REV. D
AD8001
–9–
300k 100M10M1M
FREQUENCY – Hz
–20
–10
–40
–30
CMRR – dB
910
V
OUT
V
IN
150
150
910
51
62
1G
–50
TPC 31. CMRR vs. Frequency
1
–4
–9
1M 10M 1G100M
–5
–6
–7
–8
–3
–2
–1
0
FREQUENCY – Hz
OUTPUT – dB
R
F
= 750
R
F
= 649
R
F
= 549
G = –2
R
L
= 100
V
IN
= 50mV
rms
TPC 32. –3 dB Bandwidth vs. Frequency, G = –2
TPC 33. 100 mV Step Response, G = –1
10
–20
1M 10M 100M
–10
0
20
FREQUENCY – Hz
PSRR – dB
–60
–50
–40
–30
1G
30
CURVES ARE FOR WORST-
CASE CONDITION WHERE
ONE SUPPLY IS VARIED
WHILE THE OTHER IS
HELD CONSTANT.
R
F
= 909
G = +2
–PSRR
+PSRR
–PSRR
+PSRR
TPC 34. PSRR vs. Frequency
TPC 35. 2 V Step Response, G = –1
3–4–5 210–1–2–3 54
100
20
0
10
80
90
70
60
50
40
30
100
20
0
10
80
90
70
60
50
40
30
COUNT
PERCENT
INPUT OFFSET VOLTAGE – mV
3 WAFER LOTS
COUNT = 895
MEAN = 1.37
STD DEV = 1.13
MIN = –2.45
MAX = +4.69
FREQ DIST
CUMULATIVE
TPC 36. Input Offset Voltage Distribution
REV. D
AD8001
–10–
THEORY OF OPERATION
A very simple analysis can put the operation of the AD8001, a
current feedback amplifier, in familiar terms. Being a current
feedback amplifier, the AD8001’s open-loop behavior is expressed
as transimpedance, V
O
/I
–IN
, or T
Z
. The open-loop transimped-
ance behaves just as the open-loop voltage gain of a voltage
feedback amplifier, that is, it has a large dc value and decreases
at roughly 6 dB/octave in frequency.
Since the R
IN
is proportional to 1/g
M
, the equivalent voltage
gain is just T
Z
× g
M
, where the g
M
in question is the trans-
conductance of the input stage. This results in a low open-loop
input impedance at the inverting input, a now familiar result.
Using this amplifier as a follower with gain, Figure 4, basic
analysis yields the following result.
V
V
G
TS
TS G R R
G
R
R
Rg
O
IN
Z
ZIN
IN M
+
=+ =
()
()
/
1
1
1
2
150
V
OUT
R1
R2
R
IN
V
IN
Figure 4. Follower with Gain
Recognizing that G × R
IN
<< R1 for low gains, it can be seen to
the first order that bandwidth for this amplifier is independent
of gain (G). This simple analysis in conjunction with Figure 5
can, in fact, predict the behavior of the AD8001 over a wide
range of conditions.
FREQUENCY – Hz
1M
10
100k
1M 1G100M10M
100
100k
10k
1k
T
Z
Figure 5. Transimpedance vs. Frequency
Considering that additional poles contribute excess phase at
high frequencies, there is a minimum feedback resistance below
which peaking or oscillation may result. This fact is used to
determine the optimum feedback resistance, R
F
. In practice,
parasitic capacitance at Pin 2 will also add phase in the feedback
loop, so picking an optimum value for R
F
can be difficult.
Figure 6 illustrates this problem. Here the fine scale (0.1 dB/
div) flatness is plotted versus feedback resistance. These plots
were taken using an evaluation card which is available to cus-
tomers so that these results may readily be duplicated.
Achieving and maintaining gain flatness of better than 0.1 dB at
frequencies above 10 MHz requires careful consideration of
several issues.
