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首页> 外文期刊>The Journal of Chemical Physics >CH radical production from 248 nm photolysis or discharge-jet dissociation of CHBr_3 probed by cavity ring-down absorption spectroscopy
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CH radical production from 248 nm photolysis or discharge-jet dissociation of CHBr_3 probed by cavity ring-down absorption spectroscopy

机译:腔衰荡吸收光谱法检测CHBr_3的248 nm光解或放电离解产生CH自由基

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The A-X bands of the CH radical,produced in a 248 nm two-photon photolysis or in a supersonic jet discharge of CHBr_3,have been observed via cavity ring-down absorption spectroscopy.Bromoform is a well-known photolytic source of CH radicals,though no quantitative measurement of the CH production efficiency has yet been reported.The aim of the present work is to quantify the CH production from both photolysis and discharge of CHBr_3.In the case of photolysis,the range of pressure and laser fluences was carefully chosen to avoid postphotolysis reactions with the highly reactive CH radical.The CH production efficiency at 248 nm has been measured to be PHI =N(CH)A/N(CHBr_3) = (5.0+-2.5)10~(-4) for a photolysis laser fluence of 44mJ cm~(-2) per pulse corresponding to a two-photon process only.In addition,the internal energy distribution of CH(X ~2PI) has been obtained,and thermalized population distributions have been simulated,leading to an average vibrational temperature T_(vib)=1800+-50 K and a rotational temperature T_(rot) = 300+-20K.An alternative technique for producing the CH radical has been tested using discharge-induced dissociation of CHBr_3 in a supersonic expansion.The CH product was analyzed using the same cavity ring-down spectroscopy setup.The production of CH by discharge appears to be as efficient as the photolysis technique and leads to rotationally relaxed radicals.
机译:通过腔衰荡吸收光谱法观察到CH自由基的AX谱带是在248 nm双光子光解或超音速喷射的CHBr_3中产生的。溴仿是众所周知的CH自由基的光解源。尚无关于CH产生效率的定量测量方法的报道。本研究的目的是对CHBr_3的光解和排放中的CH产生进行定量。在光解的情况下,仔细选择压力和激光通量的范围避免与高反应性CH自由基发生光解后反应。测得在248 nm处的CH产生效率PHI = N(CH)A / N(CHBr_3)=(5.0 + -2.5)10〜(-4)每个脉冲的激光能量密度仅为44mJ cm〜(-2),仅对应于两个光子过程。此外,获得了CH(X〜2PI)的内部能量分布,并对热化的种群分布进行了模拟,从而得出了平均振动温度T_(vib)= 1800 + -50 K和旋转温度T_(rot)= 300 + -20K。另一种产生CH自由基的技术已通过在超音速膨胀中使用放电诱导的CHBr_3的离解来进行了测试。放电产生的CH似乎与光解技术一样有效,并导致旋转弛豫的自由基。

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