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RESEARCH PAPER · Journal of the American Chemical Society · 2019

KLi(HC 3 N 3 O 3 )·2H 2 O: Solvent-drop Grinding Method toward the Hydro-isocyanurate Nonlinear Optical Crystal

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KLi(HC 3 N 3 O 3 )·2H 2 O: Solvent-drop Grinding Method toward the Hydro-isocyanurate Nonlinear Optical CrystalOriginal“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 rich structural chemistry in π-conjugated hydroisocyanurates: layered structures of A 2 B(H 2 C 3 N 3 O 3 ) 4 · n H 2 O (A = K, Rb, Cs; B = Mg, Ca; n = 4, 10) with high ultraviolet transparency and strong optical anisotropy47Co-crystal LiCl·(H 3 C 3 N 3 O 3 ): a promising solar-blind nonlinear optical crystal with giant nonlinearity from coplanar π-conjugated groups78CO(NH 2 ) 2 ·NH 4 Cl: an ultraviolet birefringent material with conjugated CO groups16Intrinsic zero thermal expansion in cube cyanurate K 6 Cd 3 (C 3 N 3 O 3 ) 423LiO 4 tetrahedra lock the alignment of π-conjugated layers to maximize optical anisotropy in metal hydroisocyanurates44RE(H 2 C 3 N 3 O 3 ) 2 ·(OH)· x H 2 O (RE = La, Y and Gd): potential UV birefringent materials with strong optical anisotropy originating from the (H 2 C 3 N 3 O 3 ) − group31Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation66Cs3Na(H2C3N3O3)4·3H2O: A Mixed Alkali‐Metal Hydroisocyanurate Nonlinear Optical Material Containing π‐Conjugated Six‐Membered‐Ring Units68Parallel Alignment of π-Conjugated Anions in Hydroisocyanurates Enhancing Optical Anisotropy25Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups45Nitrate nonlinear optical crystals: A survey on structure-performance relationships146How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates327Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin255Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin33RbNa(HC 3 N 3 O 3 )·2H 2 O exhibiting a strong second harmonic generation response and large birefringence as a new potential UV nonlinear optical material69CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Crystal property and spectroscopic investigation on electro-optic and physico-chemical properties of NLO crystal; 3-(3,4-Dihydroxyphenyl)-L-Alanine3“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-bonds7NaK 15 [B 4 O 5 (OH) 4 ] 6 (NO 2 ) 2 (CO 3 )·7H 2 O: assembly of an unprecedented mixed anion inorganic compound via a facile hydrothermal route4Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42Rb 3 BaTeB 7 O 15 : a novel [B 7 O 16 ] fundamental building block in a new telluroborate with [TeO 3 ] polyhedra11Second-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 Materials55Enhancement of Second-Order Optical Nonlinearity in a Lutetium Selenite by Monodentate Anion Partial Substitution58ZnIO3F: Zinc Iodate Fluoride with Large Birefringence and Wide Band Gap57Dimensionality–Band Gap–Third-Harmonic Generation Property Relationship in Novel Main-Group Metal Iodates37K4Sb(SO4)3Cl: The first apatite-type sulfate ultraviolet nonlinear optical material with sharply enlarged birefringence61Functional Chalcogenide Na2HgSn2Se6 and K2MnGe2Se6 Exhibiting Flexible Chain Structure and Intriguing Birefringence Tunability16A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107Rational Design of the Metal‐Free KBe 2 BO 3 F 2 ⋅(KBBF) Family Member C(NH 2 ) 3 SO 3 F with Ultraviolet Optical Nonlinearity201Rational Design of the Metal‐Free KBe2BO3F2⋅(KBBF) Family Member C(NH2)3SO3F with Ultraviolet Optical Nonlinearity31AGa 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 Anisotropy47High Coordinate Metal Iodate Chlorides with Diverse Structural Motifs and Tunable Birefringence10Second-order nonlinear optical-active selenide borate Zn8Se2(BO2)12: Experimental and theoretical analysis9LiGaF2(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 