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RESEARCH PAPER · Journal of the American Chemical Society · 2016

BiFSeO 3 : An Excellent SHG Material Designed by Aliovalent Substitution

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BiFSeO 3 : An Excellent SHG Material Designed by Aliovalent SubstitutionOriginalVariable dimensionality and framework found in a series of quaternary zinc selenites, A 2 Zn 3 (SeO 3 ) 4 · x H 2 O (A = Na, Rb, and Cs; 0≤ x ≤1) and Cs 2 Zn 2 (SeO 3 ) 3 ·2H 2 O7ChemInform Abstract: BiFSeO3: An Excellent SHG Material Designed by Aliovalent Substitution.0Nonlinear Optical Rod Indium-Imidazoledicarboxylate Framework as Room-Temperature Gas Sensor for Butanol Isomers29A new method for the preparation of a [Sn 2 (H 2 PO 2 ) 3 ]Br SHG-active polar crystal via surfactant-induced strategy12Ag 3 I[(MoO 3 ) 2 (IO 3 ) 2 ]: a new polar material synthesized from the structural modulation of molybdenyl iodate architectures by polarizable cation (Ag + ) and anion (I − )6Alkali earth MO x ( x = 6, 7, 9, 12) polyhedra tuned cadmium selenites with different dimensions and diverse SeO 3 2− coordinations1The activity of lone pair contributing to SHG response in bismuth borates: a combination investigation from experiment and DFT calculation28Bi(IO3)F2: The First Metal Iodate Fluoride with a Very Strong Second Harmonic Generation Effect238Bi(IO3)F2: The First Metal Iodate Fluoride with a Very Strong Second Harmonic Generation Effect71Syntheses, Crystal Structures, and Properties of Two Quaternary Selenite/Tellurite‐Nitrates with Formula of Bi(SeO 3 )(NO 3 ) and Bi 3 (μ 3 ‐OH)(TeO 3 ) 3 (NO 3 ) 216Chemistry-Inspired Adaptable Framework Structures368DFT-Based Comparative Study about the Influence of Fluorine and Hydroxyl Anions on Opto-Electric Properties of Borate Crystals: Choice for Better Anion13ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap140ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap36Pb0.65Mn2.85Ga3S8 and Pb0.72Mn2.84Ga2.95Se8: Two Quaternary Metal Chalcognides with Open-Tunnel-Framework Structures Displaying Intense Second Harmonic Generation Responses and Interesting Magnetic Properties17Li13Mn(SeO3)8: Lithium-Rich Transition Metal Selenite Containing Jahn–Teller Distortive Cations5Hg-Based Infrared Nonlinear Optical Material KHg4Ga5Se12 Exhibits Good Phase-Matchability and Exceptional Second Harmonic Generation Response101Mild Periodic Acid Flux and Hydrothermal Methods for the Synthesis of Crystalline f-Element-Bearing Iodate Compounds20Three Mixed-Alkaline Borates: Na2M2B20O32 (M = Rb, Cs) with Two Interpenetrating Three-Dimensional B-O Networks and Li4Cs4B40O64 with Fundamental Building Block B40O7730LiGaGe2S6: A Chalcogenide with Good Infrared Nonlinear Optical Performance and Low Melting Point56Li7(TeO3)3F: A Lithium Fluoride Tellurite with Large Second Harmonic Generation Responses and a Short Ultraviolet Cutoff Edge39From a Metastable Layer to a Stable Ring: A Kinetic Study for Transformation Reactions of Li2Mo3TeO12 to Polyoxometalates12A(VO 2 F)(SeO 3 ) (A = Sr, Ba) and Ba(MOF 2 )(TeO 4 ) (M = Mo, W): first examples of alkali-earth selenites/tellurites with a fluorinated d 0 -TM octahedron33A cation size effect on the framework structures in ABi 2 SeO 3 F 5 (A = K and Rb): first examples of alkali metal bismuth selenite fluorides14Design and synthesis of a nonlinear optical material BaAl 4 S 7 with a wide band gap inspired from SrB 4 O 763Pb 3 (SeO 3 )Br 4 : a new nonlinear optical material with enhanced SHG response designed via an ion-substitution strategy36Synthesis and characterization of a series of transition metal oxychlorides: MBi(SeO 3 ) 2 (H 2 O)Cl (M = Co, Ni, Cu)5Non-Centrosymmetric RbNaMgP 2 O 7 with Unprecedented Thermo-Induced Enhancement of Second Harmonic Generation239Li6M(SeO3)4 (M = Co, Ni, and Cd) and Li2Zn(SeO3)2: Selenites with Late Transition-Metal Cations32Computer-Assisted Design of a Superior Be 2 BO 3 F Deep-Ultraviolet Nonlinear-Optical Material41Anisotropy of nonlinear optical properties in monoclinic SmxY1-xCa4O(BO3)3 crystals12Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects211MIMIIP3O9 (MI = Rb, MII = Cd, Mg, Ca; MI = Cs, MII = Pb, Sr; MI = K, MII = Mg): Cation Substitution Application in Cyclophosphate Family and Nonlinear Optical Properties35Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Second-order nonlinear optical crystals with mixed anions250PbCdF(SeO 3 )(NO 3 ): A Nonlinear Optical Material Produced by Synergistic Effect of Four Functional Units52Ferroelectric Property, Switchable Dielectric, and Excellent Second Harmonic Generation Response in a Homochiral Organic Salt: l -Prolinammonium 1-Adamantane Carboxylate13Interrelationship «Composition - Structure - Property» for Acentric Selenite Crystals0Synthesis and structural variety of first Mn and Bi selenites and selenite chlorides7Ce(IO3)2F2⋅H2O: The First Rare‐Earth‐Metal Iodate Fluoride with Large Second Harmonic Generation Response66Pb 2 GaF 2 (SeO 3 ) 2 Cl: Band Engineering Strategy by Aliovalent Substitution for Enlarging Bandgap while Keeping Strong Second Harmonic Generation Response178Noncentrosymmetric cubic RbBSi2O6 polymorph with deep ultraviolet cut-off edge4Insights into the new 3d–5f heterometallic quaternary fluorides: Synthesis, crystal structures, spectroscopic properties, and thermodynamic stability3A 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 Anions23From centrosymmetric to noncentrosymmetric: cation-directed structural evolution in X 3 ZnB 5 O 10 (X = Na, K, Rb) and Cs 12 Zn 4 (B 5 O 10 ) 4 crystals26Hybridization-activated new deep ultraviolet transparent nonlinear optical material Ba 11 [Al(PO 4 ) 4 ](P 2 O 7 )(PO 4 ) 3 with balanced overall performance and parsimony-forbidden structure23LiMg(IO 3 ) 3 : an excellent SHG material designed by single-site aliovalent substitution68M 2 (SeO 3 )F 2 (M = Zn, Cd): understanding the structure directing effect of [SeO 3 ] 2− groups on constructing ordered oxyfluorides14Pb 2 Cd(SeO 3 ) 2 X 2 (X = Cl and Br): two halogenated selenites with phase matchable second harmonic generation27Pb 7 F 12 Cl 2 : a promising infrared nonlinear optical material with high laser damage threshold19Rational design of a new chalcogenide with good infrared nonlinear optical performance: SrZnSnS 452Rb 3 SbF 3 (NO 3 ) 3 : an excellent antimony nitrate nonlinear optical material with a strong second harmonic generation response fabricated by a rational multi-component design44RbSbSO 4 Cl 2 : an excellent sulfate nonlinear optical material generated due to the synergistic effect of three asymmetric chromophores79Exploration of New Birefringent Crystals in Bismuth d0 Transition Metal Selenites35Pb4B6O13: A Polar Lead Oxyborate with Uncommon ∞(B6O12)6– Layers Exhibiting a Large Second Harmonic Generation Response15Two Non-π-Conjugated Deep-UV Nonlinear Optical Sulfates268New cadmium-selenium-oxyhalides: Noncentrosymmetric Cd5(SeO3)4Cl2(H2O) and centrosymmetric Cd2(SeO3)F2, Cd2(SeO3)(OH)Br17Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)28KBiCl2SO4: The First Bismuth Chloride Sulfate Being Second-Order Nonlinear Optical Active44Mixed-Anion Inorganic Compounds: A Favorable Candidate for Infrared Nonlinear Optical Materials140New Members of SHG Active Dugganite Family, A3BC3D2O14 (A = Ba, Pb; B = Te, Sb; C = Al, Ga, Fe, Zn; D = Si, Ge, P, V): Synthesis, Structure, and Materials Properties30Two 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)33Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra73Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra18[NH4]12[(MoO2)2O(HPO4)2]4[PO4]Cl·0.5H2O: A mixed phosphomolybdate with nonlinear optical properties4Ag4Hg(SeO3)2(SeO4): a novel SHG material created in mixed valent selenium oxides by in situ synthesis36Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides63Transformation of Optical Anisotropy Origins in Perovskite-Related Materials: A First-Principles Study23K5(W3O9F4)(IO3): An Efficient Mid-Infrared Nonlinear Optical Compound with High Laser Damage Threshold114Mixed lone-pair and mixed anion compounds: Pb3(SeO3)(HSeO3)Br3, Pb3(SeO3)(OH)Br3, CdPb8(SeO3)4Cl4Br6 and RbBi(SeO3)F218[O 2 Pb 3 ] 2 (BO 3 )I: a new lead borate iodide with 1∞[O 2 Pb 3 ] double chains6Abnormal bandgap enlargement resulted in a promising