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RESEARCH PAPER · Angewandte Chemie International Edition · 2020

Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )

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Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )OriginalAn organic–inorganic hybrid birefringent material with diverse functional groups38Deep-ultraviolet transparent alkali metal–rare earth metal sulfate NaY(SO 4 ) 2 ·H 2 O as a nonlinear optical crystal: synthesis and characterization28From Ce(IO 3 ) 4 to CeF 2 (IO 3 ) 2 : fluorinated homovalent substitution simultaneously enhances SHG response and bandgap for mid-infrared nonlinear optics26In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 219NaGaI 3 O 9 F: a new alkali metal gallium iodate combined with IO 3 − and IO 3 F 2− units16Synthesis, characterization and theoretical investigation of a new chalcohalide, Ba 4 GaS 4 F 311Finding Short-Wavelength Birefringent Crystals with Large Optical Anisotropy Activated by π-Conjugated [C(NH2)3] Units45Large Second-Harmonic Response and Giant Birefringence of CeF 2 (SO 4 ) Induced by Highly Polarizable Polyhedra248Second-order nonlinear optical property of the ultraviolet transparent alkali metal-rare earth metal carbonate Na3Y(CO3)3.3H2O5Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137UV 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 Phosphate28Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application167Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application18Be2(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 Response8[ o ‐C 5 H 4 NHOH] 2 [I 7 O 18 (OH)]⋅3 H 2 O: An Organic–Inorganic Hybrid SHG Material Featuring an [I 7 O 18 (OH)] Branched Polyiodate Chain86[o‐C5H4NHOH]2[I7O18(OH)]⋅3 H2O: An Organic–Inorganic Hybrid SHG Material Featuring an [I7O18(OH)] Branched Polyiodate Chain21Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals146Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals16A2MoO2F3(IO2F2) (A = Rb, Cs): Strong Nonlinear Optical Responses and Enlarged Band Gaps through Fluorine Incorporation50Mg 2 In 3 Si 2 P 7 : A Quaternary Diamond-like Phosphide Infrared Nonlinear Optical Material Derived from ZnGeP 2130Solvothermal Syntheses of Three-Dimensional Open-Framework Thioantimonates Displaying Nonlinear Optical Responses5A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation22A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation63Giant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo 2 O 8 F149A Photochromic Zinc–Viologen Framework with a High-Contrast Nonlinear Optical Switchable Behavior24Strong 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 New Nonlinear Optical Material with N(CN)2− Anion2Review of Anisotropic 2D Materials: Controlled Growth, Optical Anisotropy Modulation, and Photonic Applications168A new I 3 O 9 3− group constructed from IO 3 − and IO 5 5− anion units in Cs 3 [Ga 2 O(I 3 O 9 )(IO 3 ) 4 (HIO 3 )]4From CeF2(SO4)·H2O to Ce(IO3)2(SO4): Defluorinated Homovalent Substitution for Strong Second-Harmonic-Generation Effect and Sufficient Birefringence53CsCu 3 SbS 4 : rational design of a two-dimensional layered material with giant birefringence derived from Cu 3 SbS 442A 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 Transparency96Guanidinium Fluorooxoborates as Efficient Metal-free Short-Wavelength Nonlinear Optical Crystals140[C 3 N 6 H 7 ] 2 [B 3 O 3 F 4 (OH)]: a new hybrid birefringent crystal with strong optical anisotropy induced by mixed functional units85A novel 2-(aminomethyl)pyridineH 2 PO 4 crystal with second-order nonlinear optical performance8Ba 2 [WO 3 F(IO 3 )][WO 3 F 2 ]: the first polar fluorinated tungsten iodate featuring a direct W–O–I bond7Ba 4 Ag 5 (IO 3 ) 6 (I 3 O 8 ) 3 (I 4 O 11 ) 2 : a nonlinear optical crystal containing two types of polyiodate anions16Cd 2 (IO 3 )(PO 4 ) and Cd 1.62 Mg 0.38 (IO 3 )(PO 4 ): metal iodate-phosphates with large SHG responses and wide band gaps28CsB 3 O 4 (OH) 2 : a new deep-ultraviolet birefringent crystal with [B 3 O 4 (OH) 2 ] anionic group8Halogen regulation triggers structural transformation from centrosymmetric to noncentrosymmetric switches in tin phosphate halides Sn 2 PO 4 X (X = F, Cl)47KLi 2 CO 3 F: a beryllium-free KBBF-type deep-UV carbonate with an enhanced interlayer interaction and large birefringence20Mg(H 2 O) 6 [(IO 2 (OH)) 2 (IO 3 )] 2 : a new iodate with a very large band gap and optical anisotropy13Nain(C2o4)(Hpo4)(H2o)5: An Ultraviolet Transparent Nonlinear Optical Oxalate-Phosphate with Large Birefringence0Unprecedented boat-shaped [Mo 2 O 5 (IO 3 ) 4 ] 2− polyanions induced a strong second harmonic generation response31Wide bandgaps and strong SHG responses of hetero-oxyfluorides by dual-fluorination-directed bandgap engineering28Chiral Ligand‐Driven Systematic Synthesis of Coordination Polymers with Non‐centrosymmetric Structures12Potential optical functional crystals with large birefringence: Recent advances and future prospects322Advances in second-order nonlinear optical sulfates38Ultrawide 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 Material12LiB5O5F2(OH)4: A new deep-ultraviolet birefringent crystal with [B5O5F2(OH)4] anionic group28Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters9Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters139Additive‐Triggered Polar Polymorph Formation: β‐Sc(IO 3 ) 3 , a Promising Next‐Generation Mid‐Infrared Nonlinear Optical Material42Additive‐Triggered Polar Polymorph Formation: β‐Sc(IO3)3, a Promising Next‐Generation Mid‐Infrared Nonlinear Optical Material3An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals81An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals22A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses15A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses96(C3N6H7)2SbF5·H2O Exhibiting Strong Optical Anisotropy from the Optimal Arrangement of π-Conjugated (C3N6H7)+ Groups31Design of a new ultraviolet nonlinear optical material KNO3SO3NH3 exhibiting an unexpected strong second harmonic generation response44Dual-Ligand-Oriented Design of Noncentrosymmetric Complexes with Nonlinear-Optical Activity11NaK5Zn2(B5O10)2 and β-K3ZnB5O10: Two Zincoborates with Deep-UV Cutoff Edge9Isoreticular Design of KTiOPO 4 -Like Deep-Ultraviolet Transparent Materials Exhibiting Strong Second-Harmonic Generation68Finding a Deep‐UV Borate BaZnB4O8 with Edge‐sharing [BO4] Tetrahedra and Strong Optical Anisotropy20Achieving Large Second Harmonic Generation Effects via Optimal Planar Alignment of Triangular Units64AIB3IIC3IIIQ8VI: A New Family for the Design of Infrared Nonlinear Optical Materials by Coupling Octahedra and Tetrahedra Units152LiNaB6O9F2: A Promising UV NLO Crystal Having Fluorine‐Directed Optimal Performances and Double Interpenetrating 3[B6O9F2]∞ Networks33Enhanced Second-Harmonic-Generation Response in a KH2PO4-Type Calcium Nitrate Carboxylate with Unusual Three-Dimensional Inorganic and Organic Connections3(C 5 H 6.16 N 2 Cl 0.84 )(IO 2 Cl 2 ): a birefringent crystal featuring unprecedented (IO 2 Cl 2 ) − anions and π-conjugated organic cations56[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 topology20Ce 3 F 4 (SO 4 ) 4 : cationic framework assembly for designing polar nonlinear optical material through fluorination degree modulation23Dramatically improved optical anisotropy by realizing stereochemically active lone pairs in a sulfate system, K 2 SO 4 ·HIO 323KNa 2 La 2 (BO 3 ) 3 : a shortite-type lanthanide borate exhibiting strong nonlinear optical activity induced by isolated [BO 3 ] triangles and distorted [LaO 9 ] polyhedra26KRb 2 (NO 3 ) 2 Cl: a new birefringent crystal exhibiting a perovskite-related framework and a short cutoff edge6Linear π-conjugated units of the D ∞h point group as superior ultraviolet birefringent units1Recent advances on the synthesis of Sb(III)-based inorganic ultraviolet nonlinear optical materials47C(NH2)3(I3O8)(HI3O8)(H2I2O6)(HIO3)4·3H2O: An Unprecedented Asymmetric Guanidinium Polyiodate with a Strong Second-Harmonic-Generation Response and a Wide Band Gap16Two Carboxylate-Cyanurates with Strong Optical Anisotropy and Large Band Gaps6Recent advances of inorganic phosphates with UV/DUV cutoff edge and large second harmonic response7α-BBO-like π-Conjugated Crystal with Large Birefringence16Alignment of Λ-Shaped Basic Building Units to Construct One New KMoO3(IO3) Polar Polymorph11A Second‐Order Nonlinear Optical Material Consisting of Two π‐Conjugated Groups10Recent Development of Sn II , Sb III ‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence130Recent Development of SnII, SbIII‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence6Wide‐Bandgap Rare‐Earth Iodate Single Crystals for Superior X‐Ray Detection and Imaging21Stereochemically Active Tin(II)‐Induced Enhancement of Birefringence in SnIISnIV(PO4)2 and SrSn(PO4)PO2(OH)23A solution processible single-crystal porous organic polymer55A BBO-like trithiocyanate with significantly enhanced birefringence and second-harmonic generation39Two Ultraviolet Optical Crystals K6B12O19F4 and K12B28O48: The Effects of Metal Cations Size and the F Ions on the Structure6A Hydrogen Bonded Supramolecular Framework Birefringent Crystal89A Hydrogen Bonded Supramolecular Framework Birefringent Crystal13“Cation Activation”: An Effective Strategy for the Enhancement of Birefringence36Halogen Bonding Assembles Anion⋅⋅⋅Anion Architectures in Non‐centrosymmetric Iodate and Bromate Crystals24Ultraviolet Crystal with Strong Optical Nonlinearity by Creating Halogen-Centered Secondary Building Blocks15(NH 4 ) 2 (I 5 O 12 )(IO 3 ) and K 1.03 (NH 4 ) 0.97 (I 5 O 12 )(IO 3 ): Mixed‐Valent Polyiodates with Unprecedented I 5 O 12 − Unit Exhibiting Strong Second‐Harmonic Generation Responses and Giant Birefringence22Introduction of the [B–O/F] Units Enhances the Band Gap and Birefringence from Na6Mg3B10O18F6 to K3NaB10O16F211Quadruple‐Bidentate Nitrate‐Ligated A 2 Hg(NO 3 ) 4 (A=K, Rb): Strong Second‐Harmonic Generation and Sufficient Birefringence59Quadruple‐Bidentate Nitrate‐Ligated A 2 Hg(NO 3 ) 4 (A=K, Rb): Strong Second‐Harmonic Generation and Sufficient Birefringence2A survey of stereoactive oxysalts for linear and nonlinear optical applications40Ce(IO3)3F and Ce(IO3)2(NO3): Two Mixed-Anion Cerium Iodates with Good Nonlinear Optical and Birefringent Properties14Sr(NO 3 )(NH 2 SO 3 )·H 2 O: First Nitrate Sulfamate Revealing Remarkable Second Harmonic Generation and Optimized Birefringence25Stereochemically Active Lone-Pair Containing Metal Substitution in Polar Axis toward a Giant Phase-Matchable Optical Nonlinear Silicate Crystal Li 3 (OH)PbSiO 463A potassium lead 2-methylmalonate-iodide nonlinear optical crystal with strong second-harmonic generation response and large birefringence2Sr(NH2SO3)(NO3)·H2O: An Ultraviolet Nonlinear Optical Material Exhibiting Strong Second-Harmonic Generation Response and Sufficient Birefringence10A 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 Polycations25NaMoO 3 (IO 3 )(H 2 O): water molecule introduction induces strong second harmonic generation response, widened band gap and large anisotropy8A2Hgx(SeO3)y (A = K, Rb, Cs): Three Alkali Metal Mercury Selenites Featuring Unique 1D [HgOm(SeO3)n]∞ Chains13Rational Design of the Alkali Metal Sn‐Based Mixed Halides with Large Birefringence and Wide Transparent Range44Achieving great optical anisotropy with the well-directed alignment of π-conjugated groups due to hydrogen bonds9Secondary‐Bond‐Driven Construction of a Polar Material Exhibiting Strong Broad‐Spectrum Second‐Harmonic Generation and Large Birefringence9Secondary‐Bond‐Driven Construction of a Polar Material Exhibiting Strong Broad‐Spectrum Second‐Harmonic Generation and Large Birefringence41K(NH4)Zn2(PO4)2: a Beryllium-Free Sr2Be2B2O7 Derivative with Enhanced Interlayer Connectivity7[Sn 3 OF]PO 4 vs. [Sn 3 F 3 ]PO 4 : enhancing birefringence by breaking the R 3 symmetry and realigning lone pairs12Ba 2 Ga 2 F 6 (IO 3 )(PO 4 ): the first fluoride-containing iodate-phosphate with a 1D [Ga 2 F 6 (IO 3 )(PO 4 )] 4− helix chain2Exploration of antimony( iii ) oxyhalides via single-site substitution in quest of large birefringence10Fully tricoordinated assembly unveils a pioneering nonlinear optical crystal (SbTeO 3 )(NO 3 )25Large optical anisotropy in noncentrosymmetric phosphate with pseudo 2D intercalated layer16New ultraviolet transparent rare-earth borates with enhanced birefringence induced by cation chemical substitution15Reticular chemistry-aided effective design of new second-order nonlinear optical selenites11Synergistic combination of different types of functional motif in Rb(NO 3 )(SO 3 NH 3 ) for realizing excellent ultraviolet optical nonlinearity18Designing Optical Anisotropy: Silver-Aminoalkylpyridine Nitrate Complexes with Tunable Structures3Two Short-Wave UV Antimony(III) Sulfates Exhibiting Large Birefringence18Giant Optical Anisotropy in a Covalent Molybdenum Tellurite via Oxyanion Polymerization43C(NH2)3MoO3(IO3): A Molybdenyl Iodate with Giant Birefringence Designed via a Cation–Anion Synergetic Interaction Strategy36Li2B5O8Cl: A New Borate Chloride with Interpenetrating 3D B–O Frameworks Enriching Structural Chemistry of Borate0(C8H6BrN2O)NO3: A Hybrid Nonlinear Optical Crystal With an Appropriate Birefringence12Edge-Sharing Tetrahedra Realizing Superior Birefringence and High Deep-Ultraviolet Transmittance in α-Be3(H2O)2(PO4)2 Crystal Synthesized by Mild Chemistry14Na3K6(CO3)3(NO3)2X·6H2O (X = NO3, Cl, Br): Exploring High-Performance UV Birefringent Crystals Induced by Coplanar π-Conjugated CO3 and NO3 Groups15An Unprecedented [BO2]‐Based Deep‐Ultraviolet Transparent Nonlinear Optical Crystal by Superhalogen Substitution33An Unprecedented [BO2]‐Based Deep‐Ultraviolet Transparent Nonlinear Optical Crystal by Superhalogen Substitution1Tunable Optical Anisotropy in Rare‐Earth Borates with Flexible [BO3] Clusters7Assembly 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, Cs2YB3O6F297Second Harmonic Generation in β-K2TeW3O12: An Acentric Crystal Designed from Centric Phase via Pressure Modulation4Recent advances and future perspectives on rare-earth-based nonlinear optical materials with π-conjugated [XO3] (X = B, C, N) units66Bi(SO4)F·H2O and Bi(SO4)(NO3)·3H2O: Chemical Substitution-Induced Birefringence Enhancement in Bismuth Sulfates6Halogen Bond Unlocks Ultra‐High Birefringence73Halogen Bond Unlocks Ultra‐High Birefringence14A3Sc(SO4)3 (A = K, Rb, Cs): Three Deep‐Ultraviolet Transparent Alkali‐Scandium Sulfates with Strong Second‐Harmonic Generation Response and High Thermal Stability14NH4Y(SO4)2·H2O and NH4YSO4F2: Two New Ammonium‐Rare Earth Metal Sulfates with Enhanced Optical Anisotropy and Deep Ultraviolet Transmission3Breaking through the ‘‘200 nm deep-ultraviolet wall’’ of phase matching region by cation structural modulation27Cs2Pb(CO3)2: a novel mixed-metal carbonate with rare Pb-C-O one-dimensional chain0CdInO(BO3): An oxyborate birefringent material explored from d10 metal compounds1

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