395 research outputs found
Π‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π±ΠΈΠΎΠΌΠ΅Ρ Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ°Ρ ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΈ Π±Π΅Π·ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠ³ΠΎ Π²ΠΈΠ΄Π΅ΠΎΠ·Π°Ρ Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ
Motion capture systems are a key tool for performing quantitative analysis and evaluation of complex in movements sports. The prospect of the development and practical application of markerless motion capture tecnology in applied biomechanics increases research interest regarding the features of using such systems, as well as evaluat ing their accuracy and reliability in comparison with marker-based motion capture systems, which are the gold standard nowadays. Markerless motion capture systems have incomparable advantages over marker-based ones.In particular, significantly reduced time costs for the registration and data processing procedures, since registration is represented by filming a video from different angles, and processing is accompanied by the use of software algorithms for tracking the silhouette of an athlete using a presetted computer avatar. However, there is still no clear answer regarding the accuracy and reliability of the data recorded using markerless motion capture systems in relation to specific sports movements. Thus, the purpose of the presented work is to assess the statistical relationship of the data based on the correlation analysis of biomechanical variables on the example of a golf swing recorded using the Qualisys motion capture system and Simi Reality Motion markerless motion capture system.Π‘ΠΈΡΡΠ΅ΠΌΡ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΡΠ²Π»ΡΡΡΡΡ ΠΊΠ»ΡΡΠ΅Π²ΡΠΌ ΠΈΠ½ΡΡΡΡΠΌΠ΅Π½ΡΠΎΠΌ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΠ΅Ρ
Π½ΠΈΠΊΠΈ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Π² ΡΠ»ΠΎΠΆΠ½ΠΎΠΊΠΎΠΎΡΠ΄ΠΈΠ½Π°ΡΠΈΠΎΠ½Π½ΡΡ
Π²ΠΈΠ΄Π°Ρ
ΡΠΏΠΎΡΡΠ°. ΠΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π° ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΈ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΡ Π² ΠΏΡΠ°ΠΊΡΠΈΠΊΡ ΠΏΡΠΈΠΊΠ»Π°Π΄Π½ΠΎΠΉ Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠΈ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π±Π΅Π·ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎΠ²ΡΡΠ°Π΅Ρ Π½Π°ΡΡΠ½ΠΎ-ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΡΠΊΠΈΠΉ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ ΠΊ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ΄ΠΎΠ±Π½ΡΡ
ΡΠΈΡΡΠ΅ΠΌ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΊ ΠΎΡΠ΅Π½ΠΊΠ΅ ΠΈΡ
ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΈ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΠΈ Π² ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Ρ ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΡΠΌΠΈ ΡΠΈΡΡΠ΅ΠΌΠ°ΠΌΠΈ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠ΅Π³ΠΎΠ΄Π½Ρ ΡΠ²Π»ΡΡΡΡΡ Π·ΠΎΠ»ΠΎΡΡΠΌ ΡΡΠ°Π½Π΄Π°ΡΡΠΎΠΌ. Π‘ΠΈΡΡΠ΅ΠΌΡ Π±Π΅Π·ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π½Π΅ΡΡΠ°Π²Π½Π΅Π½Π½ΡΠΌΠΈ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π°ΠΌΠΈ ΠΏΠ΅ΡΠ΅Π΄ ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΡΠΌΠΈ. Π ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΡΠΌΠ΅Π½ΡΡΠ΅Π½Ρ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ Π·Π°ΡΡΠ°ΡΡ Π½Π° ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΡ ΠΈ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΡ Π΄Π°Π½Π½ΡΡ
