the improvement of information density and functionality of metasurfaces. There are several examples reported so far for full-space light manipulation (more details are provided in Section S1 of the Supporting Information). For instance, the random point generator is a typical example of full-space meta-devices, [51] which can generate light spot arrays in both reflection and transmission spaces, but it is not helpful to increase the information capacity because of the spatial symmetry of scattering points. To asymmetrically cover transmission and reflection spaces, off-axis illumination [52] and planar interleaving [53] were proposed for realizing trans-reflective light-manipulation, but these designs are at the cost of the reduced information density. Meanwhile, their coupled transmitted and reflected phases will interfere with each other, which results in crosstalk. The polarization multiplexing [54] and the combination of multipolar interference and geometric phase [55] can achieve independent modulation of trans-reflective phases. Unfortunately, the unwanted amplitude variations are introduced in the modulation process, which results in performance deterioration and decreased tolerance against fabrication errors. Therefore, a new method is required to realize full-space light manipulation toward high information density, low crosstalk, and total independence.In recent years, multilayer metasurfaces have been studied to form novel optical devices such as multispectral achromatic optical devices, [56,57] color displays, [58] asymmetric devices, [59] multifocal metalenses, [60,61] and multifunctional meta-devices, [62] which benefit from the significantly increased degrees of freedom gifted by multilayer metasurfaces. However, it is difficult to use multilayered structures to form accurate and arbitrary phase-only devices such as holograms, especially in the visible range, on account of the fabrication difficulty of subwavelength multilayer nanostructures increases greatly with the shorter wavelength. Here, based on precise nano fabrication technology, we focus on expanding the light manipulation space and propose a bilayer metasurface that can independently manipulate the phase of visible light in the reflection and transmission spaces. In our design, each unit-cell of the bilayer metasurface consists of two subwavelength-scale anisotropic nanobricks, configured along the direction of optical axis. Based on geometric phase or so-called Pancharatnam-Berry (P-B) phase theory, the orientation angles of anisotropic nanobricks Light manipulation with metasurfaces is usually implemented in either transmission or reflection space. Since the other half-space is abandoned, it may hinder the improvement of information capacity and functionality of metasurfaces. Previously reported works have showcased some attempts to modulate trans-reflective phase for full-space light manipulation. However, they either fail to realize complete decoupling or introduce unwanted amplitude variation, which leads to the performance deterio...