but more importantly, on the electrode microstructures on the composite level. As a result, optimizing the electrode microstructures to achieve fast and stable ion/ electron transport for every individual AM particle is another urgent but challenging mission. [1,2] This challenge fundamentally comes from a poor understanding of the electrode microstructures and their formation process, which are sensitive to many factors, such as binder properties, slurry compositions, and electrode processing conditions. As an attempt to better understand the electrode microstructures, as illustrated in Figure 1a, we have recently got the inspiration of the concept of cell microenvironment well-known in biology, and proposed the concept of active material microenvironment (ME@AM). [2][3][4] Specifically, ME@AM is defined as the local non-active-material environment connecting the tested AM particle with its neighboring AM particles (see Figure 1b). The ME@AM skeleton consists of two primary parts: the local electron transport structure built by mainly the conductive agent (CA) and the ion transport channels determined by the pores around the AM particle, which are left for liquid electrolyte, [4][5][6] or directly built by solid electrolytes. Since the available capacity of AMs is fundamentally determined by the redox reaction of all the AM particles, it is reasonable to link the quality of ME@AM skeleton to the overall electrochemical performance, such as C-rate performance, specific capacity, energy density, cycle stability, mechanical properties, and so on. [3] The ME@AM focuses on both ionic and electronic conduction structures surrounding an individual AM particle. For high-quality electrodes, all the AM particles should be uniformly surrounded by "healthy" ME@AM skeleton with uniformly distributed CA and stable AM/CA interface. When the porous structures of ME@AM skeleton is filled by an electrolyte, the ionic conduction function of ME@AM is finally built. Thus, the features of the porous structure of the CA network, including porosity, pore tortuosity, and pore size, are all critical for the ME@AM capability of ionic conduction. It should be noted that the quality of ME@AM is a collective result contributed by many factors, such as electrode composition, [7][8][9] characteristics of Similar to the cell microenvironment in biology, the active material microenvironment (ME@AM) in battery electrodes determines the charge flux into/out the individual AM particles, and the overall device performance thereby. However, it is very challenging to understand and regulate the ME@AM structures due to the lack of advanced binders and their links to electrode microstructures. Here, to address this challenge, a high-performance sol-binder based on propylene carbonate (PC) and poly(vinylidene fluoride) is designed and the ME@AM structural evolution during its electrode fabrication is investigated. First, a pen-ink-like uniform slurry is successfully prepared in minutes with the PC solvent. Second, the sol-to-gel transition of the sol-bin...