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RESEARCH PAPER · Journal of the American Chemical Society · 2018

Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects

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Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation EffectsOriginalBa 3 B 10 O 17 Br 2 : a new barium borate halide with B–O layered structure4Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties78Cs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response129Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges16PbCdF(SeO 3 )(NO 3 ): A Nonlinear Optical Material Produced by Synergistic Effect of Four Functional Units52Why Some Noncentrosymmetric Borates Do Not Make Good Nonlinear Optical Materials: A Case Study with K3B5O8(OH)222Synthesis, crystal structures and nonlinear optical properties of polymorphism: α- and β-RbHgI3·H2O18Centrosymmetric (NH4)2SbCl(SO4)2 and Non-centrosymmetric (NH4)SbCl2(SO4): Synergistic Effect of Hydrogen-Bonding Interactions and Lone-Pair Cations on the Framework Structures and Macroscopic Centricities89Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response8The Rubidium Barium Borate Resulting from B7O15 Fundamental Building Block Exhibits DUV Cutoff Edge17Na 3 B 7 O 11 F 2 : a new sodium-rich fluorooxoborate with a unique [B 14 O 24 F 4 ] ring and a short ultraviolet absorption edge27The linear and nonlinear optical response of CsGeX3 (X=Cl, Br, and I): The finite field and first-principles investigation26Ba 4 Bi 2 (Si 8−x B 4+x O 29 ) ( x = 0.09): a new acentric metal borosilicate as a promising nonlinear optical material53Cyano-Based Materials with Giant Optical Anisotropy and Second Harmonic-Generation Effect24BaB8O12F2: a promising deep-UV birefringent material60Ba 3 B 10 O 17 F 2 ·0.1KF: the first mixed alkali/alkaline-earth metal fluorooxoborate with unprecedented double-layered B–O/F anionic arrangement17Cs 2 CdV 2 O 6 Cl 2 and Cs 3 CdV 4 O 12 Br: two new non-centrosymmetric oxyhalides containing d 0 and d 10 cations and exhibiting second harmonic generation activity19Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F27K 2 [B 4 O 5 (OH) 4 ]·H 2 O and K 2 [B 4 O 5 (OH) 4 ]: two new hydrated potassium borates with isolated [B 4 O 5 (OH) 4 ] 2− units and different structural frameworks8LiGeBO 4 : a nonlinear optical material with a balance between deep-ultraviolet cut-off edge and large SHG response induced by hand-in-hand tetrahedra21LiO 4 tetrahedra lock the alignment of π-conjugated layers to maximize optical anisotropy in metal hydroisocyanurates44M 2 (SeO 3 )F 2 (M = Zn, Cd): understanding the structure directing effect of [SeO 3 ] 2− groups on constructing ordered oxyfluorides14Pb 10 O 4 (BO 3 ) 3 I 3 : a new noncentrosymmetric oxyborate iodide synthesized by the straightforward hydrothermal method6RE(H 2 C 3 N 3 O 3 ) 2 ·(OH)· x H 2 O (RE = La, Y and Gd): potential UV birefringent materials with strong optical anisotropy originating from the (H 2 C 3 N 3 O 3 ) − group31Sn 2 B 7 O 12 F with a 2∞[B 14 O 24 ] 6− layer constructed from the unprecedented [B 7 O 16 ] 11− fundamental building block18SnGa 2 GeSe 6 , a benign addition to the AMIII2M IV Q 6 family: synthesis, crystal structure and nonlinear optical performance20Tb(HSO 4 )(SO 4 ) – a green emitting hydrogensulfate sulfate with second harmonic generation response21The very first normal-pressure tin borate Sn 3 B 4 O 9 , and the intermediate Sn 2 [B 7 O 12 ]F12Two low-dimensional metal halides: ionothermal synthesis, photoluminescence, and nonlinear optical properties19Two new tin( iv )-containing phosphate fluorides with two types of Sn( iv )–P–O–F frameworks and short cutoff edges0A Niobium Oxyiodate Sulfate with a Strong Second‐Harmonic‐Generation Response Built by Rational Multi‐Component Design114A Niobium Oxyiodate Sulfate with a Strong Second‐Harmonic‐Generation Response