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RESEARCH PAPER · Journal of the American Chemical Society · 2019

How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates

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How To Maximize Birefringence and Nonlinearity of π-Conjugated CyanuratesOriginal“Old dog, new tricks”: the lone pair effect inducing divergent optical responses in lead cyanurates containing π-bonds18Rb3Na(H2C3N3O3)4·3H2O with Large Birefringence28NaRb3B6O9(OH)3(HCO3): A Borate-Bicarbonate Nonlinear Optical Material18Structural Diversity and Giant Birefringence in Cyanates BaCNOX (X = Cl, Br, I, and CNO) Containing Linear π-Conjugated Units: A Combined Experimental and Theoretical Study132(C 3 H 7 N 6 ) + ·2Cl − ·H 2 O: an ultraviolet nonlinear optical crystal with large birefrigence and strong second-harmonic generation78Enhanced optical anisotropy via dimensional control in alkali-metal chalcogenides18Facile synthesis of cesium trithiocyanurate with high ionic conductivity and large birefringence properties17Gd(NO 3 )(Se 2 O 5 )·3H 2 O: a nitrate–selenite nonlinear optical material with a short ultraviolet cutoff edge28Hydroisocyanurates X 2 Y(H 2 C 3 N 3 O 3 ) 4 ·4H 2 O (X = K, Cs; Y = Zn, Cd) with large birefringence stemming from π-conjugated (H 2 C 3 N 3 O 3 ) − anions28Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145K 4 Cu 3 (C 3 N 3 O 3 ) 2 X (X = Cl, Br): strong anisotropic layered semiconductors containing mixed p–p and d–p conjugated π-bonds7Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42Second-order nonlinear optical materials with a benzene-like conjugated π system49Lead 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 Materials55An Exceptional Peroxide Birefringent Material Resulting from d–π Interactions99An Exceptional Peroxide Birefringent Material Resulting from d–π Interactions15ZnIO3F: Zinc Iodate Fluoride with Large Birefringence and Wide Band Gap57Strong Second Harmonic Generation in a Tungsten Bronze Oxide by Enhancing Local Structural Distortion48New Alkaline-Earth Metal Fluoroiodates Exhibiting Large Birefringence and Short Ultraviolet Cutoff Edge with Highly Polarizable (IO 3 F) 2– Units63AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses63A(H3C3N3O3)(NO3) (A = K, Rb): Alkali-Metal Nitrate Isocyanurates with Strong Optical Anisotropy47Two Light‐Metal Dihydrogenisocyanurate Hydrates Linked by Diagonal Relationship: Syntheses, Crystal Structures, and Vibrational Spectra of Li[H2N3C3O3]·1.75 H2O and Mg[H2N3C3O3]2·8 H2O4LiGaF2(IO3)2: A mixed-metal gallium iodate-fluoride with large birefringence and wide band gap39An Optimal Arrangement of (H2C4N2O3)2– Groups in the First Non-Centrosymmetric Alkali Barbiturate Li2(H2C4N2O3)·2H2O Inducing a Giant Second Harmonic Generation Response and a Striking Birefringence43A UV birefringent crystal: RbNH4(H2C3N3O3)2·2H2O14Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm38Mechanochemical Preparation and Solid-State Characterization of 1:1 and 2:1 Ionic Cocrystals of Cyanuric Acid with Alkali Halides12Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research19Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research140Explorations of Second-Order Nonlinear Optical Materials in the Alkaline Earth Barbiturate System: Noncentrosymmetric Ca(H3C4N2O3)2·H2O and Centrosymmetric Sr(H5C8N4O5)2·4H2O23Mechanochemical Synthesis of an Ionic Cocrystal with Large Birefringence Resulting from Neutral Planar π-Conjugated Groups26Synergism of multiple functional chromophores significantly enhancing the birefringence in layered non-centrosymmetric chalcohalides20The synthesis, characterization, and theoretical analysis of (NH 4 ) 3 PbCl 52A melamine-based organic–inorganic hybrid material revealing excellent optical performance and moderate thermal stability75A new rare-earth borate birefringent crystal with quasi-two-dimensional [BO 3 ] layers23An organic–inorganic hybrid birefringent material with diverse functional groups38BaTi(BO 3 ) 2 : an excellent birefringent