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Activation energies for thermal ionic and neutral desorptions from thin films of lithium halides

机译:活化能,用于卤化锂薄膜的热离子和中性解吸

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To clarify the mechanism of positive-ionic and neutral desorptions from heated lithium halide (LiX, X = F, Cl, Pr or I), a small amount (approx. 10(-12)-10(-7) mol) of LiX was deposited on a platinum plate (ca. 0.03-0.04 cm(2)) to prepare a thin film (theta(0) = 10(-1)-10(3) molecular layers at the start), and it was heated up to ca. 1500 K at a constant rate (beta = 0.4-140 K/s) in vacuum (approx. 10(-4) Pa) using our dual-ion source system which made it possible to measure simultaneously the desorption rates (D-0 and D+) of neutral molecule (LiX0) and ion (Li+). The temperature-programmed desorption spectra thus obtained were different in pattern from that observed previously with NaX where each of NaX0 and Na+ had only one peak. Namely, the high peaks (P-1(0) and P-2(+)) of LiX0 and Li+ appeared at a temperature generally lower and higher than the melting point (T-m) of each LiX, respectively, while low peaks (P-1(+), P-2(0), P-0(3) and P-3(+)) appeared usually above T-m. Theoretical analysis of the beta-dependence of peak appearance temperatures yields the activation energies (E-1(0+)-E-3(0+)) for desorption of LiX0 (or Li+) giving P-1(0+)-P-3(0+), respectively, and also the frequency factors (nu(1)(0+)-nu(2)(0+)) corresponding to respective peaks. With respect to LiF (theta(0) approximate to 13 molecular layers), for example, E-1(0) and E-1(+) were 220 and 167 kJ/mol, respectively, while nu(1)(0) and nu(1)(+) were respectively 1 x 10(17) and 8 x 10(10)/s. In conclusion, (1) each desorption obeys the first-order kinetics, (2) P-1(0)-(0)(3) originate from the desorption from LiX at the state of physical adsorption, crystal or chemisorption, (3) P-1(+)-P-3(+) are due to the desorption from active sites (high work function sites; e.g., 724 kJ/mol for LiCl)on the heterogeneous surface of LiX itself or Pt, and (4) the ionization efficiency (D+/D-0) even at P-1(+)-P-3(+) is usually less than 1% mainly because the fraction of the active sites is less than 1% of the desorbing surface area. (C) 2000 Elsevier Science B.V. All rights reserved. [References: 11]
机译:为了阐明从加热的卤化锂(LiX,X = F,Cl,Pr或I)进行正离子和中性解吸的机理,少量(大约10(-12)-10(-7)mol)LiX将其沉积在铂板上(约0.03-0.04 cm(2))以制备薄膜(theta(0)= 10(-1)-10(3)分子层开始),并将其加热至使用我们的双离子源系统,在真空中以恒定速率(β= 0.4-140 K / s)(约10(-4)Pa)可达到1500 K,这使得同时测量解吸速率(D-0和中性分子(LiX0)和离子(Li +)的D +)。如此获得的程序升温解吸光谱与以前用NaX观察到的模式不同,在NaX中,NaX0和Na +各自只有一个峰。即,LiX0和Li +的高峰(P-1(0)和P-2(+))分别出现在通常分别低于和高于每个LiX熔点(Tm)的温度下,而低峰(P -1(+),P-2(0),P-0(3)和P-3(+))通常出现在Tm之上。对峰出现温度的β依赖性的理论分析得出了LiX0(或Li +)解吸给出P-1(0 +)-P的活化能(E-1(0 +)-E-3(0+))分别为-3(0+),还有对应于各个峰值的频率因子(nu(1)(0 +)-nu(2)(0+))。对于LiF(θ(0)大约为13个分子层),例如,E-1(0)和E-1(+)分别为220和167 kJ / mol,而nu(1)(0)和nu(1)(+)分别为1 x 10(17)和8 x 10(10)/ s。综上所述,(1)每次解吸都遵循一级动力学,(2)P-1(0)-(0)(3)源自物理吸附,晶体或化学吸附状态下LiX的解吸,(3 )P-1(+)-P-3(+)是由于LiX本身或Pt异质表面上的活性位点(高功函数位点;例如,对于LiCl为724 kJ / mol)解吸而引起的;和(4 )即使在P-1(+)-P-3(+)时电离效率(D + / D-0)通常也小于1%,这主要是因为活性位点的比例小于解吸表面积的1% 。 (C)2000 Elsevier Science B.V.保留所有权利。 [参考:11]

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