AD734 [ADI]

10 MHz, 4-Quadrant Multiplier/Divider; 10兆赫,四象限乘法器/除法器
AD734
型号: AD734
厂家: ADI    ADI
描述:

10 MHz, 4-Quadrant Multiplier/Divider
10兆赫,四象限乘法器/除法器

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10 MHz, 4-Quadrant  
Multiplier/Divider  
a
AD734  
CONNECTION DIAGRAM  
FEATURES  
High Accuracy  
0.1% Typical Error  
High Speed  
14-Lead DIP  
(Q Package and N Package)  
10 MHz Full-Power Bandwidth  
450 V/s Slew Rate  
200 ns Settling to 0.1% at Full Power  
Low Distortion  
–80 dBc from Any Input  
Third-Order IMD Typically –75 dBc at 10 MHz  
Low Noise  
94 dB SNR, 10 Hz to 20 kHz  
70 dB SNR, 10 Hz to 10 MHz  
Direct Division Mode  
2 MHz BW at Gain of 100  
X1  
X2  
U0  
U1  
VP POSITIVE SUPPLY  
1
2
3
4
5
6
7
14  
13  
12  
11  
10  
9
X INPUT  
DD DENOMINATOR DISABLE  
W OUTPUT  
AD734  
TOP VIEW  
(Not to Scale)  
DENOMINATOR  
INTERFACE  
Z1  
Z INPUT  
Z2  
U2  
Y1  
ER REFERENCE VOLTAGE  
VN NEGATIVE SUPPLY  
Y INPUT  
Y2  
8
APPLICATIONS  
High Performance Replacement for AD534  
Multiply, Divide, Square, Square Root  
Modulator, Demodulator  
Wideband Gain Control, RMS-DC Conversion  
Voltage-Controlled Amplifiers, Oscillators, and Filters  
Demodulator with 40 MHz Input Bandwidth  
demodulator with input frequencies as high as 40 MHz as long  
as the desired output frequency is less than 10 MHz.  
The AD734AQ and AD734BQ are specified for the industrial  
temperature range of –40°C to +85°C and come in a 14-lead  
ceramic DIP. The AD734SQ/883B, available processed to  
MIL-STD-883B for the military range of –55°C to +125°C, is  
available in a 14-lead ceramic DIP.  
PRODUCT DESCRIPTION  
The AD734 is an accurate high speed, four-quadrant analog  
multiplier that is pin-compatible with the industry-standard  
AD534 and provides the transfer function W = XY/U. The  
AD734 provides a low-impedance voltage output with a full-  
power (20 V pk-pk) bandwidth of 10 MHz. Total static error  
(scaling, offsets, and nonlinearities combined) is 0.1% of full  
scale. Distortion is typically less than –80 dBc and guaranteed.  
The low capacitance X, Y and Z inputs are fully differential. In  
most applications, no external components are required to  
define the function.  
PRODUCT HIGHLIGHTS  
The AD734 embodies more than two decades of experience in  
the design and manufacture of analog multipliers, to provide:  
1. A new output amplifier design with more than twenty times  
the slew-rate of the AD534 (450 V/µs versus 20 V/µs) for a  
full power (20 V pk-pk) bandwidth of 10 MHz.  
2. Very low distortion, even at full power, through the use of  
circuit and trimming techniques that virtually eliminate all of  
the spurious nonlinearities found in earlier designs.  
The internal scaling (denominator) voltage U is 10 V, derived  
from a buried-Zener voltage reference. A new feature provides  
the option of substituting an external denominator voltage,  
allowing the use of the AD734 as a two-quadrant divider with a  
1000:1 denominator range and a signal bandwidth that remains  
10 MHz to a gain of 20 dB, 2 MHz at a gain of 40 dB and  
200 kHz at a gain of 60 dB, for a gain-bandwidth product of  
200 MHz.  
3. Direct control of the denominator, resulting in higher  
multiplier accuracy and a gain-bandwidth product at small  
denominator values that is typically 200 times greater than  
that of the AD534 in divider modes.  
4. Very clean transient response, achieved through the use of a  
novel input stage design and wide-band output amplifier,  
which also ensure that distortion remains low even at high  
frequencies.  
The advanced performance of the AD734 is achieved by a  
combination of new circuit techniques, the use of a high speed  
complementary bipolar process and a novel approach to laser-  
trimming based on ac signals rather than the customary dc  
methods. The wide bandwidth (>40 MHz) of the AD734’s  
input stages and the 200 MHz gain-bandwidth product of the  
multiplier core allow the AD734 to be used as a low distortion  
5. Superior noise performance by careful choice of device  
geometries and operating conditions, which provide a  
guaranteed 88 dB of dynamic range in a 20 kHz bandwidth.  
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.  
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.  
Tel: 781/329-4700  
Fax: 781/326-8703  
World Wide Web Site: http://www.analog.com  
© Analog Devices, Inc., 1999  
(T = +25؇C, +V = VP = +15 V, –V = VN = –15 V, R 2 k)  
AD734–SPECIFICATIONS  
TRANSFER FUNCTION  
A
S
S
L
X X Y Y  
(
2 )(  
)
1
1
2
W = AO  
Z Z  
(
)
1
2
U U  
(
)
1
2
A
B
S
Parameter  
Conditions  
Min Typ Max Min Typ Max Min Typ Max  
Units  
MULTIPLIER PERFORMANCE  
Transfer Function  
W = XY/10  
0.1 0.4  
1
W = XY/10  
0.1 0.25  
0.6  
W = XY/10  
0.1 0.4  
Total Static Error1  
Over TMIN to TMAX  
vs. Temperature  
–10 V X, Y 10 V  
%
%
%/°C  
%/V  
%
1.25  
TMIN to TMAX  
±VS = 14 V to 16 V  
–10 V X +10 V, Y = +10 V  
–10 V Y +10 V, X = +10 V  
X = 7 V rms, Y = +10 V, f 5 kHz  
TMIN to TMAX  
Y = 7 V rms, X = +10 V, f 5 kHz  
TMIN to TMAX  
X = 7 V rms, Y = nulled, f 5 kHz  
Y = 7 V rms, X = nulled, f 5 kHz  
X = Y = 0  
0.004  
0.01 0.05  
0.05  
0.003  
0.01 0.05  
0.05  
0.025  
–66  
0.004  
0.01 0.05  
0.05  
0.025  
–58  
vs. Either Supply  
Peak Nonlinearity  
0.025  
%
THD2  
–58  
dBc  
dBc  
dBc  
dBc  
dBc  
dBc  
–55  
–60  
–57  
–63  
–80  
–74  
–55  
–60  
–57  
Feedthrough  
–85 –60  
–85 –66  
–85 –70  
–85 –76  
–85 –60  
–85 –66  
Noise (RTO)  
Spectral Density  
Total Output Noise  
100 Hz to 1 MHz  
10 Hz to 20 kHz  
TMIN to TMAX  
1.0  
–94 –88  
–85  
1.0  
–94 –88  
–85  
1.0  
–94 –88  
–85  
µV/Hz  
dBc  
dBc  
DIVIDER PERFORMANCE (Y = 10 V)  
Transfer Function  
Gain Error  
W = XY/U  
1
