A significantly large thermoelectric "figure of merit" in a bipolar semicon
ductor is achieved by converting it, by doping, into an essentially monopol
ar semiconductor. We show here, that for a bipolar semiconductor film, havi
ng a thickness smaller than the screening length, there is an alternative t
o doping to obtain a practically monopolar semiconductor. The electric-fiel
d effect (EFE) or the ferroelectric-field effect can be used to quench the
concentration of one type of charge carriers. We show that this method is p
articularly suited for narrow-gap semiconductors and for semimetals, having
sufficiently high dielectric permittivity. We also show that this "EFE dop
ing" is free from the drawbacks of conventional doping. Our analysis demons
trates that increased values of the figure of merit are feasible. We presen
t here the theory and the figure-of-merit calculation for typical cases of
the bipolar semiconductor thermoelectric film under EFE doping. Numerical r
esults for a film of the PbTe type are presented. (C) 2001 American Institu
te of Physics.