189 research outputs found

    Cranial Nerve Palsy Should Not Be Included within a Primary Composite Endpoint in Carotid Surgery Trials

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    Status of the Circle of Willis and Intolerance to Carotid Cross-clamping

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    Commentary

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    Carotid Revascularization to Prevent Stroke

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    Current Status of Clinical Magnetic Resonance Imaging for Plaque Characterisation in Patients with Carotid Artery Stenosis

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    AbstractObjectiveThe article aims to provide an overview of the literature that assessed the agreement between magnetic resonance imaging (MRI) and histology for specific carotid plaque characteristics associated with vulnerability in terms of sensitivity and specificity.MethodsA systematic search strategy was conducted in MEDLINE and EMBASE databases resulting in 1084 articles. Finally, we included 17 papers. Due to variation in presentation, especially in MRI and histology methods, a pooled analysis could not be performed.ResultsTwo studies were performed on a 3.0-T MRI scanner; all other studies were performed on a 1.5-T scanner. Most performed sequences were two-dimensional (2D) and three-dimensional (3D) T1-weighted and all histology protocols varied slightly. Our results indicate that calcification, fibrous cap, intraplaque haemorrhage and lipid-rich necrotic cores can be identified with moderate-to-good sensitivity and specificity.ConclusionsBased on current literature, it appears premature for routine application of MRI as an imaging modality to assess carotid plaque characteristics associated with plaque vulnerability. Although MRI still holds promise, clinical application for plaque characterisation would require consensus regarding MRI settings and confirmation by histology. Predefined protocols for histology and MR imaging need to be established

    Mast cell distribution in human carotid atherosclerotic plaque differs significantly by histological segment

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    Mast cells (MCs) are important contributors to atherosclerotic plaque progression. For prospective studies on mast cell contributions to plaque instability, the distribution of intraplaque MCs needs to be elucidated. Plaque stability is generally histologically assessed by dividing the plaque specimen into segments to be scored on an ordinal scale. However, owing to competitive use, studies may have to deviate to adjacent segments, yet intersegment differences of plaque characteristics, especially MCs, are largely unknown. Therefore, the hypothesis that there is no segment to segment difference in MC distribution between atherosclerotic plaque segments was tested, and intersegment associations between MCs and other plaque characteristics was investigated.\nTwenty-six carotid atherosclerotic plaques from patients undergoing carotid endarterectomy included in the Athero-Express Biobank were analysed. The plaque was divided in 5 mm segments, differentiating between the culprit lesion (segment 0), adjacent segments (-1/+1) and more distant segments (-2/+2) for the presence of MCs. The associations between the intersegment distribution of MCs and smooth muscle cells, macrophage content, and microvessel density in the culprit lesion were studied.\nA statistically significant difference in MCs/mm2 between the different plaque segments (p 2 between the culprit and adjacent segment (pΒ = .037) and between the culprit lesion and the more distant segment (p 2 in multiple different segments were positively correlated with microvessel density and macrophage content in the culprit lesion.\nMC numbers reveal significant intersegment differences in human carotid plaques. Future histological studies on MCs should use a standardised segment for plaque characterisation as plaque segments cannot be used interchangeably for histological MC analyses.Biopharmaceutic

    ВивчСння процСсу синтСзу нанокристалічних ΠΏΠ»Ρ–Π²ΠΎΠΊ двооксиду Ρ‚ΠΈΡ‚Π°Π½Ρƒ Π² розряді ΠΌΠ°Π³Π½Π΅Ρ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΡƒ Π·Π° ΠΉΠΎΠ³ΠΎ ΠΎΠΏΡ‚ΠΈΡ‡Π½ΠΈΠΌΠΈ Ρ‚Π° ΠΏΠ»Π°Π·ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΡ–Ρ‡Π½ΠΈΠΌΠΈ характСристиками

