5 advancedmostransistors&analogdesign 12-13x2
TRANSCRIPT
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Advanced MOS transistor models:
Large Signals. Weak, Moderate and Strong Inversion.Small Signals #1
Layout Techniques:
The problem; Floorplan; Mismatches; Noise and Crosstalk Latch-up
#2
Introduction to noise in electronic circuits:Definitions. Filtered noise.Noise types in components.Noise analysis for circuits.
#3
4/29/2013Analog Integrated Systems [email protected]
2
Strong inversion
2
Subthreshold or Weak in
1( ) (1 ); ;
22
exp ; 1.4 ~ 1.8.
version
.
Boundary:
22 .
.
n Dm
GS t
Dm
T
m
D D
oxD GS t DS
Ef BS
G
GS t T G
SD D
T
G t T
O
SS
C Wi v V V n
n L V LV
v
Ig
V V
Ig
nV
g
I IV V nV V
V V
i I nnV
nV
= + = +
=
=
=
=
=
=
70mVt
V +
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! !"
#$ % !&' % "
Conventional designs: near weak inversion but not in
weak inversion: VOVD
150mV~200mV.
4/29/2013Analog Integrated Systems [email protected]
(! )" *
+& ! , -
M1
IB
VDD
vo
vI
2 2
Example:
102
100
00
E E
GS t OVD
E
OVD
V m o
V
A g r V L V L
V V V
V L VV
A
mV
= =
=
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./0//1
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( )
0
2
.
2 2
1.41 2
2 20.66
3
:1 3 30 1
exp 1 exp.
00
DGS M m
T
t t f SB f
M OX Tf SB
M t T S B
OX
M
GS M DS D M
T T
t t
IV V g
nV
V V v
nWI
v V vi I
C n V vL
V V CnV
nV
q N
C
C V V mV V mV
V
< =
= + + = = +
= =
=
=
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2
GS
( ) (1 );2
1
1 for long channelif usually
1.25 f
Strong Inversion: >
or short channel
; 6 +200mV
2
1
1
2
( )
02
H H t T t
Dm
GS
oxD GS t DS
E
n
GS
f A
t
t
A
SB
C Wi v V V
L
V L
v V V V
n
v V
nV V
Ig
V V
v
= +
=
+
= +
== =
=
+
=
+ +
=
4/29/2013Analog Integrated Systems [email protected]
Rules of thumb for vGS
:
There are unified models. Cost in complexity which
translates in computation time.
There are non-physical based models, fitting on
experimental data as BSIM3
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At high vGS
current becomes more linear again;
Mainly due to velocity saturation
Increase in electric field does not cause electrons to travel
through the channel faster due to colisions.
7 710 cm/s 10
_
cm/s
Velocity saturation
( ) is absolute max
does not depend on is a constant; not used for analog
VSDS ox SAT GS t ox SAT
GS
m SAT i WC V v V WC V g
v
= =
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Strong Inversion: Saturation
21 1 1= ( ) 2
2
Strong Inversion: Triode =
Weak Inversion: =
GS GS
Dm
GS v V
Dm OX GS t OX D
GS t
m OX DS
Dm
T
ig
v
IW Wg C V V C I
L V V L
Wg C V
L
IgnV
=
=
= =
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'0
2
0
0
1/ /
2
m m D
T
DSOX T GS t
I
g I g I InV
IWI C nV IC V V
L I
=
= =
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!
