1991
DOI: 10.1016/0039-6028(91)90911-b
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Comparison of hydrogen desorption kinetics from Si(111)7 × 7 and Si(100)2 × 1

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Cited by 281 publications
(63 citation statements)
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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 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%
“…For this surface, experiments have shown that desorption obeys an approximately second-order kinetics with an activation barrier of ~ 2.5 eV [17][18][19][20]. As for Si(100)-(2 x 1), sticking-coefficient measurements have shown that adsorption is activated with an effective barrier of 0.87 +0.1 eV [21].…”
mentioning
confidence: 99%
“…that the first-order kinetics results from the rate-limiting excitation of hydrogen atoms to a band-like delocalized state 1 was contradicted by the near-second-order kinetics observed for desorption of hydrogen from Si( 11),2-4 by measurements of the diffusion kinetics of hydrogen on Si(l 11) which suggest conventional hopping, 5 and by dynamical measurements showing that desorbing H 2 is rotationally cold and vibrationally hot, implying a highly symmetric transition state. 6 Wise et al 2 suggested that the desorption kinetics are first order due instead to pairing of hydrogen on the dimerized surface atoms, and Boland 7 and we 8 independently proposed that preferential pairing of H atoms is a consequence of the ic bond 9 , 10 on "unoccupied" dimers. Boland obtained direct evidence for preferential pairing by scanning tunneling microscopy (STM) and estimated a a bond strength of =18 kcal/mol from tunneling spectra above un-and singly-occupied dimers.…”
Section: Submitted To Journal Of Vacuum Science and Technology A Intrmentioning
confidence: 78%
“…14 The adsorbate-ordering portion of this model is precisely a one-dimensional lattice gas model with nearest neighbor interactions whose solution has been described by Hill. 16 Defining e9 and a as the surface hydrogen coverage and the fraction of "bonds" between adjacent dimers where one of the dimers is (doubly) occupied and the other is unoccupied, the solution to the mximization condition for the partition function can be written as 16 a 2 (2) (e-a) (1-e-a)…”
Section: Generalized Model and Theoretical Methodsmentioning
confidence: 99%
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