material with highly coplanar isolated [BO 3 ] groups16Co-crystal AX·(H 3 C 3 N 3 O 3 ) (A = Na, Rb, Cs; X = Br, I): a series of strongly anisotropic alkali halide cyanurates with a planar structural motif and large birefringence13Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2K 2 Pb(H 2 C 3 N 3 O 3 ) 4 (H 2 O) 4 : a potential UV nonlinear optical material with large birefringence50Sn 14 O 11 Br 6 : a promising birefringent material with a [Sn 14 O 11 Br 6 ] layer26Two bismuth iodate sulfates with enhanced optical anisotropy17Two metal-free cyanurate crystals with a large optical birefringence resulting from the combination of π-conjugated units17Zn(H 2 C 3 N 3 O 3 ) 2 ·3H 2 O: the first single- d 10 transition metal based ultraviolet hydroisocyanurate crystal with large birefringence18Finding Short-Wavelength Birefringent Crystals with Large Optical Anisotropy Activated by π-Conjugated [C(NH2)3] Units45The First Positive Uniaxial Cyanurate Crystals Containing a Crown-like Anionic Group Arrangement and Strengthened Optical Anisotropy17Discovery of NLO Semiorganic (C 5 H 6 ON) + (H 2 PO 4 ) − : Dipole Moment Modulation and Superior Synergy in Solar-Blind UV Region270Cyanurates consisting of intrinsic planar π-conjugated 6-membered rings: An emerging source of optical functional materials111Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application167Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application18Te(CS(NH2)2)4SO4·2H2O: A Three-in-One Semiorganic Nonlinear Optical Crystal with an Unusual Quadrilateral (TeS4)6– Chromophore14Steric Group Design for Enhancement of Optical Nonlinearity in Isoxazolone-Based Crystals and Terahertz-Wave Generation19Tin Chloride Sulfates A3Sn2(SO4)3–xCl1+2x (A = K, Rb, Cs; x = 0, 1) as Multifunctional Optical Materials33From Centrosymmetry to Noncentrosymmetry: Tailoring the Structural Arrangements of Carbonates with Strong Nonlinear Optical Response through Partial Anion Substitution33Fluorine‐Driven Enhancement of Birefringence in the Fluorooxosulfate: A Deep Evaluation from a Joint Experimental and Computational Study139Structure-performance relationship in tri-coordinated nonlinear optical materials toward optimal second harmonic generation and phase matching31Cs2ZnSn3S8: A Sulfide Compound Realizes a Large Birefringence by Modulating the Dimensional Structure24Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals146Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals16A 3D supramolecular framework assembled via π⋅⋅⋅π interactions and CH⋅⋅⋅Cl hydrogen-bonds with second-harmonic generation response2AZn4(OH)4(C3N3O3)2 (A = Mg, Zn): Two Zn-Based Cyanurate Crystals with Various Cation Coordination and Large Birefringence22The application and development of the first principles calculation in nonlinear optical materials1A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**175A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**272D van der Waals Layered [C(NH2)3]2SO3S Exhibits Desirable UV Nonlinear-Optical Trade-Off47Synthesis and crystal structure of the lanthanum cyanurate complex La[H2N3C3O3]3 · 8.5 H2O2An Overview on Recent Trends in Deep‐Ultraviolet (DUV) and Ultraviolet (UV) Nonlinear Optical Crystals25Enhancement of band gap and birefringence induced via π -conjugated chromophore with “tail effect”28Synthesis and Characterization of New-Type Ionic Cocrystals with Cyanuric Acid and Alkali Halides: AX·(H3C3N3O3)2 (A = Rb, Cs; X = Cl, Br)6From CeF2(SO4)·H2O to Ce(IO3)2(SO4): Defluorinated Homovalent Substitution for Strong Second-Harmonic-Generation Effect and Sufficient Birefringence53Guanidinium Fluorooxoborates as Efficient Metal-free Short-Wavelength Nonlinear Optical Crystals140Hierarchical Modulation of Optical Anisotropy Driven by Metal Cation Polyhedra in Fluorooxoborates MIIB4O6F2 (MII=Be, Mg, Pb, Zn, Cd)6[C(NH 2 ) 3 ] 2 S 2 O 8 : combining delocalized and localized π-conjugate units to achieve strong optical anisotropy21An excellent lead oxyiodide with a strong second-harmonic generation