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RESEARCH PAPER · Angewandte Chemie International Edition · 2020

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

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K 2 Sb(P 2 O 7 )F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical PerformanceOriginalGiant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )212Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )57Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”6Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”2Reply 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”1Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence92Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence13The synthesis, characterization, and theoretical analysis of (NH 4 ) 3 PbCl 52An antimony( iii ) borate with large birefringence exhibiting unwonted [B 5 O 11 ] fundamental building blocks and dimeric [Sb 2 O 6 ] clusters26An organic–inorganic hybrid birefringent material with diverse functional groups38Ba 4 Ca(B 2 O 5 ) 2 F 2 : π-conjugation of B 2 O 5 in the planar pentagonal layer achieving large second harmonic generation of pyro -borate34Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2First chiral fluorinated lead vanadate selenite Pb 2 (V 2 O 4 F)(VO 2 )(SeO 3 ) 3 with five asymmetric motifs and large optical properties24From centrosymmetric to noncentrosymmetric: effect of the cation on the crystal structures and birefringence values of (NH 4 ) n−2 AE(PO 2 F 2 ) n (AE = Mg, Sr and Ba; n = 2, 3 and 4)9In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 219Optimization of fluxes for Yb 3+ :YMgB 5 O 10 crystal growth and intense multi-wavelength emission characteristics in spectra and laser performances14RbMo 2 P 3 O 14 with large birefringence mainly induced by highly distorted [MoO 6 ] in uncommon [Mo 2 P 3 O 14 ] ∞ layers9Recent advances of oxyfluorides for nonlinear optical applications69Unexpected aliovalent cation substitution between two NLO materials LiBa 3 Bi 6 (SeO 3 ) 7 F 11 and Ba 3 Bi 6.5 (SeO 3 ) 7 F 10.5 O 0.518Ba3Sb2(PO4)4 and Cd3Sb2(PO4)4(H2O)2: Two New Antimonous Phosphates with Distinct [Sb(PO4)2] Structure Types and Enhanced Birefringence37Order and Disorder: Toward the Thermodynamically Stable α-BaMoO2F4 from the Metastable Polymorph31Bi2[B2(SeO3)6]: A Metal Boroselenite with a Unique Zero-Dimensional [B2(SeO3)6]6– Anionic Group and Large Birefringence31UV 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 Phosphate28Tin Chloride Sulfates A3Sn2(SO4)3–xCl1+2x (A = K, Rb, Cs; x = 0, 1) as Multifunctional Optical Materials33High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies323Linear and Nonlinear Optical Properties of Centrosymmetric Sb 4 O 5 SO 4 and Noncentrosymmetric Sb 4 O 4 (SO 4 )(OH) 2 Induced by Lone Pair Stereoactivity55Synthesis, characterization and optical properties of three novel lanthanide sulfates10A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation22A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation63Realization of an Ideal Cairo Tessellation in Nickel Diazenide NiN 2 : High-Pressure Route to Pentagonal 2D Materials114Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate22Noncentrosymmetric Rb3(COOH)3(H3BO3)2 vs Centrosymmetric Cs3(COOH)3(H3BO3)2142D van der Waals Layered [C(NH2)3]2SO3S Exhibits Desirable UV Nonlinear-Optical Trade-Off47Tourmaline with ultraviolet optical nonlinearity: Emergent material discovery from mineral5Unusual ferroelectric-dependent birefringence in 2D trilayered perovskite-type ferroelectric exploited by dimensional tailoring63NH4Sb2(C2O4)F5: A novel UV nonlinear optical material synthesized in deep eutectic solvents38Complex coordinated functional groups: A great genes for nonlinear optical