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RESEARCH PAPER · Chemical Science · 2018

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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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 thresholdOriginalAdduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59Cu2EuMQ4 (M = Si, Ge; Q = S, Se): Syntheses, structure study and physical properties determination26Pressure-Assisted Method for the Preparations of High-Quality AaGaS2 and AgGaGeS4 Crystals for Mid-Infrared Laser Applications11A 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 materials78BaMnSnS 4 and BaCdGeS 4 : infrared nonlinear optical sulfides containing highly distorted motifs with centers of moderate electronegativity48KBi(IO 3 ) 3 (OH) and NaBi(IO 3 ) 4 : from the centrosymmetric chain to a noncentrosymmetric double layer18Monoclinic gallium selenide: an AgGaS 2 -type structure variant with balanced infrared nonlinear optical performance43Partial substitution induced centrosymmetric to noncentrosymmetric structure transformation and promising second-order nonlinear optical properties of (K 0.38 Ba 0.81 )Ga 2 Se 495SrCdSnQ 4 (Q = S and Se): infrared nonlinear optical chalcogenides with mixed NLO-active and synergetic distorted motifs68Balanced Second-Order Nonlinear Optical Properties of Adducts CHI3·(S8)3 and AsI3·(S8)3: A Systematic Survey48Li4HgSn2Se7: The First Second-Order Nonlinear Optical-Active Selenide in the I4–II–IV2–VI7 Diamond-like Family32LiBa2MIIIQ4 (MIII = Al, Ga, In; Q = S, Se): A Series of Metal Chalcogenides with a Structural Transition12LiMII(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‐LiIO337Partial Congener Substitution Induced Centrosymmetric to Noncentrosymmetric Transformation Witnessed by K3Ga3(Ge7–xMx)Se20 (M = Si, Sn) and Their Nonlinear Optical Properties51BaGe 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 crystals48Ba 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 transformation22Coordinated 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 materials28K 4 (PO 2 F 2 ) 2 (S 2 O 7 ): first fluorooxophosphorsulfate with mixed-anion [S 2 O 7 ] 2− and [PO 2 F 2 ] − groups14Strong nonlinear optical effect attained by atom-response-theory aided design in the Na 2 M II MIV2Q 6 (M II = Zn, Cd; M IV = Ge, Sn; Q = S, Se) chalcogenide system27One-Dimensional Double Chains in Sodium-Based Quaternary Chalcogenides Displaying Intriguing Red Emission and Large Optical Anisotropy17(Na0.60Ba0.70)Ga2Se4: An Infrared Nonlinear Optical Crystal Designed using AgGaSe2 as the Template38K2Na(IO3)2(I3O8) with Strong Second Harmonic Generation Response Activated by Two Types of Isolated Iodate Anions46A2SnS5: 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)86KInSi1.32Sn0.68Se6: An Infrared Nonlinear Optical Material Containing Three Types of Tetrahedral Units19HgCuPS4: An Exceptional Infrared Nonlinear Optical Material with Defect Diamond-like Structure145Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107Chalcophosphates: A Treasure House of Infrared Nonlinear Optical Materials75Sr6(Li2Cd)A4S16 (A = Ge, Sn): How to Go beyond the Band Gap Limitation via Site-Specific Modification40AMnAs3S6 (A = Cs, Rb): Phase-Matchable Infrared Nonlinear Optical Functional Motif [As3S6]3– Obtained via Surfactant–Thermal Method32The open-framework structure of KSbGe3O9 flux-grown crystals investigated by X-ray diffraction, vibrational spectroscopy, and DFT calculations5Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95Heterovalent cations substitution to design asymmetric chalcogenides with promising nonlinear optical performances44Synthesis, crystal structure and physical properties of a new chalcogenides Rb3Ga3Ge7S208Halonitrides Zn 2 NX (X=Cl,Br): Novel Mid-Infrared Nonlinear Optical Materials30Second-order nonlinear optical and photoelectric properties of Zn4B6O12S20A Series of Pentanary Salt-Inclusion Chalcogenoborates