mid-infrared nonlinear optical material Rb 2 CdBrI 3 with an ultrahigh laser damage threshold10Ba(B 2 OF 3 (OH) 2 ) 2 with well-ordered OH/F anions and a unique B 2 OF 3 (OH) 2 dimer30Evidence of reaction intermediates in microwave-assisted synthesis of SHG active α-La(IO 3 ) 3 nanocrystals4From BiF 3 to BiF 3 ·H 2 O: diverse Bi( iii ) coordination for structural transformation and birefringence regulation14From centrosymmetric to noncentrosymmetric: intriguing structure evolution in d 10 -transition metal iodate fluorides36Large optical polarizability causing positive effects on the birefringence of planar-triangular BO 3 groups in ternary borates18Novel ultraviolet (UV) nonlinear optical (NLO) materials discovered by chemical substitution-oriented design302Recent progress in selenite and tellurite based SHG materials32Selenite bromide nonlinear optical materials Pb 2 GaF 2 (SeO 3 ) 2 Br and Pb 2 NbO 2 (SeO 3 ) 2 Br: synthesis and characterization20The functionality of tetrahedral units in fluoroxoiodates: fluorine-modulating effects in iodates with lone pair electrons3Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework132CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework22BaF 2 TeF 2 (OH) 2 : A UV Nonlinear Optical Fluorotellurite Material Designed by Band-Gap Engineering157MII2M3IIIF3(Te6F2O16) (MII = Pb, Ba; MIII = Al, Ga): New mixed anionic tellurites with isolated Te6 coplanar rings23Rational Design of the Nonlinear Optical Response in a Tin Iodate Fluoride Sn(IO3)2F290Synthesis and Characterization of Two New Second Harmonic Generation Active Iodates: K3Sc(IO3)6 and KSc(IO3)3Cl9Lead 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 Substitution58Strong Second Harmonic Generation in a Tungsten Bronze Oxide by Enhancing Local Structural Distortion48Dimensionality–Band Gap–Third-Harmonic Generation Property Relationship in Novel Main-Group Metal Iodates37Aliovalent-substituted synthesis for a non-centrosymmetric phosphate with enhanced nonlinear-optical response5Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014BiGa(SeO3)3: A Phase Matchable SHG Material Achieved by Cation Substitution19A6Sb4F12(SO4)3 (A = Rb, Cs): Two Novel Antimony Fluoride Sulfates with Unique Crown-like Clusters50AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses63Bi 3 (SeO 3 ) 3 (Se 2 O 5 )F: A Polar Bismuth Selenite Fluoride with Polyhedra of Highly Distortive Lone Pair Cations and Strong Second-Harmonic Generation Response63Ba2[MoO3(OH)(IO3)2]IO3: A Promising SHG Material Featuring a Λ-Shaped Functional Motif Achieved by Universal Mono-Site Substitution50A 2 Bi 2 (SeO 3 ) 3 F 2 (A = K and Rb): Excellent Mid-Infrared Nonlinear Optical Materials with Both Strong SHG Responses and Large Band Gaps64Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties165Pb18O8Cl15I5: A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties29Ba(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 Response69KSnI 3 ⋅ H 2 O: A New Compound with One‐Dimensional SnI 3 Chains of Pyramidal SnI 5 Polyhedra2Simple New Method for the Preparation of La(IO3)3 Nanoparticles6Hydrogen-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)10AgBi(SO 4 )(IO 3 ) 2 : aliovalent substitution induces structure dimensional upgrade and second harmonic generation enhancement37Ba 2 [FeF 4 (IO 3 ) 2 ]IO 3 : a promising nonlinear optical material achieved by chemical-tailoring-induced structure evolution8Centrosymmetric RbSnF 2 NO 3 vs. noncentrosymmetric Rb 2 SbF 3 (NO 3 ) 254First chiral fluorinated lead vanadate selenite Pb 2 (V 2 O 4 F)(VO 2 )(SeO 3 ) 3 with five asymmetric motifs and large optical properties24M(B(SeO 3 ) 3 )H 2 O (M = Al, Ga): the first boroselenites with a unique sandwich like double-layer structure9Pb 2 TiFO(SeO 3 ) 2 Br: a new polar compound with the strongest second harmonic generation in the selenite bromide family29Role of fluorine on the structure and second-harmonic-generation property of inorganic selenites and tellurites23Unexpected aliovalent cation substitution between two NLO materials LiBa 3 Bi 6 (SeO 3 ) 7 F 11 and Ba 3 Bi 6.5 (SeO 3 ) 7 F 10.5 O 0.518M(NH 2 SO 3 ) 2 (M=Sr, Ba): Two