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    Роль Ρ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ€Π΅Π·Π΅Ρ€Π²Π° ΠΊΡ€ΠΎΠ²ΠΎΡ‚ΠΎΠΊΠ° Π² ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠΈ Ρ‚Π°ΠΊΡ‚ΠΈΠΊΠΈ рСнтгСнохирургичСского Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π° ΠΏΡ€ΠΈ стСнтировании Β«Π»ΠΎΠΆΠ½Ρ‹Ρ…Β» Π±ΠΈΡ„ΡƒΡ€ΠΊΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… стСнозов ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½Ρ‹Ρ… Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΉ

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    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‘Ρ‚Π΅Π½Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ°Π³ΠΈΡΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΉ Β«Π»ΠΎΠΆΠ½Ρ‹Ρ…Β» Π±ΠΈΡ„ΡƒΡ€ΠΊΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… стСнозов ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½Ρ‹Ρ… Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΉ часто ослоТняСтся ΠΊΠΎΠΌΠΏΡ€ΠΎΠΌΠ΅Ρ‚Π°Ρ†ΠΈΠ΅ΠΉ ΡƒΡΡ‚ΡŒΡ Π±ΠΎΠΊΠΎΠ²ΠΎΠΉ Π²Π΅Ρ‚Π²ΠΈ. Π£ 40 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… со ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½Ρ‹ΠΌ Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ΠΌ стСнокардии II-III ЀК с ΠΈΠ·ΠΎΠ»ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΌ Β«Π»ΠΎΠΆΠ½Ρ‹ΠΌΒ» Π±ΠΈΡ„ΡƒΡ€ΠΊΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹ΠΌ стСнозом с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Ρ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ€Π΅Π·Π΅Ρ€Π²Π° ΠΊΡ€ΠΎΠ²ΠΎΡ‚ΠΎΠΊΠ° (ЀРК) Π±Ρ‹Π»Π° ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π° Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Π°Ρ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΡΡ‚ΡŒ суТСния ΡƒΡΡ‚ΡŒΡ Π±ΠΎΠΊΠΎΠ²ΠΎΠΉ Π²Π΅Ρ‚Π²ΠΈ послС стСнтирования ΠΌΠ°Π³ΠΈΡΡ‚Π°Π»ΡŒΠ½ΠΎΠΉ Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΈ. ΠŸΡ€ΠΈ срСднСй стСпСни суТСния ΡƒΡΡ‚ΡŒΠ΅Π² Π±ΠΎΠΊΠΎΠ²Ρ‹Ρ… Π²Π΅Ρ‚Π²Π΅ΠΉ Π½Π° 69,8 Β± 8,7%, срСдняя Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π° ЀРК составила 0,83 Β± 0,06. УстановлСно, Ρ‡Ρ‚ΠΎ Π²ΠΈΠ·ΡƒΠ°Π»ΡŒΠ½Π°Ρ ΠΎΡ†Π΅Π½ΠΊΠ° ΠΈ количСствСнная коронарная ангиография ΡΠ²Π»ΡΡŽΡ‚ΡΡ Π½Π΅Π½Π°Π΄Π΅ΠΆΠ½Ρ‹ΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ ΠΏΡ€ΠΈ ΠΎΡ†Π΅Π½ΠΊΠ΅ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠΉ значимости ΠΊΠΎΠΌΠΏΡ€ΠΎΠΌΠ΅Ρ‚Π°Ρ†ΠΈΠΈ ΡƒΡΡ‚ΡŒΠ΅Π² Π±ΠΎΠΊΠΎΠ²Ρ‹Ρ… Π²Π΅Ρ‚Π²Π΅ΠΉ. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΡƒΡŽΡ‚, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π΅ ЀРК > 0,75 ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π±Π°Π»Π»ΠΎΠ½Π½ΠΎΠΉ ангиопластики Π² ΡƒΡΡ‚ΡŒΡΡ… скомпромСтированных Π±ΠΎΠΊΠΎΠ²Ρ‹Ρ… Π²Π΅Ρ‚Π²Π΅ΠΉ Π½Π΅ ΡƒΠ»ΡƒΡ‡ΡˆΠ°Π΅Ρ‚ ΠΎΡ‚Π΄Π°Π»Π΅Π½Π½Ρ‹ΠΉ ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·, Π² Ρ‚ΠΎ врСмя ΠΊΠ°ΠΊ ассоциируСтся с ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ΠΌ риска диссСкции ΠΈΠ½Ρ‚ΠΈΠΌΡ‹ Π±ΠΎΠΊΠΎΠ²Ρ‹Ρ… Π²Π΅Ρ‚Π²Π΅ΠΉ ΠΈ ΠΈΡˆΠ΅ΠΌΠΈΡ‡Π΅ΡΠΊΠΈΠΌ ΠΏΠΎΠ²Ρ€Π΅ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ ΠΌΠΈΠΎΠΊΠ°Ρ€Π΄Π°

