This preview shows page 1. Sign up to view the full content.
40.10: , 2 2 2 ψ k dx ψ d - = and for ψ to be a solution of Eq. . 2 8 ), 3 . 40 ( 2 2 2 2 m E h m π E k = = b) The wave function must vanish at the rigid walls; the given function will vanish at
This is the end of the preview. Sign up to access the rest of the document.
This note was uploaded on 04/17/2008 for the course PHYS 2306 taught by Professor Ykim during the Spring '06 term at Virginia Tech.
- Spring '06