Deep‐Ultraviolet Transparent Sulfamates Exhibiting Strong Second Harmonic Generation Responses and Moderate Birefringence142M(NH 2 SO 3 ) 2 (M=Sr, Ba): Two Deep‐Ultraviolet Transparent Sulfamates Exhibiting Strong Second Harmonic Generation Responses and Moderate Birefringence27A2(TeO)P2O7 (A = K, Rb, Cs): Three new tellurite-pyrophosphates with large birefringence17A Series of Pentanary Salt-Inclusion Chalcogenoborates Containing a B12Q12 (Q = S, Se) Cluster Exhibiting a Kleinman-Forbidden Frequency-Doubling Effect25Bi2[B2(SeO3)6]: A Metal Boroselenite with a Unique Zero-Dimensional [B2(SeO3)6]6– Anionic Group and Large Birefringence31A New Anhydrous Polar Rare-Earth Iodate Fluoride, Ce(IO3)2F2, Exhibiting a Large Second-Harmonic-Generation Effect and Improved Overall Performance35An Insightful Picture of Nonlinear Photonics in 2D Materials and their Applications: Recent Advances and Future Prospects78Tin Chloride Sulfates A3Sn2(SO4)3–xCl1+2x (A = K, Rb, Cs; x = 0, 1) as Multifunctional Optical Materials33High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies323Hydrogen‐Bond‐Driven Synergistically Enhanced Hyperpolarizability: Chiral Coordination Polymers with Nonpolar Structures Exhibiting Unusually Strong Second‐Harmonic Generation87Hydrogen‐Bond‐Driven Synergistically Enhanced Hyperpolarizability: Chiral Coordination Polymers with Nonpolar Structures Exhibiting Unusually Strong Second‐Harmonic Generation19Linear 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 Stereoactivity55Giant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo 2 O 8 F149Controllable Syntheses, Crystal Structure Evolution, and Photoluminescence of Polymorphic Zirconium Oxyfluorides6Chemical substitution – oriented design of a new polar PbFIO3 achieving a balance between large second-harmonic generation response and wide band gap16Halogen-Ion-Induced Structural Phase Transition Giving a Polymorph of HgBr2 with Balanced Nonlinear Optical Properties8Synthesis and Characterization of Novel Nanoparticles of Lithium Aluminum Iodate LiAl(IO3)4, and DFT Calculations of the Crystal Structure and Physical Properties6A Lanthanum Ammonium Sulfate Double Salt with a Strong SHG Response and Wide Deep‐UV Transparency15A Lanthanum Ammonium Sulfate Double Salt with a Strong SHG Response and Wide Deep‐UV Transparency96Hg 2 (SeO 3 )(SO 4 ): the first sulfate selenite with large birefringence explored from d 10 transition metal compounds36Metal oxyhalides: an emerging family of nonlinear optical materials124HgSO4: An excellent mid-infrared sulfate nonlinear optical crystal with wide band gap and strong second harmonic generation response19First-principles study of the influence of lone pair electrons and molecular groups on the birefringence of phosphate and fluorophosphate13Flux synthesis, crystal structure, and characterization of a gamma-vanadate selenite polymorph1Na 3 Ti 3 O 3 (SeO 3 ) 4 F: A Phase-Matchable Nonlinear-Optical Crystal with Enlarged Second-Harmonic-Generation Intensity and Band Gap20Novel compounds Bi2Ni(SeO3)4 and Bi2Ni(SeO3)4·2H2O with cubic-like magnetic lattice and intriguing magnetic behavior0Rb5Ba2(B10O17)2(BO2): The formation of unusual functional [BO2]− in borates with deep-ultraviolet transmission window62K3ZrF4(SbF4)(SbF5) and K8(ZrF6)(Sb2Zr2F20): Two Zirconium Fluoroantimonites with Low Dimensional Structures and Wide Transparency Range12Cs2Bi2OSi2O7: A Promising Bismuth Silicate Nonlinear Optical Crystal with Face-Sharing BiO5 Polyhedra Exhibiting Strengthened Second Harmonic Generation Response and Birefringence43Second-Harmonic Generation-Positive Na 2 Ga 2 SiS 6 with a Broad Band Gap and a High Laser Damage Threshold14SrAgAsS4: A Noncentrosymmetric Sulfide with Good Infrared Nonlinear Optical Performance Induced by Aliovalent Substitution from Centrosymmetric SrGa2S412PbBi(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 Properties57Enhancements of Second Harmonic Generation and Birefringence in Traditional RbTiOPO4‐Type Crystals by Aliovalent Substitution of Ti Site1Syntheses, structures, and optical properties of n = 3 layered Dion–Jacobson perovskites, RbEu2-Bi Ti2NbO10 (0 ≤ x ≤ 2)1

