14 research outputs found
Carbon nanowalls: the next step for physical manifestation of the black body coating
The optical properties of carbon nanowall (CNW) films in the visible range have been studied and reported for the first time. Depending on the film structure, ultra-low total reflectance up to 0.13% can be reached, which makes the CNW films a promising candidate for the black body-like coating, and thus for a wide range of applications as a light absorber. We have estimated important trends in the optical property variation from sample to sample, and identified the presence of edge states and domain boundaries in carbon nanowalls as well as the film mass density variation as the key factors. Also we demonstrated that at much lower film thickness and density than for a carbon nanotube forest the CNWs yield one order higher specific light absorption
Π₯ΠΠ ΠΠΠ’ΠΠ ΠΠ‘Π’ΠΠΠ ΠΠΠ’Π§ΠΠΠ ΠΠΠΠ«Π₯ Π£ΠΠΠΠΠ«Π₯ ΠΠΠ ΠΠΠΠ©ΠΠΠΠ, ΠΠΠ‘Π’Π ΠΠΠΠΠΠΠ Π‘ ΠΠ ΠΠΠΠΠΠΠΠΠ Π‘ΠΠ‘Π’ΠΠΠ« ΠΠ ΠΠΠ£Π₯ Π€ΠΠΠΠΠ«Π₯ ΠΠΠ€Π ΠΠΠ¦ΠΠΠΠΠ«Π₯ Π ΠΠ¨ΠΠ’ΠΠ
Sensors of small angular displacements and oscillations of objects constructed using a system of two phase diffraction gratings located at some distance from each other are investigated. The scheme of the sensor, and the results of experimental studies its characteristics are presented. Experimental sensitivity for recording angular vibrations was 10-5 radians.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ Π΄Π°ΡΡΠΈΠΊΠΈ ΠΌΠ°Π»ΡΡ
ΡΠ³Π»ΠΎΠ²ΡΡ
ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΠΎΡΡΡΠΎΠ΅Π½Ρ Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΡΠΈΡΡΠ΅ΠΌΡ ΠΈΠ· Π΄Π²ΡΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΡΡΠΎΠΊ (ΠΠ ). ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΡ
Π΅ΠΌΠ° Π΄Π°ΡΡΠΈΠΊΠ°, ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΡΠ°Π±ΠΎΡΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΈ ΠΎΡΠ΅Π½ΠΊΠ° ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ Π΄Π°ΡΡΠΈΠΊΠ°. ΠΠ° ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΡΠ°Ρ
Π΄Π°ΡΡΠΈΠΊΠΎΠ² ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΠΏΡΠΈ ΡΠ΅Π³ΠΈΡΡΡΠ°ΡΠΈΠΈ ΡΠ³Π»ΠΎΠ²ΡΡ
ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΡΠΎΡΡΠ°Π²ΠΈΠ»Π° 10-5 ΡΠ°Π΄ΠΈΠ°Π½
Laser beam modulation using corner reflector and deep diffraction grating
A new scheme of the power modulator of laser beam is based on a corner-reflector unit with a relief diffraction grating that is placed on a plane of the unit and has a relief depth of several wavelengths of the laser radiation. It is shown that angular oscillations of the unit make it possible to implement modulation of the zero-order diffraction beam at a modulation depth of almost 100% and a relatively high linearity of the modulation characteristic that is reached at modulation depths of greater than 50%. Β© 2017, Pleiades Publishing, Inc
Π£ΡΡΡΠΎΠΉΡΡΠ²ΠΎ Π΄Π»Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ
In this paper we consider a new type of mechanical device for periodic modulation of laser radiation. The modulating unit consists of two phase diffraction gratings with a rectangular profile, one of which moves relative to the other. The output beam of radiation in this device can be either a zero-order beam of diffraction, or one of the first orders of diffraction. The results of numerical simulation of output waveforms are presented. In the first order, we obtain a sinusoidal form of output power modulation with an efficiency of up to 40 percent. Optimal parameters of the phase diffraction gratings are calculated. Modulation produced in the zero order of diffraction has an impulse form with an efficiency of about 80-90 percent. The specific shape of the pulses in the zero order of diffraction depends on the distance between the two gratings. The results of numerical calculations and experimental studies are in good agreement. A special advantage of this type of modulator is the possibility of increasing the frequency of mechanical modulation of the laser beam to hundreds of kHz. The results of experimental studies of the characteristics of the scheme under consideration are presented. The device makes it possible to obtain modulation frequencies up to hundreds of kHz with a harmonic waveform in the first orders of diffraction and periodic pulses in the zero order.Π Π½Π°ΡΡΠΎΡΡΠ΅ΠΉ ΡΠ°Π±ΠΎΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ Π½ΠΎΠ²ΡΠΉ ΡΠΈΠΏ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π΄Π»Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. ΠΠΎΠ΄ΡΠ»ΠΈΡΡΡΡΠΈΠΉ Π±Π»ΠΎΠΊ ΡΠΎΡΡΠΎΠΈΡ ΠΈΠ· Π΄Π²ΡΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΡΡΠΎΠΊ Ρ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΠΌ ΠΏΡΠΎΡΠΈΠ»Π΅ΠΌ, ΠΎΠ΄Π½Π° ΠΈΠ· ΠΊΠΎΡΠΎΡΡΡ
ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ°Π΅ΡΡΡ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π΄ΡΡΠ³ΠΎΠΉ. ΠΡΡ
ΠΎΠ΄Π½ΡΠΌ ΠΏΡΡΠΊΠΎΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² ΡΡΠΎΠΌ ΡΡΡΡΠΎΠΉΡΡΠ²Π΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ Π»ΠΈΠ±ΠΎ ΠΏΡΡΠΎΠΊ Π½ΡΠ»Π΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ΄ΠΊΠ° Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ, Π»ΠΈΠ±ΠΎ ΠΎΠ΄ΠΈΠ½ ΠΈΠ· ΠΏΠ΅ΡΠ²ΡΡ
ΠΏΠΎΡΡΠ΄ΠΊΠΎΠ² Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΡΠΈΠ²ΠΎΠ΄ΡΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠΎΡΠΌ Π²ΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ². Π ΠΏΠ΅ΡΠ²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ ΠΌΡ ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌ ΡΠΈΠ½ΡΡΠΎΠΈΠ΄Π°Π»ΡΠ½ΡΡ ΡΠΎΡΠΌΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ Π΄ΠΎ 40 ΠΏΡΠΎΡΠ΅Π½ΡΠΎΠ². Π Π°ΡΡΡΠΈΡΠ°Π½Ρ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΡΡΠΎΠΊ. ΠΠΎΠ΄ΡΠ»ΡΡΠΈΡ, ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠ°Ρ Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ, ΠΈΠΌΠ΅Π΅Ρ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΡΡ ΡΠΎΡΠΌΡ Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΠΎΠΊΠΎΠ»ΠΎ 80-90 ΠΏΡΠΎΡΠ΅Π½ΡΠΎΠ². ΠΠΎΠ½ΠΊΡΠ΅ΡΠ½Π°Ρ ΡΠΎΡΠΌΠ° ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ Π΄Π²ΡΠΌΡ ΡΠ΅ΡΡΡΠΊΠ°ΠΌΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΠ°ΡΡΡΡΠΎΠ² ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π°Ρ
ΠΎΠ΄ΡΡΡΡ Π² Ρ
ΠΎΡΠΎΡΠ΅ΠΌ ΡΠΎΠ³Π»Π°ΡΠΈΠΈ. ΠΡΠΎΠ±ΡΠΌ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎΠΌ ΡΡΠΎΠ³ΠΎ ΡΠΈΠΏΠ° ΠΌΠΎΠ΄ΡΠ»ΡΡΠΎΡΠ° ΡΠ²Π»ΡΠ΅ΡΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΡΠ°ΡΡΠΎΡΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ Π»ΡΡΠ° Π΄ΠΎ ΡΠΎΡΠ΅Π½ ΠΊΠΡ. ΠΡΠΈΠ²ΠΎΠ΄ΡΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΠΎΠΉ ΡΡ
