Mogyorosi K, Sarosi K, Seres I, Jojart P, Fule M, Chikan V
ELI-ALPS, ELI-HU Non-Profit Ltd., Dugonics ter 13, Szeged H-6720, Hungary.
Department of Chemistry, Kansas State University, 213 CBC Building, Manhattan, Kansas 66506-0401, United States.
J Phys Chem A. 2020 Apr 9;124(14):2755-2767. doi: 10.1021/acs.jpca.0c00361. Epub 2020 Mar 27.
Exploring the formation of diatomic radicals in femtosecond plasmas is important to establish the most dominant kinetic pathways following ionization and dissociation of small molecules. In this work, cyano radical formation has been studied from bromoform, acetonitrile, and methanol in nitrogen and argon plasmas created with a focused femtosecond laser beam operating at 100 kHz repetition rate and 1030 nm wavelength with 43 fs pulse length and 250 μJ pulse energy. Time-resolved Fourier transform fluorescence spectroscopy was applied in the ultraviolet-visible (UV-vis) spectral range for the characterization of the rotational and vibrational temperatures of the CN(B) radicals via fitting the experimental data. The high repetition rate of the laser allows efficient coupling with the step-scan Fourier transform spectroscopy method. Coulomb explosion at the very high intensity (∼10 W/cm) resulted in the formation of nascent atoms, ions, and electrons. The condensation reactions of carbon and reactive nitrogen species resulted in the formation of CN(BΣ) radicals and C(dΠ) dicarbon molecules/radicals. The CN(B) radicals were formed at the highest concentration in the case of bromoform because the weak carbon-bromine bonds resulted in reactive carbon atoms and CH radicals, which are reactive precursors for the CN(B) radical formation. In the case of acetonitrile, immediate production of CN(B) is observed with nanosecond resolution, which suggests that the CN is formed either via photodetachment or via roaming reaction associated with the Coulomb explosion of the parent molecule. The nascent rotational temperature was very high (∼6000-8500 K) and rapidly decreased in all instances within 40 ns with bromoform and acetonitrile. The highest vibrational temperature (∼7800 K) was observed in an acetonitrile/Ar mixture that decreased in about 30 ns and then increased in the observed time window. The vibrational temperature increased in all samples between 30 and 200 ns. The time dependence of fluorescence is described with a monoexponential decay in the case of acetonitrile/Ar and with biexponential decays in all other instances in the 0-250 mbar total pressure range. The shorter time constant is close to the radiative lifetime of CN(B) emission (∼60-80 ns), which can be attributed to the CN(B) radicals produced in the first few collisions at lower pressures. The longer CN(B) emission is from CN(B) created by slower chemical reactions involving carbon atoms, C radicals, and reactive nitrogen-containing species.
探索飞秒等离子体中双原子自由基的形成对于确定小分子电离和解离后最主要的动力学途径至关重要。在这项工作中,利用重复频率为100 kHz、波长为1030 nm、脉冲长度为43 fs且脉冲能量为250 μJ的聚焦飞秒激光束在氮气和氩气等离子体中研究了溴仿、乙腈和甲醇中氰基自由基的形成。在紫外可见(UV-vis)光谱范围内应用时间分辨傅里叶变换荧光光谱法,通过拟合实验数据来表征CN(B)自由基的转动温度和振动温度。激光的高重复频率使得与步进扫描傅里叶变换光谱法能够有效耦合。在极高强度(10 W/cm)下的库仑爆炸导致了新生原子、离子和电子的形成。碳和活性氮物种的缩合反应导致了CN(BΣ)自由基和C(dΠ)二碳分子/自由基的形成。在溴仿的情况下,CN(B)自由基的形成浓度最高,因为较弱的碳 - 溴键产生了活性碳原子和CH自由基,它们是CN(B)自由基形成的活性前体。在乙腈的情况下,以纳秒分辨率观察到CN(B)的即时产生,这表明CN是通过光解离或与母体分子的库仑爆炸相关的漫游反应形成的。新生转动温度非常高(6000 - 8500 K),并且在溴仿和乙腈的所有情况下,在40 ns内迅速下降。在乙腈/氩气混合物中观察到最高振动温度(7800 K),其在约30 ns内下降,然后在观察时间窗口内上升。在所有样品中,振动温度在30至200 ns之间升高。在总压力范围为0 - 250 mbar的情况下,对于乙腈/氩气,荧光的时间依赖性用单指数衰减来描述,而在所有其他情况下用双指数衰减来描述。较短的时间常数接近CN(B)发射的辐射寿命(60 - 80 ns),这可归因于在较低压力下最初几次碰撞中产生的CN(B)自由基。较长的CN(B)发射来自由涉及碳原子、C自由基和活性含氮物种的较慢化学反应产生的CN(B)。