Fabien Grasset
The transparency and versatile chemistry of nanocolloids can be exploited to fabricate novel thin films.
15 August 2007, SPIE Newsroom. DOI: 10.1117/2.1200708.0805
Thin films are material layers ranging from fractions of a nanometer to several micrometers in thickness. They can be deposited onto metal, ceramic, glass, or semiconductor bases. Among the numerous coating techniques available, chemical or physical vapor deposition and sol-gel methods are the most commonly used in industry. Thin films are mainly used for optical coating and electronic device applications. However, the preparation of low cost functional thin films with high transparency and modulated optical properties remains a challenge for laser, photocatalytic, or display panel applications.
For example, for photocatalysis—which is increasingly used in chemical waste degradation—photostable light-harvesting nanoarchitectures are required: these are nanostructures that can be used to absorb light to facilitate chemical reactions, but are nevertheless robust to the radiation. Were they available, and provided that appropriate semiconductor catalysts were selected, charge carriers could be generated by UV or visible radiation to initiate reduction and oxidation reactions with adsorbed reactants, leading to the destruction of pollutants. However, most photocatalysts consist of metal oxides that are only functional in the UV region. The result is a lack of suitable materials with the appropriate band gap for visible absorption and the required stability for practical applications.
A second example is provided by Y2O3:Eu3+, the most widely used red phosphor for field emission display applications. Much attention has been paid to the synthesis and luminescent properties of Eu3+-doped rare-earth orthoborates (REBO3) thin films. This is due to their desirable properties as ideal vacuum UV phosphors, key materials for the development of plasma display panels. For such phosphors, both luminescence efficiency and color purity are required. Unfortunately, as a red phosphor, the intensity of the red emission of REBO3:Eu3+ is often lower than that of the orange, leading to poor chromaticity.
One of the largest application areas of sol-gel chemistry is thin-film preparation. Using this approach, we started to synthesize ZnO colloidal solutions for the preparation of functional thin films. Zinc oxide is a non-toxic semiconductor with a wide bandgap (3.37eV) and a large exciton binding energy. In bulk or nanosized form, it can be used in a wide range of applications such as UV light emitters, spin functional devices, gas sensors, transparent electronics or surface acoustic wave devices. Using high concentrations of the different polymeric nanocolloids shown in Figure 1(a), we were able to prepare various functional nanomaterials: these include the gels shown in Figure 1(c); the nanosized powders shown in Figure 1(f); the functional thin films (oxynitrides or oxides) produced as plates shown in Figure 1(b) and 1(e); and the fibers shown in Figure 1(d). Recently, red-luminescent Eu,Ti-functionalized ZnO or versatile ZnTiON colored thin films were also developed.
Eu,Ti-functionalized ZnO thin films
As part of these studies, we proposed a chemical alternative to rare-earth (RE) oxides using a very simple and efficient route to prepare highly red-luminescent RE-doped thin films: see Figure 1(b) and (e).1 Using a simple doping process, trivalent europium can easily be introduced in the solution and a Ti-functionalized ZnO can then be used as a nanohost. As shown in Figure 1(b), the red fluorescence of this nanomaterial at room temperature is easily observed under illumination from a compact 4W-UV lamp operating at 254nm. We showed that it was possible to activate RE fluorescence in a highly transparent Ti-functionalized ZnO thin film with simple annealing at 400°C for 15 minutes. The five characteristic emission peaks assigned to the 5D0→7FJ transition of Eu3+ (where J = 0, 1, 2, 3, and 4) are observed, with the strongest emission (J =2) at 613nm (Figure 2, insert).
Nombre y Apellido: Juan J. Núñez C.
Asignatura: CRF
Sección: 01
Fuente: http://spie.org/x15807.xml?ArticleID=x15807
Leer: [Jn6:63]
The transparency and versatile chemistry of nanocolloids can be exploited to fabricate novel thin films.
15 August 2007, SPIE Newsroom. DOI: 10.1117/2.1200708.0805
Thin films are material layers ranging from fractions of a nanometer to several micrometers in thickness. They can be deposited onto metal, ceramic, glass, or semiconductor bases. Among the numerous coating techniques available, chemical or physical vapor deposition and sol-gel methods are the most commonly used in industry. Thin films are mainly used for optical coating and electronic device applications. However, the preparation of low cost functional thin films with high transparency and modulated optical properties remains a challenge for laser, photocatalytic, or display panel applications.
For example, for photocatalysis—which is increasingly used in chemical waste degradation—photostable light-harvesting nanoarchitectures are required: these are nanostructures that can be used to absorb light to facilitate chemical reactions, but are nevertheless robust to the radiation. Were they available, and provided that appropriate semiconductor catalysts were selected, charge carriers could be generated by UV or visible radiation to initiate reduction and oxidation reactions with adsorbed reactants, leading to the destruction of pollutants. However, most photocatalysts consist of metal oxides that are only functional in the UV region. The result is a lack of suitable materials with the appropriate band gap for visible absorption and the required stability for practical applications.
A second example is provided by Y2O3:Eu3+, the most widely used red phosphor for field emission display applications. Much attention has been paid to the synthesis and luminescent properties of Eu3+-doped rare-earth orthoborates (REBO3) thin films. This is due to their desirable properties as ideal vacuum UV phosphors, key materials for the development of plasma display panels. For such phosphors, both luminescence efficiency and color purity are required. Unfortunately, as a red phosphor, the intensity of the red emission of REBO3:Eu3+ is often lower than that of the orange, leading to poor chromaticity.
One of the largest application areas of sol-gel chemistry is thin-film preparation. Using this approach, we started to synthesize ZnO colloidal solutions for the preparation of functional thin films. Zinc oxide is a non-toxic semiconductor with a wide bandgap (3.37eV) and a large exciton binding energy. In bulk or nanosized form, it can be used in a wide range of applications such as UV light emitters, spin functional devices, gas sensors, transparent electronics or surface acoustic wave devices. Using high concentrations of the different polymeric nanocolloids shown in Figure 1(a), we were able to prepare various functional nanomaterials: these include the gels shown in Figure 1(c); the nanosized powders shown in Figure 1(f); the functional thin films (oxynitrides or oxides) produced as plates shown in Figure 1(b) and 1(e); and the fibers shown in Figure 1(d). Recently, red-luminescent Eu,Ti-functionalized ZnO or versatile ZnTiON colored thin films were also developed.
Eu,Ti-functionalized ZnO thin films
As part of these studies, we proposed a chemical alternative to rare-earth (RE) oxides using a very simple and efficient route to prepare highly red-luminescent RE-doped thin films: see Figure 1(b) and (e).1 Using a simple doping process, trivalent europium can easily be introduced in the solution and a Ti-functionalized ZnO can then be used as a nanohost. As shown in Figure 1(b), the red fluorescence of this nanomaterial at room temperature is easily observed under illumination from a compact 4W-UV lamp operating at 254nm. We showed that it was possible to activate RE fluorescence in a highly transparent Ti-functionalized ZnO thin film with simple annealing at 400°C for 15 minutes. The five characteristic emission peaks assigned to the 5D0→7FJ transition of Eu3+ (where J = 0, 1, 2, 3, and 4) are observed, with the strongest emission (J =2) at 613nm (Figure 2, insert).
Nombre y Apellido: Juan J. Núñez C.
Asignatura: CRF
Sección: 01
Fuente: http://spie.org/x15807.xml?ArticleID=x15807
Leer: [Jn6:63]
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