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RESEARCH PAPER · Angewandte Chemie International Edition · 2020

Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra

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Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing TetrahedraOriginalOptimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42Second-order nonlinear optical materials with a benzene-like conjugated π system49Similarities and differences between Mn( ii ) and Zn( ii ) coordination polymers supported by porphyrin-based ligands: synthesis, structures and nonlinear optical properties24Sr5[BO2(OH)]3(OH)3F: First hydroxyborate fluoride with the [BO2(OH)]2− unit2The nonlinear optics property of heterodinuclear (Li and Na) sexipyridine helix: A density functional theory study3Cs 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 Groups22Chiral Template‐Driven Macroscopic Chirality Control: Structure‐Second‐Harmonic Generation Properties Relationship24Centrosymmetric RbSnF 2 NO 3 vs. noncentrosymmetric Rb 2 SbF 3 (NO 3 ) 254Homochiral three-dimensional noncentrosymmetric lanthanide coordination polymers directed by chiral linkers: syntheses, crystal structures, and optical properties8In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 219Systematic centricity control using a chiral template: novel noncentrosymmetric polar niobium oxyfluorides and tantalum fluorides directed by chiral histidinium cations, [( l -hisH 2 )NbOF 5 ], [( d -hisH 2 )NbOF 5 ], [( l -hisH 2 )TaF 7 ], and [( d -hisH 2 )TaF 7 ]8The Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal0To improve the key properties of nonlinear optical crystals assembled with tetrahedral functional building units46Zn(NH 3 )CO 3 : a “three-in-one” UV nonlinear optical crystal built by a polar molecule bonding strategy18Large Second-Harmonic Response and Giant Birefringence of CeF 2 (SO 4 ) Induced by Highly Polarizable Polyhedra248Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance43Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance6Borosilicate Crystal LaBSiO5: A New Promising Ultraviolet Quasiphase Matching Material31Two Lead Halides with Strong SHG Response Obtained by the Isovalent Substitutions of Alkali Metal Cation and Halogen Anion22Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137Cyanurates consisting of intrinsic planar π-conjugated 6-membered rings: An emerging source of optical functional materials111Discovery 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 Application18α-Ca2CdP2 and β-Ca2CdP2: Two Polymorphic Phosphide-Based Infrared Nonlinear Crystals with Distorted NLO-Active Tetrahedral Motifs Realizing Large Second Harmonic Generation Effects and Suitable Band Gaps30High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies323Hydrogen‐Bond‐Driven Synergistically Enhanced Hyperpolarizability: Chiral Coordination Polymers with Nonpolar Structures Exhibiting Unusually Strong Second‐Harmonic Generation87Hydrogen‐Bond‐Driven Synergistically Enhanced Hyperpolarizability: Chiral Coordination Polymers with Nonpolar Structures Exhibiting Unusually Strong Second‐Harmonic Generation19Insights into varying dimension structures for deep-UV optical crystals NaBa2Al(P2O7)2 and NaBaAl(PO4)2 constructed separately from unique [Al(P2O7)2] chains and [Al(PO4)2] layers6A 3D supramolecular framework assembled via π⋅⋅⋅π interactions and CH⋅⋅⋅Cl hydrogen-bonds with second-harmonic generation response2Li 4 MgGe 2 S 7 : The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap213Li4MgGe2S7: The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap15Heterobimetallic Cluster‐Based Coordination Polymers: Assembly, Structures and Third‐Order Nonlinear Optical Properties4Strong 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 Response10Syntheses, Structures and Properties of Alkali and Alkaline Earth Metal Diamond-Like Compounds Li2MgMSe4 (M = Ge, Sn)12Designing A New Infrared Nonlinear Optical Material, β‐BaGa 2 Se 4 Inspired by the Phase Transition of the BaB 2 O 4 (BBO) Crystal75Designing A New Infrared Nonlinear Optical Material, β‐BaGa2Se4 Inspired by the Phase Transition of the BaB2O4 (BBO) Crystal13NaSb3O2(SO4)3·H2O: A New Alkali-Metal Antimony(III) Sulfate with a Unique Sb6O20H4 Unit and Moderate Birefringence19Pushing KTiOPO4-like Nonlinear Optical Sulfates into the Deep-Ultraviolet Spectral Region19A 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 Transparency96AZn 2 (BO 3 )Si 2 O 5 (A = Rb, Cs): first examples of KBe 2 BO 3 F 2 structure type in the borosilicate family exhibiting a deep-ultraviolet cutoff edge25KCs2Pb2(HCOO)2Cl5: A Lead Formate with Strong Second-Harmonic-Generation Response Obtained by an Anionic Substitution3Recent Development of Non-π-Conjugated Deep Ultraviolet Nonlinear Optical Materials106KPb 3 ( o -C 5 H 4 NCOO) 2 Cl 5 : a brand-new stable lead chloride with good comprehensive nonlinear optical performance5Na 4 Ga 8 S 14 : a Ga-enriched wide band gap ternary alkali-metal sulfide with unique [Ga 12 S 42 ] 12-membered rings2Wide bandgaps and strong SHG responses of hetero-oxyfluorides by dual-fluorination-directed bandgap engineering28Chiral Ligand‐Driven Systematic Synthesis of Coordination Polymers with Non‐centrosymmetric Structures12MM′B3O4F3 (M = K; M′ = Na, K, Cs): Alkali-Metal Fluorooxoborates with ∞1[B3O4F3] Chains and Deep-Ultraviolet Cutoff Edges12“Removing Center”─An Effective Structure Design Strategy for Nonlinear Optical Crystals37Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra9Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra84Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)212Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2212Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal9SrZnGeS 4 : A Dual‐Waveband Nonlinear Optical Material with a Transparency Spanning UV/Vis and Far‐IR Spectral Regions88SrZnGeS4: A Dual‐Waveband Nonlinear Optical Material with a Transparency Spanning UV/Vis and Far‐IR Spectral Regions12The Kurtz-Perry powder technique revisited: A case study on the importance of reference quality and broadband nonlinear optical measurements using LiInSe232Pressure-stabilized hexagonal perovskite-related isolated tetrahedral anion silicate La6Sr3Si6O2415Tunable Fe-deficiency modified sodium ferric silicate for improving photo-Fenton-like activity22Synthesis, characterization and theoretical calculations of four chiral schiff base materials for second harmonic generation applications7Pb5(GeO4)(Ge2O7) and Pb3.32Ca1.68(GeO4)(Ge2O7): Two Nonlinear Optical Germanates Induced by Diverse PbOx Polyhedra17Novel structural transformation in K3ReP2S8 thiophosphates originating from the rare-earth (Re) cation sizes induced local coordination asymmetry25Decentering the Symmetry via Docking B and F in the KBe2BO3F2-Family Structure0AIB3IIC3IIIQ8VI: A New Family for the Design of Infrared Nonlinear Optical Materials by Coupling Octahedra and Tetrahedra Units152Rb 2 CdSi 4 S 10 : novel [Si 4 S 10 ] T2-supertetrahedra-contained infrared nonlinear optical material with large band gap79LiRE(SO 4 ) 2 (RE = Y, Gd, Eu): noncentrosymmetric chiral rare-earth sulfates with very large band gaps21Ba5Ga2SiO4S6: a Phase-Matching Nonlinear Optical Oxychalcogenide Design via Structural Regulation Originated from Heteroanion Introduction25Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181Enhancing birefringence of non-π-conjugated sulfate systems through rare-earth metal-centered polyhedra10Hydroxyfluorooxoborate (NH 4 )[C(NH 2 ) 3 ][B 3 O 3 F 4 (OH)] for exploring the effects of cation substitution on structure and optical properties26Low temperature molten salt synthesis of noncentrosymmetric (NH 4 ) 3 SbF 3 (NO 3 ) 3 and centrosymmetric (NH 4 ) 3 SbF 4 (NO 3 ) 234Modulating optical performance by phase transition in a nonlinear optical material β-Li 2 RbBi(PO 4 ) 28Recent progress in borate-based short-wavelength nonlinear optical crystals with boron–oxygen skeleton modification28Tetrahedron-based deep-ultraviolet nonlinear optical crystal with optimized KBe 2 BO 3 F 2 -like structure and disordered cations2Toward Large Second-Harmonic Generation and Deep-UV Transparency in Strongly Electropositive Transition Metal Sulfates112A Rare‐Earth Selenite with Unexpectedly Well‐Balanced Ultraviolet Nonlinear