111 research outputs found

    БтатистичСскоС исслСдованиС Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΏΠΈΠΈ ΠΈ астигматизма Π³Π»Π°Π·Π° Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ°

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    ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π°Π½Π°Π»Ρ–Π· Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»Ρƒ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΏΡ–Ρ— Ρ‚Π° астигматизму ΠΎΡ‡Π΅ΠΉ Π²Π΅Π»ΠΈΠΊΠΎΡ— ΠΊΡ–Π»ΡŒΠΊΠΎΡΡ‚Ρ– ΠΏΠ°Ρ†Ρ–Ρ”Π½Ρ‚Ρ–Π² ΠΎΡ„Ρ‚Π°Π»ΡŒΠΌΠΎΠ»ΠΎΠ³Ρ–Ρ‡Π½ΠΎΠ³ΠΎ ΠΊΠ°Π±Ρ–Π½Π΅Ρ‚Π°. ВиявлСно Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ Ρ€ΠΎΠ·ΠΏΠΎΠ΄Ρ–Π»Ρƒ Ρ†ΠΈΡ… ΠΏΠ΅Ρ€Π²ΠΈΠ½Π½ΠΈΡ… Π°Π±Π΅Ρ€Π°Ρ†Ρ–ΠΉ ΠΎΠΊΠ° людини. Показано, Π² яких Π΄Ρ–Π°ΠΏΠ°Π·ΠΎΠ½Π°Ρ… Π²ΠΎΠ½ΠΈ Π·ΡƒΡΡ‚Ρ€Ρ–Ρ‡Π°ΡŽΡ‚ΡŒΡΡ Π½Π°ΠΉΡ‡Π°ΡΡ‚Ρ–ΡˆΠ΅.The statistical analysis of the 930 patient’s eyes refractometry results is done. The bar charts of the ametropy and astigmatism value distributions according to eyes number are obtained. Working ranges of the economy-type ophthalmology aberrometer are specified.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ статистичСский Π°Π½Π°Π»ΠΈΠ· Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² Ρ€Π΅Ρ„Ρ€Π°ΠΊΡ‚ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ 930 Π³Π»Π°Π· ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ². ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ гистограммы распрСдСлСния количСства Π³Π»Π°Π· ΠΏΠΎ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π΅ Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΏΠΈΠΈ ΠΈ астигматизма. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ Ρ€Π°Π±ΠΎΡ‡ΠΈΠ΅ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Ρ‹ ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΏΠΈΠΈ ΠΈ астигматизма Π°Π±Π΅Ρ€Ρ€ΠΎΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ эконом-класса

    Validation, reproducibility and safety of trans dermal electrical stimulation in chronic pain patients and healthy volunteers

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    <p>Abstract</p> <p>Background</p> <p>Surrogate pain models have been extensively tested in Normal Human Volunteers (NHV). There are few studies that examined pain models in chronic pain patients. Patients are likely to have altered pain mechanisms. It is of interest to test patient pain responses to selective pain stimuli under controlled laboratory conditions.</p> <p>Methods</p> <p>The Institutional Ethic Committee approved the study. 16 patients with chronic neuropathic radiculopathy and 16 healthy volunteers were enrolled to the study after obtaining informed consent. During electrical stimulation (150 minutes for volunteers and 75 minutes for patients) the following parameters were measured every 10 minutes:</p> <p>Ongoing pain: Visual Analogue Scale (VAS) and Numeric Rate Scale (NRS)</p> <p>Allodynia (soft foam brush)</p> <p>Hyperalgesia (von Frey monofilament 20 g)</p> <p>Flare</p> <p>For each endpoint, the area under the curve (AUC) was estimated from the start of stimulation to the end of stimulation by the trapezoidal rule. The individual AUC values for both periods were plotted to show the inter- and intra-subject variability. For each endpoint a mixed effect model was fitted with random effect subject and fixed effect visit. The estimate of intra-subject variance and the mean value were then used to estimate the sample size of a crossover study required to have a probability of 0.80 to detect a 25% change in the mean value. Analysis was done using GenStat 8<sup>th </sup>edition.</p> <p>Results</p> <p>Each endpoint achieved very good reproducibility for patients and NHV. Comparison between groups revealed trends towards:</p> <p>Faster habituation to painful stimuli in patients</p> <p>Bigger areas of hyperalgesia in patients</p> <p>Similar area of allodynia and flare (no statistical significance)</p> <p>Conclusion</p> <p>The differences demonstrated between patients and NHVs suggest that the electrical stimulation device used here may stimulate pathways that are affected in the pathological state.</p

