135 research outputs found

    The poetic works of Sergey Yesenin in Germany: translations, editions, and research

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    The article was submitted on 21.01.2017.This article considers the perception of Sergey Yesenin’s creative work in Germany. Having become acquainted with his works in its own language as early as the 1920s, Germany played the leading role in incorporating Yesenin into Germanlanguage culture. This research is based on the rich history of translation reception (made up of over 300 texts by over 60 translators), criticism and literary studies, and publication history. The article focuses on topical issues of modern literary studies, such as the aesthetics of reception, the dialogue of cultures, comparative studies, and imagology. The perception of the poet reflects the development of Russo-German literary connections in the 20th and 21st centuries. It is possible to single out three stages in the translation reception of Yesenin’s works: acquaintance (1920s), popularisation (1950s–1980s), and the modern period. During the third stage, the reader came closer to understanding the authentic concepts of Yesenin’s poetic semantics and techniques and a better knowledge of his creative work. The peculiarities of the publication history of the poet’s works are to a large extent determined by the above stages, as well as the cultural and historical factors caused by the division of Germany. German-language Yesenin studies are characterised by a vast scope, multiple research strategies, and prominent researchers (D. Chizhevsky, D. Gerhardt, F. Mierau, etc.). The receptive character of the perception determines the combination of literary and translation strategies, which are mutually complementary. Hence, it is quite appropriate to consider German Yesenin studies a separate branch of the world literary studies. The results of German scholars’ work are of significant importance to the history of Russian literature. The final stage of the perception model is the creative perception of the image of the poet as part of one’s native linguistic culture. Dedication poems devoted to Yesenin written by G. Vesper and H. Czechowski in the 1990s are proof of a contemporary German dialogue with the Russian poet.РассмотрСно восприятиС творчСства БСргСя ЕсСнина Π² Π“Π΅Ρ€ΠΌΠ°Π½ΠΈΠΈ. Познакомившись с Π΅Π³ΠΎ наслСдиСм Π½Π° своСм Ρ€ΠΎΠ΄Π½ΠΎΠΌ языкС ΡƒΠΆΠ΅ Π² 1920 Π³., ГСрмания являСтся Π»ΠΈΠ΄Π΅Ρ€ΠΎΠΌ ΠΏΠΎ ΠΎΠ±ΡŠΠ΅ΠΌΡƒ ΠΈ ΠΌΠ°ΡΡˆΡ‚Π°Π±Ρƒ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ ЕсСнина Π² Π½Π΅ΠΌΠ΅Ρ†ΠΊΠΎΡΠ·Ρ‹Ρ‡Π½ΡƒΡŽ ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Ρƒ. Богатая история пСрСводчСской Ρ€Π΅Ρ†Π΅ΠΏΡ†ΠΈΠΈ, ΠΊΠΎΡ‚ΠΎΡ€ΡƒΡŽ ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‚ Π±ΠΎΠ»Π΅Π΅ 300 тСкстов ΠΈ ΡΠ²Ρ‹ΡˆΠ΅ 60 ΠΏΠ΅Ρ€Π΅Π²ΠΎΠ΄Ρ‡ΠΈΠΊΠΎΠ², ΡΠ°ΠΌΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ критичСских ΠΈ литСратуровСдчСских изысканий, разнообразная ΠΈ ΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Π°Ρ эдиционная история – всС это составляСт