Containing a B12Q12 (Q = S, Se) Cluster Exhibiting a Kleinman-Forbidden Frequency-Doubling Effect25Strongly Coupled Systems for Nonlinear Optics57Introduction of Li into Ag-Based Noncentrosymmetric Sulfides for High-Performance Infrared Nonlinear Optical Materials40Three-in-One Strategy Constructing a Series of Hybrid Tetrahedral Motif-Based Selenides with Balanced Second-Order Nonlinear Optical Performance12Inorganic Chalcogenides: From Zero‐Dimensional Clusters to Three‐Dimensional Frameworks5Synthesis, crystal structure, linear and nonlinear optical properties of quaternary sulfides Ba6(Cu2X)Ge4S16 (X=Mg, Mn, Cd)23ASb5S8 (A = K, Rb, and Cs): Thermal Switching of Infrared Nonlinear Optical Properties across the Crystal/Glass Transformation39AZn4Ga5Se12 (A = K, Rb, or Cs): Infrared Nonlinear Optical Materials with Simultaneous Large Second Harmonic Generation Responses and High Laser-Induced Damage Thresholds34Stepwise Li Substitution Induced Structure Evolution and Improved Nonlinear Optical Performance for Diamond-like Sulfides28Hg 3 P 2 S 8 : A New Promising Infrared Nonlinear Optical Material with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold111Helical {[HgS]} n Chain-Induced Balanced Nonlinear-Optical Performance for Trigonal Mercury Sulfide29Designing 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) Crystal13First-principles study of opto-electronic and thermoelectric properties of SrCdSnX4 (X=S, Se, Te) alkali metal chalcogenides34Noncentrosymmetric (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 Properties145A 2 P 2 S 6 (A = Ba and Pb): a good platform to study the polymorph effect and lone pair effect to form an acentric structure28A 2 Zn 3 P 4 S 13 (A = Rb and Cs): First Infrared Nonlinear Optical Materials with Mixed Thiophosphate Functional Motifs PS 4 and P 2 S 621AAg 3 Ga 8 Se 14 (A = Rb, Cs): second-harmonic generation responses realized through the parallel arrangement of AgSe 4 and GaSe 4 tetrahedrons5Alkali 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 transitions41From 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 materials19KEu 2 In 3 B 12 S 13 : a novel type of thioborate featuring B 12 S 12 cluster and unique In 6 S 6 12-membered ring10Li-Free ternary sulphide Cs 5 Ga 9 S 16 with excellent nonlinear optical performance similar to classic LiGaS 213Unprecedented mid-infrared nonlinear optical materials achieved by crystal structure engineering, a case study of (KX)P 2 S 6 (X = Sb, Bi, Ba)59Wide bandgaps and strong SHG responses of hetero-oxyfluorides by dual-fluorination-directed bandgap engineering28Pd and octahedra do not get along: Square planar [PdS4] units in non-centrosymmetric La6PdSi2S1419Ba6(CuxZy)Sn4S16 (Z = Mg, Mn, Zn, Cd, In, Bi, Sn): High Chemical Flexibility Resulting in Good Nonlinear-Optical Properties12Material research from the viewpoint of functional motifs103Phosphogermanate Crystal: A New Ultraviolet–Infrared Nonlinear Optical Crystal with Excellent Optical Performances16Synthesis, Crystal and Electronic Structures, and Nonlinear Optical Properties of Y4Si3S1212Novel Polarized Crystal BaTeW2O9: Crystal Growth, Characterization, and Wide-Band Polarized Prism15Non‐Linear Optical Properties of the (RE)3CuGeS7 Family of Compounds16AgGaSe2-Inspired Nonlinear Optical Materials: Tetrel Selenides of Alkali Metals and Mercury34Design of Infrared Nonlinear Optical Compounds with Diamond-like Structures and Balanced Optical Performance9A comprehensive review on metal chalcogenides with three-dimensional frameworks for infrared nonlinear optical applications114Heteroanionic Control of Exemplary Second-Harmonic Generation and Phase Matchability in 1D LiAsS2–xSex43(Na0.74Ag1.26)BaSnS4: A New AgGaS2‐Type Nonlinear Optical Sulfide with a Wide Band Gap and High Laser Induced Damage Threshold14Identification of aggregated 2D cobalt tellurides using a spatial self-phase modulation technique8Ag[SC(NH2)2]2F: A Laser