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RESEARCH PAPER · Coordination Chemistry Reviews · 2018

Second-order nonlinear optical crystals with mixed anions

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Second-order nonlinear optical crystals with mixed anionsOriginalThe first investigation of europium silicate melilite for second-order nonlinear optical application: experimental and theoretical studies29Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59Second-order nonlinear optical properties of CuGa In1-Se2 (x = 0.54): Experimental and theoretical investigations4Cu2EuMQ4 (M = Si, Ge; Q = S, Se): Syntheses, structure study and physical properties determination26A Langbeinite-Type Yttrium Phosphate LiCs2Y2(PO4)336A Facile Route to Nonlinear Optical Materials: Three‐Site Aliovalent Substitution Involving One Cation and Two Anions137A Facile Route to Nonlinear Optical Materials: Three‐Site Aliovalent Substitution Involving One Cation and Two Anions23“Two in one”: an unprecedented mixed anion, Ba 2 (C 3 N 3 O 3 )(CNO), with the coexistence of isolated sp and sp 2 π-conjugated groups15A 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 birefringences50Cs 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 activity19Li 2 Na 2 [B 12 O 19 (OH) 2 ]: a new open framework borate with a pcu-type net constructed from large cyclic dodeca-oxoboron units8Mg(H 2 O) 6 B 4 O 5 (OH) 4 (H 2 O) 3 : a new hydrated borate with a short DUV cutoff edge9Monoclinic 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 495Synthesis, structure and characterization of M(IO 3 ) 2 (HIO 3 ) (M = Ca, Sr) as new anhydrous alkaline earth metal bis-iodate hydrogeniodate compounds16Li2CsB7O10(OH)4: A Deep-Ultraviolet Nonlinear-Optical Mixed-Alkaline Borate Constructed by Unusual Heptaborate Anions98Pb4B6O13: A Polar Lead Oxyborate with Uncommon ∞(B6O12)6– Layers Exhibiting a Large Second Harmonic Generation Response15Targeting the Next Generation of Deep-Ultraviolet Nonlinear Optical Materials: Expanding from Borates to Borate Fluorides to Fluorooxoborates450Transition Metal Free Monoclinic Eu8In17.33S34 and Its Anisotropic Photoelectronic Responses25Heteroanionic Materials by Design: Progress Toward Targeted Properties236Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)28Large 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 Selenide48Ba10In6Zn7S10Se16 and Ba10In6Zn7Se26: Two new infrared nonlinear optical materials with T2 super tetrahedron6KBiCl2SO4: The First Bismuth Chloride Sulfate Being Second-Order Nonlinear Optical Active44Mixed-Anion Inorganic Compounds: A Favorable Candidate for Infrared Nonlinear Optical Materials140Two Indium Sulfate Tellurites: Centrosymmetric In 2 (SO 4 )(TeO 3 )(OH) 2 (H 2 O) and Non-centrosymmetric In 3 (SO 4 )(TeO 3 ) 2 F 3 (H 2 O)33Sn2Ga2S5: A Type of IR Nonlinear-Optical Material22Nitrate nonlinear optical crystals: A survey on structure-performance relationships146LiBa2MIIIQ4 (MIII = Al, Ga, In; Q = S, Se): A Series of Metal Chalcogenides with a Structural Transition12Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides63A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48A highly distorted HgS 4 tetrahedron-induced moderate second-harmonic generation response of EuHgGeS 462Ba 6 In 6 Zn 4 Se 19 : a high performance infrared nonlinear optical crystal with [InSe 3 ] 3− trigonal planar functional motifs22BaLiTe2O5X (X = Cl, Br): mixed alkali/alkaline-earth metal tellurite halides with [Te2O5]∞ chains11Coordinated 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 materials28Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145K 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 ] − groups14Mixed-metal thiophosphate CuCd 3 PS 6 : an infrared nonlinear optical material activated by its three-in-one tetrahedra-stacking architecture33Regulated molecular rotor in phase transition materials with switchable dielectric and SHG effect31Second-order nonlinear optical materials with a benzene-like conjugated π system49Similarities and differences between Mn( ii ) and Zn( ii ) coordination polymers supported by porphyrin-based ligands: synthesis, structures and nonlinear optical properties24Sr 4 Pb 1.5 Sb 5 O 5 Se 8 : a new mid-infrared nonlinear optical material with a moderate SHG response22The functionality of tetrahedral units in fluoroxoiodates: fluorine-modulating effects in iodates with lone pair electrons3Designing Sulfide Borate as a Novel Type of Second-Order Nonlinear-Optical Material91Structure-property relationship in nonlinear optical materials with π-conjugated CO3 triangles146Two Covalent Ultraviolet Nonlinear Optical Crystals3A Series of Chalcogenide Borates RE6Ta2MgQB8O26 (RE = Sm, Eu, Gd; Q = S, Se) Featuring a B4O10 Cluster33(Na0.60Ba0.70)Ga2Se4: An Infrared Nonlinear Optical Crystal Designed using AgGaSe2 as the Template38Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement96Enhancement of Second-Order Optical Nonlinearity in a Lutetium Selenite by Monodentate Anion Partial Substitution58Designing a Deep-UV Nonlinear Optical Fluorooxosilicophosphate127Hexagonal In2Se3: A Defect Wurtzite-Type Infrared Nonlinear Optical Material with Moderate Birefringence Contributed by Unique InSe5 Unit75LiBa4Ga5Q12 (Q = S, Se): Noncentrosymmetric Metal Chalcogenides with a Cesium Chloride Topological Structure Displaying a Remarkable Laser Damage Threshold32Aliovalent-substituted synthesis for a non-centrosymmetric phosphate with enhanced nonlinear-optical response5KInSi1.32Sn0.68Se6: An Infrared Nonlinear Optical Material Containing Three Types of Tetrahedral Units19Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014BiGa(SeO3)3: A Phase Matchable SHG Material Achieved by Cation Substitution19Microscopic Insights into the Reconstructive Phase Transition of KNaNbOF5 with 19F NMR Spectroscopy8A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107Second-Order Nonlinear-Optical-Active Selenide Borate YSeBO2: Featuring a [YSeBO2]n Planar Belt39Structure-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 Ba4Ge3Se9Br222Realizing Deep-Ultraviolet Second Harmonic Generation by First-Principles-Guided Materials Exploration in Hydroxyborates111Zn4B6O13: Efficient Borate Photocatalyst with Fast Carrier Separation for Photodegradation of Tetracycline44From Ag2Zr(IO3)6 to LaZr(IO3)5F2: A Case of Constructing Wide‐band‐gap Birefringent Materials through Chemical Cosubstitution11Borates as promising electrode materials for rechargeable batteries92Two Mixed-Anion Units of [GeOSe3] and [GeO3S] Originating from Partial Isovalent Anion Substitution and Inducing Moderate Second Harmonic Generation Response and Large Birefringence55Ba(MoO 2 F) 2 (QO 3 ) 2 (Q = Se, Te): Partial Fluorination of MoO 6 Octahedra Enabling Two Polar Solids with Strong and Phase Matchable SHG Response69Investigation of the second-order nonlinear optical property of Sr6Sb6S173Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95Sb6O7(SO4)2: A Promising Ultraviolet Nonlinear Optical Material with an Enhanced Second‐Harmonic‐Generation Response Activated by SbIII Lone‐Pair Stereoactivity62Hydrogen-Bond-Assisted Alignment of [MCu(SeO 3 ) 4 Cl(H 2 O)] 4– (M = Fe, Ga) Anionic Layers to Form Two Polar Oxychlorides: Pb 2 MCu(SeO 3 ) 4 Cl(H 2 O)10A series of M 3 PS 4 (M = Ag, Cu and Ag/Cu) thiophosphates with diamond-like structures exhibiting large second harmonic generation responses and moderate ion conductivities28A series of oxysulfides RE 2 M 2 S 3 O 4 (RE = Y, Tm; M = Zr, Hf) featuring a unique MS 3 O 4 motif and {[M 2 S 3 O 4 ] 8− } ∞ wrinkle layer13Ba 2 [FeF 4 (IO 3 ) 2 ]IO 3 : a promising nonlinear optical material achieved by