Elsevier

Ceramics International

Volume 45, Issue 3, 15 February 2019, Pages 3510-3517
Ceramics International

Influence of deposition parameters on the structure and microstructure of Bi12TiO20 films obtained by pulsed laser deposition

https://doi.org/10.1016/j.ceramint.2018.11.008Get rights and content

Abstract

The structure, morphology and surface roughness of Bi12TiO20 (BTO) thin films grown on R-sapphire by pulsed laser deposition (PLD) were studied at different substrate temperatures, target-substrate distances, oxygen pressures and laser-pulse repetition rates. Although the substrate temperature seems to be the most important experimental parameter, the gas pressure and the target–substrate distance played important role on the phase formed and film thickness, with a significant effect of the laser-pulse repetition rate on the films thickness and preferred orientation of the deposited film. Single-phase γ-Bi12TiO20 was obtained on substrates at 650 °C, while several BTO metastable phases were observed in films deposited on substrates at temperatures between 500 and 600 °C. By the first time, thin films of pure and textured δ-Bi12TiO20 were successfully growth on substrates at 450 °C. When annealed, all the films deposited at lower temperatures resulted in the thermodynamically stable γ-Bi12TiO20.

Introduction

Semiconductor photocatalysts for solar energy conversion is an active area in the field of environmental research. Although the development of various materials, the design of efficient visible light-driven photocatalysts is still a great challenge [1], [2], [3], [4], [5], [6], [7]. Bismuth titanate (BTO) is a promising candidate to replace TiO2 because of its chemical stability, nontoxicity and enhanced photocatalytic reactivity. Bismuth oxide occurs in different composition and structures, such as Bi4Ti3O12 [8], [9], [10], Bi2Ti2O7 [11] Bi2Ti4O11 [12], Bi20TiO32 [13], [14], [15], [16] and Bi12TiO20 phase [3], [4], [5], [17], [18], [19], [20], [21], but there are at least three polymorphs that exhibit catalytic properties [22], [23], [24], [25] and unusual high photocatalytic activity under solar light irradiation [26], [27], [28], [29]. The Bi12TiO20 belongs to the sillenite family, where the bismuth coordinates to five oxygens of the octahedra together with the stereochemically active 6 s2 lone electron pair of Bi3+. This configuration turns this structure unique for application in photocatalysis. When synthesized as powders, two polymorphs were identified, the γ-Bi12TiO20 formed at room temperature and the δ-Bi12TiO20 that is stable only at high temperature [30], [31], [32], [33], [34]. The γ-Bi12TiO20 has the (BCC) body-centered cubic structure of γ-Bi2O3 (space group I23) while the δ-Bi12TiO20 have the (FCC) face-centered cubic structure of δ-Bi2O3 (space group Fm-3m). The γ-Bi12TiO20 showed the photocatalytic ability to degrade organic pollutants, offering a potentially efficient technology for the elimination of toxic waste chemicals [35], [36], [37], [38]. Nanostructured γ-Bi12TiO20, for example, exhibited improved photoelectrochemical activity to generate hydrogen and to degrade textile dye under UV–visible light [39]. Indeed, γ-Bi12TiO20 powders exhibited superior performance than the commercial TiO2 (P25 catalyst) under visible light irradiation [40], [41] and could degrade dyes much more efficiently than the traditional N-doped TiO2 [42].

Various methods have been used to synthesize sillenite γ-Bi12TiO20, such as chemical solution decomposition [21], [43], isopropanol-assisted hydrothermal synthesis [2], [41], [42], coprecipitation [36], [44], Pechini-based routes [45], electrochemical method [39], [46], sol-gel processing [47], the traditional solid-state reaction [48] and, recently, by means of the oxidant peroxo method (OPM) [49], [50], [51], [52].

Although several studies used ultrafine powders suspended in the reaction media, photocatalyst in the form of supported thin film provides an advantage over the drawbacks encountered in powder suspensions. In fact, there are only a few studies focused on the synthesis and applications of Bi12TiO20 thin films. [46], [53], [54], [55], [56], [57], [58]. In this context, it appears attractive to synthesize thin films of Bi12TiO20 with controlled structure and microstructure aiming applications in photocatalysis. This study presents the synthesis of Bi12TiO20 thin films growth by pulsed laser deposition (PLD) evaluating the influence of several experimental parameters, such as the control of the substrate temperature, oxygen pressure, target-substrate distance and the laser-pulse repetition frequency on the microstructural (thickness, morphology, crystallinity) and structural (orientation and phases) properties.

Section snippets

Experimental

The γ-Bi12TiO20 powders were prepared by solid-state reaction from the stoichiometric mixture of Bi2O3 (99% Prolabo-France) and TiO2 (99.8% Alfa Aesar GmbH & Co KG-Karlsruhe) powders. This stoichiometric mixture were mixed in a planetary ball mill (Retsch-PM 100) with a rotational speed of 400 rpm for one hour, pressed uniaxially at 100 MPa in pellets and fired at 750 °C for 2 h. In a second step, the fired bismuth titanate was milled again using the planetary ball mill at 400 rpm for one hour,

Results and discussion

There are several experimental parameters controlling the growth of Bi12TiO20 films deposited by PLD. Nevertheless, each parameter was analyzed separately in this study in order to determine its influence either in the crystalline structure or in the microstructure of the BTO deposited film. Among all the parameters, substrate temperature seems to be the most important variable to control the crystalline structure and preferred orientation, while oxygen pressure and target–substrate distance

Conclusions

Although the compositional complexity, thin films of Bi12TiO20 were successfully obtained by pulsed laser deposition on R-sapphire substrates. Among all the experimental parameters studied, the substrate temperature affected the crystalline structure and preferred orientation, in spite the fact that gas pressure and the target–substrate distance played important role on the phase formed and film thickness. The laser-pulse repetition rate also showed a significant effect on the films thickness

Acknowledgments

Authors acknowledge São Paulo Research Foundation/Brazil (Grant numbers 2012/07067-0, and 2013/07296-2), CNPq/Brazil and France-Brazil project (CAPES/ COFECUB n° 644/09) for financial support and the staff of CMEBA-France (ScanMAT, University of Rennes 1), which received a financial support from the European Union (CPER-FEDER 2007-2014), for the FE-SEM images.

In particular, we would like to acknowledge CEPID-Brazil (2013/07296-2) INCTMN 2008/57872-1 and CNPq 573636/2008-7. Special thanks to J.

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