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By virtue of having no moving parts our acousto-optic modulators (AOMs) are able to amplitude modulate a laser beam at very high speed. For example modulation bandwidths in excss of 50MHz are readily achievable.
By virtue of having no moving parts our acousto-optic modulators (AOMs) are able to amplitude modulate a laser beam at very high speed. For example modulation bandwidths in excss of 50MHz are readily achievable.
In an AOM a laser beam is caused to interact with a high frequency ultrasonic sound wave inside an optically polished block of crystal or glass (the interaction medium). By carefully orientating the laser with respect to the sound waves the beam can be made to reflect off the acoustic wavefronts (Bragg diffraction). Therefore, when the sound field is present the beam is deflected and when it is absent the beam passes through undeviated. By switching the sound field on and off very rapidly the deflected beam appears and disappears in response (digital modulation). By varying the amplitude of the acoustic waves the intensity of the deflected beam can similarly be modulated (analogue modulation).
It is usual to choose the deflected beam as the one that is used in the optical system because it can be switched on and off with high extinction ratio (typically >40dB) and intensity can be varied from zero to more that 85% of the incident beam. The rate at which the beam can be modulated is governed by the time it takes the acoustic wavefronts to traverse the laser beam, which depends on the beam diameter and the acoustic velocity in the interaction medium.
The sound waves are generated by a transducer, usually a thin wafer of lithium niobate, that is bonded onto the interaction medium using a highly efficient cold-weld metallic bonding process. When a high frequency electrical signal is applied to the transducer it vibrates, generating the acoustic wave. The signal is derived from an RF driver, which generates a high frequency carrier that is itself modulated by an analogue or digital input signal.
Principal applications for AO modulators are pre-press (putting image and text data onto films or plates as part of the printing process), laser imaging and displays, switching in telecom fibres, instrumentation and research.
Fiber-coupled acousto-optic modulators (FCAOM) offer an elegant and robust solution for amplitude modulation of fiber lasers, allowing direct control of the timing, intensity, and temporal shape of the laser output. Our 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.
Fiber-coupled acousto-optic modulators (FCAOM) were initially developed to modulate the intensity of light contained in fibers without having to break the fiber to install a free-space acousto-optic modulator (AOM). Traditionally, modulation in fiber lasers was achieved using a master oscillator power amplifier (MOPA). The MOPA limited the pulse shapes that could be created, and required a separate semiconductor seed laser system. Direct integration of a fiber optic acousto-optic modulator is a far simpler approach, and allows the optical path to remain closed for better power handling and reliability, in addition to lower loss.
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 1st order diffraction mode of a fiber-coupled modulator also experiences a frequency shift and beam deflection. This allows our Fiber-Q products to be used for more than just modulation, resulting in applications outside the laser such as optical heterodyne interferometry. The recent addition of visible Fiber-Q products will also enable more compact all-fiber instrument designs in biomedical applications such as microscopy and flow cytometry.
Today, we offer a line of fiber optic acousto-optic modulators 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)
We have leveraged our expertise in telecommunication component design to create a line of highly reliable fiber optic modulators, adapting our processes and designs to handle high optical power and the challenges of precision fiber alignment. We grow our own tellurium dioxide (TeO2) crystals in-house, polishing and performing all stages of fabrication to achieve low scatter and rigorous quality standards throughout the manufacturing process. This ensures consistently high reliability, high laser damage threshold and high optical performance.
We continue to lead the market in the development of fiber-coupled modulators, offering the first devices for visible wavelengths from 397 nm to 780 nm to meet the needs of sensing and quantum technology applications. Our 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.
In addition to our standard line of Fiber-Q modulators, we customize, design, and manufacture in volume for OEM needs. Furthermore, our technical support team works with our customers to identify the best RF driver for the application, taking into consideration the type of modulation required (digital or analog) as well as any specific pulse shaping needs.
We offer a wide range of standard fibre-coupled AOMs with the following characteristics: -
Wavelengths: 1310nm or 1550nm
Drive Frequencies: 40MHz, 80MHz or 110MHz
Optical Rise-Times: as low as 10ns
Materials: Tellurium Dioxide & Chalcogenide Glass
Options: Single mode, polarisation maintaining and multimode, with or without connectors. Available in two, three or four fibre package configurations.
