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NSR database version of April 11, 2024.

Search: Author = A.K.Nasirov

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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
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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
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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
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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
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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
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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
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2020GA35      J.Phys.(London) G47, 045115 (2020)

O.K.Ganiev, A.K.Nasirov

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6392.


2020VO16      Eur.Phys.J. A 56, 299 (2020)

W.von Oertzen, A.K.Nasirov

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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6318.


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
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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
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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
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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
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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
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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
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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
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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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2014VO03      Phys.Lett. B 734, 234 (2014)

W.von Oertzen, A.K.Nasirov

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
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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
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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
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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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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
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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
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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1791.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0069.


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
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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
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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
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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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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
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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.


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
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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.


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
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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
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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
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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
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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
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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)

R.V.Dzholos, A.K.Nasirov

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)

R.V.Dzholos, A.K.Nasirov

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)

R.V.Dzholos, A.K.Nasirov

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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