Digital Integrated Circuits - University of Waterloomhanis/ece637/lecture6.pdf · q Small area is a...
Transcript of Digital Integrated Circuits - University of Waterloomhanis/ece637/lecture6.pdf · q Small area is a...
Digital Integrated Digital Integrated CircuitsCircuitsA Design PerspectiveA Design Perspective
The InverterThe Inverter
IntroductionIntroduction
q The inverter is the simplest of all digital logic gates
q However, building an understanding of its properties and operation is crucial for the design and analysis of larger/ more complex logic gates.
q We will discuss: General properties of an inverter (and logic gates), and inverter implementation issues in CMOS technology.
General PropertiesGeneral Properties
q Small area is a desirable property for a digital logic gateq Larger packing densityq Small parasitic capacitancesq Shorter interconnectsq Smaller chip area, hence higher number of devices per wafer (lower
cost)
q Fewer transistors for a logic gate usually results into smaller area.Hence, minimum possible number of transistors for a given gate is important.
CMOS Inverter CMOS Inverter -- FirstFirst--Order DC AnalysisOrder DC Analysis
VOL = 0VOH = VDD
VM = f(Rn, Rp)
VDD VDD
Vin = VDD Vin = 0
VoutVout
Rn
Rp
Properties1) High and low outputs = VDD and Ground.
Voltage swing= VDD. High Noise Margins.2) Logic Levels are independent of device sizes
(ratioless logic)3) In steady state, a path exists from O/P to VDD
or GND. Thus, low output impedance. Less sensitive to noise.
4) Input resistance is extremly high, since MOS gate draws no dc input current. Steady-state input current ~ zero. An inverter can theoretically drive infinite number of gates and be functionally operational. This degrades the transient response.
5) In steady-state, no direct path exists between supply and ground rails. No static power (ignoring leakage)
PMOS Load LinesPMOS Load Lines
VDSp
IDp
VGSp=-2.5
VGSp=-1VDSp
IDnVin=0
Vin=1.5
Vout
IDnVin=0
Vin=1.5
Vin = VDD+VGSpIDn = - IDp
Vout = VDD+VDSp
DDoutDSpoutDSn
DDinGSpinGSn
DSnDSp
VVVVV
VVVVV
II
−==
−==
−=
;
;
CMOS Inverter Load CharacteristicsCMOS Inverter Load CharacteristicsID n
Vout
Vin = 2.5
Vin = 2
Vin = 1.5
Vin = 0
Vin = 0.5
Vin = 1
NMOS
Vin = 0
Vin = 0.5
Vin = 1Vin
= 1.5
Vin = 2
Vin = 2.5
Vin = 1Vin
= 1.5
PMOS
For a dc operating point to be valid, the currents through NMOS and PMOS devices must be equal (intersections) {Vin = 0, 0.5, 1, 1.5, 2, 2.5}
Operating points are located either at the high or low output levels. The Voltage Transfer Characteristics (VTC) exhibit a very narrow transition zone (high gain during switching transient – a small change in the input voltage results in a large output variation)
CMOS Inverter VTCCMOS Inverter VTC (V(VDDDD=2.5V)=2.5V)
Vout
Vin0.5 1 1.5 2 2.5
0.5
11.
52
2.5
NMOS resPMOS off
NMOS satPMOS sat
NMOS offPMOS res
NMOS satPMOS res
NMOS resPMOS sat
Vout=Vin
VM = switching threshold
Switching Threshold as a function of Transistor RatioSwitching Threshold as a function of Transistor Ratio
100 1010.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
MV(V
)
Wp/Wn
Vin=VoutPMOS and NMOS are saturated since VDS=VGS. Equate current through NMOS and PMOS.
rrV
V DDM +
≈1
VM=VDD/2 for comparable high and low noise margins. Thus, r=1.
)/()()/()/( ''pDSATpnDSATnnp kVkVLWLW =
Increasing strength of NMOS (sizing it up), moves VM closer to GND. Vice versa for PMOS case.Note: When designing CMOS circuits, it is advisable to balance the strengths of the transistors by making PMOS wider than NMOS, to obtain large noise margins + symmetrical characteristics.
Switching Threshold as a function of Transistor RatioSwitching Threshold as a function of Transistor Ratio
Points
q VM is relatively insensitive to variations in the device ratio. Small variations of the ratio do not disturb the VTC that much. Setting ratio of Wp/Wn to {3, 2.5, 2} yields switching thresholds of {1.22V, 1.18V, 1.13V}
q VM shifts towards VDD or GND depending on strength of NMOS and PMOS. Asymmetrical VTC is sometimes desirable in some designs.Example in Page 187.
Noise Margin Noise Margin -- Determining VDetermining VIHIH and Vand VILIL
VOH
VOL
Vin
Vout
VM
VIL VIH
A simplified approach
In real life applications, output voltage of a gate may not have the nominal value, owing to load, high switching speed..etc.Hence, it is desirable to define an acceptable voltage range for logic “1” and logic “0”
These expressions make it clear that a high gain in the transition region is very desirable. For infinite gain: NMH=VDD-VM, NML=VM
Logic gates have the property to restore the proper output logic values despite of non-ideal input levels.
Inverter GainInverter Gain
0 0.5 1 1.5 2 2.5-18
-16
-14
-12
-10
-8
-6
-4
-2
0
Vin (V)
gain
NMOS and PMOS are in saturation. Equate currents. Differentiate and solve for dVout/dVin
The gain is almost purely determined by technology parameters, especially the channel-length modulation.
Gain as a function of VGain as a function of VDDDD
0 0.05 0.1 0.15 0.20
0.05
0.1
0.15
0.2
Vin (V)
Vou
t (V
)
0 0.5 1 1.5 2 2.50
0.5
1
1.5
2
2.5
Vin (V)
Vou
t(V
)
Gain=-1
The gain of the inverter actually increases with a reduction of VDD . At a VDD =0.5V, which is just 100mV above VT of the transistors. So why can’t we operate all digital circuits at low VDD values?
• Yes, you get lower power consumption. But the delay of the gate drastically increases.• DC characteristics become very sensitive to variations in device parameters such at VT once VDD and intrinsic voltages become comparable.
• The signal swing is reduced. Although this is good for internal noise (crosstalk), this is bad for external noise sources that do not scale.
Impact of Process VariationsImpact of Process Variations
0 0.5 1 1.5 2 2.50
0.5
1
1.5
2
2.5
Vin
(V)
Vou
t(V)
Good PMOSBad NMOS
Good NMOSBad PMOS
Nominal
A CMOS inverter remains functional under a wide range of operating conditions. We showed that variations in device sizes have minor impact on switching threshold.
This robust behavior, which ensures functionality of the gate over a wide range of conditions, has contributed in a big way to the popularity of the static CMOS gate.