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4.2 Quantum treatment                       111
                                                        ^
                                                             y
                                                        N   ^ a ^ a                       (4:21)
                                     ^
                        The adjoint of N may be obtained as follows
                                                                          ^
                                            ^
                                            N ˆ (^ a ^ a) ˆ ^ a (^ a ) ˆ ^ a ^ a ˆ N
                                              y
                                                           y
                                                              y y
                                                                    y
                                                   y
                                                      y
                                                                                       ^
                        where the relations (3.40) and (3.37) have been used. We note that N is self-
                        adjoint, making it hermitian and therefore having real eigenvalues. Equation
                        (4.19b) may now be written in the form
                                                    ^
                                                             ^
                                                                 1
                                                    H ˆ "ù(N ‡ )                          (4:22)
                                                                 2
                              ^
                                     ^
                        Since H and N differ only by the factor "ù and an additive constant, they
                        commute and, therefore, have the same eigenfunctions.
                                                ^
                          If the eigenvalues of N are represented by the parameter ë and the
                        corresponding orthonormal eigenfunctions by ö ëi (î) or, using Dirac notation,
                        by jëii, then we have
                                                     ^
                                                     Njëiiˆ ëjëii                         (4:23)
                        and
                                     ^           ^   1               1
                                     Hjëiiˆ "ù(N ‡ )jëiiˆ "ù(ë ‡ )jëiiˆ E ë jëii          (4:24)
                                                     2               2
                                                                                   ^
                        Thus, the energy eigenvalues E ë are related to the eigenvalues of N by
                                                    E ë ˆ (ë ‡ )"ù                        (4:25)
                                                              1
                                                              2
                        The index i in jëii takes on integer values from 1 to g ë , where g ë is the
                                                                                              ^
                        degeneracy of the eigenvalue ë. We shall ®nd shortly that each eigenvalue of N
                        is non-degenerate, but in arriving at a general solution of the eigenvalue
                        equation, we must initially allow for degeneracy.
                                                                                  ^
                          From equations (4.20) and (4.21), we note that the product of N and either ^ a
                        or ^ a may be expressed as follows
                           y
                                 ^
                                                                          ^
                                                              y
                                                 y
                                        y
                                 N^ a ˆ ^ a ^ a^ a ˆ (^ a^ a ÿ 1)^ a ˆ ^ a(^ a ^ a ÿ 1) ˆ ^ a(N ÿ 1)  (4:26a)
                                                                        ^
                                         ^
                                                                      y
                                         N^ a ˆ ^ a ^ a^ a ˆ ^ a (^ a ^ a ‡ 1) ˆ ^ a (N ‡ 1)  (4:26b)
                                                            y
                                                 y
                                                    y
                                            y
                                                         y
                        These identities are useful in the following discussion.
                                              ^
                          If we let the operator N act on the function ^ ajëii, we obtain
                                   ^           ^
                                   N^ ajëiiˆ ^ a(N ÿ 1)jëiiˆ ^ a(ë ÿ 1)jëiiˆ (ë ÿ 1)^ ajëii  (4:27)
                        where equations (4.23) and (4.26a) have been introduced. Thus, we see that
                                                  ^
                        ^ ajëii is an eigenfunction of N with eigenvalue ë ÿ 1. The operator ^ a alters the
                                                         ^
                        eigenstate jëii to an eigenstate of N corresponding to a lower value for the
                        eigenvalue, namely ë ÿ 1. The energy of the oscillator is thereby reduced,
                        according to (4.25), by "ù. As a consequence, the operator ^ a is called a
                        lowering operator or a destruction operator.
                                 ^
                          Letting N operate on the function ^ a jëii gives
                                                          y
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