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Quantum Mechanics Problem 2, 2017 Due: Wednesday, March 15 every day of delay results in 20% reduction of the mark Consider a quantum system in which an electron can move freely in the xy-plane while its motion in the z-direction is restricted by the potential U (x, z) = mω 2 z 2 , 2 where m is the effective electron mass and ω is a parameter of the confining potential. A uniform magnetic field B = (B, 0, 0) directed along the x-axis is applied to the system. Use the gauge A = (0, −Bz, 0) for the vector potential. A. Write down the Hamiltonian of the electron. B. Using separation of variables, ψ(x, y, z) = eipx x/h̄ eipy y/h̄ ϕ(z) , solve the Schrodinger equation and find energy levels of the electron. Notice that the motion within the xy-plane is described by a plane wave. C. Using the result obtained in part B determine the electron dispersion p2y p2x = 0 + + , 2m∗x 2m∗y Hence determine (i) the formula for 0 which depends on the transverse quantum number, and (ii) formulas for the effective masses m∗x and m∗y . D. Consider the following values of the parameters m = 0.1me h̄ω = 10 meV B = 10 T esla , where me is the free electron mass. Find the values of m∗x and m∗y in units of me .