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Unformatted text preview: The most general solution is x x De Ce x + + = ) ( 2 . Note that the wave function is not zero in the classically forbidden region. Region 3: In this region V(x) = 0 and hence ) ( ) ( 2 ) ( 2 2 2 2 x k x mE dx x d = = h with 2 2 h mE k = and m k E 2 2 2 h = The most general solution is ikx ikx Ge Fe x + + = ) ( 3 , but in this region G = 0 since there are no particles entering from the right traveling to the left in region 3. x x = 0 E Barrier Potential Classically Forbidden V Region 1 Region 2 Region 3 x = L...
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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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