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Unformatted text preview: Physics 216 Solutions to the Midterm Exam Spring 2010 1. Suppose we define G ( t ) âĄ integraldisplay â ââ dxK ( x, t, ; x, 0) (1) where K ( x, t ; x â˛ , t â˛ ) is the propagator. Assume that the system has a timeindependent Hamiltonian and a discrete energy level spectrum. (a) Prove that the Fourier transform of G , tildewide G ( E ) âĄ lim ĮĢ â i planckover2pi1 integraldisplay â G ( t ) e iEt/ planckover2pi1 e â ĮĢt dt (2) has poles at all the discrete energy levels of the system. Take ĮĢ to be a positive infinitesimal quantity. Assuming that the Hamiltonian is timeindependent, the time evolution operator, defined by  Ī ( t ) ) = U ( t, t )  Ī ( t ) ) , is given by U ( t, t ) = e â iH ( t â t ) / planckover2pi1 . The propagator is defined by K ( x, t ; x â˛ , t â˛ ) = ( x â˛  U ( t, t )  x ) . We also assume that the spectrum of H consists of a discrete set of energy eigenvalues. Denoting the corresponding energy eigenstates by  n ) , K ( x, t ; x â˛ , t â˛ ) = summationdisplay n ( x â˛  e â iH ( t â t â˛ ) / planckover2pi1  n )( n  x ) = summationdisplay n e â iE n ( t â t â˛ ) / planckover2pi1 ( x â˛  n )( n  x ) , where H  n ) = E n  n ) . Using G ( t ) = integraldisplay â ââ dxK ( x, t ; x, 0) = summationdisplay n e â iE n t/ planckover2pi1 integraldisplay â ââ dx ( n  x ) 2 = summationdisplay n e â iE n t/ planckover2pi1 , (3) since the last integral is equal to 1 by the normalization condition of the energy eigenstates. Hence, using eq. (3) it follows that for any positive infinitesimal ĮĢ , tildewide G ( E ) âĄ lim ĮĢ â i planckover2pi1 integraldisplay â G ( t ) e iEt/ planckover2pi1 e â ĮĢt dt = lim ĮĢ â i planckover2pi1 summationdisplay n integraldisplay â e i ( E â E n ) t/ planckover2pi1 e â ĮĢt dt = summationdisplay n 1 E n â E , which has poles precisely at the discrete energy levels of the system. 1 (b) Consider the harmonic oscillator with a charge e in one dimension. You are asked to calculate the discrete energy levels of the system, when it is placed in a uniform electric field of strength E . Compute the levels in three independent ways: (i) using the WKB approximation; (ii) using the path integral technique; (iii) solving the Schrodinger equation exactly. Do you expect the same result from all three methods? The Lagrangian for the system is L = 1 2 m Ë x 2 â 1 2 mĪ 2 x 2 + e E x. (i) To compute the energy levels in the WKB approximation, we must compute the turning points of the potential, V ( x ) = 1 2 mĪ 2 x 2 â e E x. (4) The turning points are determined by setting V ( x ) = E , where E is the energy, and solving for x . The resulting equation is: x 2 â 2 e E x mĪ 2 â eE mĪ 2 = 0 ....
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This document was uploaded on 10/31/2011.
 Spring '09
 Energy

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