1 / 15

Design and Implementation of VLSI Systems (EN0160)

Design and Implementation of VLSI Systems (EN0160). Sherief Reda Division of Engineering, Brown University Spring 2007. [sources: Weste/Addison Wesley – Rabaey Pearson]. Last time Gate layouts and stick diagrams This time MOS transistor theory (ideal case).

bethan
Download Presentation

Design and Implementation of VLSI Systems (EN0160)

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. Design and Implementation of VLSI Systems (EN0160) Sherief Reda Division of Engineering, Brown University Spring 2007 [sources: Weste/Addison Wesley – Rabaey Pearson]

  2. Last time Gate layouts and stick diagrams This time MOS transistor theory (ideal case) Lecture05: MOS transistor theory

  3. gate-oxide-body sandwich = capacitor • Operating modes • Accumulation • Depletion • Inversion • The charge accumulated is proportional to the excess gate-channel voltage (Vgc-Vt)

  4. Cut off Vgs < Vt • Linear (resistor): Vgs > Vt & Vds < Vgs-Vt NMOS transistor, 0.25um, Ld = 10um, W/L = 1.5, VDD = 2.5V, VT = 0.4V Current α Vds • Saturation: Vgs > Vt and Vds ≥ Vgs-Vt Current is independent of Vds The MOS transistor has three regions of operation

  5. MOS structure looks like parallel plate capacitor while operating in inversion Gate – oxide – channel Qchannel = CV C = εoxWL/tox = CoxWL (where Cox=εox/tox) V = Vgc – Vt = (Vgs – Vds/2) – Vt How to calculate the current value?

  6. Charge is carried by electrons Carrier velocity v proportional to lateral E-field between source and drain v = μE μ called mobility E = Vds/L Time for carrier to cross channel: t = L / v Carrier velocity is a factor in determining the current

  7. Now we know How much charge Qchannel is in the channel How much time t each carrier takes to cross I=Q/t

  8. Can be ignored for small Vds In linear mode (Vgs > Vt & Vds < Vgs-Vt) • For a given Vgs, Ids is proportional (linear) to Vds

  9. In saturation mode (Vgs > Vt and Vds ≥ Vgs-Vt) • Now drain voltage no longer increases current

  10. Operation modes summary • 0.6 micron process • tox = 100 Å • m = 350 cm2/V*s • Vt = 0.7 V • W/L = 4/2 l

  11. PMOS is similar

  12. What happens when we construct a INV (PMOS+NMOS)?

  13. Inverter voltage transfer function A B C E D

  14. This lecture Ideal transistor modeling Next lecture Non ideal transistor modeling Summary

  15. Inverter current transfer function

More Related