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RESEARCH PAPER · Chemical Science · 2019

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

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CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stabilityOriginalEmergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Helix-constructed polar rare-earth iodate fluoride as a laser nonlinear optical multifunctional material25Second-order nonlinear optical materials with a benzene-like conjugated π system49K2Na(IO3)2(I3O8) with Strong Second Harmonic Generation Response Activated by Two Types of Isolated Iodate Anions46Volume Modulation of Nonlinear Optical Properties by Cation Substitution8Li4Ca2B8O16: A Borate with a Unique Fundamental Building Block and a Short Cutoff Edge14New Alkaline-Earth Metal Fluoroiodates Exhibiting Large Birefringence and Short Ultraviolet Cutoff Edge with Highly Polarizable (IO 3 F) 2– Units63Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials137Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials29LiGaF2(IO3)2: A mixed-metal gallium iodate-fluoride with large birefringence and wide band gap39NaZnCO 3 (OH): A High-Performance Carbonate Ultraviolet Nonlinear Optical Crystal Derived from KBe 2 BO 3 F 2194Cs 2 AlB 5 O 10 : a short-wavelength nonlinear optical crystal with moderate second harmonic generation response12A new rare-earth borate birefringent crystal with quasi-two-dimensional [BO 3 ] layers23Ba 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 -borate34BaZn 3 (BO 3 ) 2 F 2 : a new beryllium-free zincoborate with a KBBF-type structure11Co-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 birefringence13Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41From centrosymmetric to noncentrosymmetric: effect of the cation on the crystal structures and birefringence values of (NH 4 ) n−2 AE(PO 2 F 2 ) n (AE = Mg, Sr and Ba; n = 2, 3 and 4)9From thiophosphate to chalcohalide: mixed-anion AgS x Cl y ligands concurrently enhancing nonlinear optical effects and laser-damage threshold10Li 5 Cs(SO 4 ) 3 : a potential zero-order wave plate material with short deep-ultraviolet cutoff edge20M 6 PS 5 X (M = Ag, Cu; X = Cl, Br) chalcohalides exhibiting strong nonlinear optical responses and high laser damage resistances9NaGaI 3 O 9 F: a new alkali metal gallium iodate combined with IO 3 − and IO 3 F 2− units16Recent advances of oxyfluorides for nonlinear optical applications69π‑Conjugated Trigonal Planar [C(NH2)3]+ Cationic Group: A Superior Functional Unit for Ultraviolet Nonlinear Optical Materials52Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137Designing a Family of Aluminum-Containing Fluoroborate Crystals with Enhanced Birefringence and Second-Harmonic Generation Coefficients Based on the First-Principles Methods4K5Mg2La3(BO3)6: An Efficient, Deep-Ultraviolet Nonlinear Optical Material70Polymorphic donor–acceptor substituted chalcone: structural, spectral, dielectric and nonlinear optical properties for optical limiting applications1Exploring Deep-UV Nonlinear Optical Materials with Enhanced Second Harmonic Generation Response and Birefringence in Fluoroaluminoborate Crystals69SrAlB3O6F2: A Fluoroaluminoborate with [Al2B6O14F4] Units and Large Birefringence22Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials28NaRbB3O4F3: A New Fluorooxoborate with a Short UV Cutoff Edge Enriching the Structural Chemistry of Borate7A 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**27Finding a Series of BaBOF3 Fluorooxoborate Polymorphs with Tunable Symmetries: A Simple but Flexible Case37Identical in Formula