1.25 × U  
0.3  
W = XY/U  
1
1.25 × U  
0.15  
W = XY/U  
1
1.25 × U  
Y = 10 V, U = 100 mV to 10 V  
Y 10 V  
%
V
%
%
ns  
X Input Clipping Level  
U Input Scaling Error3  
0.3  
TMIN to TMAX  
U = 1 V to 10 V Step, X = 1 V  
0.8  
0.65  
1
(Output to 1%)  
100  
100  
100  
INPUT INTERFACES (X, Y, & Z)  
3 dB Bandwidth  
Operating Range  
40  
±12.5  
15  
40  
±12.5  
5
40  
±12.5  
15  
MHz  
V
Differential or Common Mode  
TMIN to TMAX  
X Input Offset Voltage  
mV  
mV  
mV  
mV  
mV  
mV  
dB  
dB  
dB  
nA  
25  
10  
12  
20  
15  
5
6
25  
10  
12  
20  
Y Input Offset Voltage  
TMIN to TMAX  
Z Input Offset Voltage  
10  
50  
70  
TMIN to TMAX  
f 1 kHz  
TMIN to TMAX  
f = 5 kHz  
50  
90  
Z Input PSRR (Either Supply)  
54  
50  
70  
70  
66  
56  
70  
54  
50  
70  
70  
CMRR  
85  
50  
85  
50  
85  
50  
Input Bias Current (X, Y, Z Inputs)  
300  
400  
150  
300  
300  
500  
TMIN to TMAX  
Differential  
Differential  
nA  
kΩ  
pF  
Input Resistance  
Input Capacitance  
50  
2
50  
2
50  
2
DENOMINATOR INTERFACES (U0, U1, & U2)  
Operating Range  
VN to VP-3  
1000:1  
28  
VN to VP-3  
1000:1  
28  
VN to VP-3  
1000:1  
28  
V
Denominator Range  
Interface Resistor  
U1 to U2  
kΩ  
OUTPUT AMPLIFIER (W)  
Output Voltage Swing  
Open-Loop Voltage Gain  
Dynamic Response  
3 dB Bandwidth  
Slew Rate  
TMIN to TMAX  
±12  
±12  
±12  
V
dB  
X = Y = 0, Input to Z  
From X or Y Input, CL 20 pF  
W 7 V rms  
72  
72  
72  
8
10  
450  
8
10  
450  
8
10  
450  
MHz  
V/µs  
Settling Time  
+20 V or –20 V Output Step  
To 1%  
To 0.1%  
Short-Circuit Current  
125  
200  
50  
125  
200  
50  
125  
200  
50  
ns  
ns  
mA  
TMIN to TMAX  
20  
80  
20  
80  
20  
80  
POWER SUPPLIES, ±VS  
Operating Supply Range  
Quiescent Current  
±8  
6
±16.5 ±8  
12  
±16.5 ±8  
12  
±16.5  
12  
V
mA  
TMIN to TMAX  
9
6
9
6
9
NOTES  
1Figures given are percent of full scale (e.g., 0.01% = 1 mV).  
2dBc refers to deciBels relative to the full-scale input (carrier) level of 7 V rms.  
3See Figure 10 for test circuit.  
All min and max specifications are guaranteed.  
Specifications subject to change without notice.  
REV. C  
–2–  
AD734  
ABSOLUTE MAXIMUM RATINGS1  
ORDERING GUIDE  
Supply Voltage . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±18 V  
Internal Power Dissipation2  
Temperature  
Range  
Package  
Description Option  
Package  
Model  
for TJ max = 175°C . . . . . . . . . . . . . . . . . . . . . . . . 500 mW  
X, Y and Z Input Voltages . . . . . . . . . . . . . . . . . . . . VN to VP  
Output Short Circuit Duration . . . . . . . . . . . . . . . . Indefinite  
Storage Temperature Range  
Q . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . –65°C to +150°C  
Operating Temperature Range  
AD734A, B (Industrial) . . . . . . . . . . . . . . . –40°C to +85°C  
AD734S (Military) . . . . . . . . . . . . . . . . . . –55°C to +125°C  
Lead Temperature Range (soldering 60 sec) . . . . . . . . +300°C  
Transistor Count . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81  
ESD Rating . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 500 V  
AD734AN  
AD734BN  
AD734AQ  
AD734BQ  
–40°C to +85°C  
–40°C to +85°C  
–40°C to +85°C  
–40°C to +85°C  
Plastic DIP  
Plastic DIP  
Cerdip  
N-14  
N-14  
Q-14  
Q-14  
Q-14  
Cerdip  
AD734SQ/883B –55°C to +125°C Cerdip  
AD734SCHIPS –55°C to +125°C Die  
NOTES  
1Stresses 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.  
214-Lead Ceramic DIP: θJA = 110°C/W.  
CHIP DIMENSIONS & BONDING DIAGRAM  
Dimensions shown in inches and (mm).  
(Contact factory for latest dimensions.)  
REV. C  
–3–  
AD734  
is typically less than 5 mV, which corresponds to a bias current  
of only 100 nA. This low bias current ensures that mismatches  
in the sources resistances at a pair of inputs does not cause an  
offset error. These currents remain low over the full temperature  
range and supply voltages.  
X1  
X2  
X = X – X  
1 2  
HIGH-ACCURACY  
TRANSLINER  
MULTIPLIER CORE  
XIF  
DD  
XY/U – Z  
U
XZ  
U
DENOMINATOR  
CONTROL  
WIF  
W
U 0  
U1  
The common-mode range of the X, Y and Z inputs does not  
fully extend to the supply rails. Nevertheless, it is often possible  
to operate the AD734 with one terminal of an input pair con-  
nected to either the positive or negative supply, unlike previous  
multipliers. The common-mode resistance is several megohms.  
A
O
ER  
Ru  
AD734  
U 2  
Y1  
Y2  
Z1  
Z2  
YIF  
ZIF  
Y = Y – Y  
1
Z = Z – Z  
2
1
2
The full-scale output of ±10 V can be delivered to a load resis-  
tance of 1 k(although the specifications apply to the standard  
multiplier load condition of 2 k). The output amplifier is  
stable driving capacitive loads of at least 100 pF, when a slight  
increase in bandwidth results from the peaking caused by this  
capacitance. The 450 V/µs slew rate of the AD734’s output am-  
plifier ensures that the bandwidth of 10 MHz can be maintained  
up to the full output of 20 V pk-pk. Operation at reduced supply  
voltages is possible, down to ±8 V, with reduced signal levels.  
Figure 1. AD734 Block Diagram  
FUNCTIONAL DESCRIPTION  
Figure 1 is a simplified block diagram of the AD734. Operation  
is similar to that of the industry-standard AD534 and in many  
applications these parts are pin-compatible. The main functional  
difference is the provision for direct control of the denominator  
voltage, U, explained fully on the following page. Internal sig-  
nals are actually in the form of currents, but the function of the  
AD734 can be understood using voltages throughout, as shown  
in this figure. Pins are named using upper-case characters (such  
as X1, Z2) while the voltages on these pins are denoted by sub-  
scripted variables (for example, X1, Z2).  
