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3. NANOMEMS PHYSICS: Quantum Wave Phenomena                     93


             lowest energy eigenvalue (ground state energy) is given by the sum of the
             one-electron  energies  up  to  a maximum energy level denoted by  E  and
                                                                         F
             called Fermi energy. This is obtained when N electron states with energy less
             than E  are  occupied,  and  all states with  energy greater than  E  are
                   F                                                     F
             unoccupied. To obtain an expression for  E , one pictures the states in (38)
                                                  F
             as a grid of point in  k  k  k  space where they form a fine three-dimensional
                                x  y  z                     G
             grid of spacing  π  L , such that a sphere centered at  k  =  0  would contain
                           2
             4π       1      Vk 3     Vk 3                                  G
                k ⋅        =     ⋅ 2 =     points of the grid  when  its  radius  is  k ,
                  3
              3     §  2π · 3  6π 2   3π 2
                    ¨   ¸
                    ©  L ¹
             including  spin. Since  each point in  the grid  represents one  electron,  the
             number of grid points contained  in a sphere with the largest radius,  k ,
                                                                            F
             corresponding to  E  must equal N,
                             F
               Vk 3
                  F  =  N .                                                                                              (39)
               3π 2

             Thus, the largest electron momentum is,


                       3π 2 N       ) 1  /  3
               k  =  1  /  3  =  (3π 2 n  ,                                                                 (40)
                F
                         V
             where n is the electron density in the metal, and the Fermi energy is,

                      2
                     = § 3π 2  N ·  2  /  3  =  2  ) 1  /  3
               E =      ¨ ¨    ¸ ¸  =   (3π 2 n  .                                                (41)
                 F
                     2m  ©  V  ¹     2m
             At absolute zero, all levels are filled up to  E . For an arbitrary energy E,
                                                     F
             less than  E , the total number of electrons with energy less than E is given
                       F
             by,

                             3  /  2
               N  =  V  § ¨  2m  · ¸  ,                                                                               (42)
                    3π 2  © =  2  ¹

             from where the density of states is given by,
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