15 research outputs found
Π ΠΎΠ»Ρ ΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ΅Π·Π΅ΡΠ²Π° ΠΊΡΠΎΠ²ΠΎΡΠΎΠΊΠ° Π² ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ ΡΠ°ΠΊΡΠΈΠΊΠΈ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΡ ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° ΠΏΡΠΈ ΡΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Β«Π»ΠΎΠΆΠ½ΡΡ Β» Π±ΠΈΡΡΡΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ ΡΡΠ΅Π½ΠΎΠ·ΠΎΠ² ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ Π°ΡΡΠ΅ΡΠΈΠΉ
Main vessel stenting in the Β«falseΒ» bifurcation coronary lesions compromises side branch vessel ostium often. Functional significance of the side vessel ostium narrowing after main vessel stenting was defined in 40 patients with II-III classes of stable angina pectoris with isolated Β«falseΒ» bifurcation coronary lesions by means of a fractional flow reserve (FFR). Average side branch vessel ostium narrowing was 69,8 Β± 8,7%, average value of FFR was detected 0,83 Β± 0,06. It was noted, that the visual estimation and the quantitative coronary angiography are unreliable methods in assessment of the severity of side branch vessel ostium narrowing. The results of our study demonstrate, that if FFR > 0,75 it is out of any benefit to conduct additional kissing balloon angioplasty of side brahch vessel ostium. Moreover, it was associated with high risk of side branch vessel dissection and ischemic myocardium injury.Π‘ΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ°Π³ΠΈΡΡΡΠ°Π»ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ Β«Π»ΠΎΠΆΠ½ΡΡ
Β» Π±ΠΈΡΡΡΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΡΠ΅Π½ΠΎΠ·ΠΎΠ² ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ ΡΠ°ΡΡΠΎ ΠΎΡΠ»ΠΎΠΆΠ½ΡΠ΅ΡΡΡ ΠΊΠΎΠΌΠΏΡΠΎΠΌΠ΅ΡΠ°ΡΠΈΠ΅ΠΉ ΡΡΡΡΡ Π±ΠΎΠΊΠΎΠ²ΠΎΠΉ Π²Π΅ΡΠ²ΠΈ. Π£ 40 Π±ΠΎΠ»ΡΠ½ΡΡ
ΡΠΎ ΡΡΠ°Π±ΠΈΠ»ΡΠ½ΡΠΌ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΡΠ΅Π½ΠΎΠΊΠ°ΡΠ΄ΠΈΠΈ II-III Π€Π Ρ ΠΈΠ·ΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Β«Π»ΠΎΠΆΠ½ΡΠΌΒ» Π±ΠΈΡΡΡΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΠΌ ΡΡΠ΅Π½ΠΎΠ·ΠΎΠΌ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ΅Π·Π΅ΡΠ²Π° ΠΊΡΠΎΠ²ΠΎΡΠΎΠΊΠ° (Π€Π Π) Π±ΡΠ»Π° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Π° ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½Π°Ρ Π·Π½Π°ΡΠΈΠΌΠΎΡΡΡ ΡΡΠΆΠ΅Π½ΠΈΡ ΡΡΡΡΡ Π±ΠΎΠΊΠΎΠ²ΠΎΠΉ Π²Π΅ΡΠ²ΠΈ ΠΏΠΎΡΠ»Π΅ ΡΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ°Π³ΠΈΡΡΠ°Π»ΡΠ½ΠΎΠΉ Π°ΡΡΠ΅ΡΠΈΠΈ. ΠΡΠΈ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΡΡΠΆΠ΅Π½ΠΈΡ ΡΡΡΡΠ΅Π² Π±ΠΎΠΊΠΎΠ²ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ Π½Π° 69,8 Β± 8,7%, ΡΡΠ΅Π΄Π½ΡΡ Π²Π΅Π»ΠΈΡΠΈΠ½Π° Π€Π Π ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° 0,83 Β± 0,06. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π²ΠΈΠ·ΡΠ°Π»ΡΠ½Π°Ρ ΠΎΡΠ΅Π½ΠΊΠ° ΠΈ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½Π°Ρ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½Π°Ρ Π°Π½Π³ΠΈΠΎΠ³ΡΠ°ΡΠΈΡ ΡΠ²Π»ΡΡΡΡΡ Π½Π΅Π½Π°Π΄Π΅ΠΆΠ½ΡΠΌΠΈ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌΠΈ ΠΏΡΠΈ ΠΎΡΠ΅Π½ΠΊΠ΅ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ Π·Π½Π°ΡΠΈΠΌΠΎΡΡΠΈ ΠΊΠΎΠΌΠΏΡΠΎΠΌΠ΅ΡΠ°ΡΠΈΠΈ ΡΡΡΡΠ΅Π² Π±ΠΎΠΊΠΎΠ²ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΡΡ, ΡΡΠΎ ΠΏΡΠΈ Π²Π΅Π»ΠΈΡΠΈΠ½Π΅ Π€Π Π > 0,75 ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ Π±Π°Π»Π»ΠΎΠ½Π½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠΏΠ»Π°ΡΡΠΈΠΊΠΈ Π² ΡΡΡΡΡΡ
