I. Introduction
Gas temperature measurement is essential to combustion diagnosis [1], chemical reaction monitoring, and organic chemical synthesis [2]. Typical methods for gas temperature are either intrusive or nonintrusive. Intrusive methods, such as thermocouples or gas sampling, are widely applied, but they distort turbulent gases for invasive installations [3]. Nonintrusive methods use contactless sensor and has the merits of high sensitivity, fast response, and strong ability of multiparameter simultaneous measurement. These methods are usually realized from laser spectroscopy, e.g., coherent anti-stokes Raman scattering spectroscopy [4], planar laser-induced fluorescence [5], [6], and tunable diode laser absorption spectroscopy (TDLAS) [7], [8], [9]. TDLAS is widely applied in combustion evaluations of industrial and aerospace combustors for its high adaptability, fast response, high accuracy, and versatile parameter detection [10]. In TDLAS, two spectral lines are required to obtain gas temperature and molar concentrations, and these spectral lines are scanned using narrowbanded DFB lasers for fast response and economical cost. A single DFB laser typically only covers one or two spectral lines of target molecules, and a wide spectral coverage requires an increasing number of lasers. In recent years, the dual-comb spectroscopy (DCS) is proposed for wide spectral coverage and applied to gas parameter detection using two optical frequency comb (OFC) lasers. The optical spectral band of OFC laser is usually tens to hundreds of times wider than that of the DFB laser in TDLAS, and they can be used as a reference for HITRAN database calibration [11].