Damage-Tolerant Infrared Nonlinear Optical Material9The Antiperovskite‐Type Oxychalcogenides Ae3Q[GeOQ3] (Ae = Ba, Sr; Q = S, Se) with Large Second Harmonic Generation Responses and Wide Band Gaps68From Ba3Nb2O2F12(H2O)2 to Ba0.5NbO2F2(H2O): Achieving Balanced Nonlinear Optical Performance by O/F Ratio Regulation18AIn 3 Si 4 P 9 (A = Ca, Sr): quaternary phosphides with double-helix structures exhibiting high laser-induced damage thresholds19Breaking the bottleneck of simultaneously wide band gap and large nonlinear optical coefficient by a “pore reconstruction” strategy in a salt-inclusion chalcogenide26Revisiting 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 response12Synthesis of chiral high-entropy sulfides for non-linear optical applications13The first quaternary rare-earth oxythiogermanate with second-harmonic generation and ferromagnetic behavior26K2CdGe3S8: A New Infrared Nonlinear Optical Sulfide6Recent progress in the design of IR nonlinear optical materials by partial chemical substitution: Structural evolution and performance optimization133Unbiased Screening of Novel Infrared Nonlinear Optical Materials with High Thermal Conductivity: Long‐neglected Nitrides and Popular Chalcogenides12Unbiased Screening of Novel Infrared Nonlinear Optical Materials with High Thermal Conductivity: Long‐neglected Nitrides and Popular Chalcogenides48[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 eV46Three‐in‐One Strategy Constructing the First High‐Performance Nonlinear Optical Sulfide Crystallizing with the P43 Space Group27Three-in-One Tetrahedral Functional Units Constructing Diamondlike Ag2In2SiS3.06Se2.94 with High-Performance Nonlinear-Optical Activity4LiGa(IO3)4: An Excellent NLO Material with Unprecedented 2D [Ga(IO3)4]∞− Layer Synthesized by Aliovalent Substitution20BaCu2SiS4: A New Member of the AIIBI2MIVQ4 Chalcogenide Family with a Chiral Crystal Structure6The compatibly large nonlinear optical effect and high laser-induced damage threshold in a thiophosphate CsInP2S7 constructed with [P2S7]4- and [InS6]9-15Temperature dependence of the properties of the Li0.81Ag0.19InSe2 nonlinear crystal0Flexible Anionic Groups‐Activated Structure Dissymmetry for Strong Nonlinearity in Ln 2 Ae 3 M IV 3 S 12 Family15Growth, optical, morphological, thermal, laser induced damage threshold, microhardness properties of an organic novel single crystal: Piperazinium 2-Furoate4Synthesis, crystal and electronic structures, linear and nonlinear optical properties, and photocurrent response of oxyhalides CeHaVIO 4 (Ha = Cl, Br; VI = Mo, W)10ACu4AsS4 (A = K, Rb): Two infrared nonlinear optical crystals with strong second-harmonic generation responses originating from multiple chromophores12Ga-based IR nonlinear optical materials: Synthesis, structures, and properties65Salt-inclusion chalcogenides with d-orbital components: unveiling remarkable nonlinear optical properties and dual-band photoluminescence10Salt-inclusion sulfides [K 4 Cl][M II 11 In 9 S 26 ] (M II = Zn, Cd) displaying robust nonlinear optical activity4Growth, structural, linear and nonlinear optical investigations of L-cysteine ethyl ester hydrochloride crystals for optical applications7Mixed-anion square-pyramid [SbS3I2] units causing strong second-harmonic generation intensity and large birefringence8[Na2PbI][Ga7S12]: Combining Diamond-Like Anionic Framework with Polycationic Chain toward Achieving Remarkable Nonlinear Optical Response21Mixed Anionic M(S/X)6 Polyhedra as Symmetry-Breaking Motifs to Enhance the Infrared Nonlinear Optical Response in Y–M–S–X (M = Ga, Ge; X = Cl, Br)5Design of Pentanary Mixed-Chalcogenides Ag2In2SiS6–xSex (x = 1, 2) Based on the Bucket Effect: Local Structural Difference and High-Performance Nonlinear-Optical Properties Realized by Partial Congener Substitution5Phase Matching of Infrared Nonlinear Optical Salt-Inclusion Chalcogenides Achieved by the Modulation of the Fractal Dimension of Anionic