Transcript V GS

Chapter 2
Field-Effect
Transistors(FETs)
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Outline
• Introduction
• Device Structure and Physical Operation
• Current-Voltage Characteristics
• MOSFET Circuit at DC
• The MOSFET as an amplifier
• Biasing in MOS Amplifier Circuits
• Small-signal Operation and Models
• Single-Stage MOS amplifier
• The MOSFET Internal Capacitance and High-Frequency Model
• The depletion-type MOSFET
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Introduction
• Characteristics
 Far more useful than two-terminal device
 Voltage between two terminals can control the current
flows in third terminal
 Quite small
 Low power
 Simple manufacturing process
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Introduction
• Classification of MOSFET
 MOSFET
 P channel
 Enhancement type
 Depletion type
 N channel
 Enhancement type
 Depletion type
 JFET
 P channel
 N channel
• Widely used in IC circuits
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Device Structure and Physical
Operation
• Device structure of the enhancement NMOS
• Physical operation
• p channel device
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Device Structure of the
Enhancement-Type NMOS
Perspective view
Four terminals
Channel length
and width
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Device Structure of the
Enhancement-Type NMOS
Cross-section view.
 L = 0.1 to 3 mm
W = 0.2 to 100 mm
Tox= 2 to 50 nm
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Physical Operation
•
Creating an n channel
•
Drain current controlled by vDS
•
Drain current controlled by vGS
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Creating a Channel for Current Flow
The enhancement-type
NMOS transistor with a
positive voltage applied to
the gate.
 An n channel is induced
at the top of the substrate
beneath the gate.
Inversion layer
Threshold voltage
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Drain Current Controlled by Small
Voltage vDS
An NMOS transistor with
vGS > Vt and with a small vDS
applied.
The channel depth is
uniform.
The device acts as a
resistance.
The channel conductance is
proportional to effective
voltage.
Drain current is proportional
to (vGS – Vt) vDS.
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vDS Increased
Operation of the
enhancement NMOS
transistor as vDS is
increased.
The induced channel
acquires a tapered shape.
Channel resistance
increases as vDS is
increased.
Drain current is
controlled by both of the
two voltages.
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Channel Pinched Off
• Channel is pinched off
Inversion layer disappeared at the drain point
Drain current isn’t disappeared
• Drain current is saturated and only
controlled by the vGS
• Triode region and saturation region
• Channel length modulation
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Drain Current Controlled by vGS
• vGS creates the channel.
• Increasing vGS will increase the conductance
of the channel.
• At saturation region only the vGS controls
the drain current.
• At subthreshold region, drain current has
the exponential relationship with vGS
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p Channel Device
• Two reasons for readers to be familiar with p channel device
 Existence in discrete-circuit.
 More important is the utilization of CMOS circuits.
• Structure of p channel device
 The substrate is n type and the inversion layer is p type.
 Carrier is hole.
 Threshold voltage is negative.
 All the voltages and currents are opposite to the ones of n channel
device.
 Physical operation is similar to that of n channel device.
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Complementary MOS or CMOS
The PMOS transistor is formed in n well.
Another arrangement is also possible in which an n-type body is used
and the n device is formed in a p well.
CMOS is the most widely used of all the analog and digital IC circuits.
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Current-Voltage Characteristics
•
•
•
•
•
•
Circuit symbol
Output characteristic curves
Channel length modulation
Characteristics of p channel device
Body effect
Temperature effects and Breakdown Region
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Circuit Symbol
(a)
Circuit symbol for the n-channel enhancement-type MOSFET.
(b)
Modified circuit symbol with an arrowhead on the source terminal to distinguish it
from the drain and to indicate device polarity (i.e., n channel).
(c)
Simplified circuit symbol to be used when the source is connected to the body or when
the effect of the body on device operation is unimportant.
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Output Characteristic Curves
(a) An n-channel enhancementtype MOSFET with vGS and
vDS applied and with the
normal directions of current
flow indicated.
(b) The iD–vDS characteristics for
a device with k’n (W/L) = 1.0
mA/V2.
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Output Characteristic Curves
• Three distinct region
 Cutoff region
 Triode region
 Saturation region
• Characteristic equations
• Circuit model
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Cutoff Region
• Biased voltage
vGS  Vt
• The transistor is turned off.
iD  0
• Operating in cutoff region as a switch.
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Triode Region
•
Biased voltage
vGS  Vt
vDS  vGS  Vt
•
The channel depth from uniform to tapered shape.
•
Drain current is controlled not only by vDS but also
by vGS
W 
1
2
iD  k n '
(vGS  Vt )vDS  vDS 
L 
2

