Physical Insights Into the Effect of Substrate on Graphene RF Transistor Performance and Demonstration of Novel Inverted T-Gate Architecture
Graphene has emerged as a promising material for future radio frequency (RF) device applications due to its exceptional carrier mobility, high saturation velocity, and atomically thin structure. These properties enable ultra-fast charge transport and excellent electrostatic control, making graphene an attractive candidate for high-frequency and highspeed applications. However, the technology progress is limited by RF performance-killing agents like contact resistance, substrate parasitics, and material-to-device process flow limitations. This work provides a systematic insight into the performance limiters of graphene FETs on SiO2 and SiC substrates, grown via chemical vapor deposition (CVD) and epitaxial methods. Notably, the highest extracted cut-off frequency is 55/20 GHz on the SiC/SiO2 substrate, which reflects the superiority of SiC over SiO2 as a substrate for graphene RF devices. Additionally, the work discusses DC/RF performance degradation issues due to top gate dielectric deposition and demonstrate a unique “ Inverted TGate” device architecture to mitigate the same.
Authors
- Utpreksh Patbhaje (ORCID: https://orcid.org/0009-0000-7648-1080)
- Mayank Shrivastava (ORCID: https://orcid.org/0000-0003-1005-040X)
- Aadil Bashir Dar (ORCID: https://orcid.org/0009-0003-0180-5767)
- Rupali Verma (ORCID: https://orcid.org/0009-0002-7337-3943)
- Jeevesh Kumar (ORCID: https://orcid.org/0000-0001-6178-8434)
- Anand Kumar (ORCID: https://orcid.org/0009-0009-6534-7586)
- Asif A. Shah (ORCID: https://orcid.org/0009-0005-4372-5428)
- A. M.
- Adil Meersha
Institutions
- Indian Institute of Science Bangalore (IN)
Publication Details
- Journal
- IEEE Journal of the Electron Devices Society
- Published
- 2025-01-01
- DOI
- https://doi.org/10.1109/jeds.2025.3591152
- Primary Topic
- Advancements in Semiconductor Devices and Circuit Design
- Type
- article
- Field-Weighted Citation Impact
- 0.00