Motifs18Activation of TADF in Photon Upconverting Crystals of Dinuclear Cu(I)-Iodide Complexes by Ligand Engineering21The centrosymmetric to non-centrosymmetric transformation induced by alkaline-earth cations producing infrared nonlinear optical AeMn6Ga6S16 (Ae = Ca, Sr)13Integration of Open Metal Sites in an Amino-Functionalized Sm(III)–Organic Framework toward Enhanced Third-Order Nonlinear Optical Property42Photoisomerization Dynamics of 2-[(E)-(4-fluorophenyl)diazenyl]- 1H-imidazole: A Theoretical and Experimental Insight2Theoretical Investigation of Nonlinear Optical Properties and Molecular Docking of Carbazoles Derived from Murraya Koenigii1Machine Learning Guided Discovery of Non‐Linear Optical Materials14Steric hindrance modulated efficient thermally activated delayed fluorescence with non-linear optical, ferroelectric and piezoelectric properties5Crystal growth and characterization of magnesium sulfate-doped adipic acid crystals: intense NLO response from centrosymmetric crystal3Controlling Triplet-Harvesting Pathways and Nonlinear Optical Properties in Cu(I) Iodide-Based Polymers through Ligand Engineering14Rate-Dependent Mechanoluminescence in SrZn2S2O:Mn2+ for Time-Characterized Optoelectronic Devices8A new selenide semiconductor NaMn3Ga3Se8 with strong second-harmonic generation and significant luminescence property5Oxygen‐Substitution Induced High‐Performance Nonlinear Optical Properties: Witnessed by the First Quaternary Oxythiostannate12Metal Cation Engineered UV Birefringent Crystals in π‐Conjugated Sulfonates with Record‐High Optical Anisotropy17Achieving excellent nonlinear optical performance via “dimensionality elevation”-driven transformation from centrosymmetric to non-centrosymmetric structures1Hybrid Bismuth Halide with Rich Polymorphism and Second Harmonic Generation Response8Doubling Polarizability Anisotropy of The Tetrahedral Motifs to Achieve Phase Matching for Melilite-Type Compound2SrZnGeSe4: An Infrared Nonlinear Optical Crystal Material with Wide Transmission Range and Large SHG Response6BaAl2MS6 (M = Si and Ge): the rational construction of diamond-like structures with ultrawide band gap by group-optimization approach6Quantum chemical insights into the role of azocyclic donors on second and third-order NLO responses of organic frameworks0Growth and characterization of methyl orange dye-doped adipic acid single crystals for optical filtering and thermal stability applications0Strain-engineered indirect-to-direct band gap transition, photocatalytic water splitting activity, and optical responses in ACuGa 6 S 10 (A = Rb and Cs)0van der Waals layered CuInP 2 S 6 as infrared nonlinear optical material1Exploring the photophysical and nonlinear optical properties of a methoxy-functionalized indandione-based chalcone derivative: Experimental and theoretical insights4Phenyl-Driven structural engineering of Pyridyl-Based Schiff bases for enhanced Photophysical and Third-Order nonlinear Optical Responses: An Experimental and DFT Study0{[Ge 2 S 7 ] 6– } ∞ Chains-Mediated Framework Reorganization Triggers Dimensional Upgrade and Infrared Nonlinear Optical Response3From KBa 4 Ge 3 S 10 Cl to ABa 3 EuGe 3 S 11 (A = Na, K) Synthesized by Reactive Flux Assisted Metal Oxide-Boron-Chalcogen (MOBQ) Method: Effect of Cation/Anion Cosubstitution on Crystal Structure and Nonlinear Optical Properties0Giant Birefringence and Ultrahigh Thermal Conductivity in Layered MgMoN 20First‐Principles Investigation of the Structural, Electronic, Optical, Elastic, and Thermal Properties of Defect Diamond‐Like Hg 3 P 2 S 80Reversible Symmetry Switching, Giant Birefringence, and UV Second‐Harmonic Generation in Hybrid Niobium Oxyfluorides0Reversible Symmetry Switching, Giant Birefringence, and UV Second‐Harmonic Generation in Hybrid Niobium Oxyfluorides0Tuning Head-to-Tail Packing in Polyfluorinated Schiff Bases for Enhanced NLO Response and High Refractive Index toward THz Applications0

