15 research outputs found

    ΠžΡ†Π΅Π½ΠΊΠ° ΠΏΠΎΡ‚Π΅Ρ€ΡŒ Π² оптичСских ΠΏΠ»Ρ‘Π½ΠΎΡ‡Π½Ρ‹Ρ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°Ρ… с ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚Ρ‹ΠΌΠΈ Π³Ρ€Π°Π½ΠΈΡ†Π°ΠΌΠΈ ΠΈ ΠΏΠΎΠ³Π»ΠΎΡ‰Π΅Π½ΠΈΠ΅ΠΌ

    Get PDF
    The method of small indignations with use of the optics-geometrical approach solves a problem of light propagation in a film waveguide with rough surfaces and absorption. Experimental researches specified waveguide structures are carried out. Results of these researches substantially do not correspond to conclusions of the developed theory. As a result of the analysis of the revealed discrepancies and additional calculations more exact model of scattering process in film waveguides with rough surfaces is offered.ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΌΠ°Π»Ρ‹Ρ… Π²ΠΎΠ·ΠΌΡƒΡ‰Π΅Π½ΠΈΠΉ с использованиСм ΠΎΠΏΡ‚ΠΈΠΊΠΎ-гСомСтричСского ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° Ρ€Π΅ΡˆΠ΅Π½Π° Π·Π°Π΄Π°Ρ‡Π° ΠΎ распространСнии свСта Π² ΠΏΠ»Ρ‘Π½ΠΎΡ‡Π½ΠΎΠΌ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π΅ с ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚Ρ‹ΠΌΠΈ Π³Ρ€Π°Π½ΠΈΡ†Π°ΠΌΠΈ ΠΈ ΠΏΠΎΠ³Π»ΠΎΡ‰Π΅Π½ΠΈΠ΅ΠΌ. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ исслСдования ΡƒΠΊΠ°Π·Π°Π½Π½Ρ‹Ρ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½Ρ‹Ρ… структур. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ этих исслСдований нСсколько расходятся с Π²Ρ‹Π²ΠΎΠ΄Π°ΠΌΠΈ Ρ€Π°Π·Π²ΠΈΡ‚ΠΎΠΉ Ρ‚Π΅ΠΎΡ€ΠΈΠΈ. Π’ ΠΈΡ‚ΠΎΠ³Π΅ Π°Π½Π°Π»ΠΈΠ·Π° выявлСнных нСсоотвСтствий ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° Π±ΠΎΠ»Π΅Π΅ точная модСль процСсса рассСяния Π² ΠΏΠ»Ρ‘Π½ΠΎΡ‡Π½Ρ‹Ρ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°Ρ… с ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚Ρ‹ΠΌΠΈ Π³Ρ€Π°Π½ΠΈΡ†Π°ΠΌΠΈ

    Расчётный ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· характСристик Π°Π½Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€Π° спСктра ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚ΠΎΡΡ‚ΠΈ повСрхности

    Get PDF
    The analysis of characteristics of surface roughness spectrum analyzer prototype whichuses a waveguide light scattering is performed. Calculated characteristics and layout optionsare compared with measurements. The experimental spectrum of the surface roughness ofthe gradient waveguide is presented.Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ Π°Π½Π°Π»ΠΈΠ· характСристик ΠΌΠ°ΠΊΠ΅Ρ‚Π° Π°Π½Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€Π° спСктра ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚ΠΎΡΡ‚ΠΈ повСрхности, Π² ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½ΠΎΠ΅ рассСяниС свСта. РасчётныС характСристики ΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ ΠΌΠ°ΠΊΠ΅Ρ‚Π° ΡΠΎΠΏΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‚ΡΡ с ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½Π½Ρ‹ΠΌΠΈ. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΉ спСктр ΡˆΠ΅Ρ€ΠΎΡ…ΠΎΠ²Π°Ρ‚ΠΎΡΡ‚ΠΈ повСрхности Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π°

    Π˜Π·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ свойства Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚Π½Ρ‹Ρ… Π³ΠΎΡ„Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄ΠΎΠ² с мСталличСским ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹ΠΌ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ

    No full text
    The numerical method has been employed to solve the problem of the TE-polarized light radiation from a corrugated graded-index waveguide with metal or semiconductor cladding for structures with and without a buffer layer. An analysis has been carried out of the basic radiational properties of these systems. The optimal corrugation depth has been found for metal-dielectric structures at which the radiated power reaches maximum. It is shown that the proper choice of parameters of the structure with the buffei layer and the high reflectivity of the metal cladding make it possible to emit practically the whole power of the waveguide wave in the prescribed direction. An Al-cladded structure with the buffer layer has been studied experimentally.ЧислСнным ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Ρ€Π΅ΡˆΠ΅Π½Π° Π·Π°Π΄Π°Ρ‡Π° ΠΎΠ± ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠΈ свСта Π’Π•-поляризации ΠΈΠ· Π³ΠΎΡ„Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° с мСталличСским ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹ΠΌ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΏΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ Π±ΡƒΡ„Π΅Ρ€Π½ΠΎΠ³ΠΎ слоя ΠΈ Π±Π΅Π· Π½Π΅Π³ΠΎ. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ Π°Π½Π°Π»ΠΈΠ· основных ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… характСристик этих систСм. Для мСталлодиэлСктричСских структур установлСна ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Π°Ρ Π³Π»ΡƒΠ±ΠΈΠ½Π° Π³ΠΎΡ„Ρ€Π°, ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ излучаСмая ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ максимальна. Показано, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ ΠΏΡ€Π°Π²ΠΈΠ»ΡŒΠ½ΠΎΠΌ Π²Ρ‹Π±ΠΎΡ€Π΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² структуры с Π±ΡƒΡ„Π΅Ρ€Π½Ρ‹ΠΌ слоСм ΠΈ высокой ΠΎΡ‚Ρ€Π°ΠΆΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ способности мСталличСского покрытия ΠΌΠΎΠΆΠ½ΠΎ ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚ΡŒ практичСски всю ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ‹ Π² Π·Π°Π΄Π°Π½Π½ΠΎΠΌ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ исслСдована структура с Π±ΡƒΡ„Π΅Ρ€Π½Ρ‹ΠΌ слоСм ΠΈ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΈΠ· Аl

