Optimizing hydrogen evolution performance through balancing charge dynamics across sulfur-defect-engineered CdIn2S4-NC/MoC heterojunctions
Related Experiment Video
Updated: Jul 28, 2026

Harvesting Solar Energy by Means of Charge-Separating Nanocrystals and Their Solids
Published on: August 23, 2012
Siyi Zhang1, Ni Hu1, Hui Su1
1School of Science, Hubei University of Technology, Wuhan 430068, PR China.
Abstract:
Designing efficient photocatalysts with heterojunctions is key to enhancing photocatalysis. Ignoring surface states hinders understanding of heterojunction performance, and balancing charge dynamics is crucial for optimizing photocatalytic hydrogen evolution (PHE) activity. We fabricated a Schottky junction composite featuring a dual-metal system, which consists of sulfur-defect-engineered CdIn2S4 (CIS) combined with a hollow N-doped carbon (NC)-anchored MoC heterojunction. The optimal CdIn2S4/NC/MoC (25CIS-CM) composite achieves a remarkable 58.2-fold enhancement in PHE rate compared to bare CIS under visible illumination. In-situ femtosecond transient absorption (fs-TA) measurements has shown that some thermalized electrons get trapped by shallow defects on the surface in pure CIS about 24.342 ps, while others transition into inter-bandgap trap states, exhibiting a relaxation time τ3 of approximately 282.207 ps. As the CM loading increases, τ3 gradually decreases (282.207 ps → 160.820 ps → 72.471 ps → 61.33 ps). And most higher loading of CM (50CIS-CM) results in a faster photogenerated carrier recombination time (τ4 = 2861.46 ps), ultimately causing a diminished rate for 50CIS-CM during PHE. The balance between charge trapping at shallow and deep energy levels, carrier interfacial migration, and band-edge recombination deepens our understanding of the photocatalytic mechanism of CIS-based heterojunctions and ultimately promoting the rapid development of green energy technologies.
More Related Videos
Related Concept Videos
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Imperfections in Crystal Structure: Stoichiometric Point Defects
Imperfections in Crystal Structure: Non-Stoichiometric Defects