OUTPUT – dB
0.1
0
–0.9
1M 10M 100M
–0.1
–0.2
–0.3
–0.4
–0.5
FREQUENCY – Hz
–0.6
–0.7
–0.8
G = +2
R
F
=
649
R
F
= 698
R
F
= 750
Figure 6. 0.1 dB Flatness vs. Frequency
Choice of Feedback and Gain Resistors
Because of the above-mentioned relationship between the band-
width and feedback resistor, the fine scale gain flatness will, to
some extent, vary with feedback resistance. It, therefore, is
recommended that once optimum resistor values have been
determined, 1% tolerance values should be used if it is desired to
maintain flatness over a wide range of production lots. In addition,
resistors of different construction have different associated parasitic
capacitance and inductance. Surface-mount resistors were used
for the bulk of the characterization for this data sheet. It is not
recommended that leaded components be used with the AD8001.
REV. D
AD8001
–11–
Printed Circuit Board Layout Considerations
As to be expected for a wideband amplifier, PC board parasitics
can affect the overall closed-loop performance. Of concern are
stray capacitances at the output and the inverting input nodes. If
a ground plane is to be used on the same side of the board as
the signal traces, a space (5 mm min) should be left around the
signal lines to minimize coupling. Additionally, signal lines
connecting the feedback and gain resistors should be short
enough so that their associated inductance does not cause high
frequency gain errors. Line lengths on the order of less than
5 mm are recommended. If long runs of coaxial cable are being
driven, dispersion and loss must be considered.
Power Supply Bypassing
Adequate power supply bypassing can be critical when optimiz-
ing the performance of a high frequency circuit. Inductance in
the power supply leads can form resonant circuits that produce
peaking in the amplifier’s response. In addition, if large current
transients must be delivered to the load, then bypass capacitors
(typically greater than 1 µF) will be required to provide the best
settling time and lowest distortion. A parallel combination of
4.7 µF and 0.1 µF is recommended. Some brands of electrolytic
capacitors will require a small series damping resistor 4.7 for
optimum results.
DC Errors and Noise
There are three major noise and offset terms to consider in a
current feedback amplifier. For offset errors, refer to the equation
below. For noise error the terms are root-sum-squared to give a
net output error. In the circuit in Figure 7 they are input offset
(V
IO
), which appears at the output multiplied by the noise gain
of the circuit (1 + R
F
/R
I
), noninverting input current (I
BN
× R
N
)
also multiplied by the noise gain, and the inverting input current,
which when divided between R
F
and R
I
and subsequently
multiplied by the noise gain always appears at the output as
I
BN
× R
F
. The input voltage noise of the AD8001 is a low 2 nV/
Hz. At low gains though the inverting input current noise times
R
F
is the dominant noise source. Careful layout and device
matching contribute to better offset and drift specifications for
the AD8001 compared to many other current feedback ampli-
fiers. The typical performance curves in conjunction with the
following equations can be used to predict the performance of
the AD8001 in any application.
VV
R
R
IR
R
R
IR
OUT IO
F
I
BN N
F
I
BI F
+
±××+
±×11
R
F
R
I
R
N
I
BN
V
OUT
I
BI
Figure 7. Output Offset Voltage
Driving Capacitive Loads
The AD8001 was designed primarily to drive nonreactive loads.
If driving loads with a capacitive component is desired, best
frequency response is obtained by the addition of a small series
resistance, as shown in Figure 8. The accompanying graph
shows the optimum value for R
SERIES
versus capacitive load. It is
worth noting that the frequency response of the circuit when
driving large capacitive loads will be dominated by the passive
roll-off of R
SERIES
and C
L
.
909
R
SERIES
R
L
500
I
N
C
L
Figure 8. Driving Capacitive Loads
40
0
0
25
30
10
5
20
15 2010
C
L
– pF
G = +1
R
SERIES
Figure 9. Recommended R
SERIES
vs. Capacitive Load

AD8001ARZ

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Video Amplifiers 800MHz 50mW Current Feedback
Lifecycle:
New from this manufacturer.
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