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THS4541 Datasheet(PDF) 24 Page - Texas Instruments |
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THS4541 Datasheet(HTML) 24 Page - Texas Instruments |
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24 / 64 page ![]() 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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