1992
DOI: 10.1063/1.462417
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π-bonded dimers, preferential pairing, and first-order desorption kinetics of hydrogen on Si(100)–(2×1)

Abstract: Evidence is presented that π-bonding is present in the surface dimers on clean Si(100)–(2×1) and, as a consequence, that hydrogen atoms preferentially pair on surface dimer atoms even at low coverage. We propose a simple lattice gas model in order to calculate the equilibrium distribution of doubly- and singly-occupied dimers as a function of coverage and temperature, and show that even a very conservative estimate of the enthalpy difference between hydrogen on doubly- and singly-occupied dimers can explain th… Show more

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Cited by 143 publications
(89 citation statements)
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“…4 1 " 45 As previously, for hydrogen adsorbed alone, 43 ,4 6 we attribute the near-first-order kinetics to preferential pairing of adsorbed atoms on surface dimers driven by the weak nt bonds on clean surface dimers. The presence of two types of atoms (H, X), three types of pairing (H+H, H+X, X+X), and three desorption channels necessitates a generalization of the doubly-occupied dimer model that we developed to explain the desorption kinetics of hydrogen from Si(100)2x143 and is described below.…”
Section: Competitive Pairing Modelsupporting
confidence: 72%
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“…4 1 " 45 As previously, for hydrogen adsorbed alone, 43 ,4 6 we attribute the near-first-order kinetics to preferential pairing of adsorbed atoms on surface dimers driven by the weak nt bonds on clean surface dimers. The presence of two types of atoms (H, X), three types of pairing (H+H, H+X, X+X), and three desorption channels necessitates a generalization of the doubly-occupied dimer model that we developed to explain the desorption kinetics of hydrogen from Si(100)2x143 and is described below.…”
Section: Competitive Pairing Modelsupporting
confidence: 72%
“…53 The available experimental evidence seems to favor a sequential 32 ' 5 1 desorption mechanism between H atoms paired on a single dimer. 42 -4 6 , 4 9 ,51,54 The near-first-order kinetics can be explained by preferential pairing of adsorbed hydrogen, 4 3 "46, 54 which is driven by the nt bond 55 on "unoccupied" surface dimers and has been observed directly by scanning tunneling microscopy (STM).54 Fitting the deviation from first-order kinetics at low coverage to the predictions of our doubly-occupied dimer model 4 3 leads to estimates of 5-7 kcal/mol and = 5 kcal/mol for the pairing energies of hydrogen on Si(100) 43 - 4 5 and Ge(100), 46 which is also a measure of the it bond strength on the clean surface. 4 3 ,4 6 These estimates of the pairing energy for hydrogen on Si(100) are also in reasonable agreement with values implied by recent Si-H bond strength calculations.…”
Section: Introductionmentioning
confidence: 92%
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“…The nearly constant peak temperatures, Tp, together with the asymmetric peak shape at high initial coverage, indicate near first-order desorption kinetics [9]. However, the slight increase in Tp and the more symmetric peak shape at lower initial coverages demonstrate a slight departure from first-order kinetics, as also occurs for hydrogen on Si(100) [10][11][12]. The dependence of Tp on 0 is shown in Fig.…”
Section: Resultsmentioning
confidence: 83%
“…The 71 bonds on clean surface dimers provide a driving force for pairing of adsorbates on the dimers [12,15]. For hydrogen the pairing enthalpy is approximately equal to the ii-bond strength [12,16].…”
Section: Discussionmentioning
confidence: 99%