Built by Rational Multi‐Component Design25Lone‐Pair Enhanced Birefringence in an Alkaline‐Earth Metal Tin(II) Phosphate BaSn 2 (PO 4 ) 2130CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure87CsSbF2SO4: An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO4 (KTP)‐type Structure432Designing Three Fluorooxoborates with a Wide Transmittance Window by Anionic Group Substitution15Module-Analysis-Assisted Design of Deep Ultraviolet Fluorooxoborates with Extremely Large Gap and High Structural Stability109BaB 2 O 3 F 2 : A Barium Fluorooxoborate with a Unique [B 2 O 3 F] − Layer and Short Cutoff Edge38Sr 6 Cd 2 Sb 6 O 7 S 10 : Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups124Sr6Cd2Sb6O7S10: Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups22Poly(difluorophosphazene) as the First Deep‐Ultraviolet Nonlinear Optical Polymer: A First‐Principles Prediction35Poly(difluorophosphazene) as the First Deep‐Ultraviolet Nonlinear Optical Polymer: A First‐Principles Prediction14Prediction 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 Layers24Rb7SrY2(B5O10)3: A Rare-Earth Pentaborate with Moderate Second-Harmonic Response and Interesting Phase-Matching Behavior29Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups45Ba 8 SrPb 24 O 24 Cl 18 : the first alkali-earth metal lead( ii ) oxyhalide with an intriguing multimember-ring layer9Exploring Main Group Metal Borosulfates: Similarities and Differences of Two New Borosulfates M[B2O(SO4)3] (M = Sr, Pb)21Nitrate nonlinear optical crystals: A survey on structure-performance relationships146Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin255Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin33Pb 3 Ba 3 Zn 6 (BO 3 ) 8 and α-BaZn 2 (BO 3 ) 2 : new members of the zincoborates containing two different dimensional Zn–O units8An Uncommon Hypervalent Fluorooxosilicophosphate5LiCsPbP2O7: A new alkali metal lead pyrophosphate featuring two dimensional [LiP2O7]∞ layer2Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides63CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Surface Nonlinear Optics on Centrosymmetric Dirac Nodal‐Line Semimetal ZrSiS22A new iodate-phosphate Pb 2 (IO 3 )(PO 4 ) achieving great improvement in birefringence activated by (IO 3 ) − groups53A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48“Old dog, new tricks”: the lone pair effect inducing divergent optical responses in lead cyanurates containing π-bonds18Lone pair electron effect induced differences in linear and nonlinear optical properties of bismuth borates12NaRb3B6O9(OH)3(HCO3): A Borate-Bicarbonate Nonlinear Optical Material18Alkali-earth metal lead( ii ) oxyhalide Ba 27 Pb 8 O 8 Cl 54 exhibiting interesting [Pb 4 Ba 4 O 4 ] 8+ species8(C 3 H 9 NI) 4 AgBiI 8 : a direct-bandgap layered double perovskite based on a short-chain spacer cation for light absorption66[O 2 Pb 3 ] 2 (BO 3 )I: a new lead borate iodide with 1∞[O 2 Pb 3 ] double chains6Ba 6 BO 3 Cl 9 and Pb 6 BO 4 Cl 7 : structural insights into ortho -borates with uncondensed BO 4 tetrahedra10Coordinated regulation on critical physiochemical performances activated from mixed tetrahedral anionic ligands in new series of Sr 6 A 4 M 4 S 16 (A = Ag, Cu; M = Ge, Sn) nonlinear optical materials28From BaAl 2 (BO 3 ) 2 O to SnAl 2 (BO 3 ) 2 F 2 : structure transformation based on ion regulation3From BiF 3 to BiF 3 ·H 2 O: diverse Bi( iii ) coordination for structural transformation and birefringence regulation14Large nonlinear optical effect in tungsten bronze structures via Li/Na cross-substitutions4Large optical polarizability causing positive effects on the birefringence of planar-triangular BO 3 groups in ternary borates18Li 3 CaB 2 O 5 F: a unique sandwich-like structure with diverse and wide Li ion diffusion pathways5PbSrSiO 4 : a new ultraviolet nonlinear optical material with a strong second harmonic generation response and moderate birefringence37Prediction of ternary fluorooxoborates with coplanar triangular units [BO x F 3−x ] x− from first-principles13Synthesis, characterization and crystal structure of a new mixed alkali and alkaline-earth metal borate Rb 9 Ba 24 (BO 3 ) 196Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51Designing Sulfide Borate as a Novel Type of Second-Order Nonlinear-Optical Material91KNiB4O6F3: A Layered Fluorooxoborate with Charge‐Oriented Ordering18A Promising Fluorooxoborate Framework with Flexibile Capability for Diverse Cations to Enhance the Second Harmonic Generation14PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material120An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses224An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses42Rational Design of the Nonlinear Optical Response in a Tin Iodate Fluoride Sn(IO3)2F290Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement96Alignment of Polar Moieties Leading to Strong Second Harmonic Response in KCsMoP2O951Synthesis, characterizations and theoretical analysis of a noncentrosymmetric sulfate8Large Out‐of‐Plane Second Harmonic Generation Susceptibility in Penta‐ZnS2 Sheet17A Series of Organic–Inorganic Hybrid Compounds [(C2H5)4N]InCl4–xBrx (x = 0, 2, 4): Synthesis, Crystal Structure, and Nonlinear Optical Properties37Strong Second Harmonic Generation in a Tungsten Bronze Oxide by Enhancing Local Structural Distortion48K4Sb(SO4)3Cl: The first apatite-type sulfate ultraviolet nonlinear optical material with sharply enlarged birefringence61Hydrogen-Bond-Assisted Reinforcement of Interlayer Connections in Zn2BO3X·H2O (X = Cl, Br): Two UV Nonlinear Optical Crystals with KBBF-Type Structure9A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107Rational 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 Nonlinearity31AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses63Sr5Ga8O3S14: A Nonlinear Optical Oxysulfide with Melilite-Derived Structure and Wide Band Gap48Structure-property survey and computer-assisted screening of mid-infrared nonlinear optical chalcohalides113K 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 Performance38Sr5[BO2(OH)]3(OH)3F: First hydroxyborate fluoride with the [BO2(OH)]2− unit2Different mechanism of response of asymmetric lone pair electrons around ns2 cations to birefringence and second harmonic generation7Role of Fluorooxo-Functional Units in Symmetry Breaking and Second Harmonic Generation Response Contribution in Fluorooxoborate Nonlinear Optical Crystals15KSnI 3 ⋅ H 2 O: A New Compound with One‐Dimensional SnI 3 Chains of Pyramidal SnI 5 Polyhedra2A new nonlinear optical sulfate of layered structure: Cs2Zn2(SO4)319Borates: A Rich Source for Optical Materials1089Synergism of multiple functional chromophores significantly enhancing the birefringence in layered non-centrosymmetric chalcohalides20Sn3B8O15: A Ternary Tin(II) Borate with Flexible [B8O18]12– Fundamental Building Block Formed by [B7O16]11– and [BO3]3– Groups10K 3 B 4 PO 10 and K 2 MB 4 PO 10 (M = Rb/Cs): rare mixed-coordinated borophosphates with large birefringence33A new acentric borate–nitrate Cs 3 B 8 O 13 (NO 3 ) with interpenetrating porous 3D covalent and ionic lattices8Ba 2.5 Pb 1.5 B 12 O 22 : structural transformation from a centrosymmetric to a noncentrosymmetric space group by introducing Pb into Ba 2 B 6 O 117Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2From thiophosphate to chalcohalide: mixed-anion AgS x Cl y ligands concurrently enhancing nonlinear optical effects and laser-damage threshold10K 2 Pb(H 2 C 3 N 3 O 3 ) 4 (H 2 O) 4 : a potential UV nonlinear optical material with large birefringence50M 6 PS 5 X (M = Ag, Cu; X = Cl, Br) chalcohalides exhibiting strong nonlinear optical responses and high laser damage resistances9Na 4 SnS 4 and Na 4 SnSe 4 exhibiting multifunctional physicochemical performances