Luminescent nanocrystalline (NC) Ce
3+-doped yttrium aluminum garnet (Y 3 Al 5 O 12 :Ce-YAG:Ce) is prepared by a combustion synthesis technique that yields a highly porous three-dimensional network of interconnected 18 nm nanocrystals. Tetramethyl rhodamine isothiocyanate (TRITC) was conjugated to NC YAG:Ce by using glycine as a bridging molecule. Efficient energy transfer is observed from the Ce 3+ ions to the TRITC molecules upon photoexcitation of the NC YAG: Ce-TRITC conjugates.Resonant energy transfer (ET) between a donor in the excited state and a neighboring acceptor is commonly observed between dyes, 1 quantum dots and dyes, 2,3 quantum dots, 4,5 and metal ions. 6 The ET process can occur via several mechanisms, but the electric dipole-electric dipole interaction is the most effective one over relatively long distances (up to several tens of angstroms, with a r À6 distance dependence). 6 This mechanism is particularly efficient when both donor and acceptor have allowed electric dipole resonant transitions.ET between suitable probes can be used to obtain structural information or monitor dynamic processes in biological systems but its usefulness is severely limited by fast photobleaching when dyes are used for tagging the target molecules. Semiconductor quantum dots are more stable than dyes 7 but still suffer from photoinduced degradation processes. Luminescent ions in inorganic phosphors offer the prospect of a greatly superior photo-stability associated with high quantum yields. Intermittence in emission (blinking), which is a problem in certain applications of single quantum dots, is not expected for inorganic phosphor nanocrystals as they contain a large number of luminescing ions (typically between 10 and 10 000 depending on the size of the nanocrystal and the concentration of luminescing ions). In the past few years there has been a growing interest in the properties of nanocrystalline lantha- , have been prepared in nanocrystalline form. The application of lanthanide-doped nanocrystalline phosphors as biological labels would however strongly limit the photon turnover rates due to the long (ms to ms) decay time of their intraconfigurational 4f n luminescence. One of the few exceptions for visible-emitting phosphors is Y 3 Al 5 O 12 :Ce (YAG:Ce). In YAG:Ce the 5d state of Ce 3þ is situated at a low energy resulting in a fast intraconfigurational 5d ! 4f luminescence in the visible. The luminescence life time of this emission is 65 ns.
20This luminescence decay time is ideally suited for time-gated detection of biological species, since it is slower than the autofluorescence background decay common to many biological species (typically a few ns), but is still fast enough to ensure a high turnover rate. Additional attractive features are the excitation in the blue (which further decreases the autofluorescence background obtained under UV excitation) and the large Stokes shift of the luminescence. The strong electric dipole of the Ce 3þ f-d emission also makes NC YAG:Ce a promising candidate as donor f...