Available Transfer Functions  
The uncommitted (open-loop) transfer function of the AD734 is  
X X Y Y  
(
2 )(  
)
1
1
2
W = AO  
Z Z  
(
)
1
2
,
(1)  
The AD734’s differential X, Y and Z inputs are handled by  
wideband interfaces that have low offset, low bias current and  
low distortion. The AD734 responds to the difference signals  
X = X1 – X2, Y = Y1 – Y2 and Z = Z1 – Z2, and rejects  
common-mode voltages on these inputs. The X, Y and Z  
interfaces provide a nominal full-scale (FS) voltage of ±10 V,  
but, due to the special design of the input stages, the linear  
range of the differential input can be as large as ±17 V. Also  
unlike previous designs, the response on these inputs is not  
clipped abruptly above ±15 V, but drops to a slope of one half.  
U
where AO is the open-loop gain of the output op-amp, typically  
72 dB. When a negative feedback path is provided, the circuit  
will force the quantity inside the brackets essentially to zero,  
resulting in the equation  
(X1 – X2)(Y1 – Y2) = U (Z1 – Z2)  
(2)  
This is the most useful generalized transfer function for the  
AD734; it expresses a balance between the product XY and the  
product UZ. The absence of the output, W, in this equation  
only reflects the fact that we have not yet specified which of the  
inputs is to be connected to the op amp output.  
The bipolar input signals X and Y are multiplied in a translinear  
core of novel design to generate the product XY/U. The  
denominator voltage, U, is internally set to an accurate,  
temperature-stable value of 10 V, derived from a buried-Zener  
reference. An uncalibrated fraction of the denominator voltage  
U appears between the voltage reference pin (ER) and the  
negative supply pin (VN), for use in certain applications where  
a temperature-compensated voltage reference is desirable. The  
internal denom-inator, U, can be disabled, by connecting the  
denominator disable Pin 13 (DD) to the positive supply pin  
(VP); the denom-inator can then be replaced by a fixed or  
variable external volt-age ranging from 10 mV to more than 10 V.  
Most of the functions of the AD734 (including division, unlike  
the AD534 in this respect) are realized with Z1 connected to W.  
So, substituting W in place of Z1 in the above equation results in  
an output.  
X X Y Y  
(
2 )(  
)
+ Z2.  
1
1
2
W =  
(3)  
U
The free input Z2 can be used to sum another signal to the  
output; in the absence of a product signal, W simply follows the  
voltage at Z2 with the full 10 MHz bandwidth. When not  
needed for summation, Z2 should be connected to the ground  
associated with the load circuit. We can show the allowable  
polarities in the following shorthand form:  
The high-gain output op-amp nulls the difference between  
XY/U and an additional signal Z, to generate the final output  
W. The actual transfer function can take on several forms, de-  
pending on the connections used. The AD734 can perform all  
of the functions supported by the AD534, and new functions  
using the direct-division mode provided by the U-interface.  
±X ±Y  
(
)(  
)
+ ± Z.  
±W =  
(
)
(4)  
+U  
Each input pair (X1 and X2, Y1 and Y2, Z1 and Z2) has a  
differential input resistance of 50 k; this is formed by “real”  
resistors (not a small-signal approximation) and is subject to a  
tolerance of ±20%. The common-mode input resistance is  
several megohms and the parasitic capacitance is about 2 pF.  
(
)
In the recommended direct divider mode, the Y input is set to a  
fixed voltage (typically 10 V) and U is varied directly; it may  
have any value from 10 mV to 10 V. The magnitude of the ratio  
X/U cannot exceed 1.25; for example, the peak X-input for U  
= 1 V is ±1.25 V. Above this level, clipping occurs at the  
positive and negative extremities of the X-input. Alternatively,  
The bias currents associated with these inputs are nulled by  
laser-trimming, such that when one input of a pair is optionally  
ac-coupled and the other is grounded, the residual offset voltage  
REV. C  
–4–  
AD734  
the AD734 can be operated using the standard (AD534) divider  
connections (Figure 8), when the negative feedback path is  
established via the Y2 input. Substituting W for Y2 in Equation  
(2), we get  
After temperature-correction (block TC), the reference voltage  
is applied to transistor Qd and trimmed resistor Rd, which  
generate the required reference current. Transistor Qu and  
resistor Ru are not involved in setting up the internal denominator,  
and their associated control pins U0, U1 and U2 will normally  
be grounded. The reference voltage is also made available, via  
the 100 kresistor Rr, at Pin 9 (ER); the purpose of Qr is  
explained below.  
Z Z  
(
(
)
+Y1.  
2
1
W = U  
(5)  
X X  
)
1
2
In this case, note that the variable X is now the denominator,  
When the control pin DD (denominator disable) is connected to  
VP, the internal source of Iu is shut off, and the collector cur-  
rent of Qu must provide the denominator current. The resistor  
Ru is laser-trimmed such that the multiplier denominator is  
exactly equal to the voltage across it (that is, across pins U1 and  
U2). Note that this trimming only sets up the correct internal  
ratio; the absolute value of Ru (nominally 28 k) has a  
tolerance of ±20%. Also, the alpha of Qu, (typically 0.995)  
which might be seen as a source of scaling error, is canceled by  
the alpha of other transistors in the complete circuit.  
and the above restriction (X/U 1.25) on the magnitude of the  
X input does not apply. However, X must be positive in order  
for the feedback polarity to be correct. Y1 can be used for  
summing purposes or connected to the load ground if not  
needed. The shorthand form in this case is  
±Z  
(
(
)
+ ±Y .  
±W = +U  
(
)
(
)
(
)
(6)  
+X  
)
In some cases, feedback may be connected to two of the avail-  
able inputs. This is true for the square-rooting connections  
(Fig-ure 9), where W is connected to both X1 and Y2. Setting  
X1 = W and Y2 = W in Equation (2), and anticipating the  
possibility of again providing a summing input, so setting X2 = S  
and Y1 = S, we find, in shorthand form  
In the simplest scheme (Figure 3), an externally-provided  
control voltage, VG, is applied directly to U0 and U2 and the  
resulting voltage across Ru is therefore reduced by one VBE. For  
example, when VG = 2 V, the actual value of U will be about  
1.3 V. This error will not be important in some closed-loop  
applications, such as automatic gain control (AGC), but clearly  
is not acceptable where the denominator value must be well-  
defined. When it is required to set up an accurate, fixed value of  
U, the on-chip reference may be used. The transistor Qr is  
provided to cancel the VBE of Qu, and is biased by an external  
resistor, R2, as shown in Figure 4. R1 is chosen to set the de-  
sired value of U and consists of a fixed and adjustable resistor.  
(7)  
±W = +U +Z + ±S .  
)(  
(
)
(
)
(
)
This is seen more generally to be the geometric-mean function,  
since both U and Z can be variable; operation is restricted to  
one quadrant. Feedback may also be taken to the U-interface.  
Full details of the operation in these modes is provided in the  
appropriate section of this data sheet.  
Direct Denominator Control  
+V  
14  
VP  
S
A valuable new feature of the AD734 is the provision to replace  
the internal denominator voltage, U, with any value from +10 mV  
to +10 V. This can be used (1) to simply alter the multiplier  
scaling, thus improve accuracy and achieve reduced noise levels  
when operating with small input signals; (2) to implement an  
accurate two-quadrant divider, with a 1000:1 gain range and an  
asymptotic gain-bandwidth product of 200 MHz; (3) to achieve  
certain other special functions, such as AGC or rms.  
