Skip to main content

Acousto-Optic Modulators

Product information "Acousto-Optic Modulators"

Wavelength 5.5 µm-1090 nm; Rise / Fall Time 10-160 ns/mm; Active Aperture 0.1-9.6 mm; Operating Frequency 40-200 MHz; Optical Material Crystalline Quartz, Germanium, Tellurium Dioxide; Type IR, Mid-IR, Visible, UV

Acousto-optic modulators (AOM) allow the intensity of light to be controlled and modulated at rates that far exceed mechanical shutters, even up to 70 MHz. The AO modulators available from Gooch & Housego (G&H) are optimized for low scatter and high laser damage threshold. Rise time, modulation rate, beam diameter and power handling requirements of the application need to be understood in order to identify the best acousto-optic modulator and RF driver solution.
An acousto-optic modulator (AOM) uses sound waves within a crystal to create a diffraction grating. As the power of the applied RF signal is varied, the amount of diffracted light varies proportionally. Modulators can be used like a shutter (cycling light on and off at a set frequency), or as a variable attenuator (controlling the intensity of transmitted light dynamically).
Contact our sales team to identify the best RF driver for your specific application

Applications: Heterodyne Interferometry; Intensity Levelling; Intensity Modulation; Laser Cooling; Laser Doppler Velocimetry; Laser Doppler Vibrometry (LDV); Laser Linewidth Measurements; LIDAR; Marking; Material Processing; Micromachining; Printing; Via Drilling

Series Wavelength Rise / Fall Time Active Aperture Operating Frequency Optical Material Type Downloads
I-M0XX-XC11B76-P5-GH105 5.5 µm 120 ns/mm up to 9.6 mm 40.68 - 60 MHz Germanium N/A Datasheet Driver  
I-M050-10C11V41-P3-GH75 9.4 µm 120 ns/mm up to 9.6 mm 40/60 MHz Germanium Mid-IR Datasheet Driver  
I-M041-XXC11XXX-P5-GH77 10.6 µm, 9.4 µm 120 ns/mm up to 9.6 mm 40.68 MHz Germanium Mid-IR Datasheet Driver  
AOMO 3200-1220 257 nm 10 ns 0.25 mm 200 MHz Crystalline Quartz UV Datasheet Driver  
I-M110-3C10BB-3-GH27 AOM 300 - 400 nm 113 ns/mm 3 mm 110 MHz Crystalline Quartz UV Datasheet Driver  
I-M110-2C10B6-3-GH26 AOM 400 - 540 nm 113 ns/mm 2 mm 110 MHz Crystalline Quartz Visible Datasheet Driver  
AOMO 3080-125 415 - 900 nm 25 ns 2 mm 80 MHz Tellurium Dioxide Visible Datasheet Driver Driver
AOMO 3080-120 440 - 850 nm 34 ns 1 mm 80 MHz Tellurium Dioxide Visible Datasheet Driver  
AOMO 3110-120 440 - 850 nm 18 ns 0.6 mm 110 MHz Tellurium Dioxide Visible Datasheet Driver  
AOMO 3100-125 440 - 850 nm 160 ns 1.5 mm 100 MHz Tellurium Dioxide Visible Datasheet Driver Driver
AOMO 3110-121 442 - 488 nm 18 ns 0.6 mm 110 MHz Tellurium Dioxide Visible Datasheet Driver  
AOMO 3200-120 442 - 488 nm 13 ns 0.45 mm 200 MHz Tellurium Dioxide Visible Datasheet Driver  
AOMO 3200-121 442 - 488 nm 18 ns 0.32 nm 200 MHz Tellurium Dioxide Visible Datasheet Driver  
AOMO 3200-125 470 - 690 nm 160 ns 1.5 mm 200 MHz Tellurium Dioxide Visible Datasheet Driver Driver
AOMO 3200-124 780 - 850 nm 10 ns 0.32 mm 200 MHz Tellurium Dioxide IR Datasheet Driver  
AOMO 3080-122 780 - 850 nm 25 ns 1 mm 80 MHz Tellurium Dioxide IR Datasheet Driver  
AOMO 3200-1113 870 - 1250 nm 10 ns 0.1 mm 200 MHz Tellurium Dioxide IR Datasheet Driver  
I-M041-2.5C10G-4-GH50 AOM 1030 - 1064 nm 113 ns/mm 2.5 mm 40.68 MHz Crystalline Quartz IR Datasheet Driver  
I-M080-2C10G-4-AM3 AOM 1030 - 1064 nm 113 ns/mm 2 mm 80 MHz Crystalline Quartz IR Datasheet Driver  
AOMO 3110-197 1030 - 1090 nm 18 ns 1.25 mm 110 MHz Tellurium Dioxide IR Datasheet Driver  
Manufacturer "Gooch & Housego"
Related links of the manufacturer

