excited states with T 0 = 30 210 and 32 274 cm −1 , respectively. Each electronic transition has partially resolved rotational and extensive vibrational structure with an extended progression in the metal−ligand stretch at a frequency of ∼450 cm −1 . There are also progressions in the in-plane bend in the 7 B 2 state, due to vibronic coupling, and the out-of-plane bend in the 7 B 1 state, where the calculation illustrates that this state is slightly non-planar. Electronic structure computations at the CCSD(T)/aug-cc-pVTZ and TD-DFT B3LYP/6-311++G(3df,3pd) level are also used to characterize the ground and excited states, respectively. These calculations predict a ground state Mn-O bond length of 2.18 Å. Analysis of the experimentally observed vibrational intensities reveals that this bond length decreases by 0.15 ± 0.015 Å and 0.14 ± 0.01 Å in the excited states. The behavior is accounted for by the less repulsive p x and p y orbitals causing the Mn + to interact more strongly with water in the excited states than the ground state. The result is a decrease in the Mn-O bond length, along with an increase in the H-O-H angle. The spectra have well resolved K rotational structure. Fitting this structure gives spin-rotation constants ε aa = −3 ± 1 cm −1 for the ground state and ε aa = 0.5 ± 0.5 cm −1 and aa = −4.2 ± 0.7 cm −1 for the first and second excited states, respectively, and A = 12.8 ± 0.7 cm −1 for the first excited state. Vibrationally mediated photodissociation studies determine the O-H antisymmetric stretching frequency in the ground electronic state to be 3658 cm −1 .