Visible and Near-Infrared Acousto-Optic Modulators AOMO 3350-199
AOMO 3350-199 is a compact high-speed visible and near-infrared acousto-optic modulator using tellurium dioxide as the acousto-optic medium. Designed for small-beam laser systems, it provides high-speed beam modulation, fast optical switching and precise intensity control. Fast response, high diffraction efficiency and high switching contrast meet beam-control and system-integration requirements in precision photonic systems. The excellent acousto-optic properties of tellurium dioxide and a broadband antireflection-coating design allow AOMO 3350-199 to provide stable, efficient acousto-optic interaction, reliable beam gating, pulse picking and dynamic modulation while maintaining beam quality. Its compact structure and RF integration facilitate integration into space-constrained optical systems, providing stable, reliable modulation for small-beam laser applications. Applications include laser-scanning microscopy, fluorescence excitation systems, analytical and inspection instruments, optical test platforms, research laser experimental systems and other photonics applications requiring high-speed beam control and precise laser switching, providing reliable beam modulation for high-performance laser systems.
Overview
Specifications
| Parameter | Value |
|---|---|
| Saturation RF Power [Wavelength 460 nm] | 0.63 W |
| Bragg Angle [Wavelength 460 nm] | 19.2 mrad |
| Beam Separation Angle [Wavelength 460 nm] | 38.4 mrad |
| Saturation RF Power [Wavelength 532 nm] | 0.90 W |
| Bragg Angle [Wavelength 532 nm] | 22.2 mrad |
| Beam Separation Angle [Wavelength 532 nm] | 44.4 mrad |
| Saturation RF Power [Wavelength 632 nm] | 1.00 W |
| Bragg Angle [Wavelength 632 nm] | 26.3 mrad |
| Beam Separation Angle [Wavelength 632 nm] | 52.6 mrad |
| Saturation RF Power [Wavelength 660 nm] | 1.00 W |
| Bragg Angle [Wavelength 660 nm] | 27.5 mrad |
| Beam Separation Angle [Wavelength 660 nm] | 55.0 mrad |
| Saturation RF Power [Wavelength 685 nm] | 1.00 W |
| Bragg Angle [Wavelength 685 nm] | 28.5 mrad |
| Beam Separation Angle [Wavelength 685 nm] | 57.0 mrad |
| Diffraction Efficiency [Wavelength 460 nm] | 80% |
| Rise Time [Wavelength 460 nm] | 9 ns |
| Diffraction Efficiency [Wavelength 532 nm] | 80% |
| Rise Time [Wavelength 532 nm] | 9 ns |
| Diffraction Efficiency [Wavelength 632 nm] | 70% |
| Rise Time [Wavelength 632 nm] | 9 ns |
| Diffraction Efficiency [Wavelength 660 nm] | 65% |
| Rise Time [Wavelength 660 nm] | 9 ns |
| Diffraction Efficiency [Wavelength 685 nm] | 60% |
| Rise Time [Wavelength 685 nm] | 9 ns |
| Applicable Wavelength Band | Visible Light , Near Infrared |
| Design Wavelength | 450 nm |
| Minimum Operating Wavelength | 850 nm |
| Maximum Operating Wavelength | 460–685 nm |
| Center Frequency | 350 MHz |
| Clear Aperture Dimension | 0.15 mm × 2 mm |
| Rise/Fall Time | 159 ns |
| Acousto-optic Medium | TeO₂ |
| Acoustic Velocity | 4.2 mm/μs |
| RF Bandwidth [-10 dB Return Loss] | 150 MHz(@ -10 dB Return Loss ) |
| Input Impedance | 50 Ω |
| Standing Wave Ratio | ≤1.3:1 |
| Insertion Loss | ≤4% |
| Single-Surface Reflectance | ≤1% |
| Extinction Ratio | ≥1000:1 |
| Polarization | At a 90° angle to the mounting plane |
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