32 research outputs found

    Π₯ирургичСскоС Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΌΠΎΠ»ΠΎΡ‚ΠΊΠΎΠΎΠ±Ρ€Π°Π·Π½ΠΎΠΉ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΏΠ°Π»ΡŒΡ†Π΅Π² стоп (ΠΎΠ±Π·ΠΎΡ€ Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹)

    Get PDF
    The high prevalence of hammertoe deformity in the population, the effect of this pathology on the ability and the quality of life allow us to consider this pathology as a important medical problem. The most common surgery is arthrodesis of the proximal interphalangeal joint with a Weil-osteotomy. Specific complication is a floating toe, which leads to overload of adjacent toes and metatarsal heads. For to correct the instability of the metatarsophalangeal joint, the flexor to extensor transfer Girdlestone-Taylor can be used. However, the use of this procedure had limitations associated with difficult surgery techniques and below the average cosmetic result of the procedure. In the study of the causes of hammertoe deformity, the conclusion of the importance of the plantar plate of the metatarsophalangeal joint was made. Plantar plate repair leads to the stabilization of the metatarsophalangeal joint, reduces the risk of developing a floating toe, leads to the restoration of the support function and normal biomechanics of movement and foot function. Simultaneously, the plantar plate repair technically complicates surgical treatment. An promising direction of treatment is minimally invasive technologies for correction of hammertoe deformity that can reduce the risk of infectious complications, improve the cosmetic result of the surgery and reduce the risk of postoperative contracture in the joint, the time of the operation and rehabilitation, postoperative pain, emotional stress for the patient. However, the technique this type of surgery is more difficult, it requires a long training of the surgeon. The potential risk of intraoperative damage to various anatomical structures increases, which requires use of special tools during surgery. The choice of the surgical procedures is based on the individual characteristics of the pathological changes in the patients foot, the equipment of the operating room and the experience of the surgeon. It is necessary to evaluate the elasticity of the deformity, the stability of the metatarsophalangeal joint, the presence and severity of concomitant overloading metatarsalgia, as well as to take into account the subjective personalized requirements and expectations of the patient.Широкая Ρ€Π°ΡΠΏΡ€ΠΎΡΡ‚Ρ€Π°Π½Π΅Π½Π½ΠΎΡΡ‚ΡŒ ΠΌΠΎΠ»ΠΎΡ‚ΠΊΠΎΠΎΠ±Ρ€Π°Π·Π½ΠΎΠΉ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΏΠ°Π»ΡŒΡ†Π΅Π² стоп, влияниС Π΄Π°Π½Π½ΠΎΠΉ ΠΏΠ°Ρ‚ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π½Π° Ρ‚Ρ€ΡƒΠ΄ΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ ΠΈ качСство ΠΆΠΈΠ·Π½ΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΡΡ‡ΠΈΡ‚Π°Ρ‚ΡŒ Π΅Π΅ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΠΉ мСдицинской ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠΎΠΉ. НаиболСС