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LMH3401 Datasheet, PDF (32/48 Pages) Texas Instruments – LMH3401 7-GHz, Ultra-Wideband, Fixed-Gain, Fully-Differential Amplifier
LMH3401
SBOS695A – AUGUST 2014 – REVISED DECEMBER 2014
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10.2.2.3.2 SFDR Considerations
The SFDR of the amplifier is usually set by the second-order or third-order harmonic distortion for single-tone
inputs, and by the second-order or third-order intermodulation distortion for two-tone inputs. Harmonics and
second-order intermodulation distortion can be filtered to some degree, but third-order intermodulation spurs
cannot be filtered. The ADC generates the same distortion products as the amplifier, but as a result of the
sampling and clock feedthrough, additional spurs (not linearly related to the input signal) are included.
When the spurs from the amplifier and filter are known, each individual spur can be directly added to the same
spur from the ADC, as shown in Equation 10, to estimate the combined spur (spur amplitudes in dBc):
-HDxAMP+FILTER
-HDxADC
× HDxSYSTEM = -20 log 10 20
+ 10 20
(10)
This calculation assumes the spurs are in phase, but usually provides a good estimate of the final combined
distortion.
For example, if the spur of the amplifier and filter equals the spur of the ADC, then the combined spur is 6 dB
higher. To minimize the amplifier contribution (< 1 dB) to the overall system distortion, the spur from the amplifier
and filter must be approximately 15 dB lower in amplitude than that of the converter. The combined spur
calculated in this manner is usually accurate to within ±6 dB of the actual implementation; however, higher
variations can be detected as a result of phase shift in the filter, especially in second-order harmonic
performance.
This worst-case spur calculation assumes that the amplifier and filter spur of interest is in phase with the
corresponding spur in the ADC, such that the two spur amplitudes can be added linearly. There are two phase-
shift mechanisms that cause the measured distortion performance of the amplifier-ADC chain to deviate from the
expected performance calculated using Equation 10: common-mode phase shift and differential phase shift.
Common-mode phase shift is the phase shift detected equally in both branches of the differential signal path
including the filter. Common-mode phase shift nullifies the basic assumption that the amplifier, filter, and ADC
spur sources are in phase. This phase shift can lead to better performance than predicted when the spurs
become phase shifted, and there is the potential for cancellation when the phase shift reaches 180°. However,
there is a significant challenge in designing an amplifier-ADC interface circuit to take advantage of a common-
mode phase shift for cancellation: the phase characteristic of the ADC spur sources are unknown, thus the
necessary phase shift in the filter and signal path for cancellation is also unknown.
Differential phase shift is the difference in the phase response between the two branches of the differential filter
signal path. Differential phase shift in the filter as a result of mismatched components caused by nominal
tolerance can severely degrade the even-order distortion of the amplifier-ADC chain. This effect has the same
result as mismatched path lengths for the two differential traces, and causes more phase shift in one path than
the other. Ideally, the phase response over frequency through the two sides of a differential signal path are
identical, such that even-order harmonics remain optimally out of phase and cancel when the signal is taken
differentially. However, if one side has more phase shift than the other, then the even-order harmonic
cancellation is not as effective.
Single-order RC filters cause very little differential phase shift with nominal tolerances of 5% or less, but higher-
order LC filters are very sensitive to component mismatch. For instance, a third-order Butterworth bandpass filter
with a 100-MHz center frequency and a 20-MHz bandwidth shows as much as 20° of differential phase
imbalance in a SPICE Monte Carlo analysis with 2% component tolerances. Therefore, while a prototype may
work, production variance is unacceptable. In ac-coupled applications that require second- and higher-order
filters between the LMH3401 and ADC, a transformer or balun is recommended at the ADC input to restore the
phase balance. For dc-coupled applications where a transformer or balun at the ADC input cannot be used,
using first- or second-order filters is recommended to minimize the effect of differential phase shift because of the
component tolerance.
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