mixed-signal ic design notes set 1: quick summary of device …€¦ · power supply resonances;...
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ECE194J /594J notes, M. Rodwell, copyrighted 2011
Mixed-Signal IC Design Notes set 1:
Quick Summary of Device Models
Mark RodwellUniversity of California, Santa Barbara
[email protected] 805-893-3244, 805-893-3262 fax
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Background / Review
notes. online ECE145a therefer to please required, is detailgreater If
parametersport -2 modelsct Interconne
models Transistor n.informatiokey review Quickly
ECE145Ain covered wasmaterial This
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Transmission Lines
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Transmission Lines for On-Wafer Wiring
H
W microstrip line
0V
+V
geometry voltages currents
I
I
ADS use how to learn :ipsrelationsh eapproximat are These
light. of speed theis where
: velocitynpropagatio
and 377 where
:impedance sticcharacteri
0
0
c
cv
WHHZ
r
ro
ε
ηε
η
=
Ω≈
+≅
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Transmission Lines: Waves, Voltage, Current
Ldz
LZCdzgenV
sZ
velocitynpropagatio /1
and impedance sticcharacteri /
where
currents wavereverse and forward)/()/(),(
voltages wavereverse and forward )/()/(),(
LCv
CLZ
ZvztV
ZvztVtzI
vztVvztVtzV
o
oo
=
=
+−
−=
++−=−+
−+
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Reflections
( )( )
( )( )
tcoefficien ion transmisssource and
tcoefficien reflection source 11 where
:line of beginningAt
tcoefficien reflection load 11 where
:line of endAt
so
os
os
ossgenss
ol
olll
ZZZT
ZZZZVTVV
ZZZZVV
+=
+−
=Γ+Γ=
+−
=ΓΓ=
−+
+−
LZgenV
sZ
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Pulse Reflections on Transmission Lines
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Relating Lumped and Distributed Circuits
00 / , ZCZL ττ ==
model eApproximat
charging.circuit RCinductorneglect
)||()/(
→→
<<+ CRRRRL sLsL
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Short Tramission Lines Can Be Modeled as L's and C's
00 / , ZCZL ττ ==
inductor anely approximat. small , large
:line -High 0
→CL
Z
capacitor.a ely approximat. small , large
:line -Low 0
→LC
Z
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Skin effect loss
periphery. carrying-current effective theis P where,)1(1
lengthunit per resistance series added has Line
ty.conductivi theis where2/
depth skin oneby conductor thepenetratesCurrent
δσ
σωµσδ
jP
Zsurface+
=
=
H
W
~W +2H
ECE194J /594J notes, M. Rodwell, copyrighted 2011
package resonanceand grounding
ECE194J /594J notes, M. Rodwell, copyrighted 2011
What is Ground Bounce ?
ADC digitalsections
inputbuffer
ground returncurrents
Lground
∆Vingroundbouncenoise
"Ground" simply means a reference potential shared between many circuit paths.
To the extent that it has nonzero impedance, circuits will couple in unexpected ways
RFI, resonance, oscillation, frequently result from poor ground systems
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Ground Bounce on an IC: break in a ground plane
signal line
signal line
ground plane
line 1
“ground”
line 2
“ground”
common-lead inductance
coupling / EMI due to poor ground system integrity is common in high-frequency systemswhether on PC boards...or on ICs.
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Ground Bounce: IC Packaging with Top-Surface-Only Ground
Bond wire inductance aggravates the effect: resonates with through-wafer capacitance at 5-20 GHz
Peripheral grounding allows parallel plate mode resonancedie dimensions must be <0.4mm at 100GHz
IC: parallel-plane transmission line
peripheralbond inductances
peripheralbond inductances
ECE194J /594J notes, M. Rodwell, copyrighted 2011
power-supply resonance
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Power Supply Resonance
onbondCLf π2/1=
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Power Supply Resonances; Power Supply Damping
0
10
20
30
40
50
60
70
80
0 20 40 60 80 100
pow
er s
uppl
y im
peda
nce,
Ohm
s
Frequency (GHz)
90 GHz--local resonance between power supply capacitance and supply lead inductance
~N*5GHz resonances--global standing wave on power supply bus
Power supply is certain to resonate: we must model, simulate, and add dampling during design.
