The optical properties of nano‐structural α‐<scp>Fe<sub>2</sub>O<sub>3</sub></scp> dependence on the shape

Three different crystal morphologies of α-Fe<sub>2</sub>O<sub>3</sub>, including uniform hexagonal, square, and rhombic shapes, were prepared according to the aqueous-thermal reaction. The hexagonal-shaped α-Fe<sub>2</sub>O<sub>3</sub> was enclosed by the 104 plane, while the square and rhombic structures were enclosed by the 110 plane. Two absorption peaks at 455 and 532 cm<sup>-1</sup> were found for the perpendicular (⊥) modes, and one absorption peak at 650 cm<sup>-1</sup> appeared for the parallel (||) mode for hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> during analysis by Fourier-transform infrared spectroscopy. However, the peaks of square- and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> for perpendicular (⊥) mode blueshifted, and the former two peaks merged together forming a broad band at approximately 480 cm<sup>-1</sup>. For Raman spectra determination, the peaks arose from the Brillouin zone center, and two additional peaks were observed at 660 and 1320 cm<sup>-1</sup>, belonging to 1 longitudinal optical (1LO) and 2 longitudinal optical (2LO) modes. All three materials exhibited higher intensities when excited at a wavelength of 633 cm<sup>-1</sup>. Furthermore, in the polarization state, the centers of all peak positions slightly shifted for hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub>, but all peak positions for square-shaped and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> exhibited a significant blueshift. The structure of hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> was relatively tolerant regarding the polarization properties of vibration modes; however, the symmetry of crystal square-shaped and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> changed, subsequently revealing different optical properties. RESEARCH HIGHLIGHTS: The hexagon-shaped, square-shaped, and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> enclosed by different planes were synthesized. The Fourier Transform Infrared spectrometer peaks of α-Fe<sub>2</sub>O<sub>3</sub> depended on their hexagon, square and rhombic shapes. Compared with hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub>, the Raman peaks for square and rhombi ones significantly shifted. The hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> is relatively tolerant regarding the polarization properties.

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Publication Details

Journal
Microscopy Research and Technique
Published
2024-09-02
DOI
https://doi.org/10.1002/jemt.24686
Citations
6
Primary Topic
Iron oxide chemistry and applications
Type
article
Field-Weighted Citation Impact
0.61

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The optical properties of nano‐structural α‐Fe2O3 dependence on the shape

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6 citations
Microscopy Research and Technique
Iron oxide chemistry and applications
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article

The optical properties of nano‐structural α‐Fe2O3 dependence on the shape

Yinping Zhang, Y Liu, Qinnan He, Xiaomei Jiao, Zhan Wang
article en
6 citations

Abstract

Three different crystal morphologies of α-Fe<sub>2</sub>O<sub>3</sub>, including uniform hexagonal, square, and rhombic shapes, were prepared according to the aqueous-thermal reaction. The hexagonal-shaped α-Fe<sub>2</sub>O<sub>3</sub> was enclosed by the 104 plane, while the square and rhombic structures were enclosed by the 110 plane. Two absorption peaks at 455 and 532 cm<sup>-1</sup> were found for the perpendicular (⊥) modes, and one absorption peak at 650 cm<sup>-1</sup> appeared for the parallel (||) mode for hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> during analysis by Fourier-transform infrared spectroscopy. However, the peaks of square- and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> for perpendicular (⊥) mode blueshifted, and the former two peaks merged together forming a broad band at approximately 480 cm<sup>-1</sup>. For Raman spectra determination, the peaks arose from the Brillouin zone center, and two additional peaks were observed at 660 and 1320 cm<sup>-1</sup>, belonging to 1 longitudinal optical (1LO) and 2 longitudinal optical (2LO) modes. All three materials exhibited higher intensities when excited at a wavelength of 633 cm<sup>-1</sup>. Furthermore, in the polarization state, the centers of all peak positions slightly shifted for hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub>, but all peak positions for square-shaped and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> exhibited a significant blueshift. The structure of hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> was relatively tolerant regarding the polarization properties of vibration modes; however, the symmetry of crystal square-shaped and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> changed, subsequently revealing different optical properties. RESEARCH HIGHLIGHTS: The hexagon-shaped, square-shaped, and rhombic-shaped α-Fe<sub>2</sub>O<sub>3</sub> enclosed by different planes were synthesized. The Fourier Transform Infrared spectrometer peaks of α-Fe<sub>2</sub>O<sub>3</sub> depended on their hexagon, square and rhombic shapes. Compared with hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub>, the Raman peaks for square and rhombi ones significantly shifted. The hexagon-shaped α-Fe<sub>2</sub>O<sub>3</sub> is relatively tolerant regarding the polarization properties.

Microscopy Research and TechniqueVol. 88(1)
Nanjing Normal University (CN), University College London (GB)
National Natural Science Foundation of China, National Key Research and Development Program of China
Openalex Percentile: Top 39%
Iron oxide chemistry and applications
0.61
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