一种新的吸收机制:碰撞诱导吸收

K. J. Maynard, A. D. Johnson, S. P. Daley, S. Ceyer
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引用次数: 54

摘要

在Ni(111)上氢原子的吸收是由入射能量大于60 kcal mol-1的Ar、Kr或Xe原子碰撞引起的。碰撞诱导吸收的机制涉及晶格的瞬间变形,该变形打开通道,导致氢扩散到大块金属中。利用高分辨率的电子能量损失谱可以检测嵌入的氢,并根据非弹性散射电子强度与电子冲击能的依赖关系,与化学吸收氢的振动模式区分开来。嵌入氢的振动频率为800 ~ 850 cm-1,在180 ~ 220 K之间以H2形式重新结合和解吸。氢的吸收也可以通过暴露于氢原子来实现。相当于8个单层(ML)的氢被吸收了。
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A new mechanism for absorption: collision-induced absorption
The absorption of atomic hydrogen on Ni(111) is observed to be induced by collisions with Ar, Kr or Xe atoms incident with energies in the normal direction greater than 60 kcal mol–1. The mechanism for collision-induced absorption involves momentary deformation of the lattice which opens channels leading to the bulk metal into which the hydrogen diffuses. The embedded hydrogen is detectable by high-resolution electron energy loss spectroscopy and is distinguishable from the vibrational modes of chemisorbed hydrogen on the basis of the dependence of the inelastically scattered electron intensity on electron impact energy. The embedded hydrogen has a vibrational frequency of 800–850 cm–1 and is observed to recombine and desorb as H2 between 180 and 220 K. Hydrogen absorption can also be achieved by exposure to atomic hydrogen. As much as an equivalent of 8 monolayers (ML) of hydrogen has been absorbed.
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