materials64Ba2B13O19(OH)5·5H2O: A promising nonlinear optical material with a unique 2[B13O19(OH)5]∞ two-dimensional layer9NaSb3O2(SO4)3·H2O: A New Alkali-Metal Antimony(III) Sulfate with a Unique Sb6O20H4 Unit and Moderate Birefringence19A 6 Mo 2 P 4 O 19 (A = Rb, Cs) and Rb 2 MoP 2 O 9 : new molybdophosphates with distinct polyanionic configurations5AZn 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 edge25[C(NH 2 ) 3 ]BiCl 2 SO 4 : an excellent birefringent material obtained by multifunctional group synergy40AAg 2 PS 4 (A = K, Na/K): the first-type of noncentrosymmetric alkali metal Ag-based thiophosphates exhibiting excellent second-order nonlinear optical performances21An excellent lead oxyiodide with a strong second-harmonic generation response and a large birefringence induced by the oriented arrangement of highly distorted [PbO 4 I 2 ] polyhedra13Ba 2 Zn 2 B 6 O 13 : coplanar [B 2 O 5 ] in unnoted U-shaped [B 6 O 13 ] groups achieving large birefringence6BaSc 2 (HPO 3 ) 4 (H 2 O) 2 : a new nonlinear optical phosphite exhibiting a 3D {[Sc 2 (HPO 3 ) 4 ] 2− } ∞ anionic framework and phase-matchable SHG effect32KSb(BeF 3 )F 3 : a totally fluorine strategy for achieving wide bandgap and large birefringence23Large optical anisotropy differentiation induced by the anion-directed regulation of structures29Metal oxyhalides: an emerging family of nonlinear optical materials124Nain(C2o4)(Hpo4)(H2o)5: An Ultraviolet Transparent Nonlinear Optical Oxalate-Phosphate with Large Birefringence0Synergistic 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) systems4Three-dimensional all-inorganic dual halogen emitter Cs 2 Cd 2 BrCl 5 exhibiting broadband white-light emission18High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence21High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence199Potential optical functional crystals with large birefringence: Recent advances and future prospects322Layered Perovskite-like Nitrate Cs2Pb(NO3)2Br2 as a Multifunctional Optical Material40Corrugated 1D Hybrid Metal Halide [C6H7ClN]CdCl3 Exhibiting Broadband White-Light Emission46K3ZrF4(SbF4)(SbF5) and K8(ZrF6)(Sb2Zr2F20): Two Zirconium Fluoroantimonites with Low Dimensional Structures and Wide Transparency Range12Ultrawide 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 Material12Enhanced Second-Harmonic-Generation Efficiency and Birefringence in Melillite Oxychalcogenides Sr2MGe2OS6 (M = Mn, Zn, and Cd)97Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Lone Pair-Driven Enhancement of Birefringence in Polar Alkali Metal Antimony Phosphates46RbLiZn5(PO4)4 and BaLiZn3(PO4)3: two new zinc orthophosphates with all tetrahedra-based anion frameworks11Enhancement of Birefringence in Borophosphate Pushing Phase-Matching into the Short-Wavelength Region150Yin–Yang Complementarity Strategy Achieving Giant Optical Anisotropy in a Metal-free Birefringent Material C(NH2)3(HC4O4)14Cation-anion synergetic interactions achieving tunable birefringence in quasi-one-dimensional antimony(III) fluoride oxalates58Organic Cation Modulation Triggered Second Harmonic Response in Manganese Halides with Bright Fluorescence46[C(NH2)3]2Zn(CO3)2: A Guanidinium-Templated Ultraviolet Nonlinear Optical Material20Sharp Enhancement of Birefringence in Antimony Oxalates Achieved by the Cation–Anion Synergetic Interaction Strategy38Tunable emission color of [(2-mb)tpp]2Cd1-xMnxCl4 (x = 0–1) solid solutions synthesized via mechanochemical method for anti-counterfeit luminescent paper and WLEDs29Mixed-Anion-Oriented Design of LnMGa3S6O (Ln = La, Pr, and Nd; M = Ca and Sr) Nonlinear Optical Oxysulfides with Targeted Property Balance56[C(NH2)3]2MoO2F4·H2O: Unique Chinese-Knot Structure Revealing Superior Nonlinear-Optical Properties19BaSb(H2PO2)3Cl2: An excellent