I. Introduction
Hyperspectral images (HSIs) with a large number of spectral bands have gained immense attention in the field of remote sensing due to its applications in broad research areas such as classification [1], unmixing [2], anomaly detection [3], change detection [4], etc. However, due to the limited incident energy available when capturing an image, hyperspectral imaging systems face tradeoffs between spectral resolution, spatial resolution, and signal-to-noise ratio (SNR) [5]. For this reason, hyperspectral imaging systems can provide images with high spectral resolution but with low spatial resolution. In contrast, multispectral imaging systems can provide data with high spatial resolution but with fewer spectral bands (e.g., panchromatic images or multispectral images (MSIs) with three or four spectral bands). Low spatial resolution in HSIs leads to relatively poor performance in some practical remote sensing applications, such as road topology extraction [6], and spectral unmixing [7]. Therefore, full-resolution HSIs with high spatial and spectral resolution are desired. One way to obtain such ideal HSIs is to fuse high spectral resolution HSIs with high spatial resolution PAN/MSIs. This fusion process is called HS pansharpening in the remote sensing literature, which is indeed a form of super-resolution [8].