In this contribution, defects induced zero-TQ phenomenon of Eu2+-doped phosphors is overviewed. The zero-TQ phenomenon of Eu2+ luminescence was reportedly observed largely in some phosphate, fluorophosphate or fluoroborate phosphors. It was proposed by the researchers that the defects originating from either polymorphic modifications of the host compound, non-equivalent substituting for the cationic sites by Eu2+, or mismatching in ionic sizes between Eu2+ and the sites it occupies could absorb the incident excitation light at RT, and upon heating (thermal stimulation) the energy captured in the defects of phosphor could be transferred to 5d levels of the Eu2+, resulting in zero-TQ and anomalous TQ of these phosphors. A close inspecting a collection of the relevant data indicates that the variations of IPL with temperature for those Eu2+-doped phosphors with a similar trap depth were often disparate.It is argued that it is still an open question whether zero-TQ (and anomalous TQ) could be an intrinsic property of Eu2+-doped phosphors.Since the magnitudes of IPL enhancement for a given phosphor (e.g., Na3Sc2(PO4)3:Eu2+ ) in a similar temperature span between RT and 150 oC reported by the different research groups or even by the same research group in main text and supplementary information of the article were different obviously. Despite the existence of defects in the phosphors being proved by thermoluminescence experiments, it does not mean that energy transfer from the defects to the 5d levels of Eu2+ could naturally take place. The energy transfer between donor and acceptor centers in a phosphor could take place only when the rigorous conditions could be satisfied for the specific mechanism, i.e., a resonance interaction, an exchange interaction between the two centers or through the conduction (or valance) band of the host.Furthermore, once the transfer of energy from the defect levels to the 5d levels of Eu2+ has occurred, apart from the increase in IPL of Eu2+, lifetime and internal quantum efficiency (IQE) of the phosphors should give corresponding signals simultaneously. 5d→4f transition of Eu2+ is a parity-allowed electric dipole transition, it is expected that a change in IPL with temperature should be accompanied with a change in lifetime correspondingly. Given the fact that the whole process including energy capturing by the defects, de-trapping of the stored energy via thermal stimulation, and energy transferring from the defects to Eu2+ and eventually light emitting by Eu2+ was a time-consuming process in comparison to a direct decay from the 5d to 4f manifolds of the Eu2+, afterglow of Eu2+ luminescence which refers to a delayed radiant recombination of electrons and holes due to trapping of electrons or holes is expected if the energy transfer from the defects to Eu2+ has occurred. Moreover, if an increase in IPL with temperature arises from transfer of energy stored in the defects to 5d levels of the Eu2+, an increase in IQE is expected as well, since the IPL is proportional to the product of absorbed photons and IQE of the phosphor under consideration. However, corresponding changes in temperature-dependent lifetime or IQE were unavailable in these publications.
Though the measurement method of temperature-dependent spectra is widely used by researchers in the filed of luminescent materials. Given the reasons elaborated in the text, temperature dependent IPL results alone seem not to be a reliable parameter for evaluating TQ property of Eu2+-doped phosphors unless special caution has been taken to guarantee the stability and consistence of the measuring conditions.To substantiate defects induced zero-TQ phenomenon to be an intrinsic property of the Eu2+-doped phosphors,merely an enhancement of IPL with increasing temperature is insufficient and unconvincing. Only when an increase in IQE and/or lifetime of the phosphor in question with temperature is in accordance with that predicted from an enhanced IPL, could the conclusion that the defects related energy transfer resulted in zero-TQ and anomalous TQ of Eu2+ luminescence hold.