{"title":"The optical properties of nano-structural α-Fe<sub>2</sub>O<sub>3</sub> dependence on the shape.","authors":"Yousheng Liu, Qinnan He, Zhan Wang, Xiaomei Jiao, Yinping Zhang","doi":"10.1002/jemt.24686","DOIUrl":null,"url":null,"abstract":"<p><p>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.</p>","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2024-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/jemt.24686","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
引用次数: 0
Abstract
Three different crystal morphologies of α-Fe2O3, including uniform hexagonal, square, and rhombic shapes, were prepared according to the aqueous-thermal reaction. The hexagonal-shaped α-Fe2O3 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-1 were found for the perpendicular (⊥) modes, and one absorption peak at 650 cm-1 appeared for the parallel (||) mode for hexagon-shaped α-Fe2O3 during analysis by Fourier-transform infrared spectroscopy. However, the peaks of square- and rhombic-shaped α-Fe2O3 for perpendicular (⊥) mode blueshifted, and the former two peaks merged together forming a broad band at approximately 480 cm-1. For Raman spectra determination, the peaks arose from the Brillouin zone center, and two additional peaks were observed at 660 and 1320 cm-1, 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-1. Furthermore, in the polarization state, the centers of all peak positions slightly shifted for hexagon-shaped α-Fe2O3, but all peak positions for square-shaped and rhombic-shaped α-Fe2O3 exhibited a significant blueshift. The structure of hexagon-shaped α-Fe2O3 was relatively tolerant regarding the polarization properties of vibration modes; however, the symmetry of crystal square-shaped and rhombic-shaped α-Fe2O3 changed, subsequently revealing different optical properties. RESEARCH HIGHLIGHTS: The hexagon-shaped, square-shaped, and rhombic-shaped α-Fe2O3 enclosed by different planes were synthesized. The Fourier Transform Infrared spectrometer peaks of α-Fe2O3 depended on their hexagon, square and rhombic shapes. Compared with hexagon-shaped α-Fe2O3, the Raman peaks for square and rhombi ones significantly shifted. The hexagon-shaped α-Fe2O3 is relatively tolerant regarding the polarization properties.