распространСнная опСрация Π² настоящСС врСмя ― Π°Ρ€Ρ‚Ρ€ΠΎΠ΄Π΅Π· ΠΏΡ€ΠΎΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΌΠ΅ΠΆΡ„Π°Π»Π°Π½Π³ΠΎΠ²ΠΎΠ³ΠΎ сустава Π² сочСтании с Weil-остСотомиСй. БпСцифичСскоС ослоТнСниС ― Ρ„Π»ΠΎΡ‚ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΉ ΠΏΠ°Π»Π΅Ρ† ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΏΠ΅Ρ€Π΅Π³Ρ€ΡƒΠ·ΠΊΠ΅ смСТных ΠΏΠ°Π»ΡŒΡ†Π΅Π² ΠΈ Π³ΠΎΠ»ΠΎΠ²ΠΎΠΊ ΠΏΠ»ΡŽΡΠ½Π΅Π²Ρ‹Ρ… костСй. Одной ΠΈΠ· ΠΏΡ€ΠΈΡ‡ΠΈΠ½ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ослоТнСния являСтся Π½Π΅ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΡŒ ΠΏΠ»ΡŽΡΠ½Π΅Ρ„Π°Π»Π°Π½Π³ΠΎΠ²ΠΎΠ³ΠΎ сустава, для ΠΊΠΎΡ€Ρ€Π΅ΠΊΡ†ΠΈΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ опСрация ΠΏΠΎ транспозиции сухоТилия Π΄Π»ΠΈΠ½Π½ΠΎΠ³ΠΎ сгибатСля ΠΏΠ°Π»ΡŒΡ†Π° Π½Π° ΠΏΡ€ΠΎΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½ΡƒΡŽ Ρ„Π°Π»Π°Π½Π³Ρƒ. ИспользованиС Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ ΠΈΠΌΠ΅Π΅Ρ‚ ограничСния, связанныС со слоТной Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΎΠΉ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ ΠΈ посрСдствСнным космСтичСским Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠΌ. ΠŸΡ€ΠΈ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠΈ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ ΠΌΠΎΠ»ΠΎΡ‚ΠΊΠΎΠΎΠ±Ρ€Π°Π·Π½ΠΎΠΉ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΏΠ°Π»ΡŒΡ†Π΅Π² Π±Ρ‹Π» сдСлан Π²Ρ‹Π²ΠΎΠ΄ ΠΎ Π²Π°ΠΆΠ½ΠΎΠΌ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΈ подошвСнной связки ΠΏΠ»ΡŽΡΠ½Π΅Ρ„Π°Π»Π°Π½Π³ΠΎΠ²ΠΎΠ³ΠΎ сустава, восстановлСниС ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ стабилизации сустава, восстанавливаСт ΠΎΠΏΠΎΡ€Π½ΡƒΡŽ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΡŽ ΠΈ Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΡƒΡŽ Π±ΠΈΠΎΠΌΠ΅Ρ…Π°Π½ΠΈΠΊΡƒ стопы. ΠŸΠ΅Ρ€ΡΠΏΠ΅ΠΊΡ‚ΠΈΠ²Π½Ρ‹ΠΌ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ лСчСния ΠΌΠΎΠ»ΠΎΡ‚ΠΊΠΎΠΎΠ±Ρ€Π°Π·Π½ΠΎΠΉ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ являСтся использованиС ΠΌΠ°Π»ΠΎΠΈΠ½Π²Π°Π·ΠΈΠ²Π½Ρ‹Ρ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΡΠ½ΠΈΠ·ΠΈΡ‚ΡŒ риск ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ослоТнСний, послСопСрационной ΠΊΠΎΠ½Ρ‚Ρ€Π°ΠΊΡ‚ΡƒΡ€Ρ‹ сустава, ΡΠΎΠΊΡ€Π°Ρ‚ΠΈΡ‚ΡŒ врСмя провСдСния ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ, сроки Ρ€Π΅Π°Π±ΠΈΠ»ΠΈΡ‚Π°Ρ†ΠΈΠΈ, ΡƒΠΌΠ΅Π½ΡŒΡˆΠΈΡ‚ΡŒ послСопСрационный Π±ΠΎΠ»Π΅Π²ΠΎΠΉ синдром. Π’Π΅Ρ…Π½ΠΈΠΊΠ° минимальной ΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΠΎΠΉ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ слоТнСС, Ρ‚Ρ€Π΅Π±ΡƒΠ΅Ρ‚ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ обучСния Ρ…ΠΈΡ€ΡƒΡ€Π³Π°, ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ контроля Π·Π° послСопСрационным Π²Π΅Π΄Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°, ΠΈΠΌΠ΅Π΅Ρ‚ Π±ΠΎΠ»Π΅Π΅ высокий ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΉ риск ΠΈΠ½Ρ‚Ρ€Π°ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ поврСТдСния анатомичСских