Π΅ΠΌΡ. Π£ΡΡΡΠΎΠΉΡΡΠ²ΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΠΎΠ»ΡΡΠ°ΡΡ ΡΠ°ΡΡΠΎΡΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π΄ΠΎ ΡΠΎΡΠ΅Π½ ΠΊΠΡ Ρ ΡΠΈΠ³Π½Π°Π»ΠΎΠΌ Π³Π°ΡΠΌΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠΌΡ Π² ΠΏΠ΅ΡΠ²ΡΡ
ΠΏΠΎΡΡΠ΄ΠΊΠ°Ρ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ ΠΈ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠΌΠΏΡΠ»ΡΡΠ°ΠΌΠΈ Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅
Laser beam modulation using corner reflector and deep diffraction grating
A new scheme of the power modulator of laser beam is based on a corner-reflector unit with a relief diffraction grating that is placed on a plane of the unit and has a relief depth of several wavelengths of the laser radiation. It is shown that angular oscillations of the unit make it possible to implement modulation of the zero-order diffraction beam at a modulation depth of almost 100% and a relatively high linearity of the modulation characteristic that is reached at modulation depths of greater than 50%. Β© 2017, Pleiades Publishing, Inc
Optical Spectral Filter Based on a Deep Periodic Relief Reflection Structure
Abstract: A filter based on a reflecting periodic relief diffraction structure with a relief depth of greater than one half of optical wavelength is proposed. The input-output power transfer coefficient is studied versus the optical wavelength. The filter can be configured to completely suppress radiation at a specified wavelength, and the spectral characteristic can be changed due to variation in the angle of incidence of the input beam. A method for calculation of the filter parameters is proposed, and a filter that suppresses radiation at a specified wavelength and transmits radiation at another wavelength is calculated. The filter is easy-to-implement in both visible and IR spectral ranges. Β© 2020, Pleiades Publishing, Inc
Π£ΡΡΡΠΎΠΉΡΡΠ²ΠΎ Π΄Π»Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ
In this paper we consider a new type of mechanical device for periodic modulation of laser radiation. The modulating unit consists of two phase diffraction gratings with a rectangular profile, one of which moves relative to the other. The output beam of radiation in this device can be either a zero-order beam of diffraction, or one of the first orders of diffraction. The results of numerical simulation of output waveforms are presented. In the first order, we obtain a sinusoidal form of output power modulation with an efficiency of up to 40 percent. Optimal parameters of the phase diffraction gratings are calculated. Modulation produced in the zero order of diffraction has an impulse form with an efficiency of about 80-90 percent. The specific shape of the pulses in the zero order of diffraction depends on the distance between the two gratings. The results of numerical calculations and experimental studies are in good agreement. A special advantage of this type of modulator is the possibility of increasing the frequency of mechanical modulation of the laser beam to hundreds of kHz. The results of experimental studies of the characteristics of the scheme under consideration are presented. The device makes it possible to obtain modulation frequencies up to hundreds of kHz with a harmonic waveform in the first orders of diffraction and periodic pulses in the zero order.Π Π½Π°ΡΡΠΎΡΡΠ΅ΠΉ ΡΠ°Π±ΠΎΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ Π½ΠΎΠ²ΡΠΉ ΡΠΈΠΏ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π΄Π»Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. ΠΠΎΠ΄ΡΠ»ΠΈΡΡΡΡΠΈΠΉ Π±Π»ΠΎΠΊ ΡΠΎΡΡΠΎΠΈΡ ΠΈΠ· Π΄Π²ΡΡ
ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΡΡΠΎΠΊ Ρ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΠΌ ΠΏΡΠΎΡΠΈΠ»Π΅ΠΌ, ΠΎΠ΄Π½Π° ΠΈΠ· ΠΊΠΎΡΠΎΡΡΡ
ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ°Π΅ΡΡΡ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π΄ΡΡΠ³ΠΎΠΉ. ΠΡΡ
ΠΎΠ΄Π½ΡΠΌ ΠΏΡΡΠΊΠΎΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² ΡΡΠΎΠΌ ΡΡΡΡΠΎΠΉΡΡΠ²Π΅ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ Π»ΠΈΠ±ΠΎ ΠΏΡΡΠΎΠΊ Π½ΡΠ»Π΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ΄ΠΊΠ° Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ, Π»ΠΈΠ±ΠΎ ΠΎΠ΄ΠΈΠ½ ΠΈΠ· ΠΏΠ΅ΡΠ²ΡΡ
ΠΏΠΎΡΡΠ΄ΠΊΠΎΠ² Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ. ΠΡΠΈΠ²ΠΎΠ΄ΡΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠΎΡΠΌ Π²ΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΈΠ³Π½Π°Π»ΠΎΠ². Π ΠΏΠ΅ΡΠ²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ ΠΌΡ ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌ ΡΠΈΠ½ΡΡΠΎΠΈΠ΄Π°Π»ΡΠ½ΡΡ ΡΠΎΡΠΌΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ Π΄ΠΎ 40 ΠΏΡΠΎΡΠ΅Π½ΡΠΎΠ². Π Π°ΡΡΡΠΈΡΠ°Π½Ρ ΠΎΠΏΡΠΈΠΌΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΠ°Π·ΠΎΠ²ΡΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅ΡΡΡΠΎΠΊ. ΠΠΎΠ΄ΡΠ»ΡΡΠΈΡ, ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠ°Ρ Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ, ΠΈΠΌΠ΅Π΅Ρ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΡΡ ΡΠΎΡΠΌΡ Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΠΎΠΊΠΎΠ»ΠΎ 80-90 ΠΏΡΠΎΡΠ΅Π½ΡΠΎΠ². ΠΠΎΠ½ΠΊΡΠ΅ΡΠ½Π°Ρ ΡΠΎΡΠΌΠ° ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ² Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ Π΄Π²ΡΠΌΡ ΡΠ΅ΡΡΡΠΊΠ°ΠΌΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΠ°ΡΡΡΡΠΎΠ² ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π½Π°Ρ
ΠΎΠ΄ΡΡΡΡ Π² Ρ
ΠΎΡΠΎΡΠ΅ΠΌ ΡΠΎΠ³Π»Π°ΡΠΈΠΈ. ΠΡΠΎΠ±ΡΠΌ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎΠΌ ΡΡΠΎΠ³ΠΎ ΡΠΈΠΏΠ° ΠΌΠΎΠ΄ΡΠ»ΡΡΠΎΡΠ° ΡΠ²Π»ΡΠ΅ΡΡΡ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΡΠ°ΡΡΠΎΡΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ Π»ΡΡΠ° Π΄ΠΎ ΡΠΎΡΠ΅Π½ ΠΊΠΡ. ΠΡΠΈΠ²ΠΎΠ΄ΡΡΡΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΠΎΠΉ ΡΡ
Π΅ΠΌΡ. Π£ΡΡΡΠΎΠΉΡΡΠ²ΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΠΎΠ»ΡΡΠ°ΡΡ ΡΠ°ΡΡΠΎΡΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π΄ΠΎ ΡΠΎΡΠ΅Π½ ΠΊΠΡ Ρ ΡΠΈΠ³Π½Π°Π»ΠΎΠΌ Π³Π°ΡΠΌΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠΌΡ Π² ΠΏΠ΅ΡΠ²ΡΡ
ΠΏΠΎΡΡΠ΄ΠΊΠ°Ρ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ ΠΈ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠΌΠΏΡΠ»ΡΡΠ°ΠΌΠΈ Π² Π½ΡΠ»Π΅Π²ΠΎΠΌ ΠΏΠΎΡΡΠ΄ΠΊΠ΅
ΠΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠΈΠ»ΡΡΡ, ΠΏΠΎΡΡΡΠΎΠ΅Π½Π½ΡΠΉ Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π³Π»ΡΠ±ΠΎΠΊΠΎΠΉ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠ΅ΠΉ ΡΠ΅Π»ΡΠ΅ΡΠ½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ
An optical scheme intended for filtering the wavelength spectrum of an optical signal is proposed and investigated. The filter scheme uses a relief reflecting periodic diffraction structure with a relief depth of more than half the wavelength. The input optical beam is directed to the diffraction structure at an angle. The plane of incidence is parallel to the lines of the diffraction structure. A zero-order beam of diffraction is output. The dependence of the power transfer coefficient from the input to the output on the wavelength of the emission has zeros and maxima at certain wavelengths. The transmission coefficient at maxima is close to unity. The filter can be configured to completely suppress any selected wavelength and is easily reconfigured by changing the angle of incidence of the input beam. A technique for calculating filter parameters is described. Examples of calculation of a filter for suppressing one of the spectral emission lines of an argon laser are given, provided that another strong spectral line is passed. The filter is equally simple for practical implementation in both the visible and infrared ranges.Π ΡΡ
Π΅ΠΌΠ΅ ΡΠΈΠ»ΡΡΡΠ° ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½Π° Π³Π»ΡΠ±ΠΎΠΊΠ°Ρ ΡΠ΅Π»ΡΠ΅ΡΠ½Π°Ρ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠ°Ρ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠ°Ρ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½Π°Ρ ΡΡΡΡΠΊΡΡΡΠ° (ΠΠ Π‘) Ρ Π³Π»ΡΠ±ΠΈΠ½ΠΎΠΉ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π»ΡΠ΅ΡΠ° Π±ΠΎΠ»Π΅Π΅ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½Ρ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ. ΠΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΏΡΡΠΎΠΊ Π½Π°ΠΏΡΠ°Π²Π»ΡΠ΅ΡΡΡ Π½Π° ΠΠ Π‘ ΠΏΠΎΠ΄ ΡΠ³Π»ΠΎΠΌ. ΠΠ»ΠΎΡΠΊΠΎΡΡΡ ΠΏΠ°Π΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½Π° Π»ΠΈΠ½ΠΈΡΠΌ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ. ΠΡΡΠΎΠΊ Π½ΡΠ»Π΅Π²ΠΎΠ³ΠΎ ΠΏΠΎΡΡΠ΄ΠΊΠ° Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ Π²ΡΡ
ΠΎΠ΄Π½ΡΠΌ. ΠΠ°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΏΠ΅ΡΠ΅Π΄Π°ΡΠΈ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ Ρ Π²Ρ
ΠΎΠ΄Π° Π½Π° Π²ΡΡ
ΠΎΠ΄ ΠΎΡ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΈΠΌΠ΅Π΅Ρ Π½ΡΠ»ΠΈ ΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΡ Π½Π° ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ½Π½ΡΡ
Π΄Π»ΠΈΠ½Π°Ρ
Π²ΠΎΠ»Π½. Π€ΠΈΠ»ΡΡΡ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ Π½Π°ΡΡΡΠΎΠ΅Π½ Π½Π° ΠΏΠΎΠ»Π½ΠΎΠ΅ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΠ΅ Π»ΡΠ±ΠΎΠΉ Π²ΡΠ±ΡΠ°Π½Π½ΠΎΠΉ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ ΠΈ Π»Π΅Π³ΠΊΠΎ ΠΏΠ΅ΡΠ΅ΡΡΡΠ°ΠΈΠ²Π°Π΅ΡΡΡ Π·Π° ΡΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ³Π»Π° ΠΏΠ°Π΄Π΅Π½ΠΈΡ Π²Ρ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ°. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΠΏΡΠΈΠΌΠ΅ΡΡ ΡΠ°ΡΡΡΡΠ° ΡΠΈΠ»ΡΡΡΠ° Π΄Π»Ρ ΠΏΠΎΠ΄Π°Π²Π»Π΅Π½ΠΈΡ ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π°ΡΠ³ΠΎΠ½ΠΎΠ²ΠΎΠ³ΠΎ Π»Π°Π·Π΅ΡΠ° ΠΏΡΠΈ ΡΡΠ»ΠΎΠ²ΠΈΠΈ ΠΏΡΠΎΠΏΡΡΠΊΠ°Π½ΠΈΡ Π΄ΡΡΠ³ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠΉ Π»ΠΈΠ½ΠΈΠΈ. Π€ΠΈΠ»ΡΡΡ ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΠΎ ΠΏΡΠΎΡΡ Π΄Π»Ρ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠ°ΠΊ Π² Π²ΠΈΠ΄ΠΈΠΌΠΎΠΌ, ΡΠ°ΠΊ ΠΈ ΠΈΠ½ΡΡΠ°ΠΊΡΠ°ΡΠ½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½