    The waveguide method for measuring parameters of the surface layers

    No full text
    A new method has been applied for determining the mean square deviation of surface roughness and the imaginary part of permittivity of the material near-surface region. The method is based on the scattering and absorption of light in waveguide systems of integrated optics. It has high sensitivity and ease of implementation. The advantages of the proposed method are confirmed experimentally. Β© 2012 EDP Sciences

    CHARACTERISTICS OF PHASE DIFFRACTION LATTICES, OBTAINED BY AN IONIC EXCHANGE METHOD

    No full text

    Effects of surface roughness and absorption on light propagation in graded-profile waveguides

    No full text
    This paper examines the effects of surface roughness and absorption on laser light propagation in graded-profile waveguiding structures. We derive analytical expressions for the scattering and absorption coefficients of guided waves and analyse these coefficients in relation to parameters of the waveguiding structure and the roughness of its boundary. A new approach is proposed to measuring roughness parameters of precision dielectric surfaces. Experi- mental evidence is presented which supports the main conclusions of the theory. Β© 2011 Kvantovaya Elektronika and Turpion Ltd

    EXPERIMENTAL REALIZATION OF INTEGRAL TUNNEL DEVICE FOR EXCITATION OF THE BAND WAVE-GUIDE

    No full text

    EXPERIMENTAL REALIZATION OF INTEGRAL TUNNEL DEVICE FOR EXCITATION OF THE BAND WAVE-GUIDE

    No full text

    CHARACTERISTICS OF PHASE DIFFRACTION LATTICES, OBTAINED BY AN IONIC EXCHANGE METHOD

    No full text

    Π˜Π·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ свойства Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚Π½Ρ‹Ρ… Π³ΠΎΡ„Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄ΠΎΠ² с мСталличСским ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹ΠΌ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ

    No full text
    The numerical method has been employed to solve the problem of the TE-polarized light radiation from a corrugated graded-index waveguide with metal or semiconductor cladding for structures with and without a buffer layer. An analysis has been carried out of the basic radiational properties of these systems. The optimal corrugation depth has been found for metal-dielectric structures at which the radiated power reaches maximum. It is shown that the proper choice of parameters of the structure with the buffei layer and the high reflectivity of the metal cladding make it possible to emit practically the whole power of the waveguide wave in the prescribed direction. An Al-cladded structure with the buffer layer has been studied experimentally.ЧислСнным ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Ρ€Π΅ΡˆΠ΅Π½Π° Π·Π°Π΄Π°Ρ‡Π° ΠΎΠ± ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠΈ свСта Π’Π•-поляризации ΠΈΠ· Π³ΠΎΡ„Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ Π³Ρ€Π°Π΄ΠΈΠ΅Π½Ρ‚Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π° с мСталличСским ΠΈΠ»ΠΈ ΠΏΠΎΠ»ΡƒΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠΎΠ²Ρ‹ΠΌ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΏΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ Π±ΡƒΡ„Π΅Ρ€Π½ΠΎΠ³ΠΎ слоя ΠΈ Π±Π΅Π· Π½Π΅Π³ΠΎ. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ Π°Π½Π°Π»ΠΈΠ· основных ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… характСристик этих систСм. Для мСталлодиэлСктричСских структур установлСна ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Π°Ρ Π³Π»ΡƒΠ±ΠΈΠ½Π° Π³ΠΎΡ„Ρ€Π°, ΠΏΡ€ΠΈ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ излучаСмая ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ максимальна. Показано, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ ΠΏΡ€Π°Π²ΠΈΠ»ΡŒΠ½ΠΎΠΌ Π²Ρ‹Π±ΠΎΡ€Π΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² структуры с Π±ΡƒΡ„Π΅Ρ€Π½Ρ‹ΠΌ слоСм ΠΈ высокой ΠΎΡ‚Ρ€Π°ΠΆΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ способности мСталличСского покрытия ΠΌΠΎΠΆΠ½ΠΎ ΠΈΠ·Π»ΡƒΡ‡Π°Ρ‚ΡŒ практичСски всю ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ‹ Π² Π·Π°Π΄Π°Π½Π½ΠΎΠΌ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ исслСдована структура с Π±ΡƒΡ„Π΅Ρ€Π½Ρ‹ΠΌ слоСм ΠΈ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠ΅ΠΌ ΠΈΠ· Аl
    corecore