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ADA4351-2ACPZ-R7 数据表(PDF) 33 Page - Analog Devices

部件名 ADA4351-2ACPZ-R7
功能描述  Compact, Dual-Channel, Precision, Programmable Gain Transimpedance Amplifier (PGTIA)
PDF  36 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADA4351-2ACPZ-R7 数据表(HTML) 33 Page - Analog Devices

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Data Sheet
ADA4351-2
APPLICATIONS INFORMATION
analog.com
Rev. 0 | 33 of 36
COMPENSATED AND NONCOMPENSATED
FREQUENCY RESPONSE
For any given source capacitance and desired TIA gain (RF), the
small signal frequency response may or may not be acceptable to
the application. Some response shape tuning is possible by adding
a compensation capacitor in parallel with RF. Figure 95 through
Figure 97, over a wide range of gains, show some typical response
shape trade-offs.
The lowest feedback (RF = 200 Ω) has the highest bandwidth
because the noise gain zero is relatively higher in frequency than
the higher gains with the same source capacitance. As previously
mentioned, at the lowest RF value, the output swing range is
reduced by the IR drop through the inside of the loop switch
impedance (approximately 0.7 V, see Figure 84). In each of the
conditions reported in Figure 95 through Figure 97, CIN = CD +
CSTRAY (refer to the TIA Design Theory section for definitions of
the terms). To get the total CS, add the internal input capacitances
(CCM + CDIFF) of 5.5 pF to CIN. Similarly, to get the total CF, add
the internal 3 pF to the CF,EXT shown in Figure 95 through Figure
97. For both of the 10 pF source CIN curves shown in Figure 95,
the noise gain zero and pole frequencies are beyond the 8.5 MHz
GBP; therefore, typical TIA analysis does not apply. The circuit with
CIN = 10 pF whose frequency response is shown in Figure 95 is
essentially operating as a unity-gain stage with a flat frequency
response with a 10 MHz f−3 dB.
The 100 pF CIN puts the noise gain zero just less than the GBP.
With no external CF,EXT, this zero gives a relatively low phase
margin and about 1.1 dB peaking because the noise gain pole is
much higher in frequency. Adding a 150 pF CFEXT moves the noise
gain zero down to 3 MHz with a noise gain pole at 5.2 MHz (see
Figure 95) giving a nicely overcompensated design with Q ≈ 0.62
and an f−3 dB near 4.5 MHz.
Figure 95. Small Signal Responses for RF = 200 Ω with a Range of Input CIN
(CD + CSTRAY) and External Feedback (CF,EXT) Capacitors
Going to a midrange feedback gain of 15 kΩ gives the family of
curves shown in Figure 96.
Figure 96. Small Signal Responses for RF = 15 kΩ with a Range of Input CIN
(CD + CSTRAY) and External Feedback (CF,EXT) Capacitors
The initial 10 pF source with only an internal 3 pF feedback
capacitor forms a noise gain zero below f0 (see the solid blue line
in Figure 96) but a feedback pole more than f0 giving the typical
peaked response shown by the solid blue curve shown in Figure
96. The peaking noise gain is crossing over the AOL curve with
slightly less than a 40 dB closure rate giving the approximate Q
= 1.1 and the 20log(21 kΩ/15 kΩ) = 2.9 dB peaking. Adding the
external 5.6 pF retunes the response shape to a controlled Q = 0.56
and f−3 dB ≈ 1.4 MHz, as shown by the dotted blue line shown in
Figure 96.
Testing an 100 pF external CIN, with only the internal 3 pF CF,INT,
again undercompensates the design (Q ≈ 2.7 with ≈9 dB peaking).
For this RF value, CF,EXT is required and the 16 pF shown in Figure
96 compensates this design back to Q = 0.62 with a f−3 dB = ≈730
kHz. Figure 96 is used to illustrate a typical TIA design flow and an
integrated noise analysis in those applications sections.
Using a large external RF (1 MΩ) results in the overcompensated
response shown in Figure 97 due to the internal 3 pF capacitor.
Figure 97. Small Signal Responses for RF = 1 MΩ with a Range of Input CIN
(CD + CSTRAY) Capacitors



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