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Sam PalermoAnalog & Mixed-Signal Center
Texas A&M University
Lecture 14: Two Stage Miller OTA
ECEN474/704: (Analog) VLSI Circuit Design Spring 2016
Announcements & Agenda
• HW5 (Preliminary Project Report) Due Apr. 18
• Two Stage Miller OTA• OpAmp Characterization
2
Multi-Stage Amplifiers
3
• Single-stage amplifiers typically have to trade-off gain and swing range
• Multi-stage amplifiers allow for higher gain without sacrificing swing range
• The major challenge with multi-stage amplifiers is achieving adequate phase margin to insure stability in a feedback configuration
Two Stage Miller OTA
4
42
2818
78
7842
82
78
8
42
221
1
oo
mmvmm
ooout
outmVDC
oooo
mm
oo
m
oo
mvvVDC
ggggAgG
ggR
RGAgggg
gggg
ggg
gAAA
Gain DC
Two-Stage Miller OTA – Frequency Response
5
• Stage 1 is a differential amplifier with an active load
• Stage 2 is a common-source amplifier with a large miller capacitor
• Using a Thevenin equivalent for Stage 1, we can use the common-source equations from Lecture 8
Two-Stage Miller OTA – Frequency Response
6
• The amplifier should be designed to yield one dominant pole, so we use the dominant pole approximation equations
872421
8
21
22812
28122811
and where
1
11
1esCapacitancTransistorNeglecting
OOoutOOout
L
m
LCoutout
LCoutCoutmoutp
CoutmoutLCoutCoutmoutp
rrRrrRCg
CCRRCCRCRgR
CRgRCCRCRgR
Jose Silva-Martinez -7- Texas A&M University
ELEN-474
VSS
M1 M1
01i 01i
-vd
01iM2 M2
02iM3
012i
vd
R1 C1RL CL
-v0
VDD
2
1
1
1
21
2
1
11
3
1
1
tantan180arg_
,min*
p
u
p
u
ppVDC
L
Lp
p
L
mmVDC
inmPhase
AGBWCgCg
gg
ggA
valid?) system, poledominant (if
(LHP)
(LHP)
Main equations
p1 p2 GBW
AVDCPhase Margin < 45 degrees
Phase
u
21
11pp
VDC
ssAsA
Frequency Response – No Compensation
TAMU-Elen-474 Jose Silva-Martinez-08
- 8 -
VSS
M1 M1
01i 01i
-vd
01iM2 M2
02iM3
012i
vd
R1 C1 CMRL CL
-v0
VDD
Phase compensation Pole splitting techniques!!
p1 p2
GBW
AVDC
After compensation Phase Margin > 45 degrees Bandwidth is reduced!!!
p1’
p2’u
2
1
1
1
11
1
32
31
11
3
1
1
tantan180arg_
*
pp
M
mpVDC
L
mp
ML
mp
L
mmVDC
WGBWGBinmPhase
CgAWGB
CCg
CggC
ggg
ggA
(LHP)
(LHP)
Frequency Response – Miller Compensation (Ignoring z)
TAMU-Elen-474 Jose Silva-Martinez-08
- 9 -
ZEROpp
M
mpVDC
L
mp
ML
mp
L
mmVDC
WGBWGBWGBinmPhase
CgAWGB
CCg
CggC
ggg
ggA
1
2
1
1
1
11
1
32
31
11
3
1
1
tantantan180arg_
*
(LHP)
(LHP)
VSS
M1 M1
01i 01i
-vd
01iM2 M2
02iM3
012i
vd
R1 C1 CMRL CL
-v0
VDD
Parasitic (bad) RHP zero!!
p1 p2
GBW
AVDC
After compensation Phase Margin > 45 degrees Bandwidth is reduced!!!
p1’
GBW’ZER
O
(RHP) M
mZERO C
g 3
p2’
21
11
1
pp
zVDC
ss
sAsA
Frequency Response – Miller Compensation (Considering z)
TAMU-Elen-474 Jose Silva-Martinez-08
- 10 -
VSS
M1 M1
01i 01i
-vd
01iM2 M2
02iM3
012i
vd
R1 C1 CMRL CL
-v0
VDD
ZERO
u1
2p
u1
1p
u1 tan'
tan'
tan180inargm_Phase
Parasitic (bad) RHP zero!! Can be catastrophic if close or below wu!
p1 p2
GBW
AVDC After compensation Phase Margin > 45 degrees Bandwidth is reduced!!!
p1’
GBW’ZER
O
M
3mZERO C
g
p2’
p1 p2
GBW
AVDC
After compensation Phase Margin << 45 degrees Phase is equivalent to having 3 poles below unity gain frequency Unstable!
