Analysis of Amplitude-Frequency Response of Acousto-Optic Delay Line

Гасанов, А. Р.; Gasanov, R. A.; Ахмедов, Р. A.

doi:10.3103/s0735272721010040

Cited by 4 publications

(1 citation statement)

References 13 publications

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“…In the case of Bragg diffraction, only one diffraction order is observed. The spatial position of the deflected beam and the light intensity in it is determined by the parameters of the radio frequency electrical signal connected to the terminals of the EAТ [17]. The deflected light beam passes through a slit in the diaphragm (D) and is recorded by a photodetector (PD).…”

Section: Methodsmentioning

confidence: 99%

Development of an axonometric model of photoelastic interaction in an acousto-optic delay line and its approbation

Гасанов

Hasanov

Rustamov

et al. 2022

TAPR

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The object of research is a mathematical model of the photoelastic interaction in an acousto-optic delay line (AODL). Two possible cases are discussed as applied to the ratio of the input pulse duration to the time of crossing the optical beam by an elastic wave packet. It is shown that in both cases the voltage at the output of the device is found as the sum of three components, which are formed by different mechanisms. If the duration of the input pulse is longer than the time of crossing the optical beam by an elastic wave packet, then the first component is determined by the process of entry of the leading edge of the elastic wave packet into the optical beam, the second – by the process of complete interaction of the optical beam with the elastic wave packet, and the third – by the process of exit of the trailing edge of the elastic wave packet from the optical beam. In the second case, i. e. when the duration of the input pulse is less than the time of crossing the optical beam by an elastic wave packet, the first term is determined by the process of entry of the elastic wave packet into the optical beam, the second – by the process of advancing the elastic wave packet in the aperture of the optical beam, and the third – by the process of exit of the elastic wave packet from the aperture of the optical beam. The corresponding equations for calculating the parameters of the output pulse were obtained by applying a rectangular pulse to the AODL input. It is proved that if the pulse duration at the AODL input is longer than the time of intersection of the optical beam by an elastic wave packet, then the pulse duration at its output will be equal to the duration of the input pulse. In the case when the duration of the input pulse is less than the time of crossing the optical beam by an elastic wave packet, the duration of the output pulse will be determined by the time of propagation of the elastic wave packet in the aperture of the optical beam. The obtained equations are confirmed by numerical calculations. The results of the numerical analysis were tested experimentally, which confirms the unequivocal adequacy of the proposed model of photoelastic interaction in an AODL.

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Section: Methodsmentioning

confidence: 99%