Design and Implementation of VLSI Systems EN 1600

  • Slides: 13
Download presentation
Design and Implementation of VLSI Systems (EN 1600) Lecture 08 Prof. Sherief Reda Division

Design and Implementation of VLSI Systems (EN 1600) Lecture 08 Prof. Sherief Reda Division of Engineering, Brown University Spring 2008 [sources: Weste/Addison Wesley – Rabaey/Pearson]

Summary of Shockley model for n. MOS for p. MOS

Summary of Shockley model for n. MOS for p. MOS

Ideal vs. non-ideal Non-ideal § Saturation current does not increase quadratically with Vgs §

Ideal vs. non-ideal Non-ideal § Saturation current does not increase quadratically with Vgs § Saturation current lightly increases with increase in Vds

Ideal vs. non-ideal § There is leakage current when the transistor is in cut

Ideal vs. non-ideal § There is leakage current when the transistor is in cut off § Ids depends on the temperature

At high electric field, drift velocity rolls of due to carrier scattering u n

At high electric field, drift velocity rolls of due to carrier scattering u n (m /s) Velocity saturation usat= 105 Constant velocity Constant mobility (slope = µ) xc = 1. 5 Empirically: x (V/µm)

Alpha model Pc, Pv and alpha are found by fitting the model to the

Alpha model Pc, Pv and alpha are found by fitting the model to the empirical modeling results

Channel length modulation • The reverse-bias p-n junction between drain and body forms a

Channel length modulation • The reverse-bias p-n junction between drain and body forms a depletion region with a width Ld that increases with Vdb • Increasing Vds Ø increases depletion width Ø decreases effective channel length Ø increases current Channel length modulation factor (empirical factor)

Leakage current: subthreshold Tunnel current polysilicon gate W t ox n+ L p-type body

Leakage current: subthreshold Tunnel current polysilicon gate W t ox n+ L p-type body n+ Subthreshold conduction Junction leakage q Subthreshold leakage is the biggest source in modern transistors n = 1. 4 -15 180 nm process

Leakage current: junction leakage and tunneling Junction leakage: reverse-biased p-n junctions have some leakage.

Leakage current: junction leakage and tunneling Junction leakage: reverse-biased p-n junctions have some leakage. Is depends on doping levels and area and perimeter of diffusion regions Tunneling leakage: § Carriers may tunnel thorough very thin gate oxides § Negligible for older processes (and future processes with high-k dielectrics!)

Impact of temperature • Increases in temperature increases leakage current • Increases in temperature

Impact of temperature • Increases in temperature increases leakage current • Increases in temperature decreases leakage current

Body effect § Vt is sensitive to Vsb -> body effect • What is

Body effect § Vt is sensitive to Vsb -> body effect • What is the impact on Vt if we increase/decrease the body bias?

Process variations Both MOSFETs have 30 nm channel with 130 dopant atoms in the

Process variations Both MOSFETs have 30 nm channel with 130 dopant atoms in the channel depletion region threshold voltage 0. 97 V threshold voltage 0. 57 V Process variations impact gate length, threshold voltage, and oxide thickness

Summary § § Ideal transistor characteristics Non-ideal transistor characteristics Inverter DC transfer characteristics Simulation

Summary § § Ideal transistor characteristics Non-ideal transistor characteristics Inverter DC transfer characteristics Simulation with SPICE and integration with L-Edit