We investigate the quenching of the near infrared light emission in Er 3+ complexes induced by the resonant dipolar interaction between the rare-earth ion and high frequency vibrations of the organic ligand. The nonradiative decay rate of the lanthanide ion is discussed in terms of a continuous medium approximation, which depends only on a few, easily accessible spectroscopic and structural data. The model accounts well for the available experimental results in Er 3+ complexes, and predicts an ϳ100% light emission quantum yield in fully halogenated systems. © 2006 American Institute of Physics. ͓DOI: 10.1063/1.2177431͔The research on low-cost materials emitting in the near infrared ͑NIR͒ is receiving a great deal of renewed interest for their potential in local and premise optical communication networks, and imaging and sensing applications. Among these materials, organolanthanides are very promising candidates as they combine the well-established NIR emission properties of Ln 3+ ions with the unique optical 1,2 and electrical response 3 of organic semiconductors, coupled with their easy processability.Excitation processes in lanthanide complexes differ considerably from those in inert glasses doped with transition metals. Due to the large absorption cross section of the allowed − * optical transitions, the organic ligand acts as an efficient light harvester in the ultraviolet-visible spectral window. From the organic photonic antenna the electronic excitations are quickly transferred to the rare-earth ion. The twostep excitation process permits the achievement of a large excited-state population using light fluences four to five orders of magnitude lower than those required for bare ions. Ligands also prevent deleterious formation of metal clusters, allowing the deposition of thin films with Ln 3+ densities as large as 10 21 ions/ cm 3 . All these properties make organolanthanides very attracting for the development of low-cost light sources and infrared amplifiers to integrate in planar photonic circuits for optical communications, where light signals can be generated, amplified, and processed. [1][2][3][4][5] The major drawback of these materials is related to the presence of efficient nonradiative deactivation channels, which shorten the erbium population lifetime from milliseconds to microseconds. 1,2 NIR emission quenching mainly results from the coupling of the excited state of the Ln 3+ ion with high frequency vibrations of CH and OH groups. 6 Substitution of hydrogen with heavier halogen atoms lowers the vibration frequencies and, hence, represents a possible strategy to reduce the induced emission quenching. Investigations on halogenated systems show an unambiguous improvement of the NIR light emission. 7,8 The best performances have been obtained in perfluorinated ͑PF͒ systems, which show nonradiative decay times in the submillisecond timescale. 9 NIR emission quantum yield has been drastically enhanced, but remains, however, rather low, around a few percent. Whether these results can be further impro...