Films and crystalline powder of BiI3 intercalated with ammonia

https://doi.org/10.1016/j.jeurceramsoc.2009.05.046Get rights and content

Abstract

Intercalation, i.e. the insertion of guest species in a crystalline layered structure, is an efficient route for generating new materials with novel properties. Thin films and crystalline powder of BiI3 layered semiconductor were intercalated by exposure to ammonia vapors at room temperature. The intercalated compound was studied by thermo-gravimetric analysis, differential scanning calorimetry, X-ray diffraction, UV–vis optical absorption, FTIR spectroscopy and Raman scattering. After exposure of BiI3 to ammonia the formation of a new phase, BiI3(NH3)3.83, was evidenced by thermal analysis. The intercalation process leads to a blue shift of the BiI3 optical absorption edge by 0.5 eV. The appearance of new Raman lines at 135 and 353 cm−1 in the Raman spectrum of intercalated BiI3 is considered as an evidence of the chemical interaction between the ammonia molecules and BiI3 lattice.

Introduction

During the last years, the intercalation of organic/inorganic molecules in various layered materials such as graphite, clay minerals, metal dichalcogenides, layered double hydroxides, etc. has drawn the attention of the researchers at both fundamental and practical viewpoints. The intercalation process can modify the optical and electronic properties of the two components, the host layered material and the guest molecules; moreover, the properties of the intercalated material can be tuned by the proper choice of host–guest system. These features make possible to discuss the relationships between their structure, properties and applications. In this framework, intercalation compounds have been investigated for wider applications in areas such as: photoelectrochemistry, photodetection, photocatalysis, energy storage, nonlinear optics [1].

Due to their sandwiched layer structure, in which a plane of metal ions is surrounded by two planes of halogens ions, the crystalline layered semiconductors, as PbI2, BiI3 and CdI2 are particularly interesting for intercalation with different molecules. The bonds within halogen–metal–halogen layer are strong while those between adjacent layers are weak, related to van der Waals type forces. As a result the insertion of guest molecules into the interlayer spaces is easy to achieve, leading to a change in many physical properties (optical, electrical, morphological, etc.) of the semiconductor layered crystal. In most cases, the works regarding the intercalation of layered metal iodides (PbI2, BiI3 and CdI2) with different guest species were focused on PbI2 as matrix [2], [3], [4], [5].

BiI3, a layered semiconductor with the band gap of ∼2 eV, was found interesting especially as a material for nonlinear optics. The crystal structure of bismuth tri-iodide is rhombohedral with the c-axis perpendicular to the basal plane. Each bismuth ion is octahedrally coordinated with six iodine ions, and each structural layer consists in three I–Bi–I sheets. From a planar perspective along the c-axis, only two-thirds of the possible metal sites are occupied. Thus each anion is bound at two cations. According to the band structure calculations [6], the top of the valence band in bismuth tri-iodide is formed by an admixture of the 6s2 electrons in Bi3+ with 5p6 electrons of I. The lowest energy of the conduction band originates from the 6p state of Bi3+. Thus the optical properties in BiI3 bulk crystal are described by the cationic exciton model based on the intra-cation transitions from 6s to 6p states in Bi3+ ion [7]. It has to be mentioned that in the case of BiI3 intercalated with hydrazine a shift of the cationic absorption band to higher energies was observed [8]. The process of intercalation may be accompanied by charge transfer, from the intercalate species to the host lattice. The most papers taken into account the formation of the coordination complexes as result of the chemical interaction between BiI3 and different organic molecules (tetramethylthiourea, pyridine, thiourea or triazole) [9], [10], [11], [12].

Therefore, the aim of this paper is to supply further information about the intercalation of BiI3, using ammonia, an inorganic nitrogen-containing molecule, as guest molecules. For this purpose, different techniques as thermo-gravimetric analysis, differential scanning calorimetry, X-ray diffraction, UV–vis optical absorption, FTIR spectroscopy and Raman scattering were used. Another goal of this work was to find an answer to a question which frequently arises in the context of any intercalation process, i.e.: what is the adsorption type of the guest molecules into the host matrix, a physical or a chemical one?

Section snippets

Experimental

Two kinds of samples were used in this work: micrometric crystalline powder and films of BiI3. The crystalline powder was obtained by mechanical crumbling of a BiI3 single crystal grown from melt by Bridgman method. The films of BiI3, deposited on quartz substrates, were prepared by high vacuum thermal evaporation. Intercalation was achieved by exposing the samples (films and crystalline powder) to ammonia vapors at room temperature. It is interesting to notice a visual modification: as a

Results and discussion

The thermal analysis data for the investigated powders are presented in Fig. 1 (DTA–TG – differential thermal analysis and thermal gravimetry analysis) and Fig. 2 (DSC – differential scanning calorimetry).

Pristine BiI3 presents 0.52% weight loss up to 300 °C attributable especially to the adsorbed water. Above this temperature the slope of the curve changes indicating an accentuated weight loss (−21.8%) up to 390 °C. When BiI3 is exposed to ammonia the thermal behavior changed. The weight loss

Conclusion

In this paper we have studied the intercalation of BiI3 with ammonia by X-ray diffraction, thermal analysis, UV–vis optical absorption, FTIR spectroscopy and Raman scattering. After exposing BiI3 to gaseous ammonia, the formation of a new phase, BiI3(NH3)3.83, was evidenced. This phase is stable up to ∼100 °C. In the 100–280 °C temperature range, the ammonia is released gradually as proved by thermo-gravimetric studies. The explanation resides in the different bonding type of the guest molecules

Acknowledgment

This project is funded by the Romanian Ministry of Education and Research, CEEX Program, Project no. 2-CEx06-11-19/25.07.2006.

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