Characterisation of the b3Σ+,v=0b^3Σ^+, v=0 State and Its Interaction with the A1ΠA^1Π State in Aluminium Monofluoride

preprint2020arXivOpen access

Abstract

Recently, we determined the detailed energy level structure of the X1Σ+X^1Σ^+, A1ΠA^1Π and a3Πa^3Π states of AlF that are relevant to laser cooling and trapping experiments. Here, we investigate the b3Σ+,v=0b^3Σ^+, v=0 state of the AlF molecule. A rotationally-resolved (1+2)-REMPI spectrum of the b3Σ+,v′=0←a3Π,v′′=0b^3Σ^+, v'=0 \leftarrow a^3Π, v''=0 band is presented and the lifetime of the b3Σ+,v=0b^3Σ^+, v=0 state is measured to be 190(2)~ns. Hyperfine-resolved, laser-induced fluorescence spectra of the b3Σ+,v′=0←X1Σ+,v′′=1b^3Σ^+, v'=0 \leftarrow X^1Σ^+, v''=1 and the b3Σ+,v′=0←a3Π,v′′=0b^3Σ^+, v'=0 \leftarrow a^3Π, v''=0 bands are recorded to determine fine- and hyperfine structure parameters. The interaction between the b3Σ+,v=0b^3Σ^+, v=0 and the nearby A1ΠA^1Π state is studied and the magnitude of the spin-orbit coupling between the two electronic states is derived using three independent methods to give a consistent value of 10(1)~cm−1^{-1}. The triplet character of the AA state causes an A→aA\rightarrow a loss from the main A−XA-X laser cooling cycle below the 10−6^{-6} level.

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