Analog Devices AD603 Datasheet

Low Noise, 90 MHz
a
FEATURES “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, e.g., –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 MIL-STD-883 Compliant and DESC Versions Available
APPLICATIONS RF/IF AGC Amplifier Video Gain Control A/D Range Extension Signal Measurement
PRODUCT 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 impedance (50 M), low bias (200 nA) differential input;
the scaling is 25 mV/dB, requiring a gain-control voltage of only
Variable-Gain Amplifier
AD603*
1 V to span the central 40 dB of the gain range. An over- and under-range 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 with low distortion. For a 500 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 load, or ±1 V into a 100 load.
The AD603 uses a 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 AD603A is specified for operation from –40°C to +85°C
and is available in both 8-lead SOIC (R) and 8-lead ceramic
DIP (Q). The AD603S is specified for operation from –55°C to +125°C and is available in an 8-lead ceramic DIP (Q). The
AD603 is also available under DESC SMD 5962-94572.
FUNCTIONAL BLOCK DIAGRAM
VPOS VNEG
GPOS
GNEG
VINP
COMM
*Patented. X-AMP is a trademark of Analog Devices, Inc.
SCALING
REFERENCE
V
G
GAIN
CONTROL
INTERFACE
0dB –6.02dB –12.04dB–18.06dB –24.08dB –30.1dB –36.12dB –42.14dB
RRRRRRR
2R 2R 2R 2R 2R 2R R
R = 2R LADDER NETWORK
PRECISION PASSIVE INPUT ATTENUATOR
REV. C
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 which may result from its use. No license is granted by implication or otherwise under any patent or patent rights of Analog Devices.
FIXED GAIN
AMPLIFIER
V
OUT
AD603
*NORMAL VALUES
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A. Tel: 781/329-4700 World Wide Web Site: http://www.analog.com Fax: 781/326-8703 © Analog Devices, Inc., 2000
6.44kV*
FDBK
694V*
20V*
AD603–SPECIFICATIONS
(@ TA = +25C, V Range, RL = 500 , and CL = 5 pF, unless otherwise noted.)
= 5 V, –500 mV ≤ VG +500 mV, GNEG = 0 V, –10 dB to +30 dB Gain
S
Model AD603 Parameter Conditions Min Typ Max Unit
INPUT CHARACTERISTICS
Input Resistance Pins 3 to 4 97 100 103
Input Capacitance 2pF Input Noise Spectral Density Noise Figure f = 10 MHz, Gain = max, R 1 dB Compression Point f = 10 MHz, Gain = max, R
1
Input Short Circuited 1.3 nV/Hz
= 10 8.8 dB
S
= 10 –11 dBm
S
Peak Input Voltage ±1.4 ±2V
OUTPUT CHARACTERISTICS
–3 dB Bandwidth V Slew Rate R Peak Output
2
= 100 mV rms 90 MHz
OUT
500 275 V/µs
L
R
500 Ω±2.5 ±3.0 V
L
Output Impedance f 10 MHz 2
Output Short-Circuit Current 50 mA
Group Delay Change vs. Gain f = 3 MHz; Full Gain Range ±2ns
Group Delay Change vs. Frequency V
= 0 V; f = 1 MHz to 10 MHz ±2ns
G
Differential Gain 0.2 % Differential Phase 0.2 Degree Total Harmonic Distortion f = 10 MHz, V 3rd Order Intercept f = 40 MHz, Gain = max, R
= 1 V rms –60 dBc
OUT
= 50 15 dBm
S
ACCURACY
Gain Accuracy –500 mV ≤ V
T
to T
MIN
Output Offset Voltage
T
MIN
Output Offset Variation vs. V
T
MIN
to T
to T
MAX
MAX
MAX
3
G
VG = 0 V 20 mV
–500 mV ≤ VG +500 mV 20 mV
+500 mV ±0.5
G
1 dB
±1.5 dB
30 mV
30 mV
GAIN CONTROL INTERFACE
Gain Scaling Factor 39.4 40 40.6 dB/V
to T
T
MIN
GNEG, GPOS Voltage Range
MAX
4
38 42 dB/V
–1.2 +2.0 V Input Bias Current 200 nA Input Offset Current 10 nA
Differential Input Resistance Pins 1 to 2 50 M Response Rate Full 40 dB Gain Change 40 dB/µs
POWER SUPPLY
Specified Operating Range ±4.75 ±6.3 V
Quiescent Current 12.5 17 mA
T
to T
MIN
NOTES
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 or greater, or with the addition of a 1 k 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, voltage range is guaranteed to be within the range of – VS + 4.2 V to +V
Specifications shown in boldface are tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels. All min and max specifications are guaranteed, although only those shown in boldface are tested on all production units.
