首页> 外文期刊>The Journal of Chemical Physics >PHOTOCHEMISTRY OF ADSORBED MOLECULES .18. PHOTODISSOCIATION AND EXCHANGE REACTION IN CH3BR/MGO(001) AT 193 NM
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PHOTOCHEMISTRY OF ADSORBED MOLECULES .18. PHOTODISSOCIATION AND EXCHANGE REACTION IN CH3BR/MGO(001) AT 193 NM

机译:吸附分子的光化学.18。 CH3BR / MGO(001)在193 NM处的光解离和交换反应

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Methyl photofragments from the 193 nm photodissociation of CH3Br adsorbed on MgO(001) were studied by angularly resolved time-of-flight mass spectrometry. The translational energy distributions of the photofragments showed evidence of three pathways for the release of CH3. The pathways were termed ''direct'' [DIR], ''indirect(1)'' [IND(1)], and ''indirect(2)'' [IND(2)]. The DIR methyl translational energy distribution, P(E-T') peaked at 2.3 eV, with a full width at half-maximum (FWHM) of 0.65 eV, corresponding roughly to that reported for gas phase CH3 (peak=2.5 eV, FWHM=0.5 eV). The P(E-T') of the DIR pathway was consistent with CH3 escaping directly from the topmost molecular layer without collisions. For these DIR methyls, as previously demonstrated, the angular distribution reflected the prior Br-C bond direction. In the higher coverage range, 1.5-10 monolayers (ML) angular distributions, P(Theta'), for the DIR methyls peaked at 22 degrees to the normal with FWHM of 20 degrees. At low coverage, 0.75 ML, the DIR peak shifted to similar to 40 degrees with doubled FWHM. The IND(1) methyls, despite the loss of 1.2 eV in a strong inelastic encounter, exhibited the same angular distributions and FWHM as the DIR component: 22 degrees peak, 20 degrees FWHM at high coverage; 40 degrees peak, 40 degrees FWHM at low coverage. The mechanism attributed to IND(1), which accounts for the retention of direction of methyl with concurrent substantial energy loss, is one proposed in a prior theoretical study [Barclay et al., J. Phys. Chem. 97, 12541 (1993)]: an exchange reaction favored by the adsorbate geometry; in the present case CH3+BrCH3'-->CH3Br+CH3'. The second indirect channel, IND(2), exhibited broader translational energy distribution than DIR or IND(1) peaked at 0.6 eV lower energy than IND(1), and a broad angular distribution (cos(2) Theta') peaked at the normal, characteristic of strongly inelastic encounters in which memory of the initial CH3 recoil direction is lost. (C) 1997 American Institute of Physics. [References: 36]
机译:通过角分辨飞行时间质谱法研究了吸附在MgO(001)上的CH3Br的193 nm光解离所产生的甲基碎片。光碎片的翻译能量分布显示了CH3释放的三种途径的证据。这些途径被称为“直接” [DIR],“间接(1)” [IND(1)]和“间接(2)” [IND(2)]。 DIR甲基平移能分布P(E-T')的峰值为2.3 eV,最大半峰全宽(FWHM)为0.65 eV,大致相当于气相CH3的报告峰宽(峰值= 2.5 eV,FWHM) = 0.5 eV)。 DIR途径的P(E-T')与CH3直接从最顶层的分子层逸出而没有碰撞相一致。如前所述,对于这些DIR甲基,角分布反映了先前的Br-C键方向。在更高的覆盖范围内,DIR甲基的1.5-10个单层(ML)角分布P(Theta')在相对于法线高度为20度的法线的22度处达到峰值。在0.75 ML的低覆盖率下,FWHM翻倍,DIR峰移至近似40度。尽管在强烈的非弹性碰撞中损失了1.2 eV,但IND(1)甲基仍显示出与DIR分量相同的角度分布和FWHM:高覆盖度为22度峰,FWHM为20度。 40度峰值,低覆盖下40度FWHM。在先前的理论研究中提出了一种机制,该机制归因于IND(1),该机制说明了甲基的保留方向同时伴有大量的能量损失[Barclay等人,J。Phys。化学97,12541(1993)]:吸附物几何形状有利的交换反应;在当前情况下为CH3 + BrCH3'-> CH3Br + CH3'第二个间接通道IND(2)的平移能量分布比DIR或IND(1)的峰能量要比IND(1)低0.6 eV,并且峰角分布(cos(2)Theta')的峰值更宽。正常情况下,强烈的非弹性接触的特征,其中初始CH3后坐方向的记忆消失了。 (C)1997美国物理研究所。 [参考:36]

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