Replace the slowly varying interior wave by C and eik∣x−x′∣ by one when both arguments lie within the range. The integral equation givesHenceThe integrated strength has dimensions of energy times length. For U=−αδ(x), γ=−α and this is exactly the result in part c. For a regular weak potential the approximation sums the important ratio mγ/(kℏ2) without requiring it to be small, which is why it remains useful beyond the naive first Born expansion at small momentum.
C=1−kℏ2imγC,γ=∫−∞∞U(x)dx.
C=t≃1+imγ/(kℏ2)1,r≃C−1.
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