Optical Functionality, Sc(HSeO 3 ) 331Enhancing Third-Order Nonlinear Optical Property by Regulating Interaction between Zr4(embonate)6 Cage and N, N-Chelated Transition-Metal Cation6Chain‐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 Materials5Nonlinear optical crystals KPb3(3-C5H4NCOO)2Br5 and KPb3(3-C5H4NCOO)2Cl3Br2 with new Pb-centered nitrogen-halide polyhedrons obtained by the halide anionic substitution4Four New Sb‐based Orthophosphates: Cation Regulation to Investigate Diversified Structural Architecture1Optimal Design of Mid-Infrared Nonlinear-Optical Crystals: From SrZnSnSe 4 to SrZnSiSe 422Li2.9Cs1.1(SO4)2: An Ultraviolet Transparent Sulfate as a Nonlinear Optical Crystal16The Strategy to Improve the Phase Matching Ability in Tetrahedron‐Based Deep‐Ultraviolet Nonlinear Optical Crystals21Wide band gaps in nonlinear optical materials AMgAgGa6S11 (A = K, Rb) achieved by the incorporation of dual s-block elements in Ag-based sulfide11Enlargement of Bandgap and Birefringence in Nonlinear Optical Alkali‐Metal Sulfate Crystals by the Substitution of Asymmetrical Non‐π‐Conjugated Cation8(SO3CF3)−: A Non‐π‐Conjugated Motif for Nonlinear Optical Crystals Transparent into the Deep‐Ultraviolet Region23Stereochemically Active Lone-Pair Containing Metal Substitution in Polar Axis toward a Giant Phase-Matchable Optical Nonlinear Silicate Crystal Li 3 (OH)PbSiO 463Ultrashort Phase‐Matching Wavelength and Strong Second‐Harmonic Generation in Deep‐UV‐Transparent Oxyfluorides by Covalency Reduction33Ultrashort Phase‐Matching Wavelength and Strong Second‐Harmonic Generation in Deep‐UV‐Transparent Oxyfluorides by Covalency Reduction3Ba 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 Strategy12A 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 Polycations25K(NH4)Zn2(PO4)2: a Beryllium-Free Sr2Be2B2O7 Derivative with Enhanced Interlayer Connectivity7Ba 5 Y 12 Zn[O(SiO 4 )] 8 : a novel non-centrosymmetric silicate with a short ultraviolet cut-off edge featuring [ZnSi 4 O 16 ] and [SiO 4 ] units3Exploring a new short-wavelength nonlinear optical fluoride material featuring unprecedented polar cis -[Zr 6 F 34 ] 10− clusters48External electric field driven electronic structures: tunable nonlinear optical properties of helical bilayer nanographenes2KBa 3 M 2 F 14 Cl (M = Zr, Hf): novel short-wavelength mixed metal halides with the largest second-harmonic generation responses contributed by mixed functional moieties37Reticular chemistry-aided effective design of new second-order nonlinear optical selenites11Shooting short-wavelength nonlinear optical materials with targeted balance performances in hydroxyborates through first-principles high-throughput screening4LiASi2O5 (A = K, Rb): Effects of cations on crystal structure and optical properties1Unearthing Superior Inorganic UV Second‐Order Nonlinear Optical Materials: A Mineral‐Inspired Method Integrating First‐Principles High‐Throughput Screening and Crystal Engineering124Unearthing Superior Inorganic UV Second‐Order Nonlinear Optical Materials: A Mineral‐Inspired Method Integrating First‐Principles High‐Throughput Screening and Crystal Engineering4Giant Optical Anisotropy in a Covalent Molybdenum Tellurite via Oxyanion Polymerization43Pb3[O10Pb20](SiO4)4X10 (X = Cl, Br): The First Pb-Containing Halogen Silicates with Mirror-Symmetric Pseudo-Aurivillius Bilayers3Record Second-Harmonic Generation and Birefringence in an Ultraviolet Antimonate by Bond Engineering157From Cd(SCN) 2 (CH 4 N 2 S) 2 to Cd(SCN) 2 (C 4 H 6 N 2 ) 2 : Controlling Sulfur Content in Thiocyanate Systems Significantly Improves the Overall Performance of UV Nonlinear Optical Materials9From Cd(SCN) 2 (CH 4 N 2 S) 2 to Cd(SCN) 2 (C 4 H 6 N 2 ) 2 : Controlling Sulfur Content in Thiocyanate Systems Significantly Improves the Overall Performance of UV Nonlinear Optical Materials50Synthesis, Characterization and Optical Properties of Two Novel Metal Borates1A Universal Design Strategy Achieving Large Birefringence and Short Phase‐Matching Capability of Optical Materials via Dissimilating Non‐π‐Conjugated Units6Assembly 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, Cs2YB3O6F297Ba2ScBSi2O9: A Mixed-Coordination Borosilicate with a Low B/Si Ratio Exhibiting Enhanced Second Harmonic Generation Response7A2Cd(PO3)4 (A = K, Rb, Cs): Series of cadmium polyphosphates with infinite 1[(PO3)4]ꝏ chains and deep ultraviolet transparency windows2Two α‐SiO 2 ‐Related Deep‐Ultraviolet Phase‐Matchable Optical Nonlinear Beryllium Silicate Crystals Na 2 BeSiO 4 and Li 2 BeSiO 4 with Enhanced SHG Effect10MgPO2F3: An Ultraviolet Nonlinear Optical System with an Extremely Short Phase-Matching Wavelength Achieved by Introducing Dual-Type Fluorine via Structure Prediction1K 15 La 7 (BO 3 ) 12 : A KBBF-Like Nonlinear-Optical Material with a Short Cutoff Edge and a Strong Second-Harmonic-Generation Response10Exploring Novel Mixed Metal Sulfate Hydrates with Short UV Cut-Off Edges0A Wide Band Gap Germanate with the Largest Second Harmonic Generation Response Created by Hypoxic Strategy22A Wide Band Gap Germanate with the Largest Second Harmonic Generation Response Created by Hypoxic Strategy5Na3Y2F3P2O8 and K4Y3F5P4O14: [YOF] Polyhedra Inducing Birefringence Enhancement in Non-π-Conjugated Phosphate Systems3Rational design of a high-efficiency lead halide organic-inorganic hybrid nonlinear optical switch via molecular engineering5Zero-Dimensional Oxyselenide Ba12[(Ga2OSe5)3(Si2O7)]: Enhanced Optical Anisotropy through Heteroanionic Engineering4Enhancement of optical anisotropy from [BF4] units by ligand substitution0Promising UV/DUV nonlinear optical materials with X-membered (X = multiples of 6) rings in anhydrous inorganic borates20K5NaZr4F22(H2O)2: A Hydrated Zirconium Fluoride with a Second-Harmonic Generation Effect and a Short Ultraviolet Cutoff Edge Induced by Cosubstitution with Heterovalent Cations6Borosilicates as deep-ultraviolet transparent nonlinear optical crystals: Structural motifs, performance limits and future directions9KF·[SO 2 (NH 2 ) 2 ]: the First Deep‐Ultraviolet Transparent Sulfonamide Fluoride Nonlinear Optical Crystal with Novel Cairo Pentagonal Structure13KF·[SO 2 (NH 2 ) 2 ]: the First Deep‐Ultraviolet Transparent Sulfonamide Fluoride Nonlinear Optical Crystal with Novel Cairo Pentagonal Structure5Breaking the Deep‐UV Transparency/Optical Nonlinearity Trade‐Off: Three‐Parameter Optimization in Oxyfluorides by Tailoring d 0 ‐Metal Incorporation10Breaking the Deep‐UV Transparency/Optical Nonlinearity Trade‐Off: Three‐Parameter Optimization in Oxyfluorides by Tailoring d 0 ‐Metal Incorporation4Recent achievements of d0 transition-metal-based oxyfluorides: Crystal chemistry and application in second-order NLO materials10Single-crystal Ca 3 Ge 3 O 9 calcium germanate: structure, thermal and optical properties from experimental and first-principles analyses0LiBa 2 GaSi 2 O 8 : A Noncentrosymmetric Silicate Exhibiting Wide Transmission Range and Moderate Second Harmonic Generation Response2A Deep-Ultraviolet Transparent Nonlinear Optical Hydrogen-Bonded Organic Framework21Strategically designed deep-ultraviolet optical crystals with balanced properties by small heteroatom substitution1Strong SHG, piezoelectricity, and fluorescence coexisting in a single-component organic polar crystal enabled by σ-hole interactions0BaScSi2O6F: A barium-containing rare-earth metal silicate fluoride with a short cutoff edge0Record‐Short Phase Matchability of Silicate: Charge‐Driven Lattice Distortion Enables Deep‐UV Phase Matching and Strong Optical Nonlinearity0Ternary Anion‐Engineered Rare Earth Crystals for Broadband UV Transparency and Enhanced Second‐Harmonic Generation1Confinement of Organic–Inorganic Hybrid Perovskites within MOF Cavities for Synergistic Regulation of Third-Order Nonlinear Optics0Blue–Green Emitting Phosphor Ba 2 LiAlSi 2 O 8 :Eu 2 + for Phosphor-Converted Light-Emitting Diodes via Single-Particle Diagnosis in a Quasi-Quaternary System0K 2 ZrSi 2 O 7 with a Wide Transmission Range and Enhanced Birefringence Induced by the d 0 -TM Zr-Based Units2Anion-Stabilized Incommensurate Modulation Enables Nonlinear Optical Response in Eu2SiO3.89N0.110Multidimensional Cation Modulation toward Phase-Matchable Nonlinear Optical Fluorides with Short UV Cutoff Edges0

