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Transcript of © Digital Integrated Circuits 2nd Inverter EE5900 Advanced Algorithms for Robust VLSI CAD The...
© Digital Integrated Circuits2nd Inverter
EE5900 Advanced EE5900 Advanced Algorithms for Algorithms for Robust VLSI CADRobust VLSI CAD
The InverterThe Inverter
Dr. Shiyan HuOffice: EERC [email protected]
Adapted and modified from Digital Integrated Circuits: A Design Perspective by Jan M. Rabaey, Anantha Chandrakasan, and Borivoje Nikolic.
© Digital Integrated Circuits2nd Inverter
The CMOS Inverter: A First GlanceThe CMOS Inverter: A First Glance
Vin=Vdd,Vout=0Vin=0,Vout=Vdd
V in Vout
CL
VDD
S
D
D
S
© Digital Integrated Circuits2nd Inverter
CMOS Inverter - First-Order DC AnalysisCMOS Inverter - First-Order DC Analysis
VDD VDD
Vin VDD Vin 0
VoutVout
Rn
Rp
© Digital Integrated Circuits2nd Inverter
CMOS Inverter: Transient ResponseCMOS Inverter: Transient Response
VoutVout
Rn
Rp
VDDVDD
Vin VDDVin 0(a) Low-to-high (b) High-to-low
CLCL
Delay=0.69RC
© Digital Integrated Circuits2nd Inverter
NMOS In InverterNMOS In Inverter For NMOS
1. Vin=0, Vgsn=0<Vtn, Vdsn=Vout=Vdd, NMOS is in cut-off region, X1.
2. PMOS is on. Vout=Vdd.
3. Vin=Vdd, instantaneously, Vgsn=Vdd>Vtn,Vdsn=Vout=Vdd, Vgsn-Vtn=Vdd-Vtn<Vdd, NMOS is in saturation region, X2
4. Instantaneously, Vgsp=0>Vtp. PMOS cut-off
5. NMOS is on so Vdsn->0. The operating point follows the arrow to the origin. Vout=0 at X3.Vin Vout
CL
VDD
S
D
D
S
© Digital Integrated Circuits2nd Inverter
Rising delay and Falling delayRising delay and Falling delay
Rising delay tr=time for the signal to change from 10% to 90% of Vdd
Falling delay tf=time for the signal to change from 90% to 10% of Vdd
Delay=time from input signal transition (50% Vdd) to output signal transition (50% Vdd).
© Digital Integrated Circuits2nd Inverter
NMOS falling timeNMOS falling timeFor NMOS
1. Vin=0, Vgsn=0<Vt, Vdsn=Vout=Vdd, NMOS is in cut-off region, X1
2. Vin=Vdd, instantaneously, Vgsn=Vdd>Vt,Vdsn=Vout=Vdd, Vgsn-Vtn=Vdd-Vtn<Vdd, NMOS is in saturation region, X2
3. The operating point follows the arrow to the origin. So Vout=0 at X3.
Vin Vout
CL
VDD
S
D
D
S
© Digital Integrated Circuits2nd Inverter
NMOS falling timeNMOS falling time When Vin=Vdd,
instantaneously, Vgsn=Vdd
tf=tf1+tf2 tf1: time for CL to
switch from 0.9Vdd to Vgsn-Vtn=Vdd-Vtn
tf2: time for CL to switch from Vdd-Vtn to 0.1Vdd
tf1
tf2
© Digital Integrated Circuits2nd Inverter
NMOS falling timeNMOS falling time For tf1:
Integrate Vout from 0.9Vdd to Vdd-Vt
For tf2, we have
Vgsn=Vdd
Vdsn=Vout
© Digital Integrated Circuits2nd Inverter
NMOS falling timeNMOS falling time tf=tf1+tf2
Assume Vt=0.2Vdd
© Digital Integrated Circuits2nd Inverter
Falling and Rising timeFalling and Rising time Assume Vtn=-Vtp, then we can show
that Thus, for equal rising and falling time,
set That is, Wp=2Wn since up=un/2
© Digital Integrated Circuits2nd Inverter
Where Does Power Go in CMOS?Where Does Power Go in CMOS?
