1999
DOI: 10.1016/s0009-2614(98)01375-x
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VUV photodesorption of molecular hydrogen from the hydrogenated silicon(111) surface

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Cited by 3 publications
(2 citation statements)
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“…(11) and (12) over all configurations ͕͖ and assume translational invariance from here on, i.e., in the limit L → ϱ there are no privileged sites in the lattice. Then we have ͗ i ͘ = ͗ j ͘ = ͑t͒ and ͗ i i+1 ͘ = ͗ j j+1 ͘ = C 2 ͑t͒ for all i, j, where C 2 ͑t͒ is the two-particle correlation.…”
Section: Theoretical Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…(11) and (12) over all configurations ͕͖ and assume translational invariance from here on, i.e., in the limit L → ϱ there are no privileged sites in the lattice. Then we have ͗ i ͘ = ͗ j ͘ = ͑t͒ and ͗ i i+1 ͘ = ͗ j j+1 ͘ = C 2 ͑t͒ for all i, j, where C 2 ͑t͒ is the two-particle correlation.…”
Section: Theoretical Analysismentioning
confidence: 99%
“…For example, in ultrahigh vacuum CVD for the case of Si(100), molecular hydrogen forms by recombination at localized monohydride dimers ͑H-Si-Si -H͒ [6,9,10]. Wetterauer et al [11] found that this pathway is supplemented by single atom photodesorption from a hydrogenated Si(111) surface. In plasma-enhanced CVD growth of hydrogenated amorphous and microcrystalline silicon, which are emergent alternatives to crystalline Si in many electronic devices, impinging hydrogen gas atoms recombine with Sihydrides but also with bonded hydrogen surface atoms to form H 2 .…”
Section: Introductionmentioning
confidence: 99%