2µm pulsed Microchip laser

2 Microns Laser

The 2µm pulsed source reaches a pulse energy as high as 270µJ, combining spectral tunability from 1.94 to 1.96 µm with a single longitudinal mode (SLM) output upon request
This 2µm laser operates at a repetition rate up to 5kHz and a few tens of ns pulse duration.

Its main applications include LIDAR, detection of atmospheric gases and moleculesmedical and surgical procedures, processing of plastics, and many others.

Mid-IR widely tunable OPO source

The Optical Parametric Oscillator (OPO) pulsed source combines a wide spectral tunability, from 7.5 to 13µm (or 3 to 5µm upon request), with a very narrow linewidth, down to 100MHz.
With the optional Optical Parametric Amplifier (OPA) stage, the source reaches a peak power as high as 100W with an energy of 4µJ per pulse.
Its SLM (Single Longitudinal Mode) output features a kHz repetition rate and a few tens of ns of pulse duration.

The OPO source’s main applications includes LIDAR remote gas detection in the whole LWIR or MWIR spectral region.
It was tested under severe conditions on the field: implemented in a LIDAR system, the OPO source allowed to detect succsessfully different toxic gases at 300m distance.

Nikon Digital Imaging Microscope Eclipse Ui

A Real Solution for Digital Pathology

Nikon’s new ECLIPSE Ui Digital Upright Microscope provides accurate microscopy-based observation imaging. View and share high quality images in real time with easy-to-use software for a more streamlined workflow.

Nikon Super-Resolution Microscope N-SIM S

Doubling the conventional resolution limit for live cell time-lapse imaging.

The N-SIM S Super Resolution Microscope is a unique high-speed structured illumination system that achieves acquisition speeds of up to 15 fps, enabling fast biological processes to be captured at twice the spatial resolution of conventional light microscopes (up to 115nm in XY). Combining the N-SIM S and a confocal microscope gives you the flexibility to select a location in the confocal image and switch to super-resolution to view the desired part of the location in minute detail.

Nikon Multiphoton Microscopes AX R MP

Robust multiphoton system tailored for in vivo applications

Nikon’s multiphoton confocal microscopes, which clearly visualize fine structures deep within living organisms, have evolved even further. The AX R MP, equipped with a high speed high resolution resonant scanner, can capture dynamics that span a wide area with superior spatial and temporal resolution. In addition, a greatly expanded sample area provides the flexibility needed to observe biological samples in their natural positions and accommodates additional equipment often required for in vivo imaging.

The AX R MP maximizes image size, as well as spatial and temporal resolution, providing a uniquely powerful solution for any multiphoton experiment.

Large Field of View Resonant and Galvano Scanners: FOV 22 mm
High-speed Resonant Scanner: 720 fps (at 2048 x 16 pixels)
High-resolution Resonant Scanner: 2K x 2K, Galvano scanner: 8K x 8K
High-sensitivity Improved SNR with new detectors and electronics
Flexibility Two types of stands and tilting nosepiece

For broad research areas

LDH-I Series

LDH-I Series features a large range of smart laser heads compatible with the Taiko PDL M1 driver. Laser heads from this series provide wavelengths in the spectral range from 375 to 1550 nm and include power calibrations. When coupled with a Taiko PDL M1, their optical output power can be controlled in both pulsed and continuous modes. Additionally, a wavelength calibration is available in CW mode. Each laser head is identified by the Taiko PDL M1 driver and includes not only linearized calibration data but also an operating hours counter.

LDH Series – Picosecond Laser Diode Heads for PDL 800-D/PDL 810/PDL 828

The LDH Series laser heads are ideally suited for any application that requires picosecond pulses with variable repetition rates. Since we use a wide variety of laser diode types for our LDH laser heads, we can offer a broad range of wavelengths, power values, and spectral widths. Each laser head includes control electronics specially matched to the diode and collimating optics. Different types of optical fibers can also be fitted to laser output.

LDH-FA Series – Amplified Picosecond Pulsed Laser Diode Heads

 

The picosecond pulsed laser diode heads of the LDH-FA Series are based on a Master Oscillator Fiber Amplifier (MOFA) concept with optional frequency conversion. The master oscillator generates infrared picosecond pulses with variable repetition rates up to 80 MHz using the proven gain-switching techniques from PicoQuant. The output of this seed laser is directly connected to a single or double stage fiber amplifier, which boosts the output from the seed laser by several dB while maintaining the other characteristics of the seed laser beam like the emission wavelength, polarization and the short pulse width.

Scheme of how the fibre amplification works in heads from the LDH-FA Series

VisUV – High-power Picosecond Lasers in UV, Green, Yellow, and Orange Lasers

The VisUV laser is a versatile and flexible platform based on a Master Oscillator Fiber Amplifier (MOFA) concept with frequency conversion. The master oscillator generates infrared picosecond pulses at 1064 nm with variable repetition rates up to 80 MHz using the proven gain-switching techniques from PicoQuant. The output of this seed laser is directly connected to a multi-stage fiber amplifier, which boosts the output from the seed laser by several dB while maintaining the other characteristics of the seed laser beam like the emission wavelength, polarization and the pulse width.

VisIR – High-power Picosecond Lasers in 775, 1064, 1550nm

The VisIR laser is a versatile and flexible platform based on a Master Oscillator Fiber Amplifier (MOFA) concept with frequency conversion. The master oscillator generates infrared picosecond pulses at 1064 nm, 1530 to 1560 nm, and 1950 nm (NEW!) with variable repetition rates up to 80 MHz using the proven gain-switching techniques from PicoQuant. The output of this seed laser is directly connected to a multi-stage fiber amplifier, which boosts the output from the seed laser by several dB while maintaining the other characteristics of the seed laser beam like the emission wavelength, polarization and the pulse width.