AD734
Rev. E | Page 9 of 20
SUPPLY VOLTAGE (±V
S
)
OUTPUT SWING (V)
20
–20
–15
–10
–5
15
0
5
10
89 181716151413121110
00827-034
Figure 16. Output Swing vs. Supply Voltage
Y
1
FREQUENCY (MHz)
OUTPUT AMPLITUDE (dB)
0
–30
–10
–20
10 20 10090807060504030
00827-035
X
1
FREQ =
Y
1
FREQ –1MHz
(FOR EXAMPLE,
Y
1
– X
1
= 1MHz
FOR ALL CURVES)
U = 1V
U = 2V
U = 5V
U = 10V
Figure 17. Output Amplitude vs. Input Frequency, When Used as
Demodulator
TEMPERATURE (°C)
DEVI
A
TION OF INPUT OFFSET VOLTAGE (mV)
20
–15
10
5
0
15
–5
–10
–55 –35 125105856545255–15
00827-036
INPUT OFFSET VOLTAGE
DRIFT WILL TYPICALLY BE
WITHIN SHADED AREA
Figure 18. V
OS
Drift, X Input
TEMPERATURE (°C)
DEVI
A
TION OF INPUT OFFSET VOLTAGE (mV)
60
20
0
–20
40
–40
–60
–55 –35 105 125856545255–15
00827-037
INPUT OFFSET VOLTAGE
DRIFT WILL TYPICALLY BE
WITHIN SHADED AREA
Figure 19. V
OS
Drift, Z Input
TEMPERATURE (°C)
DEVI
A
TION OF INPUT OFFSET VOLTAGE (mV)
8
–6
4
2
0
6
–2
–4
–55 –35 125105856545255–15
00827-038
INPUT OFFSET VOLTAGE
DRIFT WILL TYPICALLY BE
WITHIN SHADED AREA
Figure 20. V
OS
Drift, Y Input
AD734
Rev. E | Page 10 of 20
FUNCTIONAL DESCRIPTION
The AD734 embodies more than two decades of experience in
the design and manufacture of analog multipliers to provide:
A new output amplifier design with more than 20 times the
slew rate of the AD534 (450 V/μs vs. 20 V/μs) for a full
power (20 V p-p) bandwidth of 10 MHz.
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.
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.
Very clean transient response, achieved through the use of
a novel input stage design and wideband output amplifier,
which also ensure that distortion remains low even at high
frequencies.
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.
Figure 3 shows the lead configuration of the 14-lead PDIP and
CERDIP packages.
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 in the Direct Denominator Control
section. Internal signals are in the form of currents, but the
function of the AD734 can be understood using voltages
throughout, as shown in Figure 1.
The AD734 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 = X
1
− X
2
, Y = Y
1
− Y
2
, and Z = Z
1
− Z
2
, 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.
The bipolar input signals X and Y are multiplied in a translinear
core of novel design to generate the product XY/U. The denomina-
tor voltage, U, is internally set to an accurate, temperature-stable
value of 10 V, derived from a buried-Zener reference. An uncali-
brated 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 denominator, U, can
be disabled, by connecting the denominator disable Pin 13
(DD) to the positive supply pin (VP); the denominator can then
be replaced by a fixed or variable external voltage ranging from
10 mV to more than 10 V.
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, depending
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.
Each input pair (X1 and X2, Y1 and Y2, Z1 and Z2) has a
differential input resistance of 50 kΩ; this is formed by actual
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.
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
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.
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.
The full-scale output of ±10 V can be delivered to a load resistance
of 1 kΩ (although the specifications apply to the standard multi-
plier load condition of 2 kΩ). 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 output amplifier ensures
that the bandwidth of 10 MHz can be maintained up to the full
output of 20 V p-p. Operation at reduced supply voltages is
possible, down to ±8 V, with reduced signal levels.
