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RESEARCH PAPER · Chemistry of Materials · 2018

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

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From AgGaS2 to Li2ZnSiS4: Realizing Impressive High Laser Damage Threshold Together with Large Second-Harmonic Generation ResponseOriginalFirst principle study of nonlinear optical crystals15Research progress of mid-and far-infrared nonlinear optical crystals10Sr 5 ZnGa 6 S 15 : a new quaternary non-centrosymmetric semiconductor with a 3D framework structure displaying excellent nonlinear optical performance60LiGa 2 PS 6 and LiCd 3 PS 6 : Molecular Designs of Two New Mid-Infrared Nonlinear Optical Materials88BaM2As2S6 (M = Cd, Hg): Synthesis, crystal structure, optical and electronic properties16Ternary 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 chalcogenides11Intriguing Structural Transition Inducing Variable Birefringences in ABa2MS4Cl (A = Rb, Cs; M = Ge, Sn)32A review on structure-performance relationship toward the optimal design of infrared nonlinear optical materials with balanced performances252Pressure-Assisted Method for the Preparations of High-Quality AaGaS2 and AgGaGeS4 Crystals for Mid-Infrared Laser Applications11Ba10Zn7M6Q26: Two New Mid-infrared Nonlinear Optical Crystals with T2 Supertetrahedron 3D Framework11ABaSbQ 3 (A = Li, Na; Q = S, Se): diverse arrangement modes of isolated SbQ 3 ligands regulating the magnitudes of birefringences50Adjustable optical nonlinearity in d 10 cations containing chalcogenides via dp hybridization interaction13Ba 4 (BS 3 S) 2 S 4 : a new thioborate with unprecedented [BS 3 -S] and [S 4 ] fundamental building blocks19Cs 2 CdV 2 O 6 Cl 2 and Cs 3 CdV 4 O 12 Br: two new non-centrosymmetric oxyhalides containing d 0 and d 10 cations and exhibiting second harmonic generation activity19From 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 threshold22Theoretical Design of Layered AlGaS3 as a New Nonlinear Optical Material with a Strong Second Harmonic Generation Response5Li4HgSn2Se7: The First Second-Order Nonlinear Optical-Active Selenide in the I4–II–IV2–VI7 Diamond-like Family32LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO398LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO337Synthesis of polycrystalline CdSiP2 with Two-Temperature zone method3Li[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 Performance40First-Principles Design and Simulations Promote the Development of Nonlinear Optical Crystals299Rational design of infrared nonlinear optical chalcogenides by chemical substitution287Li2K4TiOGe4O12: A Stable Mid-Infrared Nonlinear Optical Material69A review of the AI2B II C IV DVI4 family as infrared nonlinear optical materials: the effect of each site on the structure and optical properties59Li 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 configuration36Mixed-metal thiophosphate CuCd 3 PS 6 : an infrared nonlinear optical material activated by its three-in-one tetrahedra-stacking architecture33Salt-inclusion chalcogenides: an emerging class of IR nonlinear optical materials54Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement96Lead 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 Threshold32HgCuPS4: An Exceptional Infrared Nonlinear Optical Material with Defect Diamond-like Structure145[ABa2Cl][Ga4S8] (A = Rb, Cs): Wide-Spectrum Nonlinear Optical Materials Obtained by Polycation-Substitution-Induced Nonlinear Optical (NLO)-Functional Motif