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RESEARCH PAPER · Journal of the American Chemical Society · 2013

Nonlinear Active Materials: An Illustration of Controllable Phase Matchability

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Nonlinear Active Materials: An Illustration of Controllable Phase MatchabilityOriginalFrom Solution to the Solid State: Control of Niobium Oxide–Fluoride [NbO x F y ] n − Species26Specific Chemistry of the Anions: [TaOF5]2–, [TaF6]−, and [TaF7]2–20Helical ∞1[Pb2O] Chains in Polymorphs of Pb2O(C6H5COO)211Revised Bismuth Chloroselenite System: Evidence of a Noncentrosymmmetric Structure with a Giant Unit Cell23Li2CdGeS4, A Diamond-Like Semiconductor with Strong Second-Order Optical Nonlinearity in the Infrared and Exceptional Laser Damage Threshold194Role of Acentric Displacements on the Crystal Structure and Second-Harmonic Generating Properties of RbPbCO3F and CsPbCO3F90Optical Nonlinearity in Cu2CdSnS4 and α/β-Cu2ZnSiS4: Diamond-like Semiconductors with High Laser-Damage Thresholds87Syntheses of Two Vanadium Oxide–Fluoride Materials That Differ in Phase Matchability46Enhanced Second Harmonic Generation from an Organic Self-Assembled Eutectic Binary Mixture: A Case Study with 3-Nitrobenzoic and 3,5-Dinitrobenzoic Acids23Predicting and Designing Optical Properties of Inorganic Materials72Polar Polymorphism: α-, β-, and γ-Pb2Ba4Zn4B14O31–Synthesis, Characterization, and Nonlinear Optical Properties79Hydrothermal crystal growth, piezoelectricity, and triboluminescence of KNaNbOF512A Nearly Ideal One-Dimensional S = 5/2 Antiferromagnet FeF3(4,4′-bpy) (4,4′-bpy =4,4′-bipyridyl) with Strong Intrachain Interactions51Low-Dimensional Hybrid Cuprous Halides Directed by Transition Metal Complex: Syntheses, Crystal Structures, and Photocatalytic Properties77Two Types of 2D Layered Iodoargentates Based on Trimeric [Ag3I7] Secondary Building Units and Hexameric [Ag6I12] Ternary Building Units: Syntheses, Crystal Structures, and Efficient Visible Light Responding Photocatalytic Properties109KPb 2 (PO 3 ) 5 : a novel nonlinear optical lead polyphosphate with a short deep-UV cutoff edge109A New Deep-Ultraviolet Transparent Orthophosphate LiCs 2 PO 4 with Large Second Harmonic Generation Response386BiFSeO 3 : An Excellent SHG Material Designed by Aliovalent Substitution207Investigation of nonlinear optical (NLO) properties by charge transfer contributions of amine functionalized tetraphenylethylene46Cd3(MoO4)(TeO3)2: A Polar 3D Compound Containing d10–d0 SCALP-Effect Cations85Infrared SHG Materials CsM3Se6 (M = Ga/Sn, In/Sn): Phase Matchability Controlled by Dipole Moment of the Asymmetric Building Unit102Recent achievements on middle and far-infrared second-order nonlinear optical materials434Atomic-scale observation of pressure-dependent reduction dynamics of W 18 O 49 nanowires using environmental TEM8Compositional phase diagram and microscopic mechanism of Ba 1−x Ca x Zr y Ti 1−y O 3 relaxor ferroelectrics30Crystal growth: an anisotropic mass transfer process at the interface38M 3 V 2 B 10 O 23 (M = Ca, Sr): two new vanadoborates with [V 2 B 10 O 23 ] ∞ double layers11A New Class of Lasing Materials: Intrinsic Stimulated Emission from Nonlinear Optically Active Metal–Organic Frameworks129A3Sr2P7O21 (A = Rb, Cs): Two Polyphosphates Based on Different Types of P–O Chains and Ring Structures36Li3VO4: A Promising Mid-Infrared Nonlinear Optical Material with Large Laser Damage Threshold51DFT-Based Comparative Study about the Influence of Fluorine and Hydroxyl Anions on Opto-Electric Properties of Borate Crystals: Choice for Better Anion13Preparation, structure and luminescent characterization of a series of metal–organic frameworks based on flexible ligands with nitrogen heterocycles and carboxyl6Mixed-Spin Diamond Chain Cu2FePO4F4(H2O)4 with a Noncollinear Spin Order and Possible Successive Phase Transitions18Synthesis of Ba0.6Sr0.4TiO3 platelet crystals based on Bi4Ti3O12 precursor by topochemical microcrystal conversion11Three Mixed-Alkaline Borates: Na2M2B20O32 (M = Rb, Cs) with Two Interpenetrating Three-Dimensional B-O Networks and Li4Cs4B40O64 with Fundamental Building Block B40O7730Concomitance, Reversibility, and Switching Ability of Centrosymmetric and Non-Centrosymmetric