The influence of As surface concentration C
SEon the emitter efficiency β
γand the temperature dependence of β
γare reported. The theoretical model that is used to explain the variation of β
γwith C
SEis based upon the difference in the effective energy bandgaps in the emitter and base regions

. Experimental measurements of

versus C
SEare presented. Measurements of β
γversus C
SEshow that the effective emitter doping density

reaches a maximum value at

atoms/cm
3, corresponding to the threshold above which

. For the case of a constant active base doping/cm
2Q
B, this also corresponds to an optimum in the emitter efficiency β
γ. However, it is shown that in typical sequential diffusion processing of transistors, β
γincreases monotonically with C
SEbecause

decreases. In addition, for devices fabricated in this study,

at

atoms/ cm
3for As-diffused emitters (doped oxide) was ≈ 5 times greater than for ion-implanted-diffused As emitters, showing the superiority of implantation in controlling gain. Finally, transistors that were made with

atoms/cm
3(

) showed β
gamma(85°C)/ β
γ(-15°C) ≤ 1.05.