Spectroscopy & Hyperspectral Imaging

Photon etc

Photon etc Photon etc

Photon etc. is a Canadian designer and manufacturer of highly sensitive infrared cameras, ultrafast hyperspectral imaging (wide-field, microscopy and Raman) ideal for academic research and cutting-edge industrial applications.

Website: https://www.photonetc.com

Photon etc

HyperSpectral Imagers

HYPERSPECTRAL MICROSCOPY

The global hyperspectral Raman imager (RIMA™) developed by Photon etc. offers a unique solution for rapid spectral and spatial characterization of advanced materials over large areas (up to 1 mm x 1 mm and more). By combining this rich information obtained from Raman spectroscopic fingerprints with the speed of global hyperspectral imaging, RIMA™ extends the limits of sample analysis and is a powerful non-invasive imaging modality for material and biomedical sciences.

RIMA™

RIMA

The perfect Raman imager for the analysis of nanomaterials from graphene to carbon nanotubes, RIMA™ is a state-of-the-art ultrafast hyperspectral imager available at excitation wavelengths of 532 nm, 660 nm and others.

The tool of choice for non-invasive monitoring and analysis of biological tissue, RIMA™ is a cutting-edge hyperspectral Raman imager for biomedical sciences, available at an excitation wavelength of 785 nm.

Characteristics

  • Fast global mapping (non-scanning)
  • Megapixel images in minutes
  • Stokes and anti-Stokes
  • High spatial and spectral resolution
  • Non-destructive analysis
  • Complete system (source, microscope, camera, filter, software)

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IMA™

IMA

The IMA™ hyperspectral microscopy platform delivers equally high spectral and spatial resolution. Have this modular system configured to rapidly scan the VIS, NIR and/or SWIR spectrums while mapping a combination of photoluminescence, electroluminescence, fluorescence, reflectance, and/or transmittance. Each IMA™ comes equipped with high throughput global imaging filters; this allows it to measure a megapixel hypercube faster than hyperspectral systems reliant on scanning spectrography.

IMA™ OPENS THE DOOR TO

  • Perform complex material analyses like solar cell characterization and semiconductor quality control (e.g.: perovskite, GaAs, SiC, CIS, CIGS, etc.).
  • Study IR markers in complex environments including live cells and tissue. Take for instance the spectral heterogeneity of IR fluorophores emitting in the second biological window.
  • Retrieve dark-field images and obtain a contrast of transparent and unstained samples such as polymers, crystals or live cells.

Characteristics

  • Fast global mapping (non-scanning)
  • High spatial and spectral resolution
  • Complete system (source, microscope, camera, filter, software)
  • Non-destructive analysis
  • Customization available
  • Sensitive from 400 to 1000 nm in the visible and from 900 nm up to 1700 nm in the SWIR range

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HYPERSPECTRAL WIDEFIELD IMAGERS

Allowing you to completely characterize your target with full-resolution images at any wavelength within 400-1000 nm (V-EOS™) or 1000-2300 nm (S-EOS™), Photon etc.’s widefield hyperspectral imagers will change your view of spectral analysis. Acquisition of an optimized hyperspectral cube permits spectral analysis of each and every pixel of a full-resolution image, meaning no more fastidious XY scanning of samples or limiting exposure time of remote sensing acquisitions. Resulting in more than just an increase in efficiency, V-EOS™ and S-EOS™ provide data on both spectral and spatial content, allowing you to perform novel analysis by extending the frontiers of your most demanding applications.

HYPERSPECTRAL CAMERA S-EOS™

HYPERSPECTRAL CAMERA S-EOS

The unique power of infrared HgCdTe detectors coupled to the richness of spectral information that offers our technology. Tunable on a large spectral range (1000-2300 nm), S-EOS™ offers infinite possibilities.

CHARACTERISTICS

  • Continuously tunable
  • Non-dispersive technology
  • High-performance HgCdTe camera
  • Control and analysis software

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HYPERSPECTRAL CAMERA V-EOS™

HYPERSPECTRAL CAMERA V-EOS

Giving complete information on your target with full resolution images at any wavelength in the range 400-1000 nm, Photon etc.’s V-EOS™ will change your view of spectral analysis.

CHARACTERISTICS

  • Continuously tunable
  • Non-dispersive technology
  • High-performance CCD
  • Motorized focus
  • Control and analysis software

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HYPERSPECTRAL CAMERA GRAND-EOS™

HYPERSPECTRAL CAMERA GRAND-EOS

GRAND-EOS combines a hyperspectral microscopy system with a hyperspectral wide-field imaging platform, giving access to micro and macro modalities with VNIR (400-1000 nm) and SWIR (900-1620 nm) ranges.

CHARACTERISTICS

  • Continuously tunable
  • Sensitive from 400 nm to 1620 nm
  • Non-dispersive technology
  • High-performance CCD
  • Motorized focus
  • Control and analysis software

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IR VIVO™

IR VIVO

Using near and shortwave infrared, IR VIVO benefits from reduced scattering as well as minimal tissue absorption and auto-fluorescence. This allows deeper, clearer imaging than standard optical imaging. IR VIVO takes advantage of the most recent developments in SWIR imaging. It combines Photon etc.’s ultra-low noise InGaAs camera (Alizé™ 1.7 or ZephIR™ 1.7) with novel illumination and powerful analytical software to provide an unprecedented combination of fast, high resolution and deep imaging.

