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RESEARCH PAPER · Advanced Optical Materials · 2021

AXHg3P2S8 (A = Rb, Cs; X = Cl, Br): New Excellent Infrared Nonlinear Optical Materials with Mixed‐Anion Chalcohalide Groups of Trigonal Planar [HgS2X]3− and Tetrahedral [HgS3X]5−

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AXHg3P2S8 (A = Rb, Cs; X = Cl, Br): New Excellent Infrared Nonlinear Optical Materials with Mixed‐Anion Chalcohalide Groups of Trigonal Planar [HgS2X]3− and Tetrahedral [HgS3X]5−OriginalHighly Distorted [HgS 4 ] Motif-Driven Structural Symmetry Degradation and Strengthened Second-Harmonic Generation Response in the Defect Diamond-Like Chalcogenide Hg 3 P 2 S 846Transition-metal-based chalcogenides: A rich source of infrared nonlinear optical materials184SnPQ3 (Q = S, Se, S/Se): A Series of Lone-Pair Cationic Chalcogenophosphates Exhibiting Balanced NLO Activity Originating from SnQ8 Units49Highly polarized [GeOTe 3 ] motif-driven structural order promotion and an enhanced second harmonic generation response in the new nonlinear optical oxytelluride Ba 3 Ge 2 O 4 Te 334Hg-based chalcogenides: An intriguing class of infrared nonlinear optical materials128Structural modification from centrosymmetric Rb 4 Hg 2 Ge 2 S 8 to noncentrosymmetric (Na 3 Rb)Hg 2 Ge 2 S 8 : mixed alkali metals strategy for infrared nonlinear optical material design28[ASr 4 Cl][Ge 3 S 10 ] (A = Na, K) and [KBa 4 Cl][Ge 3 S 10 ]: new salt-inclusion infrared nonlinear optical crystals with zero-dimensional [Ge 3 S 9 ] clusters32Ba 6 In 2 Ge 2 Te 15 : a THz birefringent material with an intriguing quasi-[Te 5 ] 4− chain possessing large optical anisotropy and an ultrawide transmission range7Bridging oxygen atoms in trigonal prism units driven strong second-harmonic-generation efficiency in Sr 3 Ge 2 O 4 Te 318Broad transparency and wide band gap achieved in a magnetic infrared nonlinear optical chalcogenide by suppressing d–d transitions41First polar quaternary sulphide CsLiGa 6 S 10 with mixed ordered alkali cations displaying excellent infrared nonlinear optical properties16Rational design of a promising oxychalcogenide infrared nonlinear optical crystal60The synthesis and structure–property relation analysis of metal chalcohalide crystals Cs 2 InPS 4 X 2 (X = Cl, Br) with mixed anions6Wide band gap thiophosphates ASrPS 4 (A = Li, Na, K, Rb, Cs): cation size effect induced successive structural transformation13Optimized Bridgman growth and quality improvement of LiInSe2 crystal by annealing in Li2Se vapor atmosphere12Explorations of New SHG Materials in Mercury Iodate Sulfate System**9Toward the Rational Design of Mid‐Infrared Nonlinear Optical Materials with Targeted Properties via a Multi‐Level Data‐Driven Approach110A comprehensive review on metal chalcogenides with three-dimensional frameworks for infrared nonlinear optical applications114Ternary AGa5S8 (A = K, Rb, Cs): Promising infrared nonlinear optical materials rationally realized by “one-for-multiple substitution” strategy37Chalcohalides: A Rising Type of Second‐Order Nonlinear Optical Materials28From Ba3Nb2O2F12(H2O)2 to Ba0.5NbO2F2(H2O): Achieving Balanced Nonlinear Optical Performance by O/F Ratio Regulation18[Sr 4 Cl 2 ][Si 3 S 9 ]: Ultrawide-bandgap salt-inclusion thiosilicate nonlinear optical material with unprecedented tri-polymerized [Si 3 S 9 ] clusters21A non-centrosymmetric chalcohalide synthesized through the combination of chemical tailoring with aliovalent substitution12From BPS 4 to AB 3 P 2 S 10 (A = Na, K): cations inducing dimension reduction and bandgap enlargement7Na 6 Sn 3 P 4 S 16 : Sn( ii )-chelated PS 4 groups inspired an ultra-strong SHG response22Open honeycomb frameworks of sulphides AHg 4 Ga 5 S 12 (A = Rb, Cs) exhibiting infrared nonlinear optical properties12LnLiSiS4 (Ln = La and Ce): Promising infrared nonlinear optical materials designed by aliovalent substitution from SrCdSiS437[K2PbX][Ga7S12] (X = Cl, Br, I): The First Lead‐Containing Cationic Moieties with Ultrahigh Second‐Harmonic Generation and Band Gaps Exceeding the Criterion of 2.33 eV46Na3SiS3F: A Wide Bandgap Fluorothiosilicate with Unique [SiS3F] Unit and High Laser‐Induced Damage Threshold39Halide-Induced Band Gap Enhancement from Ba2SnSe4 to KBa2SnSe4Cl2Excellent Nonlinear Optical M[M4Cl][Ga11S20] (M = A/Ba, A = K, Rb) Achieved by Unusual Cationic Substitution Strategy20A ll HgM IV S 4 (A ll = Sr, Ba, M IV = Si, Ge): A Series of Materials with Large Second Harmonic Generation Response and Wide Band Gaps27Adduct‐Type Compounds for Nonlinear Optical Crystals0Breaking Through the Trade‐Off Between Wide Band Gap and Large SHG Coefficient in Mercury‐Based Chalcogenides for IR Nonlinear Optical Application49A I B 3 II C 2 III Q 6 VI X VII : A Thioborate Halide Family for Developing Wide Bandgap Infrared Nonlinear Materials by Coupling Planar [BS 3 ] and Polycations25Na 6 Mg 3 P 4 S 16 and RbMg 2 PS 4 Cl 2 : two Mg-based thiophosphates with ultrawide bandgaps resulting from [MgS 6 ] and [MgS x Cl 6− x ] octahedra4Regulating the key performance parameters for Hg-based IR NLO chalcogenides via bandgap engineering strategy26Ga-based IR nonlinear optical materials: Synthesis, structures, and properties65Exploring a new short-wavelength nonlinear optical fluoride material featuring unprecedented polar cis -[Zr 6 F 34 ] 10− clusters48Hg 3 AsS 4 X (X = Cl and Br): two Hg-based chalcogenides as long-wave infrared nonlinear optical crystals with superior comprehensive performances33Salt-inclusion chalcogenides with d-orbital components: unveiling remarkable nonlinear optical properties and dual-band photoluminescence10Ba10In2Mn11Si3O12S18: First Hexanary Oxychalcogenide Containing an Infrequent Three-Dimensional Noncentrosysmmetric Framework8Centrosymmetric CaBaMF8 and Noncentrosymmetric Li2CaMF8 (M = Zr, Hf): Dimension Variation and Nonlinear Optical Activity Resulting from an Isovalent Cation Substitution-Oriented Design17Infrared nonlinear optical materials with multiple strongly ionic cations5The first Hg-based oxychalcogenide Sr2HgGe2OS6: Achieving balanced IR nonlinear optical properties through synergistic cation and anion substitution28Influence of Cation-Size Effects of Alkaline Earth (Ae) Metals on Dimensionality and Optical Anisotropy Regulation in K4AeP2S8 Thiophosphates5Structure‐Prediction‐Oriented Synthesis of Thiophosphates as Promising Infrared Nonlinear Optical Materials24Structure‐Prediction‐Oriented Synthesis of Thiophosphates as Promising Infrared Nonlinear Optical Materials1[Cs14Cl][Tm71Se110]: An unusual salt-inclusion chalcogenide containing different valent Tm centers and ultralow thermal conductivity10La 3 (Ga 3 S 3 O 3 )(Si 2 O 7 ): An Oxychalcogenide Demonstrating Ultrawide Optical Bandgap and Favorable Birefringence Propelled by Divergent Anionic Groups6Emergent Mid‐Infrared Nonlinear Optical Candidates With Targeted Balance Performances17Chalcophosphates: A plentiful source of infrared nonlinear optical materials42From Orthorhombic Cu8GeS6 to Cubic Cu6HgGeS6: Second-Harmonic Generation and Photocurrent Responses7Controlling d10 Metal in Phenylthiourea‐Based Hybrid Metal Halides to Actualize Dimensional Transformation and Significantly Improve the Birefringence11Vacancy-driven tetrahedral distortion leading to exceptional second harmonic generation3Homogeneous growth of bulk BaGa 4 Se 7 single crystal and femtosecond laser performance and photodarkening5Halogen‐Rich Design Strategy: Rational Synthesis of High‐Performance Tetrahedron‐Based Chalcohalides for Advanced Infrared Optical Materials2Halogen‐Rich Design Strategy: Rational Synthesis of High‐Performance Tetrahedron‐Based Chalcohalides for Advanced Infrared Optical Materials2

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  2. Transition-metal-based chalcogenides: A rich source of infrared nonlinear optical materials

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  3. SnPQ3 (Q = S, Se, S/Se): A Series of Lone-Pair Cationic Chalcogenophosphates Exhibiting Balanced NLO Activity Originating from SnQ8 Units

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  4. Highly polarized [GeOTe 3 ] motif-driven structural order promotion and an enhanced second harmonic generation response in the new nonlinear optical oxytelluride Ba 3 Ge 2 O 4 Te 3

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  5. Hg-based chalcogenides: An intriguing class of infrared nonlinear optical materials

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  6. Structural modification from centrosymmetric Rb 4 Hg 2 Ge 2 S 8 to noncentrosymmetric (Na 3 Rb)Hg 2 Ge 2 S 8 : mixed alkali metals strategy for infrared nonlinear optical material design

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  7. [ASr 4 Cl][Ge 3 S 10 ] (A = Na, K) and [KBa 4 Cl][Ge 3 S 10 ]: new salt-inclusion infrared nonlinear optical crystals with zero-dimensional [Ge 3 S 9 ] clusters

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  8. Ba 6 In 2 Ge 2 Te 15 : a THz birefringent material with an intriguing quasi-[Te 5 ] 4− chain possessing large optical anisotropy and an ultrawide transmission range

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  9. Bridging oxygen atoms in trigonal prism units driven strong second-harmonic-generation efficiency in Sr 3 Ge 2 O 4 Te 3

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  10. Broad transparency and wide band gap achieved in a magnetic infrared nonlinear optical chalcogenide by suppressing d–d transitions

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  11. First polar quaternary sulphide CsLiGa 6 S 10 with mixed ordered alkali cations displaying excellent infrared nonlinear optical properties

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  12. Rational design of a promising oxychalcogenide infrared nonlinear optical crystal

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  13. The synthesis and structure–property relation analysis of metal chalcohalide crystals Cs 2 InPS 4 X 2 (X = Cl, Br) with mixed anions

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  14. Wide band gap thiophosphates ASrPS 4 (A = Li, Na, K, Rb, Cs): cation size effect induced successive structural transformation

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  15. Optimized Bridgman growth and quality improvement of LiInSe2 crystal by annealing in Li2Se vapor atmosphere

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  16. Explorations of New SHG Materials in Mercury Iodate Sulfate System**

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  17. Toward the Rational Design of Mid‐Infrared Nonlinear Optical Materials with Targeted Properties via a Multi‐Level Data‐Driven Approach

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  18. A comprehensive review on metal chalcogenides with three-dimensional frameworks for infrared nonlinear optical applications

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  19. Ternary AGa5S8 (A = K, Rb, Cs): Promising infrared nonlinear optical materials rationally realized by “one-for-multiple substitution” strategy

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  20. Chalcohalides: A Rising Type of Second‐Order Nonlinear Optical Materials

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  21. From Ba3Nb2O2F12(H2O)2 to Ba0.5NbO2F2(H2O): Achieving Balanced Nonlinear Optical Performance by O/F Ratio Regulation

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  22. [Sr 4 Cl 2 ][Si 3 S 9 ]: Ultrawide-bandgap salt-inclusion thiosilicate nonlinear optical material with unprecedented tri-polymerized [Si 3 S 9 ] clusters

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  23. A non-centrosymmetric chalcohalide synthesized through the combination of chemical tailoring with aliovalent substitution

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  24. From BPS 4 to AB 3 P 2 S 10 (A = Na, K): cations inducing dimension reduction and bandgap enlargement

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  25. Na 6 Sn 3 P 4 S 16 : Sn( ii )-chelated PS 4 groups inspired an ultra-strong SHG response

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  28. [K2PbX][Ga7S12] (X = Cl, Br, I): The First Lead‐Containing Cationic Moieties with Ultrahigh Second‐Harmonic Generation and Band Gaps Exceeding the Criterion of 2.33 eV

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  30. Halide-Induced Band Gap Enhancement from Ba2SnSe4 to KBa2SnSe4Cl

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  31. Excellent Nonlinear Optical M[M4Cl][Ga11S20] (M = A/Ba, A = K, Rb) Achieved by Unusual Cationic Substitution Strategy

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  32. A ll HgM IV S 4 (A ll = Sr, Ba, M IV = Si, Ge): A Series of Materials with Large Second Harmonic Generation Response and Wide Band Gaps

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  33. Adduct‐Type Compounds for Nonlinear Optical Crystals

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  34. Breaking Through the Trade‐Off Between Wide Band Gap and Large SHG Coefficient in Mercury‐Based Chalcogenides for IR Nonlinear Optical Application

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  35. A I B 3 II C 2 III Q 6 VI X VII : A Thioborate Halide Family for Developing Wide Bandgap Infrared Nonlinear Materials by Coupling Planar [BS 3 ] and Polycations

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  36. Na 6 Mg 3 P 4 S 16 and RbMg 2 PS 4 Cl 2 : two Mg-based thiophosphates with ultrawide bandgaps resulting from [MgS 6 ] and [MgS x Cl 6− x ] octahedra

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  37. Regulating the key performance parameters for Hg-based IR NLO chalcogenides via bandgap engineering strategy

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  39. Exploring a new short-wavelength nonlinear optical fluoride material featuring unprecedented polar cis -[Zr 6 F 34 ] 10− clusters

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  42. Ba10In2Mn11Si3O12S18: First Hexanary Oxychalcogenide Containing an Infrequent Three-Dimensional Noncentrosysmmetric Framework

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  43. Centrosymmetric CaBaMF8 and Noncentrosymmetric Li2CaMF8 (M = Zr, Hf): Dimension Variation and Nonlinear Optical Activity Resulting from an Isovalent Cation Substitution-Oriented Design

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  46. Influence of Cation-Size Effects of Alkaline Earth (Ae) Metals on Dimensionality and Optical Anisotropy Regulation in K4AeP2S8 Thiophosphates

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  47. Structure‐Prediction‐Oriented Synthesis of Thiophosphates as Promising Infrared Nonlinear Optical Materials

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