Linear-in-dB gain control
Pin programmable gain ranges
−11 dB to +31 dB with 90 MHz bandwidth
9 dB to 51 dB with 9 MHz bandwidth
Any intermediate range, for example −1 dB to +41 dB
with 30 MHz bandwidth
Bandwidth independent of variable gain
1.3 nV/√Hz input noise spectral density
±0.5 dB typical gain accuracy
APPLICATIONS
RF/IF AGC amplifier
Video gain control
A/D range extension
Signal measurement
GENERAL DESCRIPTION
The AD603 is a low noise, voltage-controlled amplifier for use
in RF and IF AGC systems. It provides accurate, pin selectable
gains of −11 dB to +31 dB with a bandwidth of 90 MHz or 9 dB
to 51 dB with a bandwidth of 9 MHz. Any intermediate gain
range may be arranged using one external resistor. The input
referred noise spectral density is only 1.3 nV/√Hz and power
consumption is 125 mW at the recommended ±5 V supplies.
The decibel gain is linear in dB, accurately calibrated, and stable
over temperature and supply. The gain is controlled at a high
FUNCTIONAL BLOCK DIAGRAM
Variable Gain Amplifier
AD603
impedance (50 MΩ), low bias (200 nA) differential input; the
scaling is 25 mV/dB, requiring a gain control voltage of only 1 V
to span the central 40 dB of the gain range. An overrange and
underrange of 1 dB is provided whatever the selected range. The
gain control response time is less than 1 µs for a 40 dB change.
The differential gain control interface allows the use of either
differential or single-ended positive or negative control voltages.
Several of these amplifiers may be cascaded and their gain
control gains offset to optimize the system S/N ratio.
The AD603 can drive a load impedance as low as 100 Ω with
low distortion. For a 500 Ω load in shunt with 5 pF, the total
harmonic distortion for a ±1 V sinusoidal output at 10 MHz is
typically −60 dBc. The peak specified output is ±2.5 V
minimum into a 500 Ω load.
The AD603 uses a patented proprietary circuit topology—the
X-AMP®. The X-AMP comprises a variable attenuator of 0 dB
to −42.14 dB followed by a fixed-gain amplifier. Because of the
attenuator, the amplifier never has to cope with large inputs and
can use negative feedback to define its (fixed) gain and dynamic
performance. The attenuator has an input resistance of 100 Ω,
laser trimmed to ±3%, and comprises a seven-stage R-2R ladder
network, resulting in an attenuation between tap points of
6.021 dB. A proprietary interpolation technique provides a
continuous gain control function which is linear in dB.
The AD603 is specified for operation from −40°C to +85°C.
8
VPOS
6
VNEG
1
GPOS
2
GNEG
3
VINP
4
COMM
Rev. G
Information furnished by Analog Devices is believed to be accurate and reliable.
However, no responsibility is assumed by Analog Devices for its use, nor for any
infringements of patents or other rights of third parties that may result from its use.
Specifications subject to change without notice. No license is granted by implication
or otherwise under any patent or patent rights of Analog Devices. Trademarks and
registered trademarks are the property of their respective owners.
@ TA = 25°C, VS = ±5 V, –500 mV ≤ VG ≤ +500 mV, GNEG = 0 V, –10 dB to +30 dB gain range, RL = 500 Ω, and CL = 5 pF, unless otherwise
noted.
Table 1.
Parameter ConditionsMin Typ MaxUnit
INPUT CHARACTERISTICS
Input Resistance Pin 3 to Pin 4 97 100 103 Ω
Input Capacitance 2 pF
Input Noise Spectral Density
Noise Figure f = 10 MHz, gain = max, RS = 10 Ω 8.8 dB
1 dB Compression Point f = 10 MHz, gain = max, RS = 10 Ω −11 dBm
Peak Input Voltage ±1.4 ±2 V
OUTPUT CHARACTERISTICS
−3 dB Bandwidth V
Slew Rate RL ≥ 500 Ω 275 V/µs
Peak Output
2
Output Impedance f ≤ 10 MHz 2 Ω
Output Short-Circuit Current 50 mA
Group Delay Change vs. Gain f = 3 MHz; full gain range ±2 ns
Group Delay Change vs. Frequency VG = 0 V; f = 1 MHz to 10 MHz ±2 ns
Differential Gain 0.2 %
Differential Phase 0.2 Degree
Total Harmonic Distortion f = 10 MHz, V
Third Order Intercept f = 40 MHz, gain = max, RS = 50 Ω 15 dBm
ACCURACY
Gain Accuracy, f = 100 kHz; Gain (dB) = (40 VG + 10) dB −500 mV ≤ VG ≤ +500 mV, −1 ±0.5 +1 dB
T
to T
MIN
MAX
Gain, f = 10.7 MHz VG = -0.5 V −10.3 −9.0 −8.0 dB
V
V
Output Offset Voltage
T
to T
MIN
MAX
Output Offset Variation vs. V
T
to T
MIN
MAX
GAIN CONTROL INTERFACE
Gain Scaling Factor 100 kHz 39.4 40 40.6 dB/V
T
to T
MIN
MAX
10.7 MHz 38.7 39.3 39.9 dB/V
GNEG, GPOS Voltage Range
Input Bias Current 200 nA
Input Offset Current 10 nA
Differential Input Resistance Pin 1 to Pin 2 50 MΩ
Response Rate Full 40 dB gain change 80 dB/µs
POWER SUPPLY
Specified Operating Range ±4.75 ±6.3 V
Quiescent Current 12.5 17 mA
T
to T
MIN
1
Typical open or short-circuited input; noise is lower when system is set to maximum gain and input is short-circuited. This figure includes the effects of both voltage
and current noise sources.
