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ADA4622-1ARJZ-R2 Datasheet(PDF) 31 Page - Analog Devices

Part # ADA4622-1ARJZ-R2
Description  30 V, 8 MHz, Low Bias Current, Single-Supply, RRO, Precision Op Amps
PDF  38 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

ADA4622-1ARJZ-R2 Datasheet(HTML) 31 Page - Analog Devices

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Data Sheet
ADA4622-1/ADA4622-2/ADA4622-4
Rev. E | Page 31 of 38
The following basic transfer function describes the transimpedance
gain of the photodiode preamplifier:
F
F
F
PHOTO
OUT
R
sC
R
I
V
+
×
=
1
where:
IPHOTO is the output current of the photodiode.
The parallel combination of RF and CF sets the signal bandwidth
(see the I to V gain trace in Figure 96).
s refers to the s-plane.
Note that RF must be set so the maximum attainable output
voltage corresponds to the maximum diode output current,
IPHOTO, which allows use of the full output swing. The attainable
signal bandwidth with this photodiode preamplifier is a function
of RF, the gain bandwidth product (fGBP) of the amplifier, and
the total capacitance at the amplifier summing junction, including
CS and the amplifier input capacitance, CD and CM. RF and the
total capacitance produce a pole with loop frequency (fP).
S
F
P
C
R
f
π
=
2
1
With the additional pole from the amplifier open-loop response,
the two-pole system results in peaking and instability due to an
insufficient phase margin (see Figure 95).
log f
log f
G = 1
G = R2C1s
OPEN-LOOP GAIN
–180°
–135°
–90°
–45°
fP
fX
fGBP
Figure 95. Gain and Phase Plot of the Transimpedance Amplifier Design,
Without Compensation
OPEN-LOOP GAIN
f
fp
G = 1
f
fGBP
G = 1 + CS/CF
fZ
fX
fN
I TO V GAIN
–135°
–90°
–45°
45°
90°
G = RFCS(s)
Figure 96. Gain and Phase Plot of the Transimpedance Amplifier Design with
Compensation
Adding CF creates a zero in the loop transmission that compensates
for the effect of the input pole, which stabilizes the photodiode
preamplifier design because of the increased phase margin. Adding
CF also sets the signal bandwidth (see Figure 96). The signal
bandwidth and the zero frequency are determined by
F
F
Z
C
R
f
π
2
1
=
where fZ is the zero frequency.
Setting the zero at the fX frequency maximizes the signal bandwidth
with a 45° phase margin. Because fX is the geometric mean of fP
and fGBP, it can be calculated by
GBP
P
X
f
f
f
×
=
Combining these equations, the CF value that produces fX is
GBP
F
S
F
f
R
C
C
×
×
π
=
2
The frequency response in this case shows approximately 2 dB of
peaking and 15% overshoot. Doubling CF and halving the band-
width results in a flat frequency response with approximately 5%
transient overshoot.



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