Specifications subject to change without notice.
MAX
– 3.4 V over the full temperature range of –40°C to +85°C.
S
20 mA
–2–
REV. C
AD603
WARNING!
ESD SENSITIVE DEVICE
ABSOLUTE MAXIMUM RATINGS
1
Supply Voltage ±VS . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±7.5 V
Internal Voltage VINP (Pin 3) . . . . . . . . . . . ±2 V Continuous
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±V
GPOS, GNEG (Pins 1, 2) . . . . . . . . . . . . . . . . . . . . . . . ±V
for 10 ms
S
S
Internal Power Dissipation2 . . . . . . . . . . . . . . . . . . . . 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
NOTES
1
Stresses above those listed under Absolute Maximum Ratings may cause perma-
nent 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.
2
Thermal Characteristics:
8-Lead SOIC Package: θJA = 155°C/W, θJC = 33°C/W 8-Lead Ceramic Package: θJA = 140°C/W, θJC = 15°C/W
ORDERING GUIDE
PIN FUNCTION DESCRIPTIONS
Pin Mnemonic Description
Pin 1 GPOS Gain-Control Input “HI”
(Positive Voltage Increases Gain)
Pin 2 GNEG Gain-Control Input “LO”
(Negative Voltage Increases Gain) Pin 3 VINP Amplifier Input Pin 4 COMM Amplifier Ground Pin 5 FDBK Connection to Feedback Network Pin 6 VNEG Negative Supply Input Pin 7 VOUT Amplifier Output Pin 8 VPOS Positive Supply Input
CONNECTION DIAGRAMS
8-Lead Plastic SOIC (R) Package
8-Lead Ceramic DIP (Q) Package
GPOS GNEG
VINP
1
2
AD603
TOP VIEW
3
(Not to Scale)
4
8
7
6
5
VPOS VOUT VNEG FDBKCOMM
Temperature Package Package
Part Number Range Description Option
AD603AR –40°C to +85°C 8-Lead SOIC SO-8 AD603AQ –40°C to +85°C 8-Lead Ceramic DIP Q-8 AD603SQ/883B* –55°C to +125°C 8-Lead Ceramic DIP Q-8
AD603-EB Evaluation Board
AD603ACHIPS –40°C to +85°C Die AD603AR-REEL –40°C to +85°C 13" Reel SO-8 AD603AR-REEL7 –40°C to +85°C 7" Reel SO-8
*Refer to AD603 Military data sheet. Also available as 5962-9457203MPA.
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 the AD603 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. C
–3–
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
laser-trimmed 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 Pins 5 and 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 under- 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 1 is a simplified schematic. The input attenuator is a seven-section R-2R ladder network, using untrimmed resistors
of nominally R = 62.5 , 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 (SIGNAL COMMON) 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 1, 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 Pins 1 and 2. The details of the gain­control 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 16).
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 (one third of 125 ), which exhibits a Johnson noise­spectral 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 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 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 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).
VPOS VNEG
GPOS
GNEG
VINP
COMM
SCALING
REFERENCE
V
G
GAIN
CONTROL
INTERFACE
0dB –6.02dB –12.04dB–18.06dB –24.08dB –30.1dB –36.12dB –42.14dB
RRRRRRR
2R 2R 2R 2R 2R 2R R
R = 2R LADDER NETWORK
PRECISION PASSIVE INPUT ATTENUATOR
AD603
Figure 1. Simplified Block Diagram of the AD603
–4–
FIXED GAIN
AMPLIFIER
6.44kV*
694V*
20V*
*NORMAL VALUES
V
OUT
FDBK
REV. C
AD603
The Gain-Control Interface
The attenuation is controlled through a differential, high-
impedance (50 M) input, with a scaling factor which is
laser-trimmed to 40 dB per volt, that is, 25 mV/dB. An internal bandgap reference ensures stability of the scaling with respect to supply and temperature variations.
