CALCULATION AND ASSIGNMENT OF RYDBERG LEVELS IN BENZENE

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1974

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Ohio State University

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High resolution optical spectra taken by Wilkinson showed four Rydberg Series converging to the first ionization potential at 9.247 eV. He designated these series $R$, $R^{\prime}$, $R^{\prime\prime}$, $R^{\prime\prime}$. The $R$ and $R^{\prime}$ series are the most intense and presumably are due to the allowed $e_{1u} \leftarrow$ $e_{1g}$ and $a_{2u}$ $\leftarrow$ $e_{1g}$ transitions where $e_{1g}$ is the highest occupied molecular orbital and has $\pi$ symmetry, and $e_{1u}$ and $a_{2u}$ are Rydberg orbitals with Per and $P\pi$ symmetry, respectively, in the united-atom limit. The relative size of the quantum defects suggests that the R^{\prime} series is $e_{1u}$ $\leftarrow$ and $e_{1g}$ and that the R^{\prime} series is $a_{2u}$ $\leftarrow$ $e_{1g}$ while pseudopotential calculations have not been conclusive. We have carried out self-consistent-field calculations on these states with a fairly large Gaussian basis set, (10$_{s} 6p/4_{s}$), $[5_{s}$ $3p/2_{s}$] where one set of Gaussians represents C $3_{s}$ orbital and one set represents C 3$_{p}$ orbita1s. The calculated $e_{1u}$ $\leftarrow$ $e_{1g}$ excitation energy (average of $A_{1u}$, $A_{2u}$, and $E_{2u}$) is 6.71 eV., and the calculated $a_{2u}$ $\leftarrow$ $e_{1g}$ excitation energy ($E_{1u}$) is 6.94 eV. The splitting between the two is expected to be more reliable than the absolute excitation energy. The lowest energy Rydberg state computed is a $E_{1g}$ state at 6.31 eV., which comes from a forbidden excitation to an $a_{1g}$ orbital (3s in the united-atom limit).

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Author Institution: Department of Chemistry, The Ohio State University; Department of Physics, University of Chicago; Department of Chemistry, The Ohio State University

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