Page 18 - PRINCIPLES OF QUANTUM MECHANICS as Applied to Chemistry and Chemical Physics
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1.2 Wave packet                           9

                        two speci®c examples for the functional form of A(k). However, in order to
                        evaluate the integral over k in equation (1.11), we also need to know the
                        dependence of the angular frequency ù on the wave number k.
                          In general, the angular frequency ù(k) is a function of k, so that the angular
                        frequencies in the composite wave Ø(x, t), as well as the wave numbers, vary
                        from one plane wave to another. If ù(k) is a slowly varying function of k and
                        the values of k are con®ned to a small range Äk, then ù(k) may be expanded
                        in a Taylor series in k about some point k 0 within the interval Äk

                                            dù              1 d ù
                                                                2
                                                                             2
                              ù(k) ˆ ù 0 ‡       (k ÿ k 0 ) ‡        (k ÿ k 0 ) ‡         (1:13)
                                            dk   0          2 dk  2  0
                        where ù 0 is the value of ù(k)at k 0 and the derivatives are also evaluated at k 0 .
                        We may neglect the quadratic and higher-order terms in the Taylor expansion
                        (1.13) because the interval Äk and, consequently, k ÿ k 0 are small. Substitu-
                        tion of equation (1.13) into the phase for each plane wave in (1.11) then gives

                                                                      dù
                                   kx ÿ ùt   (k ÿ k 0 ‡ k 0 )x ÿ ù 0 t ÿ   (k ÿ k 0 )t
                                                                      dk  0
                                                          "            #

                                                                dù
                                           ˆ k 0 x ÿ ù 0 t ‡ x ÿ      t (k ÿ k 0 )
                                                                 dk  0
                        so that equation (1.11) becomes
                                               Ø(x, t) ˆ B(x, t)e i(k 0 xÿù 0 t)          (1:14)
                        where
                                                     …
                                                  1   1       i[xÿ(dù=dk) 0 t](kÿk 0 )
                                       B(x, t) ˆ p   A(k)e              dk          (1:15)
                                                  2ð ÿ1
                        Thus, the wave packet Ø(x, t) represents a plane wave of wave number k 0 and
                        angular frequency ù 0 with its amplitude modulated by the factor B(x, t). This
                        modulating function B(x, t) depends on x and t through the relationship
                        [x ÿ (dù=dk) 0 t]. This situation is analogous to the case of two plane waves as
                        expressed in equations (1.7) and (1.8). The modulating function B(x, t)moves
                        in the positive x-direction with group velocity v g given by

                                                            dù
                                                     v g ˆ                                (1:16)
                                                            dk   0
                        In contrast to the group velocity for the two-wave case, as expressed in
                        equation (1.9), the group velocity in (1.16) for the wave packet is not uniquely
                        de®ned. The point k 0 is chosen arbitrarily and, therefore, the value at k 0 of the
                        derivative dù=dk varies according to that choice. However, the range of k is
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