UV nonlinear optical hypophosphite exhibiting strong second-harmonic generation response32Chalcohalides: A Rising Type of Second‐Order Nonlinear Optical Materials28SbHPO3F: 2D van der Waals Layered Phosphite Exhibiting Large Birefringence32Growth, Structure, and Optical Properties of a Nonlinear Optical Niobium Borate Crystal CsNbOB2O5 with Distorted NbO5 Square Pyramids13Syntheses, structures, and characterization of new heteroanionic chalcohalides: Na2Ba17In8Q21F18 (Q = S, Se), KBa2InQ3F2 (Q = S, Se)5LiKCuP2O7: Cation substitution application with mixed-alkaline copper-containing pyrophosphate and magnetic properties2Efficient Capture of Sr2+ Ions by a Layered Potassium Neodymium Phosphate9(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 cations56A series of novel phosphites/phosphates with deep-ultraviolet cut-off edges from 0D polar to 3D non-polar architectures13An effective pathway to design and synthesize UV birefringent crystals via rational assembly of π-conjugated [CO 3 ] 2− and [NO 3 ] − triangles32Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181Dramatically improved optical anisotropy by realizing stereochemically active lone pairs in a sulfate system, K 2 SO 4 ·HIO 323Enhancing birefringence of non-π-conjugated sulfate systems through rare-earth metal-centered polyhedra10Evaluating refractive index and birefringence of nonlinear optical crystals: Classical methods and new developments45From Cs8Sb4Nb5O5F35 to Cs6Sb4Mo3O5F26: The first noncentrosymmetric fluoroantimonite with d0 transition metal30Heteroanion-introduction-driven birefringence enhancement in oxychalcogenide Ba 3 M II Ge 3 O 2 S 8 (M II = Mn, Cd)19Hg 3 O 2 (NO 3 )F: a mercury nitrate oxyfluoride with an unprecedented [(Hg 3 O 2 F) + ] ∞ cationic framework and excellent optical anisotropy21Low temperature molten salt synthesis of noncentrosymmetric (NH 4 ) 3 SbF 3 (NO 3 ) 3 and centrosymmetric (NH 4 ) 3 SbF 4 (NO 3 ) 234Na 7 (SeO 4 ) 3 (IO 3 ) and K 2 (SeO 4 )[IO 2 (OH)]: two new iodate-selenates with short-wave UV cutoff edge and large birefringence8Penta-Mn8: First Realization of Type-5 Pentagonal Tessellation in 2d Hexagonal Crystals with Intriguing Properties0Recent advances on the synthesis of Sb(III)-based inorganic ultraviolet nonlinear optical materials47Stereochemically active lone-pair-driven giant enhancement of birefringence from three-dimensional CsZn 4 Ga 5 Se 12 to two-dimensional CsZnAsSe 319Structure and optical property evolution in PbM(PO 4 )X (M = Zn, Sn; X = halogen): SHG effect and birefringence21The transformation of a zero-dimensional cluster into a one-dimensional chain structure achieving a dramatically enhanced birefringence in tin( ii )-based oxalates33Three-dimensional porous borocarbonitride composed of pentagonal motifs as a high-performance pyroelectric material0Pb2Cl2(HPO3)(H2O) and Pb3Br2(HPO3)2: Two Phosphite Halides with 3D Structural Networks and Enlarged Birefringence18Toward Large Second-Harmonic Generation and Deep-UV Transparency in Strongly Electropositive Transition Metal Sulfates112Deep Eutectic Solvents Synthesis of A2Sb(C2O4)Cl3 (A = NH4, K, Rb) with Superior Optical Performance26Rational Design of the First Ammonium Magnesium Borate with Deep-Ultraviolet Cutoff Edge and Moderate Birefringence and Further Investigation into the Nature of Ammonium in the Borate System15Structure and Characterization of K2Na3B2P3O13, a New Nonlinear Optical Borophosphate with One-Dimensional Chain Structure and Short Ultraviolet Cutoff Edge13A Rare‐Earth Selenite with Unexpectedly Well‐Balanced Ultraviolet Nonlinear Optical Functionality, Sc(HSeO 3 ) 331Controlling 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 response7Recent 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 Birefringence6Two