Difference between revisions of "F(000)"
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The expression for a [[structure factor]] evaluated in the zeroth-order case <math>h=k=l=0</math> yields the result | The expression for a [[structure factor]] evaluated in the zeroth-order case <math>h=k=l=0</math> yields the result |
Latest revision as of 13:12, 6 February 2012
The expression for a structure factor evaluated in the zeroth-order case [math]h=k=l=0[/math] yields the result
[math]F(000) = [ (\sum f_{r} )^{\,2} + (\sum f_{i} )^{\,2} ]^{1/2}[/math]
where [math]f_{r}[/math] is the real part of the scattering factors at [math]\theta = 0^\circ[/math], [math]f_{i}[/math] is the imaginary part of the scattering factors at [math]\theta = 0^\circ[/math], [math]\theta[/math] is the Bragg angle, and the sum is taken over each atom in the unit cell.
[math]F(000)[/math] is computed without dispersion effects in electron-density calculation by Fourier inversion. In all cases, non-dispersive [math]F(000)[/math] is a structure factor and not a structure amplitude: it has both magnitude and a sign.
For X-rays non-dispersive [math]F(000)[/math] is positive definite and in many cases an integer (but it is not an integer for non-stoichiometric compounds). It counts the number of electrons in the cell.
For neutrons non-dispersive [math]F(000)[/math] is either positive or negative and counts the total nuclear scattering power in the cell.