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Probing the Importance of Charge Balance and Noise Current in WSe(2)/WS(2)/MoS(2) van der Waals Heterojunction Phototransistors by Selective Electrostatic Doping

Heterojunction structures using 2D materials are promising building blocks for electronic and optoelectronic devices. The limitations of conventional silicon photodetectors and energy devices are able to be overcome by exploiting quantum tunneling and adjusting charge balance in 2D p–n and n–n junct...

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Detalles Bibliográficos
Autores principales: Ra, Hyun‐Soo, Jeong, Min‐Hye, Yoon, Taegeun, Kim, Seungsoo, Song, Young Jae, Lee, Jong‐Soo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7539183/
https://www.ncbi.nlm.nih.gov/pubmed/33042759
http://dx.doi.org/10.1002/advs.202001475
Descripción
Sumario:Heterojunction structures using 2D materials are promising building blocks for electronic and optoelectronic devices. The limitations of conventional silicon photodetectors and energy devices are able to be overcome by exploiting quantum tunneling and adjusting charge balance in 2D p–n and n–n junctions. Enhanced photoresponsivity in 2D heterojunction devices can be obtained with WSe(2) and BP as p‐type semiconductors and MoS(2) and WS(2) as n‐type semiconductors. In this study, the relationship between photocurrent and the charge balance of electrons and holes in van der Waals heterojunctions is investigated. To observe this phenomenon, a p‐WSe(2)/n‐WS(2)/n‐MoS(2) heterojunction device with both p–n and n–n junctions is fabricated. The device can modulate the charge carrier balance between heterojunction layers to generate photocurrent upon illumination by selectively applying electrostatic doping to a specific layer. Using photocurrent mapping, the operating transition zones for the device is demonstrated, allowing to accurately identify the locations where photocurrent generates. Finally, the origins of flicker and shot noise at the different semiconductor interfaces are analyzed to understand their effect on the photoresponsivity and detectivity of unit active area (2.5 µm(2), λ = 405 nm) in the p‐WSe(2)/n‐WS(2)/n‐MoS(2) heterojunction device.