response and a large birefringence induced by the oriented arrangement of highly distorted [PbO 4 I 2 ] polyhedra13KF·B(OH) 3 : a KBBF-type material with large birefringence and remarkable deep-ultraviolet transparency33Linear unit BN 2 : a novel birefringence-enhanced fundamental module with sp orbital hybridization9Metal oxyhalides: an emerging family of nonlinear optical materials124Sc 2 F 2 (B 2 O 5 ): a deep ultraviolet scandium borate fluoride exhibiting large birefringence induced by the synergistic effect of B 2 O 5 and ScO n F 2 groups38First-principles study of the influence of lone pair electrons and molecular groups on the birefringence of phosphate and fluorophosphate13Driving Nonlinear Optical Activity with Dipolar 2-Aminopyrimidinium Cations in (C4H6N3)+(H2PO3)−115Potential optical functional crystals with large birefringence: Recent advances and future prospects322Healable, Recyclable, and Programmable Shape Memory Organogels Based on Highly Malleable Catalyst-Free Carboxylate Linkages18“Removing Center”─An Effective Structure Design Strategy for Nonlinear Optical Crystals37Cd4InO(BO3)3: A New Nonlinear Optical Crystal Exhibiting Strong Second Harmonic Generation Effect and Moderate Birefringence2LiB5O5F2(OH)4: A new deep-ultraviolet birefringent crystal with [B5O5F2(OH)4] anionic group28Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species6Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species83Noncentrosymmetric (C3H7N6)6(H2PO4)4(HPO4)·4H2O and Centrosymmetric (C3H7N6)2SO4·2H2O: Exploration of Acentric Structure by Combining Planar and Tetrahedral Motifs via Hydrogen Bonds37Cation-anion synergetic interactions achieving tunable birefringence in quasi-one-dimensional antimony(III) fluoride oxalates58Directional Construction of New Nonlinear Optical Bifunctional Units through Molecular Engineering Design Inspired by the B 3 O 7 -Typed Configuration23Sharp Enhancement of Birefringence in Antimony Oxalates Achieved by the Cation–Anion Synergetic Interaction Strategy38An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals81An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals22Crystal Growth of K2HCO3F·H2O with a Very Short Cutoff Edge and Large Birefringence17A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses15A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses96Dual-Ligand-Oriented Design of Noncentrosymmetric Complexes with Nonlinear-Optical Activity11Three polar indium phosphites exhibiting diverse structural networks and SHG-activity9SbHPO3F: 2D van der Waals Layered Phosphite Exhibiting Large Birefringence32ZrF2(IO3)2 and RbGaF3(IO3): Two Promising Birefringent Crystals Featuring 1D Metal-Fluoride Cationic Chains and Wide Bandgaps22Achieving effective balance between bandgap and birefringence by confining π-conjugation in an optically anisotropic crystal39Achieving Large Second Harmonic Generation Effects via Optimal Planar Alignment of Triangular Units64A High‐Performance Nonlinear Optical Crystal with a Building Block Containing Expanded π‐Delocalization95A High‐Performance Nonlinear Optical Crystal with a Building Block Containing Expanded π‐Delocalization5Perfectly Encoding π‐Conjugated Anions in the RE5(C3N3O3)(OH)12 (RE=Y, Yb, Lu) Family with Strong Second Harmonic Generation Response and Balanced Birefringence91Perfectly Encoding π‐Conjugated Anions in the RE5(C3N3O3)(OH)12 (RE=Y, Yb, Lu) Family with Strong Second Harmonic Generation Response and Balanced Birefringence18Li0.5Na0.5AlB2O4F2: Fluoroaluminoborate with Aligned 1∞[BO2] Chain Induced by Unprecedented [AlO3F3]6− Species Features Enhanced Birefringence30Explorations of Second-Order Nonlinear Optical Materials in the Monovalent Trithiocyanurate System18(C 5 H 6.16 N 2 Cl 0.84 )(IO 2 Cl 2 ): a birefringent crystal featuring unprecedented (IO 2 Cl 2 ) − anions and π-conjugated organic cations56A 0.5 H 2 C 6 N 7 O 3 ·4H 2 O (A = Ca 2+ , Sr 2+ ) iso-cyamelurates with ultra-large π-conjugated group and excellent nonlinear optical properties10A UV solar-blind