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RESEARCH PAPER · Chemical Science · 2016

[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 thresholds

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[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 thresholdsOriginalNa 9 Sb(Ge 2 Q 6 ) 2 (Q = S, Se): two new antimony( iii ) quaternary chalcogenides with ethane-like [Ge 2 Q 6 ] 6− ligands12Infrared 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 materials433A series of pentanary inorganic supramolecular sulfides (A 3 X)[MB 12 (MS 4 ) 3 ] (A = K, Cs; X = Cl, Br, I; M = Ga, In, Gd) featuring B 12 S 12 clusters54Ba 6 Li 2 CdSn 4 S 16 : lithium substitution simultaneously enhances band gap and SHG intensity44Li 2 CdGeSe 4 and Li 2 CdSnSe 4 : biaxial nonlinear optical materials with strong infrared second-order responses and laser-induced damage thresholds influenced by photoluminescence54Na 2 CdGe 2 Q 6 (Q = S, Se): two metal-mixed chalcogenides with phase-matching abilities and large second-harmonic generation responses77Tailored synthesis of nonlinear optical quaternary chalcohalides: Ba 4 Ge 3 S 9 Cl 2 , Ba 4 Si 3 Se 9 Cl 2 and Ba 4 Ge 3 Se 9 Cl 252Two excellent phase-matchable infrared nonlinear optical materials based on 3D diamond-like frameworks: RbGaSn 2 Se 6 and RbInSn 2 Se 639Superpolyhedron-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 Relationship338K2ZnSn3Se8: A Non‐Centrosymmetric Zinc Selenidostannate(IV) Featuring Interesting Covalently Bonded [ZnSn3Se8]2− Layer and Exhibiting Intriguing Second Harmonic Generation Activity19Ba 6 Zn 7 Ga 2 S 16 : A Wide Band Gap Sulfide with Phase-Matchable Infrared NLO Properties110Coexistence of Strong Second Harmonic Generation Response and Wide Band Gap in AZn4Ga5S12 (A=K, Rb, Cs) with 3D Diamond‐like Frameworks65AgGa2PS6: A New Mid‐Infrared Nonlinear Optical Material with a High Laser Damage Threshold and a Large Second Harmonic Generation Response78Large Second-Harmonic Generation Responses Achieved by the Dimeric [Ge2Se4(μ-Se2)]4– Functional Motif in Polar Polyselenides A4Ge4Se12 (A = Rb, Cs)49Li7(TeO3)3F: A Lithium Fluoride Tellurite with Large Second Harmonic Generation Responses and a Short Ultraviolet Cutoff Edge39Absorption and Mid-IR SHG in Two-Dimensional Halogen and Hydrogen Saturated Silicene Series12Experimental and theoretical studies on the NLO properties of two quaternary non-centrosymmetric chalcogenides: BaAg 2 GeS 4 and BaAg 2 SnS 468Design and synthesis of a nonlinear optical material BaAl 4 S 7 with a wide band gap inspired from SrB 4 O 763First principle study of nonlinear optical crystals15Na 6 Zn 3 MIII2Q 9 (M III = Ga, In; Q = S, Se): four new supertetrahedron-layered chalcogenides with unprecedented vertex-sharing T 3 -clusters and desirable photoluminescence performances31NaBaM III Q 3 (M III = Al, Ga; Q = S, Se): first quaternary chalcogenides with isolated edge-sharing (MIII2Q 6 ) 6− dimers8New strategy for designing promising mid-infrared nonlinear optical materials: narrowing the band gap for large nonlinear optical efficiencies and reducing the thermal effect for a high laser-induced damage threshold142Oxyhalides: prospecting ore for optical functional materials with large laser damage thresholds76Designing Two-Dimensional KBBF Family Second-Harmonic Generation Monolayers19Strong SHG Response via High Orientation of Tetrahedral Functional Motifs in Polyselenide A2Ge4Se10 (A = Rb, Cs)31LiGa 2 PS 6 and LiCd 3 PS 6 : Molecular Designs of Two New Mid-Infrared Nonlinear Optical Materials88Modifying Disordered Sites with Rational Cations to Regulate Band-Gaps and Second Harmonic Generation Responses Markedly: Ba6Li2ZnSn4S16 vs Ba6Ag2ZnSn4S16 vs Ba6Li2.67Sn4.33S1625A review on structure-performance relationship toward the optimal design of infrared nonlinear optical materials with balanced performances252Recent advances and future perspectives on infrared nonlinear optical metal halides223Solid-State Preparation, Structural Characterization, Physical Properties, and Theoretical Studies of a Series of Novel Rare-Earth Metal Chalcogenides with Unprecedented Closed-Cavities15An unprecedented pentanary chalcohalide with Mn atoms in two chemical environments: unique bonding