[ ]
, ,
;
= ( -1)
= 0.1 to 0.3
GS DS BS
GS GS DS DS
tD Dmb m
BS t BSV V V
mb m
D D Dds
DS DS Ev V v V
Vi ig g n
v V v
g g
i i Ig
v v V L= =
= =
= =
ro,
rds,gdsvgs
G D
S
gmb vbsgm vgs
B vbs
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"#
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"# $%
_
__ _
__
__ _
_
Weak Inversion
1
Strong Inversion
triode ( =0): saturation:2
13
20
0
32 222 2
gb i OX
DS
gs i OXgs i gd i OX
gd igb i
OXOX gb i
bs i bd if SB DS
f SB
bs i
nC W L C
n
V
C W L C C C W L C
CC
W L CW L C C
C C V VV
C
=
= = =
=
= = =
=
_
22 2
0
OX
f SB
bd i
W L C
V
C
=
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"# $&%
_ _
_
_ _
gs e gd e W
gb e L
bs e bd e S S
C C W C
C L C
C C A P
= = = = = +
% % #&'
$ ! % &2 ,
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"#
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# " '
REF
REF
Mismatch in Weak inversion
Mismatch in Strong invers
exp 1 15%. .
( )( / )
ion
21 6 ~ 10%
/
Better!
OUT t t
T T
OUT n oxt
n ox GS t
i V V
I n V n V
i CW LV
I W L C v V
+
+ + +
Advanced MOS transistor models:
Large Signals. Weak, Moderate and Strong Inversion.Small Signals #1
Layout Techniques:
The problem; Floorplan; Mismatches; Noise and Crosstalk Latch-up
#2
Introduction to noise in electronic circuits:Definitions. Filtered noise.Noise types in components.Noise analysis for circuits.
#3
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/ 3, , ! !2 &
, %/ , %% ! ! ! % ! & &2 !4
% 5 !% ! %% &3 ! !% ! % 2 3
$67 8 % &2 3
,!! "((2 & %
4/29/2013Analog Integrated Systems [email protected]
! 2 % 7$6 !
,! 2 ! & %,
9 ! % ! !5*
9 ! 2 !*
9 ! 2 3
! ,2 3*
9 !:*
9 % &2
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VDD
Input
Pad
vO
M1
M2
R
D1
D4
D3
D2
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)#
57
9 ! 2 %
9& % 9 ;
9% &2 ! 2 % !
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)#
! %
! , ! * %
! & !2 ! & 2
! $& ! ! &2dd
C DD B
diV R I L
dt = +
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)#
!
, ! &
!
& ! !
! ,
Package Pin Bond L Bond C
40 Pin Plastic 1,2
10,11
15nH
4.4nH
2.4pF
0.7pF
40 Pin Plasticwith socket
1,210,11
18.6nH7.6nH
2.6pF0.8pF
40 Pin Ceramic 1,2
10,11
20.9nH
9.0nH
2.7pF
0.8pF
In RF/fast analog use smaller packages or chip on board
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)#
! ! & 3 ,2% ! ! & &,
! =, ,!& % ! 8 *
% 2 ,!! % !! ! % 8
> ! & >
,2 & % %, 0 % %
) ! &
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)#
! "
$
8
[ ] [ ]
[ ]2int int int
/ / /
/ F/cm F
S line S
ox line
R t R R L W
C x C C LW
= =
= =
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)#
/% 2 ,:& ! & /
2 2 %% ! , & ,!
: !! 2
2 %% /
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8 ! 2 !2
? !
2::2 2::@ ! ::
2
!2 4 !
!4 ! %:&
>2 !
9 A ,!
9 3 %
9 ,! %%
9 %, 2 %%
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! ! !
! !
; 2 !
!
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! 2 ! &
:
2
%* !
2
% %
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6 ! :
!4 & % ! 52 %&
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* # ' ++ ,
#-
)2 ,!" !
7 !
! %% ! !! %
%4 , ! 42 % %
,! !
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% ! % ,
,! ! ! ;
! 42 % &2 % % B
&, % % ,2 % !
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!* !
! & 22 ,! !
! ! !
Minimum size should be
avoided, higher capacitance and
higher area. Transistors
matching is proportional to
1
W L
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( "
2 2 !
&" % 3
3 &2
9 $ 3 &
9 ! 3 2 &%% !! 3
,! !! 2 !! ! !
9 / :& ,! & %
3
; ! 2 &%% ,!
&2
clock
1/
ln
N
L L
i i
C CN K
C C
= =
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( "
= 3 &
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( "
C & : 3
" &
&2
( %3
% ,!
