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Cl 2 plasma etching of Si(100): Nature of the chlorinated surface layer studied by angle-resolved x-ray photoelectron spectroscopy
83
Citations
22
References
1997
Year
EngineeringChemistrySilicon On InsulatorPlasma ProcessingSemiconductorsSiliceneMaterials ScienceCrystalline DefectsChlorinated Surface LayerCl2 PlasmaPlasma EtchingSurface CharacterizationSi Xps SignalsSurface AnalysisSurface ScienceApplied PhysicsCl 2Ion EnergySolar Cell Materials
The interaction of a Cl2 plasma with a Si(100) surface has been investigated by angle resolved x-ray photoelectron spectroscopy (XPS). It was found that the amount of chlorine incorporated into the near-surface region of Si increases with ion energy, and does not change with long exposure to the plasma. Chlorine is present as SiClx (x=1–3) with average relative coverages (integrated over depth) of [SiCl]:[SiCl2]:[SiCl3]≅1:0.33:0.13 at −240 V dc bias (mean ion energy ≈280 eV) and 1:0.34:0.087 at 0 V dc bias (mean ion energy ≈40 eV), at x-ray photoelectron spectroscopy (XPS) binding energies of 100.2, 101.2 and 102.3 eV, respectively. Moreover, there is a substantial amount of disordered Si within the chlorinated layer at high ion energy, reflected in a broadening of the 99.4 eV Si peak and the appearance of a shoulder at 98.8 eV, ascribed to Si with a dangling bond. In addition, bulk Si plasmon losses associated with the Cl(2p) and Cl(2s) core levels indicate that roughly one-third of the Cl in the near-surface region is surrounded by bulklike Si at the high ion energy. Modeling of the dependence of the relative concentration of Cl on the take-off angle was used to estimate the Cl content and thickness of the surface layer. From an inversion of the observed take-off angle dependence of the relative Cl and Si XPS signals, depth profiles were derived for the near-surface region. Cl content falls off in a graded fashion, over a depth of about 25 and 13 Å for a mean ion energies of 280 and 40 eV, respectively. The Cl areal density (coverage integrated throughout the layer) increases with increasing mean ion energy from 1.8×1015 Cl/cm2 at 40 eV to 3.5×1015 Cl/cm2 at 280 eV. From a similar inversion of the take-off angle dependence of the SiClx signals, SiCl2 and SiCl3 are found to be largely confined at the top ∼5 Å, while below the surface, disordered Si and SiCl are present.
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