Due to intensifier tube obsolescence, this hugely popular IR viewer has been discontinued. Our replacement products can be found above.

A mobile CMOS laser beam profiler with simple remote WiFi operation.

• No computer required – supplied with a tablet
• Wavelength Range = 400-1050nm
• ISO 11146-1, 11146-2 & 11146-3 compliant measurements
• Dynamic Noise Correction
• Mini USB power and data connection
• Cost-effective

A compact CMOS laser beam profiler with simple operation.

• Wavelength Range = 400-1050 nm
• ISO 11146-1, 11146-2 & 11146-3 compliant measurements
• Dynamic Noise Correction
• Mini USB power and data connection
• Cost-effective

An acousto-optic device designed to modulate, or frequency shift an 1200 nm – 2500 nm laser beam. 255 nsec/mm rise time.

An acousto-optic device designed to deflect/modulate a 440 nm to 700 nm laser beam. 40 MHz centre frequency, 20 MHz deflection bandwidth.

An acousto-optic device designed to deflect a 1064 nm laser beam. 40 MHz centre frequency, 20 MHz deflection bandwidth.

An acousto-optic device designed to modulate, or frequency shift a 10600 nm or 3390 nm laser beam by +/- 10 MHz.

An acousto-optic device designed to modulate, or frequency shift a 1060nm laser beam by +/- 30 MHz to 50 Mhz. 117 nsec / mm rise time.

An acousto-optic device designed to modulate, or frequency shift a 1060 nm laser beam. 290 nsec rise time.

An Acousto-optic device designed to deflect or modulate a 633 nm laser beam by 6.5 mrad. Centre frequency 70 MHz, deflection bandwidth 40 MHz.

An acousto-optic device designed to modulate, or frequency shift, a 440 nm – 1100 nm laser beam. 177 nsec minimum rise time, +/- 30 to 50 MHz optical shift range.

An acousto-optic device designed to modulate a 440 nm to 700 nm laser beam.

An acousto-optic device designed to modulate, or frequency shift, a 440 nm – 1100 nm laser beam. 177 nsec minimum rise time, +/- 30 to 50 MHz optical shift range.

An acousto-optic device designed to achieve high energy, short duration laser pulses. 700-2100nm, 110 nsec/mm minimum rise time.

An acousto-optic device designed to achieve high energy, short duration laser pulses. 700-2100nm, 160 nsec/mm minimum rise time.

An acousto-optic device designed to achieve high energy, short duration laser pulses. 1047-1064nm, 177 nsec/mm minimum rise time.

An acousto-optic device designed to modulate the intensity of a 300 nm – 400 nm UV laser beam. 55 nsec minimum rise time.

An Acousto optic device designed to deflect a 488 nm – 680 nm laser beam by 40 mrad. Centre Bandwidth 80 MHz, deflection bandwidth 50 MHz.

An acousto-optic device designed to modulate a 440 nm to 700 nm laser beam. 9.2 nsec minimum rise time.

An acousto-optic device designed to frequency shift a 440 nm to 1100 nm laser beam. Wide frequency shifting range.

The Model DE Series Deflector Drivers include a voltage-controlled RF oscillator and a broadband RF power amplifier in a housing with power supply, RFI line filter, and line switch.

The DFE Dual Frequency Source series are two-channel frequency generators capable of delivering up to four watts of RF power from each channel into a 50-ohm load. The DFE is used in applications where a very stable frequency difference is required.

An acousto-optic device designed to deflect a 1064 nm laser beam in 2 axes by 27 mrad. Centre bandwidth 27 MHz, deflection bandwidth 16 MHz.

A fibre pigtailed acousto-optic device designed to modulate a 1200 nm – 1600 nm laser beam.

An acousto-optic device designed to frequency shift a 1300 nm to 1550 nm laser beam by up to 100 MHz.

Electronics designed to drive a high power IntraAction acousto-optic modulator. 30 nsec rise time.

Electronics designed to drive an IntraAction acousto-optic modulator. 30 nsec rise time.

The ML series Mode Lockers are manufactured from high quality fused silica acousto-optic material. The RF sound field is generated with Lithium Niobate transducers. The user can specify window configuration, operating frequency, and mode spacing in order to optimise system performance.

The MLR Series Mode Locker is an acoustic standing-wave device with resonant mode spacing determined by the thickness of the acousto-optic material. When an integral number of acoustic half wavelengths are present across the material, standing waves are formed and modulate the laser cavity at twice the applied RF frequency.

The Model PA-8 Series Amplifiers are linear class AB broadband RF power amplifiers capable of from 10 to 100 watts power output over the frequency range of 5 MHz to 120 MHz.

The Model PA-4 is a linear class A broadband RF power amplifier capable of four watts power output over the frequency range of 10 MHz to 100 MHz.

The QE Series of acousto-optic Q-switch drivers contain a crystal controlled RF oscillator, fast modulation circuit, free running pulse generator circuit with trigger capability, and a broadband RF power amplifier in a housing with power supply, RFI line filter, line switch, and fault/interlock circuit.

Electronics designed to drive an IntraAction acousto-optic deflector or frequency shifter. 30 nsec rise time.

High performance image conversion IR viewers based on high-grade image converter are designed to observe indirect radiation of infrared laser, light emitting diodes (LED), dye and other IR-sources in 350 – 1300 nm spectral range.

High performance image conversion IR viewers based on high-grade image converter are designed to observe indirect radiation of infrared laser, light emitting diodes (LED), dye and other IR-sources in 350 – 1700 nm spectral range.

High performance image conversion IR viewers based on high-grade image converter are designed to observe indirect radiation of infrared laser, light emitting diodes (LED), dye and other IR-sources in 350 – 1700 nm spectral range.

High performance image conversion IR viewers based on high-grade image converter are designed to observe indirect radiation of infrared laser, light emitting diodes (LED), dye and other IR-sources in 350 – 2000 nm spectral range.

High performance image conversion IR viewers based on high-grade image converter are designed to observe indirect radiation of infrared laser, light emitting diodes (LED), dye and other IR-sources in 350 – 2000 nm spectral range.

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-1200
• VLT 15%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-1200
• VLT 7%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-1200
• VLT 2%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 180-400 5+
• 445-470 + 520 2+
• 524-532 3+
• VLT 38%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-534 7+
• 760-1090 5+
• 790-850 7+
• >850-960 6+
• >960-1070 7+
• VLT  22%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-534 7+
• 850-925 5+
• 925-1070 6+
• 960-1064 7+
• VLT 35%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-398 7+
• 9000-11000 7+
• VLT 93%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 850-2800 3+
• 900-2600 4+
• 950-1010 5+
• >1010-1500 7+
• >1500-2350 5+
• >2800-10600 5+
• VLT 75%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-380 5+
• 606-694 5+
• VLT 18%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-579 5+
• VLT 9%

NoIR LaserShields are the product of engineering innovation and tight manufacturing tolerances, providing an optimal balance between protection and visibility.

• 190-420 5+
• 765-1100 5+
• 775-1085 6+
• 790-1080 7+
• VLT 45%

Accurate Wavefront Correction with any deformable mirror. Phasics adaptive optics loop achieves the finest possible correction, up to last parabola aberration removal, thanks to the combination of their high resolution wavefront sensor and the deformable mirror device that best fits your set-up. An insightful support resulting from many years of experience is provided from the loop design to its installation.

High resolution wavefront measurement. Based on a patented technology, Phasics wavefront sensor simultaneously provides both phase and intensity maps of unrivalled high resolution. It combines to the SID4 software to deliver a complete diagnostic of the laser beam: wavefront aberrations, laser beam parameters, beam profiles, M2 beam quality parameter… It is compact and it easily positions at any point of the laser chain as it directly measures diverging beam.

Phasics wavefront sensor makes easy the characterization of telescopes, mirrors and any optics used in laser facilities. It delivers aberrations, PSF, Sthrel ratio, phase RMS, beam profiles or surface shape based on a high resolution wavefront measurement. Measured aberrations can then be automatically removed of further measurement. The solution applies to any optics of any wavelength, including beam expander, large mirror, flat optics. Their wavefront sensor is even more easy-to-use when it is coupled with the R-Cube, their high quality illumination unit dedicated to double-pass measurement.

Using high resolution phase imaging SID4 density is a straightforward and highly sensitive solution for neutral gas and plasma density measurement. It relies on an direct phase shift measurement with our ultra high resolution wavefront sensor, the SID4 HR.

Laser Diode Driver

• 100 mA current source
• Ultra-low drift (<10ppm/°C)
• <0.3μA current noise (LDC500)
• CC & CP mode dynamic switching
• GPIB, RS-232 and Ethernet

TEC Controller

• 36W output power
• Ultra-high stability (0.0005 °C/°C)
• Thermistor, RTD and IC sensors
• Auto-tuning of loop parameters
• CC & CT mode dynamic switching

Laser Diode Driver

• 500 mA current source
• Ultra-low drift (<10ppm/°C)
• <0.3μA current noise (LDC500)
• CC & CP mode dynamic switching
• GPIB, RS-232 and Ethernet

TEC Controller

• 36W output power
• Ultra-high stability (0.0005 °C/°C)
• Thermistor, RTD and IC sensors
• Auto-tuning of loop parameters
• CC & CT mode dynamic switching

Laser Diode Driver

• 2000 mA current source
• Ultra-low drift (<10ppm/°C)
• <0.3μA current noise (LDC500)
• CC & CP mode dynamic switching
• GPIB, RS-232 and Ethernet

TEC Controller

• 36W output power
• Ultra-high stability (0.0005 °C/°C)
• Thermistor, RTD and IC sensors
• Auto-tuning of loop parameters
• CC & CT mode dynamic switching

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organisations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organisations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organisations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organisations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organizations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.

Acuros® CQD® SWIR laser profiling cameras have been designed for use in applications requiring direct imaging of laser sources without the use of an external lens or other optical components that can impact the beam shape or path. These cameras are being adopted by laser manufacturers, producers of laser system assemblies, and laser-based manufacturing organizations. The Acuros CQD SWIR sensors are used for applications that include laser beam diagnostic imaging, laser beam profiling, and laser alignment.