Dynamic structure factor

In condensed matter physics, the dynamic structure factor (or dynamical structure factor) is a mathematical function that contains information about inter-particle correlations and their time evolution. It is a generalization of the structure factor that considers correlations in both space and time. Experimentally, it can be accessed most directly by inelastic neutron scattering or X-ray Raman scattering.

The dynamic structure factor is most often denoted ${\displaystyle S({\vec {k}},\omega )}$, where ${\displaystyle {\vec {k}}}$ (sometimes ${\displaystyle {\vec {q}}}$) is a wave vector (or wave number for isotropic materials), and ${\displaystyle \omega }$ a frequency (sometimes stated as energy, ${\displaystyle \hbar \omega }$). It is defined as:^[1]

${\displaystyle S({\vec {k}},\omega )\equiv {\frac {1}{2\pi }}\int _{-\infty }^{\infty }F({\vec {k}},t)\exp(i\omega t)\,dt}$

Here ${\displaystyle F({\vec {k}},t)}$, is called the intermediate scattering function and can be measured by neutron spin echo spectroscopy. The intermediate scattering function is the spatial Fourier transform of the van Hove function ${\displaystyle G({\vec {r}},t)}$:^[2][3]

${\displaystyle F({\vec {k}},t)\equiv \int G({\vec {r}},t)\exp(-i{\vec {k}}\cdot {\vec {r}})\,d{\vec {r}}}$

Thus we see that the dynamical structure factor is the spatial and temporal Fourier transform of van Hove's time-dependent pair correlation function. It can be shown (see below), that the intermediate scattering function is the correlation function of the Fourier components of the density ${\displaystyle \rho }$:

${\displaystyle F({\vec {k}},t)={\frac {1}{N}}\langle \rho _{\vec {k}}(t)\rho _{-{\vec {k}}}(0)\rangle }$

The dynamic structure is exactly what is probed in coherent inelastic neutron scattering. The differential cross section is :

${\displaystyle {\frac {d^{2}\sigma }{d\Omega d\omega }}=a^{2}\left({\frac {E_{f}}{E_{i}}}\right)^{1/2}S({\vec {k}},\omega )}$

where ${\displaystyle a}$ is the scattering length.