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RESEARCH PAPER · Chemistry of Materials · 2013

Ba8Sn4S15: A Strong Second Harmonic Generation Sulfide with Zero-Dimensional Crystal Structure

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Ba8Sn4S15: A Strong Second Harmonic Generation Sulfide with Zero-Dimensional Crystal StructureOriginalSHG Materials SnGa4Q7 (Q = S, Se) Appearing with Large Conversion Efficiencies, High Damage Thresholds, and Wide Transparencies in the Mid-Infrared Region141ChemInform Abstract: Ba8Sn4S15: A Strong Second Harmonic Generation Sulfide with Zero‐Dimensional Crystal Structure.0Ag 3 Ga 3 SiSe 8 : a new infrared nonlinear optical material with a chalcopyrite structure34Optical Nonlinearity in Cu2CdSnS4 and α/β-Cu2ZnSiS4: Diamond-like Semiconductors with High Laser-Damage Thresholds87Designing the syntheses and photophysical simulations of noncentrosymmetric compounds17Syntheses, structures, and optical properties of Ba 4 Ga 4 SnSe 12 and Ba 6 Ga 2 SnSe 1119Infrared nonlinear optical properties of lithium-containing diamond-like semiconductors Li 2 ZnGeSe 4 and Li 2 ZnSnSe 457Synthesis and characterization of a new mid-infrared transparent compound: acentric Ba 5 In 4 Te 4 S 713PbGa2MSe6 (M = Si, Ge): Two Exceptional Infrared Nonlinear Optical Crystals131Synthesis, crystal structure and optical property of a novel metal chalcohalide: ZnHg3Se2Cl47Metal Thiophosphates with Good Mid-infrared Nonlinear Optical Performances: A First-Principles Prediction and Analysis441All-metal electride molecules CuAg@Ca 7 M (M = Be, Mg, and Ca) with multi-excess electrons and all-metal polyanions: molecular structures and bonding modes as well as large infrared nonlinear optical responses27[A 3 X][Ga 3 PS 8 ] (A = K, Rb; X = Cl, Br): promising IR non-linear optical materials exhibiting concurrently strong second-harmonic generation and high laser induced damage thresholds189Crystal and electronic structures, and photoluminescence and photocatalytic properties of α-EuZrS 326Pb 5 Ga 6 ZnS 15 : a noncentrosymmetric framework with chains of T2-supertetrahedra41Synthesis, crystal structure and second-order nonlinear optical property of a novel pentanary selenide (K 3 I)[InB 12 (InSe 4 ) 3 ]48The structure and band gap design of high Si doping level Ag1−xGa1−xSixSe2 (x=1/2)15Na 2 Hg 3 M 2 S 8 (M = Si, Ge, and Sn): New Infrared Nonlinear Optical Materials with Strong Second Harmonic Generation Effects and High Laser-Damage Thresholds186Na 2 ZnGe 2 S 6 : A New Infrared Nonlinear Optical Material with Good Balance between Large Second-Harmonic Generation Response and High Laser Damage Threshold302A High Laser Damage Threshold and a Good Second-Harmonic Generation Response in a New Infrared NLO Material: LiSm3SiS725Analysis and prediction of mid-IR nonlinear optical metal sulfides with diamond-like structures336Non‐centrosymmetric Selenides AZn4In5Se12 (A=Rb, Cs): Synthesis, Characterization and Nonlinear Optical Properties47Infrared SHG Materials CsM3Se6 (M = Ga/Sn, In/Sn): Phase Matchability Controlled by Dipole Moment of the Asymmetric Building Unit102Recent achievements on middle and far-infrared second-order nonlinear optical materials433Ba 6 Li 2 CdSn 4 S 16 : lithium substitution simultaneously enhances band gap and SHG intensity44BaCu 2 M IV Q 4 (M IV = Si, Ge, and Sn; Q = S, Se): synthesis, crystal structures, optical performances and theoretical calculations54Band gap tuning from an indirect EuGa 2 S 4 to a direct EuZnGeS 4 semiconductor: syntheses, crystal and electronic structures, and optical properties20Centrosymmetric to noncentrosymmetric structural transformation of new quaternary selenides induced by isolated dimeric [Sn 2 Se 4 ] units: from Ba 8 Ga 2 Sn 7 Se 18 to Ba 10 Ga 2 Sn 9 Se 2210Syntheses and characterization of three new sulfides with large band gaps: acentric Ba 4 Ga 4 SnS 12 , centric Ba 12 Sn 4 S 23 and Ba 7 Sn 3 S 1327The first quaternary diamond-like semiconductor with 10-membered LiS 4 rings exhibiting excellent nonlinear optical performances104Two