Cognitive Function Estimation in Children with Tuberous Sclerosis

Tuberous sclerosis (TSC) is a genetic disease characterized by cerebral structural abnormalities (such as cortical tubers, subependymal nodes and abnormal cerebral white matter) which are detected by means of neuroimaging methods (e.g., MRI). Typically, these events cause neurological complications (i.e., epilepsy).Objective: cognitive function estimation in TSC children considering severity and nature of clinical course of the disease. 15 children with tuberous sclerosis (i.e., experimental group) and 46 children with normal development (i.e., control group) aged 6-16 years old underwent neuropsychological examination. As a result, polymorphic disorders of higher mental functions were revealed in TSC children. Neuropsychological deficit (p<0.05) was detected. Namely, voluntary attention and memorization impairments were found in TSC children with normaldevelopment. Operational thinking disorders, immaturity of dynamic and kinesthetic movement basis, somatosensory gnosis, optical spatial or quasi-three-dimensional imaging, as well as insufficient oral/aural and semantical memorization were mentioned in TSC children with mental retardation. Regardless of mental development, TSC children demonstrate neurodynamic activity disorder (p<0.05) presented by slow task performance, increased exhaustibility and attention fluctuation. According to comparison between research findings and clinical course data, severity of cognitive disorders substantially depends on epilepsy onset age because early onset results in more severe developmental disorder (p<0.05). Since tuberous sclerosis is a dynamic disease with new potential symptoms arising over a lifetime, neuropsychological testing will provide timely mental status qualification and development of corrective actions to activate the cognitive activity of a child. Keywords: tuberous sclerosis, children, higher mental function (HMF) developmental disorders

Behaviour of the Blazar CTA 102 during two giant outbursts

Blazar CTA 102 underwent exceptional optical and high-energy outbursts in 2012 and 2016-2017. We analyze its behaviour during these events, focusing on polarimetry as a tool that allows us to trace changes in the physical conditions and geometric configuration of the emission source close to the central black hole. We also use Fermi gamma-ray data in conjunction with optical photometry in an effort to localize the origin of the outbursts.AST-1615796 - Boston Universit

The analysis of change of structure of production personnel at the industrial enterprise

The article gives recommendations on increasing the level of organization of work with personnel in an industrial enterpriseВ статье даются рекомендации по повышению уровня организации работы с персоналом на промышленном предприяти

Energy Level Displacement of Excited np State of Kaonic Deuterium In Faddeev Equation Approach

We calculate the energy level displacement of the excited $np$ state of kaonic deuterium in terms of the P-wave scattering length of $K^-d$ scattering. We solve the Faddeev equations for the amplitude of $K^-d$ scattering in the fixed centre approximation and derive the complex P-wave scattering length of $K^-d$ scattering in terms of the S-wave and P-wave scattering lengths of $\bar{K}N$ scattering. The estimated uncertainty of the complex P-wave scattering length is of about $15\,$. For the calculated width $\Gamma_{2p} = 10.203\,{\rm meV}$ of the excited $2p$ state of kaonic deuterium we evaluate the yield $Y_{K^-d} = 0.27\,$ of $X$-rays for the $K_{\alpha}$ emission line of kaonic deuterium. Using the complex S-wave and P-wave scattering lengths of $\bar{K}N$ scattering, calculated in \cite{ECL1,Weise1}, we get the width $\Gamma_{2p} = 2.675\,{\rm meV}$ of the excited $2p$ state and the yield $Y_{K^-d} = 1.90 \,$ of $X$-rays for the $K_{\alpha}$ emission line of kaonic deuterium. The results, obtained in this paper, can be used for the planning of experiments on the measurements of the energy level displacement of the ground state of kaonic deuterium, caused by strong low-energy interactions.Comment: 13 page

On the influence of the magnetic field of the GSI experimental storage ring on the time-modulation of the EC-decay rates of the H-like mother ions

We investigate the influence of the magnetic field of the Experimental storage ring (ESR) at GSI on the periodic time-dependence of the orbital K-shell electron capture decay $(EC$) rates of the H--like heavy ions. We approximate the magnetic field of the ESR by a uniform magnetic field. Unlike the assertion by Lambiase et al., arXiv: 0811.2302 [nucl-th], we show that a motion of the H-like heavy ion in a uniform magnetic field cannot be the origin of the periodic time-dependence of the EC-decay rates of the H-like heavy ions.Comment: 3 pages, 1 figur

On the estimate of the sigma^(I = 1)_(KN)(0)-term value from the energy level shift of kaonic hydrogen in the ground state

Using the experimental data on the energy level shift of kaonic hydrogen in the ground state (the DEAR Collaboration, Phys. Rev. Lett. 94, 212302 (2005)) and the theoretical value of the energy level shift, calculated within the phenomenological quantum field theoretic approach to the description of strong low-energy anti-K N and anti-K NN interactions developed at Stefan Meyer Institut fuer subatomare Physik in Vienna, we estimate the value of the sigma^(I = 1)_(KN)(0)-term of low-energy anti-K N scattering. We get sigma^(I = 1)_(KN)(0) = (433 +/- 85) MeV. This testifies the absence of strange quarks in the proton structure.Comment: 7 pages, no figure

Evolution of small-scale turbulence at large Richardson numbers

The theory of stratified turbulent flow developed earlier by the authors is applied to data from different areas of the ocean. It is shown that turbulence can be amplified and supported even at large gradient Richardson numbers. The cause of that is the exchange between kinetic and potential energies of turbulence. Using the profiles of Brunt–Väisälä frequency and vertical current shear given in Forryan et al. (2013), the profiles of the kinetic energy dissipation rate are calculated. The results are in reasonable agreement with the experimental data.</p