Mixed ion−electron conductors have a wide range of important applications in devices relying on mixed ion−electron transport, mainly including conducting polymer composites and ceramics. Herein, we present a new type of mixed ion−electron conductor, an open-framework chalcogenide, (H 3 O)KCu 6 Ge 2 S 8 •nH 2 O (1), with a three-dimensional (3D) framework and two types of one-dimensional (1D) channels, occupied by hydronium ions and potassium ions, respectively. Thermogravimetric (TG) and powder X-ray diffraction (PXRD) measurements suggest that the hydrated proton species in the channels of 1 are in the form of H 2n+1 O n + (n > 1). The impedance measurements reveal that 1 is an intrinsic mixed proton− electron conductor. In the N 2 atmosphere, the conductivity (σ) of 1 increases with release of water molecules and increasing temperature with σ = 0.71 S cm −1 at 123 K and 1.61 S cm −1 at 473 K in the first cooling run, and in this case, the electron conduction is much higher than the ion conduction. At 98% relative humidity (RH), however, the situation is opposite, and the proton conductivity of 1 is higher than its electron conduction with an ion conductivity (σ i )/electron conductivity (σ e ), σ i /σ e , of 1.99 × 10 −3 /6.31 × 10 −4 S cm −1 at 298 K and 2.49 × 10 −2 /2.52 × 10 −3 S cm −1 at 343 K. To the best of our knowledge, 1 is the first example of an open-framework material with mixed proton−electron conduction, and this study demonstrates that open-framework materials, including chalcogenides, MOFs, and COFs, are good candidates for mixed proton− electron conductors.