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ADA4817-2ACPZ-R7 データシート(PDF) 24 Page - Analog Devices

部品番号 ADA4817-2ACPZ-R7
部品情報  Low Noise, 1 GHz FastFET Op Amps
PDF  29 Pages
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メーカー  AD [Analog Devices]
ホームページ  http://www.analog.com
Logo AD - Analog Devices

ADA4817-2ACPZ-R7 データシート(HTML) 24 Page - Analog Devices

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Data Sheet
ADA4817-1/ADA4817-2
APPLICATIONS INFORMATION
analog.com
Rev. H | 24 of 29
LOW DISTORTION PINOUT
The ADA4817-1/ADA4817-2 feature a low distortion pinout from
Analog Devices. The new pinout provides two advantages over the
traditional pinout. The first advantage is improved second harmonic
distortion performance, which is accomplished by the physical sep-
aration of the noninverting input pin and the negative power supply
pin. The second advantage is the simplification of the layout due to
the dedicated feedback pin and easy routing of the gain set resistor
back to the inverting input pin. This pinout allows a compact layout,
which helps to minimize parasitics and increase stability.
The designer does not need to use the dedicated feedback pin to
provide feedback for the ADA4817-1/ADA4817-2. The output pin of
the ADA4817-1/ADA4817-2 can still be used to provide feedback to
the inverting input of the ADA4817-1/ADA4817-2.
WIDEBAND PHOTODIODE PREAMP
The wide bandwidth and low noise of the ADA4817-1/ADA4817-2
make it an ideal choice for transimpedance amplifiers, such as
those used for signal conditioning with high speed photo-diodes.
Figure 63 shows a current to voltage converter with an electrical
model of a photodiode. The basic transfer function is
VOUT=IPHOTO×RF
1+sCFRF
(12)
where:
IPHOTO is the output current of the photodiode.
RF and CF are the parallel combination that sets the signal band-
width.
Figure 63. Wideband Photodiode Preamp
The stable bandwidth attainable with this preamp is a function
of RF, the gain bandwidth product of the amplifier, and the total
capacitance at the summing junction of the amplifier, including the
photodiode capacitance (CS) and the amplifier input capacitance.
RF and the total capacitance produce a pole in the loop transmis-
sion of the amplifier that can result in peaking and instability. Adding
CF creates a zero in the loop transmission that compensates for
the effect of the pole and reduces the signal bandwidth. It can be
shown that the signal bandwidth obtained with a 45° phase margin
(f(45)) is defined by
f45 = fCR
2π×RF× CS+CM+CD
(13)
where:
fCR is the amplifier crossover frequency.
RF is the feedback resistor.
CS is the source capacitance including the photodiode and the
board parasitic.
CM is the common-mode capacitance of the amplifier.
CD is the differential capacitance of the amplifier.
The CF value that produces f(45) is shown to be
CF= CS+CM+CD
2π×RF×fCR
(14)
The frequency response shows less peaking if larger CF values are
used.
Figure 64 shows the preamplifier output noise over frequency.
Figure 64. Photodiode Voltage Noise Contributions
Figure 65. Photodiode Preamp Frequency Response
The pole in the loop transmission translates to a zero in the noise
gain of the amplifier, leading to an amplification of the input voltage
noise over frequency.



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