μm38Explorations of Second-Order Nonlinear Optical Materials in the Alkaline Earth Barbiturate System: Noncentrosymmetric Ca(H3C4N2O3)2·H2O and Centrosymmetric Sr(H5C8N4O5)2·4H2O23Two Mixed-Anion Units of [GeOSe3] and [GeO3S] Originating from Partial Isovalent Anion Substitution and Inducing Moderate Second Harmonic Generation Response and Large Birefringence55Mechanochemical Synthesis of an Ionic Cocrystal with Large Birefringence Resulting from Neutral Planar π-Conjugated Groups26KSnI 3 ⋅ H 2 O: A New Compound with One‐Dimensional SnI 3 Chains of Pyramidal SnI 5 Polyhedra2Crystal growth, characterization and theoretical studies of the noncentrosymmetric compound Al3(IO3)9·(HIO3)6·18H2O4An Antimony(III) Fluoride Oxalate with Large Birefringence45A melamine-based organic–inorganic hybrid material revealing excellent optical performance and moderate thermal stability75Barium fluoroiodate crystals with a large band gap and birefringence22BaTi(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 birefringence50Two 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 birefringence18Dendrons containing boric acid and 1,3,5-tris(2-hydroxyethyl)isocyanurate covalently attached to silica-coated magnetite for the expeditious synthesis of Hantzsch esters32Finding Short-Wavelength Birefringent Crystals with Large Optical Anisotropy Activated by π-Conjugated [C(NH2)3] Units45Second-order nonlinear optical and photoelectric properties of Zn4B6O12S20The 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 Region270π‑Conjugated Trigonal Planar [C(NH2)3]+ Cationic Group: A Superior Functional Unit for Ultraviolet Nonlinear Optical Materials52Cyanurates 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– Chromophore14Tin 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 Study139Hydroxyfluorooxoborate 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 Crystals16AZn4(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 materials1Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate22Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units102Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units9La 3 Ga 3 Ge 2 S 3 O 10 : An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering63La3Ga3Ge2S3O10: An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering18An Overview on Recent Trends in Deep‐Ultraviolet (DUV) and Ultraviolet (UV) Nonlinear Optical Crystals25H{[Na(H2O)3]6F}(PO4)2 ⋅ 2(H2O): A New Polycation‐Type Phosphate with Deep Ultraviolet Transparency0Synthesis and Characterization of New-Type Ionic Cocrystals with Cyanuric Acid and Alkali Halides: AX·(H3C3N3O3)2 (A = Rb, Cs; X = Cl, Br)6Guanidinium 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( R )- and ( S )-[C 8 H 10 NO 3 ] 2 [NbOF 5 ]: noncentrosymmetric niobium oxyfluorides with large optical anisotropy3[C 3 N 6 H 7 ] 2 [B 3 O 3 F 4 (OH)]: a new hybrid birefringent crystal with strong optical anisotropy induced by mixed functional units85A flexible functional module to regulate ultraviolet optical nonlinearity for achieving a balance between a second-harmonic generation response and birefringence43From 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 materials19Metal oxyhalides: an emerging family of nonlinear optical materials124NH 4 (B 6 PO 10 (OH) 4 )·H 2 O: exhibiting the largest birefringence in borophosphates43Performance of optical materials with the derivative of planar π-conjugated groups: Recent advances and future prospects37From Pb(H 2 C 3 N 3 O 3 )(OH) to Pb(H 2 C 3 N 3 O 3 )F: Homovalent Anion Substitution-Induced Band Gap Enlargement and Birefringence Enhancement26Potential optical functional crystals with large birefringence: Recent advances and future prospects322Synthesis of chiral boron imidazolate frameworks with second-order nonlinear optics12Finding the First