Toward Atomic-Scale Control over Structural Modulations in Quasi-1D Chalcogenides for Colossal Optical Anisotropy

Optically anisotropic materials are sought after for tailoring the polarization of light. Recently, colossal optical anisotropy (Δ<i>n</i> = 2.1) was reported in a quasi-one-dimensional chalcogenide, Sr<sub>9/8</sub>TiS<sub>3</sub>. Compared to SrTiS<sub>3</sub>, the excess Sr in Sr<sub>9/8</sub>TiS<sub>3</sub> leads to periodic structural modulations and introduces additional electrons, which undergo charge ordering on select Ti atoms to form a highly polarizable cloud oriented along the <i>c</i>-axis, hence resulting in the colossal optical anisotropy. Here, further enhancement of the colossal optical anisotropy to Δ<i>n</i> = 2.5 in Sr<sub>8/7</sub>TiS<sub>3</sub> is reported through control over the periodicity of the atomic-scale modulations. The role of structural modulations in tuning the optical properties in a series of Sr<sub><i>x</i></sub>TiS<sub>3</sub> compounds with <i>x</i> = [1, 9/8, 8/7, 6/5, 5/4, 4/3, 3/2] is investigated using density-functional-theory (DFT) calculations. The structural modulations arise from various stacking sequences of face-sharing TiS<sub>6</sub> octahedra and twist-distorted trigonal prisms and are found to be thermodynamically stable for 1 < <i>x</i> < 1.5. As <i>x</i> increases, an indirect-to-direct band gap transition is predicted for <i>x</i> ≥ 8/7 along with an increased occupancy of Ti-<i>d</i><sub><i>z</i><sup>2</sup></sub> states. Together, these two factors result in a theoretically predicted maximum birefringence of Δ<i>n</i> = 2.5 for Sr<sub>8/7</sub>TiS<sub>3</sub>. Single crystals of Sr<sub>8/7</sub>TiS<sub>3</sub> were grown using a molten-salt flux method. Single-crystal X-ray diffraction measurements confirm the presence of long-range order with a periodicity corresponding to Sr<sub>8/7</sub>TiS<sub>3</sub>, which is further corroborated by atomic-scale observations using scanning transmission electron microscopy. Polarization-resolved Fourier-transform infrared spectroscopy of Sr<sub>8/7</sub>TiS<sub>3</sub> crystals shows Δ<i>n</i> ≈ 2.5, in excellent agreement with the theoretical predictions. Overall, these findings demonstrate the compositional tunability of optical properties in Sr<sub><i>x</i></sub>TiS<sub>3</sub> compounds by control over atomic scale modulations and suggest that similar strategies could be extended to other compounds having modulated structures.

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Journal
ACS Nano
Published
2025-10-20
DOI
https://doi.org/10.1021/acsnano.5c07992
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1
Primary Topic
Chalcogenide Semiconductor Thin Films
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article
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article

Toward Atomic-Scale Control over Structural Modulations in Quasi-1D Chalcogenides for Colossal Optical Anisotropy

Shantanu Singh, Jayakanth Ravichandran, Jordan A. Hachtel, Miaofang Chi et al.
1 citations
ACS Nano
Chalcogenide Semiconductor Thin Films
0.73
article

Toward Atomic-Scale Control over Structural Modulations in Quasi-1D Chalcogenides for Colossal Optical Anisotropy

Shantanu Singh, Jayakanth Ravichandran, Jordan A. Hachtel, Miaofang Chi, Gwan Yeong Jung, Wooseon Choi, Rohan Mishra, Guodong Ren, Kevin Ye, Andrew R. Lupini, Huandong Chen, Young‐Min Kim, Boyang Zhao
article en
1 citations

Abstract

Optically anisotropic materials are sought after for tailoring the polarization of light. Recently, colossal optical anisotropy (Δ<i>n</i> = 2.1) was reported in a quasi-one-dimensional chalcogenide, Sr<sub>9/8</sub>TiS<sub>3</sub>. Compared to SrTiS<sub>3</sub>, the excess Sr in Sr<sub>9/8</sub>TiS<sub>3</sub> leads to periodic structural modulations and introduces additional electrons, which undergo charge ordering on select Ti atoms to form a highly polarizable cloud oriented along the <i>c</i>-axis, hence resulting in the colossal optical anisotropy. Here, further enhancement of the colossal optical anisotropy to Δ<i>n</i> = 2.5 in Sr<sub>8/7</sub>TiS<sub>3</sub> is reported through control over the periodicity of the atomic-scale modulations. The role of structural modulations in tuning the optical properties in a series of Sr<sub><i>x</i></sub>TiS<sub>3</sub> compounds with <i>x</i> = [1, 9/8, 8/7, 6/5, 5/4, 4/3, 3/2] is investigated using density-functional-theory (DFT) calculations. The structural modulations arise from various stacking sequences of face-sharing TiS<sub>6</sub> octahedra and twist-distorted trigonal prisms and are found to be thermodynamically stable for 1 < <i>x</i> < 1.5. As <i>x</i> increases, an indirect-to-direct band gap transition is predicted for <i>x</i> ≥ 8/7 along with an increased occupancy of Ti-<i>d</i><sub><i>z</i><sup>2</sup></sub> states. Together, these two factors result in a theoretically predicted maximum birefringence of Δ<i>n</i> = 2.5 for Sr<sub>8/7</sub>TiS<sub>3</sub>. Single crystals of Sr<sub>8/7</sub>TiS<sub>3</sub> were grown using a molten-salt flux method. Single-crystal X-ray diffraction measurements confirm the presence of long-range order with a periodicity corresponding to Sr<sub>8/7</sub>TiS<sub>3</sub>, which is further corroborated by atomic-scale observations using scanning transmission electron microscopy. Polarization-resolved Fourier-transform infrared spectroscopy of Sr<sub>8/7</sub>TiS<sub>3</sub> crystals shows Δ<i>n</i> ≈ 2.5, in excellent agreement with the theoretical predictions. Overall, these findings demonstrate the compositional tunability of optical properties in Sr<sub><i>x</i></sub>TiS<sub>3</sub> compounds by control over atomic scale modulations and suggest that similar strategies could be extended to other compounds having modulated structures.

ACS NanoVol. 19(43)
University of Southern California (US), Oak Ridge National Laboratory (US), Minghsin University of Science and Technology (TW), Washington University in St. Louis (US), California Southern University (US), Institute for Basic Science (KR), Division of Materials Science and Engineering (AU), Center for Nanophase Materials Sciences, Sungkyunkwan University (KR)
Openalex Percentile: Top 22%
Chalcogenide Semiconductor Thin Films
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