AD734  
Iu  
60A  
~
DD 13  
U0  
U1  
Qu  
3
4
Rr  
100k⍀  
ER  
9
V
NC  
NC  
G
Qr  
Ru  
28k⍀  
VN  
8
U2  
5
–V  
S
Figure 2 shows the internal circuitry associated with denomina-  
tor control. Note first that the denominator is actually proportional  
to a current, Iu, having a nominal value of 356 µA for U = 10 V,  
whereas the primary reference is a voltage, generated by a buried-  
Zener circuit and laser-trimmed to have a very low temperature  
coefficient. This voltage is nominally 8 V with a tolerance of  
±10%.  
Figure 3. Low-Accuracy Denominator Control  
Iu  
+V  
VP  
14  
S
AD734  
U0  
U1  
Qu  
3
4
DD 13  
Rr  
100k⍀  
R2  
ER  
9
NOMINALLY  
356A for  
U = 10V  
VP  
14  
Iu  
LINK TO  
DISABLE  
AD734  
Qr  
Ru  
28k⍀  
NOM  
8V  
U2  
R1  
VN  
8
NC  
5
–V  
13  
9
S
DD  
ER  
VN  
Rr  
100k⍀  
3
4
U0  
U1  
Qd  
Qu  
TC  
Figure 4. Connections for a Fixed Denominator  
Rd  
NOM  
22.5k⍀  
Ru  
28k⍀  
Qr  
NOM  
8V  
Table I shows useful values of the external components for set-  
ting up nonstandard denominator values.  
8
U2  
5
NEGATIVE SUPPLY  
Figure 2. Denominator Control Circuitry  
REV. C  
–5–  
AD734  
+15V  
Table I. Component Values for Setting Up Nonstandard  
Denominator Values  
AD734  
1
2
3
4
14  
13  
X1  
VP  
X – INPUT  
؎10V FS  
0.1F  
DD  
NC  
X2  
Denominator  
R1 (Fixed)  
R1 (Variable)  
R2  
(Y – Y )  
(X – X )  
1
2
1
2
W
12  
11  
+ Z  
2
W =  
U0  
U1  
10V  
LOAD  
5 V  
3 V  
2 V  
1 V  
34.8 kΩ  
64.9 kΩ  
86.6 kΩ  
174 kΩ  
20 kΩ  
20 kΩ  
50 kΩ  
100 kΩ  
120 kΩ  
220 kΩ  
300 kΩ  
620 kΩ  
Z1  
L
GROUND  
Z2 10  
Z
2
5
6
U2  
Y1  
Y2  
OPTIONAL  
L
9
8
ER  
VN  
NC  
Y – INPUT  
؎10V FS  
0.1F  
SUMMING INPUT  
±10V FS  
7
–15V  
The denominator can also be current controlled, by grounding  
Pin 3 (U0) and withdrawing a current of Iu from Pin 4 (U1).  
The nominal scaling relationship is U = 28 × Iu, where u is  
expressed in volts and Iu is expressed in milliamps. Note,  
however, that while the linearity of this relationship is very good,  
it is subject to a scale tolerance of ±20%. Note that the common  
mode range on Pins 3 through 5 actually extends from 4 V to  
36 V below VP, so it is not necessary to restrict the connection  
of U0 to ground if it should be desirable to use some other  
voltage.  
Figure 5. Basic Multiplier Circuit  
of 32 Hz. When a tighter control of this frequency is needed, or  
when the HP corner is above about 100 kHz, an external resis-  
tor should be added across the pair of input nodes.  
At least one of the two inputs of any pair must be provided with  
a dc path (usually to ground). The careful selection of ground  
returns is important in realizing the full accuracy of the AD734.  
The Z2 pin will normally be connected to the load ground,  
which may be remote, in some cases. It may also be used as an  
optional summing input (see Equations (3) and (4), above)  
having a nominal FS input of ±10 V and the full 10 MHz  
bandwidth.  
The output ER may also be buffered, re-scaled and used as a  
general-purpose reference voltage. It is generated with respect to  
the negative supply line Pin 8 (VN), but this is acceptable when  
driving one of the signal interfaces. An example is shown in  
Figure 12, where a fixed numerator of 10 V is generated for a  
divider application. There, Y2 is tied to VN but Y1 is 10 V above  
this; therefore the common-mode voltage at this interface is still  
5 V above VN, which satisfies the internal biasing requirements  
(see Specifications table).  
In applications where high absolute accuracy is essential, the  
scaling error caused by the finite resistance of the signal source(s)  
may be troublesome; for example, a 50 source resistance at  
just one input will introduce a gain error of –0.1%; if both the  
X- and Y-inputs are driven from 50 sources, the scaling error  
in the product will be –0.2%. Provided the source resistance(s)  
are known, this gain error can be completely compensated by  
including the appropriate resistance (50 or 100 , respectively,  
in the above cases) between the output W (Pin 12) and the Z1  
feedback input (Pin 11). If Rx is the total source resistance  
associated with the X1 and X2 inputs, and Ry is the total source  
resistance associated with the Y1 and Y2 inputs, and neither Rx  
nor Ry exceeds 1 k, a resistance of Rx+Ry in series with pin  
Z1 will provide the required gain restoration.  
OPERATION AS A MULTIPLIER  
All of the connection schemes used in this section are essentially  
identical to those used for the AD534, with which the AD734 is  
pin-compatible. The only precaution to be noted in this regard  
is that in the AD534, Pins 3, 5, 9, and 13 are not internally  
connected and Pin 4 has a slightly different purpose. In many  
cases, an AD734 can be directly substituted for an AD534 with  
immediate benefits in static accuracy, distortion, feedthrough,  
and speed. Where Pin 4 was used in an AD534 application to  
achieve a reduced denominator voltage, this function can now be  
much more precisely implemented with the AD734 using alter-  
native connections (see Direct Denominator Control, page 5).  
Pins 9 (ER) and 13 (DD) should be left unconnected in this  
application. The U-inputs (Pins 3, 4 and 5) are shown  
connected to ground; they may alternatively be connected to  
VN, if desired. In applications where Pin 2 (X2) happens to be  
driven with a high-amplitude, high-frequency signal, the  
capacitive coupling to the denominator control circuitry via an  
ungrounded Pin 3 can cause high-frequency distortion. However,  
the AD734 can be operated without modification in an AD534  
socket, and these three pins left unconnected, with the above  
Operation from supplies down to ±8 V is possible. The supply  
current is essentially independent of voltage. As is true of all  
high speed circuits, careful power-supply decoupling is impor-  
tant in maintaining stability under all conditions of use. The  
decoupling capacitors should always be connected to the load  
ground, since the load current circulates in these capacitors at  
high frequencies. Note the use of the special symbol (a triangle  
with the letter ‘L’ inside it) to denote the load ground.  
caution noted.  
