“Know how to solve every problem that has been solved.” “What I cannot create, I do not understand.” — Richard Feynman

Solving the Casida eigenvalue problem yields excitation energies as eigenvalues and oscillator strengths from the eigenvectors (via transition dipoles).

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Solving the Casida eigenvalue problem yields excitation energies as eigenvalues and oscillator strengths from the eigenvectors (via transition dipoles).

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