Diffraction by Organized Layers — Question 6

Section 36-9 · Physics pages 6022–6023

Question 6 Different basis atoms can restore a reflection that equal atoms cancel A cubic lattice has a two-atom basis at (0, 0, 0) and (1/2, 1/2, 1/2), with real amplitudes fA and fB. Its structure factor is F = fA + fB(−1)h+k+l. Take fA = 2fB = 2f. Compare structure factors alone, neglecting angle-dependent experimental factors. a A B Schematic; labels, not drawing lengths, specify the data. (a) Find the even-sum and odd-sum reflection intensities and their ratio. (b) Derive the general odd-to-even intensity ratio and its equal-atom limit.
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Question 6 - Solution Different basis atoms can restore a reflection that equal atoms cancel a A B (a) Method and calculation h + k + l even : F = 3f; h + k + l odd : F = f. Ieven ∝9f2, Iodd ∝f2, Iodd/Ieven = 1/9 . (b) Interpretation and further calculation Iodd/Ieven = fA −fB fA + fB 2 . fA = fB =⇒Iodd = 0 . Physical check With unlike atoms the half-cell translation no longer reproduces an identical scattering environment; the equal-atom extinction need not survive.

Question 6

Different basis atoms can restore a reflection that equal atoms cancel

A cubic lattice has a two-atom basis at (0,0,0)(0,0,0) and (1/2,1/2,1/2)(1/2,1/2,1/2), with real amplitudes fAf_A and fBf_B. Its structure factor is F=fA+fB(−1)h+k+lF=f_A+f_B(-1)^{h+k+l}. Take fA=2fB=2ff_A=2f_B=2f. Compare structure factors alone, neglecting angle-dependent experimental factors.

Diagram shown in the original SVG worksheet.

  1. Find the even-sum and odd-sum reflection intensities and their ratio.

  2. Derive the general odd-to-even intensity ratio and its equal-atom limit.

Question 6 - Solution

Different basis atoms can restore a reflection that equal atoms cancel

Diagram shown in the original SVG worksheet.

(a) Method and calculation

h+k+leven:F=3f;h+k+lodd:F=f.h+k+l\ \text{even}:\ F=3f;\qquad h+k+l\ \text{odd}:\ F=f.Ieven∝9f2,Iodd∝f2,Iodd/Ieven=1/9.\boxed{I_{\mathrm{even}}\propto9f^2,\quad I_{\mathrm{odd}}\propto f^2,\quad I_{\mathrm{odd}}/I_{\mathrm{even}}=1/9}.

(b) Interpretation and further calculation

Iodd/Ieven=|fA−fBfA+fB|2.\boxed{I_{\mathrm{odd}}/I_{\mathrm{even}}=\left|\frac{f_A-f_B}{f_A+f_B}\right|^2}.fA=fB⇒Iodd=0.f_A=f_B\Longrightarrow\boxed{I_{\mathrm{odd}}=0}.

Physical check

With unlike atoms the half-cell translation no longer reproduces an identical scattering environment; the equal-atom extinction need not survive.