AD8114/AD8115 Data Sheet
Rev. C | Page 22 of 25
The power supplies, grounds, and other signal return paths of a
multichannel system are generally shared by the various channels.
When a current from one channel flows in one of these paths, a
voltage that is developed across the impedance becomes an input
crosstalk signal for other channels that share the common
impedance.
All these sources of crosstalk are vector quantities, so the
magnitudes cannot simply be added together to obtain the
total crosstalk. In fact, there are conditions where driving
additional circuits in parallel in a given configuration can
actually reduce the crosstalk.
Areas of Crosstalk
For a practical AD8114/AD8115 circuit, it is required that the
device be mounted to some sort of circuit board to connect it
to the power supplies and the measurement equipment. This
requirement, however, raises the issue that the crosstalk of a
system is a combination of the intrinsic crosstalk of the devices
in addition to the circuit board to which they are mounted. It is
important to try to separate these two areas of crosstalk when
attempting to minimize its effect.
In addition, crosstalk can occur among the inputs to a crosspoint
and among the output. It can also occur from input to output.
Techniques are discussed for diagnosing which part of a system
is contributing to crosstalk.
Measuring Crosstalk
Crosstalk is measured by applying a signal to one or more
channels and measuring the relative strength of that signal on a
desired selected channel. The measurement is usually expressed
as dB down from the magnitude of the test signal. The crosstalk
is expressed by
( ) ( )
( )
sAtest
sAselXT
10
log20=
where:
s = jω is the Laplace transform variable.
Asel(s) is the amplitude of the crosstalk-induced signal in the
selected channel.
Atest(s) is the amplitude of the test signal.
It can be seen that crosstalk is a function of frequency, but not a
function of the magnitude of the test signal (to first order).
In addition, the crosstalk signal has a phase relative to the
test signal associated with it.
A network analyzer is most commonly used to measure crosstalk
over a frequency range of interest. It can provide both magnitude
and phase information about the crosstalk signal.
As a crosspoint system or device grows larger, the number of
theoretical crosstalk combinations and permutations can become
extremely large. For example, in the case of the 16 × 16 matrix
of the AD8114/AD8115, we can examine the number of crosstalk
terms that can be considered for a single channel, say IN00 input.
IN00 is programmed to connect to one of the AD8114/AD8115
outputs where the measurement can be made.
First, we can measure the crosstalk terms associated with driving
a test signal into each of the other 15 inputs one at a time while
applying no signal to IN00. We can then measure the crosstalk
terms associated with driving a parallel test signal into all 15
other inputs taken two at a time in all possible combinations, then
three at a time, and so on, until there is only one way to drive a
test signal into all 15 other inputs in parallel.
Each of these cases is legitimately different from the others and
might yield a unique value depending on the resolution of the
measurement system, but it is hardly practical to measure all
these terms and then to specify them. In addition, this describes
the crosstalk matrix for just one input channel. A similar crosstalk
matrix can be proposed for every other input. In addition, if the
possible combinations and permutations for connecting inputs
to the other (not used for measurement) outputs are taken into
consideration, the numbers rather quickly grow to astronomical
proportions. If a larger crosspoint array of multiple AD8114/
AD8115 devices is constructed, the numbers grow larger still.
Some subset of all these cases must be selected to be used as a
guide for a practical measure of crosstalk. One common method is
to measure all hostile crosstalk. This term means that the crosstalk
to the selected channel is measured while all other system channels
are driven in parallel. In general, this yields the worst crosstalk
number, but this is not always the case due to the vector nature
of the crosstalk signal.
Other useful crosstalk measurements are those created by one
nearest neighbor or by the two nearest neighbors on either side.
These crosstalk measurements are generally higher than those
of more distant channels, so they can serve as a worst-case
measure for any other 1-channel or 2-channel crosstalk
measurements.
Input and Output Crosstalk
The flexible programming capability of the AD8114/AD8115
can be used to diagnose whether crosstalk is occurring more on
the input side or the output side. Some examples are illustrative.
A given input channel (IN07 in the middle for this example)
can be programmed to drive OUT07 (also in the middle). The
input to IN07 is just terminated to ground (via 50 or 75 )
and no signal is applied.
All the other inputs are driven in parallel with the same test
signal (practically that is provided by a distribution amplifier),
with all other outputs except OUT07 disabled. Since grounded
IN07 is programmed to drive OUT07, no signal should be present.
