The principle of measurements using the "microwave resonant cavity technique" applied to rare-earthdoped insulating materials is reviewed and the physical nature of the expected signals is discussed. Experimental results concerning both single crystal and powdered samples of Lu 2 SiO 5 : Ce 3+ are presented and discussed as typical examples. From measurements at various temperatures between 300 and 5K and under different pulsed laser beam powers, it is shown that detailed information on the rare earth photoionization process, photoconductivity dynamics and trapping effects may be gained, in addition to photoconductivity spectra.1 Introduction Photoconductivity studies of rare-earth (RE)-doped insulating materials using the microwave resonant cavity technique (MRCT) were conducted for the first time in our laboratory [1]. The primary goal of these investigations was indeed the determination of the RE photoionization thresholds, with the aim of locating the 4f n levels of RE ions with respect to the host conduction band (CB). As a matter of fact, the energy level diagrams of RE ions usually reported do not take this positioning into account and, consequently, lack the required information to help in understanding the complex processes associated with the absorption of high energy photons by RE-doped materials used as scintillators, ultraviolet lasing media or phosphors for fluorescent tubes and plasma display panels. MRCT was shown to be also helpful in gaining significant information on the photoionization process, photoconductivity dynamics, nature of the photoexcited electrons and trapping effects [2][3][4]. MRCT consists in detecting the dielectric response to a pulsed laser irradiation of a sample placed inside a microwave resonator. Let Q U and f 0 be respectively the cavity quality factor and resonance frequency when both the laser and microwave sources are not operating. Coupling the microwave guide to the cavity lowers its quality factor from Q U (U for unloaded cavity) to Q L (L for loaded cavity) defined by: