首页> 外文期刊>The Journal of Chemical Physics >PHOTOFRAGMENTS CH3((X)OVER-TILDE(2)A(2)'')+HCO((X)OVER-TILDE(2)A') FROM ACETALDEHYDE - DISTRIBUTIONS OF ROTATIONAL STATES AND PREFERENTIAL POPULATION OF K DOUBLETS OF HCO
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PHOTOFRAGMENTS CH3((X)OVER-TILDE(2)A(2)'')+HCO((X)OVER-TILDE(2)A') FROM ACETALDEHYDE - DISTRIBUTIONS OF ROTATIONAL STATES AND PREFERENTIAL POPULATION OF K DOUBLETS OF HCO

机译:乙醛中的CH3((X)-叠氮化物(2)A(2)'')+ HCO((X)-叠氮化物(2)A')的光片段-旋转态的分布和HCO的两倍数优先种群

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The relative rotational populations of HCO dissociated from acetaldehyde excited to the S-1 state at photolysis energies 31 412, 31 771, 32 165, 32 728, and 33 239 cm(-1) are obtained. Fluorescent spectra (B) over tilde <(2)A'-(X)over tilde> (2)A'(0,0) of HCO were detected; the intensity is corrected for both the fluorescent quantum yield and the effect of axis switching to obtain the populations of rotational states of HCO. All measured populations of rotational states of HCO, displaying a Gaussian-type pattern, cannot be described according to a Boltzmann distribution. The average energy partitioned to rotation of HCO along the b and c axes is [(270-465) +/- 25] cm(-1), about 11% of the available energy, but the average energy partitioned along the a axis remains the same (32 +/- 2) cm(-1) for all photolysis energies. The rotational energy of HCO is less than that predicted according to an impulsive model calculated with the ab initio transition state structure. Preferential population of K-a = 1 doubler states N-1(u) and N-1(l) is observed. The ratio of population varies with photolysis energy, with a maximum 12(1)(u)/12(1)(l) = 3.7 near 31 800 cm(-1). Distributions among the rotational state of HCO indicate that the energy released appears to be affected by the dynamics of the exit channel. (C) 1996 American Institute of Physics. [References: 37]
机译:获得了在光解能为31 412、31 771、32 165、32 728和33 239 cm(-1)时从乙醛激发为S-1状态解离的HCO的相对旋转种群。检测到波浪线<(2)A'-(X)上的HCO荧光光谱(B)>(2)A'(0,0)。对荧光量子产率和轴转换效应进行校正,以获得HCO旋转态的总体。不能根据玻尔兹曼分布来描述所有显示的高斯型模式的HCO旋转状态的所有测量种群。 HCO沿b和c轴旋转时分配的平均能量为[(270-465)+/- 25] cm(-1),约为可用能量的11%,但沿a轴分配的平均能量仍保持不变所有光解能量都相同(32 +/- 2)cm(-1)。 HCO的旋转能量小于根据从头算过渡状态结构计算的脉冲模型预测的旋转能量。观察到K-a = 1倍数态N-1(u)和N-1(l)的优先群体。人口比例随光解能量而变化,在31 800 cm(-1)附近最大为12(1)(u)/ 12(1)(l)= 3.7。 HCO旋转状态之间的分布表明释放的能量似乎受到出口通道动力学的影响。 (C)1996年美国物理研究所。 [参考:37]

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