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RESEARCH PAPER · Chemistry of Materials · 1998

Noncentrosymmetric Oxides

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Noncentrosymmetric OxidesOriginalPreparation of a Chiral, 2-Dimensional Network Containing Metallacrown and Copper Benzoate Building Blocks111Naturally Chiral Metal Surfaces as Enantiospecific Adsorbents219Synthesis and Characterization of Te2SeO7: A Powder Second-Harmonic-Generating Study of TeO2, Te2SeO7, Te2O5, and TeSeO4212Structural Modulation of Molybdenyl Iodate Architectures by Alkali Metal Cations in AMoO3(IO3) (A = K, Rb, Cs): A Facile Route to New Polar Materials with Large SHG Responses336New One-Dimensional Vanadyl Iodates: Hydrothermal Preparation, Structures, and NLO Properties of A[VO2(IO3)2] (A = K, Rb) and A[(VO)2(IO3)3O2] (A = NH4, Rb, Cs)161Synthesis, Structure, and Characterization of a New Second-Harmonic-Generating Tellurite: Na2TeW2O9221A Stoichiometric Model for Sillenites109Out-of-Center Distortions in d0 Transition Metal Oxide Fluoride Anions124Hydrothermal Preparation, Structures, and NLO Properties of the Rare Earth Molybdenyl Iodates, RE(MoO2)(IO3)4(OH) [RE = Nd, Sm, Eu]113Syntheses, structures, and second-harmonic generating properties in new quaternary tellurites: A2TeW3O12 (A=K, Rb, or Cs)124Alignment of acentric MoO3F33− anions in a polar material: (Ag3MoO3F3)(Ag3MoO4)Cl440Chiral selection on inorganic crystalline surfaces490X-ray powder diffraction results for the phase transitions in Sr2MWO6(M Ni, Zn, Co, Cu) double perovskite oxides100Characterization of the Structural, Optical, and Dielectric Properties of Oxynitride Perovskites AMO 2 N (A = Ba, Sr, Ca; M = Ta, Nb)441Theoretical Prediction of New High-Performance Lead-Free Piezoelectrics361A Second-Order Nonlinear Optical Material Prepared through In Situ Hydrothermal Ligand Synthesis156Bulk characterization methods for non-centrosymmetric materials: second-harmonic generation, piezoelectricity, pyroelectricity, and ferroelectricity931Organically-templated metal sulfates, selenites and selenates195Na2Te3Mo3O16: A New Molybdenum Tellurite with Second-Harmonic Generating and Pyroelectric Properties232Synthesis, Crystal Structure, and Nonlinear Optical Properties of Li6CuB4O10: a Congruently Melting Compound with Isolated [CuB4O10]6- Units222Correlations between transition temperature, tolerance factor and cohesive energy in 2+:4+ perovskites93Structure and Bonding in SnWO4, PbWO4, and BiVO4: Lone Pairs vs Inert Pairs310Two New Noncentrosymmetric Polar Oxides: Synthesis, Characterization, Second-Harmonic Generating, and Pyroelectric Measurements on TlSeVO5 and TlTeVO5115Bulk Growth and Characterization of a Novel Nonlinear Optical Crystal BaTeMo2O9125Explorations of New Types of Second‐Order Nonlinear Optical Materials in Cd(Zn)‐VV‐TeIV‐O Systems109A Polar Oxide ZnSnO3 with a LiNbO3-Type Structure300A Novel Metal−Organic Network with High Thermal Stability: Nonlinear Optical and Photoluminescent Properties111Isotope Effect on SHG Response and Ferroelectric Properties of a Homochiral Zinc Coordination Compound Containing Tetrazole Ligand98Structures and Properties of Functional Metal Selenites and Tellurites164Crystal structure and multiferroic properties of Gd-substituted BiFeO3188Flexible Polar Nanowires of Cs5BiP4Se12 from Weak Interactions between Coordination Complexes: Strong Nonlinear Optical Second Harmonic Generation102Alignment of Lone Pairs in a New Polar Material: Synthesis, Characterization, and Functional Properties of Li2Ti(IO3)6307Polar or Nonpolar? A+ Cation Polarity Control in A2Ti(IO3)6(A = Li, Na, K, Rb, Cs, Tl)307Growth, Structure, and Optical Properties of a Congruent Melting