O2 (1Δg) detection using broadband CARS

Jinbo Liu, Jingwei Guo, X. Cai, Baodong Gai, Qingkun Meng, Yuqi Jin
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Abstract

1 Δg oxygen was the active medium of chemical oxygen iodine laser (COIL), the concentration and distribution of 1 Δg oxygen was important for the output power and beam quality. However, the current test technique, such as fluorescence detection method, absorption spectrum method could not get accurate 1 Δg oxygen information, due to the interference from the iodine fluorescence or the rigorous request of the laser source and optics and detection elements. The anti-stokes Raman spectrum of 1 Δg oxygen was regarded as a potential technique to obtain desirable signal, and the coherent anti-stokes Raman scatter (CARS) was the most feasible technique to get better signal to noise ratio (SNR). In this paper, we reported a broadband nanosecond coherent anti-stokes Raman scatter (CARS) detecting system built up for the detection of the concentration and distribution of O2( 1 Δg) in COIL:The second harmonic of a Nd: YAG pulse laser was separated into two parts, one part was used to pump a broadband nanosecond dye laser to generate light of 578-580 nm, which covered both stokes lines of O2 ( 1 Δg)and O2 (3 ∑); The other part was combined with dye laser output by a dichroic mirror, and then introduced into the detection region of COIL through a focus lens. CARS signals for O2(1 Δg)and O2 (3 ∑)have different wavelengths, and their intensity was proportional to the square of the concentration of O2(1 Δg) and O2( 3 ∑). By changing the focus spot of pump and stokes laser, the concentration distribution of O2(1 Δg) and O2(3 ∑)at different position could be obtained.
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利用宽带CARS检测O2 (1Δg)
1 Δg氧是化学氧碘激光器(COIL)的活性介质,1 Δg氧的浓度和分布对输出功率和光束质量有重要影响。然而,目前的测试技术,如荧光检测法、吸收光谱法,由于碘荧光的干扰或激光光源、光学元件和检测元件的严格要求,无法获得准确的1 Δg氧信息。1 Δg氧的抗斯托克斯拉曼光谱被认为是获得理想信号的一种潜在技术,而相干抗斯托克斯拉曼散射(CARS)是获得较好信噪比的最可行技术。本文报道了一种用于检测线圈中O2(1 Δg)浓度和分布的宽带纳秒相干反斯托克斯拉曼散射(CARS)检测系统:将Nd: YAG脉冲激光器的二次谐波分离成两部分,一部分用于泵浦宽带纳秒染料激光器,产生覆盖O2(1 Δg)和O2(3∑)的578 ~ 580 nm的光;另一部分通过二向镜与输出的染料激光结合,再通过聚焦透镜引入COIL的检测区域。O2(1 Δg)和O2(3∑)的CARS信号具有不同的波长,其强度与O2(1 Δg)和O2(3∑)浓度的平方成正比。通过改变泵浦和斯托克斯激光器的焦点光斑,可以得到O2(1 Δg)和O2(3∑)在不同位置的浓度分布。
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