Crystal Forms: Polymorphism in an Organic Nonlinear Optical Material26Ion-induced structural and optical performance evolution in LBO-like crystals: experimental and theoretical investigation13PbFePO 4 F 2 with a 1/6th bond depleted triangular lattice7Surface-step-terrace tuned second-order nonlinear optical coefficients of epitaxial ferroelectric BaTiO 3 films17Functional Materials Design via Structural Regulation Originated from Ions Introduction: A Study Case in Cesium Iodate System91LiNa4B15O25: Featuring Unprecedented B15O30 Fundamental Building Block and Deep-UV Cutoff Edge20Structural Diversity from Anion Order in Heteroanionic Materials53CsFe3(SeO3)2F6 with S = 5/2 Cube Tile Lattice13MIMIIP3O9 (MI = Rb, MII = Cd, Mg, Ca; MI = Cs, MII = Pb, Sr; MI = K, MII = Mg): Cation Substitution Application in Cyclophosphate Family and Nonlinear Optical Properties35Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials197Second-order nonlinear optical crystals with mixed anions251Function of Tetrahedral ZnS3O Building Blocks in the Formation of SrZn2S2O: A Phase Matchable Polar Oxysulfide with a Large Second Harmonic Generation Response83The Rubidium Barium Borate Resulting from B7O15 Fundamental Building Block Exhibits DUV Cutoff Edge17BaB2S4: An Efficient and Air-Stable Thioborate as Infrared Nonlinear Optical Material with High Laser Damage Threshold86Two Lanthanide Borate Chlorides LnB4O6(OH)2Cl (Ln = La, Ce) with Wide Ultraviolet Transmission Windows and Large Second-Harmonic Generation Responses25Ba 4 (BS 3 S) 2 S 4 : a new thioborate with unprecedented [BS 3 -S] and [S 4 ] fundamental building blocks19Mn-Based tin sulfide Sr 3 MnSn 2 S 8 with a wide band gap and strong nonlinear optical response31SrCdSnQ 4 (Q = S and Se): infrared nonlinear optical chalcogenides with mixed NLO-active and synergetic distorted motifs68[Ge2S5(S2)]4−, A NLO‐Active Unit Leading to an Asymmetric Structure Discovered in Li2Cs4Ge2S5(S2)Cl2: An Experimental and Theoretical study18Variable Chains Found in Mixed Transition Metal Oxyfluorides with Heterocyclic Ligands9Prediction 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 Layers99Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO3/BO3F Ratio in Layers24Synthesis and characterization of a new quasi-one-dimensional antiferromagnet CoF2(H2O)2(pyrazine)19Ferroelectricity and antiferromagnetism in organic–inorganic hybrid (1,4-bis(imidazol-1-ylmethyl)benzene)CuCl 4 ·H 2 O12Enhanced optical anisotropy via dimensional control in alkali-metal chalcogenides19Synthesis, structure and characterization of three new Mg-containing phosphates with deep-UV cut-off edges9A Promising Fluorooxoborate Framework with Flexibile Capability for Diverse Cations to Enhance the Second Harmonic Generation14BaF 2 TeF 2 (OH) 2 : A UV Nonlinear Optical Fluorotellurite Material Designed by Band-Gap Engineering157Enhanced nonlinear optical functionality in birefringence and refractive index dispersion of the deep-ultraviolet fluorooxoborates123Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials131Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research19Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research139Role of Fluorooxo-Functional Units in Symmetry Breaking and Second Harmonic Generation Response Contribution in Fluorooxoborate Nonlinear Optical Crystals15Layered oxide B2S2O9 with a deep-ultraviolet band gap and a strong and robust second-harmonic generation33Synergism of multiple functional chromophores significantly enhancing the birefringence in layered non-centrosymmetric chalcohalides20A review on the recently developed promising infrared nonlinear optical materials105Ba 4 Ca(B 2 O 5 ) 2 F 2 : π-conjugation of B 2 O 5 in the planar pentagonal layer achieving large second harmonic generation of pyro -borate34A comprehensive survey on nonlinear optical phosphates: Role of multicoordinate groups106Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials25Fluorine‐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 matching31Constructing efficient HCSs/Nb 3 O 7 F hybrids based on bonding interaction to boost simulated-sunlight photocatalytic performance0CoMOF5(pyrazine)(H2O)2 (M = Nb, Ta): Two-Layered Cobalt Oxyfluoride Antiferromagnets with Spin Flop