Use the anharmonic potential function in Figure 18.7 to demonstrate that rotation and vibration are not separable degrees of freedom for large quantum numbers.
FIGURE 18.7
Potential energy V(x) as a function of the displacement x from the equilibrium bond length for a diatomic molecule. The zero of energy is chosen to be the bottom of the potential. The red curve depicts a realistic potential in which the molecule dissociates for large values of x. The purple curve shows a harmonic potential, V(x) = (1/2)kx2, which is a good approximation to the realistic potential near the bottom of the well.
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