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Unformatted text preview: (6.9) Even though we have given up normalisability, we still have the two continuity conditions. At these imply, using continuity of and , (6.10) (6.11) We thus find (6.12) (6.13) and the reflection and transmission coefficients can thus be expressed as (6.14) (6.15) Notice that ! Figure 6.2: The transmission and reflection coefficients for a square barrier. In Fig. 6.2 we have plotted the behaviour of the transmission and reflection of a beam of Hydrogen atoms impinging on a barrier of height 2 meV....
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This note was uploaded on 11/09/2011 for the course PHY PHY2053 taught by Professor Davidjudd during the Fall '10 term at Broward College.
- Fall '10