excellent phase-matchable infrared nonlinear optical materials based on 3D diamond-like frameworks: RbGaSn 2 Se 6 and RbInSn 2 Se 639Wide band gap design of new chalcogenide compounds: KSrPS 4 and CsBaAsS 422Superpolyhedron-Built Second Harmonic Generation Materials Exhibit Large Mid-Infrared Conversion Efficiencies and High Laser-Induced Damage Thresholds101Mid-Infrared Nonlinear Optical Materials Based on Metal Chalcogenides: Structure–Property Relationship338Li2HgMS4 (M = Si, Ge, Sn): New Quaternary Diamond-Like Semiconductors for Infrared Laser Frequency Conversion64Na2ZnSn2S6: A mixed-metal thiostannate with large second-harmonic generation response activated by penta-tetrahedral [ZnSn4S14]10− clusters10AgGa2PS6: A New Mid‐Infrared Nonlinear Optical Material with a High Laser Damage Threshold and a Large Second Harmonic Generation Response78Synthesis and characterization of two lead-containing metal chalcogenides: Ba5Pb2Sn3S13 and Ba6PbSn3Se137LiGaGe2S6: A Chalcogenide with Good Infrared Nonlinear Optical Performance and Low Melting Point56Design and synthesis of a nonlinear optical material BaAl 4 S 7 with a wide band gap inspired from SrB 4 O 764Four new quaternary chalcogenides A 2 Ba 7 Sn 4 Q 16 (A = Li, Na; Q = S, Se): syntheses, crystal structures determination, nonlinear optical performances investigation26K 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 performance60From AgGaS2 to Li2ZnSiS4: Realizing Impressive High Laser Damage Threshold Together with Large Second-Harmonic Generation Response134LiGa 2 PS 6 and LiCd 3 PS 6 : Molecular Designs of Two New Mid-Infrared Nonlinear Optical Materials88Crystal Structure and Optical Property of Quaternary Sulfide Ba2.77SnSb2.16S80Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials195Synthesis, Crystal Structure, and Optical Properties of Noncentrosymmetric Na2ZnSnS434Modifying Disordered Sites with Rational Cations to Regulate Band-Gaps and Second Harmonic Generation Responses Markedly: Ba6Li2ZnSn4S16 vs Ba6Ag2ZnSn4S16 vs Ba6Li2.67Sn4.33S1625Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59A facile route for synthesis of highly pure α-CaB4O7 compound12A review on the development of infrared nonlinear optical materials with triangular anionic groups38Experimental study on nonlinear−optical property of Ag4P2Se66ABaSbQ 3 (A = Li, Na; Q = S, Se): diverse arrangement modes of isolated SbQ 3 ligands regulating the magnitudes of birefringences50Investigation on two new antimony-based quaternary chalcogenides: Na 6 CdSb 4 S 10 and Na 3 CdSbSe 41Lone pair effects on ternary infrared nonlinear optical materials19Quaternary semiconductor Ba 8 Zn 4 Ga 2 S 15 featuring unique one-dimensional chains and exhibiting desirable yellow emission24Rational design of a new chalcogenide with good infrared nonlinear optical performance: SrZnSnS 452Sn 2 Ga 2 S 5 : A Polar Semiconductor with Exceptional Infrared Nonlinear Optical Properties Originating from the Combined Effect of Mixed Asymmetric Building Motifs81Ba 8 SrPb 24 O 24 Cl 18 : the first alkali-earth metal lead( ii ) oxyhalide with an intriguing multimember-ring layer9Sn2Ga2S5: A Type of IR Nonlinear-Optical Material22LiBa2MIIIQ4 (MIII = Al, Ga, In; Q = S, Se): A Series of Metal Chalcogenides with a Structural Transition12Rb10Zn4Sn4S17: A Chalcogenide with Large Laser Damage Threshold Improved from the Mn-Based Analogue28BaGe 2 Pn 2 (Pn = P, As): Two Congruent-Melting Non-chalcopyrite Pnictides as Mid- and Far-Infrared Nonlinear Optical Materials Exhibiting Large Second Harmonic Generation Effects54Nonlinear Optical Crystals for Second Harmonic Generation19Incorporating rare-earth cations with moderate electropositivity into iodates for the optimized second-order nonlinear optical performance17Non-centrosymmetric sulfides A 2 Ba 6 MnSn 4 S 16 (A = Li, Ag): syntheses, structures and properties21Raman and Infrared Phonon Spectra of Novel Nonlinear Optical Materials PbGa 2 GeS 6 and PbGa 2 GeSe 6 : Experiment and Theory4Quaternary rare-earth sulfide LaSnGa3S7: Synthesis, structure, thermal