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Updated: May 5, 2026

Novel Techniques for Observing Structural Dynamics of Photoresponsive Liquid Crystals
Published on: May 29, 2018
Vibrational dynamics, electronic structure, and influence of pressure on the phase stability of Sr3WO6 complex
Gilberto D Saraiva1, Luiz F Lobato2, Antonio J R de Castro3
1Faculdade de Educação Ciências e Letras do Sertão Central, Universidade Estadual do Ceará, Quixadá, CE 63902-098, Brazil; Centro de Ciências Sociais, Saúde e Tecnologia, Universidade Federal do Maranhão - UFMA, CEP 65900-410 Imperatriz, Maranhão, Brazil.
Abstract:
Polycrystalline β-Sr3WO6 was synthesized via a conventional solid-state reaction. Room-temperature X-ray diffraction confirms that the compound crystallizes in a triclinic structure, with space group P1 (C11). Void analysis reveals a relatively open framework with a 35.03% void fraction, while Hirshfeld surface analysis reveals that interatomic interactions are dominated by Sr···O/O···Sr contacts (49.8%), followed by W···O/O···W contributions (31.9%). First-principles calculations based on Density Functional Theory (DFT) yield Raman and infrared spectra in excellent agreement with experiment. Electronic structure analysis indicates a direct bandgap of 2.85 eV at the Γ point, classifying Sr3WO6 as a semiconductor. The high-pressure lattice dynamics were additionally examined by in-situ Raman spectroscopy from 0.2 to 11.0 GPa. Most Raman modes exhibit positive pressure coefficients, indicating progressive lattice stiffening. In the 80-340 cm-1 range, mode hardening is predominantly linear, consistent with WO6 octahedral bending, while a subset of modes (A, B, C, J, N) display negative pressure coefficients below 0.9 GPa. Marked discontinuities and intensity enhancements occur near 1.6 GPa, accompanied by the emergence of a new mode (A1) at ∼2.0 GPa. Additional spectral restructuring appears at 6.3-7.0 GPa, including new Raman features (B1, A0) and modifications in the 120-180 cm-1 region. At higher wavenumbers (340-1000 cm-1), strong blue shifts associated with W-O stretching is observed, together with the appearance of O1, Q1, T1, and U1 modes between 3.6 and 8.9 GPa. High wavenumbers modes (Y, W) evolve non-monotonically, exhibiting convolution near 2.0 GPa, resolution above 5.7 GPa, and the formation of DD1 at ∼7.0 GPa. The emergence, disappearance, and intensity evolution of Raman bands provide compelling evidence for two pressure-induced phase transformations, while confirming the structural robustness of the WO6 framework and revealing subtle symmetry modifications under elevated pressure. Finally, the structural analysis based on void distribution and Hirshfeld surfaces provides key insights into the pressure-dependent Raman behavior discussed.
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