Transitions21Achieving 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] Units9Chemical substitution – oriented design of a new polar PbFIO3 achieving a balance between large second-harmonic generation response and wide band gap16Enhancement of band gap and birefringence induced via π -conjugated chromophore with “tail effect”29Complex coordinated functional groups: A great genes for nonlinear optical materials64First-principles study of opto-electronic and thermoelectric properties of SrCdSnX4 (X=S, Se, Te) alkali metal chalcogenides34Phase Matchability Transformation in the Infrared Nonlinear Optical Materials with Diamond‐Like Frameworks63Phase matching achieved by isomorphous substitution in IR nonlinear optical material Ba 2 SnSSi 2 O 7 with an undiscovered [SnO 4 S] functional motif47Structural phase transition and switchable dielectric behaviour of a one-dimensional chain niobium oxyfluoride2Review of Heteroleptic Tetrahedra as Birefringent or Nonlinear Optical Motifs17Novel layered heterobimetallic fluorides with large optical band gaps3Dual-Ligand-Oriented Design of Noncentrosymmetric Complexes with Nonlinear-Optical Activity11Structural modeling of oxygen-fluorine ordering in transition metal inorganic oxyfluorides0Cation and anion co-partial substitution induced centrosymmetric to noncentrosymmetric structural transformation to construct nonlinear-optical rare-earth oxythiogermanates13Dual-Anion Strategy Induces Dual Enhancement Toward Ultrashort Phase-Matching Wavelength in Deep-UV Transparent d0 Transition Metal Oxyfluorides22Construction of Ideal One-Dimensional Spin Chains by Topochemical Dehydration/Rehydration Route13Phase Matching of Infrared Nonlinear Optical Salt-Inclusion Chalcogenides Achieved by the Modulation of the Fractal Dimension of Anionic Motifs17Impact of substituents at the para position of C-Nitroso over N-Nitroso diphenylamine on static and frequency dependent nonlinear optical Properties: DFT and TD-DFT7Influence of substituent at the para position of tetraphenylethylene on static and dynamic nonlinear optical properties: In-silico approach1Single‐Step Synthesis of An Ideal Chain Antiferromagnet [H 2 (4,4′‐bipyridyl)](H 3 O) 2 Fe 2 F 10 with Spin S =5/20Single‐Step Synthesis of An Ideal Chain Antiferromagnet [H 2 (4,4′‐bipyridyl)](H 3 O) 2 Fe 2 F 10 with Spin S =5/26A2Cd(PO3)4 (A = K, Rb, Cs): Series of cadmium polyphosphates with infinite 1[(PO3)4]ꝏ chains and deep ultraviolet transparency windows2Synthesis, photophysical properties, and in-silico nonlinear optics of 3-hydroxy-N-phenyl-2-naphthamide and its acetate, acrylate, and benzoate derivative1Different magnitudes of second-order Jahn-Teller effect in isostructural NaMO2F2 (M = Nb, Ta) oxyfluorides4Achieving Phase‐Matching in Nonlinear Optical Materials CsM 2 In 2 S 6 (M = Cd/In, Hg/In) by the Incorporation of Unprecedented Trigonal Planar MS 3 Motifs6Accelerating Discovery of Infrared Nonlinear Optical Materials with High Lattice Thermal Conductivity: Combining Machine Learning and First‐Principles Calculations10Nonbonding 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 Properties25Crystal growth, tautomeric forms, dyeing, UV protection activity, and in-silico nonlinear optics of multifaceted 2-nitroso-1-naphthol0La3Ga5HfO14: Rare-Earth Polyhedron Coupled with Structural Protected Octahedron for Designing Nonlinear Optical Material with Wide Bandgap and Well-Balanced Properties5Exceptional Second Harmonic Generation in Ultraviolet Nonlinear Optical Oxyfluoroniobate Crystals via Structural Fingerprint Optimization of Polar Chains22Exceptional Second Harmonic Generation in Ultraviolet Nonlinear Optical Oxyfluoroniobate Crystals via Structural Fingerprint Optimization of Polar Chains8Three-In-One: A Guanidinium-Containing Niobium Oxyfluoride with a Perovskite-like Structure Revealing Multifunctional Optical Properties1La(SO3NH2)2NO3·H2O: synergistic anion engineering of the first rare-earth nitrate sulfamate defying transparency-birefringence-nonlinearity trade-offs in ultraviolet nonlinear optics8The Achievement of a Strong Second Harmonic Generation Response and a Large Birefringence in Sulfates4A S = 3/2 Quasi-One-Dimensional Antiferromagnet CrF 3 (4,4′-Bipyridyl) Exhibiting Strong Intrachain Interaction0