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Standard cell showing power buses
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Interconnects:Summary,
Design Strategy
ECE194J /594J notes, M. Rodwell, copyrighted 2011
fewer breaks in ground plane than CPW
IC Interconnects -- Thin-Film Microstrip
narrow line spacing → IC density
... but ground breaks at device placements
still have problem with package grounding
thin dielectrics → narrow lines→ high line losses→ low current capability→ no high-Zo lines
H
W
+ HWHZ
r
oo 2/1~
εη
...need to flip-chip bond
no substrate radiation, no substrate losses
InP mm-wave PA (Rockwell)
ECE194J /594J notes, M. Rodwell, copyrighted 2011
No breaks in ground plane
IC Interconnects -- Inverted Thin-Film Microstrip
narrow line spacing → IC density
... no ground breaks at device placements
still have problem with package grounding
thin dielectrics → narrow lines→ high line losses→ low current capability→ no high-Zo lines
...need to flip-chip bond
Some substrate radiation / substrate losses
InP 150 GHz master-slave latch
InP 8 GHz clock rate delta-sigma ADC
ECE194J /594J notes, M. Rodwell, copyrighted 2011
VLSI Interconnects with Ground Integrity & Controlled Zo
negligible breaks in ground plane
narrow line spacing → IC density
negligible ground breaks @ device placements
still have problem with package grounding
thin dielectrics → narrow lines→ high line losses→ low current capability→ no high-Zo lines
...need to flip-chip bond
no substrate radiation, no substrate losses
ECE194J /594J notes, M. Rodwell, copyrighted 2011
No clean ground return ? → interconnects can't be modeled !
35 GHz static dividerinterconnects have no clear local ground returninterconnect inductance is non-localinterconnect inductance has no compact model
InP 8 GHz clock rate delta-sigma ADC
8 GHz clock-rate delta-sigma ADCthin-film microstrip wiringevery interconnect can be modeled as microstripsome interconnects are terminated in their Zosome interconnects are not terminated...but ALL are precisely modeled
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Active Devices: Bipolar Transistors
ECE194J /594J notes, M. Rodwell, copyrighted 2011
HBT Physical Structure
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Physical structure, symbolic
baseBC gradecollector
N+ sub collector
semi-insulating InP substrate
emitter
emittercontact
base contact
cT
b,contWeWebW
underWN- drift collector
base contact
collector contact
bT
cW
EB grade
drawing lar toperpendicu LengthStripe Device EL=
ECE194J /594J notes, M. Rodwell, copyrighted 2011
0
5
10
15
20
0 1 2 3 4V
ce
mA
/µm
2
Bipolar Transistor: DC characteristics: common-emitter
Vbr,ceo
bc II β=
10-12
10-10
10-8
10-6
10-4
10-2
0 0.25 0.5 0.75 1
I c , I
b (A)
Vbe
(V)
Ic
Ib
satceV ,
maxJ
ion.documentatproject design in ninformatio More
density.power Maximumeffect,Kirk :byset is This.density current operating maximuma have HBTs maxJ
ECE194J /594J notes, M. Rodwell, copyrighted 2011
HBT hybrid-Pi equivalent-circuit model
cbf τ+τ=τ
Ccbi
Ccbx
Rbe
RbbB C
ERex
Rc
Vbe
CjeCbe,diff =gmτ f
gmVbee-jωτc
mobe gR /β=
)exp( cmom jgg ωτ−=
C
