New prospects on high on-current and steep subthreshold slope for innovative Tunnel FET architectures. (September 2019)

• Record Type: Journal Article
• Authors: Diaz Llorente, C.; Colinge, J.-P.; Martinie, S.; Cristoloveanu, S.; Wan, J.; Le Royer, C.; Ghibaudo, G.; Vinet, M.
• Is Part Of: Solid-state electronics. Volume 159(2019)
• Page Start: 26
• Page End: 37
• Publication Date: 2019-09
• Subjects: Tunnel FET -- SOI -- Tunneling -- BTBT -- Extended-Source -- Pure Boron; Semiconductors -- Periodicals; Semiconducteurs -- Périodiques; 621.38152
• DOI: 10.1016/j.sse.2019.03.046
• Languages: English
• ISSNs: 0038-1101

Abstract

Abstract: We propose three innovative SOI Tunnel FET architectures to solve the recurrent issue of low ION and degraded subthreshold slope measured on TFETs. These are evaluated and compared with a standard TFET structure (with lateral tunneling) using the Sentaurus TCAD tool. Extending the source (anode) at the bottom of the body region generates vertical band-to-band tunneling. Moreover, reducing the vertical distance between the extension and the gate oxide (Lrt ) yields a very steep slope and higher ION compared to a device with only lateral tunneling, but only for gate lengths longer than 100 nm. Using an ultrahigh boron dopant concentration (10 21 cm −3 ) thin layer at the bottom for extremely small body thickness (TSi < 7 nm), increases ION even for small gate lengths (LG < 100 nm). The implementation of an embedded tip in the source enhances the maximum electric field at the source/channel junction, but the impact on the performance is limited because the tunneling area is not increased. Therefore, this architecture provides a performance similar to a standard TFET. TCAD simulations using SiGe with different germanium concentrations (30% and 50%) and pure germanium, instead of silicon, show an increase of the interband tunneling current when using an ultrahigh dopant concentration thin boron layer for small gate lengths (LG < 50 nm). The reduction of the tunneling current using a relatively thick channel (11–7 nm) can be compensated by using a higher germanium concentration to reduce the energy bandgap. However, this will increase the density of defects causing a TAT tunneling instead of interband tunneling, jeopardizing the possibility of achieving a subthreshold swing below 60 mV/dec.