Data Sheet AD8067
Rev. B | Page 17 of 24
Grounding
To minimize parasitic inductances and ground loops in high
speed, densely populated boards, a ground plane layer is critical.
Understanding where the current flows in a circuit is critical in
the implementation of high speed circuit design. The length of
the current path is directly proportional to the magnitude of the
parasitic inductances and thus the high frequency impedance of
the path. Fast current changes in an inductive ground return
creates unwanted noise and ringing.
The length of the high frequency bypass capacitor leads is
critical. A parasitic inductance in the bypass grounding works
against the low impedance created by the bypass capacitor.
Because load currents flow from supplies as well as ground, the
load should be placed at the same physical location as the
bypass capacitor ground. For large values of capacitors, which
are intended to be effective at lower frequencies, the current
return path length is less critical.
Power Supply Bypassing
Power supply pins are actually inputs and care must be taken to
provide a clean, low noise dc voltage source to these inputs. The
bypass capacitors have two functions:
Provide a low impedance path for unwanted frequencies
from the supply inputs to ground, thereby reducing the effect
of noise on the supply lines
Provide localized charge storagethis is usually
accomplished with larger electrolytic capacitors
Decoupling methods are designed to minimize the bypassing
impedance at all frequencies. This can be accomplished with a
combination of capacitors in parallel to ground. Good quality
ceramic chip capacitors (X7R or NPO) should be used and
always kept as close to the amplifier package as possible. A
parallel combination of a 0.1 µF ceramic and a 10 µF electrolytic,
covers a wide range of rejection for unwanted noise. The 10 µF
capacitor is less critical for high frequency bypassing, and in
most cases, one per supply line is sufficient.
AD8067 Data Sheet
Rev. B | Page 18 of 24
APPLICATIONS
WIDEBAND PHOTODIODE PREAMP
+
V
OUT
V
B
C
F
+ C
S
C
D
C
M
C
M
R
F
AD8067
R
SH
= 10
11
C
S
I
PHOTO
C
F
R
F
Figure 49. Wideband Photodiode Preamp
Figure 49 shows an I/V converter with an electrical model of a
photodiode.
The basic transfer function is
FF
F
PHOTO
OUT
RsC
RI
V
+
×
=
1
where I
PHOTO
is the output current of the photodiode, and the
parallel combination of R
F
and C
F
sets the signal bandwidth.
The stable bandwidth attainable with this preamp is a function
of R
F
, the gain bandwidth product of the amplifier, and the total
capacitance at the amplifier’s summing junction, including C
S
and the amplifier input capacitance. R
F
and the total capacitance
produce a pole in the amplifier’s loop transmission that can
result in peaking and instability. Adding C
F
creates a zero in the
loop transmission that compensates for the poles effect and
reduces the signal bandwidth. It can be shown that the signal
bandwidth resulting in a 45° phase margin (f
(45)
) is defined by
( )
S
F
45
CR
GBP
f
××
=
π2
GBP is the unit gain bandwidth product, R
F
is
the feedback
resistance, and C
S
is the total capacitance at the amplifier
summing junction (amplifier + photodiode + board parasitics).
The value of C
F
that produces f
(45)
can
be shown to be
GBPR
C
C
F
S
F
××
=
π2
The frequency response in this case shows about 2 dB of
peaking and 15% overshoot. Doubling C
F
and cutting the
bandwidth in half results in a flat frequency response, with
about 5% transient overshoot.
The preamps output noise over frequency is shown in Figure 50.
Table 6. RMS Noise Contributions of Photodiode Preamp
Contributor Expression
RMS
Noise
(µV)
1
R
F
× 2
5712fRkT42
F
.××××
152
Amp to f1
1fV
NOISE
×
4.3
Amp (f2 f1)
( )
1f2f
C
C2CCC
V
F
DFM
S
NOISE
×
+++
×
96
Amp (Past f2)
( )
5713f
C
C2CCC
V
F
DFM
S
NOISE
.××
+++
×
684
RSS Total
708
1
RMS noise with R
F
= 50 k, C
S
= 0.67 pF, C
F
= 0.33 pF, C
M
= 1.5 pF, and C
D
= 2.5 pF.
FREQUENCY – Hz
VOLTAGE NOISE – nV/ Hz
RF NOISE
f
1
NOISE DUE TO AMPLIFIER
VEN
f
2
1
2
π
R
F
(C
F
+ C
S
+ C
M
+ 2C
D
)
f
1
=
f
2
=
1
2
π
R
F
C
F
f
3
=
GBP
(C
S
+ C
M
+ 2C
D
+ C
F
)/C
F
VEN (C
F
+ C
S
+ C
M
+ 2C
D
)/C
F
f
3
Figure 50. Photodiode Voltage Noise Contributions
Figure 51 shows the AD8067 configured as a transimpedance
photodiode amplifier. The amplifier is used in conjunction with
a JDS uniphase photodiode detector. This amplifier has a
bandwidth of 9.6 MHz, as shown in Figure 52, and is verified by
the design equations shown in Figure 50.
AD8067
0.1µF
10µF
+5V
49.9k
50
49.9k
0.33pF
V
OUT
0.1µF
10µF
–5V
EPM 605 LL
–5V
0.33pF
NOTES
I
D
@ –5V = 0.074nA
C
D
@ –5V = 0.690pF
R
B
@ 1550nm = –49dB
Figure 51. Photodiode Preamplifier
Data Sheet AD8067
Rev. B | Page 19 of 24
Test data for the preamp is shown in Figure 52 and Figure 53.
FREQUENCY – MHz
TRANSIMPEDANCE GAIN – dB
100
65
70
75
80
85
90
95
60
0.01 0.1 1 10 100
Figure 52. Photodiode Preamplifier Frequency Response
M 50ns CH1 830mVCH1 500mV
C1 RISE
31.2ns
C1 FALL
31.6ns
T
Figure 53. Photodiode Preamplifier Pulse Response
USING THE AD8067 AT GAINS OF LESS THAN 8
A common technique used to stabilize de-compensated
amplifiers is to increase the noise gain, independent of the
signal gain. The AD8067 can be used in applications where the
signal gain is less than 8, if proper care is taken to ensure that
the noise gain of the amplifier is set to at least the recommended
minimum signal gain of 8 (see Figure 54).
The signal and noise gain equations for a noninverting
amplifier are:
R1
R3
GainSignal +=1
R1
R3
GainNoise +=1
The addition of resistor R2 modifies the noise gain equation.
Note the signal gain equation has not changed.
R2R1
R3
GainNoise
||
1+=
AD8067
C2
0.1µF
C1
10
µF
+5V
R2
50
C3
10µF
C4
0.1µF
–5V
V
OUT
R
L
R4
51
R3
600
V
IN
1
5
4
3
2
R1
301
Figure 54. Gain = 3 Schematics
This technique allows the designer to use the AD8067 in gain
configurations of less than 8. The drawback to this type of
compensation is that the input noise and offset voltages are
also amplified by the value of the noise gain. In addition, the
distortion performance is degraded. To avoid excessive
overshoot and ringing when driving a capacitive load, the
AD8067 should be buffered by a small series resistor; in this
case, a 51 Ω resistor was used.

AD8067ARTZ-REEL7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers High Gain BW Prec IC
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