Ab initio studies of ground and excited electronic states of MgAr,CdAr, and BeAr |
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Authors: | Jerry A. Boatz Keld Lars Bak Jack Simons |
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Affiliation: | (1) Department of Chemistry, University of Utah, 84112 Salt Lake City, UT, USA;(2) Present address: Astronautical Sciences Division, Phillips Laboratory, 93523 Edwards Air Force Base, CA, USA;(3) Present address: Department of Chemistry, Aarhus University, DK-8000 Aarhus C, Denmark |
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Abstract: | Summary The ground state (X1+) and several excited state (A3,c3+,C1,D1+, andE3+) potential energy surfaces for the diatomic molecules MgAr, CdAr, and BeAr have been computed using complete active space self-consistent field (CASSCF) wavefunctions and valence double- and triplezeta quality basis sets augmented with polarization and diffuse functions. Pump-and-probe laser experiments have examined the quenching, of excited singlet states of metal-rare gas complexes such as CdXe to produce triplets that dissociate to3PJmetal atoms. This quenching, which is detected for CdXe but not for CdAr or MgAr, is thought to occur via a crossing or strong coupling of a repulsive triplet curve correlating to the underlying3P state of the metal, with an attractive singlet curve that correlates to the higher1P state of the metal. The present work indicates that the attractiveC1 and repulsivec3+ curves of MgAr and CdArdo not intersect in the energetically accessible region of theC1 surface, unlike the corresponding curves for the CdXe diatom. These data are consistent with the absence of3PJ Cd atoms in the MgAr and CdAr experiments, respectively. However, an alternative quenching mechanism involving vibronic coupling between theC1 vibrational eigenstates and the continuum eigenstates of the underlying repulsive3+ surface may be operative; this possibility is examined qualitatively and predicted to be unlikely for MgAr (due to small spin-orbit coupling) and CdAr (due to unfavorable vibronic factors). BeAr, which has yet to be probed experimentally, is predicted to be bound by 770 and 900 cm–1 in theD1+ state (which has metal 2s2p character) and theE3+ state (which has Rydberg metal 2s3s character), respectively, and to display interesting potential curve intersections.Dedicated to Prof. Klaus Ruedenberg |
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Keywords: | MgAr CdAr BeAr Ground states Excited states CASSCF |
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