, ΠΏΠΎΡΠΊΠΎΠ»ΡΠΊΡ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΡΠΎΠ±ΠΎΠΉ ΡΡΠ΅ΠΌΠΊΡ Π²ΠΈΠ΄Π΅ΠΎ Ρ ΡΠ°Π·Π½ΡΡ
ΡΠ°ΠΊΡΡΡΠΎΠ², Π° ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ° ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°Π΅ΡΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΡΡ
Π°Π»Π³ΠΎΡΠΈΡΠΌΠΎΠ² ΠΎΡΡΠ»Π΅ΠΆΠΈΠ²Π°Π½ΠΈΡ ΡΠΈΠ»ΡΡΡΠ° ΡΠΏΠΎΡΡΡΠΌΠ΅Π½Π° ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΠΊΠΎΠΌΠΏΡΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π°Π²Π°ΡΠ°ΡΠ°. ΠΠ΄Π½Π°ΠΊΠΎ Π΄ΠΎ ΡΠΈΡ
ΠΏΠΎΡ Π½Π΅Ρ ΠΎΠ΄Π½ΠΎΠ·Π½Π°ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠ²Π΅ΡΠ° ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΈ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎΡΡΠΈ Π΄Π°Π½Π½ΡΡ
, ΡΠ΅Π³ΠΈΡΡΡΠΈΡΡΠ΅ΠΌΡΡ
Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΈΡΡΠ΅ΠΌ Π±Π΅Π·ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΏΡΠΈΠΌΠ΅Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΊ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΡΠΌ Π²ΠΈΠ΄Π°ΠΌ ΡΠΏΠΎΡΡΠ° ΠΈ ΡΠΏΠΎΡΡΠΈΠ²Π½ΡΠΌ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡΠΌ. Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΠΎΡΠ΅Π½ΠΊΠ° ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·ΠΈ Π΄Π°Π½Π½ΡΡ
Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΡΠ΄Π°ΡΠ° Π² Π³ΠΎΠ»ΡΡΠ΅, Π·Π°ΡΠ΅Π³ΠΈΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Qualisys ΠΈ Π±Π΅Π·ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ Π·Π°Ρ
Π²Π°ΡΠ° Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ Simi Reality Motion
Excitonic instability and electric-field-induced phase transition towards a two dimensional exciton condensate
We present an InAs-GaSb-based system in which the electric-field tunability
of its 2D energy gap implies a transition towards a thermodynamically stable
excitonic condensed phase. Detailed calculations show a 3 meV BCS-like gap
appearing in a second-order phase transition with electric field. We find this
transition to be very sharp, solely due to exchange interaction, and so, the
exciton binding energy is greatly renormalized even at small condensate
densities. This density gradually increases with external field, thus enabling
the direct probe of the Bose-Einstein to BCS crossover.Comment: LaTex, 11 pages, 3 ps figures, To appear in PR
High-pressure x-ray diffraction study on the structure and phase transitions of the defect-stannite ZnGa2Se4 and defect-chalcopyrite CdGa2S4
X-ray diffraction measurements on the sphalerite-derivatives ZnGa2Se4 and
CdGa2S4 have been performed upon compression up to 23 GPa in a diamond-anvil
cell. ZnGa2Se4 exhibits a defect tetragonal stannite-type structure (I-42m) up
to 15.5 GPa and in the range from 15.5 GPa to 18.5 GPa the low-pressure phase
coexists with a high-pressure phase, which remains stable up to 23 GPa. In
CdGa2S4, we find the defect tetragonal chalcopyrite-type structure (I-4) is
stable up to 17 GPa. Beyond this pressure a pressure-induced phase transition
takes place. In both materials, the high-pressure phase has been characterized
as a defect-cubic NaCl-type structure (Fm-3m). The occurrence of the pressure
induced phase transitions is apparently related with an increase of the cation
disorder on the semiconductors investigated. In addition, the results allow the
evaluation of the axial compressibility and the determination of the equation
of state for each compound. The obtained results are compared with those
previously reported for isomorphic digallium sellenides. Finally, a systematic
