Next to polymer electrolytes, [2] inorganic Li-ion SEs have been developed in recent years. [3] Thiophosphates, garnets, or argyrodites are the most promising inorganic materials classes, each having particular advantages and disadvantages. Despite the considerable improvement in Li + conductivity (some structures exhibit a higher conductivity than liquid electrolytes) the limited electrochemical stability window of SEs often leads to side reactions with low potential negative and high potential positive materials. [4] For this reason, in research studies the lithium negative electrode is often replaced by an In-Li alloy as this alloy provides a more stable interface with many SEs and prevents dendrite formation. [5] The use of Li as negative electrode in SSBs, however, remains an important goal as this is one of the few options to significantly increase the specific energy (Wh kg −1) and energy density (Wh L −1) of the cell. Considering positive electrode materials, the large family of layered oxides is mostly studied as their overall superior behavior is well-known from LIBs. However, also conversion-type materials such as TiS 2 , [6] CoS, [7] FeS 2 , [8] MoS 2 , [9] and NiS [10] are studied due to their much higher specific capacity. An important aspect of SSBs is the preparation of dense cathode composite structures containing SE, active material and, where needed, additives. Close contact between the phases and a suitable 3D structure is required to minimize the Copper sulfide (CuS) is an attractive electrode material for batteries, thanks to its intrinsic mixed conductivity, ductility and high theoretical specific capacity of 560 mAh g −1. Here, CuS is studied as cathode material in lithium solid-state batteries with an areal loading of 8.9 mg cm −2 that theoretically corresponds to 4.9 mAh cm −2. The configuration of the cell is LiLi 3 PS 4 [CuS (70 wt%) + Li 3 PS 4 (30 wt%)]. No conductive additive is used. CuS undergoes a displacement reaction with lithium, leading to macroscopic phase separation between the discharge products Cu and Li 2 S. In particular, Cu forms a network of micrometer-sized, well-crystallized particles that seems to percolate through the electrode. The formed copper is visible to the naked eye. The initial specific discharge capacity at 0.1 C is 498 mAh g(CuS) −1 , i.e., 84% of its theoretical value. The initial Coulomb efficiency (ICE) reaches 95%, which is higher compared to standard carbonate-based liquid electrolytes for the same cell chemistry (≈70%). After 100 cycles, the specific capacity reaches 310 mAh g(CuS) −1. With the current composition, the cell provides 58.2 Wh kg −1 at a power density of 7 W kg −1 , which is superior compared to other transition metal sulfide cathodes.