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  1. From Solution to the Solid State: Control of Niobium Oxide–Fluoride [NbO x F y ] n − Species

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  2. Specific Chemistry of the Anions: [TaOF5]2–, [TaF6]−, and [TaF7]2–

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  3. Helical ∞1[Pb2O] Chains in Polymorphs of Pb2O(C6H5COO)2

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    Clay C. Easterday, Liv R. Dedon, Mat­thias Zeller, Catherine M. Oertel

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  4. Revised Bismuth Chloroselenite System: Evidence of a Noncentrosymmmetric Structure with a Giant Unit Cell

    Crystal Growth & Design · 2014-04-23

    Almaz Aliev, Vadim M. Kovrugin, Marie Colmont, Christine Terryn, Marielle Huvé, Oleg I. Siidra, Sergey V. Krivovichev, Olivier Mentré

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  5. Li2CdGeS4, A Diamond-Like Semiconductor with Strong Second-Order Optical Nonlinearity in the Infrared and Exceptional Laser Damage Threshold

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  6. Role of Acentric Displacements on the Crystal Structure and Second-Harmonic Generating Properties of RbPbCO3F and CsPbCO3F

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  7. Optical Nonlinearity in Cu2CdSnS4 and α/β-Cu2ZnSiS4: Diamond-like Semiconductors with High Laser-Damage Thresholds

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  8. Syntheses of Two Vanadium Oxide–Fluoride Materials That Differ in Phase Matchability

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  9. Enhanced Second Harmonic Generation from an Organic Self-Assembled Eutectic Binary Mixture: A Case Study with 3-Nitrobenzoic and 3,5-Dinitrobenzoic Acids

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  11. Polar Polymorphism: α-, β-, and γ-Pb2Ba4Zn4B14O31–Synthesis, Characterization, and Nonlinear Optical Properties

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  12. Hydrothermal crystal growth, piezoelectricity, and triboluminescence of KNaNbOF5

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  13. A Nearly Ideal One-Dimensional S = 5/2 Antiferromagnet FeF3(4,4′-bpy) (4,4′-bpy =4,4′-bipyridyl) with Strong Intrachain Interactions

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  14. Low-Dimensional Hybrid Cuprous Halides Directed by Transition Metal Complex: Syntheses, Crystal Structures, and Photocatalytic Properties

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  15. Two Types of 2D Layered Iodoargentates Based on Trimeric [Ag3I7] Secondary Building Units and Hexameric [Ag6I12] Ternary Building Units: Syntheses, Crystal Structures, and Efficient Visible Light Responding Photocatalytic Properties

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  16. KPb 2 (PO 3 ) 5 : a novel nonlinear optical lead polyphosphate with a short deep-UV cutoff edge

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  17. A New Deep-Ultraviolet Transparent Orthophosphate LiCs 2 PO 4 with Large Second Harmonic Generation Response

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  18. BiFSeO 3 : An Excellent SHG Material Designed by Aliovalent Substitution

    Journal of the American Chemical Society · 2016-07-18

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  19. Investigation of nonlinear optical (NLO) properties by charge transfer contributions of amine functionalized tetraphenylethylene

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  20. Cd3(MoO4)(TeO3)2: A Polar 3D Compound Containing d10–d0 SCALP-Effect Cations

