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Ultra‐Steep‐Slope High‐Gain MoS(2) Transistors with Atomic Threshold‐Switching Gate

The fundamental Boltzmann limitation dictates the ultimate limit of subthreshold swing (SS) to be 60 mV dec(−1), which prevents the continued scaling of supply voltage. With atomically thin body, 2D semiconductors provide new possibilities for advanced low‐power electronics. Herein, ultra‐steep‐slop...

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Detalles Bibliográficos
Autores principales: Lin, Jun, Chen, Xiaozhang, Duan, Xinpei, Yu, Zhiming, Niu, Wencheng, Zhang, Mingliang, Liu, Chang, Li, Guoli, Liu, Yuan, Liu, Xingqiang, Zhou, Peng, Liao, Lei
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8922111/
https://www.ncbi.nlm.nih.gov/pubmed/35038247
http://dx.doi.org/10.1002/advs.202104439
Descripción
Sumario:The fundamental Boltzmann limitation dictates the ultimate limit of subthreshold swing (SS) to be 60 mV dec(−1), which prevents the continued scaling of supply voltage. With atomically thin body, 2D semiconductors provide new possibilities for advanced low‐power electronics. Herein, ultra‐steep‐slope MoS(2) resistive‐gate field‐effect transistors (RG‐FETs) by integrating atomic‐scale‐resistive filamentary with conventional MoS(2) transistors, demonstrating an ultra‐low SS below 1 mV dec(−1) at room temperature are reported. The abrupt resistance transition of the nanoscale‐resistive filamentary ensures dramatic change in gate potential, and switches the device on and off, leading to ultra‐steep SS. Simultaneously, RG‐FETs demonstrate a high on/off ratio of 2.76 × 10(7) with superior reproducibility and reliability. With the ultra‐steep SS, the RG‐FETs can be readily employed to construct logic inverter with an ultra‐high gain ≈2000, indicating exciting potential for future low‐power electronics and monolithic integration.