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In electronic spectra of molecules, the vibrational quantum number leading to convergence of vibrational spectral lines is given by :

  • A.\(\frac{1}{x_{e}} - 1\)
  • B.\(\frac{1}{\bar{\omega}_{e}} - 1\)
  • C.\(\frac{1}{2x_{e}} - 1\)
  • D.\(\frac{1}{\bar{\omega}_{e} x_{e}} - 1\)

Answer: C

The convergence occurs at v = 1/(2xe) − 1.

For an anharmonic oscillator the vibrational levels are

\[ \begin{aligned} \varepsilon_{v} &= \bar{\omega}_{e}(v+\tfrac{1}{2}) \\ &- \bar{\omega}_{e}x_{e}(v+\tfrac{1}{2})^{2} \end{aligned} \]

The spacing between neighbouring levels shrinks as v rises. Setting the spacing to zero gives the level where the progression converges:

\[ \begin{aligned} \Delta\varepsilon &= \bar{\omega}_{e}[1 - 2x_{e}(v+1)] = 0 \\ v_{max} &= \frac{1}{2x_{e}} - 1 \end{aligned} \]

This is the form given in Banwell. The other options drop the factor 2, or put the wavenumber \(\bar{\omega}_{e}\) in the denominator, which makes v carry units of cm instead of being a pure number.

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