структур. Π’Ρ‹Π±ΠΎΡ€ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° лСчСния основываСтся Π½Π° ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡƒΠ°Π»ΡŒΠ½Ρ‹Ρ… особСнностях патологичСских ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ стопы ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°, тСхничСских возмоТностях ΠΈ ΠΎΠΏΡ‹Ρ‚Π΅ Ρ…ΠΈΡ€ΡƒΡ€Π³Π°. ΠŸΡ€ΠΈ Π²Ρ‹Π±ΠΎΡ€Π΅ Ρ‚Π°ΠΊΡ‚ΠΈΠΊΠΈ лСчСния Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΠΎΡ†Π΅Π½ΠΈΠ²Π°Ρ‚ΡŒ ΡΠ»Π°ΡΡ‚ΠΈΡ‡Π½ΠΎΡΡ‚ΡŒ Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ, ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΏΠ»ΡŽΡΠ½Π΅Ρ„Π°Π»Π°Π½Π³ΠΎΠ²ΠΎΠ³ΠΎ сустава, Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ ΠΈ Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½ΠΎΡΡ‚ΡŒ ΡΠΎΠΏΡƒΡ‚ΡΡ‚Π²ΡƒΡŽΡ‰Π΅ΠΉ ΠΏΠ΅Ρ€Π΅Π³Ρ€ΡƒΠ·ΠΎΡ‡Π½ΠΎΠΉ ΠΌΠ΅Ρ‚Π°Ρ‚Π°Ρ€Π·Π°Π»Π³ΠΈΠΈ; ΡƒΡ‡ΠΈΡ‚Ρ‹Π²Π°Ρ‚ΡŒ пСрсонифицированныС трСбования ΠΈ оТидания ΠΊΠΎΠ½ΠΊΡ€Π΅Ρ‚Π½ΠΎΠ³ΠΎ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ хирургичСского лСчСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ², ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Π°Π²Ρ‚ΠΎΡ€ΠΎΠ², ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ опросника AOFAS для Ρ€Π΅Π·Π΅ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠΉ артропластики ΠΏΡ€ΠΎΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ ΠΌΠ΅ΠΆΡ„Π°Π»Π°Π½Π³ΠΎΠ²ΠΎΠ³ΠΎ сустава, ΡƒΠ»ΡƒΡ‡ΡˆΠΈΠ»ΠΈΡΡŒ Π² срСднСм Π² 2,4 Ρ€Π°Π·Π° (Π΄ΠΎ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ 36,1 Π±Π°Π»Π»Π°, Π½Π° ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½ΠΎΠΌ осмотрС 87,3 Π±Π°Π»Π»Π°). По Π²ΠΈΠ·ΡƒΠ°Π»ΡŒΠ½ΠΎΠΉ Π°Π½Π°Π»ΠΎΠ³ΠΎΠ²ΠΎΠΉ шкалС (ВАШ) ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»Π°ΡΡŒ ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ° Π² 4,8 Ρ€Π°Π·Π° (Π΄ΠΎ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ 7,2, Π½Π° ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½ΠΎΠΌ осмотрС 1,5). ΠŸΡ€ΠΈ восстановлСнии подошвСнной связки срСднСС ΡƒΠ»ΡƒΡ‡ΡˆΠ΅Π½ΠΈΠ΅ ΠΏΠΎ опроснику AOFAS Ρƒ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Π°Π²Ρ‚ΠΎΡ€ΠΎΠ² составило 1,8 Ρ€Π°Π·Π° (Π΄ΠΎ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ 47,2, Π½Π° ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½ΠΎΠΌ осмотрС 85,1). По шкалС ВАШ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΡƒΠ»ΡƒΡ‡ΡˆΠΈΠ»ΠΈΡΡŒ Π² 5,7 Ρ€Π°Π·Π° (Π΄ΠΎ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ 6,8, Π½Π° ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒΠ½ΠΎΠΌ осмотрС 1,2). ΠŸΡ€ΠΈ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ минимально ΠΈΠ½Π²Π°Π·ΠΈΠ²Π½Ρ‹Ρ… ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊ ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€Π΅Π½Π½ΠΎΡΡ‚ΡŒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² составила 87,3%. ΠŸΡ€ΠΈ пСрСсадкС сухоТилий послСопСрационный Π±Π°Π»Π» ΠΏΠΎ шкалС AOFAS составил 83,4. Π”ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π΄Π°Π½Π½Ρ‹Ρ… ΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°Ρ… Π½Π΅ прСдставлСно, Π»ΠΈΠ±ΠΎ ΠΎΠ½ΠΈ прСдставлСны Π² нСдостаточном объСмС