• Dynamic Power Consumption
• Short Circuit Currents
• Leakage
Charging and Discharging Capacitors
Short Circuit Path between Supply Rails during Switching
Leaking diodes and transistors
© Digital Integrated Circuits2nd Inverter
Dynamic Power DissipationDynamic Power Dissipation
Power = CL * Vdd2 * f
Need to reduce CL, Vdd, and f to reduce power.
Vin Vout
CL
Vdd
Not a function of transistor sizes
© Digital Integrated Circuits2nd Inverter
Dynamic PowerDynamic Power
Dynamic power is due to charging/discharging load capacitor CL
In charging, CL is loaded with a charge CL Vdd which requires the energy of QVdd= CL Vdd2, and all the energy will be dissipated when discharging is done. Total power = CL Vdd2
If this is performed with frequency f, clearly, total power = CL Vdd2 f
© Digital Integrated Circuits2nd Inverter
Dynamic Power- IIDynamic Power- II
If the waveform is not periodic, denote by P the probability of switching for the signal
The dynamic power is the most important power source It is quadratically dependant on Vdd It is proportional to the number of switching. We can slow down the
clock not on the timing critical path to save power. It is independent of transistor size since it only depends on the load of
the transistor.
© Digital Integrated Circuits2nd Inverter
Short Circuit CurrentsShort Circuit Currents
Vin Vout
CL
Vdd
I VD
D (m
A)
0.15
0.10
0.05
Vin (V)5.04.03.02.01.00.0
Happens when both transistors are on.
If every switching is instantaneous, then no short circuits.
Longer delay -> larger short circuit power
© Digital Integrated Circuits2nd Inverter
LeakageLeakage
Vout
Vdd
Sub-ThresholdCurrent
Drain JunctionLeakage
Sub-Threshold Current Dominant FactorSub-threshold current one of most compelling issuesin low-energy circuit design.
© Digital Integrated Circuits2nd Inverter
Subthreshold Leakage ComponentSubthreshold Leakage Component
© Digital Integrated Circuits2nd Inverter
Principles for Power ReductionPrinciples for Power Reduction
Prime choice: Reduce voltage Recent years have seen an acceleration in
supply voltage reduction Design at very low voltages still open
question (0.5V) Reduce switching activity Reduce physical capacitance
© Digital Integrated Circuits2nd Inverter
Goals of Technology ScalingGoals of Technology Scaling
Make things cheaper: Want to sell more functions (transistors)
per chip for the same money Build same products cheaper, sell the
same part for less money Price of a transistor has to be reduced
But also want to be faster, smaller, lower power
© Digital Integrated Circuits2nd Inverter
ScalingScaling
Goals of scaling the dimensions by 30%: Reduce gate delay by 30% Double transistor density
Die size used to increase by 14% per generation
Technology generation spans 2-3 years
© Digital Integrated Circuits2nd Inverter
Technology ScalingTechnology Scaling Devices scale to smaller dimensions with advancing technology. A scaling factor S describes the ratio of dimension between the
old technology and the new technology. In practice, S=1.2-1.5.
© Digital Integrated Circuits2nd Inverter
Technology Scaling - IITechnology Scaling - II In practice, it is not feasible to scale voltage since different ICs in
the system may have different Vdd. This may require extremely complex additional circuits. We can only allow very few different levels of Vdd.
In technology scaling, we often have fixed voltage scaling model. W,L,tox scales down by 1/S Vdd, Vt unchanged Area scales down by 1/S2
Cox scales up by S due to tox Gate capacitance = CoxWL scales down by 1/S scales up by S
Linear and saturation region current scales up by S Current density scales up by S3
P=Vdd*I, power density scales up by S3
Power consumption is a major design issue