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ELECTRONIC CHARGE DENSITY OF QUANTUM SYSTEMS                          215






                        where we have set
                       Thus the integration in the time variable involved in eq. (B.1) yields










                        where we have utilized the definition of the Airy function [33]



                        From the latter result, eq. (B.1) is finally cast into the form













                        Appendix C
                        Eq. (2.14) in the text can be derived in a straightforward way after choosing the z-axis
                        along the direction of the vector  , so that  .  Then       , eq.  (2.13), can
                       be written down in the form









                        By a simple variable change the integration in   is  expressible in terms  of the  Airy
                       function of proper argument [see eq. (B.3)], so that
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