Lecture 11
MOSFET – part 2
Prof. José Luís Güntzel
[email protected]
Integrated Circuits & Systems
INE 5442
Federal University of Santa Catarina
Center for Technology
Computer Science & Electronics Engineering
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.2
I D -V DS Characteristics of NMOS (I-V Curves)
Long-channel NMOS (W/L = 1.5 and Ld=10 µm) Short-channel NMOS (W/L=1.5 and Ld=0.25 µm)
Source: Rabaey; Chandrakasan; Nikolic, 2003
-4
0 0.5 1 1.5 2 2.5
0 0.5 1 1.5 2 2.5
x 10
VGS= 2.5 V
VGS= 2.0 V
VGS= 1.5 V
VGS= 1.0 V
Velocity Saturation
Linear dependence on VGS
VDS = VGS - VT
€
VDSAT =κ(VGT)VGT
VDS (V) ID (A
0 0.5 1 1.5 2 2.5
0 1 2 3 4 5 6x 10-4
VGS= 2.5 V
VGS= 2.0 V
VGS= 1.5 V
VGS= 1.0 V
Resistive
Saturation
VDS = VGS - VT
Quadratic dependence on VGS
VDS (V) ID (A
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.3
I D -V GS Characteristics of NMOS (I-V Curves)
Source: Rabaey; Chandrakasan; Nikolic, 2003
0 0.5 1 1.5 2 2.5
0 1 2 3 4 5 6x 10-4
quadratic
ID (A)
VGS (V)
0 0.5 1 1.5 2 2.5
0 0.5 1 1.5
2 2.5x 10-4
quadratic linear
VGS (V) ID (A
Long-channel NMOS (W/L = 1.5 and Ld=10 µm) Short-channel NMOS (W/L=1.5 and Ld=0.25 µm) VDS = 2.5 V (NMOS devices are saturated)
Subthreshold conductance
Subthreshold conductance
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.4
Source: Rabaey; Chandrakasan; Nikolic, 2003
-2.5! -2! -1.5! -1! -0.5! 0!
-1!
-0.8!
-0.6!
-0.4!
-0.2!
0!x 10!-4!
VGS = -1.0V VGS = -1.5V
VGS = -2.0V
VGS = -2.5V
VDS (V) ID (A
The polarities of all voltages and currents are reversed
Short-channel PMOS (Wd=0.375 and Ld=0.25 µm, W/L=1.5 )
I D -V DS Characteristics of PMOS
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.5
NMOS x PMOS (I-V Curves)
Velocity saturation is less pronounced in PMOS (due to higher value of critical electrical field, resulting
from smaller mobility of holes)
Source: Rabaey; Chandrakasan; Nikolic, 2003
-4
0 0.5 1 1.5 2 2.5
0 0.5 1 1.5 2 2.5
x 10
VGS= 2.5 V
VGS= 2.0 V
VGS= 1.5 V
VGS= 1.0 V
Velocity Saturation
VDS = VGS - VT
€
VDSAT =κ(VGT)VGT
VDS (V) ID (A
-2.5! -2! -1.5! -1! -0.5! 0!
-1!
-0.8!
-0.6!
-0.4!
-0.2!
0!x 10!-4!
VGS = -1.0V VGS = -1.5V
VGS = -2.0V
VGS = -2.5V
VDS (V) ID (A
Minimum-size (short-channel) NMOS and PMOS (Wd=0.375 and Ld=0.25 µm, W/L=1.5 )
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.6
Simple Model for Manual Analysis
Source: Rabaey; Chandrakasan; Nikolic, 2003
S D
G
B
A Single Current Source Using First-Order Expressions
Employs 5 parameters, which are positive for NMOS and negative for PMOS:
VT0, VDSAT , , ,
€
k'
n€
λ
€
γ
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.7
Simple Model versus Spice
0 0.5 1 1.5 2 2.5
0 0.5 1 1.5 2
2.5 x 10-4
VDS (V)
I D (A)
Velocity Saturated Linear
Saturated
VDSAT=VGT VDS=VDSAT
VDS=VGT
Source: Rabaey; Chandrakasan; Nikolic, 2003
Minimum-size NMOS (Wd=0.375 and Ld=0.25 µm, W/L=1.5 )
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.8
Parameters for Manual Analysis
Source: Rabaey; Chandrakasan; Nikolic, 2003
Minimum-size NMOS (Wd=0.375 and Ld=0.25 µm)
VT0 (V) (V0.5) VDSAT (V) k’(A/V2) (V-1)
NMOS 0.43 0.4 0.63 115 x 10-6 0.06
PMOS −0.4 −0.4 −1 −30 x 10-6 −0.1
€
λ
€
γ
Notice: parameters to match well in the (VDS=2.5V, VGS=2.5V) region of 0.25µm NMOS
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.9
Experimental setup
ID
S
G B
+
-
[0,3.3] step 0,5 V
+
-
[0,3.3] step 0,050 V
D
2
3 1
1
+
VDD = 3.3 V
-
+ -
V
GS+ -
V
DSDetermining the I-D Curves of PMOS
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.10
• Circuit description (SPICE) – PMOS1.cir
– http://www.inf.ufsc.br/~guntzel/ine5442/parametros
Determining the I-D Curves of PMOS
Also available NMOS1.cir
SpiceOpus (c) 6 -> source PMOS1.cir
SpiceOpus (c) 7 -> dc v3 0 3.3 50m v2 0 3.3 0.5
SpiceOpus (c) 8 -> plot i(v3) xlabel VD[V] ylabel ID[A]
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.11
SpiceOpus (c) 1 -> source PMOS1.cir SpiceOpus (c) 2 -> setplot
new New plot
Current const Constant values (constants)
SpiceOpus (c) 3 -> dc v3 0 3.3 50m v2 0 3 0.5
SpiceOpus (c) 4 -> plot 1000*i(v3) xlabel VD[V] ylabel ID [mA]
VGS=-3.3 V
VGS=-2.3 V
VGS=-2.8 V
VGS=-1.8 V VGS=-1.3 V
Determining the I-D Curves of PMOS
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.12
The Transistor as a Switch (“Zero-Order Model”)
Source: Rabaey; Chandrakasan; Nikolic, 2003 & Galup, Schneider 2010
Ron
S D
VGS ≥ VT |VGS|
Non-ideal switch
Actual NMOS
?