Squarates Nonlinear Optical Crystal NaHC4O4·H2O with Strong Second Harmonic Generation and Giant Birefringence56Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)212Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2212A Hybrid Halide Perovskite Birefringent Crystal14A Hybrid Halide Perovskite Birefringent Crystal149Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Crystal Growth and Physical Properties of the Nonlinear Optical Crystal KLi(HC3N3O3)·2H2O15Noncentrosymmetric (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 Mercury34Directional Construction of New Nonlinear Optical Bifunctional Units through Molecular Engineering Design Inspired by the B 3 O 7 -Typed Configuration23[C(NH2)3]2Zn(CO3)2: A Guanidinium-Templated Ultraviolet Nonlinear Optical Material20An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals81An Optically Anisotropic Crystal with Large Birefringence Arising from Cooperative π Orbitals22Mixed-Anion-Oriented Design of LnMGa3S6O (Ln = La, Pr, and Nd; M = Ca and Sr) Nonlinear Optical Oxysulfides with Targeted Property Balance56A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses15A Hybrid Antiperovskite with Strong Linear and Second‐Order Nonlinear Optical Responses96C(NH2)3Rb(I3O8)(IO3)(I2O6H2): An unprecedented organic–inorganic hybrid polyiodate with two different polyiodate groups13KC9H5O6(H2O): A Promising UV Nonlinear-Optical Material with Large Birefringence Based on a π-Conjugated (C9H5O6)−Group11Dual-Ligand-Oriented Design of Noncentrosymmetric Complexes with Nonlinear-Optical Activity11Three polar indium phosphites exhibiting diverse structural networks and SHG-activity9ZrF2(IO3)2 and RbGaF3(IO3): Two Promising Birefringent Crystals Featuring 1D Metal-Fluoride Cationic Chains and Wide Bandgaps22Achieving 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 Birefringence18K 3 C 6 N 7 O 3 ·2H 2 O: A Multifunctional Nonlinear Optical Cyamelurate Crystal with Colossal π-Conjugated Orbitals44Explorations of Second-Order Nonlinear Optical Materials in the Monovalent Trithiocyanurate System18Na 2 (C 4 O 4 )(H 3 BO 3 )(H 2 O) 4 ·H 3 BO 3 : the first borate-squarate with strong SHG response obtained by superior synergy11(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 hybrid halide lead-free pseudo-perovskite with large birefringence37Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181Compounds consisting of coplanar π-conjugated B3O6-typed structures: An emerging source of ultraviolet nonlinear optical materials20Cs[B 3 O 3 F 2 (OH) 2 ]: discovery of a hydroxyfluorooxoborate guided by selective organic–inorganic transformation13Design and synthesis of anisotropic crystals with π -conjugated rings toward giant birefringence36Evaluating refractive index and birefringence of nonlinear optical crystals: Classical methods and new developments45From H 12 C 4 N 2 CdI 4 to H 11 C 4 N 2 CdI 3 : a highly polarizable CdNI 3 tetrahedron induced a sharp enhancement of second harmonic generation response and birefringence50Linear π-conjugated units of the D ∞h point group as superior ultraviolet birefringent units1Mg 2 Pb 2 Si 2 O 7 F 2 : a new lead-containing alkali earth metal silicate fluoride with a short cutoff edge2Ultrastable 3D cage-like metal–organic frameworks constructed using polydentate cyanurate ligands and their gas adsorption properties6Pb2Cl2(HPO3)(H2O) and Pb3Br2(HPO3)2: Two Phosphite Halides with 3D Structural Networks and Enlarged Birefringence18Toward Large Second-Harmonic Generation and Deep-UV Transparency in Strongly Electropositive Transition Metal Sulfates112α-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 –100A Second‐Order Nonlinear Optical Material Consisting of Two π‐Conjugated Groups10[C(NH2)2NHNO2][C(NH2)3](NO3)2: A Mixed Organic Cationic Hybrid Nitrate with an Unprecedented Nonlinear-Optical-Active Unit30