2
Using resistive loads of 500 Ω or greater, or with the addition of a 1 kΩ pull-down resistor when driving lower loads.
3
The dc gain of the main amplifier in the AD603 is ×35.7; thus, an input offset of 100 µV becomes a 3.57 mV output offset.
4
GNEG and GPOS, gain control, and voltage range are guaranteed to be within the range of −VS + 4.2 V to +VS − 3.4 V over the full temperature range of −40°C to +85°C.
MAX
1
Input short-circuited 1.3 nV/√Hz
= 100 mV rms 90 MHz
OUT
RL ≥ 500 Ω ±2.5 ±3.0 V
= 1 V rms −60 dBc
OUT
−1.5 +1.5 dB
= 0.0 V +9.5 +10.5 +11.5 dB
G
= 0.5 V +29.3 +30.3 +31.3 dB
3
G
VG = 0 V −20 +20 mV
−30 +30 mV
G
−500 mV ≤ VG ≤ +500 mV −20 +20 mV
−30 +30 mV
38 42 dB/V
4
−1.2 +2.0 V
20 mA
Rev. G | Page 3 of 20
AD603
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Rating
Supply Voltage ±V
S
±7.5 V
Internal Voltage VINP (Pin 3) ±2 V Continuous
±VS for 10 ms
GPOS, GNEG (Pins 1, 2) ±V
Internal Power Dissipation
1
S
400 mW
Operating Temperature Range
AD603A −40°C to +85°C
AD603S −55°C to +125°C
Storage Temperature Range −65°C to +150°C
Lead Temperature Range (Soldering 60 sec) 300°C
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
ESD CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on
the human body and test equipment and can discharge without detection. Although this product features
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy
electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance degradation or loss of functionality.
Rev. G | Page 4 of 20
AD603
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
GPOS
GNEG
VINP
COMM
1
AD603
2
3
TOP VIEW
(Not to Scale)
4
8
7
6
5
VPOS
VOUT
VNEG
FDBK
00539-002
Figure 2. 8-Lead Plastic SOIC (R) Package
1
GPOS
GNEG
VINP
COMM
AD603
2
TOP VIEW
3
(Not to Scale)
4
Figure 3. 8-Lead Ceramic CERDIP (Q) Package
8
7
6
5
VPOS
VOUT
VNEG
FDBK
00539-003
Table 3. Pin Function Descriptions
Pin No. Mnemonic Description
1 GPOS Gain Control Input High (Positive Voltage Increases Gain).
2 GNEG Gain Control Input Low (Negative Voltage Increases Gain).
3 VINP Amplifier Input.
4 COMM Amplifier Ground.
5 FDBK Connection to Feedback Network.
6 VNEG Negative Supply Input.
7 VOUT Amplifier Output.
8 VPOS Positive Supply Input.
Rev. G | Page 5 of 20
AD603
TYPICAL PERFORMANCE CHARACTERISTICS
@ TA = 25°C, VS = ±5 V, –500 mV ≤ VG ≤ +500 mV, GNEG = 0 V, –10 dB to +30 dB gain range, RL = 500 Ω, and CL = 5 pF, unless otherwise
noted.
40
30
20
10
GAIN (dB)
0
–10
10.7MHz
Figure 4. Gain vs. V
100kHz
VG (V)
at 100 kHz and 10.7 mHz
G
2.5
2.0
1.5
1.0
0.5
0
GAIN ERROR (dB)
–0.5
–1.0
–1.5
45MHz
70MHz
10.7MHz
455kHz
70MHz
GAIN VOLTAGE (Volts)
Figure 5. Gain Error vs. Gain Control Voltage at 455 kHz,
10.7 MHz, 45 MHz, 70 MHz
4
3
2
1
0
–1
–2
GAIN (dB)
–3
–4
–5
–6
100k1M10M100M
GAIN
PHASE
FREQUENCY (Hz)
Figure 6. Frequency and Phase Response vs. Gain
(Gain = −10 dB, P
= −30 dBm)
IN
0.6–0.6–0.4–0.200.20.4
0.5–0.5 –0.4 –0.3 –0.2 –0.100.10.2 0.3 0.4
225
180
135
90
45
0
–45
–90
–135
–180
–225
00539-004
00539-005
PHASE (Degrees)
00539-006
4
3
2
1
0
–1
–2
GAIN (dB)
–3
–4
–5
–6
100k1M10M100M
GAIN
PHASE
FREQUENCY (Hz)
Figure 7. Frequency and Phase Response vs. Gain
(Gain = +10 dB, P
4
3
2
1
GAIN
0
–1
PHASE
–2
GAIN (dB)
–3
–4
–5
–6
100k1M10M100M
FREQUENCY (Hz)
= −30 dBm)
IN
Figure 8. Frequency and Phase Response vs. Gain
(Gain = +30 dB, P
7.60
7.40
7.20
7.00
6.80
GROUP DELAY (ns)
6.60
6.40
GAIN CONTROL VOLTAGE (V)
= −30 dBm)
IN
Figure 9. Group Delay vs. Gain Control Voltage
225
180
135
90
45
0
–45
–90
–135
–180
–225
225
180
135
90
45
0
–45
–90
–135
–180
–225
0.6–0.6–0.4–0.200.20.4
PHASE (Degrees)
PHASE (Degrees)
00539-009
00539-007
00539-008
Rev. G | Page 6 of 20
AD603
0.1µF
+5V
HP3326A
DUAL-
CHANNEL
SYNTHESIZER
100Ω
0.1µF
8
3
AD603
4
6
–5V
1
DATEL
DVC 8500
5
2
10×
7
PROBE
511Ω
Figure 10. Third Order Intermodulation Distortion Test Setup
Figure 13. Typical Output Voltage Swing vs. Load Resistance
(Negative Output Swing Limits First)
00539-013
10dB/DIV
Figure 11. Third Order Intermodulation Distor tion at 455 kHz