W
 k n ' (vGS  Vt )vDS
L
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Triode Region
•
Assuming that the drain-t-source voltage is
sufficiently small.
vDS  2VOV
•
The MOS operates as a linear resistance
rDS 

v DS
iD

vGS VGS
1
kn '
1
kn '
W
(VGS  Vt )
L
W
VOV
L
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Saturation Region
•
Biased voltage
vGS  Vt
vDS  vGS  Vt
•
The channel is pinched off.
•
Drain current is controlled only by vGS
W
iD  k n ' （vGS  Vt ) 2
L
1
2
•
Drain current is independent of vDS and behaves as
an ideal current source.
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Saturation Region
The iD–vGS characteristic
for an enhancement-type
NMOS transistor in
saturation
Vt = 1 V, k’n W/L = 1.0
mA/V2
Square law of iD–vGS
characteristic curve.
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Relative Levels of the Terminal
Voltages
The relative levels of the
terminal voltages of the
enhancement NMOS
transistor for operation in
the triode region and in
the saturation region.
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Channel Length Modulation
•
•
Explanation for channel length modulation

Pinched point moves to source terminal with the voltage
vDS increased.

Effective channel length reduced

Channel resistance decreased

Drain current increases with the voltage vDS increased.
Current drain is modified by the channel length
modulation
W
2
iD  k n ' （vGS  Vt )（
1＋vDS )
L
1
2
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Channel Length Modulation
The MOSFET parameter VA depends on the process technology and, for a
given process, is proportional to the channel length L.
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Channel Length Modulation
•
MOS transistors don’t behave an ideal current
source due to channel length modulation.
•
The output resistance is finite.
 iD 
ro  


v
 DS 
•
1
vGS  const.
1
VA


I D I D
The output resistance is inversely proportional to the
drain current.
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Large-Signal Equivalent Circuit
Model
Large-signal equivalent circuit model of the n-channel MOSFET in
saturation, incorporating the output resistance ro. The output
resistance models the linear dependence of iD on vDS
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Characteristics of p Channel Device
(a) Circuit symbol for the p-channel enhancement-type MOSFET.
(b) Modified symbol with an arrowhead on the source lead.
(c) Simplified circuit symbol for the case where the source is connected to the
body.
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Characteristics of p Channel Device
The MOSFET with voltages applied and the directions of current flow
indicated.
The relative levels of the terminal voltages of the enhancement-type
PMOS transistor for operation in the triode region and in the saturation
region.
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Characteristics of p Channel Device
Large-signal equivalent circuit model of the p-channel MOSFET in
saturation, incorporating the output resistance ro. The output
resistance models the linear dependence of iD on vDS
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The Body Effect
• In discrete circuit usually there is no body effect due to the
connection between body and source terminal.
• In IC circuit the substrate is connected to the most negative
power supply for NMOS circuit in order to maintain the pn
junction reversed biased.
• The body effect---the body voltage can control iD