When the differential input voltage V
= 0 V, the attenuator
G
“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 common-mode 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 Pins 5 and 7 are strapped (see next
G
+ 10 (1)
G
section) the gain becomes
Gain (dB) = 40 V
+ 20 for 0 to +40 dB
G
and
Gain (dB) = 40 V
+ 30 for +10 to +50 dB (2)
G
The high impedance gain-control input ensures minimal loading when driving many amplifiers in multiple channel or cascaded applications. The differential capability provides flexibility in choosing the appropriate signal levels and polarities for various control schemes.
For example, if the gain is to be controlled by a DAC providing a positive only ground-referenced output, the “Gain Control LO” (GNEG) pin should be biased to a fixed offset of +500 mV, to set the gain to –10 dB when “Gain Control HI” (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 2. 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
OUT
lowered to –11 dB/+31 dB; when an external resistor is placed between V
and FDBK any intermediate gain can be achieved,
OUT
for example, –1 dB/+41 dB. Figure 3 shows the nominal maxi­mum gain versus external resistor for this mode.
VC1
VPOS
VPOS
GPOS
AD603
GNEG
VINP
COMM
V
OUT
VNEG
FDBK
VNEG
V
OUT
VC2
V
IN
a. –10 dB to +30 dB; 90 MHz Bandwidth
VC1
VPOS
VPOS
GPOS
AD603
VC2
V
IN
GNEG
VINP
COMM
V
OUT
VNEG
FDBK
VNEG
2.15kV
5.6pF
V
OUT
b. 0 dB to +40 dB; 30 MHz Bandwidth
VC1
VPOS
VPOS
GPOS
AD603
VC2
V
IN
GNEG
VINP
COMM
V
OUT
VNEG
FDBK
VNEG
18pF
V
OUT
c. +10 dB to +50 dB; 9 MHz Bandwidth
Figure 2. Pin Strapping to Set Gain
52 50 48 46 44 42 40
DECIBELS
38 36 34 32 30
10 1M
Figure 3. Gain vs. R
–1:VdB (OUT)
VdB (OUT)
–2:VdB (OUT)
100 1k 10k 100k
EXT
R
EXT
, Showing Worst-Case Limits Assuming Internal Resistors Have a Maximum Tolerance of 20%
REV. C
–5–
AD603
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 2.
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% inter-
nal resistor, the overall gain accuracy is somewhat poorer. The
worst-case error occurs at about 2 k (see Figure 4).
1.2
1.0
0.8
0.6
0.4
0.2
0.0
DECIBELS
–0.2 –0.4 –0.6 –0.8 –1.0
10 1M
VdB (OUT) – VdB (O
100 1k 10k 100k
–1:VdB (OUT) – (–1):VdB (O
)
REF
R
EXT
REF
)
Figure 4. Worst-Case Gain Error, Assuming Internal Resis­tors Have a Maximum Tolerance of –20% (Top Curve) or +20% (Bottom Curve)
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 2 shows how optional capacitors may be added to extend the frequency response in high gain modes.
CASCADING TWO AD603S
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 input resistance of the following amplifier.
For two AD603s, the total gain-control range becomes 84 dB (two times 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 Signal-to-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 possible. Figure 5 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 6 shows 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) arc biased by stable voltages to provide the needed gain-offsets. These volt­ages may be provided by resistive dividers operating from a common voltage reference.
90
85
80
75
70
65
S/N RATIO – dB
60
55
50
–0.2 2.20.2 0.6 1.0 1.4 1.8
V
C
Figure 5. SNR vs. Control Voltage—Sequential Control (1 MHz Bandwidth)
The gains are offset (Figure 7) 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 of this data sheet 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
G
+ G
G
O
(3)
by the gain range chosen. In the explanatory notes that follow, we assume the maximum-bandwidth connections are used, for which G
is –20 dB.