Ordering269Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials130Salt-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 Response157Pb 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 Properties29Finding 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 μm38Na4CdGe2S7: A Sodium-Rich Quaternary Wide-Band-Gap Chalcogenide with Two-Dimensional [Ge2CdS7]∞ Layers6Sr6(Li2Cd)A4S16 (A = Ge, Sn): How to Go beyond the Band Gap Limitation via Site-Specific Modification40Phase Matching, Strong Frequency Doubling, and Outstanding Laser-Induced Damage Threshold in the Biaxial, Quaternary Diamond-like Semiconductor Li 4 CdSn 2 S 779EuHgGeSe 4 and EuHgSnS 4 : Two Quaternary Eu-Based Infrared Nonlinear Optical Materials with Strong Second-Harmonic-Generation Responses55From AgGaS 2 to AgHgPS 4 : vacancy defects and highly distorted HgS 4 tetrahedra double-induced remarkable second-harmonic generation response67A 3 Mn 2 Sb 3 S 8 (A = K and Rb): a new type of multifunctional infrared nonlinear optical material based on unique three-dimensional open frameworks53Ba 2 Ge 2 Te 5 : a ternary NLO-active telluride with unusual one-dimensional helical chains and giant second harmonic-generation tensors31Cu 4 MnGe 2 S 7 and Cu 2 MnGeS 4 : two polar thiogermanates exhibiting second harmonic generation in the infrared and structures derived from hexagonal diamond22Heterovalent cations substitution to design asymmetric chalcogenides with promising nonlinear optical performances44Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials24Second-order nonlinear optical and photoelectric properties of Zn4B6O12S20LaSiP3 and LaSi2P6: Two Excellent Rare‐Earth Pnictides with Strong SHG Responses as Mid‐ and Far‐Infrared Nonlinear Optical Crystals36α-Ca2CdP2 and β-Ca2CdP2: Two Polymorphic Phosphide-Based Infrared Nonlinear Crystals with Distorted NLO-Active Tetrahedral Motifs Realizing Large Second Harmonic Generation Effects and Suitable Band Gaps30Li 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 Gap15Stepwise 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 846Synthesis, structure, linear and nonlinear optical properties of noncentrosymmetric quaternary diamond-like semiconductors, Cu2ZnGeSe4 (CZGSe) and the novel Cu4ZnGe2Se720Transition-metal-based chalcogenides: A rich source of infrared nonlinear optical materials184The Rise of Infrared Nonlinear Optical Pnictides: Advances and Outlooks36Syntheses, Structures and Properties of Alkali and Alkaline Earth Metal Diamond-Like Compounds Li2MgMSe4 (M = Ge, Sn)12Noncentrosymmetric chalcohalide K2Ba3Ge3S9Cl2: A new nonlinear optical material with remarkable laser-induced damage threshold17Na+/Ag+ substitution induced birefringence enhancement from AgGaS2 to NaGaS218Synthesis, Crystal Growth, Electronic Properties and Optical Properties of Y6IV2.5S14 (IV=Si, Ge)9Noncentrosymmetric (KBa0.5)In2Se4 and (K0.58Ba0.71)(Ga0.89In1.11)Se4 derived from centrosymmetric BaIn2Se4 via partial cation substitution: structural chemistry and nonlinear optical activity9Partial congener substitution induced centrosymmetric to noncentrosymmetric structural transformation and nonlinear optical properties of PbSnSiS413A novel 2-(aminomethyl)pyridineH 2 PO 4 crystal with second-order nonlinear optical performance8Alkali metal partial substitution-induced improved second-harmonic generation and enhanced laser-induced damage threshold for Ag-based sulfides21Broad transparency and wide band gap achieved in a magnetic infrared nonlinear optical chalcogenide by suppressing d–d transitions41First polar quaternary sulphide CsLiGa 6 S 10 with mixed ordered alkali cations