but Not Isotypic in Configuration: Discovery of a New Highly Polymerized [B12O24] Cluster in Cs3AlB6O1212Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification89Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification9Polymorphic Pb14O8I12 and Pb7O4I6 oxyhalides featuring unprecedented [O8Pb14] clusters with broad IR transparency20Synergistic Effect of π-Conjugated [C(NH 2 ) 3 ] Cation and Sb(III) Lone Pair Stereoactivity on Structural Transformation and Second Harmonic Generation58From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra10AAl3P6O20 (A = Rb, Cs): Two deep-ultraviolet transparent nonlinear optical materials designed by aliovalent substitution11Complex coordinated functional groups: A great genes for nonlinear optical materials64K6(IO6H4)(HI2O6)(HIO3)2(IO3)4·2H2O: A Case of Iodate with Coexisting [I5+O3] and [I7+O6] Units6Flux Growth and Properties of Volatile Bromine-Containing UV Nonlinear Optical Crystal K3B6O10Br3AAg 2 PS 4 (A = K, Na/K): the first-type of noncentrosymmetric alkali metal Ag-based thiophosphates exhibiting excellent second-order nonlinear optical performances21Band gap modulation and nonlinear optical properties of quaternary tellurates Li 2 GeTeO 613Cd 4 REO(BO 3 ) 3 (RE = Sm, Eu, Tb): three new cadmium–rare earth oxyborates with both good NLO and luminescence properties6Cs 2 VOF 4 (IO 2 F 2 ): Rationally designing a noncentrosymmetric early-transition-metal fluoroiodate24CsAB 8 O 12 F 2 ·CsI (A = K + , NH 4 + ): design of two fluorooxoborates with benign layered structures via a salt-inclusion strategy28KSb(BeF 3 )F 3 : a totally fluorine strategy for achieving wide bandgap and large birefringence23Large optical anisotropy-oriented construction of a carbonate-nitrate chloride compound as a potential ultraviolet birefringent material44Li 7 SrScB 12 O 24 and Li 7 Ba 0.6 Ca 0.4 ScB 12 O 24 : two new quaternary rare-earth borates with short UV cutoff edges4Pb 2 Al 2 B 3 O 8 F 3 : structure and properties of a new fluoroaluminoborate with non-traditional chain-like B 3 O 8 groups4Variable dimensionality of the anion framework in four new borophosphates and fluoroborophosphates with short cutoff edges13Review of Heteroleptic Tetrahedra as Birefringent or Nonlinear Optical Motifs17The dependence of crystal structure and ultraviolet nonlinear optical property of KBe2BO3F2 by density functional theory and π-conjugate confinement2Atomic‐Scale Mechanism of Spontaneous Polarity Inversion in AlN on Nonpolar Sapphire Substrate Grown by MOCVD25Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra9Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra84Inorganic nonlinear optical materials7Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Synthesis, crystal structure and optical properties of the first bromine-containing iodate: Pb2IO3Br30An Optimized KBe2BO3F2‐Like Structure: The Unity of Deep‐Ultraviolet Transparency, Nonlinear Optical Property, and Ferroelectricity22Deep-ultraviolet nonlinear optical crystals: concept development and materials discovery181Decentering the Symmetry via Docking B and F in the KBe2BO3F2-Family Structure0Sn3B10O17Cl2 Achieving Birefringence Enhancement by Stereochemical Activity Lone Pair9Li2PbB2O5: A Pyroborate with Large Birefringence Induced by the Synergistic Effect of Stereochemical Active Lone Pair Cations and π-Conjugated [B2O5] Groups14A 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 Birefringence18CaBO2F: A novel deep-UV structural template with high nonlinear optical performance induced by electron delocalization25Exploring Short-Wavelength Phase-Matching Nonlinear Optical