Presentation is loading. Please wait.

Presentation is loading. Please wait.

Professor Ronald L. Carter

Similar presentations


Presentation on theme: "Professor Ronald L. Carter"— Presentation transcript:

1 Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/
Semiconductor Device Modeling and Characterization – EE5342 Lecture 31 – Spring 2011 Professor Ronald L. Carter

2 Ideal 2-terminal MOS capacitor/diode
conducting gate, area = LW Vgate -xox SiO2 y L silicon substrate tsub Vsub x ©rlc L31-20Apr2011

3 Band models (approx. scale)
metal silicon dioxide p-type s/c Eo qcox ~ 0.95 eV Eo Eo qcSi= 4.05eV qfm= 4.1 eV for Al Ec qfs,p Eg,ox ~ 8 eV EFm Ec EFp EFi Ev Ev ©rlc L31-20Apr2011

4 Flat band condition (approx. scale)
SiO2 p-Si q(fm-cox)= 3.15 eV q(cox-cSi)=3.1eV Ec,Ox qffp= 3.95eV EFm Ec Eg,ox~8eV EFi EFp Ev Ev ©rlc L31-20Apr2011

5 Equivalent circuit for Flat-Band
Surface effect analogous to the extr Debye length = LD,extr = [eVt/(qNa)]1/2 Debye cap, C’D,extr = eSi/LD,extr Oxide cap, C’Ox = eOx/xOx Net C is the series comb C’Ox C’D,extr ©rlc L31-20Apr2011

6 Accumulation for Vgate< VFB
-xox SiO2 EOx,x<0 holes p-type Si tsub Vsub = 0 x ©rlc L31-20Apr2011

7 Accumulation p-Si, Vgs < VFB
Fig 10.4a* ©rlc L31-20Apr2011

8 Equivalent circuit for accumulation
Accum depth analogous to the accum Debye length = LD,acc = [eVt/(qps)]1/2 Accum cap, C’acc = eSi/LD,acc Oxide cap, C’Ox = eOx/xOx Net C is the series comb C’Ox C’acc ©rlc L31-20Apr2011

9 Depletion for p-Si, Vgate> VFB
-xox SiO2 EOx,x> 0 Depl Reg Acceptors p-type Si tsub Vsub = 0 x ©rlc L31-20Apr2011

10 Depletion for p-Si, Vgate> VFB
Fig 10.4b* ©rlc L31-20Apr2011

11 Equivalent circuit for depletion
Depl depth given by the usual formula = xdepl = [2eSi(Vbb)/(qNa)]1/2 Depl cap, C’depl = eSi/xdepl Oxide cap, C’Ox = eOx/xOx Net C is the series comb C’Ox C’depl ©rlc L31-20Apr2011

12 Inversion for p-Si Vgate>VTh>VFB
Vgate> VFB EOx,x> 0 e- e- e- e- e- Depl Reg Acceptors Vsub = 0 ©rlc L31-20Apr2011

13 Inversion for p-Si Vgate>VTh>VFB
Fig 10.5* ©rlc L31-20Apr2011

14 Approximation concept “Onset of Strong Inv”
OSI = Onset of Strong Inversion occurs when ns = Na = ppo and VG = VTh Assume ns = 0 for VG < VTh Assume xdepl = xd,max for VG = VTh and it doesn’t increase for VG > VTh Cd,min = eSi/xd,max for VG > VTh Assume ns > 0 for VG > VTh ©rlc L31-20Apr2011

15 MOS Bands at OSI p-substr = n-channel
Fig 10.9* ©rlc L31-20Apr2011

16 Equivalent circuit above OSI
Depl depth given by the maximum depl = xd,max = [2eSi|2fp|/(qNa)]1/2 Depl cap, C’d,min = eSi/xd,max Oxide cap, C’Ox = eOx/xOx Net C is the series comb C’Ox C’d,min ©rlc L31-20Apr2011

17 MOS surface states** p- substr = n-channel
©rlc L31-20Apr2011

18 n-substr accumulation (p-channel)
Fig 10.7a* ©rlc L31-20Apr2011

19 n-substrate depletion (p-channel)
Fig 10.7b* ©rlc L31-20Apr2011

20 n-substrate inversion (p-channel)
Fig 10.7* ©rlc L31-20Apr2011

21 Values for gate work function, fm
©rlc L31-20Apr2011

22 Values for fms with metal gate
©rlc L31-20Apr2011

23 Values for fms with silicon gate
©rlc L31-20Apr2011

24 References * Semiconductor Physics & Devices, by Donald A. Neamen, Irwin, Chicago, 1997. **Device Electronics for Integrated Circuits, 2nd ed., by Richard S. Muller and Theodore I. Kamins, John Wiley and Sons, New York, 1986 ©rlc L31-20Apr2011


Download ppt "Professor Ronald L. Carter"

Similar presentations


Ads by Google