Measurement of temperature is one of the most common applications of fiber optic sensing. Since light is used as the information carrierÐin contrast to electronic devices such as thermistors and thermocouplesÐoptical temperature sensors (so-called optodes) have applications even in explosive and electromagnetic environments. [1,2] Several approaches to sensing a wide range of temperatures have been reported [3±5] and some are commercially available.[6]A frequently employed methodology consists of monitoring the temperature-dependent lifetime of luminescent materials such as rare earth phosphors, [7] doped YAG crystals, [8] or ruby crystals. [9] However such materials cannot be used to form thin and fast responding temperature-sensitive coatings. Ruthenium(II)-diimine complexes are attractive and frequently used for optical lifetime sensing of chemical parameters such as pO 2 , pH, and pCO 2 .[10±12] Outstanding features include good luminescence quantum yield, strong absorption of visible light (which makes them excitable by light-emitting diodes (LEDs)), photostability, and luminescence lifetimes in the microsecond range. The luminescence decay time of ruthenium(II) complexes is known not only to be affected by temperature, but also by chemical quenchers. By selection of an appropriate polymer matrix we have obtained materials whose luminescence is almost exclusively governed by temperature, while interferences from external quenchers such as oxygen are excluded.In particular, we have identified Ru(phen) (rutheniumtris-1,10-phenanthroline) as the most viable temperature probe that can be incorporated into matrices of sol-gels or poly(acrylonitrile)s (PANs) and then can be spread as a thin film onto solid substrates. Its luminescence decay time is particularly strongly affected in the temperature range of physiological and related applications. Furthermore, Ru(phen) is commercially available, photostable, and can be easily incorporated into solid matrices by appropriate selection of the counterion.The use of Ru(phen) in optical temperature sensing requires a sophisticated encapsulation technique because its luminescence is known to be quenched by oxygen. In addition, interferences by other oxidative or reductive quenchers, including NO x and SO 2 , can be expected. Following an investigation of a number of materials with very low permeability for molecular oxygen, we identified densified solgel glass and PAN as being most suitable candidates for embedding Ru(phen) in a non-quenchable form. The composition of the materials investigated and respective figures of merit are summarized in Table 1.The two-state model of Demas et al. [13,14] is applicable to describe the temperature dependence of the luminescence lifetime. It attributes the temperature dependence of the excited state exclusively to a thermally activated non-radiative decay. The decrease in luminescence intensity and lifetime with rising temperature can be described by an Arrhenius-type model (Eq. 1) where k 0 is the temperatureindependent decay rate fo...