nonlinear optical crystal with confined π-conjugated groups13Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181C 3 N 6 H 7 SO 3 NH 2 : non-π-conjugated tetrahedra decoupling π-conjugated groups achieving large optical anisotropy and wide band gap29Compounds consisting of coplanar π-conjugated B3O6-typed structures: An emerging source of ultraviolet nonlinear optical materials20Design and synthesis of anisotropic crystals with π -conjugated rings toward giant birefringence36KRb 2 (NO 3 ) 2 Cl: a new birefringent crystal exhibiting a perovskite-related framework and a short cutoff edge6Ultrastable 3D cage-like metal–organic frameworks constructed using polydentate cyanurate ligands and their gas adsorption properties6β-(C 3 H 7 N 6 ) 2 Cl 2 ·H 2 O and (C 3 H 7 N 6 )F·H 2 O: two UV birefringent crystals induced by uniformly aligned structural groups35Two Carboxylate-Cyanurates with Strong Optical Anisotropy and Large Band Gaps6α-BBO-like π-Conjugated Crystal with Large Birefringence16NaRb 6 (B 4 O 5 (OH) 4 ) 3 (BO 2 ) Featuring Noncentrosymmetry, Chirality, and the Linear Anionic Group BO 2 –100The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO 3 ) 2 and Y 3 F(SeO 3 ) 485The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO3)2 and Y3F(SeO3)47A Second‐Order Nonlinear Optical Material Consisting of Two π‐Conjugated Groups10Recent Development of Sn II , Sb III ‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence130Recent Development of SnII, SbIII‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence6Unveiling the Superior Optical Properties of Novel Melamine‐Based Nonlinear Optical Material with Strong Second‐Harmonic Generation and Giant Optical Anisotropy74A BBO-like trithiocyanate with significantly enhanced birefringence and second-harmonic generation39A Hydrogen Bonded Supramolecular Framework Birefringent Crystal89A Hydrogen Bonded Supramolecular Framework Birefringent Crystal13Cs 2 Mg(H 2 C 3 N 3 S 3 ) 4 ·8H 2 O: An Excellent Birefringent Material with Giant Optical Anisotropy in π-Conjugated Trithiocyanurate19“Cation Activation”: An Effective Strategy for the Enhancement of Birefringence36Birefringence Regulation by Clarifying the Relationship Between Stereochemically Active Lone Pairs and Optical Anisotropy in Tin‐based Ternary Halides56Birefringence Regulation by Clarifying the Relationship Between Stereochemically Active Lone Pairs and Optical Anisotropy in Tin‐based Ternary Halides2Naphthalene-Like Unit That Induces Strong Optical Anisotropy in C10H8NO2Br and C10H8NO2Br·H2O12Design of the Ionic Organic Nonlinear Optical Material NH 4 [LiC 3 H(CH 3 )O 4 ] with Ultrawide Band Gap and Moderate Birefringence79Design of the Ionic Organic Nonlinear Optical Material NH 4 [LiC 3 H(CH 3 )O 4 ] with Ultrawide Band Gap and Moderate Birefringence9Atomic Substitution to Tune ScO6 Distortion in Ba2MSc2(BO3)4 (M = Na, K, Ba) to Acquire a Large Birefringence15Understanding the Correlation Between Structure and Entangled Photon Pair Properties with Metal–Organic Frameworks5Roadmap on nonlinear optics–focus on Chinese research12Birefringent Glass‐Engraved Tilted Pillar Metasurfaces for High Power Laser Applications21Ultraviolet Crystal with Strong Optical Nonlinearity by Creating Halogen-Centered Secondary Building Blocks15Introduction of the [B–O/F] Units Enhances the Band Gap and Birefringence from Na6Mg3B10O18F6 to K3NaB10O16F211Li2RbSO4Cl with a Short Ultraviolet Absorption Edge and an Acentric Structure through Assembling Heteroleptic [LiO3Cl] Tetrahedra2NaCl·CH4N2O·H2O: An Organic–Inorganic Hybrid Ultraviolet Nonlinear Optical Crystal with Optimized Comprehensive Properties8Enlargement of Bandgap and Birefringence in Nonlinear Optical Alkali‐Metal Sulfate Crystals by the Substitution of Asymmetrical Non‐π‐Conjugated Cation8A potassium lead 2-methylmalonate-iodide nonlinear optical crystal with strong second-harmonic generation response and large birefringence2Designing Sulfate Crystals with Strong Optical Anisotropy through π‐Conjugated Tailoring51