chemical-tailoring-induced structure evolution8Balanced infrared nonlinear optical performance achieved by modulating the covalency and ionicity distributions in the electron localization function map42First chiral fluorinated lead vanadate selenite Pb 2 (V 2 O 4 F)(VO 2 )(SeO 3 ) 3 with five asymmetric motifs and large optical properties24K 3 Na(TaF 7 )(SiF 6 ): a mixed-anion pentanary fluoride with zero-dimensional anions exhibiting a large band gap14La 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 threshold15Na 4 SnS 4 and Na 4 SnSe 4 exhibiting multifunctional physicochemical performances as potential infrared nonlinear optical crystals and sodium ion conductors27Recent advances of oxyfluorides for nonlinear optical applications69Role of fluorine on the structure and second-harmonic-generation property of inorganic selenites and tellurites23Halonitrides 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 Effect25M3B6O10NO3 (M = K, Rb): Two New Alkali Metal Borate‐Nitrates with Noncentrosymmetric Structures20Large Second-Harmonic Response and Giant Birefringence of CeF 2 (SO 4 ) Induced by Highly Polarizable Polyhedra248Introduction of Li into Ag-Based Noncentrosymmetric Sulfides for High-Performance Infrared Nonlinear Optical Materials40ASb5S8 (A = K, Rb, and Cs): Thermal Switching of Infrared Nonlinear Optical Properties across the Crystal/Glass Transformation39Unique Unilateral-Chelated Mode-Induced d–p−π Interaction Enhances Second-Harmonic Generation Response in New Ln3LiMS7 Family41High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies323Exploring Deep-UV Nonlinear Optical Materials with Enhanced Second Harmonic Generation Response and Birefringence in Fluoroaluminoborate Crystals69Structural Transformation and Second-Harmonic-Generation Activity in Rare-Earth and d0 Transition-Metal Oxysulfides RE3NbS3O4 (RE = Ce, Sm, Gd, Dy)38A review of the structural diversity of [P x S y ] n − motifs and their potential application prospects in metal thiophosphates21Linear and Nonlinear Optical Properties of Centrosymmetric Sb 4 O 5 SO 4 and Noncentrosymmetric Sb 4 O 4 (SO 4 )(OH) 2 Induced by Lone Pair Stereoactivity55Heterobimetallic Cluster‐Based Coordination Polymers: Assembly, Structures and Third‐Order Nonlinear Optical Properties4SnPQ3 (Q = S, Se, S/Se): A Series of Lone-Pair Cationic Chalcogenophosphates Exhibiting Balanced NLO Activity Originating from SnQ8 Units49Noncentrosymmetric Rb3(COOH)3(H3BO3)2 vs Centrosymmetric Cs3(COOH)3(H3BO3)214Cd3(PO4)(TePO6): A Novel Cadmium Tellurite‐Phosphate featuring a {[TePO6]3−}∞ Chain15A Lead Mixed Halide with Three Different Coordinated Anions and Strong Second‐Harmonic Generation Response10Machine Learning with Multilevel Descriptors for Screening of Inorganic Nonlinear Optical Crystals35Highly polarized [GeOTe 3 ] motif-driven structural order promotion and an enhanced second harmonic generation response in the new nonlinear optical oxytelluride Ba 3 Ge 2 O 4 Te 334NH4Sb2(C2O4)F5: A novel UV nonlinear optical material synthesized in deep eutectic solvents38Halogen-Ion-Induced Structural Phase Transition Giving a Polymorph of HgBr2 with Balanced Nonlinear Optical Properties8Complex coordinated functional groups: A great genes for nonlinear optical materials64Sn7Br10S2: 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 Properties145(C 3 N 6 H 7 ) 2 SiF 6 ·H 2 O: an ultraviolet birefringent crystal exceeding the intrinsic energy gap of an organic reagent38AIn 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 responses11BaSc 2 (HPO 3 ) 4 (H 2 O) 2 : a new nonlinear optical phosphite exhibiting a 3D {[Sc 2 (HPO 3 ) 4 ] 2− } ∞ anionic framework and phase-matchable SHG effect32From 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 materials19Infrared nonlinear optical sulfide CsCd 4 In 5 S 12 exhibiting large second harmonic