основу исслСдования. Π˜Π½Ρ‚Π΅Ρ€Π΅Ρ соврСмСнного литСратуровСдСния ΠΊ Ρ€Π΅Ρ†Π΅ΠΏΡ‚ΠΈΠ²Π½ΠΎΠΉ эстСтикС, Π΄ΠΈΠ°Π»ΠΎΠ³Ρƒ ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€, компаративистикС ΠΈ ΠΈΠΌΠ°Π³ΠΎΠ»ΠΎΠ³ΠΈΠΈ обусловливаСт Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ ΡΡ‚Π°Ρ‚ΡŒΠΈ. ВосприятиС поэта ΠΎΡ‚Ρ€Π°ΠΆΠ°Π΅Ρ‚ Ρ€Π°Π·Π²ΠΈΡ‚ΠΈΠ΅ русско-Π½Π΅ΠΌΠ΅Ρ†ΠΊΠΈΡ… Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Ρ… связСй Π² Π₯Π₯–Π₯Π₯I Π²Π². Π’ истории пСрСводчСского восприятия поэзии ЕсСнина Π² Π“Π΅Ρ€ΠΌΠ°Π½ΠΈΠΈ выдСляСтся Ρ‚Ρ€ΠΈ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄Π°: знакомство (1920-Π΅ Π³Π³.), популяризация творчСства (1950–1980-Π΅ Π³Π³.), ΠΏΡ€ΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΠ΅ читатСля ΠΊ пониманию Π°ΡƒΡ‚Π΅Π½Ρ‚ΠΈΡ‡Π½Ρ‹Ρ… ΠΊΠΎΠ½Ρ†Π΅ΠΏΡ‚ΠΎΠ² поэтичСской сСмантики ΠΈ стиховой Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ ЕсСнина, ΠΊ Π±ΠΎΠ»Π΅Π΅ ΠΏΠΎΠ΄Ρ€ΠΎΠ±Π½ΠΎΠΌΡƒ знакомству с Π΅Π³ΠΎ ТизнСтворчСством (соврСмСнный ΠΏΠ΅Ρ€ΠΈΠΎΠ΄). Π‘ΠΏΠ΅Ρ†ΠΈΡ„ΠΈΠΊΠ° эдиционной истории Π²ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΌ опрСдСляСтся Π΄Π°Π½Π½ΠΎΠΉ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄ΠΈΠ·Π°Ρ†ΠΈΠ΅ΠΉ, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Π½ΠΎ-историчСским Ρ„Π°ΠΊΡ‚ΠΎΠΌ раздСлСния Π“Π΅Ρ€ΠΌΠ°Π½ΠΈΠΈ. НСмСцкоязычноС СсСниновСдСниС характСризуСтся большим ΠΎΡ…Π²Π°Ρ‚ΠΎΠΌ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°, Ρ€Π°Π·Π½ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠ΅ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΡΠΊΠΈΡ… ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² ΠΈ Π·Π½Π°ΠΊΠΎΠ²ΠΎΡΡ‚ΡŒΡŽ ΠΈΠΌΠ΅Π½ ΠΈΡ… Π°Π²Ρ‚ΠΎΡ€ΠΎΠ² (Π”. ЧиТСвский, Π”. Π“Π΅Ρ€Ρ…Π°Ρ€Π΄Ρ‚, Π€. ΠœΠΈΡ€Π°Ρƒ ΠΈ Π΄Ρ€.). Π Π΅Ρ†Π΅ΠΏΡ‚ΠΈΠ²Π½Ρ‹ΠΉ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ восприятия обусловливаСт слияниС литСратуровСдчСской ΠΈ пСрСводчСской ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π²Π·Π°ΠΈΠΌΠ½ΠΎ Π΄ΠΎΠΏΠΎΠ»Π½ΡΡŽΡ‚ Π΄Ρ€ΡƒΠ³ Π΄Ρ€ΡƒΠ³Π°. ΠŸΡ€Π°Π²ΠΎΠΌΠ΅Ρ€Π½ΠΎ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°Ρ‚ΡŒ Π½Π΅ΠΌΠ΅Ρ†ΠΊΠΎΠ΅ СсСниновСдСниС Π² качСствС ΡΠ°ΠΌΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π²Π΅Ρ‚Π²ΠΈ ΠΌΠΈΡ€ΠΎΠ²ΠΎΠ³ΠΎ литСратуровСдСния. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Ρ€Π°Π±ΠΎΡ‚Ρ‹ Π½Π΅ΠΌΠ΅Ρ†ΠΊΠΈΡ… ΡƒΡ‡Π΅Π½Ρ‹Ρ… ΠΈΠΌΠ΅ΡŽΡ‚ высокоС Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ для истории русской Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹. Π˜Ρ‚ΠΎΠ³ΠΎΠ²Ρ‹ΠΌ этапом Π² ΠΌΠΎΠ΄Π΅Π»ΠΈ восприятия становится творчСскоС усвоСниС ΠΎΠ±Ρ€Π°Π·Π° поэта Π² Ρ€Π°ΠΌΠΊΠ°Ρ… Ρ€ΠΎΠ΄Π½ΠΎΠΉ словСсности. Π‘ΠΎΠ·Π΄Π°Π½Π½Ρ‹Π΅ Π² 1990-Ρ… Π³Π³. стихотворСния-посвящСния ЕсСнину Π“. ВСспСра ΠΈ Π₯. ЧСховски ΠΎΡ‚Ρ€Π°ΠΆΠ°ΡŽΡ‚ творчСский Π΄ΠΈΠ°Π»ΠΎΠ³ соврСмСнных Π½Π΅ΠΌΠ΅Ρ†ΠΊΠΈΡ… Π°Π²Ρ‚ΠΎΡ€ΠΎΠ² с русским поэтом.Π‘Ρ‚Π°Ρ‚ΡŒΡ ΠΏΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π° ΠΏΡ€ΠΈ ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΊΠ΅ Π³Ρ€Π°Π½Ρ‚Π° ΠŸΡ€Π΅Π·ΠΈΠ΄Π΅Π½Ρ‚Π° Π Π€ для ΠΌΠΎΠ»ΠΎΠ΄Ρ‹Ρ… российских ΡƒΡ‡Π΅Π½Ρ‹Ρ… – Π΄ΠΎΠΊΡ‚ΠΎΡ€ΠΎΠ² Π½Π°ΡƒΠΊ (ΠΏΡ€ΠΎΠ΅ΠΊΡ‚ β„– ΠœΠ”-4756.2016.6)