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  1. “Old dog, new tricks”: the lone pair effect inducing divergent optical responses in lead cyanurates containing π-bonds

    Dalton Transactions · 2019-12-11

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  2. Rb3Na(H2C3N3O3)4·3H2O with Large Birefringence

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  3. NaRb3B6O9(OH)3(HCO3): A Borate-Bicarbonate Nonlinear Optical Material

    Inorganic Chemistry · 2019-12-17

    Fenghua Ding, Weilong Zhang, Matthew Lander Nisbet, Weiguo Zhang, P. Shiv Halasyamani, Zhihua Yang, Shilie Pan, Kenneth Reinhard Poeppelmeier

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  4. Structural Diversity and Giant Birefringence in Cyanates BaCNOX (X = Cl, Br, I, and CNO) Containing Linear π-Conjugated Units: A Combined Experimental and Theoretical Study

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  5. 2(C 3 H 7 N 6 ) + ·2Cl − ·H 2 O: an ultraviolet nonlinear optical crystal with large birefrigence and strong second-harmonic generation

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  9. Hydroisocyanurates X 2 Y(H 2 C 3 N 3 O 3 ) 4 ·4H 2 O (X = K, Cs; Y = Zn, Cd) with large birefringence stemming from π-conjugated (H 2 C 3 N 3 O 3 ) − anions

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  11. K 4 Cu 3 (C 3 N 3 O 3 ) 2 X (X = Cl, Br): strong anisotropic layered semiconductors containing mixed p–p and d–p conjugated π-bonds

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  12. Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect

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  13. Second-order nonlinear optical materials with a benzene-like conjugated π system

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

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

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  16. An Exceptional Peroxide Birefringent Material Resulting from d–π Interactions

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  18. ZnIO3F: Zinc Iodate Fluoride with Large Birefringence and Wide Band Gap

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  19. Strong Second Harmonic Generation in a Tungsten Bronze Oxide by Enhancing Local Structural Distortion

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  20. New Alkaline-Earth Metal Fluoroiodates Exhibiting Large Birefringence and Short Ultraviolet Cutoff Edge with Highly Polarizable (IO 3 F) 2– Units

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  21. AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses

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  22. A(H3C3N3O3)(NO3) (A = K, Rb): Alkali-Metal Nitrate Isocyanurates with Strong Optical Anisotropy

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  23. Two Light‐Metal Dihydrogenisocyanurate Hydrates Linked by Diagonal Relationship: Syntheses, Crystal Structures, and Vibrational Spectra of Li[H2N3C3O3]·1.75 H2O and Mg[H2N3C3O3]2·8 H2O

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  25. An Optimal Arrangement of (H2C4N2O3)2– Groups in the First Non-Centrosymmetric Alkali Barbiturate Li2(H2C4N2O3)·2H2O Inducing a Giant Second Harmonic Generation Response and a Striking Birefringence

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  27. Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm

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  28. Mechanochemical Preparation and Solid-State Characterization of 1:1 and 2:1 Ionic Cocrystals of Cyanuric Acid with Alkali Halides

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  29. Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research

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  30. Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research

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  31. Explorations of Second-Order Nonlinear Optical Materials in the Alkaline Earth Barbiturate System: Noncentrosymmetric Ca(H3C4N2O3)2·H2O and Centrosymmetric Sr(H5C8N4O5)2·4H2O

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  32. Mechanochemical Synthesis of an Ionic Cocrystal with Large Birefringence Resulting from Neutral Planar π-Conjugated Groups

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