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Energy Transfer in Organic and Hybrid Blends

Recently, we also focussed on hybrid organic/inorganic materials, which are a fast growing research area, since a lot of basic and practical interest has been raised by their optical and mechanical properties.

 

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Fig. 2. (a) ZnO microparticles imaged by SEM. (b) Surface topography of a hybrid film (A:D concentration 10%) imaged by AFM. 

 

These hybrid materials can benefit from the unique properties of both the organic and the inorganic components. Generally, light-emitting conjugated polymers constitute the organic component of optically active hybrid materials, because of their ease of processing and good opto-electronic characteristics. For the inorganic component, semiconductor and oxide micro- and nanocrystals are the most exploited materials, since they can provide a homogeneous dispersion inside the organic component and a more effective charge transfer in the composite. The interactions between the inorganic and the organic component inside a hybrid material can be mediated by radiative or nonradiative energy transfer. We carried out an extensive study of the energy transfer in hybrid inorganic-organic composite system, composed by an inorganic oxide micro-crystal as donor (ZnO) and an organic conjugated polymer as acceptor (MEH-PPV) (Fig. 2).

    To investigate the dependence of the energy transfer rate on temperature, we studied the temperature behaviour of the relative PL intensity (φ) from the acceptor molecules for composites with different A:D relative concentrations (Fig. 3). Upon decreasing temperature, the relative PL intensity (φ) decreases, the specific decrement depending on the donor/acceptor relative concentration. The T-dependence of the energy transfer has to be mainly related to changes in the donor and acceptor quantum efficiency and decay channels. The quantitative understanding of non-radiative processes in hybrid inorganic-organic materials is fundamental for the development of optimized hybrid organic/inorganic light-emitting devices and lasers whose spectral emission rely on energy transfer in active nanocomposite media.

 

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 Fig. 3. (a) PL emission spectra (A:D 10% wt) collected at different temperatures. (b) T-dependence of φ for different A:D concentrations. Points represent experimental data, the superimposed curves represent the result of our modelling.

 Publications:

[1] A. Camposeo, E. Mele, L. Persano, D. Pisignano and R. Cingolani, Phys. Rev. B 73 165201 (2006).
 
[2] A. Camposeo, E. Mele, L. Persano, D. Pisignano and R. Cingolani, Opt. Lett.  31 1429 (2006).

[3] A.A.R. Neves, A. Camposeo, R. Cingolani and D. Pisignano, Adv. Funct. Mater., in press (2007).



 

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