Description of Part Number: T-M150-0.4C2G-3-F2S:
M = Modulator
150 = Drive frequency in MHz
2 = Tellurium Dioxide (interaction material)
F2 = 2 port fibre-coupled
S or P = Single Mode or Polarisation Maintaining.
Our standard FCAOMs are listed below. For more AOMs, please send us an email.
Model | Description | Optical Power handling | Wave length | Rise/ Fall time | Operating Frequency |
STG-S-M200-0.4C2A-3-F2P STG-S-M200-0.4C2A-3-F2S | Non-hermetic, PM/SM | 450 nm | 25 ns | 200 MHz | |
S200-0.4C2N-3-F2P | Non-hermetic, PM | 450, 532, 633, 780 nm | 25 ns | 200 MHz | |
STG-S-M200-0.4C2C-3-F2P, STG-S-M200-0.4C2C-3-F2S | Non-hermetic, PM/SM | 532 nm | 25 ns | 200 MHz | |
STG-S-M200-0.4C2E-3-F2P, | PM/SM | 633 nm | 25 ns | 200 MHz | |
STG-S-M150-0.4C2G-3-F2S | Non-hermetic, SM, HI1060 | 1060 nm | 30 ns | 150 MHz | |
STG-S-M200-0.1C2G-3-F2S | Non-hermetic, SM | 1060 nm | 10 ns | 200 MHz | |
STG-T-M150-0.5C2W-3-F2S | Non-hermetic, SM | 780 nm | 30 ns | 150 MHz | |
STG-T-M150-0.5C2W-3-F2P | Non-hermetic, PM | 780 nm | 30 ns | 150 MHz | |
STG-T-M150-0.4C2G-3-F2S | Hermetic, | 5W average | 1060nm | 30ns | 150MHz |
STG-T-M200-0.1C2G-3-F2P | Hermetic, PM, | 1W average | 1060nm | 10ns | 200MHz |
STG-T-M260-0.1C2G-3-F2P | Hermetic, PM | 1060 nm | 6 ns | 260 MHz | |
STG-T-M200-0.1C2G-3-F2P | Hermetic PM | 1060 nm | 10 ns | 200 MHz | |
STG-T-M300-0.1C2G-3-F2S | HI1060 | 0.5W average | 1060nm | 6ns | 300MHz |
STG-T-M300-0.1C2G-3-F2P | Fujikura PM1550 | 1W average | 1060nm | 6ns | 300MHz |
STG-T-M200-0.1C2G-3-F2S | Hermetic SM HI1060 | 1W average | 1060nm | 10ns | 200MHz |
STG-T-M150-0.4C2G-3-F2P | Hermetic, Fujikura PM980 (SM98-PS-U25A) | 5W average | 1060nm | 30ns | 150MHz |
STG-T-M200-0.1C2J-3-F2P | Hermetic, Fujikura PM1550 (SM15-PS-U25A) | 1W average | 1550nm | 10ns | 200MHz |
STG-T-M200-0.1C2J-3-F2S | Hermetic, SMF28 | 1W average | 1550nm | 10ns | 200MHz |
STG-T-M110-0.2C2J-3-F2S | Hermetic, SMF28 | 1W average | 1550nm | 25ns | 110MHz |
STG-T-M110-0.2C2J-3-F2P | Hermetic, Fujikura PM1550 (SM15-PS-U25A) | 1W average | 1550nm | 25ns | 110MHz |
STG-T-M080-0.4C2J-3-F2S | Hermetic, SMF28 | 1W average | 1550nm | 35ns | 80MHz |
STG-T-M080-0.4C2J-3-F2P | Hermetic, PM | 1W average | 1550nm | 35ns | 80MHz |
STG-T-M080-0.4C2J-3-F2P | Hermetic, Fujikura PM1550 (SM15-PS-U25A) | 1W average | 1550nm | 35ns | 80MHz |
STG-T-M040-0.5C8J-3-F2S | SMF28 | 1W average | 1550nm | 70-100ns | 40MHz |
STG-T-M080-0.5C8J-3-F2S | Hermetic, Low power consumption | 1W average | 1550nm | 70-100ns | 80MHz |
STG-T-M080-0.5C8J-3-F2P | Hermetic, Polarisation Maintaining, Low power consumption | 1W average | 1550nm | 70-100ns | 80MHz |
STG-T-M040-0.5C8J-3-F2P | Polarisation Maintaining, | 1W average | 1550nm | 70-100ns | 40MHz |
STG-T-M080-0.3C2Z-3-F2S | Nufern SM1950 | 5W average | 2000nm | 70-100ns | 80MHz |
STG-T-M080-0.3C2Z-3-F2P | Nufern PM1950 | 5W average | 2000nm | 70-100ns | 80MHz |
STG-T-M250-0.3C16Z-3-F2P | Nufern PM-GDF | 1W average | 2000nm | 20ns | 250MHz |
Our old FCAOM models are listed in the below table. These old models may or may not be in stock or obsolete and no longer produced. Please check with our sales regarding the availability of the below models.
