首页> 外文期刊>The Journal of Chemical Physics >PHOTOCHEMISTRY OF ADSORBED MOLECULES .15. LOCALIZED ATOMIC SCATTERING IN THE PHOTOLYSIS OF HI/LIF(001) AND HI/NAF(001)
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PHOTOCHEMISTRY OF ADSORBED MOLECULES .15. LOCALIZED ATOMIC SCATTERING IN THE PHOTOLYSIS OF HI/LIF(001) AND HI/NAF(001)

机译:吸附分子的光化学.15。 HI / LIF(001)和HI / NAF(001)光解中的局部原子散射

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We have compared the ''elastic'' H atom angular-scattering, P-el(theta'), of HI(ad) photolyzed at 248 nm for LiF and NaF substrates, both experimentally and theoretically. The observed P-el(theta') for elastic scattering were similar for LiF and NaF, with a peak in the range 43 degrees-48 degrees. The P-el(theta') for H from HI/NaF was broader than that for H from HI/LiF. Energy distributions, P(E(T')), for H recoiling from HI/LiF and HI/NaF are also reported, A semiempirical potential-energy surface (pes) is given for HI adsorbed on NaF, based on an earlier one for LiF [J. Chem. Phys. 94, 978 (1991)]. Ab initio ''density function theory'' (DFT) calculations were performed to verify the suitability of this pes; the DFT points were in satisfactory agreement with the semiempirical pes. For HI/LiF the DFT calculation gave a heat of adsorption of about 9 kcal/mol, the semiempirical model gave 5 kcal/mol, and experiment gave 7 kcal/mol. We have computed H atom scattering by the classical trajectory method for two different models one involving dense and the other perforated arrangements of the HI adsorbate molecules, Comparison with tine experimental results showed that the second model gave a better description of both P-el(theta') and P(E(T')) for HI/LiF and HI/NaF. The calculations showed that the angular and energy distributions of the scattered H were sensitive to the size of the vacancies between adjacent adsorbate molecules. The study also indicates the importance of unit-cell size in relation to the size of the adsorbate molecule in determining adsorbate geometry and hence the energy and angular distributions of the scattered photofragments. (C) 1996 American Institute of Physics. [References: 26]
机译:我们在实验和理论上都比较了LiF和NaF衬底在248 nm处光解的HI(ad)的“弹性” H原子角散射P-el(θ')。对于LiF和NaF,观察到的用于弹性散射的P-el(θ')相似,其峰在43度至48度的范围内。来自HI / NaF的H的P-el(θ')比来自HI / LiF的H的P-el(θ')宽。还报道了从HI / LiF和HI / NaF进行H反冲的能量分布P(E(T'))。基于较早的HI吸附在NaF上的HI给出了半经验势能面(pes)。 LiF [J.化学物理94,978(1991)]。从头开始进行“密度泛函理论”(DFT)计算以验证该pes的适用性; DFT点与半经验值pe令人满意。对于HI / LiF,DFT计算得出的吸附热约为9 kcal / mol,半经验模型得出的吸附热为5 kcal / mol,实验得出的结果为7 kcal / mol。我们通过经典轨迹法对两个不同的模型进行了H原子散射计算,两个模型涉及HI吸附物分子的密集排列和另一个穿孔排列,与常规实验结果比较表明,第二个模型对P-el(θ ')和HI / LiF和HI / NaF的P(E(T'))。计算表明,散射氢的角度和能量分布对相邻吸附分子之间空位的大小敏感。这项研究还表明,在确定吸附物的几何形状以及由此确定的散射光碎片的能量和角度分布方面,相对于被吸附物分子的大小而言,晶胞大小的重要性。 (C)1996年美国物理研究所。 [参考:26]

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