(10× Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, P
10dB/DIV
00539-011
= 0 dBm)
IN
102
100
98
96
INPUT IMPEDANCE (Ω)
94
FREQUENCY (Hz)
Figure 14. Input Impedance vs. Frequency (Gain = −10 dB)
102
100
98
96
INPUT IMPEDANCE (Ω)
100M100k1M10M
00539-014
Figure 12. Third Order Intermodulation Distortion at 10.7 MHz
(10× Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, P
00539-012
= 0 dBm)
IN
Rev. G | Page 7 of 20
94
FREQUENCY (Hz)
Figure 15. Input Impedance vs. Frequency (Gain = +10 dB)
100M100k1M10M
00539-015
AD603
102
3V
100
98
96
INPUT IMPEDANCE (Ω)
94
FREQUENCY (Hz)
Figure 16. Input Impedance vs. Frequency (Gain = +30 dB)
1V
100
90
10
0%
INPUT GND
100MV/DIV
1V
OUTPUT GND
1V/DIV
100M100k1M10M
00539-016
–2V
451ns–49ns50ns
00539-019
Figure 19. Output Stage Overload Recovery Time
(Input Is 500 ns Period, 50% Duty Cycle Square Wave, Output is Captured
Using Tektronix 11402 Digitizing Oscilloscope)
3.5V
INPUT
500mV/DIV
GND
500mV
OUTPUT
500mV/DIV
GND
1V
200ns
00539-017
Figure 17. Gain Control Channel Response Time
4.5V
INPUT GND
1V/DIV
500mV
OUTPUT GND
500mV/DIV
–500mV
451ns–49ns50ns
Figure 18. Input Stage Overload Recovery Time
(Input is 500 ns Period, 50% Duty Cycle Square Wave, Output is Captured
Using Tektronix 11402 Digitizing Oscilloscope)
00539-018
–1.5V
456ns–44ns50ns
Figure 20. Transient Response, G = 0 dB
(Input is 500 ns Period, 50% Duty Cycle Square Wave, Output is Captured
Using Tektronix 11402 Digitizing Oscilloscope)
3.5V
INPUT GND
100mV/DIV
500mV
OUTPUT GND
500mV/DIV
–1.5V
456ns–44ns50ns
00539-021
Figure 21. Transient Response, G = +20 dB
(Input is 500 ns Period, 50% Duty Cycle Square Wave, Output is Captured
Using Tektronix 11402 Digitizing Oscilloscope)
00539-020
Rev. G | Page 8 of 20
AD603
–10
–20
–30
–40
–50
PSRR (dB)
–60
21
0
NOISE FIGURE (dB)
19
17
15
13
11
9
7
10MHz
20MHz
TA = 25°C
= 50
Ω
R
S
TEST SETUP FIGURE 23
FREQUENCY (Hz)
100M100k1M10M
Figure 22. PSRR v s. Frequency
(Worst Case is Negative Supply PSRR, Shown Here)
µ
F
0.1
+5V
HP3326A
DUAL-
CHANNEL
SYNTHESIZER
100
0.1
8
3
AD603
Ω
4
µ
F
–5V
6
DATEL
DVC 8500
5
7
2
1
HP3585A
Ω
50
SPECTRUM
ANALYZER
Figure 23. Test Setup Used for: Noise Figure, Third Order Intercept and
1 dB Compression Point Measurements
NOISE FIGURE (dB)
23
21
19
17
15
13
11
9
7
5
70MHz
30MHz
GAIN (dB)
TA = 25°C
R
= 50V
S
TEST SETUP FIGURE 23
50MHz
10MHz
3020212223242526272829
Figure 24. Noise Figure in −10 dB/+30 dB Mode
00539-022
00539-023
00539-024
5
GAIN (dB)
4030313233343536373839
00539-025
Figure 25. Noise Figure in 0 dB/40 dB Mode
0
–5
–10
–15
INPUT LEVEL (dBm)
–20
–25
INPUT FREQUENCY (MHz)
TA = 25°C
TEST SETUP FIGURE 23
70103050
00539-026
Figure 26. 1 dB Compression Point, −10 dB/+30 dB Mode, Gain = +30 dB
20
18
16
14
12
OUTPUT LEVEL (dBm)
10
0
30MHz
40MHz
70MHz
INPUT LEVEL (dBm)
TA = 25°C
TEST SETUP FIGURE 23
0–20–10
00539-027
Figure 27. Third Order Intercept −10 dB/+30 dB Mode, Gain = +10 dB
Rev. G | Page 9 of 20
AD603
20
18
16
14
12
OUTPUT LEVEL (dBm)
10
40MHz
70MHz
30MHz
TA = 25°C
= 50
Ω
R
S
RIN = 50
Ω
RL = 100
Ω
TEST SETUP FIGURE 23
8
INPUT LEVEL (dBm)
Figure 28. Third Order Intercept −10 dB/+30 dB Mode, Gain = +30 dB
–20–40–30
00539-028
Rev. G | Page 10 of 20
AD603
THEORY OF OPERATION
The AD603 comprises a fixed-gain amplifier, preceded by a
broadband passive attenuator of 0 dB to 42.14 dB, having a gain
control scaling factor of 40 dB per volt. The fixed gain is lasertrimmed in two ranges, to either 31.07 dB (×35.8) or 50 dB
(×358), or may be set to any range in between using one
external resistor between Pin 5 and Pin 7. Somewhat higher
gain can be obtained by connecting the resistor from Pin 5 to
common, but the increase in output offset voltage limits the
maximum gain to about 60 dB. For any given range, the
bandwidth is independent of the voltage-controlled gain. This
system provides an underrange and overrange of 1.07 dB in all
cases; for example, the overall gain is −11.07 dB to +31.07 dB in
the maximum bandwidth mode (Pin 5 and Pin 7 strapped).
This X-AMP structure has many advantages over former
methods of gain control based on nonlinear elements. Most
importantly, the fixed-gain amplifier can use negative feedback
to increase its accuracy. Since large inputs are first attenuated,
the amplifier input is always small. For example, to deliver a
±1 V output in the −1 dB/+41 dB mode (that is, using a fixed
amplifier gain of 41.07 dB) its input is only 8.84 mV; thus the
distortion can be very low. Equally important, the small-signal
gain and phase response, and thus the pulse response, are
essentially independent of gain.
Figure 29 is a simplified schematic. The input attenuator is a
seven-section R-2R ladder network, using untrimmed resistors
of nominally R = 62.5 Ω, which results in a characteristic
resistance of 125 Ω ±20%. A shunt resistor is included at the
input and laser trimmed to establish a more exact input
resistance of 100 Ω ±3%, which ensures accurate operation
(gain and HP corner frequency) when used in conjunction with
external resistors or capacitors.
The nominal maximum signal at input VINP is 1 V rms (±1.4 V
peak) when using the recommended ±5 V supplies, although
operation to ±2 V peak is permissible with some increase in HF
distortion and feedthrough. Pin 4 (COMM) must be connected
directly to the input ground; significant impedance in this
connection will reduce the gain accuracy.
The signal applied at the input of the ladder network is
attenuated by 6.02 dB by each section; thus, the attenuation to
each of the taps is progressively 0 dB, 6.02 dB, 12.04 dB,
18.06 dB, 24.08 dB, 30.1 dB, 36.12 dB, and 42.14 dB. A unique
circuit technique is employed to interpolate between these tap
points, indicated by the slider in Figure 29, thus providing
continuous attenuation from 0 dB to 42.14 dB. It will help in
understanding the AD603 to think in terms of a mechanical
means for moving this slider from left to right; in fact, its
position is controlled by the voltage between Pin 1 and Pin 2.
The details of the gain control interface are discussed later.
The gain is at all times very exactly determined, and a linear-indB relationship is automatically guaranteed by the exponential
nature of the attenuation in the ladder network (the X-AMP
principle). In practice, the gain deviates slightly from the ideal
law, by about ±0.2 dB peak (see, for example, Figure 5).
NOISE PERFORMANCE
An important advantage of the X-AMP is its superior noise
performance. The nominal resistance seen at inner tap points is
41.7 Ω (one third of 125 Ω), which exhibits a Johnson noise
spectral density (NSD) of 0.83 nV/√Hz (that is, √4kTR) at 27°C,
which is a large fraction of the total input noise. The first stage
of the amplifier contributes a further 1 nV/√Hz, for a total input
noise of 1.3 nV/√Hz. It will be apparent that it is essential to use
a low resistance in the ladder network to achieve the very low
specified noise level. The signal’s source impedance forms a
voltage divider with the AD603’s 100 Ω input resistance. In
some applications, the resulting attenuation may be
unacceptable, requiring the use of an external buffer or
preamplifier to match a high impedance source to the low
impedance AD603.
The noise at maximum gain (that is, at the 0 dB tap) depends on
whether the input is short-circuited or open-circuited: when
shorted, the minimum NSD of slightly over 1 nV/√Hz is
achieved; when open, the resistance of 100 Ω looking into the
first tap generates 1.29 nV/√Hz, so the noise increases to a total
of 1.63 nV/√Hz. (This last calculation would be important if the
AD603 were preceded by, for example, a 900 Ω resistor to allow
operation from inputs up to 10 V rms.) As the selected tap
moves away from the input, the dependence of the noise on
source impedance quickly diminishes.
Apart from the small variations just discussed, the signal-tonoise (S/N) ratio at the output is essentially independent of the
attenuator setting. For example, on the −11 dB/+31 dB range,
the fixed gain of ×35.8 raises the output NSD to 46.5 nV/√Hz.
Thus, for the maximum undistorted output of 1 V rms and a
1 MHz bandwidth, the output S/N ratio would be 86.6 dB, that
is, 20 log (1 V/46.5 µV).
The attenuation is controlled through a differential, high
impedance (50 MΩ) input, with a scaling factor which is lasertrimmed to 40 dB per volt, that is, 25 mV/dB. An internal band
gap reference ensures stability of the scaling with respect to
supply and temperature variations.
When the differential input voltage V
slider is centered, providing an attenuation of 21.07 dB. For the
maximum bandwidth range, this results in an overall gain of
10 dB (= −21.07 dB + 31.07 dB). When the control input is
−500 mV, the gain is lowered by 20 dB (= 0.500 V × 40 dB/V) to
−10 dB; when set to +500 mV, the gain is increased by 20 dB to
30 dB. When this interface is overdriven in either direction, the
gain approaches either −11.07 dB (= − 42.14 dB + 31.07 dB) or
31.07 dB (= 0 + 31.07 dB), respectively. The only constraint on
the gain control voltage is that it be kept within the commonmode range (−1.2 V to +2.0 V assuming +5 V supplies) of the
gain control interface.
The basic gain of the AD603 can thus be calculated using the
following simple expression:
Gain (dB) = 40 V
where V
is in volts. When Pin 5 and Pin 7 are strapped (see
G
+10 (1)
G
next section), the gain becomes
Gain (dB) = 40 V
+ 20 for 0 to +40 dB
G
= 0 V, the attenuator
G
For example, if the gain is to be controlled by a DAC providing
a positive only ground-referenced output, the Gain Control Low
(GNEG) pin should be biased to a fixed offset of 500 mV to set
the gain to −10 dB when Gain Control High (GPOS) is at zero,
and to 30 dB when at 1.00 V.
It is a simple matter to include a voltage divider to achieve other
scaling factors. When using an 8-bit DAC having an FS output
of 2.55 V (10 mV/bit), a divider ratio of 2 (generating 5 mV/bit)
would result in a gain-setting resolution of 0.2 dB/bit. The use
of such offsets is valuable when two AD603s are cascaded, when
various options exist for optimizing the S/N profile, as will be
shown later.
PROGRAMMING THE FIXED-GAIN AMPLIFIER
USING PIN STRAPPING
Access to the feedback network is provided at Pin 5 (FDBK).
The user may program the gain of the AD603’s output amplifier
using this pin, as shown in Figure 30, Figure 31, and Figure 32.
There are three modes: in the default mode, FDBK is
unconnected, providing the range +9 dB/+51 dB; when V
and FDBK are shorted, the gain is lowered to −11 dB/+31 dB;
and when an external resistor is placed between V
OUT
any intermediate gain can be achieved, for example, −1 dB/+41
dB. Figure 33 shows the nominal maximum gain vs. external
resistor for this mode.
OUT
and FDBK
and
VC1
1
GPOS
VPOS
8
VPOS
AD603
Gain (dB) = 40 V
The high impedance gain control input ensures minimal
+ 30 for +10 to +50 dB (2)
G
VIN
VC2
2
3
GNEG
VINP
VOUT
VNEG
7
6
VNEG
VOUT
loading when driving many amplifiers in multiple channel or
4
cascaded applications. The differential capability provides
COMM
flexibility in choosing the appropriate signal levels and
polarities for various control schemes.
Rev. G | Page 12 of 20
Figure 30. −10 dB to +30 dB; 90 MHz Bandwidth
FDBK
5
00539-030
AD603
V
Optionally, when a resistor is placed from FDBK to COMM,
higher gains can be achieved. This fourth mode is of limited
value because of the low bandwidth and the elevated output
offsets; it is thus not included in Figure 30, Figure 31, or
Figure 32.
The gain of this amplifier in the first two modes is set by the
ratio of on-chip laser-trimmed resistors. While the ratio of these
resistors is very accurate, the absolute value of these resistors
can vary by as much as ±20%. Thus, when an external resistor is
connected in parallel with the nominal 6.44 kΩ ±20% internal
resistor, the overall gain accuracy is somewhat poorer. The
worst-case error occurs at about 2 kΩ (see Figure 34).
1.2
1.0
0.8
0.6
0.4
0.2
0
DECIBELS
–0.2
–0.4
–0.6
–0.8
–1.0
Figure 34. Worst-Case Gain Error, Assuming Internal Resistors have a
Maximum Tolerance of −20% (Top Curve) or =20% (Bottom Curve)
–1:VdB (OUT) – (–1):VdB (O
VdB (OUT) – VdB (O
R
(Ω)
EXT
REF
REF
)
)
1M101001k10k100k
00539-034
While the gain bandwidth product of the fixed-gain amplifier is
about 4 GHz, the actual bandwidth is not exactly related to the
maximum gain. This is because there is a slight enhancing of
the ac response magnitude on the maximum bandwidth range,
due to higher order poles in the open-loop gain function; this
mild peaking is not present on the higher gain ranges. Figure 30,
Figure 31, and Figure 32 show how an optional capacitor may
be added to extend the frequency response in high gain modes.
IN
VIN
52
50
48
46
44
42
40
DECIBELS
38
36
34
32
30
Figure 33. Gain vs. R
VC1
1
GPOS
VPOS
8
VPOS
AD603
VC2
2
3
4
GNEG
VINP
COMM
VOUT
VNEG
FDBK
7
6
VNEG
2.15kΩ
5
5.6pF
Figure 31. 0 dB to 40 dB; 30 MHz Bandwidth
VC1
1
GPOS
VPOS
8
VPOS
AD603
VC2
2
3
4
GNEG
VINP
COMM
VOUT
VNEG
FDBK
7
6
VNEG
5
18pF
Figure 32. 10 dB to 50 db; 9 MHz to Set Gain
–1:VdB (OUT)
VdB (OUT)
–2:VdB (OUT)
R
(Ω)
EXT
Showing Worst-Case Limits Assuming Internal
EXT,
Resistors have a Maximum Tolerance of 20%
VOUT
VOUT
00539-031
00539-032
1M101001k10k100k
00539-033
Rev. G | Page 13 of 20
AD603
USING THE AD603 IN CASCADE
Two or more AD603s can be connected in series to achieve
higher gain. Invariably, ac coupling must be used to prevent the
dc offset voltage at the output of each amplifier from
overloading the following amplifier at maximum gain. The
required high-pass coupling network will usually be just a
capacitor, chosen to set the desired corner frequency in
conjunction with the well-defined 100 Ω input resistance of the
following amplifier.
For two AD603s, the total gain control range becomes 84 dB
(2 × 42.14 dB); the overall −3 dB bandwidth of cascaded stages
will be somewhat reduced. Depending on the pin strapping, the
gain and bandwidth for two cascaded amplifiers can range from
−22 dB to +62 dB (with a bandwidth of about 70 MHz) to
+22 dB to +102 dB (with a bandwidth of about 6 MHz).
There are several ways of connecting the gain control inputs in
cascaded operation. The choice depends on whether it is
important to achieve the highest possible instantaneous signalto-noise ratio (ISNR), or, alternatively, to minimize the ripple in
the gain error. The following examples feature the AD603
programmed for maximum bandwidth; the explanations apply
to other gain/bandwidth combinations with appropriate
changes to the arrangements for setting the maximum gain.
SEQUENTIAL MODE (OPTIMAL S/N RATIO)
In the sequential mode of operation, the ISNR is maintained at
its highest level for as much of the gain control range as
possible. Figure 35 shows the SNR over a gain range of −22 dB
to +62 dB, assuming an output of 1 V rms and a 1 MHz
bandwidth; Figure 36, Figure 37, and Figure 38 show the general
connections to accomplish this. Here, both the positive gain
control inputs (GPOS) are driven in parallel by a positive-only,
ground-referenced source with a range of 0 V to +2 V, while the
negative gain control inputs (GNEG) are biased by stable
voltages to provide the needed gain offsets. These voltages may
A1
–40.00dB–51.07dB
be provided by resistive dividers operating from a common
voltage reference.
90
85
80
75
70
65
S/N RATIO (dB)
60
55
50
VC (V)
2.2–0.20.60.21.41.01.8
00539-035
Figure 35. SNR vs. Control Voltage–Sequential Control (1 MHz Bandwidth)
The gains are offset (Figure 39) such that A2’s gain is increased
only after A1’s gain has reached its maximum value. Note that
for a differential input of –600 mV or less, the gain of a single
amplifier (A1 or A2) will be at its minimum value of −11.07 dB;
for a differential input of +600 mV or more, the gain will be at
its maximum value of 31.07 dB. Control inputs beyond these
limits will not affect the gain and can be tolerated without
damage or foldover in the response. This is an important aspect
of the AD603’s gain control response. (See the Specifications
section for more details on the allowable voltage range.) The
gain is now
Gain (dB) = 40 V
where V
is the applied control voltage and GO is determined by
G
+ GO (3)
G
the gain range chosen. In the explanatory notes that follow, it is
assumed the maximum bandwidth connections are used, for
which G
is −20 dB.
O
A2
INPUT
0dB
V
C
= 0V
–42.14dB
GPOSGNEG
V
G1
VO1 = 0.473VVO2 = 1.526V
31.07dB
–8.93dB
–42.14dB
GPOSGNEG
V
G2
31.07dB
Figure 36. AD603 Gain Control Input Calculations for Sequential Control Operation V
0dB–11.07dB
INPUT
0dB
V
= 1.0V
C
0dB
GPOSGNEG
V
G1
VO1 = 0.473VVO2 = 1.526V
31.07dB
31.07dB
–42.14dB
GPOSGNEG
V
G2
31.07dB
Figure 37. AD603 Gain Control Calculations for Sequential Control Operation V
Rev. G | Page 14 of 20
OUTPUT
–20dB
C
OUTPUT
20dB
= 1.0 V
C
00539-036
= 0 V
00539-037
AD603
0dB–28.93dB
INPUT
0dB
= 2.0V
V
C
0dB
GPOSGNEG
V
G1
VO1 = 0.473VVO2 = 1.526V
31.07dB
Figure 38. AD603 Gain Control Input Calculations for Sequential Operation V
+31.07dB
+10dB
A1A2
–8.93dB
0.4731.526
GAIN
(dB)
0
–20
1
GAIN OFFSET OF 1.07dB, OR 26.75mV.
–11.07dB
0.5
0
1
+31.07dB+28.96dB
1
1.0
20
1.50
40
2.060VC(V)
–11.07dB
62.14–22.14
Figure 39. Explanation of Offset Calibration for Sequential Control
With reference to Figure 36, Figure 37, and Figure 38, note that
V
refers to the differential gain control input to A1, and VG2
G1
refers to the differential gain control input to A2. When V
V
= −473 mV and thus the gain of A1 is −8.93 dB (recall that
G1
is 0,
G
the gain of each individual amplifier in the maximum
bandwidth mode is –10 dB for V
= 0 V); meanwhile, V
= −1.908 V so the gain of A2 is pinned at
G2
= −500 mV and 10 dB for VG
G
−11.07 dB. The overall gain is thus –20 dB. See Figure 36.
When V
= +1.00 V, VG1 = 1.00 V − 0.473 V = +0.526 V, which
G
sets the gain of A1 to at nearly its maximum value of 31.07 dB,
while V
= 1.00 V − 1.526 V = 0.526 V, which sets A2’s gain at
G2
nearly its minimum value of −11.07 dB. Close analysis shows
that the degree to which neither AD603 is completely pushed to
its maximum nor minimum gain exactly cancels in the overall
gain, which is now +20 dB. See Figure 37.
When V
= 2.0 V, the gain of A1 is pinned at 31.07 dB and that
G
of A2 is near its maximum value of 28.93 dB, resulting in an
overall gain of 60 dB (see Figure 38). This mode of operation is
further clarified by Figure 40, which is a plot of the separate
gains of A1 and A2 and the overall gain vs. the control voltage.
Figure 41 is a plot of the SNR of the cascaded amplifiers vs. the
control voltage. Figure 42 is a plot of the gain error of the
cascaded stages vs. the control voltages.
31.07dB
00539-039
–2.14dB
GPOSGNEG
V
G2
31.07dB
OUTPUT
60dB
00539-038
= 2.0 V
C
70
OVERALL GAIN (dB)
–10
–20
–30
60
50
40
30
20
10
0
A1
COMBINED
V
C
A2
Figure 40. Plot of Separate and Overall Gains in Sequential Control
90
80
70
60
50
40
S/N RATIO (dB)
30
20
10
V
C
Figure 41. SNR for Cascaded Stages—Sequential Control
2.0–0.20.20.61.01.41.8
00539-040
2.0–0.20.20.61.01.41.8
00539-041
Rev. G | Page 15 of 20
AD603
2.0
90
1.5
1.0
0.5
0
–0.5
GAIN ERROR (dB)
–1.0
–1.5
–2.0
V
C
2.2–0.2 0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0
Figure 42. Gain Error for Cascaded Stages–Sequential Control
PARALLEL MODE (SIMPLEST GAIN CONTROL
INTERFACE)
In this mode, the gain control of voltage is applied to both
inputs in parallel—the GPOS pins of both A1 and A2 are
connected to the control voltage and the GNEW inputs are
grounded. The gain scaling is then doubled to 80 dB/V,
requiring only a 1.00 V change for an 80 dB change of gain:
Gain = (dB) = 80 V
where, as before, G
in the maximum bandwidth mode, G
the GNEG pins may be connected to an offset voltage of
0.500 V, in which case G
The amplitude of the gain ripple in this case is also doubled, as
shown in Figure 43, while the instantaneous signal-to-noise
ratio at the output of A2 now decreases linearly as the gain
increases, as shown in Figure 44.