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  1. Variable dimensionality and framework found in a series of quaternary zinc selenites, A 2 Zn 3 (SeO 3 ) 4 · x H 2 O (A = Na, Rb, and Cs; 0≤ x ≤1) and Cs 2 Zn 2 (SeO 3 ) 3 ·2H 2 O

    Journal of Solid State Chemistry · 2016-10-07

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  2. ChemInform Abstract: BiFSeO3: An Excellent SHG Material Designed by Aliovalent Substitution.

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    Mingli Liang, Chun‐Li Hu, Fang Kong, Jiang‐Gao Mao

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  3. Nonlinear Optical Rod Indium-Imidazoledicarboxylate Framework as Room-Temperature Gas Sensor for Butanol Isomers

    Crystal Growth & Design · 2016-12-17

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  4. A new method for the preparation of a [Sn 2 (H 2 PO 2 ) 3 ]Br SHG-active polar crystal via surfactant-induced strategy

    Dalton Transactions · 2017-01-01

    Jie‐Ling Xie, Yu-Hua Zhou, Long-Hua Li, Jian‐Han Zhang, Jun‐Ling Song

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  5. Ag 3 I[(MoO 3 ) 2 (IO 3 ) 2 ]: a new polar material synthesized from the structural modulation of molybdenyl iodate architectures by polarizable cation (Ag + ) and anion (I − )