study of the pressure-induced phase transition in twenty-three different
sphalerite-related ABX2 and AB2X4 compounds indicates that the transition
pressure increases as the ratio of the cationic radii and anionic radii of the
compounds increases.Comment: 34 pages, 3 tables, 6 figure
Technologies for measuring the dynamic parameters of rowing based on strain gauge systems
One of the criteria for the effectiveness of flatwater rowing biomechanics is the interaction of the athlete with the surface of the water by an oar, as well as the effectiveness of transferring the efforts developed by the athlete to the boat for its advancement. The quality of an athlete's move-ments with a paddle in rowing locomotives depends on the level of development of power abilities and can be quantified using strain gauge systems. However, the lack of recommendations describ-ing the specifics of the preparation and use of such systems in training process significantly reduce the degree of their use. The article discusses the technical features and methodological founda-tions of the use of strain gauge systems to measure the efforts of an athlete when interacting with an oar in flatwater kayaking and canoeing. To substantiate the choice of the scheme of loading and securing the paddle when graduating the strain gauge system, as well as the place of its direct attachment to the forearm, the authors carried out mathematical modeling of diagrams of bending moments arising on the paddle in response to external forces, as a result of which three options for the support and orientation of the paddle are presented, depending on the location of key sup-port points. To substantiate the method of attaching the strain gauge system to the forearm, a series of tests with paddle loading was carried out, as a result of which the presence of a linear relationship between the values of the external load and the readings of the strain gauge system was assessed, as well as the repeatability of the recorded data. Based on the results of the as-sessment, recommendations are presented for the practical application of the results of the study in assessing the speed and strength training of rowers on kayaks and canoes.ΠΠ΄Π½ΠΈΠΌ ΠΈΠ· ΠΊΡΠΈΡΠ΅ΡΠΈΠ΅Π² ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΠΈ Π³ΡΠ΅Π±Π»ΠΈ Π½Π° ΠΏΠ»ΠΎΡΠΊΠΎΠΉ Π²ΠΎΠ΄Π΅ ΡΠ²Π»ΡΠ΅ΡΡΡ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΡΠΏΠΎΡΡΡΠΌΠ΅Π½Π° Ρ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ Π²ΠΎΠ΄Ρ ΠΏΡΠΈ ΠΏΠΎΠΌΠΎΡΠΈ Π²Π΅ΡΠ»Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΏΠ΅ΡΠ΅Π΄Π°ΡΠΈ ΡΡΠΈΠ»ΠΈΠΉ, ΡΠ°Π·Π²ΠΈΠ²Π°Π΅ΠΌΡΡ
ΡΠΏΠΎΡΡΡΠΌΠ΅Π½ΠΎΠΌ, Π½Π° Π»ΠΎΠ΄ΠΊΡ Π΄Π»Ρ Π΅Π΅ ΠΏΡΠΎΠ΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ. ΠΠ°ΡΠ΅ΡΡΠ²ΠΎ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΡΠΏΠΎΡΡΡΠΌΠ΅Π½Π° Ρ Π²Π΅ΡΠ»ΠΎΠΌ Π² Π³ΡΠ΅Π±Π½ΡΡ
ΡΡΠ΅Π½Π°ΠΆΠ΅ΡΠ°Ρ
Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΡΡΠΎΠ²Π½Ρ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠΈΠ»ΠΎΠ²ΡΡ
ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΠ΅ΠΉ ΠΈ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΠΎΡΠ΅Π½Π΅Π½ΠΎ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠ΅Π½Π·ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ. ΠΠ΄Π½Π°ΠΊΠΎ ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΉ, ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΠΈΡ
ΡΠΏΠ΅ΡΠΈΡΠΈΠΊΡ ΠΏΠΎΠ΄Π³ΠΎΡΠΎΠ²ΠΊΠΈ ΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ°ΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ Π² ΡΡΠ΅Π½ΠΈΡΠΎΠ²ΠΎΡΠ½ΠΎΠΌ ΠΏΡΠΎΡΠ΅ΡΡΠ΅, ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΡΠ½ΠΈΠΆΠ°Π΅Ρ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΈΡ
ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ. Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡ ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΎΡΠ½ΠΎΠ²Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Π½Π·ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ Π΄Π»Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΡΠΈΠ»ΠΈΠΉ ΡΠΏΠΎΡΡΡΠΌΠ΅Π½Π° ΠΏΡΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ Ρ Π²Π΅ΡΠ»ΠΎΠΌ Π² ΠΏΠ»Π°Π²Π°Π½ΠΈΠΈ Π½Π° ΠΏΠ»ΠΎΡΠΊΠΈΡ
Π±Π°ΠΉΠ΄Π°ΡΠΊΠ°Ρ
ΠΈ ΠΊΠ°Π½ΠΎΡ. ΠΠ»Ρ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ Π²ΡΠ±ΠΎΡΠ° ΡΡ
Π΅ΠΌΡ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΈ Π·Π°ΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ Π»ΠΎΠΏΠ°ΡΠΊΠΈ ΠΏΡΠΈ Π³ΡΠ°Π΄ΡΠΈΡΠΎΠ²ΠΊΠ΅ ΡΠ΅Π½Π·ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΌΠ΅ΡΡΠ° Π΅Π΅ Π½Π΅ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΊ ΡΠ΅Π²ΡΡ, Π°Π²ΡΠΎΡΠ°ΠΌΠΈ Π±ΡΠ»ΠΎ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π΄ΠΈΠ°Π³ΡΠ°ΠΌΠΌ ΠΈΠ·Π³ΠΈΠ±Π°ΡΡΠΈΡ
ΠΌΠΎΠΌΠ΅Π½ΡΠΎΠ², Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΡ
Π½Π° Π»ΠΎΠΏΠ°ΡΠΊΠ΅ Π² ΠΎΡΠ²Π΅Ρ Π½Π° Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ Π²Π½Π΅ΡΠ½ΠΈΡ
ΡΠΈΠ», Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ Π±ΡΠ»ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ ΡΡΠΈ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π²Π°ΡΠΈΠ°Π½ΡΡ ΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΈ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ Π»ΠΎΠΏΠ°ΡΡΠΈ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΡ ΠΊΠ»ΡΡΠ΅Π²ΡΡ
ΡΠΎΡΠ΅ΠΊ ΠΎΠΏΠΎΡΡ. ΠΠ»Ρ ΠΎΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ ΡΠΏΠΎΡΠΎΠ±Π° ΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΡΠ΅Π½Π·ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΊ ΠΏΡΠ΅Π΄ΠΏΠ»Π΅ΡΡΡ Π±ΡΠ»Π° ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π° ΡΠ΅ΡΠΈΡ ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ Ρ Π»ΠΎΠΏΠ°ΡΡΠ½ΠΎΠΉ Π½Π°Π³ΡΡΠ·ΠΊΠΎΠΉ, Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΊΠΎΡΠΎΡΡΡ
Π±ΡΠ»ΠΎ ΠΎΡΠ΅Π½Π΅Π½ΠΎ Π½Π°Π»ΠΈΡΠΈΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΌΠ΅ΠΆΠ΄Ρ Π·Π½Π°ΡΠ΅Π½ΠΈΡΠΌΠΈ Π²Π½Π΅ΡΠ½Π΅ΠΉ Π½Π°Π³ΡΡΠ·ΠΊΠΈ ΠΈ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΈΡΠΌΠΈ ΡΠ΅Π½Π·ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΏΠΎΠ²ΡΠΎΡΡΠ΅ΠΌΠΎΡΡΡ Π·Π°ΠΏΠΈΡΠ°Π½Π½ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΎΡΠ΅Π½ΠΊΠΈ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΈ ΠΏΠΎ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΈ ΠΎΡΠ΅Π½ΠΊΠ΅ ΡΠΊΠΎΡΠΎΡΡΠ½ΠΎ-ΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΠΏΠΎΠ΄Π³ΠΎΡΠΎΠ²ΠΊΠΈ Π³ΡΠ΅Π±ΡΠΎΠ² Π½Π° Π±Π°ΠΉΠ΄Π°ΡΠΊΠ°Ρ
ΠΈ ΠΊΠ°Π½ΠΎΡ
Charged vortices in superfluid systems with pairing of spatially separated carriers
It is shown that in a magnetic field the vortices in superfluid electron-hole
systems carry a real electrical charge. The charge value depends on the
relation between the magnetic length and the Bohr radiuses of electrons and
holes. In double layer systems at equal electron and hole filling factors in
the case of the electron and hole Bohr radiuses much larger than the magnetic
length the vortex charge is equal to the universal value (electron charge times
the filling factor).Comment: 4 page
Bilateral percutaneous mininephrolithotripsy: simultaneous or staged approach?
