The extent of hydrogen coverage of the Si(001) c(4 × 2) surface in the presence of hydrogen gas has been studied with dispersion corrected density functional theory. Electronic energy contributions are well described using a hybrid functional. The temperature dependence of the coverage in thermodynamic equilibrium was studied computing the phonon spectrum in a supercell approach. As an approximation to these demanding computations, an interpolated phonon approach was found to give comparable accuracy. The simpler ab initio thermodynamic approach is not accurate enough for the system studied, even if corrections by the Einstein model for surface vibrations are considered. The on-set of H2 desorption from the fully hydrogenated surface is predicted to occur at temperatures around 750 K. Strong changes in hydrogen coverage are found between 1000 and 1200 K in good agreement with previous reflectance anisotropy spectroscopy experiments. These findings allow a rational choice for the surface state in the computational treatment of chemical reactions under typical metal organic vapor phase epitaxy conditions on Si(001).
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28 May 2016
Research Article|
May 31 2016
Extent of hydrogen coverage of Si(001) under chemical vapor deposition conditions from ab initio approaches
Phil Rosenow;
Phil Rosenow
Fachbereich Chemie and Wissenschaftliches Zentrum für Materialwissenschaften,
Philipps-Universität Marburg
, Hans-Meerwein-Straße, Marburg 35032, Germany
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Ralf Tonner
Ralf Tonner
a)
Fachbereich Chemie and Wissenschaftliches Zentrum für Materialwissenschaften,
Philipps-Universität Marburg
, Hans-Meerwein-Straße, Marburg 35032, Germany
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a)
Author to whom correspondence should be addressed. Electronic mail: tonner@chemie.uni-marburg.de
J. Chem. Phys. 144, 204706 (2016)
Article history
Received:
March 11 2016
Accepted:
May 13 2016
Citation
Phil Rosenow, Ralf Tonner; Extent of hydrogen coverage of Si(001) under chemical vapor deposition conditions from ab initio approaches. J. Chem. Phys. 28 May 2016; 144 (20): 204706. https://doi.org/10.1063/1.4952603
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