RIMA™ |
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EXCITATION |
532 nm | 660 nm | 785 nm |
SPECTRAL RANGE | 190 - 4000 cm-1 | 100 - 4000 cm-1 | 130 - 3200 cm-1 |
SPECTRAL RESOLUTION | < 7 cm-1 | ||
WAVELENGTH ABSOLUTE ACCURACY | 1 cm-1 | ||
MICROSCOPE | Upright or Inverted; Scientific Grade | ||
OBJECTIVES | 20X, 50X, 60X, 100X | ||
SPATIAL RESOLUTION | Sub-micron (limited by the microscope objective N.A.) |
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MAXIMUM SCANNING SPEED |
250 µm2/min at full spectral range | ||
CAMERA* | CCD, EMCCD, sCMOS (Color 3Mp Camera available) |
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VIDEO MODE | Megapixel camera for sample vizualisation | ||
PREPROCESSING | Spatial filtering, statistical tools, spectrum extraction, data normalization, spectral calibration, overlay, central position map, etc. | ||
HYPERSPECTRAL DATA FORMAT |
HDF5, FITS | ||
SINGLE IMAGE DATA FORMAT |
HDF5, CSV, JPG, PNG, TIFF | ||
SOFTWARE | PHySpec™ control and analysis (computer included) | ||
DIMENSIONS | ≅ 150 cm x 85 cm 82 cm | ||
WEIGHT | ≅ 80 kg | ||
UPGRADES |
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SPECTRAL EXTENTION |
Anti-Stokes |
Photon etc.'s Global Imaging Technology
This video shows the conceptual difference between hyperspectral global imaging and raster scan (line-scan, push-broom). With global imaging, the gain in acquiring 3D data, 2D spatial and 1D spectral, is important since only a few monochromatic images are required to cover the complete spectral range where one needs to take the full spectrum for each point or line in the image with other technologies.