Photocatalytic performance for hydrogen evolution. a) PHE rates with different samples under visible light (λ > 420 nm, Na2S/Na2SO3 as a scavenger). b) Time courses of PHE on Cu–ZIS, Pt1/Cu–ZIS, and Pnc/ZIS. Error bars represent standard deviations from triplicate experiments (n = 3). c) Recycling performance for Pt1/Cu–ZIS. d) PHE of Pt1/Cu–ZIS with and without KSCN, indicating that SCN‐ions strongly poison Pt1/Cu–ZIS.

Photocatalytic performance for hydrogen evolution. a) PHE rates with different samples under visible light (λ > 420 nm, Na2S/Na2SO3 as a scavenger). b) Time courses of PHE on Cu–ZIS, Pt1/Cu–ZIS, and Pnc/ZIS. Error bars represent standard deviations from triplicate experiments (n = 3). c) Recycling performance for Pt1/Cu–ZIS. d) PHE of Pt1/Cu–ZIS with and without KSCN, indicating that SCN‐ions strongly poison Pt1/Cu–ZIS.

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Single-atom photocatalysts have shown their fascinating strengths in enhancing charge transfer dynamics; however, rationally designing coordination sites by metal doping to stabilize isolated atoms is still challenging. Here, a one-unit-cell ZnIn2S4 (ZIS) nanosheet with abundant Cu dopants serving as the suitable support to achieve a single atom Pt...

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... [17] Cocatalyst loading is feasible for resolving the aforementioned dilemma as it facilitates the charge-carrier separation. [18,19] Particularly, constructing the interfacial chemical bond between photocatalyst and cocatalyst provides the rapid channels at the atomic level, which reinforces the interfacial interaction with cocatalyst for accelerating the charge transfer with lower energy barrier. [20,21] The smooth construction of the above structure is highly dependent on the lattice matching between the photocatalyst and the cocatalyst. ...
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