+15V  
AD734  
0.1F  
1
2
3
4
5
6
7
14  
X1  
X2  
VP  
DD  
X – INPUT  
؎10V FS  
L
Standard Multiplier Connections  
13 NC  
(Y – Y )  
(X – X )  
Figure 5 shows the basic connections for multiplication. The X  
and Y inputs are shown as optionally having their negative  
nodes grounded, but they are fully differential, and in many  
applications the grounded inputs may be reversed (to facilitate  
interfacing with signals of a particular polarity, while achieving  
some desired output polarity) or both may be driven.  
1
1
1
2
1
2
W 12  
I
=
+
U0  
U1  
W
50k⍀  
R
10V  
S
Z1  
R
S
11  
10  
Z2  
U2  
Y1  
Y2  
ER  
9
8
NC  
Y – INPUT  
؎10V FS  
0.1F  
I
؎10mA MAX FS  
W
VN  
؎10V MAXIMUM  
LOAD VOLTAGE  
L
L
–15V  
The AD734 has an input resistance of 50 kΩ ± 20% at the X,  
Y, and Z interfaces, which allows ac-coupling to be achieved  
with moderately good control of the high-pass (HP) corner  
frequency; a capacitor of 0.1 µF provides a HP corner frequency  
Figure 6. Conversion of Output to a Current  
REV. C  
–6–  
AD734  
+15V  
NC  
Current Output  
R2  
1.6k  
AD734  
0.1F  
It may occasionally be desirable to convert the output voltage to  
a current. In correlation applications, for example, multiplica-  
tion is followed by integration; if the output is in the form of a  
current, a simple grounded capacitor can perform this function.  
Figure 6 shows how this can be achieved. The op amp forces  
the voltage across Z1 and Z2, and thus across the resistor RS, to  
be the product XY/U. Note that the input resistance of the  
Z interface is in shunt with RS, which must be calculated  
accordingly.  
1
2
3
4
14  
13  
X1  
VP  
R1  
1.6k⍀  
L
DD  
X2  
R3  
W
12  
11  
U0  
U1  
13k⍀  
E2 cos2ωt/10V  
Esinωt  
Z1  
R4  
4.32k⍀  
Z2 10  
5
6
U2  
Y1  
Y2  
9
8
ER  
VN  
NC  
0.1F  
C
L
7
L
–15V  
The smallest FS current is simply ±10 V/50 k, or ±200 µA,  
with a tolerance of about 20%. To guarantee a 1% conversion  
tolerance without adjustment, RS must be less than 2.5 k. The  
maximum full scale output current should be limited to about  
±10 mA (thus, RS = 1 k). This concept can be applied to all  
connection modes, with the appropriate choice of terminals.  
Figure 7. Frequency Doubler  
OPERATION AS A DIVIDER  
The AD734 supports two methods for performing analog  
division. The first is based on the use of a multiplier in a feed-  
back loop. This is the standard mode recommended for  
multipliers having a fixed scaling voltage, such as the AD534,  
and will be described in this Section. The second uses the  
AD734’s unique capability for externally varying the scaling  
(denominator) voltage directly, and will be described in the  
next section.  
Squaring and Frequency-Doubling  
Squaring of an input signal, E, is achieved simply by connecting  
the X and Y inputs in parallel; the phasing can be chosen to  
produce an output of E2/U or –E2/U as desired. The input may  
have either polarity, but the basic output will either always be  
positive or negative; as for multiplication, the Z2 input may be  
used to add a further signal to the output.  
Feedback Divider Connections  
Figure 8 shows the connections for the standard (AD534)  
divider mode. Feedback from the output, W, is now taken to the  
Y2 (inverting) input, which, provided that the X-input is posi-  
tive, establishes a negative feedback path. Y1 should normally  
be connected to the ground associated with the load circuit, but  
may optionally be used to sum a further signal to the output. If  
desired, the polarity of the Y-input connections can be reversed,  
with W connected to Y1 and Y2 used as the optional summation  
input. In this case, either the polarity of the X-input connections  
must be reversed, or the X-input voltage must be negative.  
When the input is a sine wave, a squarer behaves as a frequency-  
doubler, since  
(Esinwt)2 = E2 (1 – cos2wt)/2  
(8)  
Equation (8) shows a dc term at the output which will vary  
strongly with the amplitude of the input, E. This dc term can be  
avoided using the connection shown in Figure 7, where an  
RC-network is used to generate two signals whose product has  
no dc term. The output is  
+15V  
E
π
E
π
1
10 V  
AD734  
W = 4  
sin wt +  
sin wt −  
0.1F  
(9)  
4
4
2
2
X INPUT  
+0.1V TO  
+10V  
1
2
3
4
14  
13  
X1  
VP  
L
DD  
NC  
NC  
X2  
for w = 1/CR1, which is just  
W = E2(cos2wt)/( 10 V)  
(Z – Z )  
2
1
W
12  
11  
+Y1  
W = 10  
U0  
U1  
(X – X )  
(10)  
1
2
Z1  
Z INPUT  
؎10V FS  
which has no dc component. To restore the output to ±10 V  
when E = 10 V, a feedback attenuator with an approximate ratio  
of 4 is used between W and Z1; this technique can be used  
wherever it is desired to achieve a higher overall gain in the  
transfer function.  
Z2 10  
5
6
U2  
Y1  
Y2  
Y
1
9
8
ER  
VN  
0.1F  
OPTIONAL  
SUMMING  
INPUT  
L
7
L
–15V  
؎10V FS  
In fact, the values of R3 and R4 include additional compensa-  
tion for the effects of the 50 kinput resistance of all three  
interfaces; R2 is included for a similar reason. These resistor  
values should not be altered without careful calculation of the  
consequences; with the values shown, the center frequency f0 is  
100 kHz for C = 1 nF. The amplitude of the output is only a  
weak function of frequency: the output amplitude will be 0.5%  
too low at f = 0.9f0 and f = 1.1f0. The cross-connection is simply  
to produce the cosine output with the sign shown in Equation  
(10); however, the sign in this case will rarely be important.  
Figure 8. Standard (AD534) Divider Connection  
The numerator input, which is differential and can have either  
polarity, is applied to pins Z1 and Z2. As with all dividers based  
on feedback, the bandwidth is directly proportional to the  
denominator, being 10 MHz for X = 10 V and reducing to  
100 kHz for X = 100 mV. This reduction in bandwidth, and the  
increase in output noise (which is inversely proportional to the  
denominator voltage) preclude operation much below a denomi-  
nator of 100 mV. Division using direct control of the denominator  
(Figure 10) does not have these shortcomings.  
REV. C  
–7–  
AD734  
+15V  
This connection scheme may also be viewed as a variable-gain  
element, whose output, in response to a signal at the X input, is  
controllable by both the Y input (for attenuation, using Y less  
than U) and the U input (for amplification, using U less than  
Y). The ac performance is shown in Figure 11; for these results,  
Y was maintained at a constant 10 V. At U = 10 V, the gain is  
unity and the circuit bandwidth is a full 10 MHz. At U = 1 V,  
the gain is 20 dB and the bandwidth is essentially unaltered. At  
U = 100 mV, the gain is 40 dB and the bandwidth is 2 MHz.  
Finally, at U = 10 mV, the gain is 60 dB and the bandwidth is  
250 kHz, corresponding to a 250 MHz gain-bandwidth product.  
