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Photothermoelectric and photovoltaic effects both present in MoS(2)
As a finite-energy-bandgap alternative to graphene, semiconducting molybdenum disulfide (MoS(2)) has recently attracted extensive interest for energy and sensor applications. In particular for broad-spectral photodetectors, multilayer MoS(2) is more appealing than its monolayer counterpart. However,...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4300500/ https://www.ncbi.nlm.nih.gov/pubmed/25605348 http://dx.doi.org/10.1038/srep07938 |
Sumario: | As a finite-energy-bandgap alternative to graphene, semiconducting molybdenum disulfide (MoS(2)) has recently attracted extensive interest for energy and sensor applications. In particular for broad-spectral photodetectors, multilayer MoS(2) is more appealing than its monolayer counterpart. However, little is understood regarding the physics underlying the photoresponse of multilayer MoS(2). Here, we employ scanning photocurrent microscopy to identify the nature of photocurrent generated in multilayer MoS(2) transistors. The generation and transport of photocurrent in multilayer MoS(2) are found to differ from those in other low-dimensional materials that only contribute with either photovoltaic effect (PVE) or photothermoelectric effect (PTE). In multilayer MoS(2), the PVE at the MoS(2)-metal interface dominates in the accumulation regime whereas the hot-carrier-assisted PTE prevails in the depletion regime. Besides, the anomalously large Seebeck coefficient observed in multilayer MoS(2), which has also been reported by others, is caused by hot photo-excited carriers that are not in thermal equilibrium with the MoS(2) lattice. |
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