and optical properties5(Na0.60Ba0.70)Ga2Se4: An Infrared Nonlinear Optical Crystal Designed using AgGaSe2 as the Template38LiBa4Ga5Q12 (Q = S, Se): Noncentrosymmetric Metal Chalcogenides with a Cesium Chloride Topological Structure Displaying a Remarkable Laser Damage Threshold32KInSi1.32Sn0.68Se6: An Infrared Nonlinear Optical Material Containing Three Types of Tetrahedral Units19Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials131Investigation of the second-order nonlinear optical property of Sr6Sb6S173Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95Aliovalent-cation-substitution-induced structure transformation: a new path toward high-performance IR nonlinear optical materials47Halonitrides Zn 2 NX (X=Cl,Br): Novel Mid-Infrared Nonlinear Optical Materials30Introduction of Li into Ag-Based Noncentrosymmetric Sulfides for High-Performance Infrared Nonlinear Optical Materials40Inorganic Chalcogenides: From Zero‐Dimensional Clusters to Three‐Dimensional Frameworks5Phase matching achieved by isomorphous substitution in IR nonlinear optical material Ba 2 SnSSi 2 O 7 with an undiscovered [SnO 4 S] functional motif47Wide band gap thiophosphates ASrPS 4 (A = Li, Na, K, Rb, Cs): cation size effect induced successive structural transformation13Ba6(CuxZy)Sn4S16 (Z = Mg, Mn, Zn, Cd, In, Bi, Sn): High Chemical Flexibility Resulting in Good Nonlinear-Optical Properties12Solvothermal syntheses, characterizations and photocatalytic properties of two copper-rich thiostannates4Theoretical Study of Alkaline-Earth Metal (Be, Mg, and Ca)-Substituted Aluminum Nitride Nanocages With High Stability and Large Nonlinear Optical Responses2Ba6Ge2Se12 and Ba7Ge2Se17: Two Centrosymmetric Barium Seleno-Germanates with Polyatomic Anion Disorder6Stability and synthesis across barium tin sulfide material space12Two Mixed-Anion Semiconductors in the Ba–Sn–Te–S System with Low Thermal Conductivity12Structure, Second-, and Third-Harmonic Generation of Li4P2S6: A Wide Gap Material with a High Laser-Induced Damage Threshold15Vacancy‐Induced Extraordinary Second Harmonic Generation Response for Diamond‐Like Cu3PS49Phase Matching of Infrared Nonlinear Optical Salt-Inclusion Chalcogenides Achieved by the Modulation of the Fractal Dimension of Anionic Motifs18Effects of different groups on phase-matching and SHG in “3+4” Pn materials0Synthesis, Crystal Structure, and Optical Properties of a New Quaternary Tin Polychalcogenide K2BaSnSe50Impact of structural defects on the electronic and optical properties of Pb4Ga4Ge(S, Se)12 crystals2Charge Density Wave and Superconductivity in BaSbTe2S Heterolayer Crystal with 2D Te Square Nets7Stabilization of the Polar 0D Cs4Nb2–xTaxS11 with Phase-Matched Second-Harmonic Generation and High Laser-Induced Damage Threshold4Eu(II) 4 Eu(III) 2 Ge 3 S 11 O 2 : a Single‐Element Mixed‐Valence Engineering Breakthrough for Strongly Enhanced Nonlinearity and Anisotropy in Rare‐Earth Oxysulfides8Doubling Polarizability Anisotropy of The Tetrahedral Motifs to Achieve Phase Matching for Melilite-Type Compound2Structure-property relationships in IR nonlinear optical chalcogenides with stereochemically active lone pairs29Vacancy-driven tetrahedral distortion leading to exceptional second harmonic generation3Modulating Nonlinear Optical Performances in α/β-SnGa2GeS6 Polymorphs via Atomic Coordination Engineering1Ba-based IR nonlinear optical materials: synthesis, growth, structures, and properties6A stoichiometrically conserved homologous series with infinite structural diversity2Charge-order-induced directional enhancement of non-diagonal second-order nonlinear optical tensor components2KHg 4 Ga 5 S 12 : A Diamond-like Tetrahedral Chalcogenide Exhibiting Giant Phase-Matching Second Harmonic Generation6Heterovalent Coexistence‐Driven Symmetry Breaking and Dimensional Evolution: Designing Polar Heart‐Shaped Channels for Exceptional MFIR Nonlinear Optics5Laporte Selection Rule Induced the Suppression of d ‐ d Transitions and Vacancies Enhanced the Second Harmonic Generation in I 4¯‐MnGa 2 S 40