    Integrated optical ADC

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    Thesis (S.M.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2008.Includes bibliographical references (p. [133]-137).An optically-sampled frequency-demultiplexed wideband analog-to-digital converter (ADC) which has potential to exceed the performance of electronic ADCs by orders of magnitude is studied analytically and numerically. The accuracy of the ADC as a function of its parameters is analyzed and impact of various imperfections of ADC components on its operation is evaluated. A universal error compensation algorithm for improving the conversion accuracy is proposed. On the way to implementation of the integrated optical ADC, two of its critical components - ring resonator filter bank and fiber-to-chip coupler -are designed. A novel coupler from a standard single mode fiber to a strongly confining silicon waveguide is proposed. The results of characterization of the filter bank and fiber-to-chip coupler fabricated on the silicon-on-insulator platform are presented and analyzed.by Anatol Khilo.S.M

    Integrated photonic analog-to-digital converters

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    Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2011.Cataloged from PDF version of thesis.Includes bibliographical references (p. 161-172).Accurate conversion of wideband multi-GHz analog signals into the digital domain has long been a target of analog-to-digital converter (ADC) developers, driven by applications in radar systems, software radio, medical imaging, and communication systems. Aperture jitter has been a major bottleneck on the way towards higher speeds and better accuracy. Photonic ADCs, which perform sampling using ultra-stable optical pulse trains generated by mode-locked lasers, have been investigated as a promising approach to overcome the jitter problem and bring ADC performance to new levels. This work demonstrates that the photonic approach can deliver on its promise by digitizing a 41 GHz signal with 7.0 effective bits and 52 dBc spur-free dynamic range (SFDR) using a discrete-component photonic ADC. This corresponds to 15 fs jitter, a 4-5 times improvement over the jitter of the best electronic ADCs, and an order of magnitude improvement over the jitter of electronic ADCs operating above 10 GHz. The feasibility of a practical photonic ADC is demonstrated by creating an integrated ADC with a modulator, filters, and photodetectors fabricated on a single silicon chip and using it to sample a 10 GHz signal with 3.5 effective bits and 39 dBc SFDR. In both experiments, a sample rate of 2.1 GSa/s was obtained by interleaving two 1.05 GSa/s channels; higher sample rates can be achieved by increasing the channel count. A key component of a multi-channel ADC - a dual multi-channel high-performance filter bank - is successfully implemented. A concept for broadband linearization of the silicon modulator, which is another critical component of the photonic ADC, is proposed. Nonlinear phenomena in silicon microring filters and their impact on ADC performance are analyzed, and methods to reduce this impact are proposed. The results presented in the thesis suggest that a practical integrated photonic ADC, which successfully overcomes the electronic jitter bottleneck, is possible today.by Anatol Khilo.Ph.D

    ΠœΠžΠ”Π˜Π€Π˜Π¦Π˜Π ΠžΠ’ΠΠΠΠΠ― Π‘Π₯Π•ΠœΠ ОВВО Π’ΠžΠ—Π‘Π£Π–Π”Π•ΠΠ˜Π― ΠŸΠžΠ’Π•Π Π₯НОБВНЫΠ₯ ΠŸΠ›ΠΠ—ΠœΠžΠΠžΠ’