Widen the depletion layer
Reduce the channel depth
Threshold voltage is increased
Drain current is reduced
• The body effect can cause the performance degradation.
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Temperature Effects and Breakdown
Region
• Drain current will decrease when the
temperature increase.
• Breakdown
Avalanche breakdown
Punched-through
Gate oxide breakdown
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MOSFET Circuit at DC
a.
Assuming device operates in saturation thus iD satisfies with iD~vGS
equation.
b.
According to biasing method, write voltage loop equation.
c.
Combining above two equations and solve these equations.
d.
Usually we can get two value of vGS, only the one of two has
physical meaning.
e.
Checking the value of vDS
i.
if vDS≥vGS-Vt, the assuming is correct.
ii.
if vDS≤vGS-Vt, the assuming is not correct. We shall use triode
region equation to solve the problem again.
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MOSFET Circuit at DC
The NMOS transistor is
operating in the
saturation region due to
VGD  Vt
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MOSFET Circuit at DC
Assuming the MOSFET operate in the saturation region
Checking the validity of the assumption
If not to be valid, solve the problem again for triode region
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The MOSFET As an Amplifier
Basic structure of the
common-source amplifier.
Graphical construction to
determine the transfer
characteristic of the
amplifier in (a).
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The MOSFET As an Amplifier and
as a Switch
Transfer characteristic
showing operation as an
amplifier biased at point Q.
Three segments:
XA---the cutoff region
segment
AQB---the saturation
region segment
BC---the triode region
segment
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Biasing in MOS Amplifier Circuits
•
Voltage biasing scheme
 Biasing by fixing voltage
 Biasing with feedback resistor
•
Current-source biasing scheme
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Biasing in MOS Amplifier Circuits
The use of fixed bias
(constant VGS) can result in a
large variability in the value
of ID.
 Devices 1 and 2 represent
extremes among units of the
same type.
Current becomes
temperature dependent
Unsuitable biasing method
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Biasing in MOS Amplifier Circuits
Biasing using a fixed voltage at the gate, and a resistance in the source lead
(a) basic arrangement;
(b) reduced variability in ID;
(c) practical implementation using a single supply;
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Biasing in MOS Amplifier Circuits
(d) coupling of a signal source to the gate using a capacitor CC1;
(e) practical implementation using two supplies.
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Biasing in MOS Amplifier Circuits
Biasing the MOSFET
using a large drain-to-gate
feedback resistance, RG.
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Biasing in MOS Amplifier Circuits
(a) Biasing the MOSFET using a constant-current source I.
(b) Implementation of the constant-current source I using a current mirror.
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Small-Signal Operation and Models
•
The ac characteristic
 Definition of transconductance
 Definition of output resistance
 Definition of voltage gain
•
Small-signal model
 Hybrid π model
 T model
 Modeling the body effect
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The ac Characteristic
Conceptual circuit utilized to study
the operation of the MOSFET as a
small-signal amplifier.
Small signal condition
v gs  2VOV
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The ac Characteristics
•
The definition of transconductance
gm 
•
iD
vGS
 kn '
vGS VGS
The definition of output resistance
v DS
ro 
iD
•
W
VOV
L
iD  I D
VA

ID
The definition of voltage gain
Av 
vo
  g m RD
vi
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The Small-Signal Models
(a) neglecting the the channel-length modulation effect
(b) including the effect of channel-length modulation, modeled by
output resistance ro = |VA| /ID.
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The Small-Signal Models
(a) The T model of the MOSFET augmented with the drain-to-source
resistance ro.
(b) An alternative representation of the T model.
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Modeling the Body Effect
Small-signal equivalent-circuit model of a MOSFET in
which the source is not connected to the body.
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Single-Stage MOS Amplifier
•
Characteristic parameters
•
Basic structure
•
Three configurations
 Common-source configuration
 Common-drain configuration
 Common-gate configuration
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Characteristic Parameters of
Amplifier
This is the two-port network of amplifier.
Voltage signal source.
Output signal is obtained from the load resistor.
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Definitions
• Input resistance with no load
vi
Ri 
ii R  
L
• Input resistance
vi
Rin 
ii
• Open-circuit voltage gain
Avo
• Voltage gain
vo

