Anti-corruption policy in a socio-cultural space: indicators and actual strategies

The paper proposes a discussion of an essence, modern interpretation and directions of counteraction to corruption interaction. The paper analyzes wide (sociological) and narrow (formal-legal) approaches to the interpretation of corruption interaction, examines the causes and forms that activate the development of corruption in the post-Soviet space. The authors singled out and analyzed key aspects of the modern anticorruption policy carried out in Russia at the beginning of the 21st century. The author's vision of the content of the anti-corruption legislation is separately argued, specific proposals are formulated to improve the legislation in the conditions of an unstable legal system and a transitional state, and the basic guidelines for its further development are determined

Affleck-Dine baryogenesis in the local domain

For Affleck-Dine baryogenesis to proceed, there must have been two types of phase transitions. One is the destabilized-stabilized phase transition of the flat direction, which is in general induced by the Hubble parameter. The other is the phase transition related to the A-term, which induces the misalignment of the relative phase of the flat direction. In the conventional Affleck-Dine baryogenesis they are supposed to start almost simultaneously. Of course these phase transitions can take place separately, but the latter must not be later than the former because the phase transition of the A-term can not produce any baryon number when there is no condensate of the relative charge. In this paper we try to construct models where the original idea of Affleck-Dine baryogenesis is realized in a different way. We show examples in which the local domain of the false vacuum with the required condensate is formed after inflation and collapses in a safe way so that the domain wall problem is avoided. We also show examples where the phase transition of the A-term starts before the decay of the condensate. As in the conventional Affleck-Dine mechanism, the phase transition of the A-term produces baryon number in the local domain of the condensate. We construct scenarios where our mechanism produces sufficient baryon asymmetry of the Universe.Comment: 18pages, latex2e, to appear in PR

First- principle calculations of magnetic interactions in correlated systems

We present a novel approach to calculate the effective exchange interaction parameters based on the realistic electronic structure of correlated magnetic crystals in local approach with the frequency dependent self energy. The analog of ``local force theorem'' in the density functional theory is proven for highly correlated systems. The expressions for effective exchange parameters, Dzialoshinskii- Moriya interaction, and magnetic anisotropy are derived. The first-principle calculations of magnetic excitation spectrum for ferromagnetic iron, with the local correlation effects from the numerically exact QMC-scheme is presented.Comment: 17 pages, 3 Postscript figure

Theory of Coexistence of Superconductivity and Ferroelectricity : A Dynamical Symmetry Model

We propose and investigate a model for the coexistence of Superconductivity (SC) and Ferroelectricity (FE) based on the dynamical symmetries $su(2)$ for the pseudo-spin SC sector, $h(4)$ for the displaced oscillator FE sector, and $su(2) \otimes h(4)$ for the composite system. We assume a minimal symmetry-allowed coupling, and simplify the hamiltonian using a double mean field approximation (DMFA). A variational coherent state (VCS) trial wave-function is used for the ground state: the energy, and the relevant order parameters for SC and FE are obtained. For positive sign of the SC-FE coupling coefficient, a non-zero value of either order parameter can suppress the other (FE polarization suppresses SC and vice versa). This gives some support to "Matthias' Conjecture" [1964], that SC and FE tend to be mutually exclusive. For such a Ferroelectric Superconductor we predict: a) the SC gap $\Delta$ (and $T_c$) will increase with increasing applied pressure when pressure quenches FE as in many ferroelectrics, and b) the FE polarization will increase with increaesing magnetic field up to $H_c$. The last result is equivalent to the prediction of a new type of Magneto-Electric Effect in a coexistent SC-FE material. Some discussion will be given of the relation of these results to the cuprate superconductors.Comment: 46 page

Monte Carlo Methods for Estimating Interfacial Free Energies and Line Tensions

Excess contributions to the free energy due to interfaces occur for many problems encountered in the statistical physics of condensed matter when coexistence between different phases is possible (e.g. wetting phenomena, nucleation, crystal growth, etc.). This article reviews two methods to estimate both interfacial free energies and line tensions by Monte Carlo simulations of simple models, (e.g. the Ising model, a symmetrical binary Lennard-Jones fluid exhibiting a miscibility gap, and a simple Lennard-Jones fluid). One method is based on thermodynamic integration. This method is useful to study flat and inclined interfaces for Ising lattices, allowing also the estimation of line tensions of three-phase contact lines, when the interfaces meet walls (where "surface fields" may act). A generalization to off-lattice systems is described as well. The second method is based on the sampling of the order parameter distribution of the system throughout the two-phase coexistence region of the model. Both the interface free energies of flat interfaces and of (spherical or cylindrical) droplets (or bubbles) can be estimated, including also systems with walls, where sphere-cap shaped wall-attached droplets occur. The curvature-dependence of the interfacial free energy is discussed, and estimates for the line tensions are compared to results from the thermodynamic integration method. Basic limitations of all these methods are critically discussed, and an outlook on other approaches is given

A Theory for the High-T_c Cuprates: Anomalous Normal-State and Spectroscopic Properties, Phase Diagram, and Pairing

