“…The free energy of formation of both defects is determined by the enthalpy and entropy terms as given by Pi = a, -g,kT , Pv = a,g , k T , corresponding in general to (1). The excess interstitial concentration n, of the space charge layer can be calculated for each temperature from the equation The values for { 111) layers coincide surprisingly well with those calculated in our earlier paper [18], using the data for the surface potential of Sonoike and Wakabayashi [22]. Therefore, for the free energies of formation of Frenkel defects on the surface one can write in spite of the different bulk conductivity found in both measurements, one arrives a t the quite relevant conclusion that the disorder in the subsurface region is not substantially influenced by the concentration of defects in the bulk phase.…”