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4

                                                    Harmonic oscillator
















                             In this chapter we treat in detail the quantum behavior of the harmonic
                             oscillator. This physical system serves as an excellent example for illustrating
                             the basic principles of quantum mechanics that are presented in Chapter 3. The
                                 È
                             Schrodinger equation for the harmonic oscillator can be solved rigorously and
                             exactly for the energy eigenvalues and eigenstates. The mathematical process
                             for the solution is neither trivial, as is the case for the particle in a box, nor
                             excessively complicated. Moreover, we have the opportunity to introduce the
                             ladder operator technique for solving the eigenvalue problem.
                               The harmonic oscillator is an important system in the study of physical
                             phenomena in both classical and quantum mechanics. Classically, the harmonic
                             oscillator describes the mechanical behavior of a spring and, by analogy, other
                             phenomena such as the oscillations of charge ¯ow in an electric circuit, the
                             vibrations of sound-wave and light-wave generators, and oscillatory chemical
                             reactions. The quantum-mechanical treatment of the harmonic oscillator may
                             be applied to the vibrations of molecular bonds and has many other applica-
                             tions in quantum physics and ®eld theory.



                                                      4.1 Classical treatment

                             The harmonic oscillator is an idealized one-dimensional physical system in
                             which a single particle of mass m is attracted to the origin by a force F
                             proportional to the displacement of the particle from the origin
                                                             F ˆÿkx                             (4:1)
                             The proportionality constant k is known as the force constant. The minus sign
                             in equation (4.1) indicates that the force is in the opposite direction to the
                             direction of the displacement. The typical experimental representation of the
                             oscillator consists of a spring with one end stationary and with a mass m

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