首页> 外文期刊>Journal of the American Chemical Society >Adsorption Energy, Growth Mode, and Sticking Probability of Ca on Poly(methyl methacrylate) Surfaces with and without Electron Damage
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Adsorption Energy, Growth Mode, and Sticking Probability of Ca on Poly(methyl methacrylate) Surfaces with and without Electron Damage

机译:Ca在有电子损伤和无电子损伤的聚甲基丙烯酸甲酯表面上的吸附能,生长方式和黏附概率

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The adsorption of Ca atoms on pristine and electron-irradiated poly(methyl methacrylate) (PMMA) surfaces at 300 K has been studied by adsorption microcalorimetry, atomic beam/surface scattering, and low-energy He~+ ion scattering spectroscopy (ISS). On pristine PMMA, the initial sticking probability of Ca is 0.5, increasing quickly with Ca coverage. Below 0.5 ML, the heat of adsorption is 730-780 kJ/mol, much higher than Ca's sublimation energy (178 kJ/mol). The Ca here is invisible to ISS, which is attributed to Ca binding to ester groups below the CH_3/CH_2-terminated PMMA surface. The adsorption energy increases with coverage, suggesting attractions between neighboring Ca-ester complexes. Above 0.5 ML, Ca starts to grow as three-dimensional (3D) Ca clusters on top of the surface, which dominate growth after 2 ML. It is proposed that each Ca reacts with two esters to form the Ca carboxylate of PMMA, because this reaction's heat would be close to that observed. The total amount of Ca that binds to subsurface sites is estimated from the integral heat of adsorption to involve 4-6 layers of ester groups. Exposing the PMMA surface to electrons increases Ca's initial sticking probability but lowers its adsorption energy. This is attributed to electron-induced defects acting as nucleation sites for 3D Ca islands, whose growth now competes kinetically with Ca diffusing to subsurface esters. Consequently, only two layers of subsurface esters get populated at saturation. The heat eventually reaches Ca's bulk heat of sublimation on all PMMA surfaces, where pure, bulk-like Ca thin films form.
机译:通过吸附量热法,原子束/表面散射和低能He〜+离子散射光谱(ISS)研究了300 K下原始和电子辐照的聚甲基丙烯酸甲酯(PMMA)表面上Ca原子的吸附。在原始的PMMA上,Ca的初始粘附概率为0.5,随Ca覆盖率的增加而迅速增加。低于0.5 ML,吸附热为730-780 kJ / mol,远高于Ca的升华能量(178 kJ / mol)。此处的Ca对ISS不可见,这归因于Ca与CH_3 / CH_2封端的PMMA表面下方的酯基结合。吸附能随覆盖率的增加而增加,表明相邻的Ca-酯络合物之间具有吸引力。高于0.5 ML时,Ca开始在表面顶部以三维(3D)Ca簇的形式生长,在2 ML后主要控制生长。提议每个Ca与两种酯反应形成PMMA的Ca羧酸盐,因为该反应的热量接近所观察到的热量。从吸附的积分热估计结合到地下部位的Ca的总量,其中涉及4-6层酯基。将PMMA表面暴露于电子会增加Ca的初始粘附几率,但会降低其吸附能。这归因于电子诱导的缺陷,充当3D Ca岛的形核位点,其生长现在与Ca扩散到地下酯中发生了动力学竞争。因此,只有两层地下酯处于饱和状态。热量最终到达所有PMMA表面上的Ca升华体热,在那里形成纯的块状Ca薄膜。

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