displaying excellent infrared nonlinear optical properties16Metal oxyhalides: an emerging family of nonlinear optical materials124New Quaternary Sulfide LiGaSiS 4: Synthesis, Structure and Optical Properties0Rational design via dual-site aliovalent substitution leads to an outstanding IR nonlinear optical material with well-balanced comprehensive properties68Wide band gap thiophosphates ASrPS 4 (A = Li, Na, K, Rb, Cs): cation size effect induced successive structural transformation13Thiotetrelates Li 2 ZnXS 4 (X = Si, Ge, and Sn) As Potential Li-Ion Solid-State Electrolytes10Synthesis, Crystal and Electronic Structures, and Nonlinear Optical Properties of Y4Si3S1212Cation Disorder and Large Tetragonal Supercell Ordering in the Li-Rich Argyrodite Li7Zn0.5SiS612Second-Harmonic Generation-Positive Na 2 Ga 2 SiS 6 with a Broad Band Gap and a High Laser Damage Threshold14New quaternary sulfide LiGaSiS4: Synthesis, structure and optical properties0SrAgAsS4: A Noncentrosymmetric Sulfide with Good Infrared Nonlinear Optical Performance Induced by Aliovalent Substitution from Centrosymmetric SrGa2S412(Na0.74Ag1.26)BaSnS4: A New AgGaS2‐Type Nonlinear Optical Sulfide with a Wide Band Gap and High Laser Induced Damage Threshold14Ag4SnGe2S7: A Noncentrosymmetric Chalcogenide in I4–II–IV2–VI7 System with Non-Diamond-Like Structure Featuring 1D ∞[SnGe2S8]6– Infinite Chain2Ternary AGa5S8 (A = K, Rb, Cs): Promising infrared nonlinear optical materials rationally realized by “one-for-multiple substitution” strategy37Novel structural transformation in K3ReP2S8 thiophosphates originating from the rare-earth (Re) cation sizes induced local coordination asymmetry25LiAlS2: A promising infrared frequency-conversion material with ultrawide band gap and high laser-induced damage threshold19AIB3IIC3IIIQ8VI: A New Family for the Design of Infrared Nonlinear Optical Materials by Coupling Octahedra and Tetrahedra Units152Rb 2 CdSi 4 S 10 : novel [Si 4 S 10 ] T2-supertetrahedra-contained infrared nonlinear optical material with large band gap79Ag-based chalcogenides and derivatives as promising infrared nonlinear optical materials90γ-P 4 S 3 I 2 : a new metal-free infrared second-order nonlinear optical crystal designed by polymorphism strategy17Na 2 Ba[Na 2 Sn 2 S 7 ]: Structural Tolerance Factor‐Guided NLO Performance Improvement50Na2Ba[Na2Sn2S7]: Structural Tolerance Factor‐Guided NLO Performance Improvement0[Sr 4 Cl 2 ][Si 3 S 9 ]: Ultrawide-bandgap salt-inclusion thiosilicate nonlinear optical material with unprecedented tri-polymerized [Si 3 S 9 ] clusters21Breaking the bottleneck of simultaneously wide band gap and large nonlinear optical coefficient by a “pore reconstruction” strategy in a salt-inclusion chalcogenide26LaAeAl 3 S 7 (Ae = Ca, Sr): Cairo pentagonal layered thioaluminates achieving a good balance between a strong second harmonic generation response and a wide bandgap23Recent progress on sulfide infrared nonlinear optical materials with large SHG response and wide band gap26LnLiSiS4 (Ln = La and Ce): Promising infrared nonlinear optical materials designed by aliovalent substitution from SrCdSiS437Phase Competition and Strong SHG Responses of the Li2MIIMIVSe4 Family: Atom Response Theory Predictions versus Experimental Results24Na3SiS3F: A Wide Bandgap Fluorothiosilicate with Unique [SiS3F] Unit and High Laser‐Induced Damage Threshold39HgB2S4: A d10 Metal Thioborate with Giant Birefringence and Wide Band Gap31Recent advances in IR nonlinear optical chalcogenides with well-balanced comprehensive performance56Synthesis, Crystal