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RESEARCH PAPER · Small · 2023

Breaking Through the Trade‐Off Between Wide Band Gap and Large SHG Coefficient in Mercury‐Based Chalcogenides for IR Nonlinear Optical Application

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Breaking Through the Trade‐Off Between Wide Band Gap and Large SHG Coefficient in Mercury‐Based Chalcogenides for IR Nonlinear Optical ApplicationOriginalGa-based IR nonlinear optical materials: Synthesis, structures, and properties65A UV non-hydrogen pure selenite nonlinear optical material for achieving balanced properties through framework-optimized structural transformation41Fully tricoordinated assembly unveils a pioneering nonlinear optical crystal (SbTeO 3 )(NO 3 )25Partial substitution with a significant effect: coexistence of a wide band gap and large birefringence in the oxychalcogenide AEGe 2 O 4 Se (AE = Sr and Ba)17Rare-earth-based chalcogenides and their derivatives: an encouraging IR nonlinear optical material candidate70RbPbPS 4 : a promising IR nonlinear optical material achieved by lone-pair-cation-substitution-induced structure transformation23Polysulfide Anions [S x ] 2− ( x = 2, 3, 4, 5): Promising Functional Building Units for Infrared Nonlinear Optical Materials22Hg3Se(SeO3)(SO4): A Mixed-Valent Selenium Compound with Mid-Infrared Transmittance Obtained by In Situ Reaction26KREP 2 S 6 (RE = Sm, Gd, Tb, Dy): A Series of Polar Rare-Earth Thiophosphates with High Laser-Induced Damage Thresholds and Moderate Nonlinear-Optical Responses Synergistically Contributed by Isolated P 2 S 6 Units and {[RE 2 S 15 ] 24– } ∞ Layers8Hg4(Te2O5)(SO4): A Giant Birefringent Sulfate Crystal Triggered by a Highly Selective Cation153A congruent-melting rubidium zinc vanadium oxychloride exhibiting strong mid-infrared second-harmonic generation and high laser-induced damage threshold6HgC4H4O6: A mercury tartrate exhibits phase matchable second harmonic generation effect1The first Hg-based oxychalcogenide Sr2HgGe2OS6: Achieving balanced IR nonlinear optical properties through synergistic cation and anion substitution28A Rare Earth Chalcogenide Nonlinear Optical Crystal KLaGeS4: Achieving Good Balance among Band Gap, Second Harmonic Generation Effect, and Birefringence12Old tree blossoms anew: Research progress on the structures and optical properties of ultraviolet selenites56Ag 2 GeS 3 : A Diamond‐Like Chalcogenide as an IR Nonlinear Optical Material with Outstanding Second‐Harmonic Generation Response28The centrosymmetric to non-centrosymmetric transformation induced by alkaline-earth cations producing infrared nonlinear optical AeMn6Ga6S16 (Ae = Ca, Sr)13Realizing Excellent Infrared Nonlinear Optical Performance in Eu-Based Chalcogenides via Rational Cross Substitution Strategy26Emergent Mid‐Infrared Nonlinear Optical Candidates With Targeted Balance Performances17Alkali metal/mercury dual-metal sulfides as infrared nonlinear optical materials with high laser-induced damage thresholds5Designing infrared nonlinear optical crystals, Sr 2 MgSn 2 OS 6 and Sr 2 SnGa 2 OS 6 , with hybrid anionic frameworks via a double substitution strategy4Exploring new horizons in mid-to-far infrared nonlinear optical crystals: the significant potential of trigonal pyramidal [TeS 3 ] 2− functional units18Isovalent cation substitution drives structural transformation and infrared nonlinear optical activity in Eu-based chalcogenides11Stereochemically active lone pair-induced large optical anisotropy in a novel infrared birefringent crystal Ba 2 La 2 Sb 4 S 10 (S 2 )5Structural diversity and photocurrent responses of multi-component chalcogenidometalates8AgGaS2 and Derivatives: Design, Synthesis, and Optical Properties8Discovering Pseudo-Supertetrahedral Functional Units in Salt-Inclusion Nonlinear Optical Material [Ba22(SO4)5][Zn14Ga18S58]14A theoretical study on absorbers for the intermediate band solar cell from group-IV element (Si, Ge, Sn) doped AgGaS24Nonbonding Electron Inversion‐Driven Structural Engineering: Synergistic Enhancement of Linear and Nonlinear Optical Properties3Nonbonding Electron Inversion‐Driven Structural Engineering: Synergistic Enhancement of Linear and Nonlinear Optical Properties26Diamond-Like HgIn2Q4 (Q = Se, Te) Synthesized by Flux-Assisted Boron-Chalcogen Method Exhibit Noteworthy Nonlinear Optical Properties Contributed by Three Types of Tetrahedral Motifs8From Centrosymmetric Ca3Ge2O3S4 to Noncentrosymmetric Ca3Ge2O4Se3: A Nonlinear Optical Ca-Based Oxyselenide5Alkali Metal Substitution-Induced Structural Transformation for RbREP2Se6 (RE = Gd, Tb, Dy) with Second-Harmonic Generation Responses6SrZnGeSe4: An Infrared Nonlinear Optical Crystal Material with Wide Transmission Range and Large SHG Response6Zn 0.7 Hg 0.3 Ga 2 Se 4 : a defect diamond-like selenide with a balanced band gap and nonlinear optical response0Rare-Earth Selenophosphates Cs 2 YP 2 Se 7 and KYP 2 Se 6 Synthesized by the RFMOBQ Routine: Structural Evolution and Nonlinear Optical Activity2Ba 4 CdGa 2 S 6 F 4 : A Chalcohalide Birefringent Crystal with Large Band Gap Designed by the Cation and Anion Cosubstitution Strategy2Recent Progress in Hg-Based Oxysalt Crystals for Nonlinear Optics and Birefringence Applications5Synergistic Distortion Engineering: Activating Nonlinear Optical Response in Quaternary Chalcogenides via Lattice‐Induced [MnS 4 ] Asymmetry1Cd/V Ratio-Driven Centrosymmetric Transition of Crystal Structures in Cesium Cadmium Vanadate Oxychlorides Cs 3 CdV 4 O 12 Cl and CsCdV 2 O 6 Cl0Heterovalent Coexistence‐Driven Symmetry Breaking and Dimensional Evolution: Designing Polar Heart‐Shaped Channels for Exceptional MFIR Nonlinear Optics5Defect Diamond‐Like d 10 Metal Indium Selenium With Strong Second‐Harmonic Generation and Enhanced Laser‐Induced Damage Threshold2A 3 Zr 2 (PS 4 )(P 2 S 7 ) 2 (A = K, Rb, Cs) Synthesized by the Metal Oxide-Boron-Chalcogen Routine: A Series of Zirconium-Based Thiophosphate Nonlinear Optical Crystals Featuring PS 4 Tetrahedron and P 2 S 7 Dimer0Nonlinear Optical-Active NaAlP 2 S 6 Synthesized by the MOBQ Method: Synthesis, Structure, and Optical Properties0Mid‐ to Far‐Infrared Nonlinear Optical Crystals: Design Strategies, Structure–Property Relationships and Engineering Prospects0Heterometallic Ge–O–Sn-Bridged Oxychalcogenides Sr3GeSnO4Q3 (Q = S, Se) with Wide Band Gaps and Moderate Infrared Nonlinear Optical Responses0Cation-substitution-driven electronic, nonlinear optical, elastic, and thermal transport properties of layered AeHgGeSe4 (Ae = Ba, Sr): A first-principles study0EuMn6Ga6S16: A Wide Bandgap Europium-Based Nonlinear Optical Sulfide0[CN4H8]SiF6: Fluorination-guided design of deep-UV crystal with large birefringence0

