I Does Each Component of a Vector Have an Independent Fourier Transform?

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Is the Fourier transform of a function whose argument is a vector equivalent to performing a Fourier transform on the function of each vector component separately?
Given ##f(\vec{x})##, where the Fourier transform ##\mathcal{F}(f(\vec{x}))= \hat{f}(\vec{k})##.
Given ##\vec{x}=[x_1,x_2,x_3]## and ##\vec{k}=[k_1,k_2,k_3]##, is the following true?

\begin{equation}

\begin{split}

\mathcal{F}(f(x_1))&= \hat{f}(k_1)

\\

\mathcal{F}(f(x_2))&= \hat{f}(k_2)

\\

\mathcal{F}(f(x_3))&= \hat{f}(k_3)

\end{split}

\end{equation}

such that

\begin{equation}

\begin{split}

f(\vec{k})&= [\hat{f}(k_1), \hat{f}(k_1), \hat{f}(k_1)]

\end{split}

\end{equation}
 
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Your notation is not entirely clear to me. (Also, I think there are typos in (2)?)

In any case, I don't think what you want will work. Let's say that ##f## maps vectors to scalars. Then the Fourier transform ##\hat{f}## is still scalar-valued, but your vector of partial Fourier transforms is vector-valued.
 
You are correct; the equation should be the following:

\begin{equation}

\begin{split}

\hat{f}(\vec{k})&= [\hat{f}(k_1), \hat{f}(k_2), \hat{f}(k_3)]

\end{split}

\end{equation}

The Fourier transform maps vectors to vectors; otherwise one could not transform back from the Fourier conjugate space to the original vector space with the inverse Fourier transform. Information would have been lost in the mapping of a vector to a scalar.

That the Fourier conjugate of a vector is also a vector is seen in the variance relationship between Fourier conjugates, such as for example between position ##\vec{x}## and momentum ##\hbar \vec{k}##, where both are 3-vectors.
 
In your example ##f## is a scalar-valued function of 3 variables. It's Fourier transform is therefore a scalar-valued function of 3 variables. The forward and inverse transforms are then
##
\begin{eqnarray*}
\hat{f}(\vec{k}) & = & \int_{-\infty}^\infty f(\vec{x})\, e^{-i \vec{k}\cdot\vec{x}} \, d^3x\\
& = & \int_{-\infty}^\infty \int_{-\infty}^\infty \int_{-\infty}^\infty f(x_1,x_2,x_3)\, e^{-i (k_1 x_1 + k_2 x_2 + k_3 x_3)} \, dx_1 dx_2 dx_3 \\
f(\vec{x}) & = & \frac{1}{(2\pi)^3} \int_{-\infty}^\infty \hat{f}(\vec{k})\, e^{i \vec{k}\cdot\vec{x}} \, d^3k \\
& = & \frac{1}{(2\pi)^3} \int_{-\infty}^\infty \int_{-\infty}^\infty \int_{-\infty}^\infty \hat{f}(k_1,k_2,k_3)\, e^{i (k_1 x_1 + k_2 x_2 + k_3 x_3)} \, dk_1 dk_2 dk_3
\end{eqnarray*}
##

jason
 
Got it. My mistake.
 

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