4.2 Article

Synthesis, crystal structure, vibrational properties, optical properties and Hirshfeld surface analysis of a new Bi (III) halide complex: (C2H8N)3BiBr6 for optoelectronic devices

Journal

INDIAN JOURNAL OF PHYSICS
Volume 97, Issue 2, Pages 457-472

Publisher

INDIAN ASSOC CULTIVATION SCIENCE
DOI: 10.1007/s12648-022-02407-y

Keywords

Crystal structure; Hydrogen bonds; Vibrational studies; Hirshfeld surfaces analysis; Optical studies

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A new organic-inorganic material, dimethylaminium hexabromobismuthate (C2H8N)(3)BiBr6, was synthesized using the slow evaporation technique at room temperature. The compound was characterized by various spectroscopic methods, such as X-ray diffraction and Raman spectroscopy. The results show that this compound has a high-quality crystal lattice structure with discrete [BiBr6](3-) anions surrounded by dimethylaminium cations. It also exhibits a direct and wide optical bandgap, making it a potential candidate for optoelectronic devices.
A new organic-inorganic material, dimethylaminium hexabromobismuthate (C2H8N)(3)BiBr6 was elaborated by the slow evaporation technique at room temperature. This compound is synthesized and characterized by X-ray diffraction, Raman spectroscopy scattering, Hirshfeld surface analysis, C-13 NMR spectroscopy, photoluminescence and by UV-Vis spectroscopy. The crystal lattice is formed by discrete [BiBr6](3-) anions surrounded by dimethylaminium cations. Besides, the title compound crystallizes in the space group R (3) over bar of trigonal system. The unit cell parameters are a = 29.3387(9) angstrom b = 29.3387(9) angstrom and c = 8.4642(3) angstrom . The Raman and infrared spectra recorded at room temperature were interpreted by analogy with homologous materials. The cohesion of the structure is ensured by a huge network of N-H center dot center dot center dot Br hydrogen bonds and van der Waals interaction (C-H center dot center dot center dot Cl). The UV-Vis measurements, performed from 200 to 2400 nm, show a direct and wide optical bandgap evaluated at (2.840 +/- 0.005), (2.482 +/- 0.004) and (2.805 +/- 0.006) eV by different methods. The Urbach energy presents a low value estimated at (182 +/- 3) meV confirming the high quality of our compound. In addition, the evolution of the extinction coefficient (k(e)) and the refractive index n with the wavelength lambda were determined. Furthermore, we have demonstrated that n obeys to Cauchy relation. Other optical parameters such as the skin depth and the optical conductivity were calculated, and all obtained results were discussed. We have demonstrated, in addition, that the energy losses are mainly in the bulk rather than the surface of the studied material. Based on the Wemple-Di-Domenico model, the dispersion parameters E-0 and E-d relative to the (C2H8N)(3)BiBr6 sample were calculated. These encouraging results such as the obtained high and direct optical bandgap value prompt us to propose this compound as a basic material for optoelectronic devices.

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