<p>Achieving the second-order nonlinear optical (NLO) effect necessitates a non-centrosymmetric (NCS) structure, which is a prerequisite, but obtaining it effectively remains greatly challenging. In pursuit of this, a strategy known as “dimensionality elevation” has been operated to create a high-dimensional NCS framework based on a low-dimensional centrosymmetric (CS) structure. Concretely, the acentric [CdS<sub>4</sub>] tetrahedral unit serves as a linkage point in the zero-dimensional (0D) [Si<sub>4</sub>S<sub>10</sub>] T2-supertetrahedra, leading to the formation of the 3D NCS rigid sulfide, Cs<sub>2</sub>CdSi<sub>4</sub>S<sub>10</sub> (<b>1</b>), which exhibits moderate second-harmonic generation (SHG) effect (0.5 × AgGaS<sub>2</sub>@1.91 μm). To enhance the SHG coefficient, a structural modification has been made by replacing the Si-based framework with a Ga-based one and re-employing the “dimensionality elevation” strategy. This alteration prompted the tetrahedral [CdS<sub>4</sub>] units to connect with 0D T2-supertetrahedral [Ga<sub>4</sub>S<sub>10</sub>] motifs, creating the 3D NCS salt-inclusion chalcogenide [Ba<sub>4</sub>Cl<sub>2</sub>][CdGa<sub>4</sub>S<sub>10</sub>] (<b>2</b>). Notably, compared with <b>1</b>, compound <b>2</b> not only demonstrates an increased SHG response (1.3 × AgGaS<sub>2</sub> @1.91 μm) but also retains a broad band gap (3.74 eV for <b>1</b> and 3.50 eV for <b>2</b>) for exceptional laser-induced damage thresholds (LIDTs, 9.3 × and 7.3 × AgGaS<sub>2</sub> @1.06 μm for <b>1</b> and <b>2</b>, respectively), suggesting that compound <b>2</b> is an advanced infrared NLO material. This research pioneers new pathways for discovering NCS NLO materials through the “dimensionality elevation” strategy.</p>

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Achieving excellent nonlinear optical performance via “dimensionality elevation”-driven transformation from centrosymmetric to non-centrosymmetric structures

  • Lin-Tao Jiang,
  • Jun-Long Chen,
  • Ming-Shu Zhang,
  • Xiao-Ming Jiang,
  • Bin-Wen Liu,
  • Guo-Cong Guo

摘要

Achieving the second-order nonlinear optical (NLO) effect necessitates a non-centrosymmetric (NCS) structure, which is a prerequisite, but obtaining it effectively remains greatly challenging. In pursuit of this, a strategy known as “dimensionality elevation” has been operated to create a high-dimensional NCS framework based on a low-dimensional centrosymmetric (CS) structure. Concretely, the acentric [CdS4] tetrahedral unit serves as a linkage point in the zero-dimensional (0D) [Si4S10] T2-supertetrahedra, leading to the formation of the 3D NCS rigid sulfide, Cs2CdSi4S10 (1), which exhibits moderate second-harmonic generation (SHG) effect (0.5 × AgGaS2@1.91 μm). To enhance the SHG coefficient, a structural modification has been made by replacing the Si-based framework with a Ga-based one and re-employing the “dimensionality elevation” strategy. This alteration prompted the tetrahedral [CdS4] units to connect with 0D T2-supertetrahedral [Ga4S10] motifs, creating the 3D NCS salt-inclusion chalcogenide [Ba4Cl2][CdGa4S10] (2). Notably, compared with 1, compound 2 not only demonstrates an increased SHG response (1.3 × AgGaS2 @1.91 μm) but also retains a broad band gap (3.74 eV for 1 and 3.50 eV for 2) for exceptional laser-induced damage thresholds (LIDTs, 9.3 × and 7.3 × AgGaS2 @1.06 μm for 1 and 2, respectively), suggesting that compound 2 is an advanced infrared NLO material. This research pioneers new pathways for discovering NCS NLO materials through the “dimensionality elevation” strategy.