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RESEARCH PAPER · Journal of the American Chemical Society · 2016

Trigonal Planar [HgSe3]4– Unit: A New Kind of Basic Functional Group in IR Nonlinear Optical Materials with Large Susceptibility and Physicochemical Stability

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Trigonal Planar [HgSe3]4– Unit: A New Kind of Basic Functional Group in IR Nonlinear Optical Materials with Large Susceptibility and Physicochemical StabilityOriginalCrystal and electronic structures, and photoluminescence and photocatalytic properties of α-EuZrS 326Na 2 MnGe 2 Se 6 : a new Mn-based antiferromagnetic chalcogenide with large Mn⋯Mn separation17Pb 5 Ga 6 ZnS 15 : a noncentrosymmetric framework with chains of T2-supertetrahedra41ChemInform Abstract: Trigonal Planar [HgSe3]4‐ Unit: A New Kind of Basic Functional Group in IR Nonlinear Optical Materials with Large Susceptibility and Physicochemical Stability.0Crystal Growth, Structure, Resistivity, Magnetic, and Photoelectric Properties of One‐Dimensional Selenometallate Ba2BiFeSe59Cooperation of Three Chromophores Generates the Water‐Resistant Nitrate Nonlinear Optical Material Bi3TeO6OH(NO3)2113Cooperation of Three Chromophores Generates the Water‐Resistant Nitrate Nonlinear Optical Material Bi3TeO6OH(NO3)220Non‐centrosymmetric Selenides AZn4In5Se12 (A=Rb, Cs): Synthesis, Characterization and Nonlinear Optical Properties47Recent achievements on middle and far-infrared second-order nonlinear optical materials433A promising lead-free fluoride carbonate SHG material designed from a theoretical perspective16Alkali earth MO x ( x = 6, 7, 9, 12) polyhedra tuned cadmium selenites with different dimensions and diverse SeO 3 2− coordinations1Ba 5 CdGa 6 Se 15 , a congruently-melting infrared nonlinear optical material with strong SHG response52Ba 6 Li 2 CdSn 4 S 16 : lithium substitution simultaneously enhances band gap and SHG intensity44Band gap tuning from an indirect EuGa 2 S 4 to a direct EuZnGeS 4 semiconductor: syntheses, crystal and electronic structures, and optical properties20Two excellent phase-matchable infrared nonlinear optical materials based on 3D diamond-like frameworks: RbGaSn 2 Se 6 and RbInSn 2 Se 639Noncentrosymmetric chalcogenides BaZnSiSe4 and BaZnGeSe4 featuring one-dimensional structures56Mid-Infrared Nonlinear Optical Materials Based on Metal Chalcogenides: Structure–Property Relationship338BaAu2S2: A Au-Based Intrinsic Photocatalyst for High-Performance Visible-Light Photocatalysis17Li2HgMS4 (M = Si, Ge, Sn): New Quaternary Diamond-Like Semiconductors for Infrared Laser Frequency Conversion64K2ZnSn3Se8: A Non‐Centrosymmetric Zinc Selenidostannate(IV) Featuring Interesting Covalently Bonded [ZnSn3Se8]2− Layer and Exhibiting Intriguing Second Harmonic Generation Activity19ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap140ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap36Pb0.65Mn2.85Ga3S8 and Pb0.72Mn2.84Ga2.95Se8: Two Quaternary Metal Chalcognides with Open-Tunnel-Framework Structures Displaying Intense Second Harmonic Generation Responses and Interesting Magnetic Properties17Hg-Based Infrared Nonlinear Optical Material KHg4Ga5Se12 Exhibits Good Phase-Matchability and Exceptional Second Harmonic Generation Response101Large Second-Harmonic Generation Responses Achieved by the Dimeric [Ge2Se4(μ-Se2)]4– Functional Motif in Polar Polyselenides A4Ge4Se12 (A = Rb, Cs)49Li2MnSnSe4: A New Quaternary Diamond‐Like Semiconductor with Nonlinear Optical Response and Antiferromagnetic Property16LiGaGe2S6: A Chalcogenide with Good Infrared Nonlinear Optical Performance and Low Melting Point56Intra- and Intermolecular Charge Transfer in a Novel Dimer: Cooperatively Enhancing Second-Order Optical Nonlinearity27Theoretical study on Pb2VO2F5: large birefringence derived from optical anisotropies of VO2F4 groups15First principle study of nonlinear optical crystals15K 2 MnGe 3 S 8 : a new multifunctional semiconductor featuring [MnGe 3 S 8 ] 2− layers and demonstrating interesting nonlinear optical response and antiferromagnetic properties33Sr 5 ZnGa 6 S 15 : a new quaternary non-centrosymmetric semiconductor with a 3D framework structure displaying excellent nonlinear optical performance60Non-Centrosymmetric RbNaMgP 2 O 7 