which possess orbital angular momentum associated with helical phase-front. [3][4][5][6] Vector vortex beams (VVBs), as the name implies, possess the properties of both vector beams and vortex beams (i.e., with tailored phase and polarization distribution). The VVBs have been used for particle trapping, [7,8] optical communication, [9] quantum information, [10] high-resolution lithography, [11] etc. However, the applications of VVBs (as well as vortex beams) are limited as their annular intensity profiles vary with their topological charges [12] due to the incapable of amplitude control. This property may cause problems when compositing VVBs, as the intensity profiles of different VVBs cannot closely coincide with each other. To be specific, when the composited VVBs propagate, the state of polarization becomes unstable [13] and the intensity profile collapses, [14] which inevitably limits the co-propagation of multiple VVBs in optical system. Recently, Ostrovsky and co-workers [15] introduced the concept of perfect vortex beam (PVB), which has an annular intensity profile independent of topological charge. Plenty of methods to obtain the PVB have been proposed, such as using spatial light modulator, [15,16] axicon, [17] etc. By combining the generation methods of PVB with the Sagnac interferometer, perfect vector vortex beams (PVVBs) are also demonstrated, [18] which is able to possess stable state of polarization and intensity profiles upon propagation. The generation of PVVBs can be ultimately considered as the success of tailoring the APP of light. However, all these schemes to obtain the PVVBs and PVBs require a large number of bulky optical elements, which cannot be straightforwardly downsized, preventing widespread applications in miniaturized and integrated optical systems.Metasurface is planar structure that can locally manipulate the optical properties of light at subwavelength scales. [19,20] It has been widely used in many areas, including metalens, [21][22][23] holography, [24][25][26][27] vortex beams, [28][29][30][31] VVBs, [32][33][34][35][36][37] etc. However, the generation of VVBs using metasurface cannot realize arbitrary polarization and phase distributions, and mostly of them are limited to linear polarization, [32][33][34][35][36] such as radially or azimuthally polarized beams. Most importantly, all the demonstrated VVBs based on metasurface are not perfect, that is, their annular intensity profiles are dependent on the topological charges.Vector vortex beams (VVBs) possess ubiquitous applications from particle trapping to quantum information. Recently, the bulky optical devices for generating VVBs have been miniaturized by using metasurfaces. Nevertheless, it is quite challenging for the metasurface-generated VVBs to possess arbitrary polarization and phase distributions. More critical is that the VVBs' annular intensity profiles demonstrated hitherto are dependent on topological charges and are hence not perfect, posing difficulties in spatially shared co-propagation of multiple vortex be...