Oxyborate, Bi2ZnOB2O6112BaNbO(IO3)5: A New Polar Material with a Very Large SHG Response331Review: environmental friendly lead-free piezoelectric materials1074A Series of New Infrared NLO Semiconductors, ZnY6Si2S14, AlxDy3(SiyAl1−y)S7, and Al0.33Sm3SiS7134Developing chiral surfaces for enantioselective chemical processing93Noncentrosymmetric Polar Oxide Material, Pb3SeO5: Synthesis, Characterization, Electronic Structure Calculations, and Structure−Property Relationships148Cation Coordination Control of Anionic Group Alignment to Maximize SHG Effects in the BaMBO3F (M = Zn, Mg) Series128New Noncentrosymmetric Tellurite Phosphate Material: Synthesis, Characterization, and Calculations of Te2O(PO4)295Novel Bismuth and Lead Coordination Polymers Synthesized with Pyridine-2,5-Dicarboxylates: Two Single Component “White” Light Emitting Phosphors146A congruently melting and deep UV nonlinear optical material: Li3Cs2B5O10104Bulk crystal growth and characterization of a new polar polymorph of BaTeMo2O9: α-BaTeMo2O998The fruitful introduction of chirality and control of absolute configurations in molecular magnets311Inorganic Supramolecular Compounds with 3-D Chiral Frameworks Show Potential as Both Mid-IR Second-Order Nonlinear Optical and Piezoelectric Materials132Explorations of New Second-Order Nonlinear Optical Materials in the Potassium Vanadyl Iodate System267K3B6O10Cl: A New Structure Analogous to Perovskite with a Large Second Harmonic Generation Response and Deep UV Absorption Edge673Syntheses and Characterization of New Mid-Infrared Transparency Compounds: Centric Ba2BiGaS5 and Acentric Ba2BiInS595Effect of A site and B site doping on structural, thermal, and dielectric properties of BiFeO3 ceramics183Na2CsBe6B5O15: An Alkaline Beryllium Borate as a Deep-UV Nonlinear Optical Crystal318BiO(IO3): A New Polar Iodate that Exhibits an Aurivillius-Type (Bi2O2)2+ Layer and a Large SHG Response507Polymorphism of BaTeMo 2 O 9 : A New Polar Polymorph and the Phase Transformation186Alkaline-Alkaline Earth Fluoride Carbonate Crystals ABCO3F (A = K, Rb, Cs; B = Ca, Sr, Ba) as Nonlinear Optical Materials526Rational Synthesis of Noncentrosymmetric Metal–Organic Frameworks for Second-Order Nonlinear Optics1005Molecular Engineering Design to Resolve the Layering Habit and Polymorphism Problems in Deep UV NLO Crystals: New Structures in MM′Be2B2O6F (M═Na, M′═Ca; M═ K, M′═Ca, Sr)198Chiral biointerface materials220A new congruent-melting oxyborate, Pb 4 O(BO 3 ) 2 with optimally aligned BO 3 triangles adopting layered-type arrangement113A novel deep UV nonlinear optical crystal Ba3B6O11F2, with a new fundamental building block, B6O14 group180MgTeMoO6: A neutral layered material showing strong second-harmonic generation110Strong Kleinman-Forbidden Second Harmonic Generation in Chiral Sulfide: La 4 InSbS 9167UV Nonlinear Optical Crystal Ba2[B6O9(OH)4] Featuring Unique Chiral Layers with a New B18O42 Circle Based on BO3 and BO4 Units97Control of octahedral connectivity in perovskite oxide heterostructures: An emerging route to multifunctional materials discovery445Disconnection Enhances the Second Harmonic Generation Response: Synthesis and Characterization of Ba23Ga8Sb2S38249Lead-Free Nanogenerator Made from Single ZnSnO3 Microbelt140Polar octahedral rotations: A path to new multifunctional materials253Applications of metal–organic coordination polymers as precursors for preparation of nano-materials384Cs2B4SiO9: A Deep‐Ultraviolet Nonlinear Optical Crystal278Cs2B4SiO9: A Deep‐Ultraviolet Nonlinear Optical Crystal224Designing a Deep-Ultraviolet Nonlinear Optical Material with a Large Second Harmonic Generation Response598New Metal Chalcogenides Ba4CuGa5Q12 (Q = S, Se) Displaying Strong Infrared