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    А new type of resonant excitation of surface plasmons is proposed and investigated which is characterized by the equalityΒ of the phase velocities and attenuation coefficients of the plasmons and an excitation field. It has been shown that this type ofΒ resonance can be realized by means of the modified Otto scheme. The peculiarity of this scheme is the presence in a transitionΒ layer of the periodic system of wedges allowing one to form an inclined evanescent wave. The calculation shows that theΒ modified scheme can provide a local power gain of two orders greater as compared with the standard Otto scheme.ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΈ исслСдован Π½ΠΎΠ²Ρ‹ΠΉ Ρ‚ΠΈΠΏ рСзонансного возбуТдСния повСрхностных ΠΏΠ»Π°Π·ΠΌΠΎΠ½ΠΎΠ², ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ характСризуСтся равСнством Ρ„Π°Π·ΠΎΠ²Ρ‹Ρ… скоростСй ΠΈ коэффициСнтов затухания ΠΏΠ»Π°Π·ΠΌΠΎΠ½ΠΎΠ² ΠΈ Π²ΠΎΠ·Π±ΡƒΠΆΠ΄Π°ΡŽΡ‰Π΅Π³ΠΎ поля. Показано, Ρ‡Ρ‚ΠΎΒ Ρ‚Π°ΠΊΠΎΠΉ рСзонанс ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½ Π² ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ схСмС ΠžΡ‚Ρ‚ΠΎ, ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒΡŽ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ являСтся Π½Π°Π»ΠΈΡ‡ΠΈΠ΅Β Π² ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π½ΠΎΠΌ слоС пСриодичСской систСмы клиньСв, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰Π΅ΠΉ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ Π½Π°ΠΊΠ»ΠΎΠ½Π½ΡƒΡŽ ΡΠ²Π°Π½Π΅ΡΡ†Π΅Π½Ρ‚Π½ΡƒΡŽ Π²ΠΎΠ»Π½Ρƒ. РасчСт схСмы ΠΏΠΎΠΊΠ°Π·Π°Π», Ρ‡Ρ‚ΠΎ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ усилСния Π² рассматриваСмой схСмС Π² сравнСнии со стандартной схСмой ΠžΡ‚Ρ‚ΠΎΒ ΠΌΠΎΠΆΠ΅Ρ‚ Π΄ΠΎΡΡ‚ΠΈΠ³Π°Ρ‚ΡŒ Π΄Π²ΡƒΡ… порядков ΠΈ Π²Ρ‹ΡˆΠ΅

    Silicon slow-light-based photonic mixer for microwave-frequencyconversion applications

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    This paper was published in OPTICS LETTERS and is made available as an electronic reprint with the permission of OSA. The paper can be found at the following URL on the OSA website: http://dx.doi.org/10.1364/OL.37.001721. Systematic or multiple reproduction or distribution to multiple locations via electronic or other means is prohibited and is subject to penalties under law[EN] We describe and demonstrate experimentally a method for photonic mixing of microwave signals by using a silicon electro-optical MachΒΏZehnder modulator enhanced via slow-light propagation. Slow light with a group index of ~11, achieved in a one-dimensional periodic structure, is exploited to improve the upconversion performance of an input frequency signal from 1 to 10.25 GHz. A minimum transmission point is used to successfully demonstrate the upconversion with very low conversion losses of ~7ΒΏΒΏdB and excellent quality of the received I/Q modulated QPSK signal with an optimum EVM of ~8%.Financial support from FP7-224312 HELIOS project and Generalitat Valenciana under PROMETEO-2010-087 R&D Excellency Program (NANOMET) are acknowledged. F. Y.Gardes, D. J. Thomson, and G. T. Reed are supported by funding received from the UK EPSRC funding body under the grant β€œUK Silicon Photonics.” The author A. M. GutiΓ©rrez thanks D. Marpaung for his useful help.GutiΓ©rrez Campo, AM.; Brimont, ACJ.; Herrera Llorente, J.; Aamer, M.; MartΓ­ Sendra, J.; Thomson, DJ.; Gardes, FY.... (2012). Silicon slow-light-based photonic mixer for microwave-frequencyconversion applications. Optics Letters. 37(10):1721-1723. https://doi.org/10.1364/OL.37.001721S17211723371

    Sub-decibel efficiency, bi-layer, O-band fiber-to-chip grating coupler demonstrated in a 45 nm CMOS foundry platform