ΡΠΊΠΎΠΌΠΏΡΠΎΠΌΠ΅ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
Π±ΠΎΠΊΠΎΠ²ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ Π½Π΅ ΡΠ»ΡΡΡΠ°Π΅Ρ ΠΎΡΠ΄Π°Π»Π΅Π½Π½ΡΠΉ ΠΏΡΠΎΠ³Π½ΠΎΠ·, Π² ΡΠΎ Π²ΡΠ΅ΠΌΡ ΠΊΠ°ΠΊ Π°ΡΡΠΎΡΠΈΠΈΡΡΠ΅ΡΡΡ Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠΈΡΠΊΠ° Π΄ΠΈΡΡΠ΅ΠΊΡΠΈΠΈ ΠΈΠ½ΡΠΈΠΌΡ Π±ΠΎΠΊΠΎΠ²ΡΡ
Π²Π΅ΡΠ²Π΅ΠΉ ΠΈ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π°
ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΡΡΠΎΠΉΡΡΠ² Π°ΡΠΏΠΈΡΠ°ΡΠΈΠΈ ΡΡΠΎΠΌΠ±Π° ΠΏΡΠΈ ΠΎΡΡΡΡΡ ΠΎΠΊΠΊΠ»ΡΠ·ΠΈΡΡ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ Π°ΡΡΠ΅ΡΠΈΠΉ
There were analyzed 38 patients with acute coronary syndrome with ST segment elevation. Every patient was revealed by coronary angiography to have an occlusion in one of the main coronary arteries. The patients were divided in two groups by the technique of percutaneous coronary intervention. In the first group (n = 18) after mechanical recanalisation with wire we used a catheter for thrombus aspiration. Furthermore according to results after coronary angiography these patients underwent either direct stenting or predilatation with further stenting. After mechanical recanalisation in the second group (n = 20) routine stenting with predilatation were performed. The reperfusion quality was evaluated by TIMI scale by the angiography and ST segment decrease during 30 minutes after the intervention. It was statistically proved that adequate reperfusion was achieved in the group with thrombus aspiration catheter.ΠΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈ Π»Π΅ΡΠ΅Π½ΠΈΡ 38 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΈΠ½ΡΠ°ΡΠΊΡΠΎΠΌ ΠΌΠΈΠΎΠΊΠ°ΡΠ΄Π° Ρ ΠΏΠΎΠ΄ΡΠ΅ΠΌΠΎΠΌ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ° ST. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠ³ΡΠ°ΡΠΈΠΈ Π²ΠΎ Π²ΡΠ΅Ρ
Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡΡ
ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»Π°ΡΡ ΠΎΠΊΠΊΠ»ΡΠ·ΠΈΡ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· ΠΌΠ°Π³ΠΈΡΡΡΠ°Π»ΡΠ½ΡΡ
ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ. ΠΠ°ΡΠΈΠ΅Π½ΡΡ Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° Π΄Π²Π΅ Π³ΡΡΠΏΠΏΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΠ°ΠΊΡΠΈΠΊΠΈ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΡΡΠ΅ΡΠΊΠΎΠΆΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π°. Π ΠΏΠ΅ΡΠ²ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ (n = 18) ΠΏΠΎΡΠ»Π΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅ΠΊΠ°Π½Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠΌ Π² Π·ΠΎΠ½Ρ ΠΎΠΊΠΊΠ»ΡΠ·ΠΈΠΈ Π²Π²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΊΠ°ΡΠ΅ΡΠ΅Ρ Π΄Π»Ρ Π°ΡΠΏΠΈΡΠ°ΡΠΈΠΈ ΡΡΠΎΠΌΠ±Π°. ΠΠ°Π»Π΅Π΅ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π°Π½Π³ΠΈΠΎΠ³ΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ° Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΎΡΡ ΠΏΡΡΠΌΠΎΠ΅ ΡΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΈΠ»ΠΈ ΠΏΡΠ΅Π΄Π²Π°ΡΠΈΡΠ΅Π»ΡΠ½Π°Ρ Π±Π°Π»Π»ΠΎΠ½Π½Π°Ρ Π°Π½Π³ΠΈΠΎΠΏΠ»Π°ΡΡΠΈΠΊΠ° Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ ΡΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ. ΠΠΎ Π²ΡΠΎΡΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ (n = 20) ΠΏΠΎΡΠ»Π΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅ΠΊΠ°Π½Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ Π²ΡΠΏΠΎΠ»Π½ΡΠ»Π°ΡΡ Π±Π°Π»Π»ΠΎΠ½Π½Π°Ρ Π°Π½Π³ΠΈΠΎΠΏΠ»Π°ΡΡΠΈΠΊΠ° Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ ΡΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ. ΠΠ΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎΡΡΡ ΡΠ΅ΠΏΠ΅ΡΡΡΠ·ΠΈΠΈ ΠΎΡΠ΅Π½ΠΈΠ²Π°Π»Π°ΡΡ ΠΏΠΎ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΊΡΠΎΠ²ΠΎΡΠΎΠΊΠ° ΠΏΠΎ ΡΠΊΠ°Π»Π΅ TIMI ΠΏΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΊΠΎΡΠΎΠ½Π°ΡΠ½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠ³ΡΠ°ΡΠΈΠΈ ΠΈ ΠΏΠΎ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠ΅Π³ΠΌΠ΅Π½ΡΠ° ST ΠΏΠΎ Π΄Π°Π½Π½ΡΠΌ ΠΠΠ ΡΠ΅ΡΠ΅Π· 30 ΠΌΠΈΠ½ΡΡ ΠΏΠΎΡΠ»Π΅ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π°. ΠΡΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΏΠ΅ΡΠ²ΠΎΠΉ ΠΈ Π²ΡΠΎΡΠΎΠΉ Π³ΡΡΠΏΠΏ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΠΎ ΡΠ°ΡΠ΅ Π² ΠΏΠ΅ΡΠ²ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠ΄Π°Π²Π°Π»ΠΎΡΡ Π΄ΠΎΡΡΠΈΠ³Π½ΡΡΡ Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎΠΉ ΡΠ΅ΠΏΠ΅ΡΡΡΠ·ΠΈΠΈ
Superluminal source of directional pulsed wideband electromagnetic radiation
A photoemission source of directional pulsed wideband electromagnetic radiation in the microwave region is developed, and the time profile of the generated pulse is investigated. The source is a vacuum photodiode of a parabolic shape in which a Cherenkov radiation pulse is formed by an electron current wave excited by an incident laser pulse and propagating along the surface of the anode mesh with a phase velocity higher than the speed of light. Β© 2014, Allerton Press, Inc
Superluminal source of directional pulsed wideband electromagnetic radiation
A photoemission source of directional pulsed wideband electromagnetic radiation in the microwave region is developed, and the time profile of the generated pulse is investigated. The source is a vacuum photodiode of a parabolic shape in which a Cherenkov radiation pulse is formed by an electron current wave excited by an incident laser pulse and propagating along the surface of the anode mesh with a phase velocity higher than the speed of light. Β© 2014, Allerton Press, Inc
Investigation of reactions using polarized and unpolarized deuteron beam at Nuclotron: current status and perspectives
Deuteron induced reactions at intermediate energies are investigated at Internal Target Station (ITS) of Nuclotron. The dp elastic scattering data have been accumulated in the angular range (70Β° - 120Β°) in c.m from 0.3 to 2.0 GeV of deuteron energy. Part of the obtained results of differential cross sections and analyzing powers of dp elastic scattering are compared with theoretical predictions based on relativistic multi-scattering model. The dp breakup data are obtained with the detection of two outgoing protons at the angles of (19Β° - 54Β°) in laboratory frame at the deuteron energies from 0.3 to 0.5 GeV in various detector configurations. One of the tools to study spin structure of short range correlations is the measurements of the cross section, tensor analyzing power T20 and spin correlation parameter Cy,y in the d3He β p(0Β°)4He reaction at the energies between 1.0 and 1.75 GeV using polarized 3He target and extracted polarized deuteron beam from new polarized ion source at Nuclotron. For this purposes the feasibility study has been performed. Proposed experiments on extracted deuteron beam of Nuclotron is aimed to investigate: non-nucleonic degrees of freedom and baryonic resonances properties in the d(A,d(0Β°))X and d(A,Ο-(0Β°))X reactions at different energies, non-nucleonic degrees of freedom via the measurements of the tensor Ayy and vector Ay analyzing powers in d(A,Ο-)X reaction and polarization properties of the baryonic resonances in the d(A,d)X reaction and others. First measurement of vector and tensor polarization of new polarized ion source has been performed in June-July of 2016y
