Visible and Near-Infrared Acousto-Optic Modulators AOMO 3315-125

Visible and Near-Infrared Acousto-Optic Modulators AOMO 3315-125

Supplier
Sinteclaser
Part Number
AOMO 3315-125
Category
Acousto-Optic Modulator
Origin
China

AOMO 3315-125 provides 315 MHz acousto-optic frequency shifting and modulation for visible and near-infrared laser systems operating over 470–850 nm. It uses a TeO₂ acousto-optic medium with 50 MHz RF bandwidth and a 2.5 × 1.5 mm active clear aperture, supporting frequency shifting and beam control in the blue, green, red and near-infrared bands. The datasheet specifies performance at 488 nm, 532 nm, 633 nm and 800 nm, including operating RF power, Bragg angle, beam separation, diffraction efficiency and rise time. It is particularly suitable for applications requiring frequency shifts greater than the 100 MHz or 270 MHz levels. Performance is defined for an 800 µm beam diameter, and beam separation increases with wavelength. Applications include interferometry, optical testing and metrology, laser Doppler systems, scientific laser platforms and visible/near-infrared photonics.

Specification Snapshot
Beam Separation Angle [Wavelength 488 nm]
36.6 mrad
Beam Separation Angle [Wavelength 532 nm]
40 mrad
Beam Separation Angle [Wavelength 633 nm]
47.4 mrad
Beam Separation Angle [Wavelength 800 nm]
60 mrad
Diffraction Efficiency [Performance for different beam diameters; original table header "beam diameter": 30 μm (retained as in source)]
45%
Rise Time [Performance for different beam diameters; original table header "beam diameter": 30 μm (retained as in source)]
7 ns
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Overview

AOMO 3315-125 provides 315 MHz acousto-optic frequency shifting and modulation for visible and near-infrared laser systems operating over 470–850 nm. It uses a TeO₂ acousto-optic medium with 50 MHz RF bandwidth and a 2.5 × 1.5 mm active clear aperture, supporting frequency shifting and beam control in the blue, green, red and near-infrared bands. The datasheet specifies performance at 488 nm, 532 nm, 633 nm and 800 nm, including operating RF power, Bragg angle, beam separation, diffraction efficiency and rise time. It is particularly suitable for applications requiring frequency shifts greater than the 100 MHz or 270 MHz levels. Performance is defined for an 800 µm beam diameter, and beam separation increases with wavelength. Applications include interferometry, optical testing and metrology, laser Doppler systems, scientific laser platforms and visible/near-infrared photonics.

Specifications

ParameterValue
Rated RF Power [Wavelength 488 nm]0.5 W
Bragg Angle [Wavelength 488 nm]18.3 mrad
Beam Separation Angle [Wavelength 488 nm]36.6 mrad
Rated RF Power [Wavelength 532 nm]0.7 W
Bragg Angle [Wavelength 532 nm]20 mrad
Beam Separation Angle [Wavelength 532 nm]40 mrad
Rated RF Power [Wavelength 633 nm]1 W
Bragg Angle [Wavelength 633 nm]23.7 mrad
Beam Separation Angle [Wavelength 633 nm]47.4 mrad
Rated RF Power [Wavelength 800 nm]1.5 W
Bragg Angle [Wavelength 800 nm]30 mrad
Beam Separation Angle [Wavelength 800 nm]60 mrad
Diffraction Efficiency [Performance for different beam diameters; original table header "beam diameter": 30 μm (retained as in source)]45%
Rise Time [Performance for different beam diameters; original table header "beam diameter": 30 μm (retained as in source)]7 ns
Diffraction Efficiency [Performance for different beam diameters; original table header "beam diameter": 532 nm (retained as in source)]85%
Rise Time [Performance for different beam diameters; original table header "beam diameter": 532 nm (retained as in source)]128 ns
Diffraction Efficiency [Performance for different beam diameters; original table header "beam diameter": 633 nm (retained as in source)]80%
Rise Time [Performance for different beam diameters; original table header "beam diameter": 633 nm (retained as in source)]128 ns
Diffraction Efficiency [Performance for different beam diameters; original table header "beam diameter": 800 nm (retained as in source)]80%
Rise Time [Performance for different beam diameters; original table header "beam diameter": 800 nm (retained as in source)]128 ns
Applicable Wavelength BandVisible Light , Near Infrared
Minimum Operating Wavelength450 nm
Maximum Operating Wavelength850 nm
Center Frequency315 MHz
Clear Aperture Dimension1.5 mm × 2.5 mm
Rise/Fall Time159 ns
Acousto-optic MediumTeO₂
Acoustic Velocity4.2 mm/μs
RF Bandwidth [-10 dB Return Loss]50 MHz(@ -10 dB Return Loss )
Input Impedance50 Ω
Standing Wave Ratio≤ 1.5:1
Insertion Loss≤ 4%
Single-Surface Reflectance≤ 1%
Antireflection CoatingMIL-C-48497
Optical Power Density250 W/mm²
Extinction Ratio≥1000:1
PolarizationAt a 90° angle to the mounting plane

Key Features

Compact acousto-optic frequency converter for visible and near-infrared laser control Uses tellurium dioxide acousto-optic material for efficient beam interaction Supports precise laser frequency conversion, switching and modulation Helps control beam timing, optical power and laser intensity Designed for reliable integration into laboratory and OEM photonic systems Suitable for optical testing and measurement, interferometry and laser Doppler applications Supports scientific laser platforms, imaging systems and instruments Provides stable optical performance for repeatable beam-control tasks Ideal for applications requiring controlled visible and near-infrared beam handling.

Datasheet

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Supplier Information

Si
Sinteclaser
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Wuhan Sintec Optoelectronics Technology Co., Ltd. is a high-tech enterprise and a specialized and sophisticated 'Little Giant' enterprise at the upstream of the domestic laser industry chain. The company focuses on the R&D, manufacturing, sales and service of lasers and laser accessories. Its main products include femtosecond lasers, picosecond lasers, acousto-optic modulators, optical components, etc., widely used in laser equipment manufacturing, scientific research and other fields. Located in Wuhan Optical Valley, with a modern industrial park, the company provides one-stop personalized services for the laser industry, with customers all over China and products exported overseas.

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