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Unformatted text preview: University of Colorado, Department of Physics PHYS3220, Fall 09, HW#11 due Wed, Nov 4, 2PM at start of class 1. Analytic solution of the harmonic oscillator (Total: 20 pts) In this problem we go through the analytic solution of the timeindependent Schr¨ odinger equation for the harmonic oscillator ~ 2 2 m d 2 χ ( x ) dx 2 + 1 2 mω 2 x 2 χ ( x ) = Eχ ( x ) (1) a) It is convenient to simplify the problem by introducing the two dimensionless variables ξ = p mω ~ x and K = 2 E ~ ω Show that the timeindependent Schr¨ odinger equation can be written as d 2 χ ( ξ ) dξ 2 = ( ξ 2 K ) χ ( ξ ) b) Show that in the limit  x  → ∞ the above equation can be approximated as d 2 χ ( ξ ) dξ 2 ≈ ξ 2 χ ( ξ ) and an approximate solution is given by χ ( ξ ) ≈ A exp( ξ 2 / 2) + B exp(+ ξ 2 / 2) What is the constraint needed to be sure that χ ( ξ ) can be normalized? (Don’t actually try to normalize the function.) c) The original equation turns out to simplify if we extract the asymptotic (large...
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This note was uploaded on 02/27/2012 for the course PHYSICS 3220 taught by Professor Stevepollock during the Fall '08 term at Colorado.
 Fall '08
 STEVEPOLLOCK
 Physics

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