Among p–n junction devices with multilayered heterostructures with WSe 2 and MoSe 2, a device with the MoSe 2 –WSe 2 –MoSe 2 (NPN) structure showed a remarkably high photoresponse, which was 1000 times higher than the MoSe 2 –WSe 2 (NP) structure. The ideality factor of the NPN structure was estimated to be ∼1, lower than that of the NP structure. It is claimed that the NPN structure formed a thinner depletion region than that of the NP structure because of the difference of carrier concentrations of MoSe 2 and WSe 2 . Hence, the built-in electric field was weaker, and the motion of the photocarriers was facilitated. These behaviors were confirmed experimentally from a photocurrent mapping analysis and Kelvin probe force microscopy. The work function depended on the wavelength of the illuminator, and quasi-Fermi level was estimated. The surface photovoltage on the MoSe 2 region was higher than that on WSe 2 because the lower bandgap of MoSe 2 induces more electron–hole pair generation.
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Choi et al. (2020) studied this question.
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