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The final expression of the integral becomes:
However, since the helix has a pitch P, the Bragg's law of diffraction gives
constructive interference only on layer lines determined by
where is the angle between unit vectors s and s o , and n is an integer. In
the near forward direction, the layer lines are shown in Fig. 8-1, with
specific values of equal to:
for a being very small. The integration over the entire length of z can be
replace by from 0 to P. Together with a change of variable,
the total amplitude of the diffracted beam, A(h) , is proportional to:
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