with Unprecedented Thermo-Induced Enhancement of Second Harmonic Generation239Li7Cd4.5Ge4Se16 and Li6.4Cd4.8Sn4Se16: Strong Nonlinear Optical Response in Quaternary Diamond‐Like Selenide Networks10Synthesis, structure, magnetic and optoelectric properties of layered NaM0.5Sn0.5S2 (M= Mn, Fe)1A Series of Mixed-Metal Germanium Iodates as Second-Order Nonlinear Optical Materials71Crystal Chemistry and Photocatalytic Properties of RE 4 S 4 Te 3 (RE = Gd, Ho, Er, Tm): Experimental and Theoretical Investigations29Strong SHG Response via High Orientation of Tetrahedral Functional Motifs in Polyselenide A2Ge4Se10 (A = Rb, Cs)31BaM2As2S6 (M = Cd, Hg): Synthesis, crystal structure, optical and electronic properties16Nonbonding Electrons Driven Strong SHG Effect in Hg2GeSe4: Experimental and Theoretical Investigations61Quaternary sulfide Ba5Cd2Ga2S10 containing chains of edge- and corner-sharing tetrahedra16Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Ternary Mixed-Metal Cd4GeS6: Remarkable Nonlinear-Optical Properties Based on a Tetrahedral-Stacking Framework41Cation substitution inducing gap changes and covalent interaction flexibility enhancing second harmonic generation responses in d10 metal chalcogenides11Modifying Disordered Sites with Rational Cations to Regulate Band-Gaps and Second Harmonic Generation Responses Markedly: Ba6Li2ZnSn4S16 vs Ba6Ag2ZnSn4S16 vs Ba6Li2.67Sn4.33S1625Zn 3 P 2 S 8 : A Promising Infrared Nonlinear-Optical Material with Excellent Overall Properties70Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59Rational Design of a LiNbO3-like Nonlinear Optical Crystal, Li2ZrTeO6, with High Laser-Damage Threshold and Wide Mid-IR Transparency Window152Cu2EuMQ4 (M = Si, Ge; Q = S, Se): Syntheses, structure study and physical properties determination26Recent advances and future perspectives on infrared nonlinear optical metal halides223Recent progress on new infrared nonlinear optical materials with application prospect133Adjustable optical nonlinearity in d 10 cations containing chalcogenides via dp hybridization interaction13Ag 7 TaSe 6 : a new noncentrosymmetric selenide with fascinating “three in one” coordination modes and a strong second harmonic generation response13From CuFeS 2 to Ba 6 Cu 2 FeGe 4 S 16 : rational band gap engineering achieves large second-harmonic-generation together with high laser damage threshold22Partial substitution induced centrosymmetric to noncentrosymmetric structure transformation and promising second-order nonlinear optical properties of (K 0.38 Ba 0.81 )Ga 2 Se 495SnGa 2 GeSe 6 , a benign addition to the AMIII2M IV Q 6 family: synthesis, crystal structure and nonlinear optical performance20Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation66Broadening Frontiers of Infrared Nonlinear Optical Materials with π-Conjugated Trigonal-Planar Groups67Zeolitic Open-Framework Borates with Noncentrosymmetric Structures and Nonlinear Optical Properties24Two Non-π-Conjugated Deep-UV Nonlinear Optical Sulfates268[Ge2S5(S2)]4−, A NLO‐Active Unit Leading to an Asymmetric Structure Discovered in Li2Cs4Ge2S5(S2)Cl2: An Experimental and Theoretical study18Balanced Second-Order Nonlinear Optical Properties of Adducts CHI3·(S8)3 and AsI3·(S8)3: A Systematic Survey48BaHgGeSe 4 and SrHgGeSe 4 : Two New Hg-Based Infrared Nonlinear Optical Materials142Synthesis, Structure, and Characterization of Two Mixed-Cation Quaternary Chalcogenides K2BaSnQ4 (Q = S, Se)19Highly Polarizable Hg2+ Induced a Strong Second Harmonic Generation Signal and Large Birefringence in LiHgPO4265AHgSnQ4 (A = Sr, Ba; Q = S, Se): A Series of Hg-Based Infrared Nonlinear-Optical Materials with Strong Second-Harmonic-Generation Response and Good Phase Matchability76Ba 8 SrPb 24 O 24 Cl 18 : the first alkali-earth metal lead( ii ) oxyhalide with an intriguing multimember-ring layer9Li4HgSn2Se7: The First Second-Order Nonlinear Optical-Active Selenide in the I4–II–IV2–VI7 Diamond-like Family32How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates327Li[LiCs2Cl][Ga3S6]: A Nanoporous Framework of GaS4 Tetrahedra with Excellent Nonlinear Optical Performance172Li[LiCs2Cl][Ga3S6]: A Nanoporous Framework of GaS4 Tetrahedra with Excellent Nonlinear Optical Performance40Novel cyclic and linearizing cyclic Pd(II) nanohoop-based