AD734  
0.1F  
1
2
14  
VP  
X1  
X2  
L
DD  
13 NC  
12  
W =  
(10V) (Z – Z ) + S  
2 1  
D
W
3
4
5
6
7
U0  
U1  
Z1  
Z INPUT  
+10mV TO  
+10V  
11  
S
OPTIONAL  
SUMMING  
INPUT  
L
Z2 10  
U2  
Y1  
Y2  
ER  
VN  
9
8
NC  
؎10V FS  
0.1F  
L
–15V  
Figure 9. Connection for Square Rooting  
Connections for Square-Rooting  
70  
U = 10mV  
60  
The AD734 may be used to generate an output proportional to  
the square-root of an input using the connections shown in  
Figure 9. Feedback is now via both the X and Y inputs, and is  
always negative because of the reversed-polarity between these  
two inputs. The Z input must have the polarity shown, but  
because it is applied to a differential port, either polarity of  
input can be accepted with reversal of Z1 and Z2, if necessary.  
The diode D, which can be any small-signal type (1N4148  
being suitable) is included to prevent a latching condition which  
could occur if the input momentarily was of the incorrect  
polarity of the input, the output will be always negative.  
50  
U = 100mV  
40  
30  
U = 1V  
20  
10  
U = 10V  
0
Note that the loading on the output side of the diode will be  
provided by the 25 kof input resistance at X1 and Y2, and by  
the user’s load. In high speed applications it may be beneficial  
to include further loading at the output (to 1 kminimum) to  
speed up response time. As in previous applications, a further  
signal, shown here as S, may be summed to the output; if this  
option is not used, this node should be connected to the load  
ground.  
10k  
100k  
FREQUENCY – Hz  
1M  
10M  
Figure 11. Three-Variable Multiplier/Divider Performance  
The 2 Mresistor is included to improve the accuracy of the  
gain for small denominator voltages. At high gains, the X input  
offset voltage can cause a significant output offset voltage. To  
eliminate this problem, a low-pass feedback path can be used  
from W to X2; see Figure 13 for details.  
DIVISION BY DIRECT DENOMINATOR CONTROL  
The AD734 may be used as an analog divider by directly vary-  
ing the denominator voltage. In addition to providing much  
higher accuracy and bandwidth, this mode also provides greater  
flexibility, because all inputs remain available. Figure 10 shows  
the connections for the general case of a three-input multiplier  
divider, providing the function  
Where a numerator of 10 V is needed, to implement a two-  
quadrant divider with fixed scaling, the connections shown in  
Figure 12 may be used. The reference voltage output appearing  
between Pin 9 (ER) and Pin 8 (VN) is amplified and buffered  
by the second op amp, to impose 10 V across the Y1/Y2 input.  
Note that Y2 is connected to the negative supply in this applica-  
tion. This is permissible because the common-mode voltage is  
still high enough to meet the internal requirements. The transfer  
function is  
X X Y Y  
(
2 )(  
)
+ Z2,  
1
1
2
2
W =  
(11)  
U U  
(
)
1
where the X, Y, and Z signals may all be positive or negative,  
but the difference U = U1 – U2 must be positive and in the  
range +10 mV to +10 V. If a negative denominator voltage must  
be used, simply ground the noninverting input of the op amp.  
As previously noted, the X input must have a magnitude of less  
than 1.25U.  
X1 X2  
U1 U2  
W = 10 V  
+ Z2.  
(12)  
The ac performance of this circuit remains as shown in Figure 11.  
+15V  
AD734  
1
2
3
4
5
6
7
14  
13  
12  
11  
10  
9
X1  
X2  
U0  
U1  
U2  
VP  
DD  
+15V  
X – INPUT  
U
AD734  
0.1F  
(X – X ) 10V  
1
2
1
2
3
4
5
6
7
14  
13  
12  
11  
W =  
+ Z  
2
X1  
X2  
VP  
DD  
1
U –U  
1
X – INPUT  
2
0.1F  
W =  
W
Z1  
(Y – Y )  
(X – X )  
1
2
1
2
U – INPUT  
+ Z  
LOAD  
GROUND  
2M⍀  
2
U
1
L
U
– U  
W
1
2
U0  
U1  
LOAD  
GROUND  
Z2  
U
Z
2
U – INPUT  
2M⍀  
Z1  
2
L
OPTIONAL  
SUMMING  
INPUT  
L
ER  
VN  
Y1  
Y2  
U
2
0.1F  
Z2 10  
Z
2
U2  
Y1  
Y2  
OPTIONAL  
8
L
ER  
VN  
9
8
NC  
؎10V FS  
SUMMING INPUT  
0.1F  
Y – INPUT  
100k⍀  
SCALE  
ADJUST  
؎10V FS  
200k⍀  
–15V  
–15V  
OP AMP = AD712 DUAL  
Figure 10. Three-Variable Multiplier/Divider Using Direct  
Denominator Control  
Figure 12. Two-Quadrant Divider with Fixed 10 V Scaling  
REV. C  
–8–  
AD734  
The output amplitude tracks EC over the range +1 V to slightly  
more than +10 V.  
A PRECISION AGC LOOP  
The variable denominator of the AD734 and its high gain-  
bandwidth product make it an excellent choice for precise  
automatic gain control (AGC) applications. Figure 13 shows a  
suggested method. The input signal, EIN, which may have a  
peak amplitude of from 10 mV to 10 V at any frequency from  
100 Hz to 10 MHz, is applied to the X input, and a fixed posi-  
tive voltage EC to the Y input. Op amp A2 and capacitor C2  
form an integrator having a current summing node at its invert-  
ing input. (The AD712 dual op amp is a suitable choice for this  
application.) In the absence of an input, the current in D2 and  
R2 causes the integrator output to ramp negative, clamped by  
diode D3, which is included to reduce the time required for the  
loop to establish a stable, calibrated, output level once the  
circuit has received an input signal. With no input to the  
denominator (U0 and U2), the gain of the AD734 is very high  
(about 70 dB), and thus even a small input causes a substantial  
output.  
+2  
+1  
100kHZ  
0
–1  
1MHZ  
100HZ  
–2  
10m  
100m  
1
10  
INPUT AMPLITUDE – Volts  
Figure 14. AGC Amplifier Output Error vs. Input Voltage  
R3  
1M⍀  
C1  
A1  
1F  
+15V  
WIDEBAND RMS-DC CONVERTER  
AD734  
VP  
USING U INTERFACE  
The AD734 is well suited to such applications as implicit RMS-  
DC conversion, where the AD734 implements the function  
14  
13  
12  
11  
10  
9
X1  
X2  
U0  
U1  
U2  
Y1  
Y2  
1
2
E
IN  
0.1F  
D1  
DD  
W
1N914  
E
OUT  
3
4
5
6
D3  
1N914  
C2  
1F  
C1  
1F  
NC  
Z1  
Z2  
ER  
A2  
2
L
avg VIN  
[
]
(13)  
VRMS  
=
0.1F  
L
E
VRMS  
C
+1V TO  
+10V  
D2  
1N914  
7
8
VN  
using its direct divide mode. Figure 15 shows the circuit.  
