Measurement and assignment of $\it{J}$ $\geq$ 10 rotational energy levels in the 9510 to 9810 cm$^{-1}$ and 6590 to 6900 cm$^{-1}$ ranges of methane using optical frequency comb double-resonance spectroscopy
Abstract
Accurate models of high temperature methane spectra are needed in astrophysics. Previous measurements of methane hot-band transitions in the $\it{P}$6 $\leftarrow$ $\it{P}$2 polyad range have been limited to final rotational numbers of $\it{J}$ $\le$ 9, with theoretical predictions at higher $\it{J}$s remaining unvalidated. Here, we use optical-optical double resonance spectroscopy (OODR) with a 3.3 $μ$m narrow linewidth pump to excite the $ν$${_3}$ P(12, A${_1}$$^{(2)}$) methane transition ($\i...
Description / Details
Accurate models of high temperature methane spectra are needed in astrophysics. Previous measurements of methane hot-band transitions in the 6 2 polyad range have been limited to final rotational numbers of 9, with theoretical predictions at higher s remaining unvalidated. Here, we use optical-optical double resonance spectroscopy (OODR) with a 3.3 m narrow linewidth pump to excite the ν$${_3} P(12, A{_1}$$^{(2)}) methane transition (2 0) and a cavity-enhanced frequency comb centered around 1.68 m to probe the sub-Doppler ladder-type (6 2) and V-type (4 0) transitions, as well as Doppler-broadened collision-induced four-level transitions (6 2). 49 ladder-type transitions with final rotational states = 10-12 in the range of 9510 to 9810 cm (i.e., the 6 polyad) were assigned to effective Hamiltonian predictions and the ExoMol database, of which 6 reached vibrational states that had not been observed experimentally before. 19 sub-Doppler V-type transitions with final states = 11-13 in the range of 6590 to 6900 cm (i.e., the 4 polyad) were observed and assigned to the Hamiltonian and ExoMol, while only 2 of these V-type transitions could be unambiguously assigned to WKLMC and HITRAN line lists. 170 Doppler-broadened four-level double-resonance (4LDR) lines were observed, 7 of which were newly observed compared with our previous work when pumping transitions starting from the = 7 level in the ground state [Lehmann et al., J. Chem. Phys. 163, 144304 (2025)]. We could not assign these lines as they did not form combination differences with other observed 4LDR transitions.
Source: arXiv:2607.12932v1 - http://arxiv.org/abs/2607.12932v1 PDF: https://arxiv.org/pdf/2607.12932v1 Original Link: http://arxiv.org/abs/2607.12932v1
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Jul 15, 2026
Chemistry
Chemistry
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