1 / 11

IEE5328 Nanodevice Transport Theory and Computational Tools

IEE5328 Nanodevice Transport Theory and Computational Tools. (Advanced Device Physics with emphasis on hands-on calculations). Lecture #4: Ballistic I-V in 2DEG and 2DHG. Prof. Ming-Jer Chen Dept. Electronics Engineering National Chiao-Tung University

natara
Download Presentation

IEE5328 Nanodevice Transport Theory and Computational Tools

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. IEE5328 Nanodevice Transport Theory and Computational Tools (Advanced Device Physics with emphasis on hands-on calculations) Lecture #4: Ballistic I-V in 2DEG and 2DHG Prof. Ming-Jer Chen Dept. Electronics Engineering National Chiao-Tung University April 10, 2013

  2. High-Performance FETs projected by ITRS 2011 (http://www.itrs.net) Idsat (Multi-Gates and SOI) IEE5328 Prof. MJ Chen NCTU

  3. High-Performance FETs projected by ITRS 2011 (http://www.itrs.net) Idsat (Multi-Gates and SOI) IEE5328 Prof. MJ Chen NCTU

  4. Low-Power NanoFETs projected by ITRS 2011 (http://www.itrs.net) (Bulk, SOI, and Multi-Gates) IEE5328 Prof. MJ Chen NCTU

  5. Low-Power NanoFETs projected by ITRS 2011 (http://www.itrs.net) (Bulk, SOI, and Multi-Gates) IEE5328 Prof. MJ Chen NCTU

  6. Key Words: Iballistic is simply due to thermionic injection over the source-channel barrier Iballistic is Idsat you can theoretically obtain But, Iballistic is usually much higher than Idsat you can experimentally obtain • This difference is due to a handful of physical phenomena: • Effective Mobility and its reduction with channel length shrinkage • Backscattering in channel, in drain, and even in source • (rc well known in the channel) • Rsd • Injection Velocity • Source starvation • Off-equilibrium transport How can we shorten this gap such as to make experimental Idsat close to theoretical Iballistic?

  7. Two Basic Ways to calculate Iballistic: • Band Structure • 2. MOS Electrostatics Here, we focus on 2D case or the inversion layers of MOSFETs 2DEG: two-dimensional electron gas 2DHG: two-dimensional hole gas

  8. 2DEG or 2DHG Originally derived by Prof. Natori

  9. Further Reading: F.Assad, et al., “On the performance limits for Si MOSFET’s: A theoretical study,” IEEE Trans. Electron Devices, vol. 47, pp. 232-240, Jan. 2000.

More Related