vi
RL  
Av 
vo
vi
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Definitions(cont’d)
• Short-circuit current gain
Ais 
io
ii
RL  0
• Current gain
Ai 
io
ii
• Short-circuit transconductance gain
io
Gm 
vi
RL  0
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Definitions(cont’d)
• Open-circuit overall voltage gain
v0
Gvo 
vsig
RL  
• Overall voltage gain
v0
Gv 
vsig
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Definitions(cont’d)
Output resistance of amplifier proper
vx
Ro 
ix
Output resistance
Rout
vi  0
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vx

ix
vsig 0
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Definitions(cont’d)
Voltage amplifier
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Definitions(cont’d)
Voltage amplifier
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Definitions(cont’d)
Transconductance amplifier
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Relationships
• Voltage divided coefficient
vi
Rin

vsig Rin  Rsig
Rin
RL
Gv 
Avo
Rin  Rsig
RL  Ro
RL
Av  Avo
RL  Ro
Ri
Gvo 
Avo
Ri  Rsig
Avo  Gm Ro
RL
Gv  Gvo
RL  Rout
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Basic Structure of the Circuit
Basic structure of the circuit
used to realize single-stage
discrete-circuit MOS
amplifier configurations.
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The Common-Source Amplifier
Common-source amplifier
based on the circuit of basic
structure.
Biasing with constantcurrent source.
CC1 And CC2 are coupling
capacitors.
CS is the bypass capacitor.
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Equivalent Circuit of the CS
Amplifier
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Equivalent Circuit of the CS
Amplifier
Small-signal analysis performed directly on the amplifier circuit
with the MOSFET model implicitly utilized.
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Characteristics of CS Amplifier
• Input resistance Rin  RG
• Voltage gain
Av   g m (ro // RD // RL )
• Overall voltage gain
Gv  
RG
g m ( RD // RL // ro )
RG  Rsig
• Output resistance
Rout  ro // RD
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Summary of CS Amplifier
• Very high input resistance
• Moderately high voltage gain
• Relatively high output resistance
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The Common-Source Amplifier with
a Source Resistance
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Small-signal Equivalent Circuit with
ro Neglected
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Characteristics of CS Amplifier with
a Source Resistance
• Input resistance Rin  RG
• Voltage gain
g m ( RD // RL )
Av  
1  g m RS
• Overall voltage gain
Gv  
RG
g m ( RD // RL )
RG  Rsig 1  g m RS
• Output resistance
Rout  RD
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Summary of CS Amplifier with a
Source Resistance
• Including RS results in a gain reduction by
the factor (1+gmRS)
• RS takes the effect of negative feedback.
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The Common-Gate Amplifier
Biasing with constant
current source I
Input signal vsig is
applied to the source
Output is taken at the
drain
Gate is signal
grounded
CC1 and CC2 are
coupling capacitors
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The Common-Gate Amplifier
A small-signal
equivalent circuit of the
amplifier in fig. (a).
T model is used in
preference to the π
model
Neglecting ro
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The Common-Gate Amplifier Fed
with a Current-Signal Input
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Characteristics of CG Amplifier
• Input resistance Rin  1
gm
• Voltage gain
Av  g m ( RD // RL )
• Overall voltage gain
• Output resistance
g m ( RD // RL )
Gv 
1  g m Rsig
Rout  RD
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Summary of CG Amplifier
• Noninverting amplifier
• Low input resistance
• Has nearly identical voltage gain of CS
amplifier, but the overall voltage gain is
smaller by the factor (1+gmRsig）
• Relatively high output resistance
• Current follower
• Superior high-frequency performance
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The Common-Drain or SourceFollower Amplifier
Biasing with current source
Input signal is applied to gate, output signal is taken at the source.
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The Common-Drain or SourceFollower Amplifier
Small-signal equivalentcircuit model
T model makes analysis
simpler
Drain is signal grounded
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Small-Signal Analysis Performed
Directly on the Circuit
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Circuit for Determining the Output
Resistance of CD Amplifier
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Characteristics of CD Amplifier
• Input resistance Rin  RG
• Voltage gain
ro // RL
Av 
1
ro // RL 
gm
• Overall voltage gain
• Output
RG
ro // RL
Gv 
1
RG  Rsig r // R  1
o
L
gm
resistance
1
1
Rout 
// ro 
gm
gm
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Summary of CD or Source-Follow
Amplifier
•
•
•
•
•
Very high input resistance
Voltage gain is less than but close to unity
Relatively low output resistance
Voltage buffer amplifier
Power amplifier
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Summary and Comparisons
• The CS amplifier is the best suited for obtaining the bulk
of gain required in an amplifier.
• Including resistance RS in the source lead of CS amplifier
provides a number of improvements in its performance.
• The low input resistance of CG amplifier makes it useful
only in specific application. It has excellent high-frequency
response. Can be used as a current buffer.
• Source follower finds application as a voltage buffer and as
the output stage in a multistage amplifier.
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The MOSFET Internal Capacitance
and High-Frequency Model
• Internal capacitances
 The gate capacitive effect




