nucleon transfer effect.
1987DZ04 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 2041 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.11, 153 (1987) R.V.Dzholos, A.K.Nasirov, V.P.Permyakov Enhancement of Subbarrier Fusion for Complicated Nucleus because of Interaction Potential Dynamic Change in Incoming Channel Reactions NUCLEAR REACTIONS 154Sm, 208Pb(16O, X), 132Xe(132Xe, X), E not given; calculated interaction potentials.
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.
1985DZ03 Yad.Fiz. 42, 175 (1985) Effect of Residual Interaction in the Widths of Product Charge Distributions in Multi-Nucleon Transfer Reactions NUCLEAR REACTIONS 120Sn(132Xe, X), E=5.9 MeV/nucleon; 196Au(132Xe, X), E=7.5 MeV/nucleon; 209Bi(132Xe, X), E=7.3 MeV/nucleon; 208Pb(208Pb, X), E=7.9 MeV/nucleon; calculated fragment charge distribution variances, widths; deduced nucleon-nucleon interaction role.
1984DZ03 Yad.Fiz. 40, 721 (1984) Multinucleon Transfers in Deep-Inelastic Collisions of Heavy Ions NUCLEAR REACTIONS 196Au(132Xe, X), E=7.5 MeV/nucleon; 120Sn(132Xe, X), E=5.9 MeV/nucleon; 209Bi(132Xe, X), E=7.3 MeV/nucleon; 208Pb(208Pb, X), E=7.6 MeV/nucleon; calculated fragment charge distribution variance, width, position maxima time dependences. Microscopic approach, multi-nucleon transfer.
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