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A barrier of arbitrary shape can be approximated as a succession of square barriers, as shown in Figure P7.15. Write the transmission coefficient for this barrier using the result of Equation 7.9 for each of the individual barriers, assuming the transmitted wave intensity for one becomes the incident wave intensity for the barrier immediately following it in the series. Show that the form of Equation 7.10 is recovered in the case where E<U and αL ≫1 | Numerade
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