A theory of highly correlated layered superconducting materials isapplied for the cuprates. Differently from an independent-electron approximation, their low-energy excitations are approached in terms of auxiliary particles representing combinations of atomic-like electron configurations, where the introduction of a Lagrange Bose field enables treating them as bosons or fermions. The energy spectrum of this field accounts for the tendency of hole-doped cuprates to form stripe-like inhomogeneities. Consequently, it induces a different analytical behavior for auxiliary particles corresponding to "antinodal" and "nodal" electrons, enabling the existence of different pairing temperatures at T^* and T_c. This theory correctly describes the observed phase diagram of the cuprates, including the non-Fermi-liquid to FL crossover in the normal state, the existence of Fermi arcs below T^* and of a "marginal-FL" critical behavior above it. The qualitative anomalous behavior of numerous physical quantities is accounted for, including kink- and waterfall-like spectral features, the drop in the scattering rates below T^* and more radically below T_c, and an effective increase in the density of carriers with T and \omega, reflected in transport, optical and other properties. Also is explained the correspondence between T_c, the resonance-mode energy, and the "nodal gap".Comment: 28 pages, 7 figure

Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at √s=0.9 and 2.36 TeV

Measurements of inclusive charged-hadron transverse-momentum and pseudorapidity distributions are presented for proton-proton collisions at root s = 0.9 and 2.36 TeV. The data were collected with the CMS detector during the LHC commissioning in December 2009. For non-single-diffractive interactions, the average charged-hadron transverse momentum is measured to be 0.46 +/- 0.01 (stat.) +/- 0.01 (syst.) GeV/c at 0.9 TeV and 0.50 +/- 0.01 (stat.) +/- 0.01 (syst.) GeV/c at 2.36 TeV, for pseudorapidities between -2.4 and +2.4. At these energies, the measured pseudorapidity densities in the central region, dN(ch)/d eta vertical bar(vertical bar eta vertical bar and pp collisions. The results at 2.36 TeV represent the highest-energy measurements at a particle collider to date

Mean age of death and longevity for male scientists of different specialties

The article provides information on the mean age of death (MAD) for 54 256 men professionally involved in research work and assigned to one of the six categories, namely, physics, chemistry, medicine and biology, mathematics, economics, and humanities. In addition, the effect of teaching activity on MAD and longevity has been evaluated for scientists of different specialties. Special attention has been paid to the analysis of MAD of the deceased members of the Russian Academy of Sciences, including members of the USSR Academy of Sciences (1724–2013). The minimum MAD has been found for mathematicians (72.1 ± 0.21 years) and the maximum MAD for scientists in economics (74.6 ± 0.26 years). The relative number of surviving ≥90 years and ≥100 years is minimal for mathematicians (7.59 and 0.37%, respectively), whereas those numbers for economists reveal the maximum values (10.26 and 0.96%, respectively). Indicators of MAD and proportion of centenarians among the scientists who received public recognition strongly depend on the specialty. Similarly, the members of the Russian Academy of Sciences and the USSR Academy of Sciences have the highest MAD in economics (74.7 ± 1.05 years) and the lowest in mathematics (70.6 ± 0.74 years). MAD has proven to be 3.5 years higher for scientists involved in teaching at university or college compared to those who were not involved in teaching. In this case, the “gain” is significant, ranging from 3.1 years for economists and humanitarians to 4.9 years for mathematicians. The results of the study lead to the conclusion that intense scientific work contributes to an increase in life expectancy and longevity. © 2016, Allerton Press, Inc

Mean age of death and longevity for male scientists of different specialties

The article provides information on the mean age of death (MAD) for 54 256 men professionally involved in research work and assigned to one of the six categories, namely, physics, chemistry, medicine and biology, mathematics, economics, and humanities. In addition, the effect of teaching activity on MAD and longevity has been evaluated for scientists of different specialties. Special attention has been paid to the analysis of MAD of the deceased members of the Russian Academy of Sciences, including members of the USSR Academy of Sciences (1724–2013). The minimum MAD has been found for mathematicians (72.1 ± 0.21 years) and the maximum MAD for scientists in economics (74.6 ± 0.26 years). The relative number of surviving ≥90 years and ≥100 years is minimal for mathematicians (7.59 and 0.37%, respectively), whereas those numbers for economists reveal the maximum values (10.26 and 0.96%, respectively). Indicators of MAD and proportion of centenarians among the scientists who received public recognition strongly depend on the specialty. Similarly, the members of the Russian Academy of Sciences and the USSR Academy of Sciences have the highest MAD in economics (74.7 ± 1.05 years) and the lowest in mathematics (70.6 ± 0.74 years). MAD has proven to be 3.5 years higher for scientists involved in teaching at university or college compared to those who were not involved in teaching. In this case, the “gain” is significant, ranging from 3.1 years for economists and humanitarians to 4.9 years for mathematicians. The results of the study lead to the conclusion that intense scientific work contributes to an increase in life expectancy and longevity. © 2016, Allerton Press, Inc