23 research outputs found

    ВСорСтичСский Π°Π½Π°Π»ΠΈΠ· Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ гауссова ΠΏΡƒΡ‡ΠΊΠ° Π½Π° ступСнчатой Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ структурС (Π‘Π€Π‘)

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    The paper analyzes the interaction of a Gaussian beam with a phase step structure (PSS). The shape of the spatial spectrum at the output of such a scheme is examined. The most detailed description was done for the case when the size of the PSS phase difference is 180 degrees. The effects that occur at the displacement of SPS in the plane perpendicular to the direction of incidence of the laser beam were considered. Discussions for the possible practical application of the scheme were carried out.Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ ΠΏΡ€ΠΎΠ²Π΅Π΄Ρ‘Π½ Π°Π½Π°Π»ΠΈΠ· взаимодСйствия гауссова ΠΏΡƒΡ‡ΠΊΠ° со ступСнчатой Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ структурой (Π‘Π€Π‘). ИсслСдована Ρ„ΠΎΡ€ΠΌΠ° пространствСнного спСктра Π½Π° Π²Ρ‹Ρ…ΠΎΠ΄Π΅ Ρ‚Π°ΠΊΠΎΠΉ схСмы. НаиболСС Π΄Π΅Ρ‚Π°Π»ΡŒΠ½ΠΎ описан частный случай, ΠΊΠΎΠ³Π΄Π° Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π° Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΠΏΠ΅Ρ€Π΅ΠΏΠ°Π΄Π° Π‘Π€Π‘ составляСт 180 градусов. Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ эффСкты, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΈΠΌΠ΅ΡŽΡ‚ мСсто ΠΏΡ€ΠΈ смСщСнии Π‘Π€Π‘ Π² плоскости, пСрпСндикулярной Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΡŽ падСния Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ излучСния. ΠžΠ±ΡΡƒΠΆΠ΄Π°ΡŽΡ‚ΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹Π΅ практичСскиС примСнСния схСмы

    ИсслСдованиС оптоэлСктронного Π΄Π°Ρ‚Ρ‡ΠΈΠΊΠ° ΡƒΠ³Π»ΠΎΠ²Ρ‹Ρ… смСщСний Π½Π° основС Π³Π»ΡƒΠ±ΠΎΠΊΠΎΠΉ ΠΎΡ‚Ρ€Π°ΠΆΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠΉ Ρ€Π΅ΡˆΡ‘Ρ‚ΠΊΠΈ

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    An optoelectronic device for measurements of small angular displacements based on a diffraction of a laser beam on a deep reflective phasetype grating was suggested and investigated. The grating's depth is about several wavelengths. The zero diffraction order's power dependency on the incident angle of a laser beam was investigated theoretically and experimentally. There were found conditions when linear conversion of angular vibrations into changes of power of zero order took place. The experimentally measured sensitivity of the device was rad with channel bandwidth of 800 Hz and signal-to-noise ratio 10.ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΈ исслСдован оптоэлСктронный Π΄Π°Ρ‚Ρ‡ΠΈΠΊ ΠΌΠ°Π»Ρ‹Ρ… ΡƒΠ³Π»ΠΎΠ²Ρ‹Ρ… ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Ρ‰Π΅Π½ΠΈΠΉ Π½Π° основС Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ Π»Π°Π·Π΅Ρ€Π½ΠΎΠ³ΠΎ ΠΏΡƒΡ‡ΠΊΠ° Π½Π° Π³Π»ΡƒΠ±ΠΎΠΊΠΎΠΉ ΠΎΡ‚Ρ€Π°ΠΆΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠΉ Ρ€Π΅ΡˆΡ‘Ρ‚ΠΊΠ΅. ΠŸΡ€ΠΎΠ²Π΅Π΄Ρ‘Π½ тСорСтичСский Π°Π½Π°Π»ΠΈΠ· ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ исслСдования характСристик Π΄Π°Ρ‚Ρ‡ΠΈΠΊΠ°

    Linear moving meters designed on the basis of laser probing of scales of a type: Surface acoustic wave (SAW) - Diffraction grating (DG)

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    A comparative analysis of moving meters schemes of an acoustic-optical type is carried out. Reference scales formed by surface acoustic waves and diffraction gratings are used in these schemes. The system SAW-DG is probed by a laser beam. The measurement of movement is effected by change of the phase of a signal at SAW frequency in the optoelectronic channel. Repeatability, resolving power, exactitude, range of measurements are analyzed. The resolving power better than 0,05 microns can be reached using SAW wave-length in a range of 30 up to 100 microns

    Linear moving meters designed on the basis of laser probing of scales of a type: Surface acoustic wave (SAW) - Diffraction grating (DG)