Structure, and Nonlinear-Optical Properties of a Diamond-Like Chalcogenide Cu 2 GeS 313Three-in-One Tetrahedral Functional Units Constructing Diamondlike Ag2In2SiS3.06Se2.94 with High-Performance Nonlinear-Optical Activity4AgMAsS3 (M = Cd, Hg): Double d10 Cation-Containing Thioarsenites(III) Exhibiting High Photocurrent Response and Moderate Second Harmonic Generation11BaCu2SiS4: A New Member of the AIIBI2MIVQ4 Chalcogenide Family with a Chiral Crystal Structure6Ca2Ln(BS3)(SiS4) (Ln = La, Ce, and Gd): Mixed Metal Thioborate‐Thiosilicates as Well‐Performed Infrared Nonlinear Optical Materials29Enhancing second harmonic generation response in infrared nonlinear optical material through Pb substitution: A study of LiPbSiS compound2ZnGa 2 S 4 : an infrared nonlinear optical material with large second‐harmonic generation response and wide band gap28Advances in Solid-State Nonlinear Optical Materials: From Fundamentals to Applications61Alkali halide flux synthesis, crystal structure, and photoelectric response of quaternary thiosilicates K 3 Ga 3 Si 7 S 20 and K 2 ZnSi 3 S 81Multi-step cation substitution facilitating the exploration of potential infrared nonlinear optical materials6Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153LiLnGeS 4 (Ln=La−Nd): Designing High Performance Infrared Nonlinear Optical Sulfides through “Band Reformation of AGS”36LiLnGeS 4 (Ln=La−Nd): Designing High Performance Infrared Nonlinear Optical Sulfides through “Band Reformation of AGS”5Ca 2 La(MS 4 )(BS 3 ) (M = Ge/Si and Sn/Si): high-performance infrared nonlinear optical materials designed using an atomic site co-occupancy strategy9Exploring the functional properties of the diamond-like quaternary compound Li 2 ZnGeS 4 for potential energy applications: a theoretical approach2Isovalent cation substitution drives structural transformation and infrared nonlinear optical activity in Eu-based chalcogenides11AgGaS2 and Derivatives: Design, Synthesis, and Optical Properties8Phase diagram of the AgGaS2–PbGa2S4 system1KYSiSe 4 : A Rare-Earth Selenide Infrared Nonlinear Optical Crystal with Wide Infrared Transparency and Well-Balanced E g and SHG Response9Research on the damage mechanism of near-infrared stray light irradiation of Al-based functional film2Crystal growth, optical, thermal, dielectric and mechanical, laser damage threshold, and dielectric characterizations of a novel organic third-order nonlinear optical crystal: 2,4-Dichlorobenzoic acid 4-(Dimethylamino) Benzaldehyde (DADABA)1高性能硫属化物红外非线性光学材料构效关系(特邀)0Zn 4 S(C 2 H 2 N 3 ) 3 (NCS) 3 : Coordination-Driven Structural Distortion Engineering Triggers Exceptional NLO Effect in Mixed-Bonding Zinc Isothiocyanate6Harnessing tetrahedral diversity: The path to superior diamond-like IR NLO crystals13KHg 4 Ga 5 S 12 : A Diamond-like Tetrahedral Chalcogenide Exhibiting Giant Phase-Matching Second Harmonic Generation6Hydrothermal Synthesis and Electronic and Optical Characterization of Ag 2 (NH 4 )AsS 40CdY 2 Si 2 S 8 : A Wide Bandgap IR NLO Material with d 10 Metal-Induced Structure Transformation from CS to NCS1Defect Diamond‐Like d 10 Metal Indium Selenium With Strong Second‐Harmonic Generation and Enhanced Laser‐Induced Damage Threshold2First‐Principles Investigation of the Structural, Electronic, Optical, Elastic, and Thermal Properties of Defect Diamond‐Like Hg 3 P 2 S 80From AgGaSe2 to MIIGa2Se4 (MII = Zn, Cd): Heterovalent Substitution Creates Ordered Vacancies for Balanced IR-NLO Performance0Variation of Tetrahedrons and Cations Regulates LIDTs in 3D‐DL Structure MIR‐NLO Crystals0