    ΠœΠ΅Ρ‚ΠΎΠ΄ восстановлСния Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΈ ΠΏΠΎ ΠΊΠ°Ρ€Ρ‚ΠΈΠ½Π°ΠΌ ΠΈΠ·ΠΎΠ΄ΠΈΠΎΠΏΡ‚Ρ€ΠΈΠΉΠ½Ρ‹Ρ… Π·ΠΎΠ½ Π½Π° Π·Ρ€Π°Ρ‡ΠΊΠ΅ Π³Π»Π°Π·Π°

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    Π“ΠΎΠ»ΠΎΠ²Π½ΠΎΡŽ Π·Π°Π΄Π°Ρ‡Π΅ΡŽ Π΄Π°Π½ΠΎΡ— Ρ€ΠΎΠ±ΠΎΡ‚ΠΈ Ρ” створСння ΠΌΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΡƒ відновлСння Ρ„ΡƒΠ½ΠΊΡ†Ρ–Ρ— Ρ…Π²ΠΈΠ»ΡŒΠΎΠ²ΠΎΡ— Π°Π±Π΅Ρ€Π°Ρ†Ρ–Ρ— Π·Π° Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌΠΈ відСозапису ΠΊΠ°Ρ€Ρ‚ΠΈΠ½ Ρ–Π·ΠΎΠ΄Ρ–ΠΎΠΏΡ‚Ρ€Ρ–ΠΉΠ½ΠΈΡ… Π·ΠΎΠ½ Ρƒ ΠΏΠ»ΠΎΡ‰ΠΈΠ½Ρ– Π·Ρ–Π½ΠΈΡ†Ρ–. ΠŸΠ΅Ρ€ΡˆΠΎΡŽ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€ΠΎΡŽ відновлСння Ρ” Ρ†ΠΈΡ„Ρ€ΠΎΠ²Π° Ρ„Ρ–Π»ΡŒΡ‚Ρ€Π°Ρ†Ρ–Ρ Π²Ρ–Π΄Π΅ΠΎΠΊΠ°Π΄Ρ€Ρ–Π² Π· ΠΌΠ΅Ρ‚ΠΎΡŽ виділСння Ρ–Π·ΠΎΠ΄Ρ–ΠΎΠΏΡ‚Ρ€Ρ–ΠΉΠ½ΠΈΡ… Π·ΠΎΠ½ освітлСності Ρ„ΠΎΡ‚ΠΎΠΏΡ€ΠΈΠΉΠΌΠ°Ρ‡Π°. Π”Ρ€ΡƒΠ³ΠΎΡŽ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€ΠΎΡŽ Ρ” виявлСння ΠΊΡƒΡ‚ΠΎΠ²ΠΈΡ… ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚ ΠΏΡ€ΠΎΠΌΠ΅Π½Ρ–Π², Ρ‰ΠΎ Π²ΠΈΡ…ΠΎΠ΄ΡΡ‚ΡŒ Π· ΠΎΠΊΠ°. ВрСтя ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€Π° – відновлСння Ρ„ΡƒΠ½ΠΊΡ†Ρ–Ρ— Ρ…Π²ΠΈΠ»ΡŒΠΎΠ²ΠΎΡ— Π°Π±Π΅Ρ€Π°Ρ†Ρ–Ρ— Ρƒ Π·Ρ–Π½ΠΈΡ‡Π½ΠΈΡ… ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚Π°Ρ…. Для Ρ†ΡŒΠΎΠ³ΠΎ Π²ΠΈΠΊΠΎΡ€ΠΈΡΡ‚ΠΎΠ²ΡƒΡ”Ρ‚ΡŒΡΡ апроксимація ΠΏΠΎΠ»Ρ–Π½ΠΎΠΌΠ°ΠΌΠΈ Π¦Π΅Ρ€Π½Ρ–ΠΊΠ΅. Амплітуди Π°Π±Π΅Ρ€Π°Ρ†Ρ–ΠΉΠ½ΠΈΡ… ΠΌΠΎΠ΄ Π²Ρ–Π΄Π½ΠΎΠ²Π»ΡŽΡŽΡ‚ΡŒΡΡ Π·Π° допомогою ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π½Π°ΠΉΠΌΠ΅Π½ΡˆΠΈΡ… ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚Ρ–Π² Π°Π±ΠΎ сингулярним Ρ€ΠΎΠ·ΠΊΠ»Π°Π΄ΠΎΠΌ.The main objective of this paper is to develop a mathematical algorithm for reconstruction of the wave aberration function, based on processing images of isodiopter zones, video-recorded at the pupil plane. To extract isodiopter zones from a photodetector illuminance picture, the first procedure should be digital filtering of video-images. The second procedure