–15V  
OP AMP = AD712 DUAL  
+15V  
R2  
1M⍀  
R1  
1M⍀  
0.1F  
AD734  
X1  
V
1
2
14  
13  
12  
IN  
VP  
Figure 13. Precision AGC Loop  
1/2  
AD708  
L
U2b  
R1  
DD  
X2  
3.32k⍀  
L
Diode D1 and C1 form a peak detector, which rectifies the out-  
put and causes the integrator to ramp positive. When the  
current in R1 balances the current in R2, the integrator output  
holds the denominator output at a constant value. This occurs  
when there is sufficient gain to raise the amplitude of EIN to that  
required to establish an output amplitude of EC over the range  
of +1 V to +10 V. The X input of the AD734, which has finite  
offset voltage, could be troublesome at the output at high gains.  
The output offset is reduced to that of the X input (one or two  
millivolts) by the offset loop comprising R3, C3, and buffer A1.  
The low pass corner frequency of 0.16 Hz is transformed to a  
high-pass corner that is multiplied by the gain (for example,  
160 Hz at a gain of 1000).  
V
3
4
5
6
7
W
O
U0  
U1  
U2  
1/2  
AD708  
U1  
U2a  
Z1 11  
C1  
47F  
C2  
1F  
Z2  
10  
9
L
2
IN  
V
=
V
L
L
O
L
ER  
VN  
Y1  
Y2  
0.1F  
8
L
–15V  
Figure 15. A 2-Chip, Wideband RMS-DC Converter  
In this application, the AD734 and an AD708 dual op amp  
serve as a 2-chip RMS-DC converter with a 10 MHz bandwidth.  
Figure 16 shows the circuit’s performance for square-, sine-,  
and triangle-wave inputs. The circuit accepts signals as high as  
10 V p-p with a crest factor of 1 or 1 V p-p with a crest factor of  
10. The circuit’s response is flat to 10 MHz with an input of  
10 V, flat to almost 5 MHz for an input of 1 V, and to almost  
1 MHz for inputs of 100 mV. For accurate measurements of  
input levels below 100 mV, the AD734’s output offset (Z inter-  
face) voltage, which contributes a dc error, must be trimmed out.  
In applications not requiring operation down to low frequencies,  
amplifier A1 can he eliminated, but the AD734’s input  
resistance of 50 kbetween X1 and X2 will reduce the time  
constant and increase the input offset. Using a non-polar 20 µF  
tantalum capacitor for C1 will result in the same unity-gain  
high-pass corner; in this case, the offset gain increases to 20, still  
very acceptable.  
In Figure 15’s circuit, the AD734 squares the input signal, and  
its output (VIN2) is averaged by a low-pass filter that consists of  
R1 and C1 and has a corner frequency of 1 Hz. Because of the  
implicit feedback loop, this value is both the output value, VRMS  
and the denominator in Equation (13). U2a and U2b, an  
AD708 dual dc precision op amp, serve as unity-gain buffers,  
supplying both the output voltage and driving the U interface.  
Figure 14 shows the error in the output for sinusoidal inputs at  
100 Hz, 100 kHz, and 1 MHz, with EC set to +10 V. The out-  
put error for any frequency between 300 Hz and 300 kHz is  
similar to that for 100 kHz. At low signal frequencies and low  
input amplitudes, the dynamics of the control loop determine  
the gain error and distortion; at high frequencies, the 200 MHz  
gain-bandwidth product of the AD734 limit the available gain.  
,
REV. C  
–9–  
AD734  
100  
If the two X1 inputs are at frequencies f1 and f2 and the  
frequency at the Y1 input is f0, then the two-tone third-order  
intermodulation products should appear at frequencies 2f1 – f2 ±  
f0 and 2f2 – f1 ± f0. Figures 18 and 19 show the output spectra of  
the AD734 with f1 = 9.95 MHz, f2 = 10.05 MHz, and f0 =  
9.00 MHz for a signal level of f1 & f2 of 6 dBm and f0 of  
+24 dBm in Figure 18 and f1 & f2 of 0 dBm and f0 of +24 dBm  
in Figure 19. This performance is without external trimming of  
the AD734’s X and Y input-offset voltages.  
10  
1
100m  
10m  
1m  
The possible Two Tone Intermodulation Products are at 2 ×  
9.95 MHz – 10.05 MHz ± 9.00 MHz and 2 × 10.05 –  
9.95 MHz ± 9.00 MHz; of these only the third-order products  
at 0.850 MHz and 1.150 MHz are within the 10 MHz band-  
width of the AD734; the desired output signals are at  
0.950 MHz and 1.050 MHz. Note that the difference (Figure  
18) between the desired outputs and third-order products is  
approximately 78 dB, which corresponds to a computed  
third-order intercept point of +46 dBm.  
SQUARE WAVE  
SINE WAVE  
TRI-WAVE  
100␮  
10k  
100k  
1M  
10M  
INPUT FREQUENCY – Hz  
Figure 16. RMS-DC Converter Performance  
LOW DISTORTION MIXER  
The AD734’s low noise and distortion make it especially  
suitable for use as a mixer, modulator, or demodulator.  
Although the AD734’s –3 dB bandwidth is typically 10 MHz  
and is established by the output amplifier, the bandwidth of its  
X and Y interfaces and the multiplier core are typically in excess  
of 40 MHz. Thus, provided that the desired output signal is less  
than 10 MHz, as would typically be the case in demodulation,  
the AD734 can be used with both its X and Y input signals as  
high as 40 MHz. One test of mixer performance is to linearly  
combine two closely spaced, equal-amplitude sinusoidal signals  
and then mix them with a third signal to determine the mixer’s  
2-tone Third-Order Intermodulation Products.  
+15V  
AD734  
HP3326A  
COMBINE  
A + B  
0.1F  
14  
13  
12  
11  
10  
9
1
2
X1  
VP  
AD707  
DD  
X2  
HP3585A  
WITH 10X PROBE  
dBm REF TO 50⍀  
DATEL  
DVC-8500  
Figure 18. AD734 Third-Order Intermodulation Performance  
for f1 = 9.95 MHz, f2 = 10.05 MHz, and f0 = 9.00 MHz and for  
Signal Levels of f1 & f2 of 6 dBm and f0 of +24 dBm. All Dis-  
played Signal Levels Are Attenuated 20 dB by the 10X Probe  
Used to Measure the Mixer’s Output  
3
4
W
U0  
U1  
2k⍀  
Z1  
5
6
7
Z2  
U2  
Y1  
Y2  
HP3326A  
HIGH VOLTAGE  
OPTION  
ER  
0.1F  
8
VN  
–15V  
Figure 17. AD734 Mixer Test Circuit  
Figure 17 shows a test circuit for measuring the AD734’s perfor-  
mance in this regard. In this test, two signals, at 10.05 MHz and  
9.95 MHz are summed and applied to the AD734’s X interface.  
A second 9 MHz signal is applied to the AD734’s Y interface.  
The voltage at the U interface is set to 2 V to use the full  
dynamic range of the AD734. That is, by connecting the W and  
Z1 pins together, grounding the Y2 and X2 pins, and setting  
U = 2 V, the overall transfer function is  
X1Y1  
2V  
W =  
(14)  
and W can be as high as 20 V p-p when X1 = 2 V p-p and Y1 =  
10 V p-p. The 2 V p-p signal level corresponds to +10 dBm into  
a 50 input termination resistor connected from X1 or Y1 to  
ground.  
