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111.
Komolov A. S. Lazneva E. F. Gerasimova N. B. Sobolev V. S. Pshenichnyuk S. A. Borshchev O. V. Ponomarenko S. A. Handke B. 《Physics of the Solid State》2020,62(10):1960-1966
Physics of the Solid State - Unoccupied electronic states in the energy range from 5 to 20 eV above the Fermi level have been studied in ultrathin films of dimethyl-substituted... 相似文献
112.
113.
Gontchar I. I. Ponomarenko N. A. Turkin V. V. Litnevsky L. A. 《Physics of Atomic Nuclei》2004,67(11):2080-2094
Physics of Atomic Nuclei - Mean fission lifetimes of nuclei excited to energies of 80 to 400 MeV were recently measured at the GANIL accelerator by the crystal-blocking technique. Those experiments... 相似文献
114.
A. A. Avdyeva Yu. P. Zakharov V. V. Maksimov A. M. Orishich A. G. Ponomarenko V. G. Posukh V. N. Snytnikov A. S. Yatsenko 《Journal of Applied Mechanics and Technical Physics》1989,30(6):892-895
Translated from Zhurnal Prikladnoi Mekhaniki i Tekhnicheskoi Fiziki, Vol. 30, No. 6, pp. 62–66, November–December, 1989. 相似文献
115.
D. V. Batizat A. A. Glazkov A. V. Ignatenko A. A. Yarosh V. A. Ponomarenko 《Russian Chemical Bulletin》1994,43(10):1694-1697
Cyclotrimerization of perfluoroalkyl- and perfluorooxaalkylacetylenes has been studied under various conditions. A scheme of the reaction mechanim has been suggested.Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 10, pp. 1789–1792, October, 1994. 相似文献
116.
A single scan NMR multipulse sequence has been proposed to study slow motions in solids with strong dipole interactions. Calculations of the solid echo decay time in the cases of internal motions and rigid lattice have been made and compared with the experimental data obtained in polycristalline cyclohexane and in fluorite single crystals. 相似文献
117.
We have considered the influence of electromagnetic fluctuations on electron tunneling via one non-degenerate resonant level, the problem that is relevant for electron transport through quantum dots in the Coulomb blockade regime. We show that the overall effect of the fluctuations depends on whether the electron bands in external electrodes are empty or filled. In the empty band case, depending on the relation between the tunneling rate Γ and characteristic frequency Ω of the fluctuations, the field either simply shifts the conductance peak (for rapid tunneling, Γ Ω) or broadens it (for Γ Ω). In the latter case, the system can be in three different regimes for different values of the coupling g between electrons and the field. Increasing interaction strength in the region g < 1 leads to gradual suppression of the conductance peak at the bare energy of the resonant level ε0, while at g 1 it leads to the formation of a new peak of width
at the energy ε0 + Ecis a charging energy. For intermediate values of g the conductance is non-vanishing in the entire energy range from ε0 to ε0 + Ec. For filled bands the problem is essentially multi-electron in character. One consequence of this is that, in contrast to the situation with the empty band, the fluctuations of the resonant level do not suppress conductance at resonance for g < 1. At g> 1 a Coulomb gap appears in the position of the resonant level as a function of its bare energy which leads to suppression of conductance. 相似文献
118.
We consider different ways for encryption and decryption of information in communication systems using chaotic signal of a time-delay system as a carrier. A method is proposed for extracting a hidden message in the case when the parameters of the chaotic transmitter are a priori unknown. For different configurations of the transmitter the procedure of information signal extraction from the transmitted signal is demonstrated using numerical data produced by nonlinear mixing of the chaotic signal of the Mackey–Glass system and frequency-modulated harmonic signal. 相似文献
119.
A. K. Ponomarenko 《Vestnik St. Petersburg University: Mathematics》2008,41(1):53-59
For the integral over the n-dimensional space with a radially symmetric weight function, two cubature formulas of degree eleven which are invariant under the group of hyperoctahedron are constructed. The formulas for the cubature sum contain the value of the Laplacian of the integrand at the point O(0, 0, ..., 0). Examples of approximate values of the parameters in these formulas are given. 相似文献
120.