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  2. Research progress of mid-and far-infrared nonlinear optical crystals

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

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  5. BaM2As2S6 (M = Cd, Hg): Synthesis, crystal structure, optical and electronic properties

    Journal of Alloys and Compounds · 2018-05-21

    Yangwu Guo, Fei Liang, Molin Zhou, Zheshuai Lin, Jiyong Yao, Yicheng Wu

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

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

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  8. Intriguing Structural Transition Inducing Variable Birefringences in ABa2MS4Cl (A = Rb, Cs; M = Ge, Sn)

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

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

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  11. Ba10Zn7M6Q26: Two New Mid-infrared Nonlinear Optical Crystals with T2 Supertetrahedron 3D Framework

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  12. ABaSbQ 3 (A = Li, Na; Q = S, Se): diverse arrangement modes of isolated SbQ 3 ligands regulating the magnitudes of birefringences

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  13. Adjustable optical nonlinearity in d 10 cations containing chalcogenides via dp hybridization interaction

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  14. Ba 4 (BS 3 S) 2 S 4 : a new thioborate with unprecedented [BS 3 -S] and [S 4 ] fundamental building blocks

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  15. Cs 2 CdV 2 O 6 Cl 2 and Cs 3 CdV 4 O 12 Br: two new non-centrosymmetric oxyhalides containing d 0 and d 10 cations and exhibiting second harmonic generation activity

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  16. From 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 threshold

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  17. Theoretical Design of Layered AlGaS3 as a New Nonlinear Optical Material with a Strong Second Harmonic Generation Response

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  18. Li4HgSn2Se7: The First Second-Order Nonlinear Optical-Active Selenide in the I4–II–IV2–VI7 Diamond-like Family

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  19. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  20. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  21. Synthesis of polycrystalline CdSiP2 with Two-Temperature zone method

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  22. Li[LiCs2Cl][Ga3S6]: A Nanoporous Framework of GaS4 Tetrahedra with Excellent Nonlinear Optical Performance

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  23. Li[LiCs2Cl][Ga3S6]: A Nanoporous Framework of GaS4 Tetrahedra with Excellent Nonlinear Optical Performance

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  24. First-Principles Design and Simulations Promote the Development of Nonlinear Optical Crystals

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  25. Rational design of infrared nonlinear optical chalcogenides by chemical substitution

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  26. Li2K4TiOGe4O12: A Stable Mid-Infrared Nonlinear Optical Material

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  27. A review of the AI2B II C IV DVI4 family as infrared nonlinear optical materials: the effect of each site on the structure and optical properties

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  28. Li 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 configuration

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  29. Mixed-metal thiophosphate CuCd 3 PS 6 : an infrared nonlinear optical material activated by its three-in-one tetrahedra-stacking architecture

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  30. Salt-inclusion chalcogenides: an emerging class of IR nonlinear optical materials

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  31. Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement

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  32. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

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  33. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

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  34. LiBa4Ga5Q12 (Q = S, Se): Noncentrosymmetric Metal Chalcogenides with a Cesium Chloride Topological Structure Displaying a Remarkable Laser Damage Threshold

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  35. HgCuPS4: An Exceptional Infrared Nonlinear Optical Material with Defect Diamond-like Structure

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  36. [ABa2Cl][Ga4S8] (A = Rb, Cs): Wide-Spectrum Nonlinear Optical Materials Obtained by Polycation-Substitution-Induced Nonlinear Optical (NLO)-Functional Motif Ordering

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  37. Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials

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  38. Salt-Inclusion Chalcogenide [Ba4Cl2][ZnGa4S10]: Rational Design of an IR Nonlinear Optical Material with Superior Comprehensive Performance Derived from AgGaS2

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  39. α‑Li2ZnGeS4: A Wide-Bandgap Diamond-like Semiconductor with Excellent Balance between Laser-Induced Damage Threshold and Second Harmonic Generation Response

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  40. Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties

    Angewandte Chemie International Edition · 2020-09-02

    Xinglong Chen, Qun Jing, Kang Min Ok

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  41. Pb18O8Cl15I5: A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties

    Angewandte Chemie · 2020-09-02

    Xinglong Chen, Qun Jing, Kang Min Ok

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  42. Finding Optimal Mid-Infrared Nonlinear Optical Materials in Germanates by First-Principles High-Throughput Screening and Experimental Verification

    ACS Applied Materials & Interfaces · 2020-09-14

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