is to determine "in front of the eye" the angular coordinates of rays, emitting from the eye. These rays forms isodiopter zones in the pupil plane. The third procedure is to reconstruct the wave aberration function in pupil coordinates. For this purpose, the approximation with Zernike polynomials is applied. Amplitudes of aberration modes are reconstructed using the least-squares method or singular decomposition.Π“Π»Π°Π²Π½ΠΎΠΉ Π·Π°Π΄Π°Ρ‡Π΅ΠΉ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ являСтся созданиС матСматичСского Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° восстановлСния Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΈ ΠΏΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°ΠΌ видСозаписи ΠΊΠ°Ρ€Ρ‚ΠΈΠ½ ΠΈΠ·ΠΎΠ΄ΠΈΠΎΠΏΡ‚Ρ€ΠΈΠΉΠ½Ρ‹Ρ… Π·ΠΎΠ½ Π² плоскости Π·Ρ€Π°Ρ‡ΠΊΠ°. ΠŸΠ΅Ρ€Π²ΠΎΠΉ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€ΠΎΠΉ восстановлСния являСтся цифровая Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ†ΠΈΡ Π²ΠΈΠ΄Π΅ΠΎΠΊΠ°Π΄Ρ€ΠΎΠ² с Ρ†Π΅Π»ΡŒΡŽ выдСлСния ΠΈΠ·ΠΎΠ΄ΠΈΠΎΠΏΡ‚Ρ€ΠΈΠΉΠ½Ρ‹Ρ… Π·ΠΎΠ½ освСщСнности Ρ„ΠΎΡ‚ΠΎΠΏΡ€ΠΈΠ΅ΠΌΠ½ΠΈΠΊΠ°. Π’Ρ‚ΠΎΡ€ΠΎΠΉ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€ΠΎΠΉ являСтся ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΡƒΠ³Π»ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚ исходящих ΠΈΠ· Π³Π»Π°Π·Π° Π»ΡƒΡ‡Π΅ΠΉ. Π’Ρ€Π΅Ρ‚ΡŒΡ ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€Π° – восстановлСниС Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΈ Π² Π·Ρ€Π°Ρ‡ΠΊΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚Π°Ρ…. Для этого ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ аппроксимация ΠΏΠΎΠ»ΠΈΠ½ΠΎΠΌΠ°ΠΌΠΈ Π¦Π΅Ρ€Π½ΠΈΠΊΠ΅. Амплитуды Π°Π±Π΅Ρ€Ρ€Π°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ΠΌΠΎΠ΄ Π²ΠΎΡΡΡ‚Π°Π½Π°Π²Π»ΠΈΠ²Π°ΡŽΡ‚ΡΡ посрСдством ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π½Π°ΠΈΠΌΠ΅Π½ΡŒΡˆΠΈΡ… ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚ΠΎΠ² ΠΈΠ»ΠΈ сингулярного разлоТСния

