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Bulletin of the American Physical Society

Spectroscopic analysis on the 5 $^{1}\Sigma_{0}^{+}$, 3 $^{1}\Pi _{1}$, 5 $^{3}\Sigma_{1}^{+}$, and 4 $^{3}\Pi_{1}$ states of the KRb diatomic molecule using a molecular beam

Y. Lee, Bongsoo Kim, Jin‐Tae Kim

Published Jun 3, 2014• 0 citations
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The European Physical Journal D•Jul 18, 2005•20 citations
Spectroscopic analysis on the 5 1Σ0+^{1}\Sigma_{0}^{+}1Σ0+​, 3 1Π1^{1}\Pi _{1}1Π1​, 5 3Σ1+^{3}\Sigma_{1}^{+}3Σ1+​, and 4 3Π1^{3}\Pi_{1}3Π1​ states of the KRb diatomic molecule using a molecular beam
Spectroscopic investigation of the AAA and 3 1Σ+^{1}\Sigma ^{+}1Σ+ states of 39^{39}39K85^{85}85Rb
We report the spectroscopic characterization of excited electronic states of KRb by combining spectra from molecular beam (MB) experiments with those from ultracold molecules (UM) formed by photoassociation (PA) of ultracold atoms. Spectra involving the 1(1)Π, 2(3)Σ(+), and b(3)Π states in a strongly perturbed region have been identified. This approach provides a powerful method to identify the vibrational levels of the excited electronic states perturbed globally by neighboring electronic states. This is because the two sets of spectra from the UM and the MB experiments probe the same energy region from very different initial electronic states. The UM experiments utilize high v'' levels of the a(3)Σ(+) state with large internuclear separations, while the MB experiments utilize low v'' levels of the ground X(1)Σ(+) state with near-equilibrium internuclear separations. Only the Ω = 1 levels of the 2(3)Σ(+) and b(3)Π states are observed in the MB spectra, while the Ω = 0(-), 1 levels of the 2(3)Σ(+) state and the Ω = 0(±), 1, 2 levels of the b(3)Π state are observed in the UM spectra.