Double resonant absorption measurement of acetylene symmetric vibrational states probed with cavity ring down spectroscopy

• Published in: arXiv.org
• Main Authors: Karhu, J, Nauta, J, Vainio, M, Metsälä, M, Hoekstra, S, Halonen, L
• Format: Paper Journal Article
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 19.07.2016
• Subjects: Absorption; Acetylene; Cavity ringdown; Continuous radiation; Least squares method; Near infrared radiation; Optical Parametric Oscillators; Parameters; Parametric amplifiers; Physics - Chemical Physics; Physics - Instrumentation and Detectors; Physics - Optics; Signal to noise ratio; Spectrum analysis; Vibrational states
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.1607.05953

A novel mid-infrared/near-infrared double resonant absorption setup for studying infrared-inactive vibrational states is presented. A strong vibrational transition in the mid-infrared region is excited using an idler beam from a singly resonant continuous-wave optical parametric oscillator, to populate an intermediate vibrational state. High output power of the optical parametric oscillator and the strength of the mid-infrared transition result in efficient population transfer to the intermediate state, which allows measuring secondary transitions from this state with a high signal-to-noise ratio. A secondary, near-infrared transition from the intermediate state is probed using cavity ring down spectroscopy, which provides high sensitivity in this wavelength region. Due to the narrow linewidths of the excitation sources, the rovibrational lines of the secondary transition are measured with sub-Doppler resolution. The setup is used to access a previously unreported symmetric vibrational state of acetylene, \(\nu_1+\nu_2+\nu_3+\nu_4^1+\nu_5^{-1}\) in the normal mode notation. Single-photon transitions to this state from the vibrational ground state are forbidden. Ten lines of the newly measured state are observed and fitted with the linear least-squares method to extract the band parameters. The vibrational term value was measured to be at 9775.0018(45) \(\text{cm}^{-1}\), the rotational parameter \(B\) was 1.162222 \(\text{cm}^{-1}\), and the quartic centrifugal distortion parameter \(D\) was 3.998(62)\(\times 10^{-6} \text{cm}^{-1}\), where the numbers in the parenthesis are one-standard errors in the least significant digits.