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

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  2. Second-order nonlinear optical materials with a benzene-like conjugated π system

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  3. Similarities and differences between Mn( ii ) and Zn( ii ) coordination polymers supported by porphyrin-based ligands: synthesis, structures and nonlinear optical properties

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  4. Sr5[BO2(OH)]3(OH)3F: First hydroxyborate fluoride with the [BO2(OH)]2− unit

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  5. The nonlinear optics property of heterodinuclear (Li and Na) sexipyridine helix: A density functional theory study

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  6. Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups

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  8. Chiral Template‐Driven Macroscopic Chirality Control: Structure‐Second‐Harmonic Generation Properties Relationship

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  9. Centrosymmetric RbSnF 2 NO 3 vs. noncentrosymmetric Rb 2 SbF 3 (NO 3 ) 2

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  11. In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 2

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  12. Systematic centricity control using a chiral template: novel noncentrosymmetric polar niobium oxyfluorides and tantalum fluorides directed by chiral histidinium cations, [( l -hisH 2 )NbOF 5 ], [( d -hisH 2 )NbOF 5 ], [( l -hisH 2 )TaF 7 ], and [( d -hisH 2 )TaF 7 ]

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  13. The Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal

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  14. To improve the key properties of nonlinear optical crystals assembled with tetrahedral functional building units

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  15. Zn(NH 3 )CO 3 : a “three-in-one” UV nonlinear optical crystal built by a polar molecule bonding strategy

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  16. Large Second-Harmonic Response and Giant Birefringence of CeF 2 (SO 4 ) Induced by Highly Polarizable Polyhedra

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  17. Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance

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  18. Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance

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  22. Cyanurates consisting of intrinsic planar π-conjugated 6-membered rings: An emerging source of optical functional materials

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  23. Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application

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  24. Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application

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  25. α-Ca2CdP2 and β-Ca2CdP2: Two Polymorphic Phosphide-Based Infrared Nonlinear Crystals with Distorted NLO-Active Tetrahedral Motifs Realizing Large Second Harmonic Generation Effects and Suitable Band Gaps

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  26. High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies

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  28. Hydrogen‐Bond‐Driven Synergistically Enhanced Hyperpolarizability: Chiral Coordination Polymers with Nonpolar Structures Exhibiting Unusually Strong Second‐Harmonic Generation

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  29. Insights into varying dimension structures for deep-UV optical crystals NaBa2Al(P2O7)2 and NaBaAl(PO4)2 constructed separately from unique [Al(P2O7)2] chains and [Al(PO4)2] layers

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  31. Li 4 MgGe 2 S 7 : The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap

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  32. Li4MgGe2S7: The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap

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