CH 39 #35 - 2 d 2 U BE11 CE22 . 2m dx2 If were a solution...

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39.35: . 2 2 2 1 1 2 2 2 ψ CE ψ BE dx ψ d m + = + - If ψ were a solution with energy E , then 2 1 2 2 1 1 CEψ BEψ ψ CE ψ BE + = + or . ) ( ) ( 2 2 1 1 ψ E E C ψ E E B - = - This would mean that 1 ψ is a constant multiple of 2 1 2 and and , ψ ψ ψ would be wave functions
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