cordination complexes achieving nonlinear optical activity transparency trade-off optimization6An unprecedented planar π-conjugated [B 2 P 5 ] 5− group with ultra-large birefringence and nonlinearity: an ab initio study17K5(W3O9F4)(IO3): An Efficient Mid-Infrared Nonlinear Optical Compound with High Laser Damage Threshold114A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48A highly distorted HgS 4 tetrahedron-induced moderate second-harmonic generation response of EuHgGeS 462Abnormal bandgap enlargement resulted in a promising mid-infrared nonlinear optical material Rb 2 CdBrI 3 with an ultrahigh laser damage threshold10Ba 6 In 6 Zn 4 Se 19 : a high performance infrared nonlinear optical crystal with [InSe 3 ] 3− trigonal planar functional motifs22Coordinated 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 materials28Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145Mixed-metal thiophosphate CuCd 3 PS 6 : an infrared nonlinear optical material activated by its three-in-one tetrahedra-stacking architecture33New quaternary chalcogenide Ba 4 HgAs 2 S 10 originating from the combination of linear [HgS 2 ] 2− and tetrahedral [AsS 4 ] 3− modules8Non-centrosymmetric sulfides A 2 Ba 6 MnSn 4 S 16 (A = Li, Ag): syntheses, structures and properties21Ca 2 B 5 O 9 Cl and Sr 2 B 5 O 9 Cl: Nonlinear Optical Crystals with Deep-Ultraviolet Transparency Windows46Infrared Nonlinear Optical Polymorphs α- and β-SrCu 2 SnS 4 Exhibiting Large Second Harmonic Generation Responses with Requisite Phase-Matching Behavior44Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement97Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials164Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials55Enhancement of Second-Order Optical Nonlinearity in a Lutetium Selenite by Monodentate Anion Partial Substitution58Hexagonal In2Se3: A Defect Wurtzite-Type Infrared Nonlinear Optical Material with Moderate Birefringence Contributed by Unique InSe5 Unit75HgCuPS4: An Exceptional Infrared Nonlinear Optical Material with Defect Diamond-like Structure146Functional Chalcogenide Na2HgSn2Se6 and K2MnGe2Se6 Exhibiting Flexible Chain Structure and Intriguing Birefringence Tunability16A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses63Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials131Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties166Pb18O8Cl15I5: A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties29Hierarchical Contribution of Anions to Second Harmonic Generation in A2HgI4 (A = Na, Ag, Cu) Regulated Dramatically by Metal Cations4Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm38Chalcophosphates: A Treasure House of Infrared Nonlinear Optical Materials75Synthesis, Crystal Structures, Spectroscopic Characterization, and Thermal Analyses of the New Bismuth Sulfates NaBi(SO4)2·H2O and ABi(SO4)2 (A = K, Rb, Cs)5AMnAs3S6 (A = Cs, Rb): Phase-Matchable Infrared Nonlinear Optical Functional Motif [As3S6]3– Obtained via Surfactant–Thermal Method32A new nonlinear optical sulfate of layered structure: Cs2Zn2(SO4)319From AgGaS 2 to AgHgPS 4 : vacancy defects and highly distorted HgS 4 tetrahedra double-induced remarkable second-harmonic generation response68A novel promising infrared nonlinear optical selenide KAg 3 Ga 8 Se 14 designed from benchmark AgGaQ 2 (Q = S, Se)55Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95Ba 3 [Al(PO 4 ) 3 ]: rational design of a promising deep-UV transparent SHG crystal with balanced overall performance originating from the condensation of quartz-type [Al(PO 4 ) 4 ] 9− units16Ba 2 Ge 2 Te 5 : a ternary NLO-active telluride with unusual one-dimensional helical chains and giant second harmonic-generation tensors31Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering145Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2Hg 3 (Te 3 O 8 )(SO 4 ): a new sulfate tellurite with a novel structure and large birefringence explored from d 10 metal compounds39M 6 PS 5 X (M = Ag, Cu; X = Cl, Br) chalcohalides exhibiting strong nonlinear optical responses and high laser damage resistances9New nonlinear optical-active AAgGa 6 S 10 (A = K, Rb, Cs) featuring {[AgGa 6 S 10 ] − } ∞ framework and high laser damage threshold42A Series of Pentanary Salt-Inclusion Chalcogenoborates Containing a