characteristics and magnetic properties29Experimental study on nonlinear−optical property of Ag4P2Se66A 2 SrM IV S 4 (A = Li, Na; M IV = Ge, Sn) concurrently exhibiting wide bandgaps and good nonlinear optical responses as new potential infrared nonlinear optical materials78Combined experimental and theoretical investigations of Ba 3 GaS 4 I: interesting structural transformation originated from halogen substitution16SrCdSnQ 4 (Q = S and Se): infrared nonlinear optical chalcogenides with mixed NLO-active and synergetic distorted motifs68Structural modulation induced by M IIIA metals in Ba 3 MQ 4 X (M = Al, Ga, In; Q = S, Se; X = Cl, Br): an experimental and computational analysis7Synthesis and nonlinear optical properties of new gallium thiophosphate Rb 2 Ga 2 P 2 S 913Theoretical Design of Layered AlGaS3 as a New Nonlinear Optical Material with a Strong Second Harmonic Generation Response5Balanced Second-Order Nonlinear Optical Properties of Adducts CHI3·(S8)3 and AsI3·(S8)3: A Systematic Survey48Sr 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 Groups22Large Second Harmonic Generation (SHG) Effect and High Laser‐Induced Damage Threshold (LIDT) Observed Coexisting in Gallium Selenide188Large Second Harmonic Generation (SHG) Effect and High Laser‐Induced Damage Threshold (LIDT) Observed Coexisting in Gallium Selenide48[(Ba19Cl4)(Ga6Si12O42S8)]: a Two-Dimensional Wide-Band-Gap Layered Oxysulfide with Mixed-Anion Chemical Bonding and Photocurrent Response20Mixed-Anion Inorganic Compounds: A Favorable Candidate for Infrared Nonlinear Optical Materials140Li[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 Performance40A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48Rational design of infrared nonlinear optical chalcogenides by chemical substitution287A new type of novel salt-inclusion chalcogenide with ultralow thermal conductivity14A review of the AI2B II C IV DVI4 family as infrared nonlinear optical materials: the effect of each site on the structure and optical properties59Ba 13 In 12 Zn 7 S 38 and Ba 12 In 12 Zn 8 Se 38 : infrared nonlinear optical chalcogenides designed by zinc-induced non-centrosymmetry transformation22Experimental and theoretical studies of the ternary thiophosphate PbPS 3 featuring ethane-like [P 2 S 6 ] 4− units15Li 2 CdSiS 4 , a promising IR NLO material with a balanced E g and SHG response originating from the effect of Cd with d 10 configuration36Non-centrosymmetric sulfides A 2 Ba 6 MnSn 4 S 16 (A = Li, Ag): syntheses, structures and properties21Salt-inclusion chalcogenides: an emerging class of IR nonlinear optical materials54Designing Sulfide Borate as a Novel Type of Second-Order Nonlinear-Optical Material91Infrared Nonlinear Optical Polymorphs α- and β-SrCu 2 SnS 4 Exhibiting Large Second Harmonic Generation Responses with Requisite Phase-Matching Behavior44One-Dimensional Double Chains in Sodium-Based Quaternary Chalcogenides Displaying Intriguing Red Emission and Large Optical Anisotropy17LiGa0.54In0.46S2: A new infrared nonlinear optical material with large laser damage threshold designed by gallium substitution in LiInS223Lead 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 Materials55NaGaS2: An Elusive Layered Compound with Dynamic Water Absorption and Wide‐Ranging Ion‐Exchange Properties26NaGaS2: An Elusive Layered Compound with Dynamic Water Absorption and Wide‐Ranging Ion‐Exchange Properties8[ABa2Cl][Ga4S8] (A = Rb, Cs): Wide-Spectrum Nonlinear Optical Materials Obtained by Polycation-Substitution-Induced Nonlinear Optical (NLO)-Functional Motif Ordering269Partial Isovalent Anion Substitution to Access Remarkable Second-Harmonic Generation Response: A Generic and Effective Strategy for Design of Infrared Nonlinear Optical Materials114Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials130Structure-property survey and computer-assisted screening of mid-infrared nonlinear optical chalcohalides113Second-order nonlinear optical-active selenide borate Zn8Se2(BO2)12: Experimental and theoretical analysis9Evaluation of nonlinear optical properties of quaternary chalcogenide halides Ba4Si3Se9Br2 and Ba4Ge3Se9Br222New photoluminescence hybrid perovskites with ultrahigh photoluminescence quantum yield and ultrahigh thermostability temperature up to 600 K67Salt-Inclusion Chalcogenide [Ba4Cl2][ZnGa4S10]: Rational Design of an IR Nonlinear Optical Material with Superior Comprehensive Performance Derived from AgGaS2134Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties165Pb18O8Cl15I5: 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 Materials75Two Mixed-Anion Units of [GeOSe3] and [GeO3S] Originating from Partial Isovalent Anion Substitution and Inducing Moderate Second Harmonic Generation Response and Large Birefringence55Second Harmonic Generation Susceptibilities from Symmetry Adapted Wannier Functions178AMnAs3S6 (A = Cs, Rb): Phase-Matchable Infrared Nonlinear Optical Functional Motif [As3S6]3– Obtained via Surfactant–Thermal Method32α-CdP2: Large SHG Effect Originating from the Synergism of Parallel ∞1[P–] Polyanion Chains and Distorted CdP4 Tetrahedra21From AgGaS 2 to AgHgPS 4 : vacancy defects and highly distorted HgS 4 tetrahedra double-induced remarkable second-harmonic generation response67A New Nonlinear Optical Selenide Crystal AgLiGa 2 Se 4 with Good Comprehensive Performance in Mid‐Infrared Region44Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95[GaF(H 2 O)][IO 3 F]: a promising NLO material obtained by anisotropic polycation substitution42Design and synthesis of Ba 3 SiSe 5 with suitable birefringence modulated via M IV atoms in the Ba–M IV –Q (M IV = Si, Ge; Q = S, Se) system3From thiophosphate to chalcohalide: mixed-anion AgS x Cl y ligands concurrently enhancing nonlinear optical effects and laser-damage threshold10La 6 Cd 0.75 Ga 2 Q 11.5 Cl 2.5 (Q = S and Se): two new nonlinear optical chalcohalides with a large laser-induced damage threshold15M 6 PS 5 X (M = Ag, Cu; X = Cl, Br) chalcohalides exhibiting strong nonlinear optical responses and high laser damage resistances9Na 2 GaS 2 Cl: a new sodium-rich chalcohalide with two-dimensional [GaS 2 ] ∞ layers and wide interlayer space15New nonlinear optical-active AAgGa 6 S 10 (A = K, Rb, Cs) featuring {[AgGa 6 S 10 ] − } ∞ framework and high laser damage threshold42Structural diversities in centrosymmetric La 8 S 4 Cl 8 La 12 S 8 Cl 4 [SbS 3 ] 8 and non-centrosymmetric Ln 12 S 8 Cl 8 [SbS 3 ] 4 (Ln = La and Ce): syntheses, crystal and electronic structures, and optical properties10Synthesis, crystal structure and physical properties of a new chalcogenides Rb3Ga3Ge7S208Noncentrosymmetric Tetrel Pnictides RuSi4P4 and IrSi3P3: Nonlinear Optical Materials with Outstanding Laser Damage Threshold47Quaternary Chalcohalides CdSnSX2 (X = Cl or Br) with Neutral Layers: Syntheses, Structures, and Photocatalytic Properties18LaSiP3 and LaSi2P6: Two Excellent Rare‐Earth Pnictides with Strong SHG Responses as Mid‐ and Far‐Infrared Nonlinear Optical Crystals36AXHg3P2S8 (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]5−58Li 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 Gap15Highly 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 846Hg 3 P 2 S 8 : A New Promising Infrared Nonlinear Optical Material with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold111Structural, theoretical and third order nonlinear optical properties of (E)-N’-(4-chlorobenzylidene)-4-fluorobenzohydrazide monohydrate3The Rise of Infrared Nonlinear Optical Pnictides: Advances and Outlooks36Superior Infrared Nonlinear Optical Performance Achieved by Synergetic Functional Motif and Vacancy Site Modulations48Investigation into Structural Variation from 3D to 1D and Strong Second Harmonic Generation of the AHgPS4 (A+ = Na+, K+, Rb+, Cs+) Family26Designing 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) Crystal13β-BaGa 4 Se 7 : a promising IR nonlinear optical crystal designed by predictable structural rearrangement46Cd7SiAs6, a Nonchalcopyrite Arsenide with a Strong Nonlinear-Optical Response9Complex coordinated functional groups: A great genes for nonlinear optical materials64First-principles study of opto-electronic and thermoelectric properties of SrCdSnX4 (X=S, Se, Te) alkali metal chalcogenides34[ASr 4 Cl][Ge 3 S 10 ] (A = Na, K) and [KBa 4 Cl][Ge 3 S 10 ]: new salt-inclusion infrared nonlinear optical crystals with zero-dimensional [Ge 3 S 9 ] clusters32AIn 4 S 6 Cl (A = Rb and Cs) and Pb 5 Sn 3 Q 10 Cl 2 (Q = S and Se): quaternary