Data Sheet AD834
Rev. F | Page 9 of 20
00894-009
8 7 6 5
1 2 3 4
X2 X1 +V
S
W1
NOTES
1. R1, R2 SHOULD BE PRECISION TYPE
RESIS
TOR (±0.1%).
2.
ABSOLUTE VALUE ERRORS OF R1, R2
CAUSE
A SMALL FACTOR ERROR.
3. R1, R2 MISM
ATCHES ARE EXPRESSED
AS LINEARITY ERRORS.
4. V
OUT
= I
W1
R1 – U
W2
R2
(IF R1 = R2, V
OUT
= >I
W
R1).
Y1 Y2
–V
S
W2
AD834
–15V
+15V
AD707
0.1µF
0.1µF
0.1µF
0.1µF
0.1µF
0.1µF
–15V
+15V
AD707
+
+5V
–5V
V
OUT
X
Y
I
W1
1kΩ
1kΩ
1kΩ
1kΩ
A1
A2
I
W2
Figure 9. Low Frequency Test Circuit
00894-109
Figure 10. Example Layout for SOIC
AD834 Data Sheet
Rev. F | Page 10 of 20
EXPLANATION OF TYPICAL PERFORMANCE
CHARACTERISTICS AND TEST CIRCUITS
Figure 4 is a plot of the mean-square output vs. frequency for
the test circuit of Figure 8. Note that the rising response is due
to package resonances.
For frequencies above 1 MHz, ac feedthrough is dominated by
static nonlinearities in the transfer function and the finite offset
voltages. The offset voltages cause a small fraction of the funda-
mental to appear at the output, and can be nulled out (see
Figure 5).
THD data represented in Figure 6 is dominated by the second
harmonic, and is generated with 0 dBm input on the ac input
and 1 V on the dc input. For a given amplitude on the ac input,
THD is relatively insensitive to changes in the dc input ampli-
tude. Varying the ac input amplitude while maintaining a
constant dc input amplitude affects THD performance.
The squarer configuration shown in Figure 8 is used to determine
wideband performance because it eliminates the need for (and
the response uncertainties of) a wideband measurement device
at the output. The wideband output of a squarer configuration
is a fluctuating current at twice the input frequency with a mean
value proportional to the square of the input amplitude.
By placing the capacitors, C3/C5 and C4/C6, across the load
resistors, R1 and R2, a simple low-pass filter is formed, and the
mean-square value is extracted. The mean-square response can
be measured using a DVM connected across R1 and R2.
Care should be taken when laying out the board. When using
the DIP package, mount the IC socket on a ground plane with a
clear area in the rectangle formed by the pins. This is important
because significant transformer action can arise if the pins pass
through individual holes in the board; improperly constructed test
jigs have caused oscillation at 1.3 GHz.
Data Sheet AD834
Rev. F | Page 11 of 20
THEORY OF OPERATION
Figure 11 is a functional equivalent of the AD834. There are three
differential signal interfaces: the two voltage inputs (X = X1
X2 and Y = Y1 Y2), and the current output (W) which flows
in the direction shown in Figure 11 when X and Y are positive.
The outputs (W1 and W2) each have a standing current of
typically 8.5 mA.
00894-010
X-DISTORTION
CANCELLATION
AD834
MULTIPLIER CORE
CURRENT
AMPLIFIER
(W)
±4mA
FS
X2 X1 +V
S
W1
Y1
V-I
V-I
Y2 –V
S
W2
8.5mA
8.5mA
8
7
5
6
1
2
3
4
Y-DISTORTION
CANCELLATION
Figure 11. Functional Block Diagram
The input voltages are first converted to differential currents
that drive the translinear core. The equivalent resistance of the
voltage-to-current (V-I) converters is about 285 Ω, which results
in low input related noise and drift. However, the low full-scale
input voltage results in relatively high nonlinearity in the V-I
converters. This is significantly reduced by the use of distortion
cancellation circuits, which operate by Kelvin sensing the voltages
generated in the corean important feature of the AD834.
The current mode output of the core is amplified by a special
cascode stage that provides a current gain of nominally × 1.6,
trimmed during manufacturing to set up the full-scale output
current of ±4 mA. This output appears at a pair of open collec-
tors that must be supplied with a voltage slightly above the
voltage on Pin 6. As shown in Figure 12, this can be arranged
by inserting a resistor in series with the supply to Pin 6 and
taking the load resistors to the full supply. With R3 = 60 Ω, the
voltage drop across it is about 600 mV. Using two 50load
resistors, the full-scale differential output voltage is ±400 mV.
For best performance, the voltage on the output open-collectors
(Pin 4 and Pin 5) must be higher than the voltage on Pin 6 by
about 200 mV, as shown in Figure 12.
The full bandwidth potential of the AD834 can be realized only
when very careful attention is paid to grounding and decoupling.
The device must be mounted close to a high quality ground
plane and all lead lengths must be extremely short, in keeping
with UHF circuit layout practice. In fact, the AD834 shows
useful response to well beyond 1 GHz, and the actual upper
frequency in a typical application is usually determined by the
care with which the layout is affected. Note that R4 (in series
with the −V
S
supply) carries about 30 mA and thus introduces a
voltage drop of about 150 mV. It is made large enough to reduce
the Q of the resonant circuit formed by the supply lead and the
decoupling capacitor. Slightly larger values can be used, particu-
larly when using higher supply voltages. Alternatively, lossy RF
chokes or ferrite beads on the supply leads may be used.
For best performance, use termination resistors at the inputs, as
shown in Figure 12. Note that although the resistive component
of the input impedance is quite high (about 25 kΩ), the input
bias current of typically 45 μA can generate significant offset
voltages if not compensated. For example, with a source and
termination resistance of 50 Ω (net source of 25 Ω) the offset is
25 Ω × 45 μA = 1.125 m V. The offset can be almost fully cancelled
by including (in this example) another 25 Ω resistor in series with
the unused input. (In Figure 12, a 25 Ω resistor would be added
from X1 to GND and Y2 to GND.) To minimize crosstalk, ground
the input pins closest to the output (X1 and Y2); the effect is
merely to reverse the phase of the X input and thus alter the
polarity of the output.
00894-011
8 7 6 5
1 2 3 4
X2 X1 +V
S
W1
Y1 Y2
–V
S
W2
AD834
X-INPUT
±1V FS
Y-INPUT
±1V FS
TERMINATION
RESISTOR
TERMINATION
RESISTOR
R3
62Ω
R4
4.7Ω
+5V
–5V
W OUTPUT
±400mV FS
R1
49.9Ω
R1
49.9Ω
1µF
CERAMIC
1µF
CERAMIC
Figure 12. Basic Connections for Wideband Operation
TRANSFER FUNCTION
The Output Current W is the linear product of input voltages (X
and Y) divided by (1 V)
2
and multiplied by the scaling current of
4 mA:
( )
mA4
V1
2
XY
W
=
With the understanding that the inputs are specified in volts,
the following simplified expression can be used:
W = (XY)4 mA
Alternatively, the full transfer function can be written as
Ω250
1
V1
×=
XY
W
When both inputs are driven to their clipping level of about
1.3 V, the peak output current is roughly doubled to ±8 mA,
but distortion levels become very high.

AD834JRZ

Mfr. #:
Manufacturer:
Description:
Multipliers / Dividers IC 500 MHz Four-Quadrant
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