Mixed-Alkali-Metal Selenates as Short-Wave Ultraviolet Nonlinear-Optical Materials102D Perovskite Mn 2+ ‐Doped Cs 2 CdBr 2 Cl 2 Scintillator for Low‐Dose High‐Resolution X‐ray Imaging127Unveiling the Superior Optical Properties of Novel Melamine‐Based Nonlinear Optical Material with Strong Second‐Harmonic Generation and Giant Optical Anisotropy74Four New Sb‐based Orthophosphates: Cation Regulation to Investigate Diversified Structural Architecture1Sb4O3(TeO3)2(HSO4)(OH): An Antimony Tellurite Sulfate Exhibiting Large Optical Anisotropy Activated by Lone Pair Stereoactivity30A Polar Tetragonal Tungsten Bronze with Colossal Second‐Harmonic Generation18A BBO-like trithiocyanate with significantly enhanced birefringence and second-harmonic generation39A Hydrogen Bonded Supramolecular Framework Birefringent Crystal89A Hydrogen Bonded Supramolecular Framework Birefringent Crystal13“Cation Activation”: An Effective Strategy for the Enhancement of Birefringence36Cd2Nb2Te4O15: A Novel Pseudo‐Aurivillius‐Type Tellurite with Unprecedented Nonlinear Optical Properties and Excellent Stability40ASb(SO4)2 (A = Rb, Cs): Two short-wave UV antimony sulfates exhibiting large birefringence43Na4[B6O9 (OH)3](H2O) Cl: A Deep-Ultraviolet Transparent Nonlinear Optical Borate Chloride with {[B6O9 (OH)3]3–}∞ Chains5High-pressure synthesis of dysprosium carbides10Pb(OH)I: A lead(II)-based oxyhalide with a large birefringence5Improved Birefringence Activated by Tetrahedra Decorated with a Single Linear Unit38Improved Birefringence Activated by Tetrahedra Decorated with a Single Linear Unit1Multifunctional properties of a polar spin chain compound [N(C3H7)4][Cu(C8H4NO4)]·H2O exhibiting both one-dimensional magnetism and nonlinear optical activity15Centrosymmetric Rb2Sb(C2O4)2.5(H2O)3 and Noncentrosymmetric RbSb2(C2O4)F5: Two Antimony (III) Oxalates as UV Optical Materials20A survey of stereoactive oxysalts for linear and nonlinear optical applications40K2Sr4(PO3)10: A Polyphosphate with Deep-UV Cutoff Edge and Enlarged Birefringence6Enlargement of Bandgap and Birefringence in Nonlinear Optical Alkali‐Metal Sulfate Crystals by the Substitution of Asymmetrical Non‐π‐Conjugated Cation8Penta-MN8 family: First realization of type-5 pentagonal tessellation in 2D hexagonal crystals with intriguing properties6Highly Birefringent d 0 Transition Metal Fluoroantimonite in the Mid Infrared Band: Order–Disorder Regulation by Cationic Size83Two UV organic-inorganic hybrid antimony-based materials with superior optical performance derived from cation-anion synergetic interactions30Designing Sulfate Crystals with Strong Optical Anisotropy through π‐Conjugated Tailoring51Designing Sulfate Crystals with Strong Optical Anisotropy through π‐Conjugated Tailoring11Na 10 Zn(NO 3 ) 4 (SO 3 S) 4 : a nonlinear optical crystal combining inorganic π-conjugated and non-π-conjugated heteroanion groups8Two van der Waals Layered Antimony(III) Phosphites as UV Optical Materials11Hydroxyl-Driven Enhanced Birefringence in Borophosphates3Secondary‐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 Birefringence41[(C 5 H 6 N 2 ) 2 H](Sb 4 F 13 ): a polyfluoroantimonite with a strong second harmonic generation effect60Chemical perspectives on heteroanionic compounds: a potential playground for multiferroics7Designing excellent UV birefringent materials through the synergistic interaction of two highly distorted functional groups23Designing promising ultraviolet (UV) birefringent crystals with different hydrogen-bonded phosphate frameworks18Hydrogen 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 framework4K, Rb-hydroxyborates series with deep-ultraviolet KRbB 5 O 8 (OH) possessing moderate second harmonic generation response0

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