Electronic Structure and Spectroscopy of CuBe

Electronic spectra for CuBe were recorded using resonantly enhanced one-color, two-photon ionization techniques. Several vibronic progressions were observed, permitting characterization of the 4<sup>2</sup>Σ<sup>+</sup>, 5<sup>2</sup>Σ<sup>+</sup>, 3<sup>2</sup>Π and 4<sup>2</sup>Π excited states. Rotational resolution was achieved for a few bands, permitting determination of the ground state rotational constant. Attempts to record laser-induced fluorescence or two-color ionization spectra were unsuccessful. This was attributed to predissociation of the excited states. Density functional theory and <i>ab initio</i> electronic structure calculations were used to facilitate assignment of the observed states. Potential energy curves obtained from these calculations indicated that states arising from the Cu­(3d<sup>9</sup>4s<sup>2</sup>) + Be­(2s<sup>2</sup>) dissociation asymptote were well-positioned to cause predissociation of the observed states.

Publication Details

Journal
Figshare
Published
2025-02-13
DOI
https://doi.org/10.1021/acs.jpca.4c08565.s001
Primary Topic
Laser Design and Applications
Type
article
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Electronic Structure and Spectroscopy of CuBe

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Electronic Structure and Spectroscopy of CuBe

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Abstract

Electronic spectra for CuBe were recorded using resonantly enhanced one-color, two-photon ionization techniques. Several vibronic progressions were observed, permitting characterization of the 4<sup>2</sup>Σ<sup>+</sup>, 5<sup>2</sup>Σ<sup>+</sup>, 3<sup>2</sup>Π and 4<sup>2</sup>Π excited states. Rotational resolution was achieved for a few bands, permitting determination of the ground state rotational constant. Attempts to record laser-induced fluorescence or two-color ionization spectra were unsuccessful. This was attributed to predissociation of the excited states. Density functional theory and <i>ab initio</i> electronic structure calculations were used to facilitate assignment of the observed states. Potential energy curves obtained from these calculations indicated that states arising from the Cu­(3d<sup>9</sup>4s<sup>2</sup>) + Be­(2s<sup>2</sup>) dissociation asymptote were well-positioned to cause predissociation of the observed states.

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