Taking the derivative multiplies the transform by s, which effectively rotates the magnitude graph counterclockwise. Thus, may well be higher frequency components in the derivative. A more succinct way to put this is that derivation amplifies the high frequency content.
The Laplace Transform \$ \frac{1}{s+1} \$ (which would be the step response of a single pole high-pass filter)
bode(tf(1, [ 1 1 ]))

The Laplace Transform of it's derivative, \$ \frac{s}{s+1} \$
bode(tf([1 0], [ 1 1 ]))

The derivative in this case clearly has higher frequency components. Perhaps more correctly, it has much larger high frequency components than the non-derivative. One might choose to sample the first signal at 200 rads/s with some confidence, as the energy is very small at the nyquist rate, but aliasing would be substantial if you sampled the derivative at the same rate.
Thus, it depends on the nature of the signal. The derivative of a sinusoid will be a sinusoid of the same frequency, but the derivative of band limited noise will have higher frequency components than the noise.
EDIT: In response to the downvote, I'll hammer this home with a concrete example. Let me take a sine wave, and add some random normal noise to it (one tenth the magnitude of the sine wave)
The fft of this signal is:

Now, let me take the derivative of the signal:

and the fft of the derivative

Undersampling will, of course, alias either the signal or the derivative. The effects of the undersampling will be modest for the signal, and the result of undersampling the derivative will be absolutely useless.