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Introduction to CMOS VLSI Design Nonideal Transistors
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CMOS VLSI Design2 Outline Transistor I-V Review Nonideal Transistor Behavior –Velocity Saturation –Channel Length Modulation –Body Effect –Leakage –Temperature Sensitivity Process and Environmental Variations –Process Corners
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CMOS VLSI Design3 Ideal Transistor I-V Shockley 1 st order transistor models V dsat = V gs - V t
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CMOS VLSI Design4 Ideal nMOS I-V Plot 180 nm TSMC process Ideal Models – = 155(W/L) A/V 2 – V t = 0.4 V – V DD = 1.8 V = n C ox (W/L)
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CMOS VLSI Design5 Simulated nMOS I-V Plot 180 nm TSMC process BSIM 3v3 SPICE models –very elaborate model derived from the underlying device physics What differs? Berkeley Short-Channel IGFET Model (BSIM)
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CMOS VLSI Design6 Simulated nMOS I-V Plot 180 nm TSMC process BSIM 3v3 SPICE models What differs? –Less ON current –No square law –Current increases in saturation
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CMOS VLSI Design7 Velocity Saturation We assumed carrier velocity is proportional to E-field –v = E lat = V ds /L At high fields, this ceases to be true –Carriers scatter off atoms –Velocity reaches v sat Electrons: 6-10 x 10 6 cm/s Holes: 4-8 x 10 6 cm/s –Better model
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CMOS VLSI Design8 Velocity Sat I-V Effects Ideal transistor ON current increases with V 2 Velocity-saturated ON current increases with V Real transistors are partially velocity saturated –Approximate with -power law model –I ds V –1 < < 2 determined empirically
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CMOS VLSI Design9 -Power Model
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CMOS VLSI Design10 Channel Length Modulation Reverse-biased p-n junctions form a depletion region –Region between n and p with no carriers –Width of depletion L d region grows with reverse bias –L eff = L – L d Shorter L eff gives more current –I ds increases with V ds –Even in saturation
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CMOS VLSI Design11 Chan Length Mod I-V = channel length modulation coefficient –not feature size –Empirically fit to I-V characteristics
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CMOS VLSI Design12 Body Effect V t : gate voltage necessary to invert channel Increases if source voltage increases because source is connected to the channel Increase in V t with V s is called the body effect
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CMOS VLSI Design13 Body Effect Model s = surface potential at threshold –Depends on doping level N A –And intrinsic carrier concentration n i = body effect coefficient
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CMOS VLSI Design14 OFF Transistor Behavior What about current in cutoff? Simulated results What differs? –Current doesn’t go to 0 in cutoff
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CMOS VLSI Design15 Leakage Sources Subthreshold conduction –Transistors can’t abruptly turn ON or OFF Junction leakage –Reverse-biased PN junction diode current Gate leakage –Tunneling through ultra-thin gate dielectric Subthreshold leakage is the biggest source in modern transistors
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CMOS VLSI Design16 Subthreshold Leakage Subthreshold leakage exponential with V gs n is process dependent, typically 1.4-1.5
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CMOS VLSI Design17 DIBL Drain-Induced Barrier Lowering –Drain voltage also affect V t –High drain voltage causes subthreshold leakage to ________.
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CMOS VLSI Design18 DIBL Drain-Induced Barrier Lowering –Drain voltage also affect V t –High drain voltage causes subthreshold leakage to increase.
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CMOS VLSI Design19 Junction Leakage Reverse-biased p-n junctions have some leakage I s depends on doping levels –And area and perimeter of diffusion regions –Typically < 1 fA/ m 2
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CMOS VLSI Design20 Gate Leakage Carriers may tunnel thorough very thin gate oxides Predicted tunneling current (from [Song01]) Negligible for older processes May soon be critically important
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CMOS VLSI Design21 Temperature Sensitivity Increasing temperature –Reduces mobility –Reduces V t I ON ___________ with temperature I OFF ___________ with temperature
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CMOS VLSI Design22 Temperature Sensitivity Increasing temperature –Reduces mobility –Reduces V t I ON decreases with temperature I OFF increases with temperature
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CMOS VLSI Design23 So What? So what if transistors are not ideal? –They still behave like switches. But these effects matter for… –Supply voltage choice –Logical effort –Quiescent power consumption –Pass transistors –Temperature of operation
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CMOS VLSI Design24 Parameter Variation Transistors have uncertainty in parameters –Process: L eff, V t, t ox of nMOS and pMOS –Vary around typical (T) values Fast (F) –L eff : ______ –V t : ______ –t ox : ______ Slow (S): opposite Not all parameters are independent for nMOS and pMOS
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CMOS VLSI Design25 Parameter Variation Transistors have uncertainty in parameters –Process: L eff, V t, t ox of nMOS and pMOS –Vary around typical (T) values Fast (F) –L eff : short –V t : low –t ox : thin Slow (S): opposite Not all parameters are independent for nMOS and pMOS
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CMOS VLSI Design26 Environmental Variation V DD and T also vary in time and space Fast: –V DD : ____ –T: ____ CornerVoltageTemperature F T1.870 C S
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CMOS VLSI Design27 Environmental Variation V DD and T also vary in time and space Fast: –V DD : high –T: low CornerVoltageTemperature F1.980 C T1.870 C S1.62125 C
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CMOS VLSI Design28 Process Corners Process corners describe worst case variations –If a design works in all corners, it will probably work for any variation. Describe corner with four letters (T, F, S) –nMOS speed –pMOS speed –Voltage –Temperature
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CMOS VLSI Design29 Important Corners Some critical simulation corners include PurposenMOSpMOSV DD Temp Cycle time Power Subthreshold leakage Pseudo-nMOS
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CMOS VLSI Design30 Important Corners Some critical simulation corners include PurposenMOSpMOSV DD Temp Cycle time, timimg specification. conservative SSSS Power,DC power comsumption, race conditions,etc FFFF Subthreshold leakage, noise analysis FFFS Pseudo-nMOS and ratioed circuits SFFF
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