Unformatted text preview: ized to unity, times the remaining constant factors. Now imagine making the parameter a smaller and smaller, such that in the limit a → we recover the original integral. You will see that the normalized function in your result is more and more sharply peaked ab o ut x , while the area under this function remains equal to 1. In the limit a → this function becomes infinitely narrow and thus behaves as a function. Therefore establish the following relation: 2 ( ) ikx e dk x πδ ∞∞ = ∫ ....
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This note was uploaded on 02/08/2012 for the course CHEM 540 taught by Professor Mccall during the Fall '08 term at University of Illinois, Urbana Champaign.
 Fall '08
 Mccall

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