Nikolai Viktorovich Antonenko

Role of α clustering of heavy fragments in scission configurations in spontaneous fission of Fm 256 , 258

Horia Paşca, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

ro, ru (code pays fourni par la source)

Isotopic dependence of the fission threshold in nuclei with Z = 114 and Z = 120

Evgenii V. Mardyban, A. Rahmatinejad, T. M. Shneidman, G. G. Adamian et autres

ru, cn (code pays fourni par la source)

Empirical systematics for spontaneous fission and α -decay half-lives

N. S. Moiseev, Nikolai Viktorovich Antonenko, Гурген Григорьевич Адамян

ru (code pays fourni par la source)

Dependencies of the fission path of superheavy nuclei on the excitation energy and spin-orbit strength

A. N. Bezbakh, A. Rahmatinejad, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

ru (code pays fourni par la source)

Electric conductivity in open one-dimensional constriction

E. Kh. Alpomishev, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

ru, uz (code pays fourni par la source)

Influence of the Coulomb field of foil nuclei on half-lives of cluster states in fission fragments

F.O. Otakhonov, Sh. A. Kalandarov, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko et autres

An attempt is made to explain the experimentally observed binary decay of some fission fragments of 252 Cf(sf) while traversing the degrader foil. Assuming these fragments are born in metastable shape-isomer/cluster states formed during the initial binary fission, an influence of the …

ru (code pays fourni par la source)

Octupole collectivity in low-lying states of N = 126 isotones with particle-hole excited nucleon-pair approximation and realistic effective interaction

Y. Y. Cheng, R. V. Jolos, Nikolai Viktorovich Antonenko

ru, cn (code pays fourni par la source)

Alpha clusterization as a reason for the narrow symmetric mass distribution in spontaneous fission of 258 Fm

Horia Paşca, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

The influence of α -clustering of heavy fragment in the scission Cd+Te configuration on the mass and total kinetic energy distributions of the fragments of spontaneous fission of 258 Fm is studied. The origin of the total kinetic energy distribution modes is …

ro, ru (code pays fourni par la source)

Dependence of angular momentum of fission fragments on total kinetic energy in spontaneous fission of Cf 252

A. Rahmatinejad, T. M. Shneidman, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

A weak dependence of the angular momentum of $^{144}\mathrm{Ba}$ fragments, produced in the spontaneous fission of $^{252}\mathrm{Cf}$, on the total kinetic energy (TKE) was recently observed [N. P. Giha et al., Phys. Rev. C 111, 014605 (2025)]. To investigate this phenomenon, we …

ru (code pays fourni par la source)

Empirical systematics of long-range α -particle emission probabilities in fission of heavy and superheavy nuclei

N. S. Moiseev, Nikolai Viktorovich Antonenko, Гурген Григорьевич Адамян

The empirical systematics of long-range $\ensuremath{\alpha}$-particle emission probabilities ${P}_{\mathrm{LRA}}$ are investigated in spontaneous and thermal-neutron-induced fission of heavy and superheavy nuclei. The correlations between ${P}_{\mathrm{LRA}}$ and various parameters, including the fissility ${Z}^{2}/A$, the linear combination of proton and mass numbers $4Z\ensuremath{-}A$, and …

ru (code pays fourni par la source)

Galvanodissipative effect in open two-dimensional quantum system

E. Kh. Alpomishev, Гурген Григорьевич Адамян, Nikolai Viktorovich Antonenko

ru, uz (code pays fourni par la source)

Isoenergetic description of induced fission pathways within energy-density functional theory

Alan A. Dzhioev, Nikolai Viktorovich Antonenko

A thermodynamically consistent description of induced fission pathways in the superheavy nucleus $^{296}$Lv is presented within the framework of nuclear energy-density functional theory. Using self-consistent finite-temperature Hartree-Fock-Bogoliubov calculations with the Skyrme-type energy-density functional SkM$^*$, we derive and compare effective potentials corresponding to …

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