Introduction. Patients with bilateral nephrolithiasis are a challenge for the treating physician. Therefore, such patients traditionally are subject to phased surgery to reduce the rate of complications. At the same time, the enhancement of endoscopic technologies and anesthesia makes it possible to perform surgical treatment of bilateral nephrolithiasis simultaneously.Objective. To evaluate the effectiveness and safety of performing simultaneous bilateral percutaneous nephrolithotripsy (PCNL).Materials & methods. The main group comprises 19 patients (avg age 45.0 Β± 2.25 years) suffering from bilateral nephrolithiasis (13 men and 6 women). The control group include 20 patients (avg age 45.80 Β± 2.29 years) suffering from bilateral nephrolithiasis. Main group patients underwent simultaneous bilateral mini-PCNL, control group patients β staged PCNL within two hospitalisations. The visual analogue scale (VAS) was used to assess the pain severity. Patients noted subjective pain sensations on post-op days 1 and 3. QoL indicators were assessed using the SF-36 general questionnaire, as well as the Russian-language validated version of the WISQoL questionnaire.Results. There were no statistically significant differences between the parameters (the difference between the hemoglobin before and after mini-PCNL was 12 g/l; between the serum creatinine was 18 Β΅mol/l). There was a decrease in total surgery time (121.0 Β± 6.1 min) for main group patients compared to (147.0 Β± 7.3 min) control group patients (total surgery time during the first and second hospitalisations) and a reduction in hospital stay (4.50 Β± 0.23 days) for main group patients compared to control group patients (10.0 Β± 0.5 days). Complications observed by us in the two groups were comparable. The valuesobtained on the SF, RE and MH scales in main group patients were higher both on post-op day 1 (67.9 Β± 3.39; 56.90 Β± 2.85 and 63.80 Β± 3.19, respectively) and post-op day 3 (86.80 Β± 4.34; 83.70 Β± 4.19 and 82.50 Β± 4.13, respectively) compared to control group patients during the first and second hospitalizations. Statistically significant differences were also recorded according to the grades "Social functioning" and "Emotional influence" in main group patients (80.90 Β± 0.26 and 82.6 Β± 0.19, respectively).Conclusion. Simultaneous bilateral mini-PCNL is safe and effective in well-selected patients
Models of coherent exciton condensation
That excitons in solids might condense into a phase-coherent ground state was
proposed about 40 years ago, and has been attracting experimental and
theoretical attention ever since. Although experimental confirmation has been
hard to come by, the concepts released by this phenomenon have been widely
influential. This tutorial review discusses general aspects of the theory of
exciton and polariton condensates, focussing on the reasons for coherence in
the ground state wavefunction, the BCS to Bose crossover(s) for excitons and
for polaritons, and the relationship of the coherent condensates to standard
lasers.Comment: 27 pages, 6 figures. Submitted for a special issue of J. Phys. Cond.
Matt. associated with the EU network "Photon-mediated phenomena in
semiconductor nanostructures
Mimicking diffuse supernova antineutrinos with the Sun as a source
Measuring the electron antineutrino component of the cosmic diffuse supernova
neutrino background (DSNB) is the next ambitious goal for low-energy neutrino
astronomy. The largest flux is expected in the lowest accessible energy bin.
However, for E < 15 MeV a possible signal can be mimicked by a solar electron
antineutrino flux that originates from the usual 8B neutrinos by spin-flavor
oscillations. We show that such an interpretation is possible within the
allowed range of neutrino electromagnetic transition moments and solar
turbulent field strengths and distributions. Therefore, an unambiguous
detection of the DSNB requires a significant number of events at E > 15 MeV.Comment: 4 pages, 1 figur
The Relation Between the Surface Brightness and the Diameter for Galactic Supernova Remnants
In this work, we have constructed a relation between the surface brightness
() and diameter (D) of Galactic C- and S-type supernova remnants
(SNRs). In order to calibrate the -D dependence, we have carefully
examined some intrinsic (e.g. explosion energy) and extrinsic (e.g. density of
the ambient medium) properties of the remnants and, taking into account also
the distance values given in the literature, we have adopted distances for some
of the SNRs which have relatively more reliable distance values. These
calibrator SNRs are all C- and S-type SNRs, i.e. F-type SNRs (and S-type SNR
Cas A which has an exceptionally high surface brightness) are excluded. The
Sigma-D relation has 2 slopes with a turning point at D=36.5 pc: (at 1
GHz)=8.4 D
WmHzster (for
WmHzster and D36.5 pc) and (at 1
GHz)=2.7 10 D
WmHzster (for
WmHzster and D36.5 pc). We discussed the theoretical
basis for the -D dependence and particularly the reasons for the change
in slope of the relation were stated. Added to this, we have shown the
dependence between the radio luminosity and the diameter which seems to have a
slope close to zero up to about D=36.5 pc. We have also adopted distance and
diameter values for all of the observed Galactic SNRs by examining all the
available distance values presented in the literature together with the
distances found from our -D relation.Comment: 45 pages, 2 figures, accepted for publication in Astronomical and
Astrophysical Transaction
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