Page 60 - Science at the nanoscale
P. 60

9:2
                                                     RPS: PSP0007 - Science-at-Nanoscale
                   June 9, 2009
                              Brief Review of Quantum Mechanics
                          50
                                   in a hydrogen-like atom:
                                                                     2
                                                                RhcZ
                                                          E = −
                                                                  n
                                                                                         −1
                                   where R is known as the Rydberg constant (= 1.0974 × 10 m
                                                                                           ),
                                   and c corresponds to the speed of light. n is the principal quantum
                                   number and its value ranges from 1 to ∞. A common form of the
                                   equation expressed in units of electron volts is given by
                                                                                        (3.58)
                                                                 2
                                                                n
                                     Even though the exact form for the energy differs from the par-
                                   ticle in a potential box, the quantisation of energy is a common
                                   feature of bound systems where the motion of the particle is re-
                                   stricted. Equation (3.57) applies to hydrogen-like atoms, exam-
                                   ples of which include hydrogen (Z = 1), deuterium (Z = 1), He
                                                                                           +
                                   (Z = 2), and Li
                                                   (Z = 3) (see Fig. 3.9).
                                                2+
                                     How do we know that the energy levels are indeed quantised?
                                   The answer lies in the atomic spectra of an atom. When an atom
                                   is excited, it will be in one of its excited states; when the atom
                                   de-excites, it would go to an energy level with lower energy. The
                                                            +
                                               H (Z=1)
                                                          He (Z=2)
                                                                      Li (Z=3)
                                                       n
                                                       3
                                                       2
                                                       1 E = − 13.6Z 2 2 n 3 2 (eV) 2+  n 4 3  7  (3.57)  ch03
                                                13.6 eV
                                                                               2
                                                                   1
                                                            54.4 eV
                                                                               1
                                                                        122.5 eV
                                             Figure 3.9.  Energy levels of H, He and Li 2+ .
                                                                         +
   55   56   57   58   59   60   61   62   63   64   65