Similar products

Acousto-Optic Frequency Shifters
Wavelength 415-1550 nm; Type Visible, IR; Operating Frequency 40-200 MHz; Active Aperture 1.5-6 mm; Optical Material Tellurium Dioxide Transmission through an acousto-optic (AO) device causes the input light to experience a frequency shift equal to the RF drive frequency. The acousto-optic frequency shifters (AOFS) from Gooch & Housego (G&H) are optimized for the needs of applications like interferometry, with the ability to achieve high extinction ratio between modes.The product line includes standard products with frequency shifts of over 300 MHz and integrated low-power AOFS modules in which the RF driver has been built into the housing. Frequency shifters for specific application, including frequency shifts up to 600 MHz, can be customized on request. The frequency shifters are manufactured using high quality tellurium dioxide (TeO2), grown and polished in-house, for lowest insertion loss and excellent power handling. Standard AOFS products are offered for wavelengths in the visible and NIR for use with fundamental and doubled Argon Ion, Nd:YAG, He:Ne, diode, dye, and Ti:Sapphire lasers. With standard frequency shifts of over 300 MHz and custom frequency shifts up to 600 MHz, as well as models for double-pass configurations, the frequency shifters match most research and industrial needs. Frequency shifters are highly efficient acousto-optic devices, requiring very low drive power to achieve the desired frequency shift. G&H’s AOFS designs typically use the slow shear mode, resulting in slow rise time, but requiring minimal power consumption (typically < 100 mW power draw). This allows to often package the driver with the AOFS for a compact and power-efficient solution. Applications: Interferometry; Laser Cooling; Laser Doppler Velocimetry; Laser Doppler Vibrometry (LDV); Optical Heterodyne Detection Series Wavelength Type Operating Frequency Active Aperture Optical Material Downloads AOMO 3080-125 415 - 900 nm Visible 80 MHz 2 mm Tellurium Dioxide Datasheet Driver Driver AOMO 3100-125 440 - 850 nm Visible 100 MHz 1.5 mm Tellurium Dioxide Datasheet Driver Driver AOMO 3200-125 470 - 690 nm Visible 200 MHz 1.5 mm Tellurium Dioxide Datasheet Driver Driver I-FS040-1.5S2C-3-GH83 532 nm Visible 40 MHz 1.5 mm Tellurium Dioxide Datasheet Driver   I-FS040-1.5S2C-1-GH66 532 nm Visible 40 MHz 1.5 mm Tellurium Dioxide Datasheet     I-FS040-2S2E-1-GH66 630 - 690 nm Visible 40 MHz 2 mm Tellurium Dioxide Datasheet     AOFS I-FS040-2S2E-3-OL3 630 - 690 nm Visible 40 MHz 2 mm Tellurium Dioxide Datasheet Driver   I-FS080-3S2E-3-LG5 632.8 nm Visible 80 MHz 3 mm Tellurium Dioxide Datasheet Driver   AOFS 4040-191 633 - 1064 nm IR 40 MHz 2 x 6 mm Tellurium Dioxide Datasheet Driver   I-FS040-2S2J-3-GH53 1550 nm IR 40 MHz 2 x 4 mm Tellurium Dioxide Datasheet Driver  
Product number: SW11425
Manufacturer:

Acousto-Optic Mode Lockers
Type IR; Wavelength 700-1100 nm; Operating Frequency 38-80 MHz; Active Aperture 2-3 mm; Window Type Brewster, AR coated; Optical Material Fused Silica; Acousto-optic mode lockers (AOML) modulate the loss within a laser cavity at its resonant frequency, effectively “locking” the phase of the longitudinal modes to generate very narrow laser pulses of high intensity. Gooch & Housego’s mode lockers for Nd:YAG, Nd:YLF, Ti:Sapphire and Argon Ion lasers can modulate at up to 200 MHz, yielding near-theoretical mode locked laser pulse widths. Antireflection (AR) coated and Brewster angle options are available. Customized one-off mode lockers can be designed for demanding scientific and OEM applications.The acousto-optic mode lockers from Gooch & Housego are manufactured using high quality fused silica, polished and fabricated in-house to ensure high quality and reliability. >99% transmission at 1064 nm is achieved by using a durable in-house antireflection V-coat. Low scatter and tight quality controls ensure that every mode locker is capable of handling high peak laser power over the long term without damage. The standard mode lockers include operating frequencies from 38 MHz to 80 MHz. The more modes are locked together in phase, the shorter the pulse. G&H’s standing wave mode lockers can obtain near theoretical mode locked laser pulse widths, with industry-leading transmission performance. The high-Q mode lockers can be used for Nd:YAG, Nd:YLF, Ti:Sapphire and Argon ion lasers at near infrared wavelengths to achieve picosecond and femtosecond length pulses at repetition rates of up to 200 MHz. The short pulses generated are often used in applications like nonlinear optics, optical data storage, femtosecond micromachining and multiphoton microscopy. High repetition rates are often desired for scientific applications, including those using optical heterodyne detection for spectroscopy, LIDAR or telecommunications. RF driver selection impacts mode locking system performance. Active temperature control of the acoustic resonator can assist in controlling resonant frequency such that resonance at the precise frequency of the driver's oscillator can be maintained. We can assist choosing the right driver for your application. Contact our sales team to identify the best RF driver for your specific application.Applications: Femtosecond Micromachining; fs/ps Lasers (Nd:YAG, Nd:YLF, Ti:Sapphire, Argon Ion); LIDAR; Multiphoton Microscopy; Nonlinear Optics; Optical Data Storage; Optical Heterodyne Detection For Spectroscopy; Telecommunications Series Type Wavelength Operating Frequency Active Aperture Window Type Optical Material Downloads 12041-3-BR-TE AOML IR 700 - 1100 nm 41 MHz 2 mm Brewster Fused Silica Datasheet 12080-3-TE AOML IR 1064 nm 80 MHz 3 mm AR coated Fused Silica Datasheet 12038-3-TE AOML IR 1064 nm 38 MHz 3 mm AR coated Fused Silica Datasheet 12041-3-TE AOML IR 1064 nm 41 MHz 3 mm AR coated Fused Silica Datasheet 12050-3-TE AOML IR 1064 nm 50 MHz 3 mm AR coated Fused Silica Datasheet 12038-3-BR-TE AOML IR 700 - 1100 nm 38 MHz 2 mm Brewster Fused Silica Datasheet 12050-3-BR-TE AOML IR 700 - 1100 nm 50 MHz 2 mm Brewster Fused Silica Datasheet 12080-3-BR-TE AOML IR 700 - 1100 nm 80 MHz 2 mm Brewster Fused Silica Datasheet
Product number: SW11428
Manufacturer:

Acousto-Optic Multi-Channel Modulators
Type UV, Visible; Wavelength 350-850 nm; Number of Channels 4-24; Rise / Fall Time 7-23 ns; Active Aperture 0.18-0.5 mm; Operating Frequency 125-350 MHz; Acousto-optic multi-channel modulators (AOMC) allow multiple beams to be modulated or deflected independently by integrating an array of transducers with a single acousto-optic crystal. The AO multi-channel modulators manufactured by Gooch & Housego (G&H) feature reliable operation and high performance with minimized crosstalk thanks to proprietary optical and electrical designs to allow concurrent operation of up to 48 channels for modulation, and up to 8 channels for beam deflection. Multi-channel modulators are most often used for high speed applications like micromachining and direct-write lithography, as each beam can be modulated independently. They are also used to increase throughput when writing large media by writing multiple beams at the same time. A typical multi-channel modulator has parallel beams as input, each operated on by a different transducer to modulate its intensity. Available models have 2 to 48 channels for UV through NIR wavelengths, with rise times as short as 7 ns for apertures < 1 mm. Multi-channel RF drivers are available with analog or digital modulation.High laser damage threshold is achieved using low-scatter materials inspected to rigorous quality standards. We draw our own tellurium oxide (TeO2) and source high quality fused silica and crystalline quartz to ensure low insertion loss and excellent optical power handling.Applications: Marking; Material Processing; Micromachining; Printing Series Type Wavelength Number of Channels Rise / Fall Time Active Aperture Operating Frequency Optical Material Downloads AOMC 3160-8 UV 364 nm 8 21 ns 0.18 mm 160 MHz Fused Silica Datasheet AOMC 125-24 UV 350 - 365 nm 24 23 ns 0.5 mm 125 MHz Crystalline Quartz Datasheet AOMC 220-5 UV 413 nm 5 16 ns 0.24 mm 220 MHz Crystalline Quartz Datasheet AOMC 220-4 UV 350 - 365 nm 4 16 ns 0.24 mm 190 - 250 MHz Crystalline Quartz Datasheet AOMC 300-5 UV 413 nm 5 10 ns 0.2 mm 300 MHz Crystalline Quartz Datasheet AOMC 3350-6 Visible 350 - 850 nm 6 7 ns 0.33 mm 350 MHz Tellurium Dioxide Datasheet
Product number: SW11426
Manufacturer:

Acousto-Optic Q-Switches
Wavelength 1030-2100 nm; Active Aperture 1-8 mm; Operating Frequency 24-80 MHz; Optical Material Crystalline Quartz, Fused Silica; Type Water Cooled, Conduction CooledAn acousto-optic Q-switch (AOQS) works within a laser cavity to generate high intensity, pulsed light by actively controlling the Q-factor (loss) of the cavity. The acousto-optic Q-switches available from Gooch & Housego (G&H) are rugged, reliable and long-lasting. The product offering includes low insertion loss and highly efficient acousto-optic Q-switches capable of handling very high peak power. Particular attention is used to match the cavity length, repetition rate, wavelength, beam diameter, polarization state and output power of a laser to the best acousto-optic Q-switch solution.G&H offers off-the-shelf solutions for polarized or unpolarized lasers at near infrared wavelengths. G&H can accommodate large lamp pumped multimode laser beam diameters (up to 8 mm) as well as small compact diode pumped beam diameters (< 1 mm) with both water and conduction cooling. Specialized designs meet unique needs such as ultra-high single pass loss (up to 96%), high switching speeds and premium pulse-to-pulse stability.A full line of RF drivers designed specifically for Q-switching is available, with rapid fall times, tight synchronization, operation in either fixed or variable mode and advanced capabilities like first pulse suppression or multichannel operation to drive multiple Q-switches within the same cavity.Applications: Laser Marking; Lithography; Material Processing; Medical Surgery; Micromachining Series Wavelength Active Aperture Operating Frequency Optical Material Type Downloads I-QS080-1C10G-8-GH28 Q-Switch 1030 - 1064 nm 1 mm 80 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver Super Q-Switch 1064 nm 1.6, 2, 3, 4, 5, 6.5 mm 24, 27.12 MHz Crystalline Quartz Water Cooled Datasheet Driver Industry Standard AO Q-Switch 1064 nm 1.6, 2, 3, 4, 5, 6.5, 8 mm 24, 27.12, 40.68, 68 MHz Fused Silica Water Cooled Datasheet Driver Stallion Q-Switch 1064 nm 1.6, 2, 3, 4, 5, 6.5, 8 mm 24, 27.12, 40.68, 68 MHz Fused Silica Water Cooled Datasheet Driver VHE AO Q-Switch 1064 nm 1.6, 2.5, 2, 3, 4 mm 68 MHz Crystalline Quartz Water Cooled Datasheet   I-QS041-1.8C10G-4-GH21 AO Q-Switch 1064 nm 1.8 mm 40.68 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver I-QS080-1C10G-4-GH25 Q-Switch 1064 nm 1 mm 80 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver I-QS080-0.5C10G-8-GH48 Q-Switch 1064 nm 0.5 mm 80 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver I-QS080-1C10H-4-OS14 1319 - 1342 nm 1 mm 80 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver I-QS027-4S4V2-x5-ST1 Q-Switch 1550 nm 4 mm 27.12 MHz Fused Silica Water Cooled Datasheet   I-QS041-2C10V5-4-HC1 Q-Switch 1900 - 2100 nm 2 mm 40.68 MHz Crystalline Quartz Conduction-Cooled Datasheet Driver I-QS041-5C10V5-x5-ST3 Q-Switch 2100 nm 5 mm 40.68 MHz Crystalline Quartz Water Cooled Datasheet Driver    
Product number: SW11427
Manufacturer:

AOM Fiber-coupled Acousto-optic Modulators
1030 to 1064 nm; Bandwidth ±10 dB; Pigtail Style; Fiber Type SM, PM; Supersonic Wave Frequency 80, 100 MHz LightComm Technology’s AOM series of fiber coupled acousto-optic modulators is designed for pulsed fiber laser/amplifier system applications. The AOM is installed in the fiber laser cavity, laser pulses can be obtained by modulating the AOM with a TTL signal. The AOM series is available with single mode (SM) and polarization maintaining fibers. Customized solutions are available on request to meet the specific demands of your modulator solution – get in touch with AMS Technologies to discuss your requirements. Key Features: Low Insertion Loss Compact Package Stable and Reliable Performance Customized Configurations Available Operating Wavelength: 1030 to 1064 nm Bandwidth: ±10 dB Supersonic Wave Frequency: 80, 100 MHz Fiber Type: Single Mode (SM), Polarization Maintaining (PM) Applications: Fiber Amplifiers; Fiber Lasers
Product number: SW11017
Manufacturer:

Fiber-Coupled Acousto-Optic Modulators
Wavelength 450-200 nm; Pigtail Type SM, PM; Rise / Fall Time 6-100 ns; Operating Frequency 40-300 MHz; Fiber-coupled acousto-optic modulators (FCAOM) offer a robust solution for amplitude modulation of fiber lasers, allowing direct control of the timing, intensity, and temporal shape of the laser output. Gooch & Housego’s (G&H) Fiber-Q® modulators offer high extinction ratio, low insertion loss and excellent stability in both polarization maintaining (PM) and non-PM formats at modulation frequencies up to 80 MHz for visible and infrared wavelengths. Built for reliability, the Fiber-Q® series of products features a rugged hermetic design in a compact, low-profile package, ideal for ease of integration into all-fiber and OEM systems, including medical laser systems.Each Fiber-Q® acousto-optic modulator requires an RF driver to generate the RF signal creating the acoustic wave within the embedded AO crystal. Modulation of the beam through the Fiber-Q will depend upon the frequency and intensity of the applied RF signal. Contact our sales team to identify the best RF driver for your specific application, taking into consideration the type of modulation required (digital or analog) as well as any specific pulse shaping needs.A fiber-coupled acousto-optic modulator (FCAOM) can directly control the temporal characteristics of the active output from a fiber laser, offering a wider variety of pulse shapes. As a byproduct of the acousto-optic effect, light passing through the first order diffraction mode of a fiber-coupled modulator also experiences a frequency shift and beam deflection. This allows the Fiber-Q® products to be used for more than just modulation, resulting in applications outside the laser such as optical heterodyne interferometry. G&H’s fiber optic acousto-optic modulators are designed for low insertion loss, high extinction ratio and excellent return loss. Typical optical performance for the Fiber-Q® series includes: Insertion loss: as low as 2 dB, depending on model Extinction ratio: 50 dB Return loss: 40 dB Polarization extinction ratio: 20 dB (for polarization-maintaining models) G&H has developed the first devices for visible wavelengths from 397 nm to 780 nm to meet the needs of sensing and quantum technology applications. The fast switch rate Fiber-Q® devices enable efficient, high speed optical pulse picking at infrared wavelengths for all-fiber laser systems. Most devices are also offered in 3-port configurations.Applications: Industrial Lasers; Sensing; Scientific Research; Telecommunication; Quantum Technology; Optical Heterodyne Interferometry; Microscopy; Flow Cytometry Series Product Code Wavelength Pigtail Type Rise / Fall Time Operating Frequency Downloads Fiber-Q 1060 nm 150 MHz Non-Hermetic Fiber-Coupled AOM S-M150-0.4C2G-3-F2S 1060 nm SM 30 ns 150 MHz Datasheet Datasheet Datasheet Driver Fiber-Q 1060 nm 200 MHz Non-Hermetic Fiber-Coupled AOM S-M200-0.1C2G-3-F2P 1060 nm SM 10 ns 200 MHz Datasheet  Driver   Driver  Driver Fiber-Q 450 nm 200 MHz S-M200-0.4C2A-3-F2P, S-M200-0.4C2A-3-F2S 450 nm PM, SM 25 ns 200 MHz Datasheet  Driver   Driver  Driver  Fiber-Q 532 nm 200 MHz S-M200-0.4C2C-3-F2P, S-M200-0.4C2C-3-F2S 532 nm PM, SM 25 ns 200 MHz Datasheet  Driver  Driver     Fiber-Q 633 nm 200 MHz Fiber Coupled AOM S-M200-0.4C2E-3-F2P, S-M200-0.4C2E-3-F2S 633 nm PM, SM 25 ns 200 MHz Datasheet  Driver   Driver    Fiber-Q PM 1550 nm, 40 MHz (AMTIR) T-M040-0.5C8J-3-F2P 1550 nm PM 100 ns 40 MHz Datasheet  Driver  Driver  Driver  Fiber-Q 1550 nm 40 MHz (AMTIR) T-M040-0.5C8J-3-F2S 1550 nm SM 100 ns 40 MHz Datasheet Datasheet Datasheet Driver  Fiber-Q PM 2000 nm 80 MHz Hermetic Fiber Coupled AOM T-M080-0.3C2Z-3-F2P 2000 nm PM 100 ns 80 MHz Datasheet  Driver      Fiber-Q 2000 nm 80 MHz Hermetic Fiber Coupled AOM T-M080-0.3C2Z-3-F2S 2000 nm SM 100 ns 80 MHz Datasheet  Driver     Fiber-Q PM 1550nm 80MHz Hermetic Fiber-Coupled AOM T-M080-0.4C2J-3-F2P 1550 nm PM 35 ns 80 MHz Datasheet  Driver     Fiber-Q 1550 nm 80 MHz Hermetic Fiber Coupled AOM T-M080-0.4C2J-3-F2S 1550 nm SM 35 ns 80 MHz Datasheet  Driver     PM Fiber-Q Polarization Maintaining 1550 nm Hermetic Fiber Coupled Acousto-Optic Modulator, 80 MHz (Low Power Consumption) T-M080-0.5C8J-3-F2P 1550 nm PM 100 ns 80 MHz Datasheet  Driver      Fiber-Q 1550 nm Hermetic Fiber Coupled Acousto-Optic Modulator, 80 MHz (Low Power Consumption) T-M080-0.5C8J-3-F2S 1550 nm PM 100 ns 80 MHz Datasheet  Driver      Fiber-Q PM 1550 nm 110 MHz Hermetic Fiber Coupled AOM T-M110-0.2C2J-3-F2P 1550 nm PM 25 ns 110 MHz Datasheet Driver       Fiber-Q 1550 nm 110 MHz Hermetic Fiber Coupled AOM T-M110-0.2C2J-3-F2S 1550 nm SM 25 ns 110 MHz Datasheet  Driver      Fiber-Q PM 1060 nm 150 MHz Hermetic Fiber Coupled AOM T-M150-0.4C2G-3-F2P 1060 nm PM 30 ns 150 MHz Datasheet  Driver     Fiber-Q 1060 nm 150 MHz Hermetic Fiber-Coupled AOM T-M150-0.4C2G-3-F2S 1060 nm SM 30 ns 150 MHz Datasheet  Driver     Fiber-Q, 780 nm, 150 MHz Fiber Coupled AOM T-M150-0.5C2W-3-F2P, T-M150-0.5C2W-3-F2S 780 nm PM, SM 50 ns 150 MHz Datasheet  Driver     Fiber-Q PM 1060 nm 200 MHz Hermetic Fiber Coupled AOM T-M200-0.1C2G-3-F2P 1030 - 1090 nm PM 10 ns 200 MHz Datasheet  Driver Driver     Fiber-Q 1060 nm 200 MHz Fiber Coupled AOM T-M200-0.1C2G-3-F2S 1060 nm SM 10 ns 200 MHz Datasheet  Driver  Driver  Driver  Fiber-Q PM 1550 nm 200 MHz Hermetic Fiber-Coupled AOM T-M200-0.1C2J-3-F2P 1550 nm PM 10 ns 200 MHz Datasheet  Driver Driver     Fiber-Q 1550 nm 200 MHz Hermetic Fiber-Coupled AOM T-M200-0.1C2J-3-F2S 1550 nm SM 10 ns 200 MHz Datasheet  Driver Driver     Fiber-Q 2000 nm (2µm) 250 MHz Fiber Coupled AOM T-M250-0.3C16Z-3-F2P 2000 nm PM 20 ns 250 MHz Datasheet  Driver      Fiber-Q 1060 nm 300 MHz Hermetic Fiber Coupled AOM T-M300-0.1C2G-3-F2P, T-M300-0.1C2G-3-F2S 1060 nm PM, SM 6 ns 300 MHz Datasheet  Driver      Fiber-Q 1550 nm Fiber Coupled Acousto-Optic Modulator T-M300-0.1C16J-3-F2P 1550 nm PM 6 ns 300 MHz Datasheet Driver      
Product number: SW11440
Manufacturer:

MBC-CHIP Chip-Size, Single-Function Modulator Bias Controller
Chip Style; Input Signal Current 0.8-80 µA; Typ. Locking Accuracy 1°; Bias Voltage -10-10 V; Pilot Tone Frequency 9.8 kHz; Dimensions 45.7x20.3x12.7 mm OZ Optics’ MBC-CHIP chip-size modulator bias controller is a single-function, chip-size, OEM version of the MBC family of modulator bias controllers. It is designed especially for digital system applications. The small size of the board makes it easy to be integrated into the system. This chip-size MBC is designed to lock the working point of the modulator at positive slope quadrature (quad+), negative slope quadrature (quad-), null or peak points of its characteristic curve respectively. The locking mode and slope has to be specified before ordering. The Chip size MBC is designed to use the built-in PD of the modulator but the user may also use an external PD by soldering it to the MBC-Chip. Key Features: Single-function Unit With Q+/Q-, Null/Peak Options Low Profile: 45.7 x 20.3 x 12.7 mm Access for External Photodetector Input Signal Current: 0.8 µA to 80 µA Locking Accuracy: 1° Typ., 3° Max. DC Bias Voltage: -10 V to +10 V Pilot Tone Frequency: 9.8 kHz Pilot Tone Amplitude Range: 0 mV to 300 mV VC DC Voltage: -10 V to +10 V Applications: Modulator Bias Control in Digital Systems; Locking the Modulator’s Working Point at Positive Slope Quadrature (quad+), Negative Slope Quadrature (quad-), Null or Peak Points of its Characteristic Curve
Product number: SW11940
Manufacturer:

Customers also viewed

Mounted Precision Molded Aspheric Lenses
Focal Length 1.50-22.00 mm; Numerical Aperture 0.13-0.71; Design Wavelength 405-7800 nm; Outer Diameter 6.24-14.25 mm; Thread MT6, MT8, MT9, MT12, MT14 With 27 of GH Optics’ standard precision molded aspheric lenses mounted into five different stainless steel lens holders, this series of components allow for very easy assembly. Our mounted precision molded aspheric lenses feature MT6, MT8, MT9, MT12 or MT14 threads for screwing the components into your systems, but they can also be soldered or welded to suitable structures in the required position. GH Optics’ series of mounted precision molded glass aspheric lenses can be used for applications in the visible (VIS) and infrared (IR) wavebands, such as small beam collimation, focusing, and fiber coupling. In these applications, aspheric lenses avoid spherical aberrations known from spherical lenses and can therefore reduce the complexity of both the design process and the resulting optical system. While the cost and effort involved in the traditional production of aspheric lenses has often prevented the use of this type of lens in cost-sensitive applications, GH Optics manufactures affordable aspheric lenses with high, reproducible quality by molding glass preforms in molds of high precision. On request, most aspheric lenses in our portfolio can be mounted into a custom assembly specified by the customer. For large-volume applications we recommend to contact your regional AMS Technologies office, so that we can tailor a solution based on your technical needs. Three types of glass are available for our series of mounted precision molded aspheric lenses for visible and NIR wavelenghts, all RoHS compliant: Lens Series Glass Type Refractive Index Abbe Number CTE dn/dT RoHS Compliance MD D-ZK3 1.586 60.71 7.6×10-6/°C 3.2×10-6/°C yes ME D-ZLaF52La 1.806 40.79 6.9×10-6/°C 6.5×10-6/°C yes MG D-LaK6 1.690 52.65 6.9×10-6/°C 6.5×10-6/°C yes   For our mounted precision molded infrared aspheric lenses, two types of chalcogenide glass are available, comparable to infrared glass of other leading brands in the market and featuring high transmission as well as RoHS compliance:  Lens Series Glass Type Glass Material Refractive Index @10 µm Abbe Number @10 µm CTE dn/dT RoHS Compliance M2 GH2 Ge28Sb12Se60 2.6044 93.63 142×10-7/°C 70.4×10-6/°C yes M6 GH6 As40Se60 2.7775 137.71 209×10-7/°C 31.3×10-6/°C yes   Mounted precision molded aspheric lenses for visible and NIR wavelengths can be coated with a range of visible and NIR coatings, including four standard AR coatings (VA, VB, VC, VQ) featuring average reflectance values of ≤0.6%, ≤0.5%, or even ≤0.25%, for wavelength ranges of 380 nm to 700 nm, 600 nm to 1100 nm, 1050 nm to 1650 nm, or 1300 nm to 1700 nm respectively. Other customized coatings like HD (High Density) or SWB (Short Wave Blocking) are available on request. Lens Code Thread Outer Diameter (OD) Effective Focal Length (EFL) Lens Numerical Aperture (NA) Clear Aperture (CA) Design Wavelength (DW) MD1560 MT6 6.24 mm 1.50 mm 0.58 1.60 mm 780 nm MF2570 MT8 8.24 mm 2.50 mm 0.66 3.30 mm 405 nm ME2860 MT8 8.24 mm 2.80 mm 0.64 3.60 mm 830 nm MD3170 MT9 9.24 mm 3.10 mm 0.68 5.00 mm 830 nm MD4060 MT9 9.24 mm 4.00 mm 0.64 5.10 mm 685 nm MG4060 MT9 9.24 mm 4.00 mm 0.60 4.80 mm 408 nm MD4530 MT6 6.24 mm 4.50 mm 0.30 2.70 mm 635 nm MD4540 MT8 8.24 mm 4.50 mm 0.40 3.70 mm 980 nm ME4560 MT9 9.24 mm 4.50 mm 0.55 5.07 mm 780 nm MD4650 MT9 9.24 mm 4.60 mm 0.54 4.80 mm 655 nm MD5020 MT6 6.24 mm 5.00 mm 0.15 1.60 mm 1550 nm MD5560 MT9 9.24 mm 5.50 mm 0.58 6.00 mm 635 nm MD6020 MT8 8.24 mm 6.00 mm 0.21 2.50 mm 1550 nm MD6230 MT8 8.24 mm 6.20 mm 0.30 3.70 mm 635 nm ME6240 MT9 9.24 mm 6.20 mm 0.40 5.00 mm 780 nm ME7530 MT9 9.24 mm 7.50 mm 0.30 4.54 mm 780 nm MD8050 MT12 12.22 mm 8.00 mm 0.50 8.00 mm 780 nm MD9630 MT9 9.24 mm 9.60 mm 0.27 5.20 mm 635 nm MD9930 MT9 9.24 mm 9.90 mm 0.27 5.20 mm 650 nm MDA050 MT14 14.25 mm 10.00 mm 0.51 10.00 mm 635 nm MDA130 MT9 9.24 mm 11.00 mm 0.25 5.50 mm 635 nm MDA320 MT9 9.24 mm 13.00 mm 0.20 5.20 mm 633 nm MDA520 MT9 9.24 mm 15.30 mm 0.16 5.00 mm 785 nm MDA820 MT9 9.24 mm 18.40 mm 0.15 5.50 mm 785 nm MDB210 MT9 9.24 mm 22.00 mm 0.13 5.50 mm 670 nm M23070 MT9 9.24 mm 3.00 mm 0.71 5.00 mm 7.8 µm M24060 MT9 9.24 mm 4.00 mm 0.56 5.00 mm 4.0 µm    Key Features: Stainless Steel Holder Assembly With Glue Threaded Interface for Easy Assembly Rapid Prototype Focal Length: 1.50 mm to 22.00 mm Lens Numerical Aperture: 0.13 to 0.71 Design Wavelength: 405 nm to 7.8 µm Assembly Outer Diameter: 6.24 mm, 8.24 mm, 9.24 mm, 12.22 mm, 14.25 mm Thread: MT6, MT8, MT9, MT12, MT14 Applications: Laser; Telecom; Medical; Imaging; And Many More  
Product number: SW11895
Manufacturer:

PK 300-24 Cabinet Cooler - 280W Cooling Capacity - TEC based
The PK 300 is an eco-friendly thermoelectric cooler that utilizes advanced Peltier technology. It is maintenance-free, requiring no refrigerants or filter mats, and features separate internal and external air circuits. With an IP67 protection rating, this compact device can operate in any position and is ideal for various applications. Accessories such as power supplies and temperature controllers are available to enhance its functionalityVoltage: 24 VDcCooling capacity: 280 WAmperage 15 ATemperature range: -10 - +60 °CHousing: stainless steelProtection class: IP67
Product number: C009273-6
Manufacturer:

€1,692.90*
TPA Tapered Lasers/Amplifiers
650-980 nm; Gain Width 6-30 nm; Input Power 10-80 mW; Output Power 250-3000 mW; Forward Current 750-4500 mA; Amplification 10-23 dBToptica eagleyard’s TPA series of tapered amplifiers (TPA) are semiconductor optical amplifiers combining excellent beam quality with highest output power from a single emitter. Their monolithic design comprises a single mode ridge waveguide section with a tapered structure. These components are the first choice for master oscillator power amplifier setups, inheriting all spectral properties of a seed source such as a DFB laser or an ECDL built with a gain chip.Tapered Amplifiers are improving poor signal to noise ratios wherever generating spectral and beam profile properties comes at the price of an attenuated power level. They are of great help in gathering deepest knowledge about hidden processes not only in the micro-world. They are enabling the realization of complex scientific equipment.Key Features:Tapered Amplifiers for Single Frequency LasersAR-coated Front and Rear FacetWavelength Range: 650 to 980 nmOutput Power: 0.25 to 3 W CWExcellent Beam PropertiesPackages: C-Mount (2,3,4 mm), ButterflyProductWavelengthMax. Power LevelPackageTuning RangeTPA-0650-00250-2007-CMT02-0000650 nm250 mWC-Mount 2 mm650-655 nmTPA-0670-00500-2004-CMT02-0000670 nm500 mWC-Mount660-675 nmTPA-0670-00500-3006-BTU02-0000670 nm1 WStandard Butterfly660-675 nmTPA-0765-01500-3006-CMT03-0000765 nm1500 mWC-Mount 3 mm755-770 nmTPA-0765-01500-3006-BTU02-0000 765 nm 1,5 W Standard Butterfly760-773 nm TPA-0780-01000-3006-CMT03-0000780 nm1000 mWC-Mount 3 mm770-790 nmTPA-0780-03000-4006-CMT04-0000780 nm3000 mWC-Mount 4 mm770-790 nmTPA-0780-03000-4006-BTU02-0000780 nm3 WStandard Butterfly775-790 nmTPA-0795-02000-4006-BTU02-0000795 nm2 WStandard Butterfly790-805 nmTPA-0795-02000-4006-CMT04-0000795 nm2000 mWC-Mount 4 mm790-805 nmTPA-0808-02000-4006-CMT04-0000808 nm2000 mWC-Mount 4 mm802-810 nmTPA-0830-01000-4006-CMT04-0000830 nm1000 mWC-Mount 4 mm830-840 nmTPA-0845-02000-4006-CMT04-0000845 nm2000 mWC-Mount 4 mm835-855 nmTPA-0850-00500-3006-CMT03-0000850 nm500 mWC-Mount 3 mm848-855 nmTPA-0850-02000-4006-BTU02-0000850 nm2 WStandard Butterfly830-860 nmTPA-0850-02000-4006-CMT04-0000850 nm2000 mWC-Mount 4 mm848-855 nmTPA-0870-00500-3006-CMT03-0000870 nm500 mWC-Mount 3 mm868-880 nmTPA-0895-02500-4006-BTU02-0000895 nm2,5 WStandard Butterfly894-913 nmTPA-0960-02000-4006-CMT04-0000960 nm2000 mWC-Mount 4 mm950-970 nmTPA-0970-02500-4006-CMT04-0000970 nm2500 mWC-Mount 4 mm955-985 nmTPA-0980-00500-3006-CMT03-0000980 nm500 mWC-Mount 3 mm965-985 nmApplications: Bose/Einstein-, Cs-, Rb-, K-and Raman Spectroscopy; Atomic Co-magnetometers; High-precision Angular Velocity Sensing; Fundamental Physics Tests Even at Very Large Scale
Product number: SW10677
Manufacturer:

