The positron-annihilation method was used to investigate the DX center
s in Te-doped AlxGa1-xAs grown by metal-organic vapor-phase epitaxy. V
acancy defects were found in all layers. The vacancy signal disappears
when the DX center is ionized either optically or thermally. After th
e optical ionization the vacancy signal reappears when the temperature
increases over 50 K. The optical cross section of 4X10(-17) cm(2) was
determined for the removal of the positron trapping at a vacancy. Bec
ause the properties of the vacancy signal correlate exactly with those
determined earlier for the DX(Te) center, we conclude that the vacanc
y detected by positrons belongs to the atomic structure of the DX(Te)
center. This result is in agreement with the vacancy-interstitial mode
l, which predicts that in the case of group-VI(Te) doping the DX cente
r is formed by the distortion of the Ga atom towards the interstitial
position. The positron results indicate further that the open volume o
f the vacancy related to the DX(Te) center is smaller compared to an i
solated monovacancy in GaAs or to the vacancy in the DX(Si) center in
AlxGa1-xAs. This means that the distortion in the vacancy-interstitial
configuration is smaller in the DX(Te) than in the DX(Si) center.