Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub>: promising low-birefringence materials for UV and deep UV zero-order waveplates

Zero-order waveplates, which are used to modulate the polarization of light, play a crucial role in scientific instrumentation, optical communications, and the laser industry. However, owing to the limitations imposed by birefringence and absorption edges, only few materials can produce desirable birefringence with suitable transparency in the ultraviolet (UV) and deep ultraviolet (DUV) regions. Borates represent promising materials with widely adjustable birefringence. In this study, we successfully synthesized two new borates, Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub>, using solid-state reactions in vacuum-sealed tubes; the fundamental building blocks (FBBs) of the two compounds are B<sub>3</sub>O<sub>7</sub> and B<sub>9</sub>O<sub>19</sub> units, respectively. Notably, Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub> possess very low birefringence values of 0.0058 at 546 nm and 0.0068 at 546 nm, respectively, considerably lower than that of a commercial quartz waveplate (0.0092 at 532 nm). UV-Vis-NIR diffuse reflectance measurements show that the UV cutoff edges of Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub> are lower than 320 and 200 nm, corresponding to the bandgaps of 3.20 and 6.20 eV, respectively. These two compounds can serve as potential zero-order waveplate materials in the UV and DUV regions.

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Publication Details

Journal
Dalton Transactions
Published
2025-01-01
DOI
https://doi.org/10.1039/d5dt01706h
Citations
1
Primary Topic
Crystal Structures and Properties
Type
article
Field-Weighted Citation Impact
0.43
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article

Li2CeRbB18O30 and Li2Cs2SrB18O30: promising low-birefringence materials for UV and deep UV zero-order waveplates

Xiao-Ming Wang, Shilie Pan, Feng Zhang, Zhiyuan Zhang et al.
1 citations
Dalton Transactions
Crystal Structures and Properties
0.43
article

Li2CeRbB18O30 and Li2Cs2SrB18O30: promising low-birefringence materials for UV and deep UV zero-order waveplates

Xiao-Ming Wang, Shilie Pan, Feng Zhang, Zhiyuan Zhang, Juanjuan Lu
article en
1 citations

Abstract

Zero-order waveplates, which are used to modulate the polarization of light, play a crucial role in scientific instrumentation, optical communications, and the laser industry. However, owing to the limitations imposed by birefringence and absorption edges, only few materials can produce desirable birefringence with suitable transparency in the ultraviolet (UV) and deep ultraviolet (DUV) regions. Borates represent promising materials with widely adjustable birefringence. In this study, we successfully synthesized two new borates, Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub>, using solid-state reactions in vacuum-sealed tubes; the fundamental building blocks (FBBs) of the two compounds are B<sub>3</sub>O<sub>7</sub> and B<sub>9</sub>O<sub>19</sub> units, respectively. Notably, Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub> possess very low birefringence values of 0.0058 at 546 nm and 0.0068 at 546 nm, respectively, considerably lower than that of a commercial quartz waveplate (0.0092 at 532 nm). UV-Vis-NIR diffuse reflectance measurements show that the UV cutoff edges of Li<sub>2</sub>CeRbB<sub>18</sub>O<sub>30</sub> and Li<sub>2</sub>Cs<sub>2</sub>SrB<sub>18</sub>O<sub>30</sub> are lower than 320 and 200 nm, corresponding to the bandgaps of 3.20 and 6.20 eV, respectively. These two compounds can serve as potential zero-order waveplate materials in the UV and DUV regions.

Dalton TransactionsVol. 54(39)
Xinjiang Technical Institute of Physics & Chemistry (CN), University of Chinese Academy of Sciences (CN)
Openalex Percentile: Top 36%
Crystal Structures and Properties
0.43
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