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Unformatted text preview: the experimentally observed quantisation of observables such as energy. Eigenfunctions of The operator multiplies with . Solving the equation (8.11 ) we find that the solution must be exactly localised at . The function that does that is called a Dirac function . This is defined through integration, (8.12 ) and is not normalisable, (8.13 ) © 2005 Niels Walet, University of Manchester...
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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