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note
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Originally we chose a Fibonacci model in order to exploit analytic and experimental work on localization and band gaps (e.g., [44]). However, in practice even computer-numerically-controlled machining of the grooves resulted in small random variations, as revealed by high-resolution optical scans [31]. Numerical modeling shows that these small variations are visible in the multiple scattering coda. Hence, for this work the model is effectively random.
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