BEHAVIOR OF SI PHOTOELECTRODES UNDER HIGH-LEVEL INJECTION CONDITIONS .3. TRANSIENT AND STEADY-STATE MEASUREMENTS OF THE QUASI-FERMI LEVELS AT SI CH3OH CONTACTS/
Cn. Kenyon et al., BEHAVIOR OF SI PHOTOELECTRODES UNDER HIGH-LEVEL INJECTION CONDITIONS .3. TRANSIENT AND STEADY-STATE MEASUREMENTS OF THE QUASI-FERMI LEVELS AT SI CH3OH CONTACTS/, JOURNAL OF PHYSICAL CHEMISTRY B, 101(15), 1997, pp. 2850-2860
Real-time measurements of the photovoltage rise and decay at the back
of lightly doped, thin, long lifetime Si photoelectrodes were recorded
subsequent to a variety of spatial and temporal carrier generation im
pulses. The functional form of the rising portion of the photovoltage
signal is sensitive to charge transport processes, and this signal was
used to validate experimentally the hypothesis that charge transport
in these samples under high level injection is primarily driven by dif
fusion, as opposed to drift. The decay of the photovoltage signal back
to its equilibrium value yielded information concerning the surface r
ecombination velocity, S-f, of the various Si/CH3OH redox couple conta
cts. These data validated the relatively high surface quality of the S
i/liquid interface in contact with a variety of redox species. Further
more, the low surface recombination velocities are in agreement with p
rior theoretical and experimental estimates of interfacial charge-tran
sfer rate constants for semiconductors in contact with nonadsorbing, o
uter-sphere, redox species. The front surface recombination velocity d
ata also provided a needed boundary condition for modeling the carrier
concentration dynamics and allowed quantification of the difference b
etween the quasi-Fermi levels at the back and front surfaces of the sa
mples at all times of experimental interest. Digital simulation and an
alytical modeling were performed to compute the gradients in the quasi
-Fermi levels for samples operated under steady-state, open-circuit, h
igh level injection conditions. In no case was the difference between
the quasi-Fermi level value at the back of the sample and its value at
the solid/liquid contact greater than 10 meV. These data, combined wi
th those described in parts 1 and 2, comprise a relatively complete pi
cture of the transport and recombination processes that occur at these
types of semiconductor/liquid contacts.