Sorta.
Cross-correlation and convolution are closely linked. Cross-correlation of $f(t)$ and $g(t)$ is the same as the convolution of $\bar{f}(-t)$ and $g(t)$, where $\bar{f}$ is the complex conjugate of $f$.
For certain types of $f$s, called Hermitian functions, cross correlation and convolution and convolution would produce exactly the same results. Thus, you're correct that convolution and cross-correlation can sometimes be interchanged. Even if your function is not Hermitian, you might be able to get away with using either method, depending on your goal.
However, neither cross-correlation nor convolution necessarily involve a Fourier transform. Both transforms are defined has happening purely in the time domain, and a naive implementation would just operate there.
That said, the Convolution Theorem says that convolution in one domain is equivalent to element-wise multiplication in the other. That is
$$\mathscr{F}(f\ast g) = \mathscr{F}(f) \cdot \mathscr{F}(g)$$
where $\mathscr{F}$ is the Fourier transform$^1$.
With a little bit of rearrangement$, one can instead write
$$f \ast g = \mathscr{F}^{-1}\big(\mathscr{F}(f) \cdot \mathscr{F}(g)\big)$$
uses the Fourier transform to compute convolution. Similar logic lets one compute the cross correlation in the same way:
$$ f \star g = \mathscr{F}^{-1} \bigg( \overline{\mathscr{F}(f)} \cdot \mathscr{F}(g)\bigg)$$
This may seem like a round-about way of performing convolution, but it can often be more efficient. Convolving two sequences of length $n$ in the time domain requires $O\bigl(n^2\bigr)$ time. However, the Fourier transform can be performed in $O\bigl(n \log n\bigr)$ time$^2$ each while the pointwise multiplication takes $O(n)$ time. If your sequences are large and of approximately equal size, this approach can be faster.
1. You may need to correct for a normalizing factor of $2\pi$ or its square root, depending on how you defined the Fourier transform.
2.In addition to the asymptotic speed-up, many FFT implementations are incredibly well-tuned, so this works both in theory and in practice! FFTW is a good place to start if you're curious about that.