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THS4541 Datasheet(PDF) 24 Page - Texas Instruments

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Part # THS4541
Description  THS4541-Q1 Negative Rail Input, Rail-to-Rail Output, Precision, 850-MHz Fully Differential Amplifier
PDF  64 Pages
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Manufacturer  TI1 [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI1 - Texas Instruments

THS4541 Datasheet(HTML) 24 Page - Texas Instruments

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Frequency (Hz)
0
5
10
15
20
25
30
35
40
10M
100M
1G
D062
Aol Gain
Gain = 0.1
Gain = 1
Gain = 2
‡
Rf
1
Rg
s
Rf Cf
Cin
Cin
NG
1
1
Cf
s
Rf Cf
§
·
¨
¸
©
¹
Rf
402
FDA
Output
Pin
+
±
Cf
200 fF
Rg
221
Vout
Cin
1.7 pF
Vin
24
THS4541-Q1
SLOS930B – NOVEMBER 2015 – REVISED NOVEMBER 2019
www.ti.com
Product Folder Links: THS4541-Q1
Submit Documentation Feedback
Copyright © 2015–2019, Texas Instruments Incorporated
NG is critically important for bandwidth and all output error terms (such as DC offset and noise). For lower-speed
devices, normally only the DC noise gain is considered. However, for the THS4541-Q1, with loop gain crossover
at greater than 300 MHz, the feedback network produces a parasitic pole to the differential summing junctions
that causes the noise gain to increase with frequency. This pole causes a lower crossover frequency than might
be expected with added phase shift around the loop. Consider the feedback network (single-ended) of Figure 65,
showing a parasitic 0.2 pF on the feedback 402-Ω resistor. The 0.85-pF differential input capacitance of the
THS4541-Q1 is converted to single-ended as a 1.7-pF parasitic for this single-sided analysis circuit (the Rg
shown is Rg2 in Figure 61).
Figure 65. Feedback Network for the Gain of 2 Configuration Using 402 Ω and Matching to a 50-Ω Source
The response shape from Vout to Vin in Figure 65 has a pole and then a zero. To describe NG, invert the
Laplace transform of Vin and Vout from Figure 65 to provide the frequency-dependent NG response of
Equation 1, where a zero comes in first and then a pole.
(1)
The zero location is key. Using the gain of 2 values of Figure 65, the estimated zero in the NG is 588 MHz.
Limiting the parasitic capacitance at the summing junctions, either differentially or signal-ended, to a ground or
power plane is critical in board layouts.
Using this feedback model, and the open-loop gain and phase data for the THS4541-Q1, allows the Aol and NG
curves over frequency to be drawn, as shown in Figure 66, where the peaking in the noise gain pulls the
intersection point back in frequency.
Figure 66. Aol and Noise Gain Plots for the Lower Gains of Figure 61



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