Sharp optics and low distortions
HySpex Mjolnir offers extremely sharp optics per pixel and per spectral band for both the VNIR and SWIR spectral range. The V-1240 has 1240 spatial pixels and 400 bands, and the spatial resolution (FWHM) is as low as 1.1 times the spatial sampling. Spectrally, the resolution (FWHM) at 400 bands is 1.5 times the spectral sampling across the whole FOV and spectral range, yielding extremely sharp images. With these specifications, the cameras have less than 10% of a band smile and less than 10% of a pixel keystone.
The S-620 has 620 spatial pixels and 300 spectral bands in the SWIR spectral range. The sharpness, keystone and smile effect is comparable or even better than the V-1240. The keystone and smile specifications of a hyperspectral system are some of the most important specifications of a hyperspectral camera. At the same time, they are among the parameters that get overlooked most frequently in a selection phase.
Keystone in a data set will generate unphysical spectra.
A camera, specified to have 1240 pixels should be expected to be able to record 1240 unique and correct spectral signatures – reproducing the real radiance from each pixel in the scene.
Some suppliers offer solutions specified to have 50% or more keystone. A camera with 50% keystone, will acquire data where 50% of the spectral signature in a given pixel originates from the pixel next to it. This is different from the linear mixture of two spectral signatures recorded by a pixel containing two different objects.
The keystone effect in the data will have some part of the spectral signature coming from one of the objects, while other parts of the spectra have a 50% influence from the object next to it – in essence generating an unphysical spectral signature. This effect will effectively reduce the spatial resolution, and larger objects are required to get one pure pixel. Keystone will also introduce effects like misidentification/classification or false alarms in your data product.
Detector with high speed and low noise floor
A small hyperspectral system will smaller pixel pitch on the detector than larger camera. This implies a smaller full well (charge capacity) on the detector pixels. In combination with having a high light throughput in the optics, it is also important to have a very low noise floor (read noise) on the detector. Lower noise floor means a higher dynamic range in the images.
As an example, the Mjolnir V-1240 has 2.3 electrons noise floor. Assume this system is mounted on a fixed-wing UAV flying at low altitude (i.e. short integration time), with a low sun angle yielding very challenging conditions with a lot of shadows. In the acquired data, the signal acquired from the shaded scene generates 24 photoelectrons in one pixel and band. Mjolnir V-1240, with the 2.3 electrons noise floor, will have an SNR of 10.43 for this signal. A noisier system, however, with e.g. 13 electrons read noise, will only have an SNR of 1.85, if all other parameters are identical.
Good SNR across the full spectral range
A smaller pixel pitch (to scale down the system size) means smaller full well, compared to systems with larger pitch. A smaller full well will give a smaller peak SNR. Peak SNR is approximately the square root of the full well if the noise floor is small. The full well of the detector used for V-1240 is about 10000 electrons, yielding a peak SNR of approximately 100 in the native sensor resolution. To get higher SNR, the dispersion in the camera covers more bands than the output cube. This is a good solution if the read noise is sufficiently low. For Mjolnir V-1240, 3.24 pixels are binned together, which effectively increase the full well with a factor 3.24. The peak SNR is thus about 180 at the full output resolution (1240 pixels x 400 bands). This will, of course, increase the readout noise; however, not more than approximately 4.14 electrons – which is still very good. The peak SNR alone is of limited use as it only indicates the maximum SNR obtained in a band that is close to saturation, but the total quantum efficiency of the whole system as a function of wavelength is also needed.
To obtain really useful information, the SNR curve needs to be specified for a given input radiance and a given (and operationally realistic) integration time. This information should be part of any test report for any system. A poorly designed system can be specified for the full range 400-1000nm, and have a decent peak SNR in the middle of the spectral range, but still, be unusable for several tens of nanometers at the start and end of the spectral range. A qualitative assessment of the SNR characteristics can be done by viewing single-band images at the edges of the spectral range of the system, as shown in the figure below.