O
–6–
REV. C
A1 A2
–40.00dB
AD603
–51.07dB
INPUT
0dB
V
= 0V
C
–42.14dB
GPOS GNEG
V
G1
VO1 = 0.473V
31.07dB
–8.93dB
a.
0dB
INPUT
0dB
V
= 1.0V
C
0dB
GPOS GNEG
V
G1
VO1 = 0.473V
31.07dB
31.07dB
b.
0dB
INPUT
0dB
V
= 2.0V
C
0dB
GPOS GNEG
V
G1
VO1 = 0.473V
31.07dB
31.07dB
c.
Figure 6. AD603 Gain Control Input Calculations for Sequential Control Operation
+31.07dB
+10dB
+31.07dB
A1 A2
*
+28.96dB
*
–11.07dB
0.473 1.526
–11.07dB
GAIN
(dB)
–8.93dB
0 0.5 1.0 1.50 2.0 VC (V)
–20 0 20 40 60 62.14–22.14
*GAIN OFFSET OF 1.07dB, OR 26.75mV
Figure 7. Explanation of Offset Calibration for Sequential Control
With reference to Figure 6, note that VG1 refers to the differen­tial gain-control input to A1 and V gain-control input to A2. When V
refers to the differential
G2
is zero, VG1 = –473 mV and
G
thus the gain of A1 is –8.93 dB (recall that the gain of each indi­vidual amplifier in the maximum-bandwidth mode is –10 dB
= –500 mV and 10 dB for VG = 0 V); meanwhile, VG2 =
for V
G
–1.908 V so the gain of A2 is “pinned” at –11.07 dB. The over­all gain is thus –20 dB. This situation is shown in Figure 6a.
When V
= +1.00 V, VG1 = 1.00 V – 0.473 V = +0.526 V,
G
which 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
G2
A2’s gain at nearly its minimum value –11.07 dB. Close analysis shows that the degree to which neither AD603 is completely pushed to its maximum or minimum gain exactly cancels in the overall gain, which is now +20 dB. This is depicted in Figure 6b.
–42.14dB
GPOS GNEG
V
G2
–42.14dB
GPOS GNEG
V
G2
–2.14dB
GPOS GNEG
V
G2
When V
G
V
= 1.526V
O2
–11.07dB
V
= 1.526V
O2
–28.93dB
V
= 1.526V
O2
31.07dB
31.07dB
31.07dB
OUTPUT –20dB
OUTPUT 20dB
OUTPUT 60dB
= +2.0 V, the gain of A1 is pinned at 31.07 dB and that of A2 is near its maximum value of 28.93 dB, resulting in an overall gain of 60 dB (see Figure 6c). This mode of operation is further clarified by Figure 8, which is a plot of the separate gains of A1 and A2 and the overall gain versus the control voltage. Figure 9 is a plot of the gain error of the cascaded amplifiers versus the control voltage. Figure 10 is a plot of the gain error of the cascaded stages versus the control voltages.
70
60
50
40
30
20
10
OVERALL GAIN – dB
0
–10
–20 –30
–0.2 2.20.2
A1
0.6 0.1 1.4 1.8 V
C
COMBINED
A2
Figure 8. Plot of Separate and Overall Gains in Sequential Control
REV. C
–7–
AD603
90
80
70
60
50
40
S/N RATIO – dB
30
20
10
–0.2 2.20.2 0.6 1.0 1.4 1.8
V
C
Figure 9. SNR for Cascaded Stages—Sequential Control
2.0
1.5
1.0
0.5
0.0
2.0
1.5
1.0
0.5
0.0
–0.5
GAIN ERROR – dB
–1.0
–1.5
–2.0
–0.2
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 V
C
Figure 11. Gain Error for Cascaded Stages–Parallel Control
90
85
80
75
70
–0.5
GAIN ERROR – dB
–1.0
–1.5
–2.0
–0.2
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.0 2.2 V
C
Figure 10. 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
depends on the range selected; for example,
O
in the maximum-bandwidth mode, G
+ G
G
O
is +20 dB. Alternatively,
O
(4)
the GNEG pins may be connected to an offset voltage of +0.500 V, in which case, G
is –20 dB.