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  2. A UV non-hydrogen pure selenite nonlinear optical material for achieving balanced properties through framework-optimized structural transformation

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  3. Fully tricoordinated assembly unveils a pioneering nonlinear optical crystal (SbTeO 3 )(NO 3 )

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  6. RbPbPS 4 : a promising IR nonlinear optical material achieved by lone-pair-cation-substitution-induced structure transformation

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  7. Polysulfide Anions [S x ] 2− ( x = 2, 3, 4, 5): Promising Functional Building Units for Infrared Nonlinear Optical Materials

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  8. Hg3Se(SeO3)(SO4): A Mixed-Valent Selenium Compound with Mid-Infrared Transmittance Obtained by In Situ Reaction

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  9. KREP 2 S 6 (RE = Sm, Gd, Tb, Dy): A Series of Polar Rare-Earth Thiophosphates with High Laser-Induced Damage Thresholds and Moderate Nonlinear-Optical Responses Synergistically Contributed by Isolated P 2 S 6 Units and {[RE 2 S 15 ] 24– } ∞ Layers

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  10. Hg4(Te2O5)(SO4): A Giant Birefringent Sulfate Crystal Triggered by a Highly Selective Cation

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  11. A congruent-melting rubidium zinc vanadium oxychloride exhibiting strong mid-infrared second-harmonic generation and high laser-induced damage threshold

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  12. HgC4H4O6: A mercury tartrate exhibits phase matchable second harmonic generation effect

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  13. The first Hg-based oxychalcogenide Sr2HgGe2OS6: Achieving balanced IR nonlinear optical properties through synergistic cation and anion substitution

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  16. Ag 2 GeS 3 : A Diamond‐Like Chalcogenide as an IR Nonlinear Optical Material with Outstanding Second‐Harmonic Generation Response

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  17. The centrosymmetric to non-centrosymmetric transformation induced by alkaline-earth cations producing infrared nonlinear optical AeMn6Ga6S16 (Ae = Ca, Sr)

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  20. Alkali metal/mercury dual-metal sulfides as infrared nonlinear optical materials with high laser-induced damage thresholds

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