Recent years have seen a growing interest in optical sensors based on oxygen-induced or temperature-induced changes in the luminescence intensity of organic dyes [1][2][3][4]. Probes available for optical temperature sensor are fluorescent, thermal-quenchable and non oxygen-quenchable organic and inorganic dyes, such as coumarin, perylene, pyronin and rare earth metal compounds [5][6][7]. One of the candidate probes available for the optical temperature sensor is fullerene. Fullerenes possess useful electronic and photochemical properties [8][9][10]. As the fluorescence lifetime of fullerene C 60 is estimated to be 1.1 ns, the fluorescence of C 60 is not quenched by oxygen [11]. Thus, the fluorescence intensity of C 60 is changed by temperature changes. Thus, fullerene is attractive compound for optical temperature sensing based on the fluorescence intensity change thermally.In this letter we describe a new optical temperature sensing material, fullerene C 60 immobilized in polymethylmethacrylate (PMMA) film, and its temperature sensing properties.
ExperimentalC 60 was obtained from Tokyo Kasei Inc. and was purified by recrystalization with toluene-benzene. PMMA (average M.W. 280 000, GPC grade) was purchased from Aldrich. The C 60 immobilized in PMMA film was formed by casting a mixture of 20 wt. % PMMA and C 60 in toluene onto 1.4 × 5.0 cm non-luminescent glass slides. The C 60 concentration in the film was approximately 1.0 × 10 -3 mol dm -3 . The films were dried at room temperature and stored in the dark prior to use. The thickness of the films was determined by the use of a micron-sensitive calliper. The thickness of the prepared film was c.a. 50 µm. The fluorescence spectrum of the C 60 film was measured using a Shimadzu RF-5300PC spectrofluorophotometer with a 150 W Xenon lamp as the excitation light source. The excitation and emission bandpasses were 10 and 5.0 nm, respectively. The sample film was mounted at a 45º angle to minimize light scattering from the sample and substrate. The temperature (260-373 K) was controlled using an Oxford Instrument Optistat-DN cryostat system. All the experiments were carried out under ambient condition.Theory of optical temperature sensing based on the fluorescence intensity change of C 60 film is as follows. The quantum yield (Φ) in the absence of quencher is given bywhere I a is the absorption intensity. k L and k D are the rate constants for the fluorescence and the radiationless deactivation, respectively. The deactivation term, k D is decomposed into a temperature-independent part k 0 and a temperature-dependent part k 1 that is related to thermally activated intersystem crossing. The k 1 can be assumed to have an Arrhenius form as follows:where A, E and R are a constant, the Arrhenius activation energy and the universal gas constant, respectively. The eq.(1) is re-written by the eq. (2) of the radiationless deactivation rate: Keyword. Optical temperature sensing -fullerene -fluorescence quenching -Arrhenius activation energy -polymer film.