1 / 39

Semiconductor Device Modeling and Characterization – EE5342 Lecture 35 – Spring 2011

Semiconductor Device Modeling and Characterization – EE5342 Lecture 35 – Spring 2011. Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/. Flat-band parameters for p-channel (n-subst). Fully biased p- channel V T calc. p-channel V T for V C = V B = 0. Fig 10.21*.

lynne
Download Presentation

Semiconductor Device Modeling and Characterization – EE5342 Lecture 35 – Spring 2011

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. Semiconductor Device Modeling and Characterization – EE5342 Lecture 35 – Spring 2011 Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/

  2. Flat-band parametersfor p-channel (n-subst)

  3. Fully biased p-channel VT calc

  4. p-channel VT forVC = VB = 0 Fig 10.21*

  5. Ion implantation

  6. “Dotted box” approx

  7. Mobilities

  8. Differential chargesfor low and high freq high freq. From Fig 10.27*

  9. Ideal low-freqC-V relationship Fig 10.25*

  10. Comparison of lowand high freq C-V Fig 10.28*

  11. Effect of Q’ss onthe C-V relationship Fig 10.29*

  12. n-channel enhancementMOSFET in ohmic region 0< VT< VG Channel VS = 0 0< VD< VDS,sat EOx,x> 0 e-e- e- e- e- n+ n+ Depl Reg p-substrate Acceptors VB < 0

  13. Conductance ofinverted channel • Q’n = - C’Ox(VGC-VT) • n’s = C’Ox(VGC-VT)/q, (# inv elect/cm2) • The conductivity sn = (n’s/t) q mn • G = sn(Wt/L) = n’s q mn (W/L) = 1/R, so • I = V/R = dV/dR, dR = dL/(n’sqmnW)

  14. Basic I-V relationfor MOS channel

  15. I-V relation for n-MOS (ohmic reg) ohmic ID non-physical ID,sat saturated VDS VDS,sat

  16. Universal draincharacteristic ID VGS=VT+3V 9ID1 ohmic saturated, VDS>VGS-VT VGS=VT+2V 4ID1 VGS=VT+1V ID1 VDS

  17. Characterizing then-ch MOSFET VD ID D G B S VGS VT

  18. Low field ohmiccharacteristics

  19. MOSFET DeviceStructre Fig. 4-1, M&A*

  20. 4-7a (A&M)

  21. Figure 4-7b (A&M)

  22. Figure 4-8a (A&M)

  23. Figure 4-8b (A&M)

  24. Body effect data Fig 9.9**

  25. MOSFET equivalentcircuit elements Fig 10.51*

  26. n-channel enh.circuit model G RG Cgd RDS Cgs RD S D Cbd RB Cbs Idrain Cgb DSS DSD RB B

  27. MOS small-signal equivalent circuit Fig 10.52*

  28. MOSFET circuitparameters

  29. MOSFET circuitparameters (cont)

  30. Substrate bias effect on VT (body-effect)

  31. Body effect data Fig 9.9**

  32. Fully biased n-channel VT calc

  33. Values for fmswith silicon gate

  34. Q’d,max and xd,max forbiased MOS capacitor Fig 8.11** |Q’d,max|/q (cm-2) xd,max (microns)

  35. I-V relation for n-MOS ohmic ID non-physical ID,sat saturated VDS VDS,sat

  36. MOS channel-length modulation Fig 11.5*

  37. Analysis of channellength modulation

  38. References • CARM = Circuit Analysis Reference Manual, MicroSim Corporation, Irvine, CA, 1995. • M&A = Semiconductor Device Modeling with SPICE, 2nd ed., by Paolo Antognetti and Giuseppe Massobrio, McGraw-Hill, New York, 1993. • **M&K = Device Electronics for Integrated Circuits, 2nd ed., by Richard S. Muller and Theodore I. Kamins, John Wiley and Sons, New York, 1986. • *Semiconductor Physics and Devices, by Donald A. Neamen, Irwin, Chicago, 1997

More Related