Cirrus Logic offers a variety of low-voltage CMOS chopper-stabilized amplifiers.
The chopper-stabilized amplifiers designed at Cirrus Logic are unique. These amplifiers offer performance benefits
that combine the best features of bipolar amplifiers with the best features of chopper amplifiers. The intent of this
application note is to understand Cirrus Logic's unique technology and to see how it can be applied in various measurement applications. But before the applications are discussed, the following provides a brief overview of the concepts involved in a chopper-stabilized amplifier.
2. CHOPPER AMPLIFIER AND CHOPPER-STABILIZED AMPLIFIER BASICS
Not everyone is familiar with chopper amplifiers and chopper-stabilized amplifiers. A look back at some history can
help us understand how the chopper-stabilized amplifier operates.
Figure 1 illustrates the block diagram of a chopper-stabilized amplifier. A chopper-stabilized amplifier is a DC am-
plifier whose offset is stabilized by a chopping amplifier. The basic amplifier diagram in Figure 1 is called the Goldberg configuration, named after E. A. Goldberg, an engineer who designed and patented electron tube-based,
chopper-stabilized amplifiers for RCA (Radio Corporation of America) in the 1940s and 1950s.
The Goldberg configuration was later used in a transistorized chopper-stabilized amplifier designed and sold
by Zeltex Corporation in the 1970s for about $125 (US). The Zeltex chopper-stabilized amplifier follows the basic
block diagram of Figure 1. The input signal (e
signal paths. (The Goldberg configuration amplifier could only be used as an inverting amplifier.) The first path is
into Amplifier #1 of Figure 1. Components R1-C1 act as a high-pass filter that prevents the DC portion of the signal
from passing directly into Amplifier #1. The second path is through a low-pass filter composed of R2 and C2. The
R2-C2 filter limits the bandwidth of the signal to be chopped by the chopper amplifier. Amplifier #2 is the chopper
R4
Oscillator
) at the inverting input of the amplifier travels through two different
amplifier. The chopper amplifier is really a modulation system in which the DC and very low-frequency portion of the
input signal is alternately turned on and off. This results in the signal being modulated at the carrier (chopping) frequency. An oscillator in the chopper amplifier toggles switches S1 and S2 on and off simultaneously. When switch
S1 is conducting, the input to the chopper amplifier is ground. When switch S1 is off, the input signal is allowed to
pass into Amplifier #2. The effect of chopping is to turn the DC input signal into a square wave (AC) signal whose
amplitude changes between ground and the amplitude of the input signal. This signal is then amplified by the AC
amplifier. Once the signal is amplified as an AC signal, it is restored to ground reference by the output chopping
switch. This resulting signal, which is a ground-referenced square wave, is then filtered with a low-pass filter composed of resistors R5 and R6 in conjunction with capacitor C5. The corner frequency of this filter is very low – typically only fractions of a Hertz. The time constant must be very long to maintain the voltage on the filter capacitor
over the half cycle when the chopped signal is not presented to the output filter.
Figure 2 illustrates the DC amplifier portion of the Zeltex device. This amplifier was constructed with a matched bi-
polar transistor pair as the front end. The open loop gain of the DC amplifier is about 94 dB.
Figure 3 illustrates the actual chopper amplifier portion of the Zeltex amplifier. The amplifier AC gain is about 3000,
but because the signal is on only 50% of the time, the effective gain is only half as much. Therefore the AC amplifier
gain is about 1500, or about 63 dB. The chopping oscillator operates at about 200 Hz. Note that the chopper output
is filtered by a low-pass filter with an extremely low corner frequency.
+15V
-IN
From AC
Amplifier
51k
1N459
26
C1
0.1uFR1200k
0.005uF
17
2N2914
35
51k
2N4248
10M
500k56k
10pF
2.4k
100k
-15V
Figure 2. Amplifier 1: DC Amplifier Portion of the Zeltex Module
E304
2N4248
680
OUT
2AN300REV1
+15V
AN300
10k
150
2N4299
10k
22uF
150
10k
51k
C4
0.033uF
2N3565
22uF
From
Oscillator
R6
51kR5200k
S2
2N2946
fc = 0.009Hz
C5
1N459
68uF
To DC
1N459
R2
100k
From
Oscillator
R3
100k
C2
0.033uF
C3
4700pF
S1
M5079
R4
2.0M
3.9k
E305
1k
18k
68uF
-15V
Figure 3. Amplifier 2: Chopper Amplifier Portion of the Zeltex Module
The gain transfer functions of the two amplifiers are multiplied together (or added when stated in dB). The combination of the two amplifiers produces an open loop gain of about 160 dB. One of the difficulties in the design of the
chopper-stabilized amplifier combination is ensuring stability. The DC performance of the combined amplifiers is dictated by the performance of the chopping input. Input current of the Zeltex amplifier was dominated by charge injection in the chopping switch at the input of the chopper amplifier. Offset voltage and offset voltage drift of the amplifier
combination was determined by how close the chopping switch at the input of the chopper amplifier approximated
the ideal. The Zeltex amplifier achieved less than 100 pA of input bias current with an offset voltage drift less than
50 nV / °C.
Figure 4 illustrates a typical chopper-stabilized amplifier designed using electron tubes with the amplifiers connected
in the Goldberg configuration. The circuit has the same layout as the block diagram of Figure 1. The chopping
switches were mechanical vibrating switches (about 400 Hz) manufactured by Airpax Corporation. The output filter
exhibits an extremely long time constant.
E.A. Goldberg filed a U.S. patent (#2,684,999; assigned to RCA) for a tube-based chopper-stabilized amplifier on
April 28, 1948. But the invention of the chopper architecture itself predates this. J. W. Milnor filed for a U.S. patent
on a chopper amplifier on January 17, 1918.
AN300REV13
DC Amp
AN300
R2
330
C4
3nF
R8
220k
Z
f
C2
350pF
100k
220k
C3
10pF
+300V
10k
e
IN
C5
0.01uF
AC Amp
Figure 4. Chopper-stabilized Amplifier Using Electron Tubes and Mechanical Vibrating Swit ches
680k
C1
R3
10k
2uF
R1
10M
5751
R7
1k
Z
i
fc = 0.008 Hz
C6
2uF
R4
10M
V2A
2M
2.2M
½ 5751
760k
Output
6AQ5
-250V
-400V
+300V
R5
2.2M
C7
0.01uF
2.2M
R6
1k
220k
0.1uF
5751
220k
0.1uF
1M1M1k
1k
220k
½ 5751
0.1uF
1k
NOTE: 5751 = Ruggedized 12AX7.
3. MODERN CHOPPER-STABILIZED AMPLIFIERS
Monolithic chopper-stabilized amplifiers became available in the late 1970s. Different chopping architectures have
been promoted by various vendors. The various architectures will not be examined in detail here. Before discussing the particulars of the Cirrus Logic chopper-stabilized amplifiers, it will be beneficial to understand some differences found in bipolar versus MOS transistors.
For many years bipolar transistors dominated monolithic amplifier designs. Bipolar transistors have some distinct
advantages over CMOS transistors for some performance parameters. The bipolar transistor provides higher
transconductance (I/V gain) for a specific value of operating current. The bipolar device, because of its construction, also provides lower noise than can easily be achieved in a MOS transistor, for devices of similar silicon area.
The wide band spot noise level is lower in the bipolar transistor. And a much lower 1/f noise corner can be
achieved in a bipolar transistor. Bipolar transistors can also be better matched when manufactured together on the
same silicon die.
Most recently, the most prominent semiconductor processes being developed to shrink the geometry size of
devices is being applied to CMOS technology. CMOS is favored because it can provide lower power consumption
for massive digital chips with millions of transistors. Smaller transistors mean the availability of more transistors in
a given area of silicon. This results in smaller device package sizes. In the last decade, more analog and mixed
signal devices have been designed to take advantage of the smaller geometry CMOS processes. This includes
monolithic amplifiers based upon CMOS processes.
4AN300REV1
AN300
As mentioned previously, bipolar transistors have long dominated the world of operational amplifiers. Let's look at
some of the differences of parameters of bipolar transistors versus MOS transistors. Understanding the differences between these two technologies can help explain some of the constraints on the architectural choices used
in the design of CMOS chopper-stabilized amplifiers.
The construction of bipolar transistors and MOS transistors are very different. The difference in construction results
in large differences in some performance parameters. One area of significant difference is noise performance.
Figure 5 illustrates a noise plot for a bipolar transistor. This hypothetical but typical device exhibits a spot noise at 1
kHz of 4 nV/√Hz
difficulty achieving this level of noise performance. Figure 6 illustrates a noise plot for a hypothetical but typical
MOS transistor. This device exhibits a spot noise of 17 nV/√Hz
with a 1/f corner at 2.5 Hz. Because of the difference in construction, a MOS transistor would have
at 50 kHz with a 1/f corner at 2000 Hz.
Bipolar Transistor Noise
100
10
1
0.11101001k
Figure 5. Noise Performance Plot for a Bipolar Transistor
Frequency (Hz)
MOS Transisitor Noise
1000
100
10
1
101001k10k100k
Frequency (Hz)
Figure 6. Noise Performance Plot for a MOS Transistor
Note from Figure 5 that the magnitude of the noise of the bipolar transistor at 0.1 Hz is about 20 nV/√Hz. The spot
noise in the example MOS transistor does not match this 20 nV/√Hz
value until the frequency for the MOS transistor is at about 5 kHz. A MOS transistor can be designed to achieve a lower spot noise and a lower 1/f corner frequency than what is shown in Figure 6 by significantly increasing the size of the device and by increasing its
AN300REV15
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