Observation of the hole-confinement effect in boron delta-doped Si qua
ntum wells has been demonstrated using the deep-level transient spectr
oscopy (DLTS) technique, based on the concept of treating the quantum
well as a big ''trap.'' For the same doping thickness but different do
ping densities, i.e., different boron sheet doping concentrations, the
well depths acid the subband positions are different and the peak shi
ft of DLTS spectra is thus expected and is observed experimently for t
wo samples with sheet doping concentrations of about 2.4 x 10(13) and
6.0 x 10(13) cm(-2), respectively. A self-consistent calculation of th
e subbands in the quantum wells verifies that the detected activation
processes in DLTS correspond to the hole emissions from the hole groun
d states in the delta-doped quantum wells to the top of the wells.