AVS 66th International Symposium & Exhibition
    Electronic Materials and Photonics Division Tuesday Sessions
       Session EM+2D+AP+NS+PS-TuM

Paper EM+2D+AP+NS+PS-TuM6
Mechanism of Chalcogen Passivation of GaAs Surfaces

Tuesday, October 22, 2019, 9:40 am, Room A214

Session: New Devices and Materials for Electronics and Photonics
Presenter: Takayuki Suga, UEC-Tokyo, Japan
Authors: T. Suga, UEC-Tokyo, Japan
S. Goto, UEC-Tokyo, Japan
A. Ohtake, NIMS, Japan
J.N. Nakamura, UEC-Tokyo, Japan
Correspondent: Click to Email

GaAs surfaces are stabilized by surface treatments with Se or S through the reduction of the dangling bond density [1,2]. It has long been thought that the Se- or S-treated GaAs(111)B-(1x1) surface has a simple structure; the outermost As atoms of the ideal (111)B surface are completely replaced by Se or S atoms, the Se- or S-terminated model [3]. In general, the structural stability of compound semiconductor surfaces can be explained in terms of the so-called electron-counting rule (ECR) [4]. The Se- or S-terminated model, however does not satisfy ECR. Recently, the atomic structure of the Se-treated GaAs(111)B surface has been revisited [5] and another structure model has been proposed, where the Se atoms substitute 3/4 of the topmost surface As atoms in a (2x2) unit [6]. This mixed Se/As-terminated model satisfies ECR, being electronically stable [6]. We have depicted phase diagrams of Se- or S- treated GaAs(111)B surface at 0K as functions of the chemical potentials of Se (ΔμSe(S)) and As (ΔμAs). The (2x2) As-trimer and the mixed Se(S)/As-terminated surfaces appear under Se poor condition. It is noted that the Se- or S-terminated surface also becomes stable as ΔμSe or ΔμS increases, respectively, even though these surfaces are not qualified for ECR.

The Se(S)-treated GaAs(111)B surface is prepared experimentally by molecular beam epitaxy under a finite temperature and a gas pressure. Therefore, it is necessary to consider the free energy of a molecule in vapor phase. In this study, we investigate the stabilization of the Se- or S-treated GaAs(111)B surface structures by considering the beam equivalent pressure of As and Se(S) in a growth temperature using the first-principles calculations within the density functional theory. The chemical potentials of molecules are derived from the partition functions for the translation, the rotation, and the vibrational motions.

In the phase diagram for the actual experiment condition, T=800K, the mixed Se/As terminated surface appears in the Se pressure of 10-15-10-5 Torr, being consistent with the recent experiment [5]. Surprisingly, the Se-terminated surface also becomes stable as the Se pressure increases. We will discuss the stabilization mechanism of the chalcogen-treated GaAs surfaces.

[1]J. Fan, H. Oigawa and Y. Nannichi, Jpn. J. Appl. Phys. 27, L2125 (1998).

[2]T. Scimeca, Y. Watanabe, R. Berrigan, and M. Oshima, Phys. Rev. B 46, 10201 (1992).

[3]V. N. Bessolov and M.V. Lebedev, Semiconductors 32, 11 (1998).

[4]M.D. Pashley, Phys. Rev. B 40, 10481 (1989).

[5]A. Ohtake and Y. Sakuma, Cryst. Growth Des. 17, 363 (2017).

[6]A. Ohtake, S. Goto and J. Nakamura, Sci. Rep. 8, 1220 (2018).