AVAILABLE TRANSFER FUNCTIONS
The uncommitted (open-loop) transfer function of the AD734 is
(
)
(
)
(
=
21
2121
O
ZZ
U
YYXX
AW
)
(1)
where A
O
is the open-loop gain of the output op amp, typically
72 dB. When a negative feedback path is provided, the circuit
forces the quantity inside the brackets essentially to zero,
resulting in the equation
(X
1
X
2
)(Y
1
Y
2
) = U (Z
1
Z
2
) (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 the input to be connected to the op amp
output is not specified.
AD734
Rev. E | Page 11 of 20
Most of the functions of the AD734 (including division, unlike
the AD534 in this respect) are realized with Z1 connected to W.
Therefore, substituting W in place of Z
1
in Equation 2 results in
an output.
2
2121
))((
Z
U
YYXX
W +
=
(3)
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. The allowable polarities can be
shown in the following shorthand form:
Z
U
YX
W ±+
+
±±
=±
)(
))((
)(
(4)
In the recommended direct divider mode, the Y input is set to a
fixed voltage (typically 10 V) and U is varied directly; it can 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 AD734
can be operated using the standard (AD534) divider connections
(see Figure 27), when the negative feedback path is established
via the Y2 input. Substituting W for Y
2
in Equation 2,
(
)
()
1
21
12
Y
XX
ZZ
UW +
= (5)
In this case, note that the variable X is now the denominator,
and the previous restriction (X/U ≤ 1.25) on the magnitude of
the X input does not apply. However, X must be positive for the
feedback polarity to be correct. Y
1
can be used for summing
purposes or connected to the load ground if not needed. The
shorthand form in this case is
)(
)(
)(
)()( Y
X
Z
UW ±+
+
±
+=±
(6)
In some cases, feedback can be connected to two of the available
inputs. This is true for the square-rooting connections (see
Figure 28), where W is connected to both X1 and Y2. Set X
1
=
W and Y
2
= W in Equation 2, and anticipating the possibility of
again providing a summing input, set X
2
= S and Y
1
= S, so that,
in shorthand form,
)())(()( SZUW ±+++=±
(7)
This is seen more generally to be the geometric-mean function,
because both U and Z can be variable; operation is restricted to
one quadrant. Feedback can also be taken to the U interface.
Full details of the operation in these modes is provided in the
Wideband RMS-to-DC Converter Using U Interface section.
DIRECT DENOMINATOR CONTROL
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
To simply alter the multiplier scaling, thus improve accu-
racy and achieve reduced noise levels when operating with
small input signals.
To implement an accurate two-quadrant divider, with a
1000:1 gain range and an asymptotic gain-bandwidth
product of 200 MHz.
To achieve certain other special functions, such as
AGC or rms.
Figure 21 shows the internal circuitry associated with
denominator 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 ha
very low temperature coefficient. This voltage is nominally 8
with a tolerance of ±10%
,
ve a
V
.
TC
4
3
5
14
9
13
8
U0
Iu
Qu
Qr
Ru
28k
Rr
100k
Rd
NOM
22.5k
Qd
VP
VN
LINK TO
DISABLE
DD
ER
U1
U2
AD734
NOMINALLY
356µA for
U = 10V
NOM
8V
NEGATIVE SUPPLY
00827-004
+
Figure 21. Denominator Control Circuitry
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 denomina-
tor, and their associated control pins, U0, U1, and U2, are
normally grounded. The reference voltage is also made
available, via the 100 kΩ resistor, Rr, at Pin 9 (ER).
When the control pin, DD (denominator disable), is connected
to VP, the internal source of Iu is shut off, and the collector
current 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 Pin U1 and
Pin U2). Note that this trimming only sets up the correct
internal ratio; the absolute value of Ru (nominally 28 kΩ) has a
tolerance of ±20%. Also, the alpha of Qu (typically 0.995), which
may be seen as a source of scaling error, is canceled by the alpha of
other transistors in the complete circuit.
In the simplest scheme (see Figure 22), an externally provided
control voltage, V
G
, is applied directly to U0 and U2 and the
resulting voltage across Ru is therefore reduced by one V
BE
. For
example, when V
G
= 2 V, the actual value of U is about 1.3 V.

AD734ANZ

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Description:
Multipliers / Dividers 10MHz 4-Quadrant
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