    Roughness distributions for 1/f^alpha signals

    Full text link
    The probability density function (PDF) of the roughness, i.e., of the temporal variance, of 1/f^alpha noise signals is studied. Our starting point is the generalization of the model of Gaussian, time-periodic, 1/f noise, discussed in our recent Letter [T. Antal et al., PRL, vol. 87, 240601 (2001)], to arbitrary power law. We investigate three main scaling regions, distinguished by the scaling of the cumulants in terms of the microscopic scale and the total length of the period. Various analytical representations of the PDF allow for a precise numerical evaluation of the scaling function of the PDF for any alpha. A simulation of the periodic process makes it possible to study also non-periodic signals on short intervals embedded in the full period. We find that for alpha=<1/2 the scaled PDF-s in both the periodic and the non-periodic cases are Gaussian, but for alpha>1/2 they differ from the Gaussian and from each other. Both deviations increase with growing alpha. That conclusion, based on numerics, is reinforced by analytic results for alpha=2 and alpha->infinity. We suggest that our theoretical and numerical results open a new perspective on the data analysis of 1/f^alpha processes.Comment: 12 pages incl. 6 figures, with RevTex4, for A4 paper, in v2 some references were correcte

    Miniband-related 1.4–1.8 ΞΌm luminescence of Ge/Si quantum dot superlattices

    Get PDF
    The luminescence properties of highly strained, Sb-doped Ge/Si multi-layer heterostructures with incorporated Ge quantum dots (QDs) are studied. Calculations of the electronic band structure and luminescence measurements prove the existence of an electron miniband within the columns of the QDs. Miniband formation results in a conversion of the indirect to a quasi-direct excitons takes place. The optical transitions between electron states within the miniband and hole states within QDs are responsible for an intense luminescence in the 1.4–1.8 Β΅m range, which is maintained up to room temperature. At 300 K, a light emitting diode based on such Ge/Si QD superlattices demonstrates an external quantum efficiency of 0.04% at a wavelength of 1.55 Β΅m

    A simple test of the Gaussian character of noise

    No full text
    The test consists in the measurement of the noise intensity at the output of a bandpass filter, and the estimation of the accuracy of the measurement. The confidence interval for the estimate is calculated under the assumption that the noise is stationary and Gaussian. This assumption is called "zero-hypothesis". If a considerable part of the experimental data is outside the confidence interval, then the zero-hypothesis does not hold. The effect of noise being non-Gaussian is investigated analytically. Experimental data of 1/f noise in GaAs epitaxial films are presented and discussed

    A new tool for the investigation of the nature of 1/f noise

    No full text

    Nieuwe analyse methode voor 1/f ruis

    No full text

    Bispectrum of the 1/F noise in diodes on quantum dots and wells

    No full text
    The bispectrum of the 1/f noise is investigated in the present work. For the Gaussian noise it equals zero. LEDs on self-organized InAs/GaAs quantum dots and laser diodes on In0.2Ga0.8As/GaAs/InGaP quantum wells made in Russia were tested. The voltage noise was analyzed in a wide interval of currents through the diodes. Estimates of the probability density function and semi-invariants of the noise have not revealed any appreciable deviations from the Gauss law. Noise spectra Sv(f)in the range 1 Hz - 20 kHz were analyzed. In most cases the frequency exponent Ξ³s of the spectrum is close to one, the Hooge’s parameter Ξ±H has magnitude of the order 10-4. The bispectrum Bv(f1,f2of the noise is a complex function of frequencies f1 and f2. Its absolute value is decreasing while moving from the beginning of the frequency plane Of1f2. The decrease along the bisector (f1 = f2 = f) follows the power law characterized by the frequency exponent Ξ³B β‰ˆ 1.5 Ξ³s. The dependence of the "height" of |Bv(f,f)| on the current through the diode is qualitatively similar to this one for the spectrum. The power law describes these dependences, however the exponents are essentially different
    corecore