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OPA855 Datasheet(PDF) 20 Page - Texas Instruments

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Part # OPA855
Description  OPA856 1.1-GHz Unity-Gain Bandwidth, 0.9 nV /?숰z , Bipolar Input Amplifier
PDF  33 Pages
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Manufacturer  TI [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI - Texas Instruments

OPA855 Datasheet(HTML) 20 Page - Texas Instruments

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9.2.2 Detailed Design Procedure
The OPA856 meets the growing demand for wideband, low-noise photodiode amplifiers. The closed-loop
bandwidth of a transimpedance amplifier is a function of the following:
1. The total input capacitance (CIN). This total includes the photodiode capacitance, the input capacitance of the
amplifier (common-mode and differential capacitance) and any stray capacitance from the PCB.
2. The op amp gain bandwidth product (GBWP).
3. The transimpedance gain (RF).
Figure 9-1 shows the OPA856 configured as a TIA, with the photodiode reverse biased so that the diode cathode
is tied to a positive bias voltage. In this configuration, the diode sources current into the op amp feedback loop
so that the output swings in a negative direction relative to the input common-mode (VOFFSET) voltage. The
feedback resistance (RF) and the input capacitance (CIN) form a zero in the noise gain that results in instability if
left unchecked. To counteract the effect of the zero, a pole is inserted into the noise gain transfer function by
adding the feedback capacitor (CF).
The Transimpedance Considerations for High-Speed Amplifiers Application Report discusses theories and
equations that show how to compensate a transimpedance amplifier for a particular transimpedance gain and
input capacitance. The bandwidth and compensation equations from the application report are available in a
Microsoft Excel ™ calculator. What You Need To Know About Transimpedance Amplifiers – Part 1 provides a
link to the calculator. Calculating the expected bandwidth with an approximate input capacitance of 4 pF and a
feedback capacitor of 1 pF yields a bandwidth of approximately 200 MHz.
The amplifier was tested in a transimpedance configuration by using a photodiode with an optical fiber input
connection. A tunable laser connected through an optical modulator was used to create the modulated optical
excitation to the photodiode. Figure 9-2 shows the test setup configuration for the frequency response
measurement. The network analyzer's swept frequency output drives the optical modulators electrical input
which in turn drives the photodiode. The OPA856 output drives the network analyzer's input.
+
±
1 NŸ
5V
ON
OFF
1 pF
169
71.5
1330 nm
-
-
-
Optical
Modulator
Tunable Laser
Network Analyzer
OPA856
200-Ÿ ORDG PDWFKHG
to 50-Ÿ LQSXW
Fiber connected
photodiode
Figure 9-2. OPA856 Transimpedance Frequency Response Test Setup
Figure 9-4 shows the frequency response measurements for a small signal and large signal (~1 Vpp) output.
The plot contains noticeable noise and variations because the test environment did not have complete capability
to accurately manage the thermal drift, perform optical connection integrity analysis, and calibrate the optical
path. A more stringently controlled optical environment could achieve more stable results, but was beyond the
scope of these measurements. The results in Figure 9-4 correlate well with predicted results of approximately
200 MHz of bandwidth. It is expected that the results would not perfectly match calculated values because it is
challenging to perfectly account for all parasitic capacitances that affect the input and feedback capacitance in
the transimpedance calculations.
OPA856
SBOS623 – OCTOBER 2020
www.ti.com
20
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Copyright © 2020 Texas Instruments Incorporated
Product Folder Links: OPA856



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