# 31.5: The Structure Factor and the Electron Density Are Related by a Fourier Transform

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## Fourier Transform

In mathematics, a Fourier transform is an operation that converts one real function into another. In the case of FTIR, a Fourier transform is applied to a function in the time domain to convert it into the frequency domain. One way of thinking about this is to draw the example of music by writing it down on a sheet of paper. Each note is in a so-called "sheet" domain. These same notes can also be expressed by playing them. The process of playing the notes can be thought of as converting the notes from the "sheet" domain into the "sound" domain. Each note played represents exactly what is on the paper just in a different way. This is precisely what the Fourier transform process is doing to the collected data of x-ray diffraction. This is done in order to determine the electron density around the crystalline atoms in real space. In the previous section, we treated the lattice points as individual, localized electron densities. In reality, the electron density of a unit cell is distributed over a much larger space. The following equations can be used to determine the electrons' positions:

\[p(x,y,z) = \sum_{h=-\infty}^{\infty} \sum_{k=-\infty}^{\infty} \sum_{l=-\infty}^{\infty}F(hkl) e ^{-2\pi i (hx/a+ky/b+lz/c)} \label{1}\]

Employing a Fourier transform

\[F(hkl) \propto \int _{-\infty}^{\infty} \int _{-\infty}^{\infty} \int _{-\infty}^{\infty} p(x,y,z) e ^{2\pi i (hx/a+ky/b+lz/c)} dx\;dy\;dz \label{2}\]

\[F(q) = | F(q) | e^{i \phi(q)} \label{3}\]

where \(p(xyz)\) is the electron density function, and \(F(hkl)\) is the electron density function in real space. Equation \(\ref{2}\) represents the Fourier expansion of the electron density function. To solve for \(F(hkl)\), equation \(\ref{1}\) needs to be evaluated over all values of h, k, and l, resulting in equation \(\ref2\). The resulting function \(F(hkl)\) is generally expressed as a complex number (as seen in equation \(\ref{3}\) above) with \(| F(q)|\) representing the magnitude of the function and \(\phi\) representing the phase.

The structure factor may also be expressed as

\[ \begin{align} \mathbf{F}_{hkl} &= F_{hkl} e^{i\alpha_{hkl}} = \sum_j f_je^{2\pi i (hx_j + ky_j + lz_j)} = \sum_j f_j\cos[2\pi (hx_j + ky_j + lz_j)] + i\sum_{j} f_j\sin[2\pi (hx_j + ky_j + lz_j)] \\[4pt] &= A_{hkl} + iB_{hkl} \end{align}\]

where the sum is over all atoms in the unit cell, *x*_{j},*y*_{j},*z*_{j} are the positional coordinates of the *j *th atom, *f*_{j} is the scattering factor of the *j *th atom, and \(α_{hkl}\) is the phase of the diffracted beam.The intensity of a diffracted beam is directly related to the amplitude of the structure factor, but the phase must normally be deduced by indirect means. In structure determination, phases are estimated and an initial description of the positions and anisotropic displacements of the scattering atoms is deduced. From this initial model, structure factors are calculated and compared with those experimentally observed. Iterative refinement procedures attempt to minimize the difference between calculation and experiment until a satisfactory fit has been obtained.

Figure \(\PageIndex{1}\) shows an electron density map of a quinoline derivative (and one water molecule) that was determined from X-ray diffraction data.

## Contributor

Tom Neils - Grand Rapids Community College