    Π Π•Π–Π˜Πœ ΠžΠ”ΠΠžΠ§ΠΠ‘Π’ΠžΠ’ΠΠžΠ™ Π“Π•ΠΠ•Π ΠΠ¦Π˜Π˜ Π’ ΠžΠŸΠ’ΠžΠ­Π›Π•ΠšΠ’Π ΠžΠΠΠžΠœ Π“Π•ΠΠ•Π ΠΠ’ΠžΠ Π• Π‘Π’Π§ НА Π›Π˜ΠΠ˜Π―Π₯ Π—ΠΠ”Π•Π Π–ΠšΠ˜ Π‘ ΠžΠŸΠ’Π˜Π§Π•Π‘ΠšΠ˜Πœ Π£Π‘Π˜Π›Π•ΠΠ˜Π•Πœ

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    The theoretical investigation of the single-frequency oscillation in all-optical gain optoelectronic oscillator based on fiberoptic delay lines is performed. It is shown that there is no need in microwave phase shifters within the optoelectronic oscillator loop in order to provide low phase noise and spurious level oscillations. Threshold of the dynamical instabilities in the all-optical gain optoelectronic oscillator is calculated. It is shown that the reproducibility of the oscillation frequency is provided by means of the continuous tuning of the loop gain during the switching-on.Β Π’ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Π΅ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ тСорСтичСскоС исслСдованиС квазигармоничСской Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ Π² оптоэлСктронном Π³Π΅Π½Π΅Ρ€Π°Ρ‚ΠΎΡ€Π΅ Π½Π° линиях Π·Π°Π΄Π΅Ρ€ΠΆΠΊΠΈ с оптичСским усилСниСм. Π Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°ΡŽΡ‚ΡΡ особСнности примСнСния Π‘Π’Π§-Ρ„Π°Π·ΠΎΠ²Ρ€Π°Ρ‰Π°Ρ‚Π΅Π»Π΅ΠΉ для обСспСчСния квазигармоничСской Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ с Π½ΠΈΠ·ΠΊΠΈΠΌ Ρ„Π°Π·ΠΎΠ²Ρ‹ΠΌ ΡˆΡƒΠΌΠΎΠΌ ΠΈ ΡƒΡ€ΠΎΠ²Π½Π΅ΠΌ дискрСтных ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΡ… Π² спСктрС Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ рассчитано ΠΏΠΎΡ€ΠΎΠ³ΠΎΠ²ΠΎΠ΅ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ коэффициСнта усилСния ΠΊΠΎΠ½Ρ‚ΡƒΡ€Π° ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связи, ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ Π² оптоэлСктронном Π³Π΅Π½Π΅Ρ€Π°Ρ‚ΠΎΡ€Π΅ Π½Π° линиях Π·Π°Π΄Π΅Ρ€ΠΆΠΊΠΈ с оптичСским усилСниСм наступаСт Ρ€Π΅ΠΆΠΈΠΌ динамичСских Π½Π΅ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚Π΅ΠΉ Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅Ρ‚ΠΎΠ΄ обСспСчСния установлСния Π³Π΅Π½Π΅Ρ€Π°Ρ†ΠΈΠΈ Π² оптоэлСктронном Π³Π΅Π½Π΅Ρ€Π°Ρ‚ΠΎΡ€Π΅ Π½Π° частотС максимального усилСния.

    ВСплофизичСскиС свойства ΠΈ структура ΠΎΡ‚Π»ΠΎΠΆΠ΅Π½ΠΈΠΉ Π½Π° повСрхностях Π½Π°Π³Ρ€Π΅Π²Π° энСргСтичСского оборудования

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    The paper shows influence of heating surface material, design peculiarities, operational conditions of heat exchangers and water-chemical regime on chemical and structural composition of deposits, their heat conduction and porosity.Показано влияниС ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° повСрхности Π½Π°Π³Ρ€Π΅Π²Π°, конструктивных особСнностСй, условий эксплуатации Ρ‚Π΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π½Ρ‹Ρ… устройств ΠΈ Π²ΠΎΠ΄Π½ΠΎ-химичСского Ρ€Π΅ΠΆΠΈΠΌΠ° Π½Π° химичСский ΠΈ структурный состав ΠΎΡ‚Π»ΠΎΠΆΠ΅Π½ΠΈΠΉ, ΠΈΡ… Ρ‚Π΅ΠΏΠ»ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒ ΠΈ ΠΏΠΎΡ€ΠΈΡΡ‚ΠΎΡΡ‚ΡŒ

    The Role of Interdiffusion and Spatial Confinement in the Formation of Resonant Raman Spectra of Ge/Si(100) Heterostructures with Quantum-Dot Arrays

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    The phonon modes of self-assembled Ge/Si quantum dots grown by molecular-beam epitaxy in an apparatus integrated with a chamber of the scanning tunneling microscope into a single high-vacuum system are investigated using Raman spectroscopy. It is revealed that the Ge-Ge and Si-Ge vibrational modes are considerably enhanced upon excitation of excitons between the valence band Ξ›3\Lambda_3 and the conduction band Ξ›1\Lambda_1 (the E1 and E1 + Ξ”1\Delta_1 transitions). This makes it possible to observe the Raman spectrum of very small amounts of germanium, such as one layer of quantum dots with a germanium layer thickness of 10 \r{A}. The enhancement of these modes suggests a strong electron-phonon interaction of the vibrational modes with the E1 and E1 + Ξ”1\Delta_1 excitons in the quantum dot. It is demonstrated that the frequency of the Ge-Ge mode decreases by 10 cm^-1 with a decrease in the thickness of the Ge layer from 10 to 6 \r{A} due to the spatial-confinement effect. The optimum thickness of the Ge layer, for which the size dispersion of quantum dots is minimum, is determined.Comment: 14 pages, 9 figure
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