Page 220 - PRINCIPLES OF QUANTUM MECHANICS as Applied to Chemistry and Chemical Physics
P. 220

8.1 Permutations of identical particles           211
                                                     ^                                   (8:11a)
                                                     PØ S ˆ Ø S
                                                     ^
                                                     PØ A ˆÿØ A                          (8:11b)
                        The factor 2 ÿ1=2  in equations (8.10) normalizes Ø S and Ø A if Ø(1, 2) is
                        normalized. The combination Ø S is symmetric with respect to particle
                        interchange because it remains unchanged when the two particles are ex-
                        changed. The function Ø A , on the other hand, is antisymmetric with respect to
                        particle interchange because it changes sign, but is otherwise unchanged, when
                        the particles are exchanged.
                          The functions Ø A and Ø S are orthogonal. To demonstrate this property, we
                        note that the integral over all space of a function of two or more variables must
                        be independent of the labeling of those variables
                         …    …                           …    …
                               f (x 1 , ... , x N )dx 1 ... dx N ˆ       f (y 1 , ... , y N )dy 1 ... dy N (8:12)
                        In particular, we have
                                          ……                 ……
                                             f (1, 2) dq 1 dq 2 ˆ  f (2, 1) dq 1 dq 2
                        or
                                          hØ(1, 2)jØ(2, 1)iˆhØ(2, 1)jØ(1, 2)i             (8:13)

                        where f (1, 2) ˆ Ø (1, 2)Ø(2, 1). Application of equation (8.13) to hØ S jØ A i
                        gives
                                                            ^     ^
                                                hØ S jØ A iˆhPØ S jPØ A i                 (8:14)
                        Applying equations (8.11) to the right-hand side of (8.14), we obtain

                                                hØ S jØ A iˆÿhØ S jØ A i
                        Thus, the scalar product hØ S jØ A i must vanish, showing that Ø A and Ø S are
                        orthogonal.
                          If the wave function for the system is initially symmetric (antisymmetric),
                        then it remains symmetric (antisymmetric) as time progresses. This property
                                                          È
                        follows from the time-dependent Schrodinger equation
                                                @Ø(1, 2)
                                                            ^
                                              i"         ˆ H(1, 2)Ø(1, 2)                 (8:15)
                                                   @t
                              ^
                        Since H(1, 2) is symmetric, the time derivative @Ø=@t has the same symmetry
                        as Ø. During a small time interval Ät, therefore, the symmetry of Ø does not
                        change. By repetition of this argument, the symmetry remains the same over a
                        succession of small time intervals, and by extension over all time.
                          Since Ø S does not change and only the sign of Ø A changes if particles 1 and


                        2 are interchanged, the respective probability densities Ø Ø S and Ø Ø A are
                                                                            S
                                                                                       A
                        independent of how the particles are labeled. Neither speci®es which particle
   215   216   217   218   219   220   221   222   223   224   225