nkTqIg cmo /=
( )( ) ./1 toproportion in vary ,,,
, toproportion in vary ,, : lengthemitter of fingers HBT Given
max, Efingerccexbb
Efingercbxcbije
Efinger
LNIRRRLNCCC
LN
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Active Devices: MOSFETs
ECE194J /594J notes, M. Rodwell, copyrighted 2011
MOSFETS
N+ source N+ drain
source contact (silicide) drain contact (silicide)
N+ polygate
gate metal(silicide) dielectric
sidewall
gate oxide
P substrate
S D S D S D S
G
G
Wg
Cross-Section Layout (multi-finger)
P substrate
gatedielectric
N+polysilicongate
inversionlayer
ECE194J /594J notes, M. Rodwell, copyrighted 2011
MOSFET DC Characteristics
ID
VDS
increasingVGS
gthgsgoxD LVVWcI 2/)(current limitedmobility
2, −=
−
µµ
)(current limitedvelocity
, thgssatgoxvD VVvWcI −=−
1
Expression dGeneralize
,
2
,
=
+
µD
D
vD
D
II
II
Id
VgsVth
mobility-limited
velocity-limited
: voltageknee thenlarger tha voltagesdrainFor
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Knee Voltage: Mobility-Limited Case
VGD=Vth
regionscurrent -constant and Ohmic the betweenboundary thedefines voltageknee The
ID
VDS
increasingVGS
Ohm
ic constant-current
thgsdsdg VVVV −=−= whenoccurs curve in knee the
regime, limited-mobility theIn
IDRDVGD=Vth
IDRS
s.resistance drain & source parasitic theacross drops by voltage increasedfurther is Voltage KneeThe
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Knee Voltage: Velocity-Limited Case
µ/ whenoccurs curve in knee theregime, limited- velocity theIn
gsatds LvV =
s.resistance drain & source parasitic theacross drops by voltage
increasedfurther is Voltage Knee theAgain,
VDS=vsatLg/µ
IDRD
VDS=vsatLg/µ
IDRS
ECE194J /594J notes, M. Rodwell, copyrighted 2011
MOSFET Transconductance
gthgsgoxGS
Dm
gthgsgoxD
LVVWcVIg
LVVWcI
/)(
2/)( limitedmobility
2,
−=∂∂
=→
−=
−
µ
µµ
satgoxGS
Dm
thgssatgoxvD
vWcVIg
VVvWcI
=∂∂
=→
−=−
)( limitedvelocity
,
Id
VgsVth
∆V
gm
VgsVth
∆V
mobility-limited
velocity-limited
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Linear vs. Square-Law Characteristics: 90 nm
ECE194J /594J notes, M. Rodwell, copyrighted 2011
90 nm MOSFET DC Characteristics
3V~1/ V 6.0||mm/S 7.0μm/mS 7.0/
channel-P
3V~1/ V 6.0mm/S 4.1μm/mS 4.1/
channel-N
λ
λ
=
===
=
===
th
satoxgm
th
satoxgm
VvcWg
VvcWg
ECE194J /594J notes, M. Rodwell, copyrighted 2011
Device Structure and Model
( ) ( )( )
( )
mi
gds
ggd
ggeq
gs
thgsgeq
geffeq
m
gRNWGNWC
NWLT
C
VVNWT
NWvT
g
/1~
~
or ~
∝
∝
−
ε
µεε
gdb
gsb
gs
gd
endg
g
sg
NWCNWC
NWRNWR
NR
NW
LR
∝
∝
∝
∝
+
/1/1
212~ ρ
CgdRg
Ri
Cgs Vg’s’
gmVg’s’ Gds
Rs
RdG
D
S
Csb
Cdb
CgdRg
Ri
Cgs Vg’s’
gmVg’s’ Gds
Rs
G
D
S
Csb
Cdb
S D S D S D S
G
G
Wg
contacts substrate ample -fingers gateshort -
using Increase maxf
widthgate fingers, gate # == gWN
ECE194J /594J notes, M. Rodwell, copyrighted 2011
CgdRin
Cgsx Vg’s’
gmxVg’s’ GdsxG
D
S
Cdb
Csb
Oversimplified Model
igsin
sm
dsdsx
sm
gsgsx
sm
mmx
RRRRRg
GG
RgC
C
Rggg
+++
+
+
~
1
~
1~
1~
etc analysis, hand roughFor CgdRg
Ri
Cgs Vg’s’
gmVg’s’ Gds
Rs
G
D
S
Csb
Cdb
gdgdsigs
gddsmgdmgs
CRGRRRff
CRRgCgCf
π
π
τ
τ
2)(2~
)(//~2/1sfrequencie cutoff eApproximat
max +++
+++
ECE194J /594J notes, M. Rodwell, copyrighted 2011
End