Model | Description | Driver |
T-M040-0.5C8H-3-F2S | 1310nm (1285~1325nm), RF frequency 40MHz, average optical power handling ≤1W, SMF (SingleMode Fibre) | MLP040-0.4DC MLP040-0.4AC-A1 MLP040-0.4DS2 MLP040-0.4AS2-A1 |
T-M040-0.5C8J-3-F2S | 1550nm (1530~1565nm), RF frequency 40MHz, average optical power handling ≤1W, SMF (SMF28) | MLP040-0.4DC MLP040-0.4AC-A1 MLP040-0.4DS2 MLP040-0.4AS2-A1 |
T-M040-0.5C8J-3-F2P | 1550nm (1530~1565nm), RF frequency 40MHz, average optical power handling ≤1W, PMF (Fujikura PM1550) | MLP040-0.4DC MLP040-0.4AC-A1 MLP040-0.4DS2 MLP040-0.4AS2-A1 |
T-M080-0.4C2J-3-F2P | 1550nm, RF frequency 80MHz & RF power ≤3W, average optical power handling 1W, fiber Fujikura PM1550 (SM15-PSU25A), no connector | 1080AF-AINA-3.0 HCR 1080AF-DINA-3.0 HCR |
T-M080-0.4C2J-3-F2S | 1550nm, RF frequency 80MHz & RF power ≤3W, average optical power handling 1W, fiber SMF28), no connector | 1080AF-AINA-3.0 HCR 1080AF-DINA-3.0 HCR |
T-M150-0.4C2G-3-F2P | 1060nm, RF frequency 150MHz & RF power ≤2W, average optical power handling 5W, fiber Fujikura PM980 (SM98-PS-U25A) ), no connector | 1150AF-AINA-3.0 HCR 1150AF-DINA-3.0 HCR |
T-M150-0.4C2G-3-F2S | 1060nm, RF frequency 150MHz & RF power ≤2W, average optical power handling 5W, fiber HI1060), no connector | 1200AF-AINA-3.0 HCR 1200AF-DINA-3.0 HCR |
T-M200-0.1C2J-3-F2P | 1550nm, RF frequency 200MHz & RF power ≤3W, average optical power handling 1W, fiber Fujikura PM1550 (SM15-PSU25A) ), no connector | 1200AF-AINA-3.0 HCR 1200AF-DINA-3.0 HCR |
T-M200-0.1C2J-3-F2S | 1550nm, RF frequency 200MHz & RF power ≤3W, average optical power handling 1W, fiber SMF-28), no connector | 1200AF-AINA-3.0 HCR 1200AF-DINA-3.0 HCR |
T-M200-0.1C2G-3-F2P | 1060nm, RF frequency 200MHz & power 3W, average optical power handling 1W, fiber Fujikura PM980 (SM98-PS-U25A) ), no connector | 1200AF-AINA-3.0 HCR 1200AF-DINA-3.0 HCR |
T-M200-0.1C2G-3-F2S | 1060nm, RF frequency 200MHz & RF power ≤3W, average optical power handling 1W, fiber SMF-28), no connector | 1200AF-AINA-3.0 HCR 1200AF-DINA-3.0 HCR |
I-FS060-2F-F2P | 852nm, RF frequency 60MHz & RF power ≤1W, PM fiber 2m | |
MM065-1C2V5-5-F2XY-Z | TeO2, 2um, 65MHz, random, rise time 75ns, RF ≤4W, single mode fiber 9/125 or PM fiber 8/125 | 31065-4xx |
MM065-1C2V12-5-F2XY-Z | TeO2, 1.95um, 65MHz, random, rise time 100ns, RF ≤4W, single mode fiber 9/125 or PM fiber 8/125 | 31065-4xx |
MFS150-.2C17J-3-F2P-X-GH | GaP, 1.55um, 150MHz, 10ns risetime, RF<2W, PM fiber 8/125 | |
15200-.2-1.55-LTD-GaP-FO | Gap, 1.55um wavelength, linear polorisation, rise/fall time 10ns, 8/125 PM fiber, 200MHz, RF 2W | 21200-2xx |
15200-.2-1.06-LTD-GaP-FO-GH | Gap, 1.06um wavelength, linear polorisation, rise/fall time 10ns, 6/125 PM fiber, 200MHz, RF 2W | 21200-2xx |
23050-1-1.95-LTD-FO-2HP-PM-CSF | TeO2, 1950nm wavelength, 50MHz, linear polarized, 100ns risetime, PM fiber GDF 10/130um, 0.15/0.46NA, RF<4W | |
23080-1-.85-LTD-FO | TeO2, 850nm wavelength,80MHz, random, 50ns risetime, single mode or PM fiber 5/125, RF<1W | |
23080-1-1.06-LTD-FO | TeO2, 1060nm, 80MHz, random, risetime 50ns, single mode fiber 6/125 (PM 6/125 optional), <0.5W @ 1060nm, Used external to laser cavity, RF <1.25W | 21080-1xx |
23080-1-1.06-LTD-FO-HP | TeO2, 1060nm, 80MHz, random, risetime 50ns, single mode fiber 6/125 (PM 6/125 optional), <2W @ 1060nm, Used external to laser cavity, RF <1.25W | 21080-1xx |
23080-1-1.06-LTD-FO-2HP | TeO2, 1060nm, 80MHz, random, risetime 50ns, single mode fiber 6/125 (PM 6/125 optional), <2W @ 1060nm, may be used internal to laser cavity), RF <1.25W | 21080-1xx |
23080-1-1.3-LTD-FO | TeO2, 1300nm, 80MHz, random, risetime 50ns, single mode fiber 9/125 (PM 8/125 optional), RF <1.5W | 21080-2xx |
23080-1-1.55-LTD-FO | TeO2, 1520-1570nm, 80MHz, random, risetime 50ns, single mode fiber 9/125, RF <2W | 21080-2xx |
26035-2-1.3-LTD-FO | AMTIR, 1300nm, 35MHz, random, risetime 100ns, single mode fiber 9/125 (PM 8/125 optional), RF <0.5W | 21035-0.4xx |
26035-2-1.55-LTD-FO | AMTIR, 1520-1570nm (1570-1620nm optional), 35MHz, random, risetime 100ns, single mode fiber 9/125 (PM 8/125 optional), RF <0.5W | 21035-0.4xx |
26050-1-1.55-LTD-FO | AMTIR, 1520-1570nm (1570-1620nm optional), 50MHz, random, risetime 100ns, single mode fiber 9/125 (PM 8/125 optional), RF <0.5W | 21050-0.4xx |
26055-1-1.55-LTD-FO | AMTIR, 1520-1570nm (1570-1620nm optional), 55MHz, random, risetime 100ns, single mode fiber 9/125, 3 ports, RF <1W | 21055-0.4xx |
26055-1-1.55-LTD-3FO | AMTIR, 1550nm, 55MHz, random, risetime 100ns, single mode fiber 9/125, 3 ports, RF <1W | 21055-0.4xx |
26055-1-1.55-LTD-4FO | AMTIR, 1550nm, 55MHz, random, risetime 100ns, single mode fiber 9/125, 4 ports, RF <0.5W | 21055-0.4xx |
47040-2-.63-6.5DEG-LTD-FO-PM | TeO2, 633nm, 40MHz, linear polarized, 440ns risetime, PM fiber 4/125, 1 meter long, RF<0.5W | 21040-0.4xx |
54035-1.55-.5AS-FO | AMTIR, 1520-1570nm (1570-1620nm optional), 35MHz, random, risetime 100ns, single mode fiber 9/125, 1, 2, 3 or 4 channels | Driver integrated |
54055-1.55-.5DS-3FO | AMTIR, 1550nm, 55MHz, random, risetime 100ns, single mode fiber 9/125, 3 ports | Driver integrated |
54080-1.55-2DS | TeO2, 1520-1570nm (1570-1620nm optional), 80MHz, random, risetime 50ns, single mode fiber 9/125, 1, 2, 3 or 4 channels | Driver integrated |
Remark:
xx in the driver model (such as 21200-2xx) may be DM, AM, DS or AS
Standard connector is FC/PC (not applicable for T-M080, T-M150 and T-M200 series). We also commonly supply the following options: FC/APC, SC/PC & SC/APC. (Remark: 1. FC = Named as “Frank Charlie”, screw-in type metal plug connector; 2. SC = Named as “Sam Charlie”, square type plastic connector. 3. PC = Polished Connector, usually with Return Loss (RL) > 40dB (min) [eg. FC/PC, SC/PC]; 4. APC = 8 deg Angled-Polished Connector, usually with RL > 50dB (min) [eg. FC/APC, SC/APC])
For more information, please doanload the catalogue here.
We specialise in providing optical components for high power fibre laser and amplifier systems. In-house control of critical manufacturing processes, from crystalline material selection and orientation, cutting, polishing and AR coating through to fibre coupling, ensure our components are of the highest optical quality.
The ‘Fibre-Q’ Acousto-Optic Modulator is designed for use in pulsed fibre laser amplifier systems. In addition to the standard product shown, custom configurations are available for specialized applications.
Ordering Code Explanation: T-M150-0.4C2G-3-F2S (Modulator, 150MHz, 0.4mm active aperture, compressional mode, Tellurium Dioxide, 1064nm, SMA female bulk head connector, 2 fibre, single mode (Hi1060)
Key Features:
Low insertion loss
Compact, low profile package
Rugged hermetic design
Stable performance
Custom configurations available
General Specifications:
Model | T-M040-0.5C8H-3-F2S | T-M040-0.5C8J-3-F2S |
Interaction material: | Amtir-1 | Amtir-1 |
Wavelength: | 1310 (other wavelengths available on request) | 1550 (other wavelengths available on request) |
Average optical power handling: | 1W | 1W |
Peak (pulse) optical power handling: | 1kW typical (dependent on pulse width) | 1kW typical (dependent on pulse width) |
Insertion loss: | < 2.5dB | < 2.5dB |
Return loss: Extinction ratio (1st order on / off) | > 40dB (>50dB version available on request) > 50dB | > 40dB (>50dB version available on request) > 50dB |
Rise-time / fall-time: | 70ns | 70ns |
Frequency: | 40MHz | 40MHz |
VSWR: | < 1.3:1 | < 1.3:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | < 0.4W | < 0.4W |
Frequency shift: | 40MHz (up-shift) | 40MHz (up-shift) |
Fibre type: | SMF28 (900μm black sleeving, 1.5m length) | SMF28 (900μm black sleeving, 1.5m length) |
Fibre termination: | Bare fibre | Bare fibre |
Application | Sensing (heterodyne interferometry) Intensity modulation | Sensing (heterodyne interferometry) Intensity modulation |
Model | T-M040-0.5C8J-3-F2P | T-M080-0.4C2J-3-F2P |
Interaction material: | Amtir-1 | TeO2 |
Wavelength: | 1550 (other wavelengths available on request) | 1550 (other wavelengths available on request) |
Average optical power handling: | 1W | 1W |
Peak (pulse) optical power handling: | 1kW | 30kW typical (dependent on pulse width) |
Insertion loss: | < 2.5dB | <3dB |
Return loss: Extinction ratio (1st order on/off) | > 40dB (>50dB version available on request) > 50dB | > 40dB (>50dB version available on request) > 50dB |
Rise-time / fall-time: | 70ns | 35ns |
Frequency: | 40MHz | 80MHz |
VSWR: | < 1.3:1 | < 1.2:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | < 0.4W | < 3.0W |
Frequency shift: | 40MHz (up-shift) | 80MHz (up-shift) |
Fibre type: | PM1550(SM15-PS-U25A, 900um PVDF sleeving, 1.5m length) | PM1550(SM15-PS-U25A, 900um PVDF sleeving, 1.5m length) |
Fibre termination: | FC/APC | Bare fibre |
Application | Sensing (heterodyne interferometry) Intensity modulation | Sensing (heterodyne interferometry) Intensity modulation, Pulse picking |
Model | T-M080-0.4C2J-3-F2S | T-M150-0.4C2G-3-F2S |
Interaction material: | TeO2 | TeO2 |
Wavelength: | 1550nm (other wavelengths available on request) | 1060nm (other wavelengths available on request) |
Average optical power handling: | 1W | 5W |
Peak (pulse) optical power handling: | 30kW typical (dependent on pulse width) | 30kW typical (dependent on pulse width) |
Insertion loss: | <3dB | <2dB |
Return loss: Extinction ratio (1st order on/off) | > 40dB (>50dB version available on request) > 50dB | > 40dB (>50dB version available on request) > 50dB |
Rise-time / fall-time: | 35ns | 30ns |
Frequency: | 80MHz | 150MHz |
VSWR: | < 1.2:1 | < 1.2:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | < 3.0W | <2W |
Frequency shift: | 80MHz (up-shift) | 150MHz upshift |
Fibre type: | SMF28(900um black sleeving, 1.5m length) | Nufern FUD 3583 10/125 NA 0.08, 900um black sleeving, 1.5m length |
Fibre termination: | Bare fibre | Bare fibre |
Application | Sensing (heterodyne interferometry) Intensity modulation, Pulse picking | Fibre laser, Fibre amplifier Pulse picker |
Model | T-M150-0.4C2G-3-F2P | T-M200-0.1C2J-3-F2S |
Interaction material: | TeO2 | TeO2 |
Wavelength: | 1060nm (other wavelengths available on request) | 1550nm (other wavelengths available on request) |
Average optical power handling: | 5W | 1W |
Peak (pulse) optical power handling: | 30kW typical (dependent on pulse width) | 100uJ, based on 10ns pulse |
Insertion loss: | <2.5dB | <6dB |
Return loss: Extinction ratio (1st order on/off) | > 40dB (>50dB version available on request) > 50dB | > 40dB (>50dB version available on request) > 50dB |
Rise-time / fall-time: | 30ns | 10ns |
Frequency: | 150MHz | 200MHz |
VSWR: | < 1.2:1 | < 1.5:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | <2W | <3W |
Frequency shift: | 150MHz upshift | 200MHz upshift |
Fibre type: | Fujikura PM980 (SM98-PS-U25A) 900um black sleeving, 1.5m length | SMF28(900um black sleeving, 1.5m length) |
Fibre termination: | Bare fibre | Bare fibre |
Application | Fibre laser, Fibre amplifier, Pulse picker | Fibre laser, Pulse picker, Optical sensing |
Model | T-M200-0.1C2J-3-F2P | T-M200-0.1C2G-3-F2S |
Interaction material: | TeO2 | TeO2 |
Wavelength: | 1550nm (other wavelengths available on request) | 1060nm (other wavelengths available on request) |
Average optical power handling: | 1W | 1W |
Peak (pulse) optical power handling: | 100uJ, based on 10ns pulse | 1kW typical (dependent on pulse width) |
Insertion loss: | <6dB | <4dB |
Return loss: Extinction ratio (1st order on/off) | > 40dB (>50dB version available on request) > 50dB | > 40dB (>50dB version available on request) > 50dB |
Rise-time / fall-time: | 10ns | 10ns |
Frequency: | 200MHz | 200MHz |
VSWR: | < 1.5:1 | < 1.5:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | <3W | <2.5W |
Frequency shift: | 200MHz upshift | 200MHz upshift |
Fibre type: | Fujikura PM1550 (SM15-PS-U25A) 900um black sleeving, 1.5m length | HI1060(900um PVDF sleeving, 1.5m length) |
Fibre termination: | Bare fibre | Bare fibre |
Application | Fibre laser, Pulse picker, Optical sensing | Fibre laser, Pulse picker, Optical sensing |
Model | T-M200-0.1C2G-3-F2P | FS060-2F-F2P |
Interaction material: | TeO2 | TeO2 |
Wavelength: | 1060nm (other wavelengths available on request) | 852nm |
Average optical power handling: | 1W | >25mW |
Peak (pulse) optical power handling: | 1kW typical (dependent on pulse width) | |
Insertion loss: | <4dB | <3dB |
Return loss: Extinction ratio (1st order on/off) | > 40dB (>50dB version available on request) > 50dB | >40dB |
Rise-time / fall-time: | 10ns | |
Frequency: | 200MHz | 60MHz |
VSWR: | < 1.5:1 | |
Input impedance: | 50Ω | 50Ω |
RF power: | <3W | <1W |
Frequency shift: | 200MHz upshift | |
Fibre type: | Fujikura PM980 (SM98-PS-U25A) 900um black sleeving, 1.5m length | PM fiber 2m length |
Fibre termination: | Bare fibre | SMA Female |
Application | Fibre laser, Pulse picker, Optical sensing |
Model | MM065-1C2V5-5-F2XY-Z | MM065-1C2V12-5-F2XY-Z |
Interaction material: | TeO2 | TeO2 |
Acousto mode | Longitudinal | Longitudinal |
Wavelength: | 2um | 1.95um |
Window configuration | AR coated | AR coated |
Insertion loss: | <3.5dB | <3.5dB |
Contrast ratio | > 40dB | > 40dB |
Rise-time / fall-time: | 75ns | 100ns |
Frequency: | 65MHz | 65MHz |
VSWR: | < 1.2:1 | < 1.2:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | <4W | <4W |
Fibre type: | 9/125 single mode, 1meter long: X=S 8/125 polarization maintaining: X=P | 9/125 single mode, 1meter long: X=S 8/125 polarization maintaining: X=P |
Fibre termination: | FC/PC, SC/PC, FC/APC, SC/APC | FC/PC, SC/PC, FC/APC, SC/APC |
Model | MFS150-.2C17J-3-F2P-X-GH | 15200-.2-1.55-LTD-GaP-FO |
Interaction material: | GaP | GaP |
Acousto mode | Longitudinal | Longitudinal |
Wavelength: | 1.55um | 1.55um |
Window configuration | AR coated | AR coated |
Insertion loss: | <3.5dB | <3.5dB |
Contrast ratio | > 35dB | > 35dB |
Rise-time / fall-time: | 10ns | 10ns |
Frequency: | 150MHz | 200MHz |
VSWR: | < 1.5:1 | < 1.5:1 |
Input impedance: | 50Ω | 50Ω |
RF power: | <2W | <2W |
Fibre type: | 8/125, polarization maintaining fiber, 1 meter long | 8/125, polarization maintaining fiber, 1 meter long |
Fibre termination: | FC/PC, SC/PC, FC/APC, SC/APC | FC/PC, SC/PC, FC/APC, SC/APC |
Model | 23050-1-1.95-LTD-FO-2HP-PM-CSF |
Interaction material: | TeO2 |
Acousto mode | Longitudinal |
Wavelength: | 1950um |
Window configuration | AR coated |
Optical power | <2W average/CW |
Back reflection | -30dB |
Insertion loss: | <3.5dB |
Contrast ratio | > 40dB |
Rise-time / fall-time: | 100ns |
Frequency: | 50MHz |
VSWR: | < 1.2:1 |
Input impedance: | 50Ω |
RF power: | <4W |
Fibre type: | Polarization Maintaining GDF, 10/130 um 0.15/0.46 NA |
Fibre termination: | FC/PC |
Custom-AOMs available upon request. Please send us an email if you have any further enquiry.
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Office: 10 Bukit Batok Crescent #07-02 The Spire Singapore 658079
Tel: +65 63167112
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