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Figure 6
Flat-plate (transmission) geometry. Same colour scheme as in Fig. 4[link]. Here again we set [Z_{l\semi m,0} = \pm (2l+1)], its upper bound from equation (14)[link]. Negative intensity regions again indicate the need for tighter bounds on the coefficients. (Top) [{\cal S}(Q)] and its modification with the (2,0) component; (middle) with the (8,0) component; (bottom) with the (8,4) component.

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