O
The amplitude of the gain ripple in this case is also doubled, as shown in Figure 11, while the instantaneous signal-to-noise ratio at the output of A2 now decreases linearly as the gain increased (Figure 12).
65
IS/N RATIO – dB
60
55
50
–0.2
0
0.2 0.4 0.6 0.8 1.0 1.2 V
C
Figure 12. ISNR for Cascaded Stages–Parallel Control
Low Gain Ripple Mode (Minimum Gain Error)
As can be seen from Figures 9 and 10, 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 13 shows that much lower gain ripple when configured in this manner. Figure 14 plots the ISNR as a function of gain; it is very similar to that in the “Parallel Mode.”
–8–
REV. C
AD603
3.0
2.5
2.0
1.5
1.0
0.5
0.0
–0.5
GAIN ERROR – dB
–1.0 –1.5 –2.0 –2.5 –3.0
–0.1
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1 V
C
Figure 13. Gain Error for Cascaded Stages–Low Ripple Mode
90
85
80
75
70
65
IS/N RATIO – dB
60
55
50
–0.2
0
0.2 0.4 0.6 0.8 1.0 1.2 V
C
Figure 14. ISNR vs. Control Voltage–Low Ripple Mode
THEORY OF THE AD603 A Low Noise AGC Amplifier
Figure 15 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-in-dB 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, here provided 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 pins 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 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 col-
lector current of Q1, which increases with the amplitude of the
C7
0.1mF
C1
+
C3 100mF
RT 100V
0.1mF
2
1
2.49kV
C4
0.1mF
10V
R1
R2
2.49kV
J1
NOTES
1
RT PROVIDES A 50V INPUT IMPEDANCE
2
C3 AND C5 ARE TANTALUM
10V
R13
2.49kV
A1
0.1mF
AD603
+
C5
2
100mF
R5
5.49kV
5.5V 6.5V
SEQUENTIAL GAIN
0.1mF
C2
10V
R3
2.49kV
C6
0.1mF
1V OFFSET FOR
R6
1.05kV
Figure 15. A Low Noise AGC Amplifier
C8
R4
2.49kV
THIS CAPACITOR SETS AGC TIME CONSTANT
10V
R14
2.49kV
A2
AD603
R7
3.48kV
V
C
AV
0.1mF
AGC LINE
10V
AGC
1.54kV
2N3906
2N3904
806V
Q2
Q1
10V
C10
0.1mF
C11
0.1mF
C9
0.1mF
J2
R9
R8
R10
1.24kV
R11
3.83kV 5V R12
4.99kV
REV. C
–9–
AD603
output signal. The automatic gain control voltage, V time-integral of this error current. In order for V
AGC
(and thus
AGC
, is the
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, until
AGC
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.
During the time V of Q1, Q1 conducts; when V
is negative with respect to the base voltage
OUT
is positive, it is cut off. Since
OUT
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 typically about 700 mV, or 2 V
is forced to be just the V
OUT
BE
peak-to-peak. This voltage,
of Q1 at 600 µA,
BE
hence 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, first 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
is now the sum of VBE and a
OUT
voltage that is PTAT and which can be chosen to have an equal but opposite TC to that of the V
. This is actually nothing more
BE
than an application of the “bandgap 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 bandgap 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 would add a PTAT voltage of 500 mV at 300 K, increasing by 1.66 mV/°C. In prac-
tice, 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 inexpensive 2N3904/2N306 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
AGC
helps to minimize distortion
AV
sine 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 radio and TV stations, etc. In bench evaluation, we recommend placing all of the components in 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.
