The (3 x 3) reconstruction of the InSb (l 1 1) surface has been analysed using grazing incidence X-ray diffraction. The reconstruction is characterized by hexamers above a complete InSb double-layer centred around an Sb atom. No vacancies are found in the structure as predicted theoretically. The results agree with scanning tunnelling microscopy measurements.
Results and discussionThe (1 1 1) surface of InSb is terminated by Sb atoms and has a (3 × 3) reconstruction. In contrast to the In terminated (1 1 1) surface which has a (2 x 2) reconstruction [1] little is known about the atomic structure of this polar surface. From total energy calculations [2] no vacancies are expected which have been observed for InSb (1 1 1) (2 × 2) and GaAs (1 1 1) (2 × 2) [3].The InSb (1 1 1) surface was prepared in UHV by Ar + ion bombardment and annealing at 673 K for about 3 h followed by slow cooling to room temperature (2 K/min). The data were collected at the W1 wiggler beam line at the Hamburger Synchrotron Strahlungs Laboratory (HASYLAB) at an X-ray incidence angle of ~i = 1"0° and an X-ray wavelength of 2 = 1.316/~. The data set consists of 278 independent reflections, corresponding to 71 in-plane superlattice reflections (q± =/xc*~0) and to 24 superstructure lattice rods measured up to a maximum momentum transfer normal to the sample surface, q± = 0.64 ~,-1 * Corresponding author.The large out-of-plane dataset was essential for deriving an unambiguous structure model since it allows the calculation of Patterson sections. The Figs. l(a) and l(b) show the Patterson functions calculated on the basis of the q± = 0 dataset and the dataset including the q±-~0 reflections, respectively. Correspondingly, Fig. l(a) shows the Patterson function projected along z, the coordinate normal to the sample surface. In contrast, in Fig. l(b) the section P(u v 0) is shown where two (positive) interatomic vectors are indicated by 1 and 2. Additional maxima are also observed and they will be discussed elsewhere [4]. The interpretation of these vectors was the key for solving the structure.The (in-plane) vectors observed in the P(uvO) function can be related to interatomic vectors within a six-membered ring shown in Fig. 2. The assignment of the atoms to In and Sb was made on the basis of the bonding angles (sp z hybridization of In and p-type bonding of Sb). The whole structure on the basis of the best fit to the measured data (Rw = 0.045, GOF = 1.09) is shown in Fig. 3. A different ring structure has been determined for the (x/~ x x//~) surface of GaAs from STM measurements I-5].