“…The silica hybrid materials containing the two dyes were prepared using the modified templateds ynthesis depicted in Figure 1, where JM,h aving an average number of 45 -CH 2 CH 2 O-units, is embedded along the folded P123 chains, whereas the iridium(III) complex is expected to be localised inside the core hydrophobic regionofthe micelles,b eing totally insoluble in water.D onor-acceptor (D-A) 1:1r atios were used in the construction of two HGCs whichw erep repared using D:A:P123 molarp ercentages of 1:1:98 and 5:5:90, yielding the samples namedh ereafter 1%IrD-1%JM and 5%IrD-5%JM,r espectively.O verall dye loadings highert han 10 % were avoided for two main reasons:i )tom aintain the ordered hexagonal arrangement of the cylindrical micelles within the silica, which starts losing its long-scale order beyondt he above dye loading, [47] and in turn to ensure the reliability of the geometricalm odel used to interpret the optical properties, and ii)tom inimise the occurrence of potentialt riplet-triplet annihilation between IrD molecules, incurred by the closer proximity of dye molecules as their concentration increases, which would be detrimental for the efficiency of energy transfer between IrD and JM dyes. Al ow concentration of these molecules naturally leads to ag reater average distance between them and reduces aggregation overall, makingt he assumption of as tatistical distribution of intermolecular distances arising from ar andom spatiald ispersion of dyes, which has indeed been appliedi nt he literature to rationalise dye speciesb ehaviour in polymericm atrices; [55] additionally,t he complexity of the excited state deactivation dynamics is expected to generally decrease with ar eduction in aggregation processes,a s fewer new radiative de-excitation pathways should arise.…”