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    We demonstrate a grating coupler with 0.85 dB fiber-to-chip coupling loss in the O-band (1,300 nm), implemented in a 45 nm CMOS foundry platform.Accepted manuscrip

    ΠΠ˜Π—ΠšΠžΠ§ΠΠ‘Π’ΠžΠ’ΠΠžΠ• ΠžΠ‘Π ΠΠ’ΠΠžΠ• ΠΠšΠ£Π‘Π’ΠžΠžΠŸΠ’Π˜Π§Π•Π‘ΠšΠžΠ• Π ΠΠ‘Π‘Π•Π―ΠΠ˜Π• Π‘Π•Π‘Π‘Π•Π›Π•Π’Π«Π₯ Π‘Π’Π•Π’ΠžΠ’Π«Π₯ ΠŸΠ£Π§ΠšΠžΠ’

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    The features of acousto-optic diffraction of a Bessel light beam (BLB) on a Bessel acoustic beam (BAB) in transversely anisotropic crystals are investigated. The scheme of acousto-optic (AO) interaction is considered when the incident TH-polarized BLB propagating along the optical c axis of an optically uniaxial crystal is excited in the crystal of the TE- po-la rized BLB due to the process of anisotropic THβ†’TE diffraction. The diffraction problem is solved for transversely isotropic crystals, whose cylindrical symmetry is fully consistent with the symmetry of both BLB and BAB propagating along the optical axis and the AO interaction occurs without distortion of the spatial structure of beams. It is shown that in the process of backward acousto-optic scattering, the use of Bessel light beams with a large cone angle makes it possible to significantly reduce the frequency of the acoustic wave necessary for satisfying the longitudinal synchronism condition (values of less than 1 GHz). It is established that the efficiency of the AO interaction of the BLB and the BAB is determined not only by the intensity of the acoustic field, longitudinal wave detuning and the interaction length, but also by the period of transverse oscillations of Bessel beams. These oscillations determine the value of the overlap integrals and, consequently, the effective AO parameters. When the conditions of longitudinal and transverse synchronisms are realized, it is possible to achieve the high diffraction efficiency close to unity. The angular width of transverse synchronism is equal to about 0.5 mrad and increases with increasing acoustic power. It is shown that when the BLB is diffracted, the order of its phase dislocation changes by a value that is equal to the order of BAB phase dislocation. Because of the narrow angular spectrum of a scattered field, the back ward AO diffraction of Bessel light beams is promising for the development of low-frequency AO filters and spectrum analyzers. The property of self-reconstruction of the transverse profile of an optical field is promising for applications of Bessel light beams in defectroscopy.Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ особСнности акустооптичСской Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ бСссСлСва свСтового ΠΏΡƒΡ‡ΠΊΠ° (Π‘Π‘ΠŸ) Π½Π° бСссСлСвом акустичСском ΠΏΡƒΡ‡ΠΊΠ΅ (Π‘ΠΠŸ) Π² ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… кристаллах. РассмотрСна схСма акустооптичСского (АО) взаимодСйствия, ΠΊΠΎΠ³Π΄Π° ВН-поляризованный (ΠΈΠ»ΠΈ Π΅-поляризованный) Π‘Π‘ΠŸ ΠΏΠ°Π΄Π°Π΅Ρ‚ Π½Π° оптичСски одноосный кристалл Π² Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ оптичСской оси с ΠΈ Π·Π° счСт Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠΉ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ ВН→ВЕ ΠΏΠ°Π΄Π°ΡŽΡ‰ΠΈΠΉ Π΅-Π‘Π‘ΠŸ Π²ΠΎΠ·Π±ΡƒΠΆΠ΄Π°Π΅Ρ‚ Π² кристаллС рассСянный ΠΎ-Π‘Π‘ΠŸ. Π—Π°Π΄Π°Ρ‡Π° АО Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ Ρ€Π΅ΡˆΠ°Π΅Ρ‚ΡΡ для ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… кристаллов, цилиндричСски