Unformatted text preview: The overlap between two arbitrary wave functions is da a a da a a I ∫ ∫ ∗ = > >< < >= >=< < ) ( ) (      φ . Transformation from Arep to Brep: Suppose there is another hermitian operator B op . > >= b b b B op   , where b is a continuous ( real ) variable. We can expand the ket  ψ > in terms of the eigenkets of B op ( the Brepresentation ) we get ∫ > >= db b b  ) (  with 1   = >< ∫ db b b . The coefficient functions ψ (a) are related to the coefficient functions ψ (a\b) by ∫ ∫ > < = > >< < >= >=< =< db b b a db b b a I a a a ) (       ) ( , where <ab> is the “transformation function”....
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This note was uploaded on 05/29/2011 for the course PHY 4064 taught by Professor Fields during the Spring '07 term at University of Florida.
 Spring '07
 FIELDS
 mechanics

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