Abstract Near unity photoluminescence quantum yield in monolayer MoS 2 , makes it an excellent candidate for optoelectronic applications. In contrast, bulk MoS 2 experiences a transition from a direct to an indirect bandgap, which diminishes its potential for optoelectronic devices. In this work, the ability to preserve the direct bandgap of MoS 2 while simultaneously enhancing its absorption, mobility, and other optoelectronic properties via stacking monolayers is demonstrated. A scalable method for stacking large‐area monolayer MoS 2 films grown by chemical vapor deposition (CVD) is presented. The approach employs poly(methyl methacrylate) (PMMA) as a carrier polymer and an aluminum mesh to support the films during transfer from the donor to the receiver substrate, maintaining its geometry and preventing folding. The assembled monolayer stacks exhibit a monotonic increase in photoluminescence (PL), absorption, and mobility, while retaining monolayer‐like Raman signatures and a direct bandgap. Notably, a four‐layer stack demonstrates a remarkable increase of more than 225% in PL, 250% in absorption, and 94% in field‐effect mobility compared to single‐monolayer MoS 2 . The preservation of monolayer‐like Raman and direct bandgap behavior in the stacks is attributed to an increased interlayer spacing and twist angle observed between the layers.
Abbas et al. (2025) studied this question.
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