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Príomhchruthaitheoirí: Krumins, V., Tamanis, M., Ferber, R., Oleynichenko, A. V., Skripnikov, L. V., Zaitsevskii, A., Pazyuk, E. A., Stolyarov, A. V., Pashov, A.
Formáid: Preprint
Foilsithe / Cruthaithe: 2022
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Rochtain ar líne:https://arxiv.org/abs/2201.06830
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author Krumins, V.
Tamanis, M.
Ferber, R.
Oleynichenko, A. V.
Skripnikov, L. V.
Zaitsevskii, A.
Pazyuk, E. A.
Stolyarov, A. V.
Pashov, A.
author_facet Krumins, V.
Tamanis, M.
Ferber, R.
Oleynichenko, A. V.
Skripnikov, L. V.
Zaitsevskii, A.
Pazyuk, E. A.
Stolyarov, A. V.
Pashov, A.
contents Laser-induced fluorescence spectra of the $c^3Σ^+(v_{c},J_{c}=N_{c})\rightarrow a^3Σ^+(v_{a},N_{a} = J_{c} \pm 1)$ transitions excited from the ground $X^1Σ^+$ state of $^{39}$K$^{133}$Cs molecule were recorded with Fourier-transform spectrometer IFS125-HR (Bruker) at the highest achievable spectral resolution of 0.0063 cm${}^{-1}$. Systematic study of the hyperfine structure (HFS) of the $a^3Σ^+$ state for levels with $v_{a} \in [0, 27]$ and $N_{a} \in [24, 90]$ shows that the splitting monotonically increases with $v_{a}$. The spectroscopic study was supported by ab initio calculations of the magnetic hyperfine interaction in $X^1Σ^+$ and $a^3Σ^+$ states. The discovered variation of the electronic matrix elements with the internuclear distance $R$ is in a good agreement with the observed $v_{a}$-dependencies of the HFS. Overall set of available experimental data on the $a^3Σ^+$ state was used to improve the potential energy curve particularly near a bottom, providing the refined dissociation energy $D_e$=267.21(1) cm${}^{-1}$. The ab initio HFS matrix elements, combined with the empirical $X^1Σ^+$ and $a^3Σ^+$ PECs in the framework of the invented coupled-channel deperturbation model, reproduce the experimental term values of both ground states within 0.003 cm${}^{-1}$ accuracy up to their common dissociation limit.
format Preprint
id arxiv_https___arxiv_org_abs_2201_06830
institution arXiv
publishDate 2022
record_format arxiv
spellingShingle The $a^3Σ^+$ state of KCs revisited: hyperfine structure analysis and potential refinement
Krumins, V.
Tamanis, M.
Ferber, R.
Oleynichenko, A. V.
Skripnikov, L. V.
Zaitsevskii, A.
Pazyuk, E. A.
Stolyarov, A. V.
Pashov, A.
Atomic Physics
Atomic and Molecular Clusters
Chemical Physics
Computational Physics
Laser-induced fluorescence spectra of the $c^3Σ^+(v_{c},J_{c}=N_{c})\rightarrow a^3Σ^+(v_{a},N_{a} = J_{c} \pm 1)$ transitions excited from the ground $X^1Σ^+$ state of $^{39}$K$^{133}$Cs molecule were recorded with Fourier-transform spectrometer IFS125-HR (Bruker) at the highest achievable spectral resolution of 0.0063 cm${}^{-1}$. Systematic study of the hyperfine structure (HFS) of the $a^3Σ^+$ state for levels with $v_{a} \in [0, 27]$ and $N_{a} \in [24, 90]$ shows that the splitting monotonically increases with $v_{a}$. The spectroscopic study was supported by ab initio calculations of the magnetic hyperfine interaction in $X^1Σ^+$ and $a^3Σ^+$ states. The discovered variation of the electronic matrix elements with the internuclear distance $R$ is in a good agreement with the observed $v_{a}$-dependencies of the HFS. Overall set of available experimental data on the $a^3Σ^+$ state was used to improve the potential energy curve particularly near a bottom, providing the refined dissociation energy $D_e$=267.21(1) cm${}^{-1}$. The ab initio HFS matrix elements, combined with the empirical $X^1Σ^+$ and $a^3Σ^+$ PECs in the framework of the invented coupled-channel deperturbation model, reproduce the experimental term values of both ground states within 0.003 cm${}^{-1}$ accuracy up to their common dissociation limit.
title The $a^3Σ^+$ state of KCs revisited: hyperfine structure analysis and potential refinement
topic Atomic Physics
Atomic and Molecular Clusters
Chemical Physics
Computational Physics
url https://arxiv.org/abs/2201.06830