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  21. Infrared SHG Materials CsM3Se6 (M = Ga/Sn, In/Sn): Phase Matchability Controlled by Dipole Moment of the Asymmetric Building Unit

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  22. Recent achievements on middle and far-infrared second-order nonlinear optical materials

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  23. Atomic-scale observation of pressure-dependent reduction dynamics of W 18 O 49 nanowires using environmental TEM

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  24. Compositional phase diagram and microscopic mechanism of Ba 1−x Ca x Zr y Ti 1−y O 3 relaxor ferroelectrics

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  26. M 3 V 2 B 10 O 23 (M = Ca, Sr): two new vanadoborates with [V 2 B 10 O 23 ] ∞ double layers

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  27. A New Class of Lasing Materials: Intrinsic Stimulated Emission from Nonlinear Optically Active Metal–Organic Frameworks

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  28. A3Sr2P7O21 (A = Rb, Cs): Two Polyphosphates Based on Different Types of P–O Chains and Ring Structures

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  29. Li3VO4: A Promising Mid-Infrared Nonlinear Optical Material with Large Laser Damage Threshold

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  30. 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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  31. Preparation, structure and luminescent characterization of a series of metal–organic frameworks based on flexible ligands with nitrogen heterocycles and carboxyl

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  32. Mixed-Spin Diamond Chain Cu2FePO4F4(H2O)4 with a Noncollinear Spin Order and Possible Successive Phase Transitions

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  33. Synthesis of Ba0.6Sr0.4TiO3 platelet crystals based on Bi4Ti3O12 precursor by topochemical microcrystal conversion

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  34. 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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  35. Concomitance, Reversibility, and Switching Ability of Centrosymmetric and Non-Centrosymmetric Crystal Forms: Polymorphism in an Organic Nonlinear Optical Material

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  36. Ion-induced structural and optical performance evolution in LBO-like crystals: experimental and theoretical investigation

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  37. PbFePO 4 F 2 with a 1/6th bond depleted triangular lattice

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  38. Surface-step-terrace tuned second-order nonlinear optical coefficients of epitaxial ferroelectric BaTiO 3 films

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  39. Functional Materials Design via Structural Regulation Originated from Ions Introduction: A Study Case in Cesium Iodate System

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  40. LiNa4B15O25: Featuring Unprecedented B15O30 Fundamental Building Block and Deep-UV Cutoff Edge

    Inorganic Chemistry · 2018-02-14

    Yun Mo Yang, Qingrong Kong, Zhihua Yang, Shilie Pan

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  41. Structural Diversity from Anion Order in Heteroanionic Materials

    Chemistry of Materials · 2018-04-30

    Nenian Charles, Richard J. Saballos, James M. Rondinelli

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  42. CsFe3(SeO3)2F6 with S = 5/2 Cube Tile Lattice

    Inorganic Chemistry · 2018-05-09

    Hongcheng Lu, Hiroshi Kageyama

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  43. MIMIIP3O9 (MI = Rb, MII = Cd, Mg, Ca; MI = Cs, MII = Pb, Sr; MI = K, MII = Mg): Cation Substitution Application in Cyclophosphate Family and Nonlinear Optical Properties

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  44. Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials

    Journal of the American Chemical Society · 2018-07-27

    Bing‐Hua Lei, Zhihua Yang, Hongwei Yu, Chao Cao, Zhi Li, Cong Hu, Kenneth Reinhard Poeppelmeier, Shilie Pan

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  45. Second-order nonlinear optical crystals with mixed anions

    Coordination Chemistry Reviews · 2018-08-06

    Yu Pan, Sheng‐Ping Guo, Bin‐Wen Liu, Huaiguo Xue, Guo‐Cong Guo

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  46. Function of Tetrahedral ZnS3O Building Blocks in the Formation of SrZn2S2O: A Phase Matchable Polar Oxysulfide with a Large Second Harmonic Generation Response

    Chemistry of Materials · 2018-08-22

    Yoshihiro Tsujimoto, Christian A. Juillerat, Weiguo Zhang, Kotaro Fujii, Masatomo Yashima, P. Shiv Halasyamani, Hans‐Conrad zur Loye

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  47. The Rubidium Barium Borate Resulting from B7O15 Fundamental Building Block Exhibits DUV Cutoff Edge

    Inorganic Chemistry · 2018-10-12

    Yun Mo Yang, Xiaoyu Dong, Shilie Pan, Hongping Wu

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