Page 222 - Strategies and Applications in Quantum Chemistry From Molecular Astrophysics to Molecular Engineer
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ELECTRONIC CHARGE DENSITY OF QUANTUM SYSTEMS                           205

                       result for   expressed in  terms  of Airy  function and its  first derivative.  The  only
                       applications of the result thus deduced will be restricted to the case of a model of
                       independent particles moving in a quadratic potential while simultaneously acted by a
                       static  electric field: the  predicted electric  dipole moment induced  by the  field in the
                       system is shown to be the exact value, despite the fact that the electronic charge density
                       resulting from the approach is only an approximation to the correct one.


                       2. An approximate approach to the electronic density

                       The system under study is assumed to consist of   electrons, possibly in the presence
                       of a  nuclear framework.  An  orbital picture of the quantum  behaviour of the system is
                       then introduced on  accepting the validity of an independent-particle model where each
                       electron moves  in the  field of  an  effective potential   which  afterwards is  left
                       substantially unspecified. We emphasize, however, that the choice of   is an essential
                       step of  any  modeling.  Besides  semiempirical forms,  effective potentials
                       functionally dependent on the electron numeral density  are  intuitively bound to play
                       a prominent role in applications.
                       The one-electron  Hamiltonian  operator             kinetic  energy operator,
                       generates a complete spectrum of orbitals   according to the Schrödinger equation



                       The ground state of the system corresponds to  electrons occupying the   lowest-
                       energy   levels, so that the electron numeral density   is




                       To attain an expression of   which does not make explicit reference to the occupied
                       orbitals, we rewrite eq. (2.2) in the form



                       where we have introduced the Heavisidefunction  and the Fermi level energy  If
                       we make use of the following standard representation of




                       from eq.  (2.1)  and the completeness of the  spectrum of orbitals  supported by   the
                       electron density n   (2.3), can be expressed as



                       (atomic  units with          are  used  throughout  this  paper). Eq.  (2.5) is  a well
                       known result [12,14-17,20,24,25], that makes evident the key-role played by the diagonal
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