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  1. 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

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

    Journal of Solid State Chemistry · 2018-09-25

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

    Inorganic Chemistry · 2018-11-09

    Changbao Huang, Mingsheng Mao, Haixin Wu, Jiaren Ma

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  4. A 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 materials

    Chemical Science · 2019-01-01

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  5. BaMnSnS 4 and BaCdGeS 4 : infrared nonlinear optical sulfides containing highly distorted motifs with centers of moderate electronegativity

    Inorganic Chemistry Frontiers · 2019-01-01

    Yang-Jie Lin, Run Ye, Long‐Qi Yang, Xiao‐Ming Jiang, Bin‐Wen Liu, Hui‐Yi Zeng, Guo‐Cong Guo

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  6. KBi(IO 3 ) 3 (OH) and NaBi(IO 3 ) 4 : from the centrosymmetric chain to a noncentrosymmetric double layer

    Dalton Transactions · 2019-01-01

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  7. Monoclinic gallium selenide: an AgGaS 2 -type structure variant with balanced infrared nonlinear optical performance

    Journal of Materials Chemistry C · 2019-01-01

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  8. Partial substitution induced centrosymmetric to noncentrosymmetric structure transformation and promising second-order nonlinear optical properties of (K 0.38 Ba 0.81 )Ga 2 Se 4

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  9. SrCdSnQ 4 (Q = S and Se): infrared nonlinear optical chalcogenides with mixed NLO-active and synergetic distorted motifs

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  10. Balanced Second-Order Nonlinear Optical Properties of Adducts CHI3·(S8)3 and AsI3·(S8)3: A Systematic Survey

    Inorganic Chemistry · 2019-03-15

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

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  12. LiBa2MIIIQ4 (MIII = Al, Ga, In; Q = S, Se): A Series of Metal Chalcogenides with a Structural Transition

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  13. 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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  14. 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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  15. Partial Congener Substitution Induced Centrosymmetric to Noncentrosymmetric Transformation Witnessed by K3Ga3(Ge7–xMx)Se20 (M = Si, Sn) and Their Nonlinear Optical Properties

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  16. BaGe 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 Effects

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  17. A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals

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  18. Ba 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 transformation

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  19. Coordinated 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 materials

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  20. K 4 (PO 2 F 2 ) 2 (S 2 O 7 ): first fluorooxophosphorsulfate with mixed-anion [S 2 O 7 ] 2− and [PO 2 F 2 ] − groups

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  21. Strong nonlinear optical effect attained by atom-response-theory aided design in the Na 2 M II MIV2Q 6 (M II = Zn, Cd; M IV = Ge, Sn; Q = S, Se) chalcogenide system

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  22. One-Dimensional Double Chains in Sodium-Based Quaternary Chalcogenides Displaying Intriguing Red Emission and Large Optical Anisotropy

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  23. (Na0.60Ba0.70)Ga2Se4: An Infrared Nonlinear Optical Crystal Designed using AgGaSe2 as the Template

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  24. K2Na(IO3)2(I3O8) with Strong Second Harmonic Generation Response Activated by Two Types of Isolated Iodate Anions

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  26. A2SnS5: A Structural Incommensurate Modulation Exhibiting Strong Second‐Harmonic Generation and a High Laser‐Induced Damage Threshold (A=Ba, Sr)

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  27. KInSi1.32Sn0.68Se6: An Infrared Nonlinear Optical Material Containing Three Types of Tetrahedral Units

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

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  29. Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se20

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  30. A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs

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  31. Chalcophosphates: A Treasure House of Infrared Nonlinear Optical Materials

    Crystal Growth & Design · 2020-10-23

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  32. Sr6(Li2Cd)A4S16 (A = Ge, Sn): How to Go beyond the Band Gap Limitation via Site-Specific Modification

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  33. AMnAs3S6 (A = Cs, Rb): Phase-Matchable Infrared Nonlinear Optical Functional Motif [As3S6]3– Obtained via Surfactant–Thermal Method

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