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" !-
, !
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( "
, ! ,2 !
! & &, % %, &
&
$ , % & , % !, 8 ! !
, %
%% ,!
! , 2 8 3 ! & C
, 5 8>
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#
>!: ! % & 2 !4 %
8 $8 ! 2
>!: 2 5 :
, &2 %%
A2 , ! & % !
2
A2 & ! & &2 2 2
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#
& !
2
& ! & % :?
>2 % : : ! ! 3 % :
, 3 % : ,
! , : :
! : : ! & !22
,! ! &
@ :
@ :
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02 %, 5 : ,3 ! % &2
9 2 & &2 & 9 &3 % & &2 &
2 ,! !
9 ,! ! &2 ! & ,! %%! %
9 2 !
9 C % :
Advanced MOS transistor models:
Large Signals. Weak, Moderate and Strong Inversion.Small Signals #1
Layout Techniques:
The problem; Floorplan; Mismatches; Noise and Crosstalk Latch-up
#2
Introduction to noise in electronic circuits:Definitions. Filtered noise.Noise types in components.Noise analysis for circuits.
#3
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(
>9)
9 D
>
D:9 )
9
D" /! "
/% " 2 2 &
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(
/! D % ,!!
/ "9D !; &2 ! 4 % &
9 8 / &
9 %
9 ,! ! ! !! 2 &
9 ! &, ! 5
2 2
0
1Noise power lim ( )
T
rmst
x t dt XT
= =
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(
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(
D
9 ! !! - / %%-
2 2 2
no(rms) n1(rms) n2(rms)
n1(rms) n2(rms) no(rms)
example: uncorrelated
10V; 5V 11.2V
V V V
V V V
= +
= = =
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().
D 2
9D; (; &,!
9 %42 ;
9 / 2; ! &,!
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(
).
7 63 3
( ) Vn KV ff
=
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().
6
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(
#
( )2
2 1
2
0
2 2 1
2 2 1
Noise spectral density: ; depending on frequency,
[units of ] Hz
Noise Power ( )
1) Thermal noise (white):
Resistors: MOS Transistors :
4 V Hz
14 A Hz
: 1 k ; 300K
T
n
n
x f
x
x f df
v kTR
i kTR
ex R T
=
=
=
= =
2 2 1
2 2 1
_
14 V Hz
4 A Hz
; : 2 / 3 for long channels,
1 MHz; 0.2V 1 for short channels (empirical)
n
m
n m
n rms
v kTg
i kT g
ex
f v
=
=
=
= = =
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( #
2 2 1
2 2 1
-25 2
2) noise in forward biased junctions:
2 A Hz
quiescient current white noise
3) noise in MOS :
1V Hz
depends on technology (in the order of 10 V F)
freque
=
=
n C
n
ox
Shot
i qI
Flicker
Kv
C WL f
K
ncy dependent: "1/ noise"f
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(
#
.E!71
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().
.E!71
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(
+ # " #+
VDD
M5
M3
M2M1
M4
vin-vin+
vout
vn5(t)
vn1(t) vn2(t)
vn3(t) v n4(t)
( )
( ) ( )
1
1 2
3
3 4
5
5 3
2 22 2 2
1 1 3 3
2
2 2 2 31 3
1
2
output referred noise
( ) 2 ( ) 2 ( )
input referred noise
( ) 2 ( ) 2 ( )
no nom o
n n
no nom o
n n
no m
n m
no m o n m o n
mneq n n
m
V Vg R
V V
V Vg R
V V
V g
V g
V f g R V f g R V f
gV f V f V f
g
= =
= = =
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(
+ # " #+
D 7 F = 7
: %%
*
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2
1
2
12 23 1 11 2(rms)2 2
1 1 1 3 1 1 1 1 3
ln2
( ) 2 ln
p
f
oxn n nneq neq
ox p ox pf
K f
C fK L K LK fV f V
C f W L W L W L C f W L
= + = +