Any signal that is present can be attributed to the other 15 hostile
input signals because no other outputs are driven. (They are all
disabled.) Thus, this method measures the all-hostile input
contribution to crosstalk into IN07. Of course, the method can
be used for other input channels and combinations of hostile
inputs.
Data Sheet AD8114/AD8115
Rev. C | Page 23 of 25
For output crosstalk measurement, a single input channel is
driven (IN00, for example) and all outputs other than a given
output (IN07 in the middle) are programmed to connect to
IN00. OUT07 is programmed to connect to IN15 (far away
from IN00), which is terminated to ground.
Thus OUT07 should not have a signal present since it is
listening to a quiet input. Any signal measured at the OUT07
can be attributed to the output crosstalk of the other 16 hostile
outputs. Again, this method can be modified to measure other
channels and other crosspoint matrix combinations.
Effect of Impedances on Crosstalk
The input side crosstalk can be influenced by the output
impedance of the sources that drive the inputs. The lower the
impedance of the drive source, the lower the magnitude of the
crosstalk. The dominant crosstalk mechanism on the input side
is capacitive coupling. The high impedance inputs do not have
significant current flow to create magnetically induced crosstalk.
However, significant current can flow through the input
termination resistors and the loops that drive them. Thus,
the printed circuit board on the input side can contribute to
magnetically coupled crosstalk.
From a circuit standpoint, the input crosstalk mechanism looks
like a capacitor coupling to a resistive load. For low frequencies,
the magnitude of the crosstalk is given by
( )( )
sCRXT
MS
×=
10
log20
where:
R
S
is the source resistance.
C
M
is the mutual capacitance between the test signal circuit
and the selected circuit.
s is the Laplace transform variable.
From the equation, it can be observed that this crosstalk
mechanism has a high-pass nature; it can be minimized by
reducing the coupling capacitance of the input circuits and
lowering the output impedance of the drivers. If the input is
driven from a 75 terminated cable, the input crosstalk can be
reduced by buffering this signal with a low output impedance
buffer.
On the output side, the crosstalk can be reduced by driving a
lighter load. Although the AD8114/AD8115 is specified with
excellent differential gain and phase when driving a standard
150 video load, the crosstalk is higher than the minimum
obtainable due to the high output currents. These currents
induce crosstalk via the mutual inductance of the output pins
and bond wires of the AD8114/AD8115.
From a circuit standpoint, this output crosstalk mechanism
looks like a transformer, with a mutual inductance between the
windings, that drives a load resistor. For low frequencies, the
magnitude of the crosstalk is given by
)
/(log20
10
L
R
sMxyXT ×=
where:
Mxy is the mutual inductance of Output X to Output Y.
R
L
is the load resistance on the measured output.
This crosstalk mechanism can be minimized by keeping
the mutual inductance low and increasing R
L
. The mutual
inductance can be kept low by increasing the spacing of
the conductors and minimizing their parallel length.
AD8114/AD8115 Data Sheet
Rev. C | Page 24 of 25
OUTLINE DIMENSIONS
COMPLIANT TO JEDEC STANDARDS MS-026-BED
TOP VIEW
(PINS DOWN)
1
25
26
51
50
75
76100
0.50
BSC
LEAD PITCH
0.27
0.22
0.17
1.60 MAX
0.75
0.60
0.45
VIEW A
PIN 1
1.45
1.40
1.35
0.15
0.05
0.20
0.09
0.08
COPLANARITY
VIEW A
ROTATED 90° CCW
SEATING
PLANE
3.5°
14.20
14.00 SQ
13.80
16.20
16.00 SQ
15.80
051706-A
Figure 50. 100-Lead Low Profile Quad Flat Package [LQFP]
(ST-100-1)
Dimension shown in millimeters
ORDERING GUIDE
Model
1, 2
Temperature Range Package Description Package Option
AD8114ASTZ 40°C to +85°C 100-Lead Low Profile Quad Flat Package [LQFP] ST-100-1
AD8115ASTZ 40°C to +85°C 100-Lead Low Profile Quad Flat Package [LQFP] ST-100-1
1
Details of the lead finish composition can be found on the Analog Devices website at www.analog.com by reviewing the Material Description of each relevant package.
2
Z = RoHS Compliant Part.

AD8114ASTZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog & Digital Crosspoint ICs 225MHz 16 x 16
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union

Products related to this Datasheet