p1’
uZERO
p2’
z Impact on Frequency Response
TAMU-Elen-474 Jose Silva-Martinez-08
- 11 -
VSS
M1 M1
01i 01i
-vd
01iM2 M2
02iM3
012i
vd
R1 C1 CMRL CL
-v0
VDD
M4VBIB1
IB2
Adding a series resistance
RZ
321
111
1
ppp
zVDC
sss
sAsA
13
1CRZ
p
MZm
z
CRg
3
11
(Generally high frequency & can be ignored)
p2
Z
Z
cancel can
LFP to RHP from zero pushes
infinity to zero RHP the pushes
)(initially frequencyhigher a to RHP push will R zero-Nonmargin phase improve to R design Can
Mm
MLZ
mZ
mZ
CgCCCR
gR
gR
3
1
3
3
1
1
Two Stage Miller OTA Noise
12
2
42
82
784
22
22
2
42
84
2
42
8278
2
22381
PSD Voltage Noise Referred-Input
223
8
PSDCurrent NoiseReferred-Output
oo
mm
mmm
mm
oi
oo
mm
oo
mmmm
o
gggg
ggggkT
Gfi
fv
gggg
ggggggkT
fi
Jose Silva-Martinez -13- Texas A&M University
ELEN-474
OPAMP Characterization
Main parameters to be measured:
•DC gain (104-106) V/V)•Frequency Limitations
•Bandwith (Few Hertz~1kHz)•Gain-Bandwidth product (1~100 Mhz)
•Output resistance •Input Impedance•Signal Swing
•Common-mode input range•Output swing
•Stability•DC Offset•Slew-rate•CMRR•PSRR
For this section, see: CMOS Analog design, Allen & Holberg2nd edition, HPR, 2002.
Jose Silva-Martinez -14- Texas A&M University
ELEN-474
OPAMP Characterization
DC gain (104-106) V/V) :
•Very difficult to measure in open-loop due to DC offsets.
+
-V00
How to measure/characterize it?
•Stabilize for DC
•For DC, the OPAMP operates in closed loop!!•For frequencies higher than 1/RCCC, the OPAMP operates in open-loop with a grounded load given by RC.
+
-V0
RCCC
Vi
Jose Silva-Martinez -15- Texas A&M University
ELEN-474
OPAMP: DC CharacterizationHow to measure/characterize it?
•At DC
•If A(s)B(s) <<1 then the measured gain is dominated by the OPAMP transfer function!
+
-V0
RCCC
Vi
CC
CC
C
i
o
CsR11
sC1R
sC1
)s(B
)s(B)s(A1)s(A
vv
A(s)
)s(Avv
1)s(A1
)s(Avv
i
o
i
o
AVDC
P1GBW
OPAMP (open-loop)
CCDC1P CR
1A
CCCR1
Make sure to set RCCCsuch that
Jose Silva-Martinez -16- Texas A&M University
ELEN-474
OPAMP Characterization
DC Offset
+
-V0~VoffsetA(s)
Voffset
Jose Silva-Martinez -17- Texas A&M University
ELEN-474
OPAMP Characterization: GBW and stability
+
-V0A(s)
Vin
AVDC
P1
GBW
OPAMP (open-loop)
+
-V0A(s)
Vin
t
Vi
Enough phase margin
Jose Silva-Martinez -18- Texas A&M University
ELEN-474
OPAMP Characterization: GBW and stability
+
-V0A(s)
Vin
AVDC
P1
OPAMP (open-loop)
+
-V0A(s)
Vin
t
Vi
Not enough phase margin
Jose Silva-Martinez -19- Texas A&M University
ELEN-474
OPAMP Characterization: Slew-Rate (max speed)
+
-V0A(s)
Vin
t
VSS
VDD
Slew-Rate
)t(Vodtdmax
Min output level
Max output level
Jose Silva-Martinez -20- Texas A&M University
ELEN-474
OPAMP Characterization: Output Swing
+
-A(s)
Vin
t
Vmin
Vmax
Low-Frequency Gain
DC Offset
ifreqlow V
VoA
vivo
Use a slow triangular input signal such that the raising and falling edges are not determined by slew rate limitations
Output swing
vi
vo
Small signal (~ 10 mV)
Jose Silva-Martinez -21- Texas A&M University
ELEN-474
OPAMP Characterization: Input and Output impedance
+
-A(s)Vin
iin
R
CRC
Zin
+
-
RCCC
A(s)
Vin
iin
RC and CC as large as possible!!
At Low frequencies:Zmeasured Zo (Why????)
At medium frequencies: Zmeasured = Zo||RC
Be sure that the OPAMP (all internal transistors) is properly biased during characterization!!
Next Time
• OpAmp Feedback & Stability• Common-Mode Feedback Techniques
22