2.0
1.5
1.0
0.5
0
–0.5
GAIN ERROR (dB)
–1.0
+ GO (4)
G
depends on the range selected; for example,
O
is +20 dB. Alternatively,
O
is −20 dB.
O
00539-042
85
80
75
70
65
IS/N RATIO (dB)
60
55
50
V
C
1.2–0.200.20.40.60.81.0
00539-044
Figure 44. ISNR for Cascaded Stages—Parallel Control
LOW GAIN RIPPLE MODE (MINIMUM GAIN ERROR)
As can be seen in Figure 42 and Figure 43, the error in the gain
is periodic, that is, it shows a small ripple. (Note that there is
also a variation in the output offset voltage, which is due to the
gain interpolation, but this is not exact in amplitude.) By
offsetting the gains of A1 and A2 by half the period of the
ripple, that is, by 3 dB, the residual gain errors of the two
amplifiers can be made to cancel. Figure 45 shows much lower
gain ripple when configured in this manner. Figure 46 plots the
ISNR as a function of gain; it is very similar to that in the
parallel mode.
3.0
2.5
2.0
1.5
1.0
0.5
0
–0.5
–1.0
GAIN ERROR (dB)
–1.5
–2.0
–2.5
–3.0
V
C
Figure 45. Gain Error for Cascaded Stages—Low Ripple Mode
1.1–0.1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
00539-045
–1.5
–2.0
V
C
Figure 43. Gain Error for Cascaded Stages—Parallel Control
2.2–0.2 0 0.2 0.4 0.61.0 1.20.81.6 1.8 2.01.4
00539-043
Rev. G | Page 16 of 20
AD603
90
85
80
75
70
65
IS/N RATIO (dB)
60
55
50
V
C
1.2–0.200.20.40.60.81.0
00539-046
Figure 46. ISNR vs. Control Voltage—Low Ripple Mode
Rev. G | Page 17 of 20
AD603
APPLICATIONS
A LOW NOISE AGC AMPLIFIER
Figure 47 shows the ease with which the AD603 can be
connected as an AGC amplifier. The circuit illustrates many of
the points previously discussed: It uses few parts, has linear-indB gain, operates from a single supply, uses two cascaded
amplifiers in sequential gain mode for maximum S/N ratio, and
an external resistor programs each amplifier’s gain. It also uses a
simple temperature-compensated detector.
The circuit operates from a single 10 V supply. Resistors R1, R2,
R3, and R4 bias the common pins of A1 and A2 at 5 V. This pin
is a low impedance point and must have a low impedance path
to ground, provided here by the 100 µF tantalum capacitors and
the 0.1 µF ceramic capacitors.
The cascaded amplifiers operate in sequential gain. Here, the
offset voltage between the Pin 2 (GNEG) of A1 and A2 is 1.05 V
(42.14 dB × 25 mV/dB), provided by a voltage divider
consisting of resistors R5, R6, and R7. Using standard values, the
offset is not exact, but it is not critical for this application.
The gain of both A1 and A2 is programmed by resistors R13
and R14, respectively, to be about 42 dB; thus the maximum
gain of the circuit is twice that, or 84 dB. The gain control range
can be shifted up by as much as 20 dB by appropriate choices of
R13 and R14.
The circuit operates as follows. A1 and A2 are cascaded.
Capacitor C1 and the 100 Ω of resistance at the input of A1
form a time constant of 10 µs. C2 blocks the small dc offset
voltage at the output of A1 (which might otherwise saturate A2
at its maximum gain) and introduces a high-pass corner at
about 16 kHz, eliminating low frequency noise.
A half-wave detector is used, based on Q1 and R8. The current
into capacitor C
is just the difference between the collector
AV
current of Q2 (biased to be 300 µA at 300 K, 27°C) and the
collector current of Q1, which increases with the amplitude of
the output signal.
The automatic gain control voltage, V
this error current. In order for V
AGC
, is the time integral of
AGC
(and thus the gain) to
remain insensitive to short-term amplitude fluctuations in the
output signal, the rectified current in Q1 must, on average,
exactly balance the current in Q2. If the output of A2 is too
small to do this, V
will increase, causing the gain to increase,
AGC
until Q1 conducts sufficiently.
Consider the case where R8 is zero and the output voltage V
OUT
is a square wave at, say, 455 kHz, which is well above the corner
frequency of the control loop.
10V
C7
0.1µF
C1
0.1µF
10V
R2
2.49kΩ
5.49kΩ
3
4
J1
2
C3
100µFC40.1µF
1
RT
100Ω
R1
2.49kΩ
+
1
RT PR OVIDES A 5 0Ω INPUT IMPEDANCE.
2
C3 AND C5 ARE TANTALUM.
