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RESEARCH PAPER · Angewandte Chemie International Edition · 2022

Sr3[SnOSe3][CO3]: A Heteroanionic Nonlinear Optical Material Containing Planar π‐conjugated [CO3] and Heteroleptic [SnOSe3] Anionic Groups

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Sr3[SnOSe3][CO3]: A Heteroanionic Nonlinear Optical Material Containing Planar π‐conjugated [CO3] and Heteroleptic [SnOSe3] Anionic GroupsOriginal[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 2 [WO 3 F(IO 3 )][WO 3 F 2 ]: the first polar fluorinated tungsten iodate featuring a direct W–O–I bond7Synthesis, structural evolution and optical properties of a new family of oxychalcogenides [Sr 3 VO 4 ][MQ 3 ] (M = Ga, In, Q = S, Se)10Improved Polarization in the Sr6Cd2Sb6O7Se10 Oxyselenide through Design of Lateral Sublattices for Efficient Photoelectric Conversion4Improved Polarization in the Sr6Cd2Sb6O7Se10 Oxyselenide through Design of Lateral Sublattices for Efficient Photoelectric Conversion16Deep Ultraviolet-Transparent Materials with Strong Second-Harmonic Response50[C(NH2)3]2MoO2F4·H2O: Unique Chinese-Knot Structure Revealing Superior Nonlinear-Optical Properties19Oxychalcogenides as Promising Ultraviolet Nonlinear Optical Candidates: Experimental and Theoretical Studies of AEGeOS2(AE = Sr and Ba)24AeMg6Ga6S16 (Ae = Ca, Sr, Ba): The First Double Alkaline‐Earth Metal Chalcogenides with Excellent Performances29Rb 2 CdSi 4 S 10 : novel [Si 4 S 10 ] T2-supertetrahedra-contained infrared nonlinear optical material with large band gap79The Antiperovskite‐Type Oxychalcogenides Ae3Q[GeOQ3] (Ae = Ba, Sr; Q = S, Se) with Large Second Harmonic Generation Responses and Wide Band Gaps68Ba5Ga2SiO4S6: a Phase-Matching Nonlinear Optical Oxychalcogenide Design via Structural Regulation Originated from Heteroanion Introduction25Oxychalcogenides: A Promising Class of Materials for Nonlinear Optical Crystals with Mixed‐Anion Groups35[M(OH) 2 ] 3 (IO 3 )(SeO 4 )·H 2 O (M = Ga and In): metal iodate–selenate nonlinear optical materials with a hexagonal tungsten oxide-type topology20Honeycomb layered topology construction for exceptional long-wave infrared nonlinear optical crystals29Modulating optical performance by phase transition in a nonlinear optical material β-Li 2 RbBi(PO 4 ) 28Recent progress in the design of IR nonlinear optical materials by partial chemical substitution: Structural evolution and performance optimization133Rational Design of a Rare‐Earth Oxychalcogenide Nd3[Ga3O3S3][Ge2O7] with Superior Infrared Nonlinear Optical Performance64Chain‐like [S x ] ( x =2–6) Units Realizing Giant Birefringence with Transparency in the Near‐Infrared for Optoelectronic Materials53Chain‐like [S x ] ( x =2–6) Units Realizing Giant Birefringence with Transparency in the Near‐Infrared for Optoelectronic Materials5AKTeO2(CO3) (A = Li, Na): The First Carbonatotellurites Featuring a Zero-Dimensional [Te2C2O10]4– Cluster and a Wide Band Gap5Designing a Strong Second-Harmonic Generation Polar Iodate by the Structure-Directing Properties of the “Tumbler-like” [Zn(IO3)(I2O5(OH))] Polyanions20Na3SiS3F: A Wide Bandgap Fluorothiosilicate with Unique [SiS3F] Unit and High Laser‐Induced Damage Threshold39Cd2Nb2Te4O15: A Novel Pseudo‐Aurivillius‐Type Tellurite with Unprecedented Nonlinear Optical Properties and Excellent Stability40[Ba4(S2)][ZnGa4S10]: Design of an Unprecedented Infrared Nonlinear Salt‐Inclusion Chalcogenide with Disulfide‐Bonds36Heteroanionic LaBrVIO4 (VI = Mo, W): Excellence in Both Nonlinear Optical Properties and Photoluminescent Properties11LiGa(IO3)4: An Excellent NLO Material with Unprecedented 2D [Ga(IO3)4]∞− Layer Synthesized by Aliovalent Substitution20A 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 Gaps27Chiral and Polar Duality Design of Heteroanionic Compounds: Sr18Ge9O5S31 Based on [Sr3OGeS3]2+ and [Sr3SGeS3]2+ Groups20Ga-based IR nonlinear optical materials: Synthesis, structures, and properties65“Three‐in‐One”: A New Hg‐Based Selenide Hg 7 P 2 Se 12 Exhibiting Wide Infrared Transparency Range and Strong Nonlinear Optical Effect80Ba 2 GeF 2 Q 3 (Q = S, Se) and Ba 3 GeF 2 Se 4 : new F-based chalcohalides with enhanced birefringence9Chemical perspectives on heteroanionic compounds: a potential playground for multiferroics7From NaGa(IO3)3F to NaGa(IO3)2F2 and NaGa(IO3)4: The Effects of Chemical Substitution between F– Anions and IO3– Groups on the Structures and Properties of Gallium Iodates13Hydrogen bonding bolstered head-to-tail ligation of functional chromophores in a 0D SbF 3 ·glycine adduct for a short-wave ultraviolet nonlinear optical material32New ultraviolet transparent rare-earth borates with enhanced birefringence induced by cation chemical substitution15Partial substitution with a significant effect: coexistence of a wide band gap and large birefringence in the oxychalcogenide AEGe 2 O 4 Se (AE = Sr and Ba)17Rare-earth-based chalcogenides and their derivatives: an encouraging IR nonlinear optical material candidate70Tunable third‐order NLO properties of acene derivatives with molecular structural modification7Pinalites: Optical Properties and Quantum Magnetism of Heteroanionic A3MO5X2 Compounds6Ba10In2Mn11Si3O12S18: First Hexanary Oxychalcogenide Containing an Infrequent Three-Dimensional Noncentrosysmmetric Framework8Theoretical Investigation of Structural, Electronic and Optical Properties of Cs3MoO4(HCO3) with NLO Active Functional Units2LaMg6Ga6S16: a chemical stable divalent lanthanide chalcogenide70Assembly of π‐Conjugated [B 3 O 6 ] Units by Mer‐Isomer [YO 3 F 3 ] Octahedra to Design a UV Nonlinear Optical Material, Cs 2 YB 3 O 6 F 211Assembly of π‐Conjugated [B3O6] Units by Mer‐Isomer [YO3F3] Octahedra to Design a UV Nonlinear Optical Material, Cs2YB3O6F297C6N7(NH2)3·H3PO4: Strong Second Harmonic Generation and Giant Birefringence Benefiting from Amino Substitution Strategy24Ae3[TO3][SnOQ3] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se) and Ba3[CO3][MQ4] (M = Ge, Sn; Q = S, Se): Design and Syntheses of a Series of Heteroanionic Antiperovskite-Type Oxychalcogenides29ACuGa 6 S 10 (A = Rb, Cs): Design and Synthesis of Two New Cavity‐Chalcopyrite Chalcogenides Based on “Iterative Substitution” Strategy4BaPb2(CO3)2F2: Enhancing Birefringence by a Multiunit Synergy Effect9Balanced IR Nonlinear Optical Performance Achieved by Cation–Anion Module Cosubstitution in V-Based Salt-Inclusion Oxychalcogenides22Looking Back the Nonlinear Optical Crystals in a Functionalized Unit's Perspective109Rational design of a series of non-centrosymmetric antiperovskite and double antiperovskite borate fluorides13La 3 (Ga 3 S 3 O 3 )(Si 2 O 7 ): An Oxychalcogenide Demonstrating Ultrawide Optical Bandgap and Favorable Birefringence Propelled by Divergent Anionic Groups6Tin chalcohalide Sn 11 (PS 4 ) 4 I 10 obtained from structural-template-oriented synthesis: exhibiting balanced infrared nonlinear optical performance6Emergent Mid‐Infrared Nonlinear Optical Candidates With Targeted Balance Performances17Rare‐Earth Substitution Induced Symmetry Breaking for The First Sc‐Based Nonlinear Optical Chalcogenide with High‐Performance30Bulk crystal growth and optical properties of a novel organic–inorganic hybrid nonlinear optical thiocyanate: [Mn(CH 3 CONH 2 ) 2 ] [Hg(SCN) 4 ]10Ca 2 La(MS 4 )(BS 3 ) (M = Ge/Si and Sn/Si): high-performance infrared nonlinear optical materials designed using an atomic site co-occupancy strategy9Designing infrared nonlinear optical crystals, Sr 2 MgSn 2 OS 6 and Sr 2 SnGa 2 OS 6 , with hybrid anionic frameworks via a double substitution strategy4M 3 MoO 4 (HCO 3 ) (M = Rb and Cs): cation-tuned synthesis of two noncentrosymmetric molybdate-carbonates with isolated [MoO 4 ] and [HCO 3 ] groups0NaCaGa 3 S 6 : a mixed alkali metal and alkaline earth metal sulfide with a distinctive [Ga 5 S 10 ] ∞ layered framework0Hetero‐Anionic Oxychalcogenides with Structures and Properties Tuned by the O:S Ratio14Two-in-one: assembling hybrid supertetrahedra chromophores and achieving high-performance “hexagonal warriors” in nonlinear optical crystals6Zero-Dimensional Oxyselenide Ba12[(Ga2OSe5)3(Si2O7)]: Enhanced Optical Anisotropy through Heteroanionic Engineering4Phase-Matching Second-Harmonic Generation in Zero-Dimensional Zinc Thiocyanates Ligated with Chiral Amino Acids6Ca 7 (TeO 3 ) 6 (MoO 4 ): A Promising Mid-Infrared Nonlinear Optical Crystal Activated via a Module-Oriented Dimensionality Reduction Strategy34Syntheses, Structures, and Characterization of Alkali-Metal Molybdates, A3Cl[Mo2O7] (A = K, Rb and Cs)3Synergistic Enhancement of Band Gap and Optical Anisotropy via Functional-Site Cosubstitution in Antiperovskite-Type Chalcohalides [Ba2K][X][MS4] (M = Ge, Si; X = Cl, Br)2Unlocking Strong Second‐Harmonic Generation in Deep‐UV‐Transparent Polar Organic Sulfonates through Connectivity Regulation6Ba 3 S[SnOS 3 ] and [Ba 2 Sn]S[Ge 2 O 7 ]: two antiperovskite oxychalcogenides with good IR nonlinear optical performances2KCd(IO 3 ) 2 Cl: A New UV NLO Crystal with Balanced Optical Properties Engineering via Target‐Driven Multi‐Ion Substitution Strategy7A Homoatomic Heteroleptic Coordination Strategy for Exceptional Infrared Linear and Nonlinear Optical Properties in ANb 2 PS 4 (S 2 ) 3 (A = K,Rb,Cs)3Stable lead succinate-iodides with strong second-harmonic generation response and large birefringence0(C 6 H 7 N 2 O)NO 3 : π-Conjugation-Driven Synergistic Enhancement of Second-Harmonic Generation and Birefringence0Ba 4 CdGa 2 S 6 F 4 : A Chalcohalide Birefringent Crystal with Large Band Gap Designed by the Cation and Anion Cosubstitution Strategy2LiMn(IO 3 ) 3 : A Noncentrosymmetric Iodate Synthesized by Polyhedral Volume Ratio Modulation0Coordination-Mode-Modulated Symmetry Breaking for Nonlinear Optical Crystals0Λ‐Shaped Dimers Enables Polar Antiperovskites Through A‐Site Displacement Mechanism0

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  1. [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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  3. Synthesis, structural evolution and optical properties of a new family of oxychalcogenides [Sr 3 VO 4 ][MQ 3 ] (M = Ga, In, Q = S, Se)

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  4. Improved Polarization in the Sr6Cd2Sb6O7Se10 Oxyselenide through Design of Lateral Sublattices for Efficient Photoelectric Conversion

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  8. Oxychalcogenides as Promising Ultraviolet Nonlinear Optical Candidates: Experimental and Theoretical Studies of AEGeOS2(AE = Sr and Ba)

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  9. AeMg6Ga6S16 (Ae = Ca, Sr, Ba): The First Double Alkaline‐Earth Metal Chalcogenides with Excellent Performances

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  10. Rb 2 CdSi 4 S 10 : novel [Si 4 S 10 ] T2-supertetrahedra-contained infrared nonlinear optical material with large band gap

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  11. The Antiperovskite‐Type Oxychalcogenides Ae3Q[GeOQ3] (Ae = Ba, Sr; Q = S, Se) with Large Second Harmonic Generation Responses and Wide Band Gaps

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  13. Oxychalcogenides: A Promising Class of Materials for Nonlinear Optical Crystals with Mixed‐Anion Groups

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  14. [M(OH) 2 ] 3 (IO 3 )(SeO 4 )·H 2 O (M = Ga and In): metal iodate–selenate nonlinear optical materials with a hexagonal tungsten oxide-type topology

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  15. Honeycomb layered topology construction for exceptional long-wave infrared nonlinear optical crystals

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  29. Chiral and Polar Duality Design of Heteroanionic Compounds: Sr18Ge9O5S31 Based on [Sr3OGeS3]2+ and [Sr3SGeS3]2+ Groups

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  31. “Three‐in‐One”: A New Hg‐Based Selenide Hg 7 P 2 Se 12 Exhibiting Wide Infrared Transparency Range and Strong Nonlinear Optical Effect

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  32. Ba 2 GeF 2 Q 3 (Q = S, Se) and Ba 3 GeF 2 Se 4 : new F-based chalcohalides with enhanced birefringence

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  44. Assembly of π‐Conjugated [B 3 O 6 ] Units by Mer‐Isomer [YO 3 F 3 ] Octahedra to Design a UV Nonlinear Optical Material, Cs 2 YB 3 O 6 F 2

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  47. Ae3[TO3][SnOQ3] (Ae = Sr, Ba; T = Si, Ge; Q = S, Se) and Ba3[CO3][MQ4] (M = Ge, Sn; Q = S, Se): Design and Syntheses of a Series of Heteroanionic Antiperovskite-Type Oxychalcogenides

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  48. ACuGa 6 S 10 (A = Rb, Cs): Design and Synthesis of Two New Cavity‐Chalcopyrite Chalcogenides Based on “Iterative Substitution” Strategy

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  49. BaPb2(CO3)2F2: Enhancing Birefringence by a Multiunit Synergy Effect

    Inorganic Chemistry · 2024-12-02

    Yuan Hua Lin, Rongfang Zhang, Yucheng Hao, Ming-Yang Cao, Xuanlin Pan, Jiang‐Gao Mao

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  50. Balanced IR Nonlinear Optical Performance Achieved by Cation–Anion Module Cosubstitution in V-Based Salt-Inclusion Oxychalcogenides

    Chemistry of Materials · 2024-12-03

    Mao-Yin Ran, Sheng-Hua Zhou, Bingxuan Li, Xintao Wu, Hua Lin, Qi‐Long Zhu

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