Structure factor: Difference between revisions

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where <math>k</math> is the scattering wave-vector modulus
where <math>k</math> is the scattering wave-vector modulus


:<math>k= \frac{4 \pi }{\lambda \sin \left( \frac{\theta}{2}\right)}</math>
:<math>k= |\mathbf{k}|= \frac{4 \pi }{\lambda \sin \left( \frac{\theta}{2}\right)}</math>


The structure factor is basically a [[Fourier analysis | Fourier transform]] of the [[pair distribution function]] <math>{\rm g}(r)</math>.
The structure factor is basically a [[Fourier analysis | Fourier transform]] of the [[pair distribution function]] <math>{\rm g}(r)</math>,


At zero wavenumber, ''i.e.'' <math>|k|=0</math>,
:<math>S(|\mathbf{k}|)= 1 + \rho \int \exp (i\mathbf{k}\cdot \mathbf{r}) \mathrm{g}(r) ~\mathrm{d}\mathbf{r}</math>
 
At zero wavenumber, ''i.e.'' <math>|\mathbf{k}|=0</math>,


:<math>S(0) = k_BT \left. \frac{\partial \rho}{\partial p}\right\vert_T</math>
:<math>S(0) = k_BT \left. \frac{\partial \rho}{\partial p}\right\vert_T</math>

Revision as of 12:06, 5 August 2008

The structure factor, , for a monatomic system is defined by:


where is the scattering wave-vector modulus

The structure factor is basically a Fourier transform of the pair distribution function ,

At zero wavenumber, i.e. ,

References

  1. A. Filipponi, "The radial distribution function probed by X-ray absorption spectroscopy", J. Phys.: Condens. Matter, 6 pp. 8415-8427 (1994)