| Top Acousto-Optic Devices |
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| 640 nm - 1100 nm, TeO2 Acousto-Optic Tunable Filter | |
Acousto-Optic Tunable Filter
from G&H
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| The AOTF 2986-01 from G&H is a TeO2 Acousto-Optic Tunable Filter that operates at a wavelength of 640 nm - 1100 nm. It has an active aperture of 2.5 mm and acoustic velocity of 0.68 mm/µs. This vertically or horizontally polarised AOTF has an RF frequency range of 48 MHz - 86 MHz and RF bandpass (FWHM) of 280 kHz (1060 nm). It uses patented side lobe suppression technology to achieve excellent out-of-band suppression. |
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| 1200 nm - 2000 nm, Acousto-Optic Tunable Filter for Spectroscopy Applications | |
Acousto-Optic Tunable Filter
from Sintec Optronics
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| The STBR-TEAF_-1.2-2.0_ from Sintec Optronics is a Tellurium Dioxide Acousto-Optic Tunable Filter that has a spectral range of 1200 nm - 2000 nm. It has a drive RF frequency of 50 MHz - 90 MHz and an optical aperture of 3 - 10 mm x 3 - 10 mm. This AOTF has a spectral resolution of 4 nm - 16 nm and is ideal for industrial or process control near-infrared (NIR) spectroscopy applications. |
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| 500 nm - 2000 nm, Femtosecond Laser Pulse Picker | |
Pulse Picker
from EKSMA Optics
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| The UP2-KTP-5.5 from EKSMA Optics is a Femtosecond Laser Pulse Picker that operates at a wavelength of 500 nm - 2000 nm. It delivers an average power of 2 W and has a maximum laser repetition rate of 100 MHz (for single pulse picking). This water-cooled pulse picker has an HV pulse duration of up to 5000 ns, and HV pulse rise & fall time below 7 ns. It has an operating rate of up to 1 MHz (driver) and a clear aperture of Ø5.5 mm. |
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| 500 nm - 1600 nm, Pulse Picker for Femtosecond Laser Systems | |
Pulse Picker
from APE Angewandte Physik & Elektronik GmbH
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| The pulseSelect Broadband from APE Angewandte Physik & Elektronik GmbH is a Pulse Picker that operates at a wavelength of 500 nm - 1600 nm. It has an input frequency of 72 MHz - 81 MHz and a contrast ratio above 500:1 (non-adjacent pulses) & 75:1 (adjacent pulses). This pulse picker has an output repetition rate from single-shot to 3 MHz and is ideal for femtosecond laser system applications. |
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| 532 nm TeO2 Acousto Optic Deflector for Micromachining Applications | |
Acousto-Optic Deflector
from L3Harris Technologies
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| The H-424 from L3Harris Technologies is a Linear Tellurium dioxide (TeO2) Acousto-Optic Deflector (AOD) that operates at a wavelength of 532 nm. It has a deflection bandwidth of 55 MHz - 95 MHz and nominal center frequency of 75 MHz. This AOD is ideal for applications such as predeflection, modulation, pointing adjustment & micromachining in visible & NIR laser systems. |
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| 1064 nm Acousto-Optic Mode Locker for Low Power Laser Application | |
Acousto-Optic Mode Locker
from Laser 2000
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| The FSML-50-20-BR-1064 from Laser 2000 is a Fused Silica Acousto-Optic Mode Locker that operates at a wavelength of 1064 nm. It has an active aperture of 3 mm x 3 mm and a carrier frequency of 50 MHz. This acousto-optic mode locker has a modulation rate of 3 dB bandwidth and is ideal for low-power lasers, analog light intensity modulation & digital switching on/off applications. |
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| 9.3/10.6 µm, Mid-Infrared Acousto-Optic Modulator | |
Acousto-Optic Modulator
from ISOMET
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| The M1396-G40L-7 from ISOMET is a Mid-Infrared Acousto-Optic Modulator that operates at a wavelength of 9.3 μm or 10.6 μm. It delivers an optical output power of up to 250 W and has a spectral range of 2.5 μm - 11 μm. This AOM has a single crystal germanium medium that produces acoustic waves with a velocity of 5.5 mm/µs and center frequency of 40 MHz. It has an active aperture area of 7 mm (H) x 14 mm (L). |
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| 1064 nm Quartz Crystal Acousto-Optic Q-Switch | |
Acousto-Optic Q-Switch
from Wavelength Opto-Electronic
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| The AOQS0001-QL080-015-1064 from Wavelength Opto-Electronic is a Quartz Crystal Acousto-Optic Q-Switch that operates at a wavelength of 1064 nm. It has an operating frequency of 80 MHz and active aperture of 1.5 mm. This AOQS operates within laser cavities to generate high-peak-power & short-pulse lasers by actively modulating the cavity's Q-factor through controlled loss of zero-order beams to achieve pulsing. |
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