B12Q12 (Q = S, Se) Cluster Exhibiting a Kleinman-Forbidden Frequency-Doubling Effect25Ternary rare-earth sulfides RE3GaS6 (RE = Ho, Er): Crystal chemistry, second-order nonlinear optical properties and theoretical investigation18Inorganic Chalcogenides: From Zero‐Dimensional Clusters to Three‐Dimensional Frameworks5AXHg3P2S8 (A = Rb, Cs; X = Cl, Br): New Excellent Infrared Nonlinear Optical Materials with Mixed‐Anion Chalcohalide Groups of Trigonal Planar [HgS2X]3− and Tetrahedral [HgS3X]5−58Structure-performance relationship in tri-coordinated nonlinear optical materials toward optimal second harmonic generation and phase matching31A3Te(Zn2Ge)Ge2O14 (A = Sr, Ba, and Pb): New Langasite Mid-infrared Nonlinear Optical Materials by Rational Chemical Substitution32Highly Distorted [HgS 4 ] Motif-Driven Structural Symmetry Degradation and Strengthened Second-Harmonic Generation Response in the Defect Diamond-Like Chalcogenide Hg 3 P 2 S 847A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation22A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation64Transition-metal-based chalcogenides: A rich source of infrared nonlinear optical materials184Helical {[HgS]} n Chain-Induced Balanced Nonlinear-Optical Performance for Trigonal Mercury Sulfide29Investigation into Structural Variation from 3D to 1D and Strong Second Harmonic Generation of the AHgPS4 (A+ = Na+, K+, Rb+, Cs+) Family26Highly polarized [GeOTe 3 ] motif-driven structural order promotion and an enhanced second harmonic generation response in the new nonlinear optical oxytelluride Ba 3 Ge 2 O 4 Te 334AAl3P6O20 (A = Rb, Cs): Two deep-ultraviolet transparent nonlinear optical materials designed by aliovalent substitution11Halogen-Ion-Induced Structural Phase Transition Giving a Polymorph of HgBr2 with Balanced Nonlinear Optical Properties8Hg-based chalcogenides: An intriguing class of infrared nonlinear optical materials129Structural modification from centrosymmetric Rb 4 Hg 2 Ge 2 S 8 to noncentrosymmetric (Na 3 Rb)Hg 2 Ge 2 S 8 : mixed alkali metals strategy for infrared nonlinear optical material design28Recent Development of Non-π-Conjugated Deep Ultraviolet Nonlinear Optical Materials106[Retracted] Application Value Analysis of Nanooptical Materials in Martial Art Single‐Kick Protective Equipment1Ba 2 HgTe 5 : a Hg-based telluride with giant birefringence induced by linear [HgTe 2 ] units17Ba 6 In 2 Ge 2 Te 15 : a THz birefringent material with an intriguing quasi-[Te 5 ] 4− chain possessing large optical anisotropy and an ultrawide transmission range7Interesting dimensional transition through changing cations as the trigger in multinary thioarsenates displaying variable photocurrent response and optical anisotropy22Lead Tellurite Crystals BaPbTe2O6 and PbVTeO5F with Large Nonlinear-/Linear-Optical Responses due to Active Lone Pairs and Distorted Octahedra20Two non-centrosymmetric scandium borate nonlinear optical crystals containing the B5O10 anion group26SrZnSnSe4: A quaternary selenide with large second harmonic generation and birefringence40Infrared nonlinear optical performances of a new sulfide β-PbGa2S415Material research from the viewpoint of functional motifs103NaGa3Se5: An Infrared Nonlinear Optical Material with Balanced Performance Contributed by Complex {[Ga3Se5]−}∞ Anionic Network14BaSi7P10 and SrSi7P10: Two Infrared Nonlinear Optical Phosphides with T2 Supertetrahedra Exhibiting Strong Second‐Harmonic Generation Effects22AgGaSe2-Inspired Nonlinear Optical Materials: Tetrel Selenides of Alkali Metals and Mercury34Hg2P2S6: A layered mercury hexathiodiphosphate (IV) with large birefringence11Ba 3 HgGa 2 S 7 : A Zero-Dimensional Quaternary Sulfide Featuring a Unique [Hg 2 Ga 4 S 14 ] 12– String and Exhibiting a High Photocurrent Response27KC9H5O6(H2O): A Promising UV Nonlinear-Optical Material with Large Birefringence Based on a π-Conjugated (C9H5O6)−Group11Ag[SC(NH2)2]2F: A Laser Damage-Tolerant Infrared Nonlinear Optical Material9Achieving Large Second Harmonic Generation Effects via Optimal Planar Alignment of Triangular Units64Na 2 Ba[Na 2 Sn 2 S 7 ]: Structural Tolerance Factor‐Guided NLO Performance Improvement50Na2Ba[Na2Sn2S7]: Structural Tolerance Factor‐Guided NLO Performance Improvement0

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