Nonlinear Optical Response117Metal Chalcogenides: A Rich Source of Nonlinear Optical Materials683CsPbCO3F: A Strong Second-Harmonic Generation Material Derived from Enhancement via p−π Interaction271High-Pressure Synthesis, Crystal Structure, and Phase Stability Relations of a LiNbO 3 -Type Polar Titanate ZnTiO 3 and Its Reinforced Polarity by the Second-Order Jahn–Teller Effect153Cs 3 Zn 6 B 9 O 21 : A Chemically Benign Member of the KBBF Family Exhibiting the Largest Second Harmonic Generation Response360A New UV Nonlinear Optical Material CsZn2B3O7: ZnO4 Tetrahedra Double the Efficiency of Second-Harmonic Generation121Designing a robustly metallic noncenstrosymmetric ruthenate oxide with large thermopower anisotropy174Origin of Ferroelectricity in a Family of Polar Oxides: The Dion—Jacobson Phases113Rb2CdBr2I2: A New IR Nonlinear Optical Material with a Large Laser Damage Threshold154Deep-Ultraviolet Transparent Phosphates RbBa 2 (PO 3 ) 5 and Rb 2 Ba 3 (P 2 O 7 ) 2 Show Nonlinear Optical Activity from Condensation of [PO 4 ] 3– Units355EXAFS and XANES analysis of oxides at the nanoscale255Na3Ba2(B3O6)2F: Next Generation of Deep-Ultraviolet Birefringent Materials190Sr 2 (OH) 3 NO 3 : the first nitrate as a deep UV nonlinear optical material with large SHG responses166Understanding ferroelectricity in layered perovskites: new ideas and insights from theory and experiments293Recent advances on second-order NLO materials based on metal iodates328Beryllium-Free Rb3Al3B3O10F with Reinforced Interlayer Bonding as a Deep-Ultraviolet Nonlinear Optical Crystal270Study of ZnSnO3-Nanowire Piezophotocatalyst Using Two-Step Hydrothermal Synthesis99Pb17O8Cl18: A Promising IR Nonlinear Optical Material with Large Laser Damage Threshold Synthesized in an Open System223Pb2Ba3(BO3)3Cl: A Material with Large SHG Enhancement Activated by Pb-Chelated BO3 Groups279RbMgCO3F: A New Beryllium-Free Deep-Ultraviolet Nonlinear Optical Material342Design and Synthesis of the Beryllium‐Free Deep‐Ultraviolet Nonlinear Optical Material Ba3(ZnB5O10)PO4302Oxychalcogenide BaGeOSe2: Highly Distorted Mixed-Anion Building Units Leading to a Large Second-Harmonic Generation Response96‘Ferroelectric’ metals reexamined: fundamental mechanisms and design considerations for new materials164BaCdSnS 4 and Ba 3 CdSn 2 S 8 : syntheses, structures, and non-linear optical and photoluminescence properties98KPb 2 (PO 3 ) 5 : a novel nonlinear optical lead polyphosphate with a short deep-UV cutoff edge109Electronic, Crystal Chemistry, and Nonlinear Optical Property Relationships in the Dugganite A3B3CD2O14 Family147Magnetic materials based on 3d metal phosphonates130Deep-Ultraviolet Transparent Cs 2 LiPO 4 Exhibits an Unprecedented Second Harmonic Generation162“All-Three-in-One”: A New Bismuth–Tellurium–Borate Bi3TeBO9 Exhibiting Strong Second Harmonic Generation Response223Toward the Rational Design of Novel Noncentrosymmetric Materials: Factors Influencing the Framework Structures601LiRb 2 PO 4 : a new deep-ultraviolet nonlinear optical phosphate with a large SHG response95Cooperation of Three Chromophores Generates the Water‐Resistant Nitrate Nonlinear Optical Material Bi3TeO6OH(NO3)2113Phase-referenced nonlinear spectroscopy of the α-quartz/water interface179Mixed-Metal Carbonate Fluorides as Deep-Ultraviolet Nonlinear Optical Materials258Chirality in adsorption on solid surfaces171Enhancing optical anisotropy of crystals by optimizing bonding electron distribution in anionic groups237Bi3OF3(IO3)4: Metal Oxyiodate Fluoride Featuring a Carbon-Nanotube-like Topological Structure with Large Second Harmonic Generation Response120A brief review on perovskite multiferroics147M4Mg4(P2O7)3 (M = K, Rb): Structural