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  2. ChemInform Abstract: Ba8Sn4S15: A Strong Second Harmonic Generation Sulfide with Zero‐Dimensional Crystal Structure.

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  3. Ag 3 Ga 3 SiSe 8 : a new infrared nonlinear optical material with a chalcopyrite structure

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  4. Optical Nonlinearity in Cu2CdSnS4 and α/β-Cu2ZnSiS4: Diamond-like Semiconductors with High Laser-Damage Thresholds

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  6. Syntheses, structures, and optical properties of Ba 4 Ga 4 SnSe 12 and Ba 6 Ga 2 SnSe 11

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  10. Synthesis, crystal structure and optical property of a novel metal chalcohalide: ZnHg3Se2Cl4

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  43. Sr 5 ZnGa 6 S 15 : a new quaternary non-centrosymmetric semiconductor with a 3D framework structure displaying excellent nonlinear optical performance

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  46. Crystal Structure and Optical Property of Quaternary Sulfide Ba2.77SnSb2.16S8

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  47. Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials

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  48. Synthesis, Crystal Structure, and Optical Properties of Noncentrosymmetric Na2ZnSnS4

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  49. Modifying Disordered Sites with Rational Cations to Regulate Band-Gaps and Second Harmonic Generation Responses Markedly: Ba6Li2ZnSn4S16 vs Ba6Ag2ZnSn4S16 vs Ba6Li2.67Sn4.33S16

    Crystal Growth & Design · 2018-08-16

    Ruihuan Duan, Rui‐An Li, Pengfei Liu, Hua Lin, Yue Wang, Li‐Ming Wu

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  50. Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold

    Inorganic Chemistry · 2018-08-23

    Sheng‐Ping Guo, Zongdong Sun, Yang Chi, Huaiguo Xue

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