10V
R13
8
A1
AD603
1
R5
2.49kΩ
6
5
7
2
C5
100µFC60.1µF
5.5V6.5V
C2
0.1µF
2
+
1V OFFSET FOR
SEQUENTIAL GAIN
2.49kΩ
R6
1.05kΩ
R3
C8
0.1µF
10V
Figure 47. A Low Noise AGC Amplifier
R4
2.49kΩ
THIS CAPACITOR SETS
AGC TIME CONSTANT
10V
8
6
3
AD603
4
1
A2
5
2
R14
2.49kΩ
7
0.1µF
R7
3.48kΩ
V
AGC
C
AV
AGC LINE
10V
1.54kΩ
2N3906
2N3904
806Ω
Q2
Q1
R9
R8
R10
1.24kΩ
R11
3.83kΩ
5V
R12
4.99kΩ
C10
0.1µF
C11
0.1µF
C9
0.1µF
J2
00539-047
Rev. G | Page 18 of 20
AD603
During the time V
voltage of Q1, Q1 conducts; when V
Since the average collector current of Q1 is forced to be 300 µA,
and the square wave has a duty cycle of 1:1, Q1’s collector
current when conducting must be 600 µA. With R8 omitted, the
peak amplitude of V
600 µA, typically about 700 mV, or 2 V
voltage, the amplitude at which the output stabilizes, has a
strong negative temperature coefficient (TC), typically
−1.7 mV/°C. Although this may not be troublesome in some
applications, the correct value of R8 will render the output
stable with temperature.
To understand this, note that the current in Q2 is made to be
proportional to absolute temperature (PTAT). For the moment,
continue to assume that the signal is a square wave.
When Q1 is conducting, V
voltage that is PTAT and that can be chosen to have an equal
but opposite TC to that of the V
than an application of the band gap voltage reference principle.
When R8 is chosen such that the sum of the voltage across it
and the V
V
OUT
of Q1 is close to the band gap voltage of about 1.2 V,
BE
will be stable over a wide range of temperatures, provided,
of course, that Q1 and Q2 share the same thermal environment.
Since the average emitter current is 600 µA during each half
cycle of the square wave, a resistor of 833 Ω would add a PTAT
voltage of 500 mV at 300 K, increasing by 1.66 mV/°C. In
practice, the optimum value will depend on the type of
transistor used and, to a lesser extent, on the waveform for
which the temperature stability is to be optimized; for the
is negative with respect to the base
OUT
is positive, it is cut off.
OUT
is forced to be just the VBE of Q1 at
OUT
peak-to-peak. This
BE
is now the sum of VBE and a
OUT
. This is actually nothing more
BE
inexpensive 2N3904/2N3906 pair and sine wave signals, the
recommended value is 806 Ω.
This resistor also serves to lower the peak current in Q1 when
more typical signals (usually sinusoidal) are involved, and the
1.8 kHz LP filter it forms with C
due to ripple in V
. Note that the output amplitude under sine
AGC
helps to minimize distortion
AV
wave conditions will be higher than for a square wave, since the
average value of the current for an ideal rectifier would be 0.637
times as large, causing the output amplitude to be 1.88
(= 1.2/0.637) V, or 1.33 V rms. In practice, the somewhat
nonideal rectifier results in the sine wave output being regulated
to about 1.4 V rms, or 3.6 V p-p.
The bandwidth of the circuit exceeds 40 MHz. At 10.7 MHz, the
AGC threshold is 100 µV (−67 dBm) and its maximum gain is
83 dB (20 log 1.4 V/100 µV). The circuit holds its output at
1.4 V rms for inputs as low as −67 dBm to +15 dBm (82 dB),
where the input signal exceeds the AD603’s maximum input
rating. For a 30 dBm input at 10.7 MHz, the second harmonic is
34 dB down from the fundamental and the third harmonic is
35 dB down.
CAUTION
Careful component selection, circuit layout, power supply
decoupling, and shielding are needed to minimize the AD603’s
susceptibility to interference from signals such as those from
radio and TV stations. In bench evaluation, it is recommended
to place all of the components into a shielded box and using
feedthrough decoupling networks for the supply voltage. Circuit
layout and construction are also critical, since stray capacitances
and lead inductances can form resonant circuits and are a
potential source of circuit peaking, oscillation, or both.
Rev. G | Page 19 of 20
AD603
OUTLINE DIMENSIONS
0.005 (0.13)
PIN 1
0.200 (5.08)
MAX
0.200 (5.08)
0.125 (3.18)
0.023 (0.58)
0.014 (0.36)
CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.
Part Number Temperature Range Package Description Package Option
AD603AR −40°C to +85°C 8-Lead SOIC R-8
AD603AR-REEL −40°C to +85°C 8-Lead SOIC, 13" Reel R-8
AD603AR-REEL7 −40°C to +85°C 8-Lead SOIC, 7" Reel R-8
AD603ARZ
AD603ARZ-REEL
AD603ARZ-REEL7
AD603AQ −40°C to +85°C 8-Lead CERDIP Q-8
AD603SQ/883B
AD603-EB Evaluation Board
AD603ACHIPS DIE
1
Z = Pb-free part.
2
Refer to AD603 Military data sheet. Also available as 5962-9457203MPA.
1
0.055 (1.40)
8
1
MAX
5
4
0.070 (1.78)
0.030 (0.76)
MIN
0.100 (2.54) BSC
0.405 (10.29) MAX
0.310 (7.87)
0.220 (5.59)
0.060 (1.52)
0.015 (0.38)
0.150 (3.81)
MIN
SEATING
PLANE
(Q-8)
0.320 (8.13)
0.290 (7.37)
15°
0°
0.015 (0.38)
0.008 (0.20)
5.00 (0.1968)
4.80 (0.1890)
4.00 (0.1574)
3.80 (0.1497)
0.25 (0.0098)
0.10 (0.0040)
COPLANARITY
0.10
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN
85
1.27 (0.0500)
SEATING
PLANE
COMPLIANT TO JEDEC STANDARDS MS-012-AA
Figure 49. 8-Lead Standard Small Outline Package [SOIC-N]