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    НавСдСно Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΈ Π΅ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ дослiдТСння ΠΏΠ»Π°Π·ΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌiΡ‡Π½ΠΈΡ… i ΠΎΠΏΡ‚ΠΈΡ‡Π½ΠΈΡ… характСристик Ρ†ΠΈΠ»iΠ½Π΄Ρ€ΠΈΡ‡Π½ΠΎΠ³ΠΎ Π³Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ розряду ΠΌΠ°Π³Π½Π΅Ρ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΡƒ Π² ΡƒΠΌΠΎΠ²Π°Ρ… Π±Π΅Π·ΠΏΠ΅Ρ€Π΅Ρ€Π²Π½ΠΎΠ³ΠΎ ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŽ спСктра, Π²ΠΈΠΏΡ€ΠΎΠΌiнюваного плазмою Π² Π΄iΠ°ΠΏΠ°Π·ΠΎΠ½i 350–820 Π½ΠΌ. Π’ΠΈΠ·Π½Π°Ρ‡Π΅Π½ΠΎ ΡƒΠΌΠΎΠ²ΠΈ для синтСзу Π±iΠ½Π°Ρ€Π½ΠΎΡ— сполуки TiΠžβ‚‚, якi Π·Π°Π±Π΅Π·ΠΏΠ΅Ρ‡ΡƒΡŽΡ‚ΡŒΡΡ ΠΏiΠ΄Ρ‚Ρ€ΠΈΠΌΠΊΠΎΡŽ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ΠΈ iнтСнсивностi ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΈΡ… Π»iΠ½iΠΉ Ρ€Π΅Π°Π³ΡƒΡŽΡ‡ΠΈΡ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚iΠ² i ΠΏΠ»Π°Π·ΠΌΠΎΡƒΡ‚Π²ΠΎΡ€ΡŽΡŽΡ‡ΠΎΠ³ΠΎ Π³Π°Π·Ρƒ. Розглянуто ΠΌΠΎΠΆΠ»ΠΈΠ²iΡΡ‚ΡŒ ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŽ ΡƒΠΌΠΎΠ² одСрТання ΠΏΠ»iΠ²ΠΎΠΊ TiΠžβ‚‚ як ΠΏΠΎ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΈΡ… характСристиках ΠΏΠ»Π°Π·ΠΌΠΈ розряду, Ρ‚Π°ΠΊ i ΠΏΠΎ Π·ΠΌiΠ½i розрядної Π½Π°ΠΏΡ€ΡƒΠ³ΠΈ. Π•Π»iпсомСтричнi дослiдТСння нанокристалiΡ‡Π½ΠΈΡ… ΠΏΠ»iΠ²ΠΎΠΊ двооксиду Ρ‚ΠΈΡ‚Π°Π½Ρƒ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ наявнiΡΡ‚ΡŒ залСТностi ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠ° пСрСломлСння Π²iΠ΄ Ρ‚ΠΎΠ²Ρ‰ΠΈΠ½ΠΈ ΠΏΠ»iΠ²ΠΊΠΈ.We present the results of experimental researches of plasmodynamic and optical characteristics of a magnetron-type cylindrical gas discharge. The study was carried out provided a permanent monitoring of the spectrum emitted by plasma in the range 350–820 nm. For the synthesis of binary compound TiOβ‚‚, we have determined conditions which can be ensured by a support of the intensity of spectral lines emitted by reacting components and plasma-forming gas. A possibility to control the conditions of the fabrication of a TiOβ‚‚ film with the use of both the spectral characteristics of a discharge plasma and a variation of the discharge voltage has been analyzed. Ellipsometric and spectral studies of nanocrystalline titanium dioxide films revealed the dependence of the refractive index of a film on the film thickness.ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ исслСдования плазмодинамичСских ΠΈ оптичСских характСристик цилиндричСского Π³Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ разряда ΠΌΠ°Π³Π½Π΅Ρ‚Ρ€ΠΎΠ½Π½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ° Π² условиях Π½Π΅ΠΏΡ€Π΅Ρ€Ρ‹Π²Π½ΠΎΠ³ΠΎ контроля спСктра, ΠΈΠ·Π»ΡƒΡ‡Π°Π΅ΠΌΠΎΠ³ΠΎ ΠΏΠ»Π°Π·ΠΌΠΎΠΉ Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ 350–820 Π½ΠΌ. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ условия для синтСза Π±ΠΈΠ½Π°Ρ€Π½ΠΎΠ³ΠΎ соСдинСния TiΠžβ‚‚, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‚ΡΡ ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠ°Π½ΠΈΠ΅ΠΌ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ интСнсивности ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… Π»ΠΈΠ½ΠΈΠΉ Ρ€Π΅Π°Π³ΠΈΡ€ΡƒΡŽΡ‰ΠΈΡ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ ΠΈ ΠΏΠ»Π°Π·ΠΌΠΎΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰Π΅Π³ΠΎ Π³Π°Π·Π°. РассмотрСна Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ контроля условий получСния ΠΏΠ»Π΅Π½ΠΎΠΊ TiOβ‚‚ ΠΊΠ°ΠΊ ΠΏΠΎ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹ΠΌ характСристикам ΠΏΠ»Π°Π·ΠΌΡ‹ разряда, Ρ‚Π°ΠΊ ΠΈ ΠΏΠΎ измСнСнию разрядного напряТСния. ЭллипсомСтричСскиС ΠΈ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½Ρ‹Π΅ исслСдования нанокристалличСских ΠΏΠ»Π΅Π½ΠΎΠΊ диоксида Ρ‚ΠΈΡ‚Π°Π½Π° ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ зависимости показатСля прСломлСния ΠΎΡ‚ Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Ρ‹ ΠΏΠ»Π΅Π½ΠΊΠΈ
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