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RESEARCH PAPER · Journal of the American Chemical Society · 2017

New Compressed Chalcopyrite-like Li2BaMIVQ4 (MIV = Ge, Sn; Q = S, Se): Promising Infrared Nonlinear Optical Materials

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New Compressed Chalcopyrite-like Li2BaMIVQ4 (MIV = Ge, Sn; Q = S, Se): Promising Infrared Nonlinear Optical MaterialsOriginalLi 3 Ge 3 Se 6 : the first ternary lithium germanium selenide with interesting ∞ [Ge 6 Se 12 ] n chains constructed by ethane-like [Ge 2 Se 6 ] 6− clusters8A Polyselenide with a Novel Se78– Unit: the Structure of Sr19–xPbxGe11Se44 with x = 5.0 and 6.44Experimental and theoretical studies on the NLO properties of two quaternary non-centrosymmetric chalcogenides: BaAg 2 GeS 4 and BaAg 2 SnS 468First principle study of nonlinear optical crystals15Four new quaternary chalcogenides A 2 Ba 7 Sn 4 Q 16 (A = Li, Na; Q = S, Se): syntheses, crystal structures determination, nonlinear optical performances investigation26Na 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− dimers8RbSe 3 B 2 O 9 (OH) and CsSe 3 B 2 O 9 (OH): one dimensional boroselenite-based anionic frameworks with second harmonic generation properties15Remarkable multimember-ring configurations in a new family of Na 7 M II Sb 5 S 12 (M II = Zn, Cd, Hg) exhibiting various three-dimensional tunnel structures25Sr 5 ZnGa 6 S 15 : a new quaternary non-centrosymmetric semiconductor with a 3D framework structure displaying excellent nonlinear optical performance60CsCu5Se3: A Copper-Rich Ternary Chalcogenide Semiconductor with Nearly Direct Band Gap for Photovoltaic Application41From AgGaS2 to Li2ZnSiS4: Realizing Impressive High Laser Damage Threshold Together with Large Second-Harmonic Generation Response134Li7Cd4.5Ge4Se16 and Li6.4Cd4.8Sn4Se16: Strong Nonlinear Optical Response in Quaternary Diamond‐Like Selenide Networks10Pushing Nonlinear Optical Oxides into the Mid-Infrared Spectral Region Beyond 10 μm: Design, Synthesis, and Characterization of La3SnGa5O14145Effect of Element Substitution on Structural Transformation and Optical Performances in I2BaMIVQ4 (I = Li, Na, Cu, and Ag; MIV = Si, Ge, and Sn; Q = S and Se)63Rb 3 VO(O 2 ) 2 CO 3 : A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response207Rb3VO(O2)2CO3: A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response42LiGa 2 PS 6 and LiCd 3 PS 6 : Molecular Designs of Two New Mid-Infrared Nonlinear Optical Materials88Strong Infrared Nonlinear Optical Efficiency and High Laser Damage Threshold Realized in Quaternary Alkali Metal Sulfides Na2Ga2MS6 (M = Ge, Sn) Containing Mixed Nonlinear Optically Active Motifs48Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95K2ZnGe3S8: A Congruent-Melting Infrared Nonlinear-Optical Material with a Large Band Gap41Ternary 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 Ba6Li2.67Sn4.33S1625Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59Intriguing Structural Transition Inducing Variable Birefringences in ABa2MS4Cl (A = Rb, Cs; M = Ge, Sn)32Second-order nonlinear optical properties of CuGa In1-Se2 (x = 0.54): Experimental and theoretical investigations4A review on structure-performance relationship toward the optimal design of infrared nonlinear optical materials with balanced performances252Second‐Order Nonlinear Optical Tensor Coefficients of LiXTe2 (X = Al, Ga, In) Chalcopyrite Semiconductors7Cu2EuMQ4 (M = Si, Ge; Q = S, Se): Syntheses, structure study and physical properties determination26BaB2S4: An Efficient and Air-Stable Thioborate as Infrared Nonlinear Optical Material with High Laser Damage Threshold85Recent advances and future perspectives on infrared nonlinear optical metal halides223Pressure-Assisted Method for the Preparations of High-Quality AaGaS2 and AgGaGeS4 Crystals for Mid-Infrared Laser Applications11Noncentrosymmetric cubic RbBSi2O6 polymorph with deep ultraviolet cut-off edge4A 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 materials78ABaSbQ 3 (A = Li, Na; Q = S, Se): diverse arrangement modes of isolated SbQ 3 ligands regulating the magnitudes of birefringences50Centric-to-acentric structure transformation induced by a stereochemically active lone pair: a new insight for design of IR nonlinear optical materials90From 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 threshold22Metal-cation substitutions induced the enhancement of second harmonic generation in A 8 BS 6 (A = Cu, and Ag; B = Si, Ge, and Sn)14Mn-Based tin sulfide Sr 3 MnSn 2 S 8 with a wide band gap and strong nonlinear optical response30Partial substitution induced centrosymmetric to noncentrosymmetric structure transformation and promising second-order nonlinear optical properties of (K 0.38 Ba 0.81 )Ga 2 Se 495Pb 7 F 12 Cl 2 : a promising infrared nonlinear optical material with high laser damage threshold19Planar graphitic ZnS, buckling ZnS monolayers and rolled-up nanotubes as nonlinear optical materials: first-principles simulation13Structural 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, crystal structures and nonlinear optical properties of β-RbCdI 3 ·H 2 O and CsCdI 3 ·H 2 O8BaV2O6·H2O: A nonlinear optical crystal with a large bandgap7Photo-tunable linear and nonlinear optical response of cyclophanediene-dihydropyrene photoswitches9MnSiP2: A New Mid-IR Ternary Phosphide with Strong SHG Effect and Ultrabroad Transparency Range66Synthesis, growth and characterization of semi-organic nonlinear optical L-threnoninum sodium fluoride (LTSF) crystal for photonics application25Hierarchy in nonlinear optical responses induced by metal cation tailoring effect in the In-containing chalcogenide compounds4Ba10In6Zn7S26-nZnS: An Inorganic Composite System with Interface Phase-Matching Tuned for High-Performance Infrared Nonlinear Optical Materials13[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 Survey48Synthesis, Structure, and Characterization of Two Mixed-Cation Quaternary Chalcogenides K2BaSnQ4 (Q = S, Se)19Ba10In6Zn7S10Se16 and Ba10In6Zn7Se26: Two new infrared nonlinear optical materials with T2 super tetrahedron6Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS229Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2186Mixed-Anion Inorganic Compounds: A Favorable Candidate for Infrared Nonlinear Optical Materials140Sn 2 Ga 2 S 5 : A Polar Semiconductor with Exceptional Infrared Nonlinear Optical Properties Originating from the Combined Effect of Mixed Asymmetric Building Motifs81BaCuSiTe 3 : A Noncentrosymmetric Semiconductor with CuTe 4 Tetrahedra and Ethane-like Si 2 Te 6 Units11LiBa2MIIIQ4 (MIII = Al, Ga, In; Q = S, Se): A Series of Metal Chalcogenides with a Structural Transition12Ionothermal Synthesis of Metal Chalcogenides M2Ag3Sb3S7 (M = Rb, Cs) Displaying Nonlinear Optical Activity in the Infrared Region33Cotemplating Assembly and Structural Variation of Three-Dimensional Open-Framework Sulfides17BaGe 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 Effects54A 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 substitution287[O 2 Pb 3 ] 2 (BO 3 )I: a new lead borate iodide with 1∞[O 2 Pb 3 ] double chains6A highly distorted HgS 4 tetrahedron-induced moderate second-harmonic generation response of EuHgGeS 462A review of the AI2B II C IV DVI4 family as infrared nonlinear optical materials: the effect of each site on the structure and optical properties59Abnormal 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 motifs22Enhanced optical anisotropy via dimensional control in alkali-metal chalcogenides18Li 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 configuration36M 4 LiBe 4 P 7 O 24 and M 4 Li(Li 3 P)P 7 O 24 (M = Cs, Rb): deep-ultraviolet nonlinear-optical phosphates with a tetrahedra-substituted paracelsian-like framework9Mixed-metal thiophosphate CuCd 3 PS 6 : an infrared nonlinear optical material activated by its three-in-one tetrahedra-stacking architecture33Non-centrosymmetric sulfides A 2 Ba 6 MnSn 4 S 16 (A = Li, Ag): syntheses, structures and properties21Structural Tolerance Factor Approach to Defect-Resistant I2-II-IV-X4 Semiconductor Design38AGaSnS4 (A = Rb, Cs): Three sulfides and their structure diversity8An assessment of the structural, electronic, optical and thermoelectric properties of the BaAg2GeS4 compound11Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement96Cd4SiQ6 (Q = S, Se): Ternary Infrared Nonlinear Optical Materials with Mixed Functional Building Motifs21Lead 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 Materials55LiBa4Ga5Q12 (Q = S, Se): Noncentrosymmetric Metal Chalcogenides with a Cesium Chloride Topological Structure Displaying a Remarkable Laser Damage Threshold32A2SnS5: A Structural Incommensurate Modulation Exhibiting Strong Second‐Harmonic Generation and a High Laser‐Induced Damage Threshold (A=Ba, Sr)30A2SnS5: A Structural Incommensurate Modulation Exhibiting Strong Second‐Harmonic Generation and a High Laser‐Induced Damage Threshold (A=Ba, Sr)86HgCuPS4: An Exceptional Infrared Nonlinear Optical Material with Defect Diamond-like Structure145Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014[ABa2Cl][Ga4S8] (A = Rb, Cs): Wide-Spectrum Nonlinear Optical Materials Obtained by Polycation-Substitution-Induced Nonlinear Optical (NLO)-Functional Motif Ordering269Syntheses and crystal structures of the quaternary thiogermanates Cu4FeGe2S7and Cu4CoGe2S74Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials130Synthesis, growth, structural, thermal, mechanical and optical properties of barium guanidinium dichloride (BaGuCl2) single crystal for NLO applications7Na2MgSnS4 – a new member of the A 2 I B II C IV X 4 family of compounds6Na2MgSnS4 – a new member of the A(2)(I)B(II)C(IV)X(4) family of compounds0Salt-Inclusion Chalcogenide [Ba4Cl2][ZnGa4S10]: Rational Design of an IR Nonlinear Optical Material with Superior Comprehensive Performance Derived from AgGaS2134α‑Li2ZnGeS4: A Wide-Bandgap Diamond-like Semiconductor with Excellent Balance between Laser-Induced Damage Threshold and Second Harmonic Generation Response157Finding Optimal Mid-Infrared Nonlinear Optical Materials in Germanates by First-Principles High-Throughput Screening and Experimental Verification79Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm38Sr6(Li2Cd)A4S16 (A = Ge, Sn): How to Go beyond the Band Gap Limitation via Site-Specific Modification40AB 11 O 16 (OH) 2 (A = K and Cs): interpenetrating 2D layers with large birefringence7Phase Matching, Strong Frequency Doubling, and Outstanding Laser-Induced Damage Threshold in the Biaxial, Quaternary Diamond-like Semiconductor Li 4 CdSn 2 S 779Synthesis, crystal structure, and electronic structure of Li2PbSiS4: a quaternary thiosilicate with a compressed chalcopyrite-like structure4From AgGaS 2 to AgHgPS 4 : vacancy defects and highly distorted HgS 4 tetrahedra double-induced remarkable second-harmonic generation response67A novel promising infrared nonlinear optical selenide KAg 3 Ga 8 Se 14 designed from benchmark AgGaQ 2 (Q = S, Se)55Investigation of the second-order nonlinear optical property of Sr6Sb6S173Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95A review on the recently developed promising infrared nonlinear optical materials103Aliovalent-cation-substitution-induced structure transformation: a new path toward high-performance IR nonlinear optical materials47Applying band gap engineering to tune the linear optical and nonlinear optical properties of noncentrosymmetric chalcogenides La 4 Ge 3 Se x S 12− x ( x = 0, 2, 4, 6, 8, 10)21Ba 2 Ge 2 Te 5 : a ternary NLO-active telluride with unusual one-dimensional helical chains and giant second harmonic-generation tensors31Balanced infrared nonlinear optical performance achieved by modulating the covalency and ionicity distributions in the electron localization function map42Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering144Heterovalent cations substitution to design asymmetric chalcogenides with promising nonlinear optical performances44Halonitrides Zn 2 NX (X=Cl,Br): Novel Mid-Infrared Nonlinear Optical Materials30A 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 Frameworks5Unique Unilateral-Chelated Mode-Induced d–p−π Interaction Enhances Second-Harmonic Generation Response in New Ln3LiMS7 Family41Cs2ZnSn3S8: A Sulfide Compound Realizes a Large Birefringence by Modulating the Dimensional Structure24AZn4Ga5Se12 (A = K, Rb, or Cs): Infrared Nonlinear Optical Materials with Simultaneous Large Second Harmonic Generation Responses and High Laser-Induced Damage Thresholds34Synthesis, Structure, Characterization, and Calculation of a Noncentrosymmetric Fluorine-Containing Indium Iodate, Ba[InF3(IO3)2]10BaCdGeSe4: Synthesis, structure and nonlinear optical properties13Li 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 Gap15A3Te(Zn2Ge)Ge2O14 (A = Sr, Ba, and Pb): New Langasite Mid-infrared Nonlinear Optical Materials by Rational Chemical Substitution32Stepwise Li Substitution Induced Structure Evolution and Improved Nonlinear Optical Performance for Diamond-like Sulfides28Highly 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 846Structural, Optical, and Electronic Properties of Two Quaternary Chalcogenide Semiconductors: Ag2SrSiS4 and Ag2SrGeS420Triclinic Layered A2ZnSi3S8 (A = Rb and Cs) with Large Optical Anisotropy and Systematic Research on the Inherent Structure–Performance Relationship in the A2MIIBMIV3Q8 Family11Giant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo 2 O 8 F149Transition-metal-based chalcogenides: A rich source of infrared nonlinear optical materials184The Rise of Infrared Nonlinear Optical Pnictides: Advances and Outlooks36Superior Infrared Nonlinear Optical Performance Achieved by Synergetic Functional Motif and Vacancy Site Modulations48Noncentrosymmetric chalcohalide K2Ba3Ge3S9Cl2: A new nonlinear optical material with remarkable laser-induced damage threshold17β-BaGa 4 Se 7 : a promising IR nonlinear optical crystal designed by predictable structural rearrangement46Na+/Ag+ substitution induced birefringence enhancement from AgGaS2 to NaGaS218Rational Crystal Structure Design and Nonlinear-Optical Properties of Noncentrosymmetric RbCu2NbS47Noncentrosymmetric (KBa0.5)In2Se4 and (K0.58Ba0.71)(Ga0.89In1.11)Se4 derived from centrosymmetric BaIn2Se4 via partial cation substitution: structural chemistry and nonlinear optical activity9Sn7Br10S2: The First Ternary Halogen‐Rich Chalcohalide Exhibiting a Chiral Structure and Pronounced Nonlinear Optical Properties24Sn7Br10S2: The First Ternary Halogen‐Rich Chalcohalide Exhibiting a Chiral Structure and Pronounced Nonlinear Optical Properties145AAg 2 PS 4 (A = K, Na/K): the first-type of noncentrosymmetric alkali metal Ag-based thiophosphates exhibiting excellent second-order nonlinear optical performances21Alkali metal partial substitution-induced improved second-harmonic generation and enhanced laser-induced damage threshold for Ag-based sulfides21Infrared nonlinear optical sulfide CsCd 4 In 5 S 12 exhibiting large second harmonic generation response16LaBS 3 revisited: a promising mid-infrared nonlinear optical material34Li-Free ternary sulphide Cs 5 Ga 9 S 16 with excellent nonlinear optical performance similar to classic LiGaS 213Na 4 Ga 8 S 14 : a Ga-enriched wide band gap ternary alkali-metal sulfide with unique [Ga 12 S 42 ] 12-membered rings2Rational design of a promising oxychalcogenide infrared nonlinear optical crystal60Rb2MGe3S8 (M=Zn, Cd): Non-Centrosymmetry Transformation Led by Structure Change of [MGe3S8]2- Unit※4Unprecedented mid-infrared nonlinear optical materials achieved by crystal structure engineering, a case study of (KX)P 2 S 6 (X = Sb, Bi, Ba)59Wide band gap thiophosphates ASrPS 4 (A = Li, Na, K, Rb, Cs): cation size effect induced successive structural transformation13

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  1. Li 3 Ge 3 Se 6 : the first ternary lithium germanium selenide with interesting ∞ [Ge 6 Se 12 ] n chains constructed by ethane-like [Ge 2 Se 6 ] 6− clusters

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  2. A Polyselenide with a Novel Se78– Unit: the Structure of Sr19–xPbxGe11Se44 with x = 5.0 and 6.4

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  3. 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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  4. First principle study of nonlinear optical crystals

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  5. Four new quaternary chalcogenides A 2 Ba 7 Sn 4 Q 16 (A = Li, Na; Q = S, Se): syntheses, crystal structures determination, nonlinear optical performances investigation

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  6. 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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  7. 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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  8. RbSe 3 B 2 O 9 (OH) and CsSe 3 B 2 O 9 (OH): one dimensional boroselenite-based anionic frameworks with second harmonic generation properties

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  10. 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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  12. From AgGaS2 to Li2ZnSiS4: Realizing Impressive High Laser Damage Threshold Together with Large Second-Harmonic Generation Response

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  13. Li7Cd4.5Ge4Se16 and Li6.4Cd4.8Sn4Se16: Strong Nonlinear Optical Response in Quaternary Diamond‐Like Selenide Networks

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  14. Pushing Nonlinear Optical Oxides into the Mid-Infrared Spectral Region Beyond 10 μm: Design, Synthesis, and Characterization of La3SnGa5O14

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  15. Effect of Element Substitution on Structural Transformation and Optical Performances in I2BaMIVQ4 (I = Li, Na, Cu, and Ag; MIV = Si, Ge, and Sn; Q = S and Se)

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  16. Rb 3 VO(O 2 ) 2 CO 3 : A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response

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  19. Strong Infrared Nonlinear Optical Efficiency and High Laser Damage Threshold Realized in Quaternary Alkali Metal Sulfides Na2Ga2MS6 (M = Ge, Sn) Containing Mixed Nonlinear Optically Active Motifs

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  21. K2ZnGe3S8: A Congruent-Melting Infrared Nonlinear-Optical Material with a Large Band Gap

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  22. Ternary Mixed-Metal Cd4GeS6: Remarkable Nonlinear-Optical Properties Based on a Tetrahedral-Stacking Framework

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  23. Cation substitution inducing gap changes and covalent interaction flexibility enhancing second harmonic generation responses in d10 metal chalcogenides

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  24. 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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  27. Second-order nonlinear optical properties of CuGa In1-Se2 (x = 0.54): Experimental and theoretical investigations

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

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  29. Second‐Order Nonlinear Optical Tensor Coefficients of LiXTe2 (X = Al, Ga, In) Chalcopyrite Semiconductors

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  30. Cu2EuMQ4 (M = Si, Ge; Q = S, Se): Syntheses, structure study and physical properties determination

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  31. BaB2S4: An Efficient and Air-Stable Thioborate as Infrared Nonlinear Optical Material with High Laser Damage Threshold

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

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  33. Pressure-Assisted Method for the Preparations of High-Quality AaGaS2 and AgGaGeS4 Crystals for Mid-Infrared Laser Applications

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