Triode region
Saturation region
Cutoff region
Overlap capacitance
 The junction capacitances
 Source-body depletion-layer capacitance
 drain-body depletion-layer capacitance
• High-frequency model
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The Gate Capacitive Effect
• MOSFET operates at triode region
C gs  C gd  12 WLCox
• MOSFET operates at saturation region
C gs  23 WLC ox

C gd  0
• MOSFET operates at cutoff region
C gs  C gd  0

C gb  WLCox
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Overlap Capacitance
• Overlap capacitance results from the fact that the source
and drain diffusions extend slightly under the gate oxide.
• The expression for overlap capacitance
Cov  WLovCox
• Typical value
Lov  0.05  0.1L
• This additional component should be added to Cgs and Cgd
in all preceding formulas.
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The Junction Capacitances
• Source-body depletion-layer capacitance
C sb 
C sb0
V
1＋ SB
Vo
• drain-body depletion-layer capacitance
C db 
C db 0
V
1＋ DB
Vo
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High-Frequency Model
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High-Frequency Model
(b) The equivalent circuit for the case in which the source is connected
to the substrate (body).
(c) The equivalent circuit model of (b) with Cdb neglected (to simplify
analysis).
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The MOSFET Unity-Gain
Frequency
• Current gain
Io
gm

I i s(Cgs  Cgd )
• Unity-gain frequency
gm
fT 
2 (Cgs  Cgd )
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The Depletion-Type MOSFET
• Circuits symbol
• Structure
• Characteristic curves
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Circuit Symbol for the n-Channel
Depletion-Type MOSFET
(a) Circuit symbol for the n-channel depletion-type MOSFET.
(b) Simplified circuit symbol applicable for the case the substrate
(B) is connected to the source (S).
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Physical Structure
• The structure of depletion-type MOSFET is
similar to that of enhancement-type MOSFET
with one important difference: the depletion-type
MOSFET has a physically implanted channel.
• There is no need to induce a channel.
• The depletion MOSFET can be operated at both
enhancement mode and depletion mode.
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Characteristic Curves
Transistor with current and
voltage polarities indicated.
Typical value for discrete
transistor: Vt = –4 V and
kn(W/L) = 2 mA/V2
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The Output Characteristic Curves
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The iD–vGS Characteristic in
Saturation
the iD–vGS characteristic in saturation.
Expression of characteristic equation
W
iD  12 k n ' （vGS  Vt ) 2
L
Drain current with vGS  0
I DSS
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W 2
 k n ' Vt
L
1
2
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The iD–vGS Characteristic in
Saturation
Sketches of the iD–vGS characteristics for MOSFETs of enhancement and
depletion types
The characteristic curves intersect the vGS axis at Vt.
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