We present a simple method to measure the cathodoluminescence of charging and non-charging phosphor powder layers at low primary electron beam energy. The method is based on comparing a non-charging surface of a conducting material such as copper or indium tin oxide with charging surfaces of non-conducting phosphors. The phosphors that were investigated were ZnO:Zn, which is slightly conductive and supposed not to charge upon electron bombardment, and Y 2 O 3 :Eu, which charges at sufficiently high current density. It was found that the luminous efficacies of ZnO:Zn and Y 2 O 3 :Eu at 5 keV primary beam energy were 23 and 16 lm/w respectively, larger than reported in the literature. This is partly explained by calculating the efficacy from the summation of the luminances measured in the reflected and transmitted mode. This method also minimizes the inaccuracy introduced by the effect of the coating weight. The ratio between luminances measured in reflection and transmission is described in terms of a one-dimensional light scattering theory. Previously we have reported on the various intrinsic luminescent phenomena, such as cathodoluminescence (CL), photoluminescence (PL) of nanometer sized rare earth doped yttrium oxide particles, crystallites and periodic nanostructures for photonic bandgap studies.
1-5More recently we have given an account on a CL study on double layers of zinc doped zinc oxide (ZnO:Zn) and nanometer sized (NS) europium doped yttrium oxide particles (Y 2 O 3 :Eu). 6 The objective of that study was to increase the light output of phosphor layers by making double layers of low and high voltage phosphors. In that study it was not possible to show that this approach was successful, mainly because the penetration depth at 5 kV in a thin top layer was insufficient to excite the bottom layer. Other problems were charging of the NS Y 2 O 3 :Eu top layer, which led to non-reproducible results and focusing effects of the electron beam. In this paper a new method will be introduced for determining the CL efficacy of phosphor powder layers that may charge upon electron bombardment. Furthermore, the optical behavior of the micrometer sized ZnO:Zn and the NS Y 2 O 3 :Eu particles in terms of a one-dimensional light scattering theory will be described.The challenge of measuring the CL of insulating phosphor layers at low electron beam energy is that the use of a top layer of aluminum (Al) to prevent charging of the phosphor grains cannot be used. This charging is negative in the case of the secondary emission coefficient γ being <1, or positive in the case that γ > 1. In principle the surface potential could approach that of the primary beam, and deflect the incoming beam. In practice no evidence of this happening has been observed in this work. What appears to be happening is that the thin surface layer charges up until it reaches the dielectric breakdown threshold of the material and then discharges, before resuming charging. As a result the surface potential fluctuates rapidly. This behavior can clearly b...