Application to the Electronic Maps of Contour

As a first implementation of the previous results, the Bragg s law for the central diffraction fringe can be considered, i.e., adapting the relation (5.5) to the actual needs  

Quantum Nanochemistry— Volume IV Quantum Solids and Orderability 

In any case, beyond the direct involvement of the Bragg s law in the above results, the problem of the phase determination appears, for the stmcture factor amplitude of Eqs. (5.259)-(5.261). 

Such a determination of the phase may use the real and imaginary components of the structure factor expression, since identified at exponential level with a generalized form of the relation (5.261) (Putz, 2003)  

Moreover, by Eq. (5.264) the ideal structure factor can be rewritten as a function of atomic scattering factors fj of the (/) atoms involved, i.e., contained on the diffraction planes and placed at the r distance towards the referential centered at the level of the unit cell, under the form prescribed by the transformation (5.48), as adapted to this analysis  

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