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IntroductiontoAcousto-OpticsTechnologyAcousto-Opticdevicesareusedinlaserequipmentforelectroniccontroloftheintensityandpositionofthelaserbeam

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Introduction to Acousto-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 n 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(shù)及AOM介紹文件

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


Model #AMM-100-8-70-1550
波長(zhǎng) 1550 nm
基底 Amtir
光功率密度 3 W/mm2
中心頻率 100 MHz
射頻帶寬 10 MHz
有效孔徑 0.3 mm
光直徑 0.2 mm
上升時(shí)間 70 ns
數(shù)字調(diào)制帶寬 8 MHz
布拉格角 31 mrad
分離角 62 mrad
聲波速度 2.52E+03
射頻功率 <1.0 W
透光率 >95%
衍射效率 ~80%
輸入阻抗 50 ohms
V.S.W.R. 2.1:1
光偏振態(tài) Random


Model # QZF-200-100-370
波長(zhǎng)范圍 370nm
頻移 200MHz
射頻帶寬 100MHz
有效孔徑 0.3 mm
光傳輸 > 98 %
衍射效率 ~65% (at ~2.5W RF Power)
布拉格角 6 mrad
分離角 12 mrad
聲波速度 5.96 E+3 m/sec
射頻功率 ~2.5 W
輸入阻抗 50ohms
V.S.W.R 2:1
光的偏振 Linear
射頻連接器 SMA


Model # TEF-362-50-795
波長(zhǎng)范圍 795nm
頻移 362MHz
射頻帶寬 50MHz
有效孔徑 0.3 mm
光傳輸 > 98 %
衍射效率 50-60%
布拉格角 32 mrad
分離角 64 mrad
聲波速度 4.2E+3 m/sec
射頻功率 ~2 W
輸入阻抗 50ohms
V.S.W.R 2:1
光的偏振 Linear (Vertical or Horizontal)
射頻連接器 SMA


Model # TEF-600-400-689
波長(zhǎng)范圍 689nm
頻移 600MHz
射頻帶寬 400MHz
有效孔徑 0.075 mm
光傳輸 > 95 %
衍射效率 40~45%
布拉格角 49 mrad
分離角 98 mrad
射頻功率 ~1 W
輸入阻抗 50ohms
V.S.W.R 2:1
光的偏振 Linear
射頻連接器 SMA


Model # GPF-1000-200-780
基板 GaP
波長(zhǎng)范圍 780nm
頻移 1000MHz
射頻帶寬 200MHz
有效孔徑 0.075mm
光傳輸 >80%
衍射效率 ~25%
波前畸變 l/10
布拉格角 62mrad
分離角 124mrad
聲波速度 6.31E+3 m/s
射頻功率 ~1W
輸入阻抗 50ohms
V.S.W.R 3:01
光的偏振 Linear (horizontal)
射頻連接器 SMA


Model # TEF-1500-100-795
基板 TeO2
波長(zhǎng)范圍 795nm
頻移 1500MHz
射頻帶寬 100MHz
有效孔徑 0.075mm
衍射效率 15-20%
布拉格角 142mrad
分離角 284mrad
聲波速度 4.2E+3 m/s
射頻功率 1.0 W
輸入阻抗 50ohms
V.S.W.R 2:1
光的偏振 Linear (horizontal or vertical)
射頻連接器 SMA


Model # GPF-1500-200-780
數(shù)據(jù) 780 nm
基底 GaP
光功率密度 100 W/mm2
光傳輸 >80%
移頻偏移 1500 MHz
射頻帶寬 200 MHz
活動(dòng)直徑 0.075 mm
布拉格角 93 mrad
夾角 186 mrad
聲速度(米/秒 ) 6.31E+03
射頻功率(瓦特) 1 W
衍射效率 ~30%
輸入阻抗 50 ohms
電壓駐波比 2:01
光學(xué)偏振 Linear
類型 Air-cooled


Model # GPF-1700-200-795
基底 GaP
波長(zhǎng)范圍 795nm
頻移 1700MHz
射頻帶寬 200MHz
有效孔徑 0.075mm
光傳輸 >80%
衍射效率 ~30%
波前畸變 l/10
布拉格角 107mrad
分離角 107mrad
聲波速度 6.31E+3 m/s
射頻功率 1W
輸入阻抗 50ohms
V.S.W.R 2.1:1
光的偏振 Linear (horizontal)
射頻連接器 SMA


Model#GPF-3400-100-795
基板 GaP
波長(zhǎng)范圍 795nm
頻移 3400MHz
射頻帶寬 100MHz
有效孔徑 25mm
光傳輸 >80%
衍射效率 ~1%
波前畸變 l/10
布拉格角 212mrad
分離角 424mrad
聲波速度 6.31E+3 m/s
射頻功率 ~1W
輸入阻抗 50ohms
V.S.W.R 0.125694444
光的偏振 Linear
射頻連接器 SMA


Model #AMM-100-8-70-1550-2FP
波長(zhǎng) 1550 nm
光學(xué)范圍 130 mW (C.W)
中心頻率 100 MHz
數(shù)字調(diào)制帶寬 8 MHz
有效孔徑 0.3 mm
晶體內(nèi)束直徑 0.2 mm
上升時(shí)間 70 ns
布拉格角 31 mrad
分離角 62 mrad
聲波速度 2.50E+03
射頻功率 1.0 W
光傳輸 >95%
輸入阻抗 50 ohms
V.S.W.R. 2.1:1
光偏振態(tài) Random (Option: Linear with PM fiber)
Case Type 2 Port Fiber Optically Pigtailed
光纖類型 9 m core, 125 m cladding Single Mode
光纖連接頭 FC
拋光的光纖末端 APC
光纖長(zhǎng) 1 m
纖維夾套 900 mm OD
背反射 50-60 dB
插損 2.5-3.5 dB


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