–10–
REV. C
2.50
2.00
1.50
1.00
0.50
0.00
GAIN ERROR – dB
–0.50
–1.00
–1.50
–0.5
45MHz
70MHz
10.7MHz
455kHz
70MHz
–0.4 –0.3–0.2 –0.1 0.0 0.2 0.3 0.4 0.5 0.6
GAIN VOLTAGE – Volts
Figure 16. Gain Error vs. Gain Control Voltage at 455 kHz, 10.7 MHz, 45 MHz, 70 MHz
GAIN – dB
100k 1M 10M 100M
FREQUENCY – Hz
Figure 19. Frequency and Phase Response vs. Gain (Gain = +30 dB,
= –30 dBm, Pin 5 Connected to
P
IN
Pin 7)
GAIN – dB
100k 1M 10M 100M
FREQUENCY – Hz
Figure 17. Frequency and Phase Response vs. Gain (Gain = –10 dB,
= –30 dBm, Pin 5 Connected to
P
IN
Pin 7)
7.60
7.40
7.20
7.00
6.80
GROUP DELAY – ns
6.60
6.40 –0.4 –0.2 0 0.2 0.4 0.6
–0.6
GAIN CONTROL VOLTAGE – Volts
Figure 20. Group Delay vs. Gain Control Voltage
AD603
GAIN – dB
100k 1M 10M 100M
Figure 18. Frequency and Phase Response vs. Gain (Gain = +10 dB, P
= –30 dBm, Pin 5 Connected to
IN
Pin 7)
HP3326A
DUAL
CHANNEL
SYNTHESIZER
Figure 21. Third Order Intermodula­tion Distortion Test Setup
FREQUENCY – Hz
+5V
AD603
100
V
0.1mF
–5V
0.1mF
DATEL
DVC 8500
103
PROBE
511V
HP3585A SPECTRUM ANALYZER
10dB/DIV
Figure 22. Third Order Intermodula-
×
tion Distortion at 455 kHz (10
Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, PIN = 0 dBm, Pin 5 Con­nected to Pin 7)
REV. C
10dB/DIV
Figure 23. Third Order Intermodula-
×
tion Distortion at 10.7 MHz (10
Probe Used to HP3585A Spectrum Analyzer, Gain = 0 dB, PIN = 0 dBm, Pin 5 Con­nected to Pin 7)
–11–
–1.0 –1.2 –1.4
–1.6 –1.8 –2.0 –2.2 –2.4 –2.6 –2.8 –3.0 –3.2
NEGATIVE OUTPUT VOLTAGE LIMIT – Volts
–3.4
0
50 100 200 500 1000 2000
LOAD RESISTANCE – V
Figure 24. Typical Output Voltage Swing vs. Load Resistance (Negative Output Swing Limits First)
AD603
FREQUENCY – Hz
INPUT IMPEDANCE – V
100k
102
100
98
96
1M 10M 100M
94
102
100
98
96
INPUT IMPEDANCE – V
94
100k
1M 10M 100M
FREQUENCY – Hz
Figure 25. Input Impedance vs.
Frequency (Gain = –10 dB)
1V
100
90
10
0%
1V
200ns
102
100
98
96
INPUT IMPEDANCE – V
94
100k
1M 10M 100M
FREQUENCY – Hz
Figure 26. Input Impedance vs.
Frequency (Gain = +10 dB)
4.5V
INPUT GND
1V/DIV
500mV
OUTPUT GND
500mV/DIV
Figure 27. Input Impedance vs.