chalcohalides with mixed anionic coordination exhibit photocurrent responses11Bridging oxygen atoms in trigonal prism units driven strong second-harmonic-generation efficiency in Sr 3 Ge 2 O 4 Te 318First polar quaternary sulphide CsLiGa 6 S 10 with mixed ordered alkali cations displaying excellent infrared nonlinear optical properties16From 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 materials19KNa 0.78 Eu 0.27 In 3.80 B 12 S 12 : a novel hexanary thioborate featuring a B 12 S 12 cluster and diverse InS x ( x = 4, 5, 6) units9Metal oxyhalides: an emerging family of nonlinear optical materials124Pb 3 SBrI 3 : the first Pb-based chalcohalide with multiple halogens features a unique two-dimensional structure composed of diverse Pb-centered polyhedra12Rational design via dual-site aliovalent substitution leads to an outstanding IR nonlinear optical material with well-balanced comprehensive properties68The synthesis and structure–property relation analysis of metal chalcohalide crystals Cs 2 InPS 4 X 2 (X = Cl, Br) with mixed anions6A new salt-inclusion chalcogenide exhibiting distinctive [Cd11In9S26]3− host framework and decent nonlinear optical performances16Optimizing the Nonlinear Optical Performance of an A-N-M-Q (A: Alkali Metal; N: d10 Metal; M: Main Group Metal; Q: Chalcogen) System44Material research from the viewpoint of functional motifs103RbBiP2S6: A Promising IR Nonlinear Optical Material with a Giant Second-Harmonic Generation Response Designed by Aliovalent Substitution80BaSi7P10 and SrSi7P10: Two Infrared Nonlinear Optical Phosphides with T2 Supertetrahedra Exhibiting Strong Second‐Harmonic Generation Effects22Hg2P2S6: A layered mercury hexathiodiphosphate (IV) with large birefringence11[Cs6Cl][Ga5GeQ12] (Q = S, Se): two novel porous layered chalcohalides exhibiting two-band emission and ion exchange properties6Ag[SC(NH2)2]2F: A Laser Damage-Tolerant Infrared Nonlinear Optical Material9Synthesis, Crystal and Electronic Structures, Nonlinear Optical Properties, and Magnetic Properties of Two Thiophosphates: KInP2S7 and KCrP2S79Syntheses, structures, and characterization of new heteroanionic chalcohalides: Na2Ba17In8Q21F18 (Q = S, Se), KBa2InQ3F2 (Q = S, Se)5Ba5Ga2SiO4S6: a Phase-Matching Nonlinear Optical Oxychalcogenide Design via Structural Regulation Originated from Heteroanion Introduction25Oxychalcogenides: A Promising Class of Materials for Nonlinear Optical Crystals with Mixed‐Anion Groups35Recent Advances in Infrared Nonlinear Optical Crystal7[Sr 4 Cl 2 ][Si 3 S 9 ]: Ultrawide-bandgap salt-inclusion thiosilicate nonlinear optical material with unprecedented tri-polymerized [Si 3 S 9 ] clusters21LaAeAl 3 S 7 (Ae = Ca, Sr): Cairo pentagonal layered thioaluminates achieving a good balance between a strong second harmonic generation response and a wide bandgap23Revisiting two thiophosphate compounds constituting d 0 transition metal HfP 2 S 6 and d 10 transition metal α-Ag 4 P 2 S 6 as multifunctional materials for combining second harmonic generation response and photocurrent response12Intense d‐p Hybridization in Nb3O15 Tripolymer Induced the Largest Second Harmonic Generation Response and Birefringence in Germanates51Intense d‐p Hybridization in Nb3O15 Tripolymer Induced the Largest Second Harmonic Generation Response and Birefringence in Germanates7Polar Phosphorus Chalcogenide Cage Molecules: Enhancement of Nonlinear Optical Properties in Adducts38Polar Phosphorus Chalcogenide Cage Molecules: Enhancement of Nonlinear Optical Properties in Adducts1Tunable Salt-Inclusion Chalcogenides for Ion Exchange, Photoluminescence, and Scintillation12Salt-inclusion chalcogenides: Double functional moieties design strategy toward excellent nonlinear optical materials12Recent progress in the design of IR nonlinear optical materials by partial chemical substitution: Structural evolution and performance optimization133Rational Design of a Rare‐Earth Oxychalcogenide Nd3[Ga3O3S3][Ge2O7] with Superior Infrared Nonlinear Optical Performance64[K2PbX][Ga7S12] (X = Cl, Br, I): The First Lead‐Containing Cationic Moieties with Ultrahigh Second‐Harmonic Generation and Band Gaps Exceeding the Criterion of 2.33 eV46Chain‐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 Materials5

