MIT OpenCourseWarehttp://ocw.mit.edu 5.74 Introductory Quantum Mechanics II Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.5.74, Problem Set #0 Spring 2009 Not graded These are some problems to make sure that you are up to speed on the basics of solving numerical problems. 1. Numerically solving for eigenstates and eigenvalues of an arbitrary 1D potential. Obtain the energy eigenvalues En and wavefunctions ψ(r) for the anharmonic Morse npotential below. (Values of the parameters correspond to HF). Tabulate En for n = 0 to 5, and plot the corresponding ψ n(r) . VD= e⎡⎣1− e−α x⎤⎦ 2 Equilibrium bond energy: De = 6.091×10-19 J Equilibrium bond length: r0 = 9.109×10-11 m =− r0xr Force constant: k = 1.039×103 J m-2 α= kD2 e(If you aren’t familiar with these problems, study the notes and worksheets on the Discrete Value Representation). 2. Resonant driving of two level system. If two states k and l are coupled with a sinusoidal potential, the differential equations that describe their probability amplitude are b& k = 2 − h ibl Vkl ei(ωkl −ω)t b&l =−ibkVlke−i(ωkl −ω)t 2h Numerically solve for the probability of being in state k and l for times t = 0 to t =1 ps given that the system is in state k at t = 0. You can take the coupling to be Vh/ c = 100 cm−1 . Compare the behavior for detuning from resonance oflk(ωkl−ω) /2π c = 0 cm−1 and 100 cm−1. (If you aren’t familiar with numerically solving differential equations, study your software’s implementation of the Runga-Kutta
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