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condensed matter physics Condensed matter physics is the field of physics that deals with the macroscopic and microscopic physical properties of matter, especially the solid and liquid State of matter, phases, that arise from electromagnetic forces between atoms and elec ...
, 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 In condensed matter physics and crystallography, the static structure factor (or structure factor for short) is a mathematical description of how a material scatters incident radiation. The structure factor is a critical tool in the interpretation ...
that considers correlations in both space ''and'' time. Experimentally, it can be accessed most directly by
inelastic neutron scattering Neutron scattering, the irregular dispersal of free neutrons by matter, can refer to either the naturally occurring physical process itself or to the man-made experimental techniques that use the natural process for investigating materials. Th ...
or X-ray Raman scattering. The dynamic structure factor is most often denoted S(\vec,\omega), where \vec (sometimes \vec) is a wave vector (or wave number for isotropic materials), and \omega a frequency (sometimes stated as energy, \hbar\omega). It is defined as: :S(\vec,\omega) \equiv \frac\int_^ F(\vec,t)\exp(i\omega t)\,dt Here F(\vec,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 In mathematics, the Fourier transform (FT) is an integral transform that takes a function as input then outputs another function that describes the extent to which various frequencies are present in the original function. The output of the tr ...
of the van Hove function G(\vec,t): :F(\vec,t) \equiv \int G(\vec,t)\exp (-i\vec\cdot\vec)\,d\vec 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 \rho: :F(\vec,t) = \frac\langle \rho_(t)\rho_(0) \rangle The dynamic structure is exactly what is probed in coherent inelastic neutron scattering. The
differential cross section In physics, the cross section is a measure of the probability that a specific process will take place in a collision of two particles. For example, the Rutherford cross-section is a measure of probability that an alpha particle will be deflect ...
is : :\frac = a^2\left(\frac\right)^ S(\vec,\omega) where a is the
scattering length The scattering length in quantum mechanics describes low-energy scattering. For potentials that decay faster than 1/r^3 as r\to \infty, it is defined as the following low-energy limit: : \lim_ k\cot\delta(k) =- \frac\;, where a is the scatterin ...
.


The van Hove function

The van Hove function for a spatially uniform system containing N point particles is defined as: :G(\vec,t) = \left\langle \frac \int \sum_^\sum_^N \delta vec'+\vec-\vec_j(t)delta vec'-\vec_i(0)d\vec' \right\rangle It can be rewritten as: :G(\vec,t) = \left\langle \frac\int \rho(\vec'+\vec,t)\rho(\vec',0) d\vec'\right\rangle


References


Further reading

* *Lovesey, Stephen W. (1986). Theory of Neutron Scattering from Condensed Matter - Volume I: Nuclear Scattering.
Oxford University Press Oxford University Press (OUP) is the publishing house of the University of Oxford. It is the largest university press in the world. Its first book was printed in Oxford in 1478, with the Press officially granted the legal right to print books ...
. . Condensed matter physics Neutron scattering {{scattering-stub