ΠΠΎΠ²ΡΠ΅ ΠΎΠΏΡΠΎΡΠ»Π΅ΠΊΡΠΎΡΠ½Π½ΡΠ΅ ΡΡ Π΅ΠΌΡ, ΠΏΠΎΡΡΡΠΎΠ΅Π½Π½ΡΠ΅ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ΅Π»ΡΠ΅ΡΠ½ΡΡ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠΈΡ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ ΡΡΡΡΠΊΡΡΡ Ρ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΠΌ ΠΏΡΠΎΡΠΈΠ»Π΅ΠΌ
The article describes a number of new schemes designed to measure small angular displacements and oscillations, to modulate laser radiation, and also to filter the spectrum of optical radiation in the visible and infrared wavelengths. The operation of these schemes is based on the effects observed when a laser beam is reflected from deep diffractive relief structures with a rectangular profile, with a relief depth from a quarter of the wavelength to several wavelengths due to laser radiation. The applications of these devices are varied. For example, sensors of small angular displacements and vibrations can be used in the study of vibrations and in the design of seismometers and tiltmeters. A mechanically driven modulator operates in the low-frequency modulation region, but can provide analogue modulation of the radiation power with different modulation depths from zero to one hundred percent. Optical filters built on the basis of deep relief reflective structures have oscillating dependences of the transmission coefficient on the wavelength. It is possible to select parameters in such a way that the filter has a zero transmission coefficient at a given wavelength and a transmission coefficient close to unity in another given area. The advantages of a filter of this type can be attributed simply to its production and the possibility of realigning the spectral characteristics of the filter within wide limits.Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ ΡΡΠ΄ Π½ΠΎΠ²ΡΡ
ΡΡ
Π΅ΠΌ, ΠΏΡΠ΅Π΄Π½Π°Π·Π½Π°ΡΠ΅Π½Π½ΡΡ
Π΄Π»Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΌΠ°Π»ΡΡ
ΡΠ³Π»ΠΎΠ²ΡΡ
ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ, Π΄Π»Ρ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, Π° ΡΠ°ΠΊΠΆΠ΅ Π΄Π»Ρ ΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΈ ΡΠΏΠ΅ΠΊΡΡΠ° ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² Π²ΠΈΠ΄ΠΈΠΌΠΎΠΌ ΠΈ Π² ΠΈΠ½ΡΡΠ°ΠΊΡΠ°ΡΠ½ΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ Π΄Π»ΠΈΠ½ Π²ΠΎΠ»Π½. Π ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ°Π±ΠΎΡΡ ΡΡΠΈΡ
ΡΡ
Π΅ΠΌ Π»Π΅ΠΆΠ°Ρ ΡΡΡΠ΅ΠΊΡΡ, Π½Π°Π±Π»ΡΠ΄Π°Π΅ΠΌΡΠ΅ ΠΏΡΠΈ ΠΎΡΡΠ°ΠΆΠ΅Π½ΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ° ΠΎΡ Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅Π»ΡΠ΅ΡΠ½ΡΡ
ΡΡΡΡΠΊΡΡΡ, ΠΈΠΌΠ΅ΡΡΠΈΡ
ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΠΉ ΠΏΡΠΎΡΠΈΠ»Ρ, Ρ Π³Π»ΡΠ±ΠΈΠ½ΠΎΠΉ ΡΠ΅Π»ΡΠ΅ΡΠ° ΠΎΡ ΡΠ΅ΡΠ²Π΅ΡΡΠΈ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ Π΄ΠΎ Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΈΡ
Π΄Π»ΠΈΠ½ Π²ΠΎΠ»Π½ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π»Π°Π·Π΅ΡΠ°. ΠΠ±Π»Π°ΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΉ ΡΡΠΈΡ
ΡΡΡΡΠΎΠΉΡΡΠ² ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·Π½Ρ. ΠΠ°ΠΏΡΠΈΠΌΠ΅Ρ, Π΄Π°ΡΡΠΈΠΊΠΈ ΠΌΠ°Π»ΡΡ
