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IntroductiontoAcousto-OpticsTechnologyAcousto-Opticdevicesareusedinlaserequipmentforelectroniccontroloftheintensityandpositionofthelaserbeam

Introduction toAcousto-Optics Technology

Acousto-Optic devices are used in laser equipment for electronic control of the intensity and position of the laser beam. In this note, we will explain the theory and application of acousto-optic modulators.
Acousto-optic interaction occurs in all optical mediums when an acoustic wave and a laser beam are present and interact with each other. When an acoustic wave is launched into the optical medium, it generates a refractive index wave that behaves like a sinusoidal grating. An incident laser beam passing through this granting will be diffracted into several orders. With appropriate design, the first order beam has the highest efficiency. Its angular position is linearly proportional to the acoustic frequency, so that the higher the frequency, the larger the diffracted angle.

Where, λ, is the optical wavelength in air, fa, is the acoustic frequently, and , Va is the acoustic velocity, and Q, is the angle between the incident laser beam and the diffracted laser beam.
A diagram of the angular relationship between the acoustic wave and the laser beams is shown in Figure 1.
The intensity of light diffracted (deflected) is proportional to the acoustic power (Pac), the material figure of merit (M2 ), geometric factors (L/H) and inversely proportional to the square of the wavelength.

With acousto-optics, both the deflection as well as the modulation of the amplitude of the optical beam are possible. Also, in the acousto-optic interaction, the laser beam frequency is shifted by an amount equal to the acoustic frequency. This frequency shift can be used for heterodyne detection applications, where precise phase information is measured.


聲光技術及AOM介紹文件

https://pan..com/s/17kbsu19U0PkxoBTkjqPV1A (提取碼:ji4c)


型號 單位 TEM-80-20-633
基板- TeO2
波長nm 633 (With High Power AR Coating)
中心頻率MHz 80
數字調制帶寬MHz 20
有效孔徑mm 0.5
上升沿ns 27
晶體內束直徑mm 0.134
光傳輸% >98
衍射效率% 75-80
波前畸變- λ/10
布拉格角mrad 6
分離角mrad 12
聲波速度m/s 4.20E+03
射頻功率W ~1
輸入阻抗ohms 50
V.S.W.R - 2:1
光偏振- Linear
射頻連接器- SMA


型號 單位 TEM-800-200-852
基板- TeO2
波長nm 852
中心頻率MHz 800
數字調制帶寬MHz 400
有效孔徑mm 0.05
上升沿ns 3
晶體內束直徑mm 0.013
數字調制帶寬 MHz200
模擬視頻帶寬MHz128
光傳輸% >95
衍射效率% 20-25
消光比- >1000:1
波前畸變- λ/10
布拉格角mrad 81
分離角mrad 162
聲波速度m/s 4.20E+03
射頻功率W 1
輸入阻抗ohms 50
V.S.W.R - 2:01
光功率密度W/mm25
光偏振- Linear
射頻連接器- SMA

聲光偏轉器

IntroductiontoA-ODeflectors/Scanner

聲光鎖模器

ModelFSML-80-20-BR-1

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