In order to study the behavior of photoinjected electrons
in dye-sensitized
solar cells (DSC), steady-state microwave reflectance measurements
(33 GHz, Ka band) have been carried out on a working cell filled with
electrolyte. The experimental arrangement allowed simultaneous measurement
of the light-induced changes in microwave reflectance and open circuit
voltage as a function of illumination intensity. In addition, frequency-resolved
intensity-modulated microwave reflectance measurements were used to
characterize the relaxation of the electron concentration at open
circuit by interfacial transfer to tri-iodide ions in the electrolyte.
The dependence of the free and trapped electron concentrations on
open circuit voltage were derived, respectively, from conductivity
data (obtained by impedance spectroscopy) and from light-induced near
IR transmittance changes. These electron concentrations were used
in the fitting of the microwave reflectivity response, with electron
mobility as the main variable. Changes in the complex permittivity
of the mesoporous films were calculated using Drude–Zener theory
for free electrons and a simple harmonic oscillator model for trapped
electrons. Comparison of the calculated microwave reflectance changes
with the experimental data showed that the experimental response arises
primarily from the perturbation of the real component of the complex
permittivity by the high concentration of trapped electrons present
in the DSC under illumination. The results suggest that caution is
needed when interpreting the results of microwave reflectance measurements
on materials with high concentrations of electron (or hole) traps,
since an a priori assumption that the microwave response
is solely determined by changes in conductivity (i.e., by free electrons)
may be incorrect. The intensity-modulated microwave reflectance measurements
showed that relaxation of the free and trapped electron concentrations
occurs on a similar time scale, confirming that the free and trapped
electron populations remain in quasi-equilibrium during the decay
of the electron concentration.