симмСтричная гСомСтрия ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… ΠΏΠΎΠ»Π½ΠΎΡΡ‚ΡŒΡŽ согласована ΠΏΠΎ симмСтрии с Π‘Π‘ΠŸ ΠΈ Π‘ΠΠŸ, Ρ€Π°ΡΠΏΡ€ΠΎΡΡ‚Ρ€Π°Π½ΡΡŽΡ‰ΠΈΡ…ΡΡ вдоль оптичСской оси, ΠΈ процСсс АО взаимодСйствия происходит Π±Π΅Π· искаТСния пространствСнной структуры ΠΏΡƒΡ‡ΠΊΠΎΠ². Показано, Ρ‡Ρ‚ΠΎ Π² процСссС ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠ³ΠΎ акустооптичСского рассСяния использованиС бСссСлСвых свСтовых ΠΏΡƒΡ‡ΠΊΠΎΠ² с большим ΡƒΠ³Π»ΠΎΠΌ конуса позволяСт Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΡƒΠΌΠ΅Π½ΡŒΡˆΠΈΡ‚ΡŒ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΡƒΡŽ для выполнСния условия ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ синхронизма частоту акустичСской Π²ΠΎΠ»Π½Ρ‹ (Π΄ΠΎ Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ ΠΌΠ΅Π½Π΅Π΅ 1 Π“Π“Ρ†). УстановлСно, Ρ‡Ρ‚ΠΎ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ АО взаимодСйствия Π‘Π‘ΠŸ ΠΈ Π‘ΠΠŸ опрСдСляСтся Π½Π΅ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ ΠΈΠ½Ρ‚Π΅Π½ΡΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ акустичСского поля, ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠΉ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ расстройкой ΠΈ Π΄Π»ΠΈΠ½ΠΎΠΉ взаимодСйствия, ΠΊΠ°ΠΊ Π² случаС плоских Π²ΠΎΠ»Π½, Π½ΠΎ ΠΈ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠΉ структурой бСссСлСвых ΠΏΡƒΡ‡ΠΊΠΎΠ². Π­Ρ‚Π° структура опрСдСляСт Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρƒ ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΠΎΠ² пСрСкрытия ΠΈ, ΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎ, эффСктивныС АО ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹. ΠŸΡ€ΠΈ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΈΠΈ условий ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ ΠΈ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠ³ΠΎ синхронизмов Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ достиТСниС высокой эффСктивности Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ, Π±Π»ΠΈΠ·ΠΊΠΎΠΉ ΠΊ Π΅Π΄ΠΈΠ½ΠΈΡ†Π΅, Π° угловая ΡˆΠΈΡ€ΠΈΠ½Π° основного максимума составляСт ΠΏΡ€ΠΈ этом Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρƒ ~0,5 ΠΌΡ€Π°Π΄ ΠΈ возрастаСт ΠΏΡ€ΠΈ ΡƒΠ²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠΈ акустичСской мощности. УстановлСно, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ Π‘Π‘ΠŸ происходит трансформация порядка Π΅Π³ΠΎ Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ дислокации Π½Π° Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρƒ, Ρ€Π°Π²Π½ΡƒΡŽ порядку Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ дислокации Π‘ΠΠŸ. Из-Π·Π° ΠΌΠ°Π»ΠΎΠΉ ΡˆΠΈΡ€ΠΈΠ½Ρ‹ ΡƒΠ³Π»ΠΎΠ²ΠΎΠ³ΠΎ спСктра рассСянного Π‘Π‘ΠŸ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠ΅ акустооптичСскоС рассСяниС бСссСлСвых свСтовых ΠΏΡƒΡ‡ΠΊΠΎΠ² пСрспСктивно для Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ низкочастотных акустооптичСских Ρ„ΠΈΠ»ΡŒΡ‚Ρ€ΠΎΠ² ΠΈ спСктроанализаторов, Π° свойство саморСконструкции ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎΠΉ структуры пСрспСктивно для ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΉ бСссСлСвых ΠΏΡƒΡ‡ΠΊΠΎΠ² Π² дСфСктоскопии.Β 

    ΠžΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΠΈ акустооптичСского взаимодСйствия оптичСских ΠΈ акустичСских бСссСлСвых ΠΏΡƒΡ‡ΠΊΠΎΠ² Π² ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… оптичСски ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… кристаллах

