


Vol 104, No 9 (2016)
- Year: 2016
- Articles: 10
- URL: https://ogarev-online.ru/0021-3640/issue/view/9702
Biophysics
Spontaneous spiral wave breakup caused by pinning to the tissue defect
Abstract
The work presents a mechanism of spiral wave initiation due to the specific boundary conditions on a border of cardiac tissue defect. There are known scenarios when anatomical or functional defects in cardiac tissue may provoke the spiral wave origination, including unidirectional blockage while passing through the narrow gates, bent over critical curvature wave fronts, inhomogeneous recovery of the tissue, etc. We show a new scenario of spiral wave breakup on a small defect, which is unexcitable but permeable for ionic currents supporting the excitation wave. It was believed that such defects stabilize the rotating wave; however, as shown, instead of stabilizing it leads to the spiral breakup and subsequent multiplication of the rotating waves.



Fields, Particles, and Nuclei
Measurement of QCD parameters by using the single dressed gluon approximation
Abstract
This article is based on renormalization analysis by using the single dressed gluon (SDG) approximation. This model is used to measure the coupling constant in perturbative as well as in the nonperturbative part of the QCD theory. We employ the event shape observables 〈BT〉, 〈BW〉, 〈1 − T〉, 〈C〉, and 〈ρ〉. By fitting both Monte Carlo and the real data with SDG, we find the mean values \({\alpha _S}\left( {{M_{{Z^0}}}} \right)\) = (0.1215 ± 0.0030) GeV and ν = (1.2685 ± 0.0173) GeV in the perturbative and nonperturbative regions, respectively. Our results are consistent with those obtained from other experiments at different energies. We explain all these features in this paper.



Phonon–particle coupling effects in the single-particle energies of semi-magic nuclei
Abstract
A method is presented to evaluate the particle–phonon coupling (PC) corrections to the single-particle energies in semi-magic nuclei. In such nuclei, always there is a collective low-lying 2+ phonon, and a strong mixture of single-particle and particle–phonon states often occurs. As in magic nuclei the so-called gL2 approximation, where gL is the vertex of the L-phonon creation, can be used for finding the PC correction δΣPC(ε) to the initial mass operator Σ0. In addition to the usual pole diagram, the phonon “tadpole” diagram is also taken into account. In semi-magic nuclei, the perturbation theory in δΣPC(ε) with respect to Σ0 is often invalid for finding the PC-corrected single-particle energies. Instead, the Dyson equation with the mass operator Σ(ε) = Σ0 + δΣPC(ε) is solved directly, without any use of the perturbation theory. Results for a chain of semi-magic Pb isotopes are presented.



Miscellaneous
Black hole and hawking radiation by type-II Weyl fermions
Abstract
The type-II Weyl and type-II Dirac fermions may emerge behind the event horizon of black holes. Correspondingly, the black hole can be simulated by creation of the region with overtilted Weyl or Dirac cones. The filling of the electronic states inside the “black hole” is accompanied by Hawking radiation. The Hawking temperature in the Weyl semimetals can reach the room temperature, if the black hole region is sufficiently small, and thus the effective gravity at the horizon is large.



New qualitative results of the atomic theory
Abstract
The polarizability α of many atoms and positive ions is related to their energy gap Δ and valence m by the expression αΔ2 ≅ m (in atomic units). The parameter Δ corresponds to a dipolar transition from the ground state to the first excited P state without a change in the principal quantum number n. This relation holds for univalent (m = 1) Na, K, Rb, Cs, Fr and bivalent (m = 2) Mg, Ca, Zn, Sr, Cd, Ba, Yb, Hg atoms. The above relation agrees with the experiment for positive ions Mg+ and Ca+ (m = 1) and Al+ and Ga+ (m = 2). The polarizability has been found for atoms and ions of the type Zn+, In+, Tl+, for which experimental data are unavailable. A method of calculating α for ions of the types C++, Al++, Si++ and Si+++, P+++, As+++ has been suggested based on the approximate relation α ≅(2/3〈r2〉0)2/m with the parameter 〈r2〉0 expressed in terms of the valence m, the charge number q of the atomic or ionic residue, and the ionization potential \({J_q} = \frac{{{q^2}}}{{2v_s^2}}\) as \({\left\langle {{r^2}} \right\rangle _0} = \frac{m}{{2{q^2}}}\nu _s^2\left( {1 + 5\nu _s^2} \right)\). The hydrogen dependence of 〈r2〉0 on the parameter νs has been derived by analytical continuation from the integer values νs = 1 and 2. A variational estimate of the van der Waals constant characterizing the interaction of two spherically symmetric atoms at large distances has been given.



Optics and Laser Physics
Longitudinal whispering-gallery modes in metal microcavities
Abstract
Longitudinal waves in microcavities emerging because of spatial dispersion are investigated. It is shown that longitudinal modes similar to whispering-gallery modes exist in microcavities of this kind. These longitudinal modes should exist in metal microcavities in the vicinity of the plasma frequency.



Plasma, Hydro- and Gas Dynamics
Acceleration of ions by “slow” intense laser light in low-density targets
Abstract
The mechanism of synchronized acceleration of ions by slow intense laser light is studied in application to available low-density targets of a new generation, which open prospects for experimental detection of a new effect of acceleration of protons.



Condensed Matter
Resonance absorption of terahertz radiation in nanoperforated graphene
Abstract
Recent measurements of the conductivity of nanoperforated graphene are interpreted in terms of edges states existing near the edge of each nanohole. The perimetric quantization of edge states should result in the formation of a quasi-equidistant ladder of quasistationary energy levels. Dirac fermions filling this ladder rotate about each nanohole in the direction determined by the valley index. It is shown that the irradiation of this system by circularly polarized terahertz radiation leads to a resonance in absorption in one of the valleys. The magnitude of absorption at the resonance frequency can be controlled by means of gate voltage.



Magnetotransport in thin epitaxial Bi2Se3 films
Abstract
The magnetoconductivity of thin Bi2Se3 films covered by a protective Se layer and grown at (111) BaF2 substrates is studied. It is shown that the negative magnetoconductivity observed at low magnetic fields and caused by the effect of weak antilocalization, as well as the Shubnikov−de Haas oscillations at higher fields, is determined only by the magnetic field component perpendicular to the film plane. The obtained experimental results can be reasonably interpreted under the assumption that the studied films exhibit two-dimensional topologically protected electron states. Moreover, the contribution of these states to the total conductivity turns out to be the dominant one.



Scientific Summaries
Magnetic ratchet effects in a two-dimensional electron gas
Abstract
The effect of the magnetic field on the generation of an electric current in a two-dimensional electronic ratchet is theoretically studied. Mechanisms of the formation of magnetically induced photocurrent are proposed for a structure with a two-dimensional electron gas (quantum well, graphene, or topological insulator) with a lateral asymmetric superlattice consisting of metallic strips on the external surface of the structure. The ratchet with the spatially oscillating magnetic field generated by the ferromagnetic lattice, as well as the nonmagnetic ratchet placed in the uniform magnetic field both classically weak and strong quantizing, is considered. It is established that the ratio of the amplitude of the magnetic oscillations of photocurrent to the ratchet photocurrent in zero field can exceed two orders of magnitude.


