Up to now, the field of PEC water splitting is dominated by inorganic semiconductors consisting of earth abundant elements (e.g., silicon, [7-12] metal oxides, [13-16] metal sulfides, [17,18] dichalcogenide, [19] etc.). However, the high cost and poor stability of noble metal (e.g., Pt) as cocatalysts seriously restrict the practical applications of inorganic semiconductors for the PEC hydrogen evolution reaction (HER). Compared with traditional inorganic semiconductors, organic semiconductors (e.g., graphitic carbon nitride [g-C 3 N 4 or polyheptazine], [20-23] polythiophene, [24,25] conjugated covalent organic frameworks [COFs], [26] conjugated acetylenic polymers [CAPs] [27-29]) have attracted increasing attentions benefitting from their tunable bandgaps, engineered band edge positions, and molecular-level desirable active centers. [6] However, the PEC HER performance of current organic photocathodes falls far behind inorganic counterparts mainly due to their severe recombination of photoinduced holes and electrons. Recently, diverse strategies have been explored for promoting the charge separation of organic semiconductors, mainly focusing on the heterojunction or homojunction As attractive materials for photoeletrochemical hydrogen evolution reaction (PEC HER), conjugated polymers (e.g., conjugated acetylenic polymers [CAPs]) still show poor PEC HER performance due to the associated serious recombination of photogenerated electrons and holes. Herein, taking advantage of the in situ conversion of nanocopper into Cu 2 O on copper cellulose paper during catalyzing of the Glaser coupling reaction, a general strategy for the construction of a CAPs/Cu 2 O Z-scheme heterojunction for PEC water reduction is demonstrated. The as-fabricated poly(2,5-diethynylthieno[3,2-b]thiophene) (pDET)/Cu 2 O Z-scheme heterojunction exhibits a carrier separation efficiency of 16.1% at 0.3 V versus reversible hydrogen electrode (RHE), which is 6.7 and 1.4-times higher respectively than those for pDET and Cu 2 O under AM 1.5G irradiation (100 mW cm −2) in the 0.1 m Na 2 SO 4 aqueous solution. Consequently, the photocurrent of the pDET/Cu 2 O Z-scheme heterojunction reaches ≈520 µA cm −2 at 0.3 V versus RHE, which is much higher than pDET (≈80 µA cm −2), Cu 2 O (≈100 µA cm −2), and the state-of-the-art cocatalyst-free organic or organicsemiconductor-based heterojunctions/homojunctions photocathodes (1-370 µA cm −2). This work advances the design of polymer-based Z-scheme heterojunctions and high-performance organic photoelectrodes.