I. Introduction
With the continuous advancement of global remote sensing technology, enhancing the resolutions of spatial imaging platforms is considered fundamental to the development of Earth observation technology. High-resolution optical remote sensing satellites play crucial roles in the environmental monitoring, disaster response, urban planning, and national security domains [1], [2], [3], [4], [5]. Nevertheless, improving the spatial resolutions of optical remote sensing systems imposes inherent challenges due to physical limitations, particularly the size and mass constraints of satellite platforms. The weight of traditional space optical imaging systems often increases nearly cubically with the increase in aperture size [6], [7]. These space optical imaging systems are critical for capturing high-quality images, yet their weights and volumes are strictly limited due to the capacity constraints of launch vehicles, which can impact launch costs. Moreover, optical systems, including their apertures, focal lengths, and overall architectures, must be designed within these constraints, often at the expense of sacrificing potential resolution enhancements [8], [9], [10], [11].