Engineering of Pyrophosphates for Nonlinear Optical Applications240Beryllium‐Free β‐Rb2Al2B2O7 as a Possible Deep‐Ultraviolet Nonlinear Optical Material Replacement for KBe2BO3F2185Learning from data to design functional materials without inversion symmetry95Mid-Infrared Nonlinear Optical Materials Based on Metal Chalcogenides: Structure–Property Relationship342Chemistry-Inspired Adaptable Framework Structures368ABi2(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 Bandgap140Cs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response129Rb 3 VO(O 2 ) 2 CO 3 : A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response206Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Rational Design of a LiNbO3-like Nonlinear Optical Crystal, Li2ZrTeO6, with High Laser-Damage Threshold and Wide Mid-IR Transparency Window152A Niobium Oxyiodate Sulfate with a Strong Second‐Harmonic‐Generation Response Built by Rational Multi‐Component Design114Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO 3 /BO 3 F Ratio in Layers99A room-temperature ferroelectric semimetal331Creating visible-to-near-infrared mechanoluminescence in mixed-anion compounds SrZn2S2O and SrZnSO146Chiral Surface and Geometry of Metal Nanocrystals149Structure-property relationship in nonlinear optical materials with π-conjugated CO3 triangles145CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework132BaF 2 TeF 2 (OH) 2 : A UV Nonlinear Optical Fluorotellurite Material Designed by Band-Gap Engineering157Chiral-perovskite optoelectronics907Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra148Bond-length distributions for ions bonded to oxygen: results for the transition metals and quantification of the factors underlying bond-length variation in inorganic solids127CsZn2BO3X2 (X2=F2, Cl2, and FCl): A Series of Beryllium‐Free Deep‐Ultraviolet Nonlinear‐Optical Crystals with Excellent Properties142K 2 Sb(P 2 O 7 )F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance297A 3 BBi(P 2 O 7 ) 2 (A = Rb, Cs; B = Pb, Ba): Isovalent Cation Substitution to Sustain Large Second-Harmonic Generation Responses106Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )213Borates: A Rich Source for Optical Materials1097Chiral Photocurrent in Parity-Violating Magnet and Enhanced Response in Topological Antiferromagnet129Chiral Photocurrent in Parity-Violating Magnet and Enhanced Response in Topological Antiferromagnet158Conduction Band Control of Oxyhalides with a Triple-Fluorite Layer for Visible Light Photocatalysis109UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate194Metal oxyhalides: an emerging family of nonlinear optical materials125High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence198Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2215Semiconducting piezoelectric heterostructures for piezo- and piezophotocatalysis231Chiral carbon dots: synthesis, optical properties, and emerging applications284Chirality in the Solid State: Chiral Crystal Structures in Chiral and Achiral Space Groups121Chiral Mesostructured Inorganic Materials with Optical Chiral Response111Local Polarity-Induced Assembly of Second-Order Nonlinear Optical Materials129Chiral metal–organic frameworks for photonics136NaRb 6 (B 4 O 5 (OH) 4 ) 3 (BO 2 ) Featuring Noncentrosymmetry, Chirality, and the Linear Anionic Group BO 2 –101Novel oxygen vacancy-rich Bi2MoO6-SOVs/MgFe2O4 S-scheme heterojunction piezo-photocatalytic for efficient degradation of norfloxacin and theoretical calculations103Unearthing Superior Inorganic UV Second‐Order Nonlinear Optical Materials: A Mineral‐Inspired Method Integrating First‐Principles High‐Throughput Screening and Crystal Engineering124

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