ΡΠ³Π»ΠΎΠ²ΡΡ
ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ ΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½Ρ ΠΏΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ Π²ΠΈΠ±ΡΠ°ΡΠΈΠΉ ΠΈ ΠΏΡΠΈ ΠΊΠΎΠ½ΡΡΡΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ΅ΠΉΡΠΌΠΎΠΌΠ΅ΡΡΠΎΠ² ΠΈ Π½Π°ΠΊΠ»ΠΎΠ½ΠΎΠΌΠ΅ΡΠΎΠ². ΠΠΎΠ΄ΡΠ»ΡΡΠΎΡ Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΎΠΌ ΡΠ°Π±ΠΎΡΠ°Π΅Ρ Π² ΠΎΠ±Π»Π°ΡΡΠΈ Π½ΠΈΠ·ΠΊΠΈΡ
ΡΠ°ΡΡΠΎΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ, Π½ΠΎ ΠΌΠΎΠΆΠ΅Ρ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΡΡ Π°Π½Π°Π»ΠΎΠ³ΠΎΠ²ΡΡ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΡ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ Π³Π»ΡΠ±ΠΈΠ½Π°ΠΌΠΈ ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ ΠΎΡ Π½ΡΠ»Ρ Π΄ΠΎ ΡΡΠ° ΠΏΡΠΎΡΠ΅Π½ΡΠΎΠ². ΠΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠΈΠ»ΡΡΡΡ, ΠΏΠΎΡΡΡΠΎΠ΅Π½Π½ΡΠ΅ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π³Π»ΡΠ±ΠΎΠΊΠΈΡ
ΡΠ΅Π»ΡΠ΅ΡΠ½ΡΡ
ΠΎΡΡΠ°ΠΆΠ°ΡΡΠΈΡ
ΡΡΡΡΠΊΡΡΡ, ΠΈΠΌΠ΅ΡΡ ΠΎΡΡΠΈΠ»Π»ΠΈΡΡΡΡΠΈΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΠΏΠ΅ΡΠ΅Π΄Π°ΡΠΈ ΠΎΡ Π΄Π»ΠΈΠ½Ρ Π²ΠΎΠ»Π½Ρ. ΠΠΎΠΆΠ½ΠΎ Π²ΡΠ±ΡΠ°ΡΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΠ°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, ΡΡΠΎΠ±Ρ ΡΠΈΠ»ΡΡΡ ΠΈΠΌΠ΅Π» Π½ΡΠ»Π΅Π²ΠΎΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ ΠΏΠ΅ΡΠ΅Π΄Π°ΡΠΈ Π½Π° Π·Π°Π΄Π°Π½Π½ΠΎΠΉ Π΄Π»ΠΈΠ½Π΅ Π²ΠΎΠ»Π½Ρ ΠΈ Π±Π»ΠΈΠ·ΠΊΠΈΠΉ ΠΊ Π΅Π΄ΠΈΠ½ΠΈΡΠ΅ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ ΠΏΠ΅ΡΠ΅Π΄Π°ΡΠΈ Π² Π΄ΡΡΠ³ΠΎΠΉ Π·Π°Π΄Π°Π½Π½ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ. Π Π΄ΠΎΡΡΠΎΠΈΠ½ΡΡΠ²Π°ΠΌ ΡΠΈΠ»ΡΡΡΠ° Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠΏΠ° ΠΌΠΎΠΆΠ½ΠΎ ΠΎΡΠ½Π΅ΡΡΠΈ ΠΏΡΠΎΡΡΠΎΡΡ Π΅Π³ΠΎ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΈ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΈ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΎΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΡΠΈΠ»ΡΡΡΠ° Π² ΡΠΈΡΠΎΠΊΠΈΡ
ΠΏΡΠ΅Π΄Π΅Π»Π°Ρ
ΠΠ°ΠΊΠ΅Ρ ΡΠ΅ΠΉΡΠΌΠΎΠΌΠ΅ΡΡΠ° Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π΄Π°ΡΡΠΈΠΊΠ° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π³Π»ΡΠ±ΠΎΠΊΠΎΠΉ ΠΎΡΡΠ°ΠΆΠ°ΡΡΠ΅ΠΉ ΡΠ°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΠ΅ΡΠΊΠΈ
The new type of the device for measuring seismics is developed and tested. The vibration sensor unit is built on the base of a corner reflector and a deep phase diffraction grating with a rectangular profile. The article shows the scheme of the device, describes the principle of its operation.Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π° ΠΈ ΠΈΡΠΏΡΡΠ°Π½Π° ΡΡ
Π΅ΠΌΠ° ΠΏΡΠΈΠ±ΠΎΡΠ°, ΠΏΡΠ΅Π΄Π½Π°Π·Π½Π°ΡΠ΅Π½Π½ΠΎΠ³ΠΎ Π΄Π»Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ Π·Π΅ΠΌΠ½ΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ. ΠΠ»ΠΎΠΊ Π΄Π°ΡΡΠΈΠΊΠ° ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΏΠΎΡΡΡΠΎΠ΅Π½ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ³ΠΎΠ»ΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΎΡΡΠ°ΠΆΠ°ΡΠ΅Π»Ρ ΠΈ Π³Π»ΡΠ±ΠΎΠΊΠΎΠΉ ΡΠ°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΠ΅ΡΠΊΠΈ Ρ ΠΏΡΡΠΌΠΎΡΠ³ΠΎΠ»ΡΠ½ΡΠΌ ΠΏΡΠΎΡΠΈΠ»Π΅ΠΌ. Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΡΡ
Π΅ΠΌΠ° ΡΡΡΡΠΎΠΉΡΡΠ²Π°, ΠΎΠΏΠΈΡΠ°Π½ ΠΏΡΠΈΠ½ΡΠΈΠΏ Π΅Π³ΠΎ ΡΠ°Π±ΠΎΡΡ