What is the value of Ron? Abrupt transition from on to off?
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.13
The Transistor as a Switch (“Zero-Order Model”)
Source: Rabaey; Chandrakasan; Nikolic, 2003
IDSAT
VDD
VDS (VDDVDD/2)
ID
VDS > VDSAT : transistor is in velocity
saturation
or
with Resistance is inversely proportional to W/L
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.14
The Transistor as a Switch
Source: Rabaey; Chandrakasan; Nikolic, 2003
For VDD >> VT + VDSAT/2, Req is practically independent of VDD Once VDD achieves VT, Req increases significantly!
Simulated R
eqx V
DDMOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.15
The Transistor as a Switch
Source: Rabaey; Chandrakasan; Nikolic, 2003
VDD (V) 1 1.5 2 2.5
NMOS (kΩ) 35 19 15 13
PMOS (kΩ 115 55 38 31
R
eqof NMOS and PMOS Transistors in 0.25 µm (W/L=1, L=L
min)
For larger devices, divide Req by W/L
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.16
Dynamic Response of MOS Transistor
Is a function of time it takes to (dis)charge:
its intrinsic capacitances
interconnect lines and load capacitances
Origin of intrinsic capacitances:
The basic MOS structure
The channel charge
The depletion regions of reverse-biased pn-junctions of drain and source
Capacitance values depends on the applied voltages
(nonlinear capacitors)
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.17
MOS Gate Capacitance
If:
No lateral diffusion
Transistor in cut-off
C
gate= C
oxx WL
where C
ox= ε
oxt
oxMOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.18
MOS Structure Capacitances
t
ox Gate oxideL
Gate-bulk overlap Polysilicon gate
L
dW Top view
Cross section
x
dx
dLateral diffusions (Area =
x
d x W)Ld = designed length; L = effective length
Overlap capacitances (linear):
CGS0 = CGD0 =
= Cox xd W = C0 W
where C0 = Cgs0 or Cgd0 = overlap capacitance per
unit transistor
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.19
Gate Capacitance (Piece-Wise Linear Model)
Most important regions in digital design: saturation and cut-off
Source: Rabaey; Chandrakasan; Nikolic, 2003
Cut-off Linear Saturation
Operation region
CGCB CGCS CGCD CGC
= CGCB +CGCS +CGCD
CG
Cutoff CoxWL 0 0 CoxWL CoxWL + 2CoWL
Linear 0 CoxWL/2 CoxWL/2 CoxWL CoxWL + 2CoWL
Saturation 0 (2/3) CoxWL 0 (2/3) CoxWL (2/3) CoxWL + 2CoWL
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.20
Gate Capacitance
CGC as a function of VGS (VDS = 0 thus, linear mode)
CGC as a function of the degree of saturation
Source: Rabaey; Chandrakasan; Nikolic, 2003
VT Transistor is off
(cap between gate and body) Degree of saturation
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.21
Junction Capacitances (Diffusion Capacitances)
Bottom
Side wall
Side wall
Channel Source
ND
Channel-stop implant NA+
SubstrateNA W
xj
LS
Source: Rabaey; Chandrakasan; Nikolic, 2003
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.22
MOS Capacitances
p-substrate
S
n
+n
+Field oxide
substrate (bulk) contact
G D
CGS CGD
CSB CGB CDB
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.23
MOS Capacitances
Consider as NMOS transistor with the following parameters:
t
ox= 6 nm L= 0.24 μm W= 0.36 μm L
D=L
S= 0.625 μm C
0= 3 x 10
-10F/m
C
j0= 2 x 10
-3f/m2
C
jsw0= 2.75 x 10
-10F/m
Determine the zero-bias value of all relevant capacitances.
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.24
Capacitances in a 0.25 µm CMOS Process
Source: Rabaey; Chandrakasan; Nikolic, 2003
Cox
(fF/μm2)
CGD0 (fF/μm)
CJ (fF/μm2)
mj Φb (V)
CJSW (fF/μm)
mjsw Φbsw
(V)
NMOS 6 0.31 2 0.5 0.9 0.28 0.44 0.9
PMOS 6 0.27 1.9 0.48 0.9 0.22 0.32 0.9
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.25
1. RABAEY, J; CHANDRAKASAN, A.; NIKOLIC, B.
Digital Integrated Circuits: a design perspective.
2
ndEdition. Prentice Hall, 2003. ISBN:
0-13-090996-3.
2. WESTE, Neil; HARRIS, David. CMOS VLSI Design: a circuits and systems perspective.
Addison-Wesley, 4
thEdition, 2010. ISBN 978-0321547743.
References
MOSFET
Lecture 11 – 2012/2 Prof. José Luís Güntzel INE/CTC/UFSC
Integrated Circuits and Systems Slide 11.26