generation response16KEu 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 ring10Metal oxyhalides: an emerging family of nonlinear optical materials124Na 3 B 6 O 10 (HCOO): an ultraviolet nonlinear optical sodium borate-formate33Rb2MGe3S8 (M=Zn, Cd): Non-Centrosymmetry Transformation Led by Structure Change of [MGe3S8]2- Unit※4Where the extraordinaries meet: a cascade of isosymmetrical superionic phase transitions and negative thermal expansion in a novel silver salt-inclusion borate halide15Quaternary Noncentrosymmetric Rare-Earth Sulfides Ba4RE2Cd3S10 (RE = Sm, Gd, or Tb): A Joint Experimental and Theoretical Investigation17From Cc to P 6 3 mc : Structural Variation in La 3 S 2 Cl 2 [SbS 3 ] and La 3 OSCl 2 [SbS 3 ] Induced by the Isovalent Anion Substitution22Two non-centrosymmetric scandium borate nonlinear optical crystals containing the B5O10 anion group26Na 3 Ti 3 O 3 (SeO 3 ) 4 F: A Phase-Matchable Nonlinear-Optical Crystal with Enlarged Second-Harmonic-Generation Intensity and Band Gap20Advances in second-order nonlinear optical sulfates38Ba2B10O16(OH)2·(H3BO3)(H2O): A Possible Deep-Ultraviolet Nonlinear-Optical Barium Borate36CsY(SO4)2·4H2O: A Deep-Ultraviolet Birefringent Crystal Induced by an Edge-Sharing Connection26K3ZrF4(SbF4)(SbF5) and K8(ZrF6)(Sb2Zr2F20): Two Zirconium Fluoroantimonites with Low Dimensional Structures and Wide Transparency Range12Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material51Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material12NaGa3Se5: An Infrared Nonlinear Optical Material with Balanced Performance Contributed by Complex {[Ga3Se5]−}∞ Anionic Network14A deep ultraviolet transparent birefringent monofluorophosphate: Cd2.5(NH4)2(PO3F)3Cl ⋅ 2H2O4Mixed Anion Semiconductor In8S2.82Te6.18(Te2)33SrAgAsS4: A Noncentrosymmetric Sulfide with Good Infrared Nonlinear Optical Performance Induced by Aliovalent Substitution from Centrosymmetric SrGa2S412Noncentrosymmetric (C3H7N6)6(H2PO4)4(HPO4)·4H2O and Centrosymmetric (C3H7N6)2SO4·2H2O: Exploration of Acentric Structure by Combining Planar and Tetrahedral Motifs via Hydrogen Bonds37AgGaSe2-Inspired Nonlinear Optical Materials: Tetrel Selenides of Alkali Metals and Mercury34First Investigation of Nonlinear Optical Oxychalcogenide with Three‐Dimensional Anionic Framework and Special Windmill‐Like Functional Motifs †28Electrocarboxylation of Aryl Epoxides with CO2for the Facile and Selective Synthesis of β‐Hydroxy Acids17Electrocarboxylation of Aryl Epoxides with CO2for the Facile and Selective Synthesis of β‐Hydroxy Acids113Designing a deep-UV nonlinear optical monofluorophosphate22Chiral Lead-Free Double Perovskite Single-Crystalline Microwire Arrays for Anisotropic Second-Harmonic Generation45(C3N6H7)2SbF5·H2O Exhibiting Strong Optical Anisotropy from the Optimal Arrangement of π-Conjugated (C3N6H7)+ Groups31Sb5O7I: Exploration of Ternary Antimony-Based Oxyhalide as a Nonlinear-Optical Material27[Cs6Cl][Ga5GeQ12] (Q = S, Se): two novel porous layered chalcohalides exhibiting two-band emission and ion exchange properties6PbBi(SeO 3 ) 2 F and Pb 2 Bi(SeO 3 ) 2 Cl 3 : Coexistence of Three Kinds of Stereochemically Active Lone-Pair Cations Exhibiting Excellent Nonlinear Optical Properties57Oxychalcogenides as Promising Ultraviolet Nonlinear Optical Candidates: Experimental and Theoretical Studies of AEGeOS2(AE = Sr and Ba)24Ternary AGa5S8 (A = K, Rb, Cs): Promising infrared nonlinear optical materials rationally realized by “one-for-multiple substitution” strategy37Dual-Ligand-Oriented Design of Noncentrosymmetric Complexes with Nonlinear-Optical Activity11Three polar indium phosphites exhibiting diverse structural networks and SHG-activity9Novel structural transformation in K3ReP2S8 thiophosphates originating from the rare-earth (Re) cation sizes induced local coordination asymmetry25