    Dalton Transactions · 2017-01-01

    Chang‐Yu Meng, Pei Zhang, Rongfang Wang, Lei Geng

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  6. Alkali earth MO x ( x = 6, 7, 9, 12) polyhedra tuned cadmium selenites with different dimensions and diverse SeO 3 2− coordinations

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  7. The activity of lone pair contributing to SHG response in bismuth borates: a combination investigation from experiment and DFT calculation

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  8. Bi(IO3)F2: The First Metal Iodate Fluoride with a Very Strong Second Harmonic Generation Effect

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  9. Bi(IO3)F2: The First Metal Iodate Fluoride with a Very Strong Second Harmonic Generation Effect

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  10. Syntheses, Crystal Structures, and Properties of Two Quaternary Selenite/Tellurite‐Nitrates with Formula of Bi(SeO 3 )(NO 3 ) and Bi 3 (μ 3 ‐OH)(TeO 3 ) 3 (NO 3 ) 2

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  11. Chemistry-Inspired Adaptable Framework Structures

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  12. DFT-Based Comparative Study about the Influence of Fluorine and Hydroxyl Anions on Opto-Electric Properties of Borate Crystals: Choice for Better Anion

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  13. ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap

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  14. ABi2(IO3)2F5 (A=K, Rb, and Cs): A Combination of Halide and Oxide Anionic Units To Create a Large Second‐Harmonic Generation Response with a Wide Bandgap

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  15. Pb0.65Mn2.85Ga3S8 and Pb0.72Mn2.84Ga2.95Se8: Two Quaternary Metal Chalcognides with Open-Tunnel-Framework Structures Displaying Intense Second Harmonic Generation Responses and Interesting Magnetic Properties

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  16. Li13Mn(SeO3)8: Lithium-Rich Transition Metal Selenite Containing Jahn–Teller Distortive Cations

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  17. Hg-Based Infrared Nonlinear Optical Material KHg4Ga5Se12 Exhibits Good Phase-Matchability and Exceptional Second Harmonic Generation Response

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  18. Mild Periodic Acid Flux and Hydrothermal Methods for the Synthesis of Crystalline f-Element-Bearing Iodate Compounds

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  19. Three Mixed-Alkaline Borates: Na2M2B20O32 (M = Rb, Cs) with Two Interpenetrating Three-Dimensional B-O Networks and Li4Cs4B40O64 with Fundamental Building Block B40O77

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  20. LiGaGe2S6: A Chalcogenide with Good Infrared Nonlinear Optical Performance and Low Melting Point

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  21. Li7(TeO3)3F: A Lithium Fluoride Tellurite with Large Second Harmonic Generation Responses and a Short Ultraviolet Cutoff Edge

    Inorganic Chemistry · 2017-11-13

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  22. From a Metastable Layer to a Stable Ring: A Kinetic Study for Transformation Reactions of Li2Mo3TeO12 to Polyoxometalates

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  23. A(VO 2 F)(SeO 3 ) (A = Sr, Ba) and Ba(MOF 2 )(TeO 4 ) (M = Mo, W): first examples of alkali-earth selenites/tellurites with a fluorinated d 0 -TM octahedron

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  24. A cation size effect on the framework structures in ABi 2 SeO 3 F 5 (A = K and Rb): first examples of alkali metal bismuth selenite fluorides

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  25. Design and synthesis of a nonlinear optical material BaAl 4 S 7 with a wide band gap inspired from SrB 4 O 7

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  26. Pb 3 (SeO 3 )Br 4 : a new nonlinear optical material with enhanced SHG response designed via an ion-substitution strategy

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  27. Synthesis and characterization of a series of transition metal oxychlorides: MBi(SeO 3 ) 2 (H 2 O)Cl (M = Co, Ni, Cu)

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  41. Pb 2 GaF 2 (SeO 3 ) 2 Cl: Band Engineering Strategy by Aliovalent Substitution for Enlarging Bandgap while Keeping Strong Second Harmonic Generation Response

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  42. Noncentrosymmetric cubic RbBSi2O6 polymorph with deep ultraviolet cut-off edge

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

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