GPED Simulator Gas Phase Electron Diffraction |
Douglas
Cameron |
Finite Temperature Approximation
As an approximation to full molecular dynamics (here) this program approximates the effects of molecular vibration by broadening the intermolecular distances with a parameter q which is proportional to temperature.
The RMS amplitude, lij,
between two atoms is q*sqrt(rij). Then, for example with C60
which has only carbon, the scattered intensity is computed as:
intensity(s) = Sum over i,j of: f02 * sin(s*(rij-lij2/rij)
)/(s*rij) * exp(-0.5*(lij*s)2)
The lij distribution most closely matches Hedberg's T=1003K data with q=0.055.