Investigation of reactions using polarized and unpolarized deuteron beam at Nuclotron: current status and perspectives
Deuteron induced reactions at intermediate energies are investigated at Internal Target Station (ITS) of Nuclotron. The dp elastic scattering data have been accumulated in the angular range (70Β° - 120Β°) in c.m from 0.3 to 2.0 GeV of deuteron energy. Part of the obtained results of differential cross sections and analyzing powers of dp elastic scattering are compared with theoretical predictions based on relativistic multi-scattering model. The dp breakup data are obtained with the detection of two outgoing protons at the angles of (19Β° - 54Β°) in laboratory frame at the deuteron energies from 0.3 to 0.5 GeV in various detector configurations. One of the tools to study spin structure of short range correlations is the measurements of the cross section, tensor analyzing power T20 and spin correlation parameter Cy,y in the d3He β p(0Β°)4He reaction at the energies between 1.0 and 1.75 GeV using polarized 3He target and extracted polarized deuteron beam from new polarized ion source at Nuclotron. For this purposes the feasibility study has been performed. Proposed experiments on extracted deuteron beam of Nuclotron is aimed to investigate: non-nucleonic degrees of freedom and baryonic resonances properties in the d(A,d(0Β°))X and d(A,Ο-(0Β°))X reactions at different energies, non-nucleonic degrees of freedom via the measurements of the tensor Ayy and vector Ay analyzing powers in d(A,Ο-)X reaction and polarization properties of the baryonic resonances in the d(A,d)X reaction and others. First measurement of vector and tensor polarization of new polarized ion source has been performed in June-July of 2016y
Deuteron beam polarimeter at Nuclotron internal target
The current deuteron beam polarimetry at the Nuclotron is provided by the Internal Target polarimeter based on the use of the asymmetry in dpelastic scattering at large angles in the cms at 270 MeV. The upgraded deuteron beam polarimeter has been used to obtain the vector and tensor polarizations during 2016/2017 runs for the DSS experimental program. The polarimeter has been also used to tune the polarized ion source parameters for 6 different spin modes. The data analysis has been performed using the developed software based on C++ language and ROOT5 librar
Deuteron beam polarization measurement at 270 MeV at Nuclotron internal target
The current deuteron beam polarimetry at Nuclotron is provided by the Internal Target polarimeter based on the use of the asymmetry in dp-elastic scattering at large angles in the cms at 270 MeV. The upgraded deuteron beam polarimeter has been used to obtain the vector and tensor polarization during 2016 runs for the DSS experimental program. The polarimeter has been used also for tuning of the polarized ion source parameters for 6 different spin modes. The data analysis has been performed using developed software based on C++ language and ROOT5 library