Crystals by Employing KBe2BO3F2 as the Template95La2B3O4(OH)3(SO4)2: A new rare-earth borate-sulfate with second-harmonic generation response5Li0.5Na0.5AlB2O4F2: Fluoroaluminoborate with Aligned 1∞[BO2] Chain Induced by Unprecedented [AlO3F3]6− Species Features Enhanced Birefringence30NaHSO4·H2O: A Promising Deep-Ultraviolet Nonlinear-Optical Bisulfate with Large Birefringence and a Second-Harmonic-Generation Effect16Aluminoborates as Nonlinear Optical Materials79Aluminoborates as Nonlinear Optical Materials14A 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 materials181Deep-ultraviolet nonlinear-optical crystal BaNa2[PO3(OH)]2 with large birefringence and strong second-harmonic-generation response8Enhancement of birefringence and refractive index dispersion optimization from iodates to fluorooxoiodates1Evaluating refractive index and birefringence of nonlinear optical crystals: Classical methods and new developments45Solvent-free synthesis of magnesium phosphite-oxalates that show second-harmonic generation responses5The first polyanion-substitution-driven centrosymmetric-to-noncentrosymmetric structural transformation realizing an excellent nonlinear optical supramolecule [Cd 4 P 2 ][CdBr 4 ]17Three new aluminoborates: from 1D tube to 3D framework9Two Acentric Aluminoborates Incorporated d10 Cations: Syntheses, Structures, and Nonlinear Optical Properties24Small Changes, Big Impact: Tungsten Bronzes with Extremely Large Second Harmonic Generation Achieved by the Transition Metal Doping on the B‐Site26A Rare‐Earth Selenite with Unexpectedly Well‐Balanced Ultraviolet Nonlinear Optical Functionality, Sc(HSeO 3 ) 331Recent progress in ultraviolet and deep-ultraviolet nonlinear optical aluminoborates17Structural Motif Cosubstitution Strategy for Designing Fluoroaluminoborate with the Sr2Be2B2O7-Type Double-Layered Structure14Cs 3 [(BOP) 2 (B 3 O 7 ) 3 ]: A Deep-Ultraviolet Nonlinear Optical Crystal Designed by Optimizing Matching of Cation and Anion Groups169Fluorooxoborate Promoting the Exploration of Short-Wavelength Linear and Nonlinear Optical Crystals with Expected Properties and Versatile Structures27The Strategy to Improve the Phase Matching Ability in Tetrahedron‐Based Deep‐Ultraviolet Nonlinear Optical Crystals21Enlargement of Bandgap and Birefringence in Nonlinear Optical Alkali‐Metal Sulfate Crystals by the Substitution of Asymmetrical Non‐π‐Conjugated Cation8Tailored Synthesis of Two Metal Borates KSrM3B2O9 (M = Al and Ga) Exhibiting Wide Ultraviolet Transparency4Breaking the Inherent Interarrangement of [B3O6] Clusters for Nonlinear Optics with Orbital Hybridization Enhancement142Rb 3 MgB 5 O 10 and LiBaAl(BO 3 ) 2 : covalent tetrahedra MO 4 -containing borates with deep-ultraviolet cutoff edges9Rational Design of the Alkali Metal Sn‐Based Mixed Halides with Large Birefringence and Wide Transparent Range44“One stone two birds” design of borates featuring edge-sharing [BO 4 ] and different B–O configurations in one structure utilizing covalent tetrahedra8A UV non-hydrogen pure selenite nonlinear optical material for achieving balanced properties through framework-optimized structural transformation41Ca 3 Al 2 B 8 O 18 : borate with a graphene-like layer featuring two types of topological six-membered rings induced by [AlO 4 ] units7CsAlB 3 O 6 Cl: the rational construction of a KBBF-type structure with aligned 2 ∞ [AlB 3 O 6 Cl] layers via introducing unprecedented [AlO 3 Cl] tetrahedra5From BaAlBO 3 F 2 to BaAlB 3 O 6 F 2 and BaAl 2 (B 3 O 6 ) 2 F 2 : the enhancement of birefringence and band gap by extending the π-conjugated system combined with [Al–O/F] functional groups13Galloborates as ultraviolet nonlinear optical crystals: advances and perspectives8New antimony fluorooxoborates with strong birefringence and unprecedented structural characterisation19Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Design of Deep-Ultraviolet Zero-Order Waveplate Materials by Rational Assembly of [AlO2F4] and [SO4] Groups9Synthesis, structures and properties of two new nitrate optical materials: Rb3ZnNO3Cl4 and Rb5Na(NO3)4Cl24Toward the ultraviolet (UV) or deep-UV nonlinear optical crystals: The combination of π-conjugated planar [XY3] and tetrahedral [XY4]80KPO2(NHCONH2)2: A Promising Deep-Ultraviolet Nonlinear Optical Phosphate Containing Polar [PO2(NHCONH2)2]− Tetrahedra15Rational Combination of π‐Conjugated and Non‐π‐Conjugated Groups Achieving Strong Nonlinear Optical Response, Large Optical Anisotropy, and UV Light‐Switchable Fluorescence65A perspective on deep-ultraviolet nonlinear optical materials13(C 8 H 7 N 2 O 2 ) 2 [Bi 2 Br 8 ]·2H 2 O and (C 8 H 7 N 2 O 2 ) 6 [Bi 2 Cl 10 ]Cl 2 ·2H 2 O: Exploring Birefringent Crystals in Hybrid Halide Systems5(C3N2H5)B3O3F2(OH)2: Realizing Large Birefringence via a Synergistic Effect between Anion F/OH‐Ratio Optimization and Cation Activation25K3Y3(BO3)4: A Potential UV Nonlinear-Optical Crystal Designed by a Chemical Substitution Strategy14Rb 1.87 Cs 1.13 B 8 O 13 (NO 3 ): a new acentric borate-nitrate with two types of three-dimensional interpenetrating lattices1K 15 La 7 (BO 3 ) 12 : A KBBF-Like Nonlinear-Optical Material with a Short Cutoff Edge and a Strong Second-Harmonic-Generation Response10Looking Back the Nonlinear Optical Crystals in a Functionalized Unit's Perspective109“Three functions in one”: multifunctional rare-earth cyamelurates with magnetism, luminescence, and giant optical nonlinearity6BaAlPO 4 F 2 : structure and properties of the first barium fluoroaluminophosphate with the mixed anion group [Al 2 PO 8 F 5 ]1Coordinated assembly of alkali and alkaline earth metals with the perfluorinated [AlF 6 ] group to design deep-ultraviolet zero-order waveplate materials2KNa 2 Y 2 B 2 O 6 F 3 : a beryllium free deep-UV nonlinear optical crystal with well-balanced properties2LiBa 3 Al 2 B 3 O 11 : a deep-ultraviolet transparent optical borate featuring a 2D [Al 2 B 3 O 11 ] ∞ layered structure0层状结构深紫外非线性光学晶体研究进展(特邀)2新型非线性光学晶体和双折射晶体的研究进展(特邀)4混合阴离子无水无机硼酸盐深紫外非线性光学晶体的研究进展(特邀)4An alkali and rare earth metal mixed cyanurate KLa2(C3N3O3)2Cl with large birefringence: Synthesis and characterization2A Promising Deep Ultraviolet Nonlinear Optical Crystal Activated by the Ordered Structure Design40A Promising Deep Ultraviolet Nonlinear Optical Crystal Activated by the Ordered Structure Design3Review of KBe2BO3F2-like second-order nonlinear optical materials and their structure-performance relationships13[C( NH2 )3] 2SiF6 : Design of Deep Ultraviolet Crystals with Large Birefringence Based on a Fluorination‐Oriented Strategy13Three-In-One: A Guanidinium-Containing Niobium Oxyfluoride with a Perovskite-like Structure Revealing Multifunctional Optical Properties2Modulation of Crystal Structure and Birefringence: Cation Size Effect in Alkali Metal Fluoroaluminoborates4Low‐Dimensional Organic–Inorganic Hybrid Metal Halide with Large Optical Anisotropy9A-Site Cation Substitution toward Structural Transformation in Phosphates Exhibiting Short UV Transparency and Second Harmonic Response3Promising UV/DUV nonlinear optical materials with X-membered (X = multiples of 6) rings in anhydrous inorganic borates20A Band‐Orientation Co‐Anchoring Strategy for the Design of a High‐Performance