Tables for
Volume B
Reciprocal space
Edited by U. Shmueli

International Tables for Crystallography (2006). Vol. B, ch. 1.2, p. 10   | 1 | 2 |

Section 1.2.2. General scattering expression for X-rays

P. Coppensa*

aDepartment of Chemistry, Natural Sciences & Mathematics Complex, State University of New York at Buffalo, Buffalo, New York 14260-3000, USA
Correspondence e-mail:

1.2.2. General scattering expression for X-rays

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The total scattering of X-rays contains both elastic and inelastic components. Within the first-order Born approximation (Born, 1926[link]) it has been treated by several authors (e.g. Waller & Hartree, 1929[link]; Feil, 1977[link]) and is given by the expression [I_{\rm total} ({\bf S}) = I_{\rm classical} {\textstyle\sum\limits_{n}} \left|{\textstyle\int} \psi_{n}^{*} \exp (2\pi i{\bf S}\cdot {\bf r}_{j}) \psi_{0}\; \hbox{d}{\bf r}\right|^{2}, \eqno(] where [I_{\rm classical}] is the classical Thomson scattering of an X-ray beam by a free electron, which is equal to [(e^{2}/mc^{2})^{2} (1 + \cos^{2} 2\theta)/2] for an unpolarized beam of unit intensity, ψ is the n-electron space-wavefunction expressed in the 3n coordinates of the electrons located at [{\bf r}_{j}] and the integration is over the coordinates of all electrons. S is the scattering vector of length [2\sin \theta/\lambda].

The coherent elastic component of the scattering, in units of the scattering of a free electron, is given by [I_{\rm coherent, \, elastic} ({\bf S}) = \left|{\textstyle\int} \psi_{0}^{*}\right| {\textstyle\sum\limits_{j}} \exp (2\pi i{\bf S}\cdot {\bf r}_{j}) |\psi_{0} \;\hbox{d}{\bf r}|^{2}. \eqno(]

If integration is performed over all coordinates but those of the jth electron, one obtains after summation over all electrons [I_{\rm coherent, \, elastic} ({\bf S}) = |{\textstyle\int} \rho ({\bf r}) \exp (2\pi i{\bf S}\cdot {\bf r}) \;\hbox{d}{\bf r}|^{2}, \eqno(] where [\rho({\bf r})] is the electron distribution. The scattering amplitude [A({\bf S})] is then given by [A({\bf S}) = {\textstyle\int} \rho ({\bf r}) \exp (2\pi i{\bf S}\cdot {\bf r}) \;\hbox{d}{\bf r} \eqno(] or [A({\bf S}) = \hat{F} \{\rho ({\bf r})\}, \eqno(] where [\hat{F}] is the Fourier transform operator.


Born, M. (1926). Quantenmechanik der Stoszvorgänge. Z. Phys. 38, 803.Google Scholar
Feil, D. (1977). Diffraction physics. Isr. J. Chem. 16, 103–110.Google Scholar
Waller, I. & Hartree, D. R. (1929). Intensity of total scattering X-rays. Proc. R. Soc. London Ser. A, 124, 119–142.Google Scholar

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