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    A comparative analysis of moving meters schemes of an acoustic-optical type is carried out. Reference scales formed by surface acoustic waves and diffraction gratings are used in these schemes. The system SAW-DG is probed by a laser beam. The measurement of movement is effected by change of the phase of a signal at SAW frequency in the optoelectronic channel. Repeatability, resolving power, exactitude, range of measurements are analyzed. The resolving power better than 0,05 microns can be reached using SAW wave-length in a range of 30 up to 100 microns

    Experimental investigation of laser beam diffraction on phase step and its practical applications

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    The change in shape of the spatial spectrum, which is a result of the interaction of a focused laser beam with a phase step structure (PSS), is investigated. As a laser beam passes through a PSS, a spatial spectrum of radiation in the form of two peaks with a deep gap in between is generated. The change in the peaks' structure as the PSS moves relative to the optical axis of the laser beam is studied in detail. On the basis of the experimental results, a new scheme for measuring small linear and angular deviations is proposed. Β© The Institution of Engineering and Technology 2014

    Experimental investigation of laser beam diffraction on phase step and its practical applications

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    The change in shape of the spatial spectrum, which is a result of the interaction of a focused laser beam with a phase step structure (PSS), is investigated. As a laser beam passes through a PSS, a spatial spectrum of radiation in the form of two peaks with a deep gap in between is generated. The change in the peaks' structure as the PSS moves relative to the optical axis of the laser beam is studied in detail. On the basis of the experimental results, a new scheme for measuring small linear and angular deviations is proposed. Β© The Institution of Engineering and Technology 2014

    Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ΅ исслСдованиС акустооптичСского взаимодСйствия Π² Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½ΠΎΠΌ ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€ΠΎΠΌΠ΅Ρ‚Ρ€Π΅

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    ΠŸΡ€ΠΈΠ²ΠΎΠ΄ΡΡ‚ΡΡ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ исслСдования ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‚ΠΎΡ‡Π½Ρ‹Ρ… характСристик ΠΈ эффСктивности считывания сигналов Π² устройствах Π½Π° повСрхностных акустичСских Π²ΠΎΠ»Π½Π°Ρ… с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ полоскового Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½ΠΎ-оптичСского ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€ΠΎΠΌΠ΅Ρ‚Ρ€Π°. Π­ΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΉ ΠΌΠ°ΠΊΠ΅Ρ‚ Π±Ρ‹Π» ΠΈΠ·Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½ Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ΅ ΠΈΠ· Π½ΠΈΠΎΠ±Π°Ρ‚Π° лития YZ-срСза. Он содСрТал полосковый Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ΄Π½Ρ‹ΠΉ Π΄Π²ΡƒΡ…ΠΏΠ»Π΅Ρ‡Π΅Π²ΠΎΠΉ ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€ΠΎΠΌΠ΅Ρ‚Ρ€ с элСктродами для элСктрооптичСской ΠΊΠΎΡ€Ρ€Π΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²ΠΊΠΈ Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ сдвига Ρ„Π°Π· ΠΌΠ΅ΠΆΠ΄Ρƒ оптичСскими Π²ΠΎΠ»Π½Π°ΠΌΠΈ Π² ΠΏΠ»Π΅Ρ‡Π°Ρ… ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€ΠΎΠΌΠ΅Ρ‚Ρ€Π° ΠΈ Π²ΠΎΠ·Π±ΡƒΠ΄ΠΈΡ‚Π΅Π»ΡŒ повСрхностных акустичСских Π²ΠΎΠ»Π½ встрСчно-ΡˆΡ‚Ρ‹Ρ€Π΅Π²ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ°. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΌΠΎΠ³ΡƒΡ‚ Π½Π°ΠΉΡ‚ΠΈ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΠΏΡ€ΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ схСм ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ сигналов с использованиСм ΠŸΠΠ’ ΠΈ ΠΏΡ€ΠΈ конструировании оптичСских модуляторов

    An optical setup for measuring amplitude and phase distributions of surface acoustic waves

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    The setup is intended for measuring amplitude and phase distributions of surface acoustic wave fields in a frequency range of 10-100 MHz. Optimal parameters of the setup and its elements are presented. The threshold detection amplitude of surface acoustic waves is 10-4 nm for a 1-kHz reception bandwidth. The phase channel instability does not exceed 0.2Β° during the measurement cycle. The relative difference between the velocities at the free and metal-coated surfaces is obtained from phase measurements with a test sample. The result is in good agreement with reference data. Β© 1998 MAHK Hayka/Interperiodica Publishing

    Modulator of laser radiation

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    A new mechanical modulator of laser radiation is proposed. The working principle is based on the specific diffraction of coherent radiation by a deep reflection grating with rectangular profile. The modulator can be used in various wavelength ranges. Β© 2012 Pleiades Publishing, Inc
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