Frequency (Gain = +30 dB)
8V
INPUT GND 100mV/DIV
1V
OUTPUT GND
1V/DIV
Figure 28. Gain-Control Channel Response Time
3.5V
INPUT
500mV/DIV
500mV
–1.5V
–44ns 50ns 456ns
Figure 31. Transient Response, G = 0 dB, Pin 5 Connected to Pin 7
OUTPUT
500mV/DIV
(Input is 500 ns Period, 50% Duty­ Cycle Square Wave, Output Is
Captured Using Tektronix 11402
Digitizing Oscilloscope)
GND
GND
–500mV
–49ns 50ns 451ns
Figure 29. Input Stage Overload Recovery Time, Pin 5 Connected to Pin 7 (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
–1.5V
OUTPUT GND
500mV/DIV
–44ns 50ns 456ns
Figure 32. Transient Response, G = +20 dB, Pin 5 Connected to Pin 7 (Input is 500 ns Period, 50% Duty­ Cycle Square Wave, Output Is
Captured Using Tektronix 11402
Digitizing Oscilloscope)
–2V
–49ns 50ns 451ns
Figure 30. Output Stage Overload Recovery Time, Pin 5 Connected to Pin 7 (Input Is 500 ns Period, 50% Duty-Cycle Square Wave, Output Is Captured Using Tektronix 11402 Digitizing Oscilloscope)
0 –10 –20 –30 –40
PSRR – dB
–50 –60
100k
1M 10M 100M
FREQUENCY – Hz
Figure 33. PSRR vs. Frequency (Worst Case Is Negative Supply PSRR, Shown Here)
–12–
REV. C
AD603
+5V
mF
HP3326A
DUAL
CHANNEL
SYNTHESIZER
100
0.1mF
0.1
HP3585A
50V
AD603
V
–5V
DATEL
DVC 8500
SPECTRUM
ANALYZER
Figure 34. Test Setup Used for: Noise Figure, 3rd Order Intercept and 1 dB Compression Point Measurements
0
–5
–10
–15
INPUT LEVEL – dBm
–20
TA = 258C TEST SETUP
FIGURE 34
23
30MHz
21 19
17 15
13 11
NOISE FIGURE – dB
9
7
5
21 22 23 24 25 26 27 28 29 30
20
70MHz
50MHz
GAIN – dB
10MHz
TA = 258C R
= 50V
S
TEST SETUP FIGURE 34
Figure 35. Noise Figure in –10 dB/ +30 dB Mode
20
18
16
14
12
OUTPUT LEVEL – dBm
10
30MHz
40MHz
70MHz
TA = 258C TEST SETUP
FIGURE 34
21
10MHz
19
17
20MHz
15
13
11
NOISE FIGURE – dB
9
7
5
30
31 32 33 34 35 36 37 38 39 40
GAIN – dB
TA = 258C
= 50V
R
S
TEST SETUP FIGURE 34
Figure 36. Noise Figure in 0 dB/+40 dB Mode
20
18
16
14
12
OUTPUT LEVEL – dBm
10
30MHz
40MHz
70MHz
TA = 258C
= 50V
R
S
= 50V
R
IN
= 100V
R
L
TEST SETUP FIGURE 34
–25
10
30 50 70
INPUT FREQUENCY – MHz
Figure 37. 1 dB Compression Point, –10 dB/+30 dB Mode, Gain = 30 dB
8
–20
–10 0
INPUT LEVEL – dBm
Figure 38. 3rd Order Intercept –10 dB/ +30 dB Mode, Gain = 10 dB
8
–40
–30 –20
INPUT LEVEL – dBm
Figure 39. 3rd Order Intercept, –10 dB/ +30 dB Mode, Gain = 30 dB
REV. C
–13–
AD603
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
8-Lead Cerdip (Q-8)
0.200 (5.08) MAX
0.200 (5.08)
0.125 (3.18)
0.023 (0.58)
0.014 (0.36)
0.1574 (4.00)
0.1497 (3.80)
PIN 1
0.0098 (0.25)
0.0040 (0.10) SEATING
0.005 (0.13) MIN
8
1
0.405 (10.29)
0.1 968 (5.00)
0.1 890 (4.80)
85
0.0500 (1.27)
PLANE
0.055 (1.4) MAX
5
0.310 (7.87)
0.220 (5.59)
4
PIN 1
MAX
0.100
(2.54)
BSC
0.060 (1.52)
0.015 (0.38)
0.070 (1.78)
0.030 (0.76)
0.150 (3.81) MIN
SEATING PLANE
8-Lead SOIC (SO-8)
0.2440 (6.20)
0.2284 (5.80)
41
BSC
0.0192 (0.49)
0.0138 (0.35)
0.0688 (1.75)
0.0532 (1.35)
0.0098 (0.25)
0.0075 (0.19)
0.320 (8.13)
0.290 (7.37)
15°
0°
0.0196 (0.50)
0.0099 (0.25)
88
0.0500 (1.27)
08
0.0160 (0.41)
C1851a–0–1/00 (rev. C)
0.015 (0.38)
0.008 (0.20)
3 458
–14–
PRINTED IN U.S.A.
REV. C
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