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RESEARCH PAPER · Angewandte Chemie · 2019

CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure

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CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type StructureOriginalK9[B4O5(OH)4]3(CO3)X·7H2O (X = Cl, Br): Syntheses, Characterizations, and Theoretical Studies of Noncentrosymmetric Halogen Borate–Carbonates with Short UV Cutoff Edges16Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS229Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2186Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO 3 /BO 3 F Ratio in Layers99Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO3/BO3F Ratio in Layers24Synthesis, characterization and theoretical calculation of a noncentrosymmetric compound, Cs0.92B0.92Si5.08O122Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra73Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra18LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO398LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO337Histidinium‐Driven Chirality Control of Self‐Assembled Hybrid Molybdenum Oxyfluorides24Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework132CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework22Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials164Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials55Rational Design of the Metal‐Free KBe 2 BO 3 F 2 ⋅(KBBF) Family Member C(NH 2 ) 3 SO 3 F with Ultraviolet Optical Nonlinearity201Rational Design of the Metal‐Free KBe2BO3F2⋅(KBBF) Family Member C(NH2)3SO3F with Ultraviolet Optical Nonlinearity31Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials137Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials29K 2 Sb(P 2 O 7 )F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance297K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance38Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties165Pb18O8Cl15I5: A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties29Anionic Aliovalent Substitution from Structure Models of ZnS: Novel Defect Diamond‐like Halopnictide Infrared Nonlinear Optical Materials with Wide Band Gaps and Large SHG Effects78Anionic Aliovalent Substitution from Structure Models of ZnS: Novel Defect Diamond‐like Halopnictide Infrared Nonlinear Optical Materials with Wide Band Gaps and Large SHG Effects19Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups75Cs3Pb2(CH3COO)2X5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups22An Antimony(III) Fluoride Oxalate with Large Birefringence45Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”3Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”1Sb6O7(SO4)2: A Promising Ultraviolet Nonlinear Optical Material with an Enhanced Second‐Harmonic‐Generation Response Activated by SbIII Lone‐Pair Stereoactivity62Na 7 (IO 3 )(SO 4 ) 3 : the first noncentrosymmetric alkaline-metal iodate-sulfate with isolated [IO 3 ] and [SO 4 ] units28Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials24UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate196UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate28Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response130Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response8KCs2[Pb2Br5(HCOO)2]: A Polar 3D Lead‐Bromide Framework Exhibiting Strong Second‐Harmonic Generation Response10[Ag(NH 3 ) 2 ] 2 SO 4 : A Strategy for the Coordination of Cationic Moieties to Design Nonlinear Optical Materials**6[Ag(NH3)2]2SO4: A Strategy for the Coordination of Cationic Moieties to Design Nonlinear Optical Materials**85Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units102Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units9La 3 Ga 3 Ge 2 S 3 O 10 : An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering63La3Ga3Ge2S3O10: An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering18Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification89Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification9A Lead Mixed Halide with Three Different Coordinated Anions and Strong Second‐Harmonic Generation Response10A Lanthanum Ammonium Sulfate Double Salt with a Strong SHG Response and Wide Deep‐UV Transparency15A Lanthanum Ammonium Sulfate Double Salt with a Strong SHG Response and Wide Deep‐UV Transparency96Hierarchical Modulation of Optical Anisotropy Driven by Metal Cation Polyhedra in Fluorooxoborates MIIB4O6F2 (MII=Be, Mg, Pb, Zn, Cd)6KPb 3 ( o -C 5 H 4 NCOO) 2 Cl 5 : a brand-new stable lead chloride with good comprehensive nonlinear optical performance5High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence21High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence199Crystal Structure and Theoretical Analysis of Cs2Ca3(SO4)47Explorations of New SHG Materials in Mercury Iodate Sulfate System**9A Hybrid Halide Perovskite Birefringent Crystal14A Hybrid Halide Perovskite Birefringent Crystal149Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material51Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material12Quantum Sensing with Extreme Light24A hybrid halide lead-free pseudo-perovskite with large birefringence37An efficient calcium-based sorbent for flue gas dry-desulfurization: promotion roles of nitrogen oxide and oxygen23Enhancement of birefringence and refractive index dispersion optimization from iodates to fluorooxoiodates1The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO 3 ) 2 and Y 3 F(SeO 3 ) 485The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO3)2 and Y3F(SeO3)47Four New Sb‐based Orthophosphates: Cation Regulation to Investigate Diversified Structural Architecture1Nonlinear optical inorganic sulfates: The improvement of the phase matching ability driven by the structural modulation41Design, Synthesis, Crystal Structure, and Thermal Studies of Ni0.779SbF3(SO4): A New Electrode Material for Electrochemical Supercapacitors8The Birefringence Modulation in Short‐Wave Ultraviolet Sulfates with Functional π‐Conjugated Cations and Polymerized Heteroleptic Tetrahedral Anions18CdF(C 6 H 4 NO 2 )(H 2 O): a UV nonlinear optical material with unprecedented SHG and birefringence via π-conjugated rings and a unique “Warren truss structure”11M 3 MoO 4 (HCO 3 ) (M = Rb and Cs): cation-tuned synthesis of two noncentrosymmetric molybdate-carbonates with isolated [MoO 4 ] and [HCO 3 ] groups0Realizing large birefringence via S-substitution and anisotropic arrangement optimization4Hydrothermal Synthesis, Crystal Structure, and Thermal Studies of CuSb6O8(SO4)2 and Its Applications toward Dye Management, Hydrogen Evolution Reaction, and Antibacterial Studies2All-three-in-one: Pb2(H2PO4)2(C2O4) significantly enhanced birefringence in phosphate materials4Thermal Evolution and Crystal Structure Features of Cs2SO4 and Cs2Ca3(SO4)4 Sulfates2[Ga(C 2 H 6 OS) 6 ](SbBr 6 ): A Highly Luminescent Organic–Inorganic Hybrid Bimetallic Bromide Synthesized via a Cation Hybridization Strategy8Designing High-Performance Short-Wave UV Tellurium-Based Mixed Halides Birefringent Crystals via Halogen Substitution Engineering4Non-centrosymmetric ZnSO4·Zn(OH)2: synthesis, crystal structure, and its applications towards photocatalytic methylene blue degradation and solvent-free Knoevenagel condensation reaction1pH‐Regulated Ring‐Opening/Closing Transformation in Polyoxometalates Enables High‐Performance Nonlinear Optical Crystals1Tailoring ordered structures with distorted [TeO 3 ] and aligned [ScO 6 ] motifs for balanced nonlinear optical properties in rare-earth tellurate crystals5A dobrovolskyite-type Na4Ca(SO4)3 sulfate: structural phase transition, thermal expansion and ionic conductivity0Strain-engineered indirect-to-direct band gap transition, photocatalytic water splitting activity, and optical responses in ACuGa 6 S 10 (A = Rb and Cs)0Cation‐Dominated Second‐Order Nonlinear Optical Response Enabled by π‐Conjugated Guanidinium Derivatives0Lateral‐Site Unblocking Enables Bilateral π ‐Chromophore Organization for Giant Birefringence in One‐Dimensional Lead Hybrids0Rational Construction of Fluoride Crystals With Record Birefringence via Water‐Regulated Hydrogen‐Bond Network Reconfiguration0

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  2. Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2

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  3. Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2

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  4. Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO 3 /BO 3 F Ratio in Layers

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  5. Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO3/BO3F Ratio in Layers

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  6. Synthesis, characterization and theoretical calculation of a noncentrosymmetric compound, Cs0.92B0.92Si5.08O12

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  7. Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra

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  9. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  10. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  11. Histidinium‐Driven Chirality Control of Self‐Assembled Hybrid Molybdenum Oxyfluorides

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  12. Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect

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  13. CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework

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  14. CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework

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  15. Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)3

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  16. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

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  17. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

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  18. Rational Design of the Metal‐Free KBe 2 BO 3 F 2 ⋅(KBBF) Family Member C(NH 2 ) 3 SO 3 F with Ultraviolet Optical Nonlinearity

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  19. Rational Design of the Metal‐Free KBe2BO3F2⋅(KBBF) Family Member C(NH2)3SO3F with Ultraviolet Optical Nonlinearity

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  20. Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials

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  22. K 2 Sb(P 2 O 7 )F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance

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  30. An Antimony(III) Fluoride Oxalate with Large Birefringence

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  31. Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”

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  32. Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”

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  33. Sb6O7(SO4)2: A Promising Ultraviolet Nonlinear Optical Material with an Enhanced Second‐Harmonic‐Generation Response Activated by SbIII Lone‐Pair Stereoactivity

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  34. Na 7 (IO 3 )(SO 4 ) 3 : the first noncentrosymmetric alkaline-metal iodate-sulfate with isolated [IO 3 ] and [SO 4 ] units

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  35. Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials

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  36. UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate

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  37. UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate

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  38. Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response

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  39. Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response

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  41. [Ag(NH 3 ) 2 ] 2 SO 4 : A Strategy for the Coordination of Cationic Moieties to Design Nonlinear Optical Materials**

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  43. Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units

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  44. Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units

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  45. La 3 Ga 3 Ge 2 S 3 O 10 : An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering

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  46. La3Ga3Ge2S3O10: An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering

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  47. Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification

    Angewandte Chemie International Edition · 2021-10-11

    Chao Wu, Xingxing Jiang, Lin Lin, Wenyan Dan, Zheshuai Lin, Zhipeng Huang, Mark Graeme Humphrey, Chi Zhang

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  48. Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification

    Angewandte Chemie · 2021-10-11

    Chao Wu, Xingxing Jiang, Lin Lin, Wenyan Dan, Zheshuai Lin, Zhipeng Huang, Mark Graeme Humphrey, Chi Zhang

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  49. A Lead Mixed Halide with Three Different Coordinated Anions and Strong Second‐Harmonic Generation Response

    Chemistry - A European Journal · 2021-10-15

    Qirui Shui, Ruibiao Fu, Ziqi Zhou, Zuju Ma, Hong‐Xin Tang, Xin‐Tao Wu

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  50. A Lanthanum Ammonium Sulfate Double Salt with a Strong SHG Response and Wide Deep‐UV Transparency

    Angewandte Chemie · 2021-12-11

    Chao Wu, Xingxing Jiang, Yilei Hu, Chunbo Jiang, Tianhui Wu, Zheshuai Lin, Zhipeng Huang, Mark Graeme Humphrey, Chi Zhang

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