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  1. The first investigation of europium silicate melilite for second-order nonlinear optical application: experimental and theoretical studies

    Dalton Transactions · 2018-01-01

    Yang Chi, Huaiguo Xue, Sheng‐Ping Guo

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

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

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  4. 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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  5. A Langbeinite-Type Yttrium Phosphate LiCs2Y2(PO4)3

    Inorganic Chemistry · 2018-10-09

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  6. A Facile Route to Nonlinear Optical Materials: Three‐Site Aliovalent Substitution Involving One Cation and Two Anions

    Angewandte Chemie International Edition · 2018-12-27

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  7. A Facile Route to Nonlinear Optical Materials: Three‐Site Aliovalent Substitution Involving One Cation and Two Anions

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  8. “Two in one”: an unprecedented mixed anion, Ba 2 (C 3 N 3 O 3 )(CNO), with the coexistence of isolated sp and sp 2 π-conjugated groups

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  9. 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

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  10. 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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  11. 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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  12. Li 2 Na 2 [B 12 O 19 (OH) 2 ]: a new open framework borate with a pcu-type net constructed from large cyclic dodeca-oxoboron units

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  13. Mg(H 2 O) 6 B 4 O 5 (OH) 4 (H 2 O) 3 : a new hydrated borate with a short DUV cutoff edge

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

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  15. 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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  16. Synthesis, structure and characterization of M(IO 3 ) 2 (HIO 3 ) (M = Ca, Sr) as new anhydrous alkaline earth metal bis-iodate hydrogeniodate compounds

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  17. Li2CsB7O10(OH)4: A Deep-Ultraviolet Nonlinear-Optical Mixed-Alkaline Borate Constructed by Unusual Heptaborate Anions

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  18. Pb4B6O13: A Polar Lead Oxyborate with Uncommon ∞(B6O12)6– Layers Exhibiting a Large Second Harmonic Generation Response

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  19. Targeting the Next Generation of Deep-Ultraviolet Nonlinear Optical Materials: Expanding from Borates to Borate Fluorides to Fluorooxoborates

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  20. Transition Metal Free Monoclinic Eu8In17.33S34 and Its Anisotropic Photoelectronic Responses

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  21. Heteroanionic Materials by Design: Progress Toward Targeted Properties

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  22. Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)

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  23. Large Second Harmonic Generation (SHG) Effect and High Laser‐Induced Damage Threshold (LIDT) Observed Coexisting in Gallium Selenide

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  24. Large Second Harmonic Generation (SHG) Effect and High Laser‐Induced Damage Threshold (LIDT) Observed Coexisting in Gallium Selenide

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  25. Ba10In6Zn7S10Se16 and Ba10In6Zn7Se26: Two new infrared nonlinear optical materials with T2 super tetrahedron

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  28. Two Indium Sulfate Tellurites: Centrosymmetric In 2 (SO 4 )(TeO 3 )(OH) 2 (H 2 O) and Non-centrosymmetric In 3 (SO 4 )(TeO 3 ) 2 F 3 (H 2 O)

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  29. Sn2Ga2S5: A Type of IR Nonlinear-Optical Material

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  30. Nitrate nonlinear optical crystals: A survey on structure-performance relationships

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

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  32. Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides

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

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