as potential infrared nonlinear optical crystals and sodium ion conductors27NaKB 6 O 9 F 2 : a new complex alkali metal fluorooxoborate with puckered layers10RbPb 8 O 4 Cl 9 : the first alkali metal lead oxyhalide with distorted [PbO 3 Cl 3 ] and [PbOCl 5 ] mixed-anion groups6Recent advances of oxyfluorides for nonlinear optical applications69The tin sulfates Sn(SO 4 ) 2 and Sn2(SO4)3: crystal structures, optical and thermal properties10Ultraviolet nonlinear optical crystals A 3 SrBi(P 2 O 7 ) 2 (A = K, Rb) with large second harmonic generation responses15Pb3Ba7B7O20F: A new nonlinear optical material exhibiting large second harmonic generation response induced by its unprecedented Pb-B-O framework13Order and Disorder: Toward the Thermodynamically Stable α-BaMoO2F4 from the Metastable Polymorph31Borosilicate Crystal LaBSiO5: A New Promising Ultraviolet Quasiphase Matching Material31Molecular Engineering toward an Enlarged Optical Band Gap in a Bismuth Sulfate via Homovalent Cation Substitution26Discovery 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 Application18Hierarchical molecular design of high-performance infrared nonlinear Ag2HgI4 material by defect engineering strategy128From Centrosymmetry to Noncentrosymmetry: Tailoring the Structural Arrangements of Carbonates with Strong Nonlinear Optical Response through Partial Anion Substitution33Unique Unilateral-Chelated Mode-Induced d–p−π Interaction Enhances Second-Harmonic Generation Response in New Ln3LiMS7 Family41Sr2Pb(BeB5O10)(BO3): An Excellent Ultraviolet Nonlinear-Optical Beryllium Borate by the Pb-Modified Construction of a Conjugated System and Lone-Pair Effect14The First Mixed Calcium Zinc Borate with a Flexible [B8O17] Fundamental Building Block and Short UV Cutoff Edge7Synthesis, Crystal Structure, and Nonlinear Optical Property of an Anhydrous Sulfate KTb(SO4)216Noncentrosymmetric Rb3(COOH)3(H3BO3)2 vs Centrosymmetric Cs3(COOH)3(H3BO3)214Tin(II)-Induced Large Birefringence Enhancement in Metal Phosphates22Finding a Series of BaBOF3 Fluorooxoborate Polymorphs with Tunable Symmetries: A Simple but Flexible Case37Thermal anomalies and phase transitions in Pb2Sc2Si2O9 and Pb2In2Si2O91A first-principle investigate about the different response of birefringence and SHG from AB3O6 (A = Bi, Sb) compounds5From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra10NH4Sb2(C2O4)F5: A novel UV nonlinear optical material synthesized in deep eutectic solvents38Two molybdenyl carbonates with different dimensional structures exhibiting huge differences in band gaps7Ba2B13O19(OH)5·5H2O: A promising nonlinear optical material with a unique 2[B13O19(OH)5]∞ two-dimensional layer9A 2 B 6 O 9 F 2 (A = NH 4 , K): new members of A 2 B 6 O 9 F 2 family with deep-UV cutoff edges and moderate birefringence17From oxides to oxysulfides: the mixed-anion GeS 3 O unit induces huge improvement in the nonlinear optical effect and optical anisotropy for potential nonlinear optical materials19Na 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 edge8Variable dimensionality of the anion framework in four new borophosphates and fluoroborophosphates with short cutoff edges13Review of Heteroleptic Tetrahedra as Birefringent or Nonlinear Optical Motifs17MM′B3O4F3 (M = K; M′ = Na, K, Cs): Alkali-Metal Fluorooxoborates with ∞1[B3O4F3] Chains and Deep-Ultraviolet Cutoff Edges12Advances in second-order nonlinear optical sulfates38

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  2. Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties

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  5. The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges

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  32. A Niobium Oxyiodate Sulfate with a Strong Second‐Harmonic‐Generation Response Built by Rational Multi‐Component Design

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