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    Some basic properties of acousto-optical (AO) diffraction involving Bessel light and acoustic beams in anisotropic crystals are investigated. Hexagonal symmetry crystals are considered and are optically uniaxial and positive and acoustically transversely isotropic. It is shown that, unlike the case of AO diffraction of plane waves, the transition to Bessel beams allows one to realize a number of new diffraction channels having specific configurations of the wave vectors of interacting waves while maintaining the axial symmetry of the optical scheme as a whole. The diffraction channels for anisotropic scattering are classified and the main parameters of the scattered Bessel light beam and the parameters of the Bessel acoustic beam are calculated for each of them. The possibility of implementing the isotropic-type diffraction was revealed, which makes it possible to increase the efficiency of AO conversion. The parameters of this-type diffraction are determined for two scattering channels, namely, for scattering by a direct Bessel acoustic beam and by a backward propagating acoustic beam.Due to the appearance of a set of scattering channels and with regard to the fact that Bessel light and acoustic beams have helical wave front dislocations, as well as suppressed diffraction spreading, the study of the features of AO diffraction of such beams in optically positive crystals has both a scientific and practical interest.Β Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ особСнности акустооптичСской (АО) Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ с участиСм бСссСлСвых свСтового ΠΈ акустичСского ΠΏΡƒΡ‡ΠΊΠΎΠ² Π² Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹Ρ… кристаллах. РассмотрСны кристаллы гСксагональной симмСтрии, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΡΠ²Π»ΡΡŽΡ‚ΡΡ оптичСски ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌΠΈ, Π° акустичСски – ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½ΠΎ ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½Ρ‹ΠΌΠΈ. Показано, Ρ‡Ρ‚ΠΎ Π² ΠΎΡ‚Π»ΠΈΡ‡ΠΈΠ΅ ΠΎΡ‚ случая АО Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ плоских Π²ΠΎΠ»Π½, ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄ ΠΊ бСссСлСвым ΠΏΡƒΡ‡ΠΊΠ°ΠΌ позволяСт Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Ρ‚ΡŒ ряд Π½ΠΎΠ²Ρ‹Ρ… ΠΊΠ°Π½Π°Π»ΠΎΠ² Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ, ΠΈΠΌΠ΅ΡŽΡ‰ΠΈΡ… спСцифичСскиС ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ Π²ΠΎΠ»Π½ΠΎΠ²Ρ‹Ρ… Π²Π΅ΠΊΡ‚ΠΎΡ€ΠΎΠ² Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… Π²ΠΎΠ»Π½ ΠΏΡ€ΠΈ сохранСнии аксиальной симмСтрии оптичСской схСмы Π² Ρ†Π΅Π»ΠΎΠΌ. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° классификация ΠΊΠ°Π½Π°Π»ΠΎΠ² Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ для Π°Π½ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠ³ΠΎ рассСяния ΠΈ для Π½ΠΈΡ… рассчитаны основныС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ рассСянного бСссСлСва свСтового ΠΏΡƒΡ‡ΠΊΠ° ΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ бСссСлСва акустичСского ΠΏΡƒΡ‡ΠΊΠ°. ΠžΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΈΠ·ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ° Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ, Ρ‡Ρ‚ΠΎ позволяСт ΠΏΠΎΠ²Ρ‹ΡΠΈΡ‚ΡŒ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ АО прСобразования. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ Π΅Π³ΠΎ характСристики для Π΄Π²ΡƒΡ… ΠΊΠ°Π½Π°Π»ΠΎΠ² рассСяния, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ, рассСяния Π½Π° ΠΏΠΎΠΏΡƒΡ‚Π½ΠΎΠΌ бСссСлСвом акустичСском ΠΏΡƒΡ‡ΠΊΠ΅ ΠΈ Π½Π° ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΌ.Из-Π·Π° многообразия ΠΊΠ°Π½Π°Π»ΠΎΠ² рассСяния, Π° Ρ‚Π°ΠΊΠΆΠ΅ с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ Ρ‚ΠΎΠ³ΠΎ, Ρ‡Ρ‚ΠΎ бСссСлСвы свСтовой ΠΈ акустичСский ΠΏΡƒΡ‡ΠΊΠΈ ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ Π²ΠΈΠ½Ρ‚ΠΎΠ²Ρ‹ΠΌΠΈ дислокациями Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ Ρ„Ρ€ΠΎΠ½Ρ‚Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½Π½Ρ‹ΠΌ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹ΠΌ расплываниСм, ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ особСнностСй АО Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ Ρ‚Π°ΠΊΠΈΡ… ΠΏΡƒΡ‡ΠΊΠΎΠ² Π² оптичСски ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… кристаллах прСдставляСт ΠΊΠ°ΠΊ Π½Π°ΡƒΡ‡Π½Ρ‹ΠΉ, Ρ‚Π°ΠΊ ΠΈ практичСский интСрСс.
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