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  1. “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

    Dalton Transactions · 2019-01-01

    Jian Tang, Fei Liang, Xianghe Meng, Kaijin Kang, Tixian Zeng, Wenlong Yin, Mingjun Xia, Zheshuai Lin, Bin Kang

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  2. A rich structural chemistry in π-conjugated hydroisocyanurates: layered structures of A 2 B(H 2 C 3 N 3 O 3 ) 4 · n H 2 O (A = K, Rb, Cs; B = Mg, Ca; n = 4, 10) with high ultraviolet transparency and strong optical anisotropy

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  3. Co-crystal LiCl·(H 3 C 3 N 3 O 3 ): a promising solar-blind nonlinear optical crystal with giant nonlinearity from coplanar π-conjugated groups

    Chemical Communications · 2019-01-01

    Fei Liang, Naizheng Wang, Xiaomeng Liu, Zheshuai Lin, Yicheng Wu

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  4. CO(NH 2 ) 2 ·NH 4 Cl: an ultraviolet birefringent material with conjugated CO groups

    CrystEngComm · 2019-01-01

    Wang Ya, Jian Wei Han, Abudukadi Tudi, Zhizhong Zhang, Zhihua Yang, Shilie Pan

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  5. Intrinsic zero thermal expansion in cube cyanurate K 6 Cd 3 (C 3 N 3 O 3 ) 4

    Inorganic Chemistry Frontiers · 2019-01-01

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  6. LiO 4 tetrahedra lock the alignment of π-conjugated layers to maximize optical anisotropy in metal hydroisocyanurates

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  7. RE(H 2 C 3 N 3 O 3 ) 2 ·(OH)· x H 2 O (RE = La, Y and Gd): potential UV birefringent materials with strong optical anisotropy originating from the (H 2 C 3 N 3 O 3 ) − group

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    Xia Hao, Min Luo, Chensheng Lin, Donghong Lin, Liling Cao, Ning Ye

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  8. Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation

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  9. Cs3Na(H2C3N3O3)4·3H2O: A Mixed Alkali‐Metal Hydroisocyanurate Nonlinear Optical Material Containing π‐Conjugated Six‐Membered‐Ring Units

    European Journal of Inorganic Chemistry · 2019-04-08

    Xianghe Meng, Fei Liang, Jian Tang, Kaijin Kang, Qian Huang, Wenlong Yin, Zheshuai Lin, Mingjun Xia

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  10. Parallel Alignment of π-Conjugated Anions in Hydroisocyanurates Enhancing Optical Anisotropy

    Inorganic Chemistry · 2019-06-21

    Xianghe Meng, Fei Liang, Jian Tang, Kaijin Kang, Tixian Zeng, Wenlong Yin, Ruixin Guo, Zheshuai Lin, Mingjun Xia

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  11. Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups

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

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  13. How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates

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  14. Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin

    Angewandte Chemie International Edition · 2019-09-17

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  15. Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin

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  16. RbNa(HC 3 N 3 O 3 )·2H 2 O exhibiting a strong second harmonic generation response and large birefringence as a new potential UV nonlinear optical material

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  17. CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability

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  18. Crystal property and spectroscopic investigation on electro-optic and physico-chemical properties of NLO crystal; 3-(3,4-Dihydroxyphenyl)-L-Alanine

    Heliyon · 2019-12-01

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

    Dalton Transactions · 2019-12-11

    Xianghe Meng, Kaijin Kang, Fei Liang, Jian Tang, Zheshuai Lin, Wenlong Yin, Mingjun Xia

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

    ACS Omega · 2019-12-13

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  21. 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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  22. 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

    Crystal Growth & Design · 2019-12-27

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  23. 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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  24. Enhanced optical anisotropy via dimensional control in alkali-metal chalcogenides

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  25. Facile synthesis of cesium trithiocyanurate with high ionic conductivity and large birefringence properties

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  26. Gd(NO 3 )(Se 2 O 5 )·3H 2 O: a nitrate–selenite nonlinear optical material with a short ultraviolet cutoff edge

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  27. 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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  28. Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook

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  29. 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

    Chemical Communications · 2020-01-01

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