This question says that RMS bandwidth (effective bandwidth) is defined based on the carrier frequency of a signal. This makes intuitive sense to me that the carrier frequency shouldn't determine the value of the RMS bandwidth, just the pulse shape. However looking at Parseval's Theorem it is not immediately clear to me that upconversion of a signal to bandpass plays out in this way. For example let $x(t)$ be a low pass signal with energy from -B to B in the frequency domain and let
$$s(t) = x(t)\cos(2\pi f_c t).$$
Then from Parseval's Theorem we have $$\int_{0}^{\infty}\bigg(\frac{\partial s(t)}{\partial t}\bigg)^2 dt = \int_{-\infty}^{\infty} f^2|S(f)|^2 df$$ $$= \int_{-(f_c + B)}^{-(f_c - B)} f^2 |X(f)|^2 df + \int_{f_c - B}^{f_c + B} f^2 |X(f)|^2 df$$
which leads me to believe that the energy relies upon the carrier frequency. What am I missing here? Please forgive any scaling factors, I'm concerned with the general behavior not if there is a constant multiplier. Thanks!