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Professor Ronald L. Carter

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1 Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/
EE5342 – Semiconductor Device Modeling and Characterization Lecture 24 - Spring 2004 Professor Ronald L. Carter L24 April 19

2 Ideal 2-terminal MOS capacitor/diode
conducting gate, area = LW Vgate -xox SiO2 y L silicon substrate tsub Vsub x L24 April 19

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 L24 April 19

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 L24 April 19

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 L24 April 19

6 Accumulation for Vgate< VFB
-xox SiO2 EOx,x<0 holes p-type Si tsub Vsub = 0 x L24 April 19

7 Accumulation p-Si, Vgs < VFB
Fig 10.4a* L24 April 19

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 L24 April 19

9 Depletion for p-Si, Vgate> VFB
-xox SiO2 EOx,x> 0 Depl Reg Acceptors p-type Si tsub Vsub = 0 x L24 April 19

10 Depletion for p-Si, Vgate> VFB
Fig 10.4b* L24 April 19

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 L24 April 19

12 Inversion for p-Si Vgate>VTh>VFB
Vgate> VFB EOx,x> 0 e- e- e- e- e- Depl Reg Acceptors Vsub = 0 L24 April 19

13 Inversion for p-Si Vgate>VTh>VFB
Fig 10.5* L24 April 19

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 L24 April 19

15 MOS Bands at OSI p-substr = n-channel
Fig 10.9* L24 April 19

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 L24 April 19

17 MOS surface states** p- substr = n-channel
L24 April 19

18 n-substr accumulation (p-channel)
Fig 10.7a* L24 April 19

19 n-substrate depletion (p-channel)
Fig 10.7b* L24 April 19

20 n-substrate inversion (p-channel)
Fig 10.7* L24 April 19

21 Values for gate work function, fm
L24 April 19

22 Values for fms with metal gate
L24 April 19

23 Values for fms with silicon gate
L24 April 19

24 Typical fms values Fig 10.15* fms (V) NB (cm-3) L24 April 19

25 Flat band with oxide charge (approx. scale)
SiO2 p-Si +<--Vox-->- q(Vox) Ec,Ox q(ffp-cox) q(fm-cox) Ex Eg,ox~8eV EFm Ec EFi EFp q(VFB) Ev VFB= VG-VB, when Si bands are flat Ev L24 April 19

26 Flat-band parameters for n-channel (p-subst)
L24 April 19

27 Flat-band parameters for p-channel (n-subst)
L24 April 19

28 Inversion for p-Si Vgate>VTh>VFB
Vgate> VFB EOx,x> 0 e- e- e- e- e- Depl Reg Acceptors Vsub = 0 L24 April 19

29 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 L24 April 19

30 MOS Bands at OSI p-substr = n-channel
Fig 10.9* 2q|fp| qfp xd,max L24 April 19

31 Computing the D.R. W and Q at O.S.I.
Ex Emax x L24 April 19

32 Calculation of the threshold cond, VT
L24 April 19

33 Equations for VT calculation
L24 April 19

34 Fully biased n-MOS capacitor
VG Channel if VG > VT VS VD EOx,x> 0 n+ e- e- e- e- e- e- n+ p-substrate Vsub=VB Depl Reg Acceptors y L24 April 19 L

35 MOS energy bands at Si surface for n-channel
Fig 8.10** L24 April 19

36 Computing the D.R. W and Q at O.S.I.
Ex Emax x L24 April 19

37 Q’d,max and xd,max for biased MOS capacitor
Fig 8.11** xd,max (mm) L24 April 19

38 Fully biased n- channel VT calc
L24 April 19

39 n-channel VT for VC = VB = 0
Fig 10.20* L24 April 19

40 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 L24 April 19


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