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  1. Na 9 Sb(Ge 2 Q 6 ) 2 (Q = S, Se): two new antimony( iii ) quaternary chalcogenides with ethane-like [Ge 2 Q 6 ] 6− ligands

    RSC Advances · 2016-01-01

    Xiaowen Wu, Yi Hu, Hui Pan, Zhi Su

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  2. Infrared SHG Materials CsM3Se6 (M = Ga/Sn, In/Sn): Phase Matchability Controlled by Dipole Moment of the Asymmetric Building Unit

    Chemistry of Materials · 2016-12-26

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  3. Recent achievements on middle and far-infrared second-order nonlinear optical materials

    Coordination Chemistry Reviews · 2016-12-27

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  4. A series of pentanary inorganic supramolecular sulfides (A 3 X)[MB 12 (MS 4 ) 3 ] (A = K, Cs; X = Cl, Br, I; M = Ga, In, Gd) featuring B 12 S 12 clusters

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  5. Ba 6 Li 2 CdSn 4 S 16 : lithium substitution simultaneously enhances band gap and SHG intensity

    Journal of Materials Chemistry C · 2017-01-01

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  6. Li 2 CdGeSe 4 and Li 2 CdSnSe 4 : biaxial nonlinear optical materials with strong infrared second-order responses and laser-induced damage thresholds influenced by photoluminescence

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  9. Two excellent phase-matchable infrared nonlinear optical materials based on 3D diamond-like frameworks: RbGaSn 2 Se 6 and RbInSn 2 Se 6

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  10. Superpolyhedron-Built Second Harmonic Generation Materials Exhibit Large Mid-Infrared Conversion Efficiencies and High Laser-Induced Damage Thresholds

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  12. K2ZnSn3Se8: A Non‐Centrosymmetric Zinc Selenidostannate(IV) Featuring Interesting Covalently Bonded [ZnSn3Se8]2− Layer and Exhibiting Intriguing Second Harmonic Generation Activity

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  14. Coexistence of Strong Second Harmonic Generation Response and Wide Band Gap in AZn4Ga5S12 (A=K, Rb, Cs) with 3D Diamond‐like Frameworks

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  15. AgGa2PS6: A New Mid‐Infrared Nonlinear Optical Material with a High Laser Damage Threshold and a Large Second Harmonic Generation Response

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  16. Large Second-Harmonic Generation Responses Achieved by the Dimeric [Ge2Se4(μ-Se2)]4– Functional Motif in Polar Polyselenides A4Ge4Se12 (A = Rb, Cs)

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  17. Li7(TeO3)3F: A Lithium Fluoride Tellurite with Large Second Harmonic Generation Responses and a Short Ultraviolet Cutoff Edge

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  19. Experimental and theoretical studies on the NLO properties of two quaternary non-centrosymmetric chalcogenides: BaAg 2 GeS 4 and BaAg 2 SnS 4

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  20. Design and synthesis of a nonlinear optical material BaAl 4 S 7 with a wide band gap inspired from SrB 4 O 7

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  21. First principle study of nonlinear optical crystals

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  22. Na 6 Zn 3 MIII2Q 9 (M III = Ga, In; Q = S, Se): four new supertetrahedron-layered chalcogenides with unprecedented vertex-sharing T 3 -clusters and desirable photoluminescence performances

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  23. NaBaM III Q 3 (M III = Al, Ga; Q = S, Se): first quaternary chalcogenides with isolated edge-sharing (MIII2Q 6 ) 6− dimers

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  24. New strategy for designing promising mid-infrared nonlinear optical materials: narrowing the band gap for large nonlinear optical efficiencies and reducing the thermal effect for a high laser-induced damage threshold

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  25. Oxyhalides: prospecting ore for optical functional materials with large laser damage thresholds

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  27. Strong SHG Response via High Orientation of Tetrahedral Functional Motifs in Polyselenide A2Ge4Se10 (A = Rb, Cs)

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  28. LiGa 2 PS 6 and LiCd 3 PS 6 : Molecular Designs of Two New Mid-Infrared Nonlinear Optical Materials

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

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  30. A review on structure-performance relationship toward the optimal design of infrared nonlinear optical materials with balanced performances

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  31. Recent advances and future perspectives on infrared nonlinear optical metal halides

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