Figure 19. AD734 Third-Order Intermodulation Performance  
for f1 = 9.95 MHz, f2 = 10.05 MHz, and f0 = 9.00 MHz and for  
Signal Levels of f1 & f2 of 0 dBm and f0 of +24 dBm. All Dis-  
played Signal Levels Are Attenuated 20 dB by the 10X Probe  
Used to Measure the Mixer’s Output  
REV. C  
–10–  
Typical Characteristics–  
AD734  
V
= ؎15V  
S
V
R
C
= ؎15V  
X = 1.4V RMS  
Y = 10V  
V
R
C
= ؎15V  
S
S
0.06  
0.3  
0.2  
= 2k⍀  
= 2k⍀  
LOAD  
LOAD  
LOAD  
LOAD  
R
= 500⍀  
LOAD  
= 20pF  
= 20pF  
0.04  
0.02  
C
= 20pF  
LOAD  
0.1  
0
0.1  
0
0.05  
–0.02  
–0.1  
–0.2  
0
–0.05  
–0.1  
–0.04  
–0.06  
–0.3  
–0.4  
–0.08  
100k  
1M  
FREQUENCY – Hz  
10M  
–2V  
0
2V  
–2V  
0
SIGNAL AMPLITUDE  
2V  
SIGNAL AMPLITUDE  
Figure 20. Differential Gain at  
Figure 21. Differential Phase at  
Figure 22. Gain Flatness, 300 kHz to  
3.58 MHz and RL = 2 k  
3.58 MHz and RL = 2 kΩ  
10 MHz, RL = 500 Ω  
0
100  
100  
80  
INPUT SIGNAL = 7V RMS  
–40  
Y INPUT, X = 10V  
80  
Y INPUT, X NULLED  
–60  
60  
60  
VN  
X INPUT, Y NULLED  
–80  
X INPUT, Y = 10V  
40  
VP  
40  
COMMON-MODE  
20  
–100  
20  
0
SIGNAL = 7V RMS  
0
1k  
10k  
100k  
1M  
10M  
1k  
10k  
100k  
1M  
10M  
1k  
10k  
100k  
1M  
10M  
FREQUENCY – Hz  
FREQUENCY – Hz  
FREQUENCY – Hz  
Figure 25. Feedthrough vs. Frequency  
Figure 23. CMRR vs. Frequency  
Figure 24. PSRR vs. Frequency  
0
0
0
TEST INPUT = 1V RMS  
U = 2V  
OTHER INPUT = 2V DC  
TEST INPUT = 7V RMS  
FREQUENCY = 1MHz  
–20  
–20  
–20  
–40  
–60  
–80  
OTHER INPUT = 10V DC  
= Ն2k⍀  
VP = 15V  
R
VN = –15V  
LOAD  
R
= 2k⍀  
LOAD  
–40  
–40  
–60  
X INPUT. Y = 10V DC  
X INPUT  
X INPUT  
–60  
Y INPUT  
Y INPUT  
Y INPUT. X = 10V DC  
–80  
–80  
–100  
1k  
10k  
100k  
FREQUENCY – Hz  
1M  
10M  
1k  
10k  
100k  
FREQUENCY – Hz  
1M  
10M  
–10dBm  
10dBm  
707mV RMS  
30dBm  
7V RMS  
70.7mV RMS  
SIGNAL LEVEL  
Figure 26. THD vs. Frequency,  
U = 2 V  
Figure 27. THD vs. Frequency,  
U = 10 V  
Figure 28. THD vs. Signal Level,  
f = 1 MHz  
REV. C  
–11–  
AD734–Typical Characteristics  
5
V
= ؎15V  
S
4
X = 1.4V rms  
Y = 10V  
R
0
3
= 500⍀  
LOAD  
–30  
–60  
C
= 20pF, 47pF,  
100pF  
2
1
LOAD  
INCREASING  
C
LOAD  
V
= ؎15V  
S
X = 1.4V rms  
Y = 10V  
–90  
0
–120  
–1  
R
= 500⍀  
LOAD  
LOAD  
C
= 20pF, 47pF, 100pF  
–150  
–180  
–2  
–3  
INCREASING  
–4  
–5  
C
LOAD  
100k  
1M  
FREQUENCY – Hz  
10M  
100k  
1M  
10M  
Figure 31. Pulse Response vs.  
LOAD, CLOAD = 0 pF, 47 pF,  
100 pF, 200 pF  
FREQUENCY – Hz  
C
Figure 30. Phase vs. Frequency  
vs. CLOAD  
Figure 29. Gain vs. Frequency vs.  
CLOAD  
0
20  
15  
10  
–10  
U = 5V  
U = 2V  
U = 10V  
U = 1V  
5
0
–20  
–5  
X
Y
FREQ =  
FREQ –1MHz  
1
1
–10  
–15  
–20  
(E.G., Y – X = 1MHz  
FOR ALL CURVES)  
1
1
–30  
10 20 30 40 50 60 70 80 90 100  
Y
FREQUENCY – MHz  
1
8
9
10 11 12 13 14 15 16 17 18  
SUPPLY VOLTAGE – ؎V  
Figure 32. Output Swing vs.SSupply  
Voltage  
Figure 33. Output Amplitude vs. Input  
Frequency, When Used as Demodulator  
20  
15  
10  
5
8
60  
INPUT OFFSET VOLTAGE  
DRIFT WILL TYPICALLY BE  
WITHIN SHADED AREA  
INPUT OFFSET VOLTAGE  
DRIFT WILL TYPICALLY BE  
WITHIN SHADED AREA  
INPUT OFFSET VOLTAGE  
DRIFT WILL TYPICALLY BE  
WITHIN SHADED AREA  
6
4
2
40  
20  
0
0
–5  
0
–2  
–4  
–6  
–20  
–40  
–60  
–10  
–15  
–55 –35 –15  
5
25 45 65 85 105 125  
–55 –35 –15  
5
25 45 65 85 105 125  
–55 –35 –15  
5
25 45 65 85 105 125  
TEMPERATURE – ؇C  
TEMPERATURE – ؇C  
TEMPERATURE – ؇C  
Figure 34. VOS Drift, X Input  
Figure 36. VOS Drift, Y Input  
Figure 35. VOS Drift, Z Input  
OUTLINE DIMENSIONS  
Dimensions shown in inches and (mm).  
14-Lead Plastic DIP (N) Package  
14-Lead Ceramic DIP (Q) Package  
14  
1
8
0.280 (7.11)  
0.240 (6.10)  
PIN 1  
7
0.325 (8.25)  
0.300 (7.62)  
0.795 (20.19)  
0.725 (18.42)  
0.060 (1.52)  
0.015 (0.38)  
0.195 (4.95)  
0.115 (2.93)  
0.210  
(5.33)  
MAX  
0.130  
(3.30)  
MIN  
0.015 (0.381)  
0.008 (0.204)  
0.160 (4.06)  
0.115 (2.93)  
SEATING  
PLANE  
0.022 (0.558)  
0.014 (0.356)  
0.070 (1.77)  
0.045 (1.15)  
0.100  
(2.54)  
BSC  
REV. C  
–12–  

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