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280                          Molecular structure


                                               U (R)







                                                        R e
                                                  0
                                                                                R


                                                2D e
                             Figure 10.2 The Morse potential for the ground state of a diatomic molecule.



                                  (b) If the Rydberg potential is expanded according to equation (10.30), relate the
                                     parameter b to ì, ù, and D e .
                                  (c) Relate the quantities x e , á e , and U (0) in equation (10.50) to ì, ù, and D e
                                     for the Rydberg potential.
                             10.6 Consider a diatomic molecule in its ground electronic and rotational states. Its
                                  energy levels are given by equation (10.50) with J ˆ 0. The value of U(R)at
                                  R ˆ R e is ÿD e .

                                  (a) If the anharmonic factor x e is positive, show that the spacing of the energy
                                     levels decreases as the vibrational quantum number n increases.
                                  (b) When the vibrational quantum number n becomes suf®ciently large that the
                                     difference in energies between adjacent levels becomes zero, the molecule
                                     dissociates into its constituent atoms. By setting equal to zero the derivative
                                     of E n0 with respect to n, ®nd the value of n in terms of x e at which
                                     dissociation takes place.
                                  (c) Relate the well depth D e to the anharmonic factor x e and compare with the
                                     corresponding expressions in problems 10.4 and 10.5.
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