Surface-shift low-energy photoelectron diffraction: Clean and hydrogenated GaAs(110) surface-structure relaxation (original) (raw)

Surface structure of GaAs(2 5 11)

Physical Review B, 2002

GaAs samples with orientations vicinal to ͑2 5 11͒ within 1°were prepared by molecular beam epitaxy and analyzed in situ by scanning tunneling microscopy, low-energy electron diffraction, and reflection high-energy electron diffraction. In addition, first-principles electronic structure calculations were carried out. GaAs͑2 5 11͒ is a stable surface whose orientation is located within the stereographic triangle. For a wide range of As-rich conditions a (1ϫ1) reconstruction forms that is characterized by an inclined series of three As dimers and that fulfills the electron counting rule. The terrace size is limited only by the macroscopic off-orientation of the samples. The surface is perturbed by thin stripes of the nearby orientation ͑3 7 15͒. While the dangling bond densities of GaAs͑2 5 11͒ and GaAs͑3 7 15͒ are almost equal, GaAs͑3 7 15͒ violates the electron counting rule. The analysis of this perturbation suggests that, in general, on semiconductor surfaces the gain in stability arising from the minimization of the number of dangling bonds is significantly greater than the gain arising from reaching a semiconducting ground state. Upon annealing of the samples in ultrahigh vacuum, a fairly rough surface structure develops whose mean orientation is different from ͑2 5 11͒.

GaAs(110) surface electronic structure by metastable deexcitation spectroscopy

Physical Review B, 1995

Metastable deexcitation spectroscopy was applied to study the surface valence electronic structure of clean cleaved GaAs(110). Metastable deexcitation spectroscopy was flanked by angle-resolved photoemission. An effective surface density of states was derived from the experimental spectrum through deconvolution. Two groups of states were observed in the 0 -4 and 5 -8 eV range of binding energy, respectively. These features were ascribed to emission from surface states. A plane-by-plane tight-binding density-of-states calculation was performed. More quantitative insights were obtained by comparing experimental and theoretical results. The most prominent feature of the first group of states of deconvolution was assigned to surface state As. Contributions from states A4, A3 A1, and A2 were also observed. The doublet of the second group of features was identified with Cq and C1. Relative amplitudes of effective surface density of states were related to surface charge density.

Theoretical Study of the Surface Optical Properties of Clean and Hydrogenated GaAs(110)

physica status solidi (a), 1999

We present a calculation of the electronic and optical properties of the GaAs : H surface performed within the first-principles density functional theory (DFT) in the local density approximation (LDA). The geometry and electronic structure are analyzed and compared with those of the clean surface. The reflectance anisotropy spectrum and the differential reflectivity are then computed. Taking into account the usual underestimation of the LDA gaps with respect to the experimental values, the comparison between our theoretical spectra with available experimental reflectance data shows a satisfactory agreement, allowing for the interpretation of the main structures in terms of electronic transitions.

Surface electronic structure of GaAs(311)A studied by angle-resolved photoelectron spectroscopy

Surface Science, 1996

The valence and core electronic structure of the sputtered and annealed 1 × 1 periodic GaAs(311)A surface has been studied by angle-resolved photoelectron spectroscopy. Five surface bands are identified and their dispersions along high symmetry lines in the surface Brillouin zone are mapped out. While electron-counting indicates a metallic surface, the experiment show no evidence for partly occupied surface bands. Analysis of the core level spectra reveals one As and two Ga surface shifted components. The results are discussed in terms of surface geometry models.

The morphology of high-index GaAs surfaces

Applied Surface Science, 2000

Ž. Ž. Ž. In this contribution, an overview of the research work in our group on the GaAs 112 , 113 and 114 surfaces is Ž. presented. Samples were prepared by molecular beam epitaxy MBE and analyzed in situ by low-energy electron diffraction Ž. Ž. Ž. LEED , core level spectroscopy and scanning tunneling microscopy STM. The GaAs 112 A surface is unstable and Ä 4 Ž. Ä 4 decomposes into five facets of the orientations 110 , 111 and 124. Real space images reveal that the facets form Ž. depressions whose horizontal cross-section is an irregular pentagon. For the GaAs 113 A surface, our results support the Ž. Ž. Ž. 8 = 1 reconstruction proposed by Wassermeier et al. On the GaAs 114 A surface a c 2 = 2 reconstruction was found. A Ž. Ž. structure model based on the GaAs 001-2 = 4 a reconstruction is in agreement with all our results.

GaAs(001) surface reconstructions: geometries, chemical bonding and optical properties

Applied Surface Science, 2002

We re-examine the GaAs(0 0 1) surface by means of first-principles calculations based on a real-space multigrid method. The cð4 Â 4Þ; ð2 Â 4Þ and ð4 Â 2Þ surface reconstructions minimize the surface energy for anion-rich, stoichiometric and cation-rich surfaces, respectively. Structural models proposed in the literature to explain the Ga-rich GaAs(0 0 1) ð4 Â 6Þ surface are dismissed on energetic grounds. The electronic properties of the novel zð4 Â 2Þ structure are discussed in detail. We calculate the reflectance anisotropy of the energetically most favoured surfaces. A strong influence of the surface geometry on the optical anisotropy is found. #

Geometric ordering, surface chemistry, band bending, and work function at decapped GaAs(100) surfaces

Physical Review B, 1992

We present a comprehensive study of epitaxially grown and As-coated GaAs(100) surfaces as a function of As desorption temperature and background pressure. We have used low-energy electron diffraction to determine surface reconstruction, and core-level and valence-band soft-x-ray photoemission spectroscopy to perform chemical and electronic characterization of these surfaces. We find gradual changes in surface geometry and composition, and a limited (-120 meV) Fermi-level movement over numerous reconstructions in the 250-650'C annealing temperature range. The surface ionization potential and work function exhibit large changes between different surface reconstructions. In conjunction with other techniques, work-function measurements present evidence of surface inhomogeneity for many of the desorption temperatures and surface reconstructions. This inhomogeneity appears related to the existence of differently reconstructed patches on the surface. Our results emphasize the complexity of reconstructed GaAs(100) surfaces and the advantages of a multiple-technique approach for their characterization.

Structure and energetics of Ga-rich GaAs() surfaces

Surface Science, 2002

The atomic structures and energies of Ga-rich GaAs(0 0 1) surface reconstructions are examined by means of firstprinciples total-energy calculations based on a real-space multigrid method. Our calculations confirm the existence of the novel f(4 Â 2) structure suggested by Lee et al. [Phys. Rev. Lett. 85 (2000) 3890]. (4 Â 6) surface reconstructions suggested to explain STM experiments are found to be unstable. The calculations indicate that the adsorption of Ga adatoms in the trenches of the f(4 Â 2) surface could possibly explain the observed structures. The diffusion of Ga/As adatoms on the Ga-rich GaAs surface is predicted to be anisotropic and should preferably take place parallel to the [1 1 0]/[1 1 1 0] direction, respectively. Ó