Structure factor: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) No edit summary |
Carl McBride (talk | contribs) mNo edit summary |
||
Line 6: | Line 6: | ||
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 11:06, 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. ,