FFW-X SM WDMs
Gooch & Housego’s FFW-X wavelength division multiplexers (WDMs) are single mode (SM) optical fiber components and modules. They enable two or three wavelengths to be combined or separated. For the FFW-X series, Gooch &Housego (G&H) utilizes low-loss fused fiber technology – no light leaves the fiber and therefore no alignment is required and there are no unwanted reflections. Furthermore, the output fiber pigtails may be directly integrated into beam delivery systems. These high-performance parts are available in many wavelength configurations (including a duplexing version), fiber and connector options, with standard as well as subminiature packages. They can therefore be readily specified in a wide variety of applications, enabling rapid design cycles and new project builds. Visible Wavelength Combiners:Designed for applications in display systems, sensors and biomedical equipment, G&H’s FFW-xxxxxxxxx single mode visible wavelength fused fiber combiners enable any two or three primary colors in the visible wavelength region to be combined or separated. Visible wavelength combiners are available for either two (red/green, blue/green, red/blue light) or three wavelengths, providing full RGB operation and enabling full color displays. All variants are available on a custom basis, so please contact AMS Technologies to discuss your specific requirements. Near Infrared WDMs:Designed for applications in fiber laser, sensing, biomedical, military and avionics, the FFW-xxxxxxxxx near infrared WDMs enable the low-loss combining or splitting of a pair of wavelengths within the 700 nm to 1199 nm region. G&H can rapidly produce such custom WDMs, with typical minimum wavelength separation of 50 nm. Specific applications could include combining two sensor wavelengths onto one fiber, splitting laser harmonics, or combining wavelengths in fiber lasers. WDMs for 2 µm Operation:Gooch & Housego’s FFW-xxxxxxxxx fused WDMs for 2 µm operation combine multiple wavelengths of light in single mode (SM) fiber whilst maintaining low loss. G&H proprietary manufacturing technology provides low loss with low polarization dependence (PDL). The all-fiber construction offers excellent reliability and high power handling characteristics. These high-performance parts are available in many wavelength configurations, housing, fiber and connector options and can therefore be readily specified in a wide variety of applications, enabling rapid design cycles and new project builds. Duplexing WDMs 1310/1550 nm & 1625 nm (FFW-4xxxx11xx):G&H’s FFW-4xxxx11xx series of duplexing WDMs enable the low-loss combining or splitting of a pair of wavelengths. 1310 nm/C band or 1310 nm/L band components are used to double network bandwidth whilst the 1310/1625 nm component is used to add or drop a supervisory wavelength from a system. G&H proprietary manufacturing technology provides uniquely low excess loss and wavelength dependence along with low polarization and temperature dependence for all ports. In addition to the standard wavelengths, other combinations such as 1550/1625 nm are available. Please contact AMS Technologies with your specific requirements. FFW-X SM Pump Signal WDMsGooch & Housego’s FFW-X single mode (SM) fused pump signal wavelength division multiplexers (WDMs) are used for multiplexing signal and pump power in erbium-doped power amplifiers, pumped by wavelengths from 960 to 1480 nm. Proprietary manufacturing technology provides uniquely low excess loss, along with low polarization and temperature dependence for all ports. The ultra-low loss of these components promotes high efficiency of use of pump power and low noise figure. Fused Pump Signal WDMs 980 nm (FFW-xxxxx2xxx):G&H’s FFW-xxxxx2xxx series of fused pump signal WDMs, 980 nm, multiplex signal and pump power in 980, 960 or 1060 nm-pumped erbium-doped fiber amplifiers. Wavelength configurations allow for 960, 980 or 1060 nm pumping and C, L or C+L signal bands. Reliability is assured through qualification to Telcordia GR-1221, with a field proven FIT rate of <1. Fused Pump Signal WDMs 1480 nm (FFW-3xxxx21xx):The Gooch & Housego FFW-3xxxx21xx series of fused pump signal WDMs, 1480 nm, multiplex signal and pump power in 1480 nm-pumped erbium-doped fiber amplifiers. Wavelength configurations are 1480 nm – C band and 1480 nm – L band. Subminiature Pump Signal WDMs (FFW-5x1xx2xx0):G&H’s FFW-5x1xx2xx0 series of subminiature pump signal WDMs provide low-loss multiplexing of pump and signal in an ultra-short 32 mm length package. Designed for space-constrained optical amplifiers, the product is manufactured using ø80 µm cladding fiber. This enables low fiber bend radius without compromising mechanical integrity. Key Features: Combining or Separating Two or Three Wavelengths Wide Range of Regular Parts Available Custom Wavelength Capability All Fiber – No Lens Alignment Low or Ultra-low Light Loss No Unwanted Reflections High Power Handling Custom Designs Available Key Features FFW-X SM Pump Signal WDMs: Promotes Low Amplifier Noise Figure Promotes Low Pump Power Wastage Ultra-low Excess Loss: <0.05 dB Typical C, L or C+L Signal Bands Wide Range of Regular Parts Available Miniature Versions (32 mm Package Length) Available High Power Handling Telcordia GR-1221 Compliance (980 nm, Subminiature) Proven Reliability Applications: Fiber Lasers; Sensors, Biomedical Equipment; Research; Visible and Display Systems; Avionics; Defense; Telecoms; Optical Networking; Instrumentation; IR Imaging; Industrial, IR Counter Measures; C, L or C+L Band EDFAs; C or L Band Pump/Signal Multiplexing; 960, 980, 1060 or 1480 nm Pump Rejection; Fiber Gyros; Sensors
Product number: SW11337
Manufacturer:

PZ3-PM3-APC-E-850B Fiber Stretchers
The PZ3-PM3-APC-E-850B is an advanced fiber stretcher designed to meet the rigorous demands of optical interferometric measurements and sensing systems. Engineered by Optiphase, a leader in all-fiber interferometer solutions, this mid-range model boasts a unique multi-layer winding approach that enhances modulation functionality while maintaining high operational frequencies. This enclosed fiber stretcher features FC/APC connectors, ensuring seamless connectivity and optimal performance at a wavelength of 850.0 nm. The incorporation of PM fiber with a Bowtie structure further optimizes polarization-maintaining capabilities, crucial for maintaining signal integrity in complex optical systems. Belonging to the esteemed PZ3 family, the PZ3-PM3-APC-E-850B exemplifies the superior craftsmanship and innovative technology synonymous with Optiphase's fiber stretchers. Designed for versatility, these devices are suitable for a wide array of applications, including open-loop demodulation, sensor simulation, variable optical delay, and general-purpose fiber interferometry. Unlike other systems, the PZ3 series does not require proprietary drivers; they can be operated using standard laboratory equipment, making them both cost-effective and user-friendly. With a capacitive impedance of approximately 42 nF, these stretchers offer reliable operation across various frequencies, ensuring precise control and modulation. Key Features Enhanced modulation function with a unique multi-layer winding approach, ensuring high operational frequency without compromising performance. Designed for bipolar voltage drive, providing greater convenience compared to systems requiring unipolar operation with offset voltage drive. Enclosed design with FC/APC connectors facilitates quick setup and robust connectivity, enhancing user experience and operational efficiency. Utilizes PM fiber with a Bowtie structure, optimizing polarization-maintaining capabilities crucial for precise optical measurements. Operates effectively with standard electronics, eliminating the need for proprietary drivers and reducing setup complexity and cost. Capacitive impedance of 42 nF ensures stable performance across a broad frequency range, maximizing modulation accuracy. Compact and robust enclosure design ensures durability and ease of integration into existing optical systems, supporting long-term use. Applications Ideal for open-loop demodulation applications where precise modulation control is critical for accurate data interpretation. Suitable for sensor simulation tasks, enabling researchers to replicate real-world conditions within controlled environments. Perfect for variable optical delay applications, allowing users to manipulate phase shifts with high precision and reliability. Widely used in general-purpose fiber interferometry, facilitating detailed analysis and measurement of optical signals. Supports large angle modulation of interferometric phase, expanding its utility across diverse scientific and industrial applications. Extensively used in optical communication systems, enhancing signal integrity and reducing noise interference. Applicable in research and development settings, offering flexibility and adaptability for evolving technological needs. What's next? As you consider integrating the PZ3-PM3-APC-E-850B into your optical systems, you will benefit from its user-friendly design and advanced features, which set new standards in fiber stretching technology. This product exemplifies the commitment to innovation and quality that Optiphase brings to the field of optical measurement and sensing. For those seeking comprehensive solutions in optical technologies, AMS Technologies offers unparalleled expertise and support. As a leading provider in the industry, AMS Technologies ensures that customers receive tailored solutions that meet their specific requirements, supported by a team of skilled professionals dedicated to advancing optical technology.
Product number: C040986-0
Manufacturer:

€3,908.57*
pcs
Acousto-Optic Deflectors
Wavelength 266-1100 nm; Type IR, Visible, UV, Mid-IR; Scan Angle 4,9-60 mrad; Active Aperture 1.0-60 mm; Operating Frequency 9.4 µm-432 MHz; Optical Material Germanium, Sapphire, Fused Silica, Crystalline Quartz, Tellurium Dioxide G&H acousto-optic deflectors (AODF) provide precise spatial control of an optical beam, whether performing 1D or 2D scanning or executing beam deflection through a fixed angle. The acousto-optic deflectors offer highly uniform diffraction efficiency across the full scan angle, with consistent power throughput for scanning applications like material processing and digital imaging. Gooch & Housego offers a wide range of standard deflectors and RF drivers for wavelengths from 266-1500 nm. Key Features: Visible and NIR wavelength products based on tellurium dioxide crystals, grown in-house UV wavelength products based on fused silica and crystal quartz Broad bandwidth products based on a longitudinal mode approach using a phased array of piezoelectric elements High efficiency products based on slow shear deflection using parallel tangents off-axis interactions Selecting the right RF driver is important to achieve the desired scanning speed and accuracy. Deflectors used in scanning or writing applications require a variable frequency source which is both stable and highly linear. 2D UV beam scanning may be achieved by cascading two UV deflectors in series. Gooch & Housego’s flexible functionality AODF Dual Driver with phase synchronized outputs offers the optimum in RF driver control for 2D scanning.Applications: Digital Imaging; Heterodyne Interferometry; Laser Cooling; Laser Marking; Laser Tweezers; Material Processing; Micromachining; Microscopy; On-Line Process Control; Optical Inspection; Photolithography; Printing Series Wavelength Type Scan Angle Active Aperture Operating Frequency Optical Material Downloads AODF 4070 N/A Mid-IR 60 mrad 9 mm 9.4 µm Germanium Datasheet Driver Driver AODF 2690-UV 266 - 355 nm N/A up to 4.9 mrad up to 7 mm 100 - 432 MHz Sapphire Datasheet Driver Driver AODF 4200-UV 266 nm UV 5.5 mrad 1.0 x 60.0 mm 135 - 265 MHz Fused Silica Datasheet Driver Driver AODF 4170 355 nm UV 4.9 mrad 7 mm 130 - 210 MHz Crystalline Quartz Datasheet Driver Driver AODF 4100-UV 364 nm UV 29.5 mrad 4.0 x 14.0 mm 75 - 125 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4200-VI 405 - 488 nm Visible 58 mrad 4.8 mm 150 - 250 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4090-7 440 - 530 nm Visible 44 mrad 8.5 mm 60 - 115 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4100-VI 488 nm Visible 39.5 mrad 4.0 - 14 mm 75 - 125 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4055-4 780 - 980 nm IR 44.3 mrad 3.5 x 14 mm 35 - 70 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4210-IR 830 nm IR 27.6 mrad 2.0 - 6.0 mm 140 - 280 MHz Tellurium Dioxide Datasheet Driver Driver AODF 4090-6 1064 nm IR 56 mrad 2 mm 72.5 - 107.5 MHz Tellurium Dioxide Datasheet Driver   AODF 4075-IR 1065 - 1100 nm IR 8.1 mrad 2.5 mm 59 - 91 MHz Tellurium Dioxide Datasheet Driver Driver
Product number: SW11403
Manufacturer: