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RESEARCH PAPER · Angewandte Chemie International Edition · 2022

Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2

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Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2Original(N 2 H 6 )[HPO 3 F] 2 : maximizing the optical anisotropy of deep-ultraviolet fluorophosphates33[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 units855d → 4f transition of a lanthanide-activated MGa 2 S 4 (M = Ca, Sr) semiconductor for mechanical-to-light energy conversion mediated by structural distortion12Ba 2 Zn 2 B 6 O 13 : coplanar [B 2 O 5 ] in unnoted U-shaped [B 6 O 13 ] groups achieving large birefringence6Na 3 YB 8 O 15 : a new rare-earth borate with an infinite one-dimensional [B 8 O 15 ] ∞ chain and a short ultraviolet cutoff edge8Performance of optical materials with the derivative of planar π-conjugated groups: Recent advances and future prospects36Sn 9O 4Br 9X (X = Cl, Br): Two New Sn(II) Oxyhalides Exhibiting Large Birefringence Derived from Highly Distortive Polyhedra of Lone Pair Cations0Synergistic effect of 2 [V 2 P 2 O 14 ] ∞ layers and hydrogen bonds inducing large birefringence in M(VO) 2 (PO 4 ) 2 ·4H 2 O (M = Ca, Sr, Ba) systems4Graphical Abstract: Angew. Chem. Int. Ed. 21/20220Organic–Inorganic Hybrid Noncentrosymmetric (Morpholinium) 2 Cd 2 Cl 6 Single Crystals: Synthesis, Nonlinear Optical Properties, and Stability43RbBiP2S6: A Promising IR Nonlinear Optical Material with a Giant Second-Harmonic Generation Response Designed by Aliovalent Substitution80Three Co-based tartratoborates with fundamental building blocks [B(C4H2O6)2]5− from facile condensation reactions2Fluorescent Zn(II)-Based Metal-Organic Framework: Interaction with Organic Solvents and CO2 and Methane Capture11From CsKTaF7 to CsNaTaF7: Alkali Metal Cations Regulation to Generate SHG Activity**22Two Metal Phosphate Nonlinear Optical Materials Simultaneously Exhibiting Ultraviolet Transparence and a Large Birefringence49Difluoro(oxalato)borates as Short-Wavelength Optical Crystals with Bifunctional [BF 2 C 2 O 4 ] Units37Rearrangement of [B2O5] Dimers within [B7O14] Clusters Enables Enhanced Optical Anisotropy in Li3Cs6Al2B14O28F4New Low-Dimensional Lead-Free Perovskite (2-AMP)2BiX7·H2O (X = Cl, Br) Crystals: Synthesis, Stability, and Nonlinear Optical Properties27Study of the Crystalline Perfection, Homogeneity, Chemical Etching on the Surface, and Third‐Order Nonlinear Optical Properties of (1 1 0) Oriented Hydroxyethylammonium D‐Tartrate Monohydrate Single Crystal and Hirshfeld Surface Analysis10Design of a new ultraviolet nonlinear optical material KNO3SO3NH3 exhibiting an unexpected strong second harmonic generation response44PbBi(SeO 3 ) 2 F and Pb 2 Bi(SeO 3 ) 2 Cl 3 : Coexistence of Three Kinds of Stereochemically Active Lone-Pair Cations Exhibiting Excellent Nonlinear Optical Properties57Ag4SnGe2S7: A Noncentrosymmetric Chalcogenide in I4–II–IV2–VI7 System with Non-Diamond-Like Structure Featuring 1D ∞[SnGe2S8]6– Infinite Chain2Ternary AGa5S8 (A = K, Rb, Cs): Promising infrared nonlinear optical materials rationally realized by “one-for-multiple substitution” strategy37(C4H10NO)PbX3 (X = Cl, Br): Design of Two Lead Halide Perovskite Crystals with Moderate Nonlinear Optical Properties35NaK5Zn2(B5O10)2 and β-K3ZnB5O10: Two Zincoborates with Deep-UV Cutoff Edge9Novel structural transformation in K3ReP2S8 thiophosphates originating from the rare-earth (Re) cation sizes induced local coordination asymmetry25SbHPO3F: 2D van der Waals Layered Phosphite Exhibiting Large Birefringence32Sn3B10O17Cl2 Achieving Birefringence Enhancement by Stereochemical Activity Lone Pair9Li2PbB2O5: A Pyroborate with Large Birefringence Induced by the Synergistic Effect of Stereochemical Active Lone Pair Cations and π-Conjugated [B2O5] Groups14In Situ Kinetic Observations on Crystal Nucleation and Growth386Emerging Chalcohalide Materials for Energy Applications164Explorations of Second-Order Nonlinear Optical Materials in the Monovalent Trithiocyanurate System18Na 2 (C 4 O 4 )(H 3 BO 3 )(H 2 O) 4 ·H 3 BO 3 : the first borate-squarate with strong SHG response obtained by superior synergy11LiNaB6O9F2: A Promising UV NLO Crystal Having Fluorine‐Directed Optimal Performances and Double Interpenetrating 3[B6O9F2]∞ Networks33LiKCuP2O7: Cation substitution application with mixed-alkaline copper-containing pyrophosphate and magnetic properties2Rb 3 B 5 O 8 F 2 and K 0.6 Rb 2.4 B 5 O 8 F 2 : two new deep-ultraviolet transparent nonlinear optical fluorooxoborates designed by cation regulation13Noncentrosymmetric versus Centrosymmetric: Halogen Induced Variable Coordination Modes of Sn2+ and Structural Transition in Sn3B3O7X (X = Cl and Br)17A new polar alkaline earth–rare earth iodate: Ba 2 Ce(IO 3 ) 8 (H 2 O)10Accurate design and synthesis of nonlinear optical crystals employing KBe2BO3F2 as structural template55Achieving broadband ultraviolet to mid-infrared transparency in germanate-based nonlinear optical crystals Cs 3 REGe 3 O 9 (RE = Y, Gd)16Ba 3 (BS 3 )(PS 4 ): the first alkaline-earth metal thioborate–thiophosphate with strong optical anisotropy originating from planar [BS 3 ] units8Cs[B 3 O 3 F 2 (OH) 2 ]: discovery of a hydroxyfluorooxoborate guided by selective organic–inorganic transformation12Discovery of SrZn 2 B 6 O 12 with an unprecedented quadruple-layered configuration0Enhancement of birefringence and refractive index dispersion optimization from iodates to fluorooxoiodates1Enhancing birefringence of non-π-conjugated sulfate systems through rare-earth metal-centered polyhedra10High stability and moderate second-order nonlinear optical properties of hybrid lead-free perovskite [(CH 3 ) 3 NCH 2 Cl]CdCl 3 bulk crystals12K 5 [B 3 O 3 F 4 (OH)] 2 (NO 3 ): the first hydroxyfluorooxoborate-nitrate with a short ultraviolet cutoff edge and large birefringence17KRb 2 (NO 3 ) 2 Cl: a new birefringent crystal exhibiting a perovskite-related framework and a short cutoff edge6Liasi2o5 (a = K, Rb): Effects of Cations on Crystal Structure and Optical Properties0LiCs 3 AlB 7 O 14 : achieving enhanced optical anisotropy via [AlO 4 ] tetrahedron introduction to rearrange the anionic framework5Mg 2 Pb 2 Si 2 O 7 F 2 : a new lead-containing alkali earth metal silicate fluoride with a short cutoff edge2Modulating optical performance by phase transition in a nonlinear optical material β-Li 2 RbBi(PO 4 ) 28Recent advances in F-containing iodate nonlinear optical materials6Recent progress on sulfide infrared nonlinear optical materials with large SHG response and wide band gap26Synthesis of chiral high-entropy sulfides for non-linear optical applications13Two Noncentrosymmetric Alkali Metal Phosphates Mznpo4 (M = Rb, Cs) with Honeycomb-Like Structures0BaB2P2O8F2: A Fluoroborophosphate with [B2P2O8F2]∞ Layers and Deep-Ultraviolet Cutoff Edge4Organic Kainate Single Crystals for Second-Harmonic and Broadband THz Generation25Controlling the Nonlinear Optical Behavior and Structural Transformation with A‐Site Cation in α‐AZnPO4 (A = Li, K)20Recent advances of inorganic phosphates with UV/DUV cutoff edge and large second harmonic response7Li3B8O13X (X = Cl and Br): Two New Noncentrosymmetric Crystals with Large Birefringence Induced by BO3 Units18First theoretical framework of superalkali metals [M3X(M = Li, Na, k; X = O, S, F, N)] doped all-boron B38 nanocluster: A promising class of nonlinear optical materials for optoelectronic applications34Recent Development of Sn II , Sb III ‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence129Recent Development of SnII, SbIII‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence6Two Mixed-Alkali-Metal Selenates as Short-Wave Ultraviolet Nonlinear-Optical Materials10Na2BaB12O18F4: A Mixed Alkali/Alkaline-Earth Metal Fluorooxoborate with Two Unprecedented Interpenetrating Three-Dimensional B–O/F Anionic Networks and a Short Ultraviolet Cutoff Edge9Sn9O4Br9X (X = Cl, Br): Two new Sn(II) oxyhalides exhibiting large birefringence derived from highly distortive polyhedra of lone pair cations9Design, synthesis and characterization of a novel oxygen-containing heterocycle crystal with NLO properties5Remarkable phase-matchable second-harmonic generation realized by strong polarities of [PbSe3] and [GaSe4] functional motifs in PbGa4Se718Synthesis and Crystal Structure of the Zinc Borate Zn3B4O96A Polar Tetragonal Tungsten Bronze with Colossal Second‐Harmonic Generation18The Electronic Properties of Cadmium Naphthalene Diimide Coordination Complex8Stereochemically Active Tin(II)‐Induced Enhancement of Birefringence in SnIISnIV(PO4)2 and SrSn(PO4)PO2(OH)23Theoretical Prediction‐Assisted Synthesis and Characterization of Infrared Nonlinear Optical Material NaSrBS324Na3SiS3F: 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 Stability40Target-Oriented Synthesis of Borate Derivatives Featuring Isolated [B3O3] Six-Membered Rings as Structural Features20The new non‐centrosymmetric zinc borate Zn2B10O17 with a unique crystal structure5Achieving the full-wavelength phase-matching for efficient nonlinear optical frequency conversion in C(NH2)3BF4515Design Principles for Noncentrosymmetric Materials23Ultraviolet Crystal with Strong Optical Nonlinearity by Creating Halogen-Centered Secondary Building Blocks15Cs4Zn5P6S18I2: the Largest Birefringence in Chalcohalide Achieved by Highly Polarizable Nonlinear Optical Functional Motifs21Physicochemical and Nonlinear Optical Properties of a Stilbazolium Family Single Crystal with Third Order Nonlinear Optical Activity6Tuning nonlinear optical properties of tetracyclopentatetraphenylnene by superhalogens doping: Quantum chemical perspective of novel NLO materials for modern optoelectronic applications14Heterologous Isomorphic Substitution Induces Optical Property Enhancement for Deep-UV Crystals: a Case in Rb[B3O3F2(OH)2]9Enhanced ammonia gas sensing by cost-effective SnO2 gas sensor: Influence of effective Mo doping39LiGa(IO3)4: An Excellent NLO Material with Unprecedented 2D [Ga(IO3)4]∞− Layer Synthesized by Aliovalent Substitution20A Non‐π‐Conjugated Molecular Crystal with Balanced Second‐Harmonic Generation, Bandgap, and Birefringence10Mixed Anionic Tetrahedra Guided Design of New Infrared Nonlinear Optical Material Cs 3 Ga 8 S 13 Cl with High Laser‐Induced Damage Threshold26Insight into (Z)-ethyl-2-(2-((E)-2,4-dinitro benzylidene amino)-4-oxo-3-phenylthiazolidin-5-ylidene) acetate in-silico anti-SARS-CoV-2 performance: Synthesis, structural-spectral characterizations and DFT computations8Synthesis and crystal structure of the non-centrosymmetric zinc borate Zn10.4B6.2O21H2.61Tailored Synthesis of Two Metal Borates KSrM3B2O9 (M = Al and Ga) Exhibiting Wide Ultraviolet Transparency4Breaking the Inherent Interarrangement of [B3O6] Clusters for Nonlinear Optics with Orbital Hybridization Enhancement143Theoretical study of static and frequency-dependent nonlinear optical properties of 1-phenyl-2,5-di(thiophen-2-yl)-1H-pyrrole based D-π-A chromophores through π-linkers modifications: A gateway towards giant nonlinear optical compounds16Ba 4 B 14 O 25 : A Deep Ultraviolet Transparent Nonlinear Optical Crystal with Strong Second Harmonic Generation Response Achieved by a Boron‐Rich Closed‐Loop Strategy12Hydroxyl-Driven Enhanced Birefringence in Borophosphates3A 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 Polycations24PbTeB 4 O 9 : a lead tellurium borate with unprecedented fundamental building block [B 4 O 10 ] and large birefringence12Two noncentrosymmetric alkali metal phosphates MZnPO4 (M = Rb, Cs) with honeycomb-like structures8Chiral and Polar Duality Design of Heteroanionic Compounds: Sr18Ge9O5S31 Based on [Sr3OGeS3]2+ and [Sr3SGeS3]2+ Groups20Advances in Solid-State Nonlinear Optical Materials: From Fundamentals to Applications61Multifunctional Chiral d 10 ‐Metal Coordination Polymers: Tunable Photoluminescence and Efficient Second‐Harmonic Generation with Circular Dichroic Response18Temperature-Induced Reversible Photoluminescence Switching and Ultraviolet-Pumped Light-Emitting Diode Applications of a Perovskite (C6H10N2)2MnCl6·2H2O Crystal26Secondary‐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 Connectivity7A bifunctional primitive strategy induces enhancements of large second harmonic generation and wide UV transmittance in rare-earth borates containing [B 5 O 10 ] groups21A nonlinear optical crystal with deep-ultraviolet transparency and appropriate birefringence achieved using π-conjugated confined [B 3 O 3 F 4 (OH)] 2−14A-site cation manipulation of exemplary second harmonic generation response and optical anisotropy in rare-earth borates18Ca 3 Al 2 B 8 O 18 : borate with a graphene-like layer featuring two types of topological six-membered rings induced by [AlO 4 ] units7Designing excellent UV birefringent materials through the synergistic interaction of two highly distorted functional groups23Discovery of a new bimetallic borate with strong optical anisotropy activated by π-conjugated [B 2 O 5 ] units3Discovery of excellent ultraviolet nonlinear optical materials in chlorates and bromates with highly stereochemically active lone pairs12From 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 Iodates13Halide-driven polarity tuning and optimized SHG-bandgap balance in (C 4 H 11 N 2 )ZnX 3 (X = Cl, Br, I)34Hydrogen bonding bolstered head-to-tail ligation of functional chromophores in a 0D SbF 3 ·glycine adduct for a short-wave ultraviolet nonlinear optical material32K 2 MgMoP 2 O 10 and K 3 Mg 2 MoP 3 O 14 : two new molybdophosphates exhibiting different optical anisotropies induced by variable dimensionality of the anion framework4Nh4ca[B5o7(Oh)4]·H2o: A Biaxial Mixed-Cation Pentaborate with Moderate Birefringence0Novel antimony phosphates with enlarged birefringence induced by lone pair cations4Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Research progress in optical materials with cationic organic planar π-conjugated groups containing CN bonds34Simple aliovalent cation substitution to induce strong optical anisotropy enhancement in a rare thioantimonate( v ) family3Syntheses, structures and characterization of noncentrosymmetric MZnPO 4 (M = K, NH 4 )4LiASi2O5 (A = K, Rb): Effects of cations on crystal structure and optical properties1Synthesis, crystal structure and luminescent properties of a quinary borate-phosphate compound CsNa2Dy2(BO3)(PO4)21One-Dimensional and Two-Dimensional Zn(II) Coordination Polymers with Ditopic Imidazo[1,5-a]pyridine: A Structural and Computational Study6Design of deep-ultraviolet zero-order waveplate materials using LiB3O5 as the template8Ultra-Broad-Band-Excitable Cu-Based Halide (C4H10N)4Cu4I8 with High Stability for LED Applications23Toward the ultraviolet (UV) or deep-UV nonlinear optical crystals: The combination of π-conjugated planar [XY3] and tetrahedral [XY4]80Guanidinium Vanadate [C(NH2)3]3VO4·2H2O Revealing Enhanced Second-Harmonic Generation and Wide Band Gaps13AYSO4F2 (A = K, Rb): [YO4F4] Polyhedra Enhancement of Birefringence in Non-π-Conjugated Sulfate Systems9Polysubstitution Induced Centrosymmetric-to-Noncentrosymmetric Structural Transformation and Nonlinear-Optical Behavior: The Case of Na0.45Ag0.55Ga3Se52Na3K6(CO3)3(NO3)2X·6H2O (X = NO3, Cl, Br): Exploring High-Performance UV Birefringent Crystals Induced by Coplanar π-Conjugated CO3 and NO3 Groups15Zn(C6H4NO2)2·4H2O: A Solar-Blind Birefringent Crystal5Structure‐Prediction‐Oriented Synthesis of Thiophosphates as Promising Infrared Nonlinear Optical Materials24Structure‐Prediction‐Oriented Synthesis of Thiophosphates as Promising Infrared Nonlinear Optical Materials1Breaking Boundaries: Giant Ultraviolet Birefringence in Dimension‐Reduced Zn‐Based Crystals66Breaking Boundaries: Giant Ultraviolet Birefringence in Dimension‐Reduced Zn‐Based Crystals8Gradual Increase in Birefringence of Antimony Oxalates through Precise Tuning of the Sb3+/[C2O4]2– Ratio6Unraveling Superior Elasticity and Controlled Thermal Expansion in Trigonal MBO3 (M=Al, Ga) with Isolated [BO3] Group: A Theoretical Perspective9A Rare-Earth-Based Borate Optical Crystal with Enlarged Dihedral Angles of Distinct [BO3] Groups Exhibiting a Wide UV Transparent Range8(C5H12N2S)Hg(NO3)2: A Mercury Nitrate Nonlinear Optical Crystal Motivated by Heteroatom Coordination Strategy9Investigations of structure, thermal stability and optical properties of a new NLO crystal (C3H5N2)+(CF3COO)-0Constructing Ultraviolet Nonlinear Optical Crystals with Superior Thermal Stability Based on Organic π-Conjugated [HCOO] Groups6A2Cd(PO3)4 (A = K, Rb, Cs): Series of cadmium polyphosphates with infinite 1[(PO3)4]ꝏ chains and deep ultraviolet transparency windows2Li2NaB3S2O12: A Deep-UV Transparent Borosulfate with Moderate Birefringence Derived from the [B3S2O12]∞ Infinite Chain Designed by the High Boron-to-Sulfur Ratio Strategy6NH 4 Ca[B 5 O 7 (OH) 4 ] H 2 O: A Biaxial Mixed‐Cation Pentaborate with Moderate Birefringence0Oxygen Vacancies and Lattice Distortion Synergistically Enhanced Piezocatalysis of CaZn 2 (BO 3 ) 2 for Nonantibiotic Pharmaceutical Degradation27Amino substitution strategy achieves significant blue shift while preserving high optical anisotropy: A2(H3C3N4S2)2•H2O (A =NH4, K, Rb, Cs)6Unveiling Noncentrosymmetric Pyridine Carboxylates from Centrosymmetric Templates through Motif Configuration Modulation in Zero-Dimensional System7

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