Page 102 - PRINCIPLES OF QUANTUM MECHANICS as Applied to Chemistry and Chemical Physics
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3.7 Postulates of quantum mechanics               93
                                                       @Ø
                                                              ^
                                                     i"    ˆ HØ                           (3:55)
                                                        @t
                              ^
                        where H is the Hamiltonian operator of the system and, in general, changes
                        with time. However, in this book we only consider systems for which the
                        Hamiltonian operator is time-independent. To solve the time-dependent SchroÈ-
                        dinger equation, we express the state function Ø(q, t) as the product of two
                        functions
                                                   Ø(q, t) ˆ ø(q)÷(t)                     (3:56)
                        where ø(q) depends only on the spatial variables and ÷(t) depends only on the
                        time. In Section 2.4 we discuss the procedure for separating the partial
                        differential equation (3.55) into two differential equations, one involving only
                        the spatial variables and the other only the time. The state function Ø(q, t)is
                        then shown to be
                                                 Ø(q, t) ˆ ø(q)e ÿiEt="                   (3:57)

                        where E is the separation constant. Since it follows from equation (3.57) that
                                                          2         2
                                                  jØ(q, t)j ˆjø(q)j
                        the probability density is independent of the time t and Ø(q, t)isa stationary
                        state.
                          The spatial differential equation, known as the time-independent Schrodin-
                                                                                           È
                        ger equation, is
                                                    ^
                                                    Hø(q) ˆ Eø(q)
                        Thus, the spatial function ø(q) is actually a set of eigenfunctions ø n (q) of the
                                            ^
                        Hamiltonian operator H with eigenvalues E n . The time-independent SchroÈdin-
                        ger equation takes the form
                                                   ^
                                                  Hø n (q) ˆ E n ø n (q)                  (3:58)
                        and the general solution of the time-dependent Schrodinger equation is
                                                                      È
                                                       X
                                             Ø(q, t) ˆ     c n ø n (q)e ÿiE n t="         (3:59)
                                                         n
                        where c n are arbitrary complex constants.
                          The appearance of the Hamiltonian operator in equation (3.55) as stipulated
                        by postulate 5 gives that operator a special status in quantum mechanics.
                        Knowledge of the eigenfunctions and eigenvalues of the Hamiltonian operator
                        for a given system is suf®cient to determine the stationary states of the system
                        and the expectation values of any other dynamical variables.
                          We next address the question as to whether equation (3.59) is actually the
                                                                      È
                        most general solution of the time-dependent Schrodinger equation. Are there
                        other solutions that are not expressible in the form of equation (3.59)? To
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