GAAS EPITAXIAL LAYERS OBTAINED BY CLOSE-SPACED VAPOR TRANSPORT IN H2-FINE CONTROL OF THE GROWTH-RATE AND ITS EFFECT ON THE ELECTRICAL-PROPERTIES OF THE LAYERS(H2O AND H2+CO2 AMBIENTS )
D. Cossement et al., GAAS EPITAXIAL LAYERS OBTAINED BY CLOSE-SPACED VAPOR TRANSPORT IN H2-FINE CONTROL OF THE GROWTH-RATE AND ITS EFFECT ON THE ELECTRICAL-PROPERTIES OF THE LAYERS(H2O AND H2+CO2 AMBIENTS ), Canadian journal of physics, 72(1-2), 1994, pp. 44-50
In view of developing the close-spaced vapor transport technique (CSVT
) to obtain III/V homojunction solar cells, it is necessary to finely
control the growth rate of GaAs epitaxial layers. This has been perfor
med either by controlling the water vapor pressure, P(H2O), injected i
n the reactor along with H-2, in H-2 + H2O ambient, or by controlling
the water vapor pressure generated in situ by the reaction of H-2 + CO
2 in the reactor. For H-2 + CO2 ambient, P(CO2), controls P(H2O) accor
ding to the following reaction: 2 H-2(g) + CO2(g) reversible 2 H2O(g)
+ C(s). The growth rates calculated with a diffusion controlled model
are in agreement with the experimental values for both ambients, inclu
ding the observation of a maximum in the evolution of the growth rate
with P(CO2). Controlling the growth rate of GaAs by changing P(H2O) af
fects the carrier density (N(A) - N(D)) of P-type layers grown from Zn
-doped GaAs, sources. In both ambients (N(A) - N(D)) is a function of
P(H2O)1/2. Such a behavior is also obtained for the calculated carrier
densities. It is the result of the transport of Zn as ZnO in CSVT. In
H-2 + CO2 ambient, where H2O and C are generated in situ, carbon is n
ot incorporated as a major p-type doping impurity, contrarily to expec
tations. n-type GaAs layers were also obtained from Te-doped GaAs sour
ces. In that case, the measured N(A) - N(D) values are not affected by
changes in P(H2O) because water is not involved in the transport of T
e in CSVT.