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The Fourier Transform

We define the forward Fourier transform $\tilde{h}(f)$ of a time domain quantity $h(t)$ to be

\begin{displaymath}
\tilde{h}(f)=\int_{-\infty}^\infty dt h(t)  e^{- 2 \pi i f t}
\end{displaymath} (16.1)

and the inverse Fourier transform to be
\begin{displaymath}
h(t)=\int_{-\infty}^\infty df \tilde{h}(f)  e^{2 \pi i f t}.
\end{displaymath} (16.2)

If the function $h(t)$ is sampled at $N$ consecitive points with sampling interval $\Delta t$, that is
\begin{displaymath}
h_j \equiv h(t_j) ,\quad t_j = j\Delta t,
\end{displaymath} (16.3)

we only have $N$ input values, so we can only produce $N$ independent values for the Fourier transform. Further, we can only produce values in the interval $(-f_c,f_c)$ where $f_c$ is the Nyquist critical frequency
\begin{displaymath}
f_c = \frac{1}{2\Delta t}.
\end{displaymath} (16.4)

We compute estimates of the Fourier transform at the $N + 1$ discrete values
\begin{displaymath}
f_k \equiv \frac{k}{N\Delta t}\quad k = -\frac{N}{2},\ldots,\frac{N}{2}.
\end{displaymath} (16.5)

There are only $N$ independent values here as the extremevales of $k$ correspond to the upper and lower limites of the Nyquist critical frequency range and are equal. We now proceed to define the discrete Fourier transform. Consider
$\displaystyle \tilde{h}(f_k)$ $\textstyle =$ $\displaystyle \int_{-\infty}^\infty dt h(t)  e^{-2 \pi i f t}$ (16.6)
  $\textstyle \approx$ $\displaystyle \sum_{j=0}^{N-1} \Delta t  h(t_j) e^{-2 \pi i f_k t_j}$ (16.7)
  $\textstyle \approx$ $\displaystyle \Delta t \sum_{j=0}^{N-1} h_j e^{-2 \pi i j k / N} .$ (16.8)

According to T010095, we define the discrete Fourier transform (DFT) to be
\begin{displaymath}
\tilde{h}_k = \sum_{j=0}^{N-1} h_j e^{-i 2 \pi j k / N}
\end{displaymath} (16.9)

and then we can recover $\tilde{h}(f_k)$ by
\begin{displaymath}
\tilde{h}(f_k) = \Delta t  \tilde{h}_k.
\end{displaymath} (16.10)

The inverse Fourier transform is
\begin{displaymath}
h(t)=\int_{-\infty}^\infty dt \tilde{h}(f)  e^{2 \pi i f t} .
\end{displaymath} (16.11)

Using
\begin{displaymath}
\Delta f = f_{k+1} - f_k = \frac{k+1}{N\Delta t} - \frac{k}{N\Delta t} =
\frac{1}{N\Delta t}
\end{displaymath} (16.12)

we may write
$\displaystyle h(t_j)$ $\textstyle \approx$ $\displaystyle \sum_{k=0}^{N-1} \tilde{h}(f_k) e^{2 \pi i f_k t_j / N}
\Delta f$ (16.13)
  $\textstyle =$ $\displaystyle \sum_{k=0}^{N-1} \Delta \tilde{h}_k e^{2 \pi i j k / N}\frac{1}{N\Delta t}$ (16.14)
  $\textstyle =$ $\displaystyle \frac{1}{N} \sum_{k=0}^{N-1} \tilde{h}_k e^{2 \pi i j k / N}$ (16.15)

which is the inverse DFT according to T010095. Note that the LAL ``reverse'' DFT functions do not include the factor $1/N$ in their output.


next up previous contents index
Next: Power Spectral Densities Up: Conventions Previous: Conventions   Contents   Index
LAL test account 2003-10-23