    ИспользованиС устройств аспирации Ρ‚Ρ€ΠΎΠΌΠ±Π° ΠΏΡ€ΠΈ острых ΠΎΠΊΠΊΠ»ΡŽΠ·ΠΈΡΡ… ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½Ρ‹Ρ… Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΉ

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    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.ΠŸΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ обслСдования ΠΈ лСчСния 38 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с ΠΈΠ½Ρ„Π°Ρ€ΠΊΡ‚ΠΎΠΌ ΠΌΠΈΠΎΠΊΠ°Ρ€Π΄Π° с подъСмом сСгмСнта ST. По Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ Π²ΠΎ всСх Π½Π°Π±Π»ΡŽΠ΄Π΅Π½ΠΈΡΡ… ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΡΠ»Π°ΡΡŒ окклюзия ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· ΠΌΠ°Π³ΠΈΡΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½Ρ‹Ρ… Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΉ. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Π±Ρ‹Π»ΠΈ Ρ€Π°Π·Π΄Π΅Π»Π΅Π½Ρ‹ Π½Π° Π΄Π²Π΅ Π³Ρ€ΡƒΠΏΠΏΡ‹ Π² зависимости ΠΎΡ‚ Ρ‚Π°ΠΊΡ‚ΠΈΠΊΠΈ выполнСния чрСскоТного ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½ΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π°. Π’ ΠΏΠ΅Ρ€Π²ΠΎΠΉ Π³Ρ€ΡƒΠΏΠΏΠ΅ (n = 18) послС мСханичСской Ρ€Π΅ΠΊΠ°Π½Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠΌ Π² Π·ΠΎΠ½Ρƒ окклюзии Π²Π²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΊΠ°Ρ‚Π΅Ρ‚Π΅Ρ€ для аспирации Ρ‚Ρ€ΠΎΠΌΠ±Π°. Π”Π°Π»Π΅Π΅ Π² зависимости ΠΎΡ‚ ангиографичСского Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π° Π²Ρ‹ΠΏΠΎΠ»Π½ΡΠ»ΠΎΡΡŒ прямоС стСнтированиС пораТСния ΠΈΠ»ΠΈ ΠΏΡ€Π΅Π΄Π²Π°Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ баллонная ангиопластика с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠΌ стСнтированиСм. Π’ΠΎ Π²Ρ‚ΠΎΡ€ΠΎΠΉ Π³Ρ€ΡƒΠΏΠΏΠ΅ (n = 20) послС мСханичСской Ρ€Π΅ΠΊΠ°Π½Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ Π²Ρ‹ΠΏΠΎΠ»Π½ΡΠ»Π°ΡΡŒ баллонная ангиопластика с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠΌ стСнтированиСм. ΠΠ΄Π΅ΠΊΠ²Π°Ρ‚Π½ΠΎΡΡ‚ΡŒ Ρ€Π΅ΠΏΠ΅Ρ€Ρ„ΡƒΠ·ΠΈΠΈ ΠΎΡ†Π΅Π½ΠΈΠ²Π°Π»Π°ΡΡŒ ΠΏΠΎ стСпСни восстановлСния ΠΊΡ€ΠΎΠ²ΠΎΡ‚ΠΎΠΊΠ° ΠΏΠΎ шкалС TIMI ΠΏΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ ΠΊΠΎΡ€ΠΎΠ½Π°Ρ€Π½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ ΠΈ ΠΏΠΎ сниТСнию сСгмСнта ST ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ Π­ΠšΠ“ Ρ‡Π΅Ρ€Π΅Π· 30 ΠΌΠΈΠ½ΡƒΡ‚ послС окончания Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π°. ΠŸΡ€ΠΈ сравнСнии Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠΏΠ΅Ρ€Π²ΠΎΠΉ ΠΈ Π²Ρ‚ΠΎΡ€ΠΎΠΉ Π³Ρ€ΡƒΠΏΠΏ установлСно, Ρ‡Ρ‚ΠΎ достовСрно Ρ‡Π°Ρ‰Π΅ Π² ΠΏΠ΅Ρ€Π²ΠΎΠΉ Π³Ρ€ΡƒΠΏΠΏΠ΅ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² ΡƒΠ΄Π°Π²Π°Π»ΠΎΡΡŒ Π΄ΠΎΡΡ‚ΠΈΠ³Π½ΡƒΡ‚ΡŒ Π°Π΄Π΅ΠΊΠ²Π°Ρ‚Π½ΠΎΠΉ Ρ€Π΅ΠΏΠ΅Ρ€Ρ„ΡƒΠ·ΠΈΠΈ

    Superluminal source of directional pulsed wideband electromagnetic radiation

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    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

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    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

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    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

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    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

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    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

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    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
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