NIR-II IMAGING PROPERTIES

  • High spatial resolution
  • High temporal resolution (real-time dynamics)
  • Non-ionizing & non-invasive
  • Good penetration depth (10x greater than traditional visible optical systems)

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Photon etc

TUNABLE SOURCES & FILTERS

The Laser Line Tunable Filter (LLTF) is a non-dispersive tunable bandpass filter based on volume holographic gratings. It delivers the highest signal throughput in the industry and is also unique in that it combines very high optical density (> OD6) and outstanding out-of-band rejection with wide tunability. A single filter can be tuned from 400 nm to 1000 nm (VIS) or 1000 nm to 2300 nm (SWIR), with bandwidths (FWHM) of <2.5 nm and <5 nm respectively. Custom and extended spectral ranges (up to 2500 nm) and bandwidths (sub-nm) are also available. Photon etc’s LLTF can be coupled with a supercontinuum laser to provide a Tunable Laser Source (TLS); the LLTF is compatible with any VIS-NIR broadband source

LASER LINE TUNABLE FILTER

LASER LINE TUNABLE FILTER

The incomparable efficiency and out-of-band rejection offered by our unique optical filtering technology are ideal for tunable excitation sources in fluorescence and Raman spectroscopy.

CHARACTERISTICS

  • Efficiency up to 60%
  • High out-of-band rejection
  • Wide tuning range
  • Free-space or fibre coupled
  • User-friendly control software
  • Up to 20W input power
  • Options & accessories available

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THE HYPERCUBE™

Hypercube

The HyperCube™ will transform your microscope into a high-resolution spectral imaging system, opening new research perspectives in biological imaging. Designed to fit commercial microscopes, cameras and a vast variety of excitation modules, The HyperCube™ gives access to the detailed composition of your sample.

CHARACTERISTICS

  • Fast global mapping (non-scanning)
  • High spatial and spectral resolution
  • Easy integration
  • Non-destructive analysis
  • Customization available

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Photon etc

SWIR Cameras – Fast and Low Noise InGaAs and HgCdTe Cameras

SWIR cameras

Extending the boundaries of industrial imaging, Photon etc. has developed affordable SWIR cameras sensitive from 800 nm to 2.9 µm. Using a sensitive InGaAs or HgCdTe (MCT) FPA, ZEPHIR™ collects images at an astounding 340 frame-per-second rate while reaching unrivalled low noise levels with the integration of a four-stage TE cooler. Our BOREA™ line uses a Stirling micro cooler and has lower noise levels than its TE cooled competitors. Initially designed for demanding faint flux applications such as hyperspectral imaging, our cameras are well-suited for spectroscopy, astronomy or industrial applications in quality control and sorting.

 

ZEPHIR 1.7

Based on a sensitive InGaAs FPA, and integrating a four-stage TE cooler, ZephIR 1.7™ delivers an astounding 200 frame-per-second rate while reaching unrivalled low noise levels. Perfectly adapted for challenging scientific applications.

  • 220 frame-per-second
  • 4-stages TEC
  • Low noise level
  • InGaAs FPA
  • Optimal from 0.8 to 1.7 µm

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ZEPHIR 2.5

Based on a sensitive HgCdTe FPA, and integrating a four-stage TE cooler, ZephIR™ delivers an astounding 340 frame-per-second rate while reaching unrivalled low noise levels. Perfectly adapted for industrial applications in quality control and sorting as well as for scientific research.

  • 340 frame-per-second
  • 4 stages TEC
  • Low noise level
  • HgCdTe (MCT) FPA
  • 0.85 to 2.5 µm

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ZEPHIR 2.9

Based on a sensitive HgCdTe FPA, and integrating a four-stage TE cooler, ZephIR delivers an astounding 340 frame-per-second rate while reaching unrivalled low noise levels. Perfectly adapted for industrial applications in quality control and sorting as well as for scientific research.

  • 340 frame-per-second
  • 4 stages TEC
  • Low noise level
  • HgCdTe (MCT) FPA
  • 0.85 to 2.9 µm

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ALIZÉ™ 1.7 CAMERA

ALIZE? 1.7 CAMERA

Alizé™ 1.7 InGaAs Camera

Continuing its push to extend the boundaries of scientific and industrial imaging, Photon etc. presents its high performance, quality for value, air-cooled SWIR camera line. Based on a sensitive InGaAs FPA and integrating a four-stage TE cooler, Alizé™ 1.7 delivers an astounding 190 frame-per-second rate while reaching very low noise levels. First designed for demanding faint-flux applications such as small animal imaging in the second biological window, these cameras also bring new capabilities for industrial applications in quality control and sorting.

CHARACTERISTICS

  • 220 frame-per-second
  • 4-stages TEC
  • Low noise level
  • InGaAs FPA

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Accessories- HypIRia™ Objective lenses

The HypIRia™ are the only telecentric objective lenses optimized for 1 to 2.9 µm. Designed for machine vision and industrial applications, their heavy duty stainless steel and aluminum housing makes them quite resistant to harsh environment. They are well-suited for high-end scientific applications, mostly with spectroscopy or multiband due to their wide field and telecentrism. They succeed at providing a wide aperture over such a long spectral range while still limiting distortion and chromatism. This wide aperture allows an amazing throughput which offers high quality imaging even for low-light imaging. All surfaces have an anti-reflective broadband coating effective over the whole spectral range. The manual fine focus allows for a very precise adjustments of the image. They come in three different focal lengths (11 mm, 15 mm and 25 mm) and their input ports (SM1 and M45) can easily be coupled with standard filters and protective windows. The H11 has a particularily wide field of view, making it stand out even more.

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