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Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc/
EE5342 – Semiconductor Device Modeling and Characterization Lecture 20 March 31, 2010 Professor Ronald L. Carter
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Schedule Change Classes WILL be held on
4/5/10 4/7/10 Dr. Russell will be filling in The previously scheduled make-up classes will be cancelled 4/16/10 (Friday) 4/23/10 (Friday) Project 2 Test changed to W 4/28/10 L20 03/31/10
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Inversion for p-Si Vgate>VTh>VFB
Vgate> VFB EOx,x> 0 e- e- e- e- e- Depl Reg Acceptors Vsub = 0 L20 03/31/10
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Inversion for p-Si Vgate>VTh>VFB
Fig 10.5* L20 03/31/10
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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 L20 03/31/10
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MOS Bands at OSI p-substr = n-channel
Fig 10.9* L20 03/31/10
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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 L20 03/31/10
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MOS surface states** p- substr = n-channel
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n-substr accumulation (p-channel)
Fig 10.7a* L20 03/31/10
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n-substrate depletion (p-channel)
Fig 10.7b* L20 03/31/10
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n-substrate inversion (p-channel)
Fig 10.7* L20 03/31/10
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Values for gate work function, fm
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Values for fms with metal gate
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Values for fms with silicon gate
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Typical fms values Fig 10.15* fms (V) NB (cm-3) L20 03/31/10
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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 L20 03/31/10
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Flat-band parameters for n-channel (p-subst)
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Flat-band parameters for p-channel (n-subst)
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Inversion for p-Si Vgate>VTh>VFB
Vgate> VFB EOx,x> 0 e- e- e- e- e- Depl Reg Acceptors Vsub = 0 L20 03/31/10
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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 L20 03/31/10
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MOS Bands at OSI p-substr = n-channel
Fig 10.9* 2q|fp| qfp xd,max L20 03/31/10
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Computing the D.R. W and Q at O.S.I.
Ex Emax x L20 03/31/10
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Calculation of the threshold cond, VT
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Equations for VT calculation
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n-channel VT for VC = VB = 0
Fig 10.20* L20 03/31/10
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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 L20 03/31/10 L
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Fully biased MOS capacitor in inversion
Channel VG>VT VS=VC VD=VC EOx,x> 0 n+ e- e- e- e- e- e- n+ p-substrate Vsub=VB Depl Reg Acceptors y L20 03/31/10 L
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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 L20 03/31/10
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Flat-band parameters for n-channel (p-subst)
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MOS energy bands at Si surface for n-channel
Fig 8.10** L20 03/31/10
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Computing the D.R. W and Q at O.S.I.
Ex Emax x L20 03/31/10
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Q’d,max and xd,max for biased MOS capacitor
Fig 8.11** |Q’d,max|/q (cm-2) xd,max (microns) L20 03/31/10
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Fully biased n- channel VT calc
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L20 03/31/10
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Computing the threshold voltage
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L20 03/31/10
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n-channel VT for VC = VB = 0
Fig 10.20* L20 03/31/10
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Flat-band parameters for p-channel (n-subst)
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Fully biased p- channel VT calc
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p-channel VT for VC = VB = 0
Fig 10.21* L20 03/31/10
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Ion implantation L20 03/31/10
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“Dotted box” approx L20 03/31/10
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L20 03/31/10
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Mobilities L20 03/31/10
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Differential charges for low and high freq
From Fig 10.27* L20 03/31/10
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Ideal low-freq C-V relationship
Fig 10.25* L20 03/31/10
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Comparison of low and high freq C-V
Fig 10.28* L20 03/31/10
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Effect of Q’ss on the C-V relationship
Fig 10.29* L20 03/31/10
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n-channel enhancement MOSFET in ohmic region
0< VT< VG Channel VS = 0 0< VD< VDS,sat EOx,x> 0 n+ e-e- e- e- e- n+ Depl Reg p-substrate Acceptors VB < 0 L20 03/31/10
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Conductance of inverted 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) L20 03/31/10
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Basic I-V relation for MOS channel
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I-V relation for n-MOS (ohmic reg)
ID non-physical ID,sat saturated VDS,sat VDS L20 03/31/10
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Universal drain characteristic
ID VGS=VT+3V 9ID1 ohmic saturated, VDS>VGS-VT VGS=VT+2V 4ID1 VGS=VT+1V ID1 VDS L20 03/31/10
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Characterizing the n-ch MOSFET
VD ID D G S B VT VGS L20 03/31/10
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Low field ohmic characteristics
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MOSFET Device Structre Fig. 4-1, M&A*
L20 03/31/10
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4-7a (A&M) L20 03/31/10
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Figure 4-7b (A&M) L20 03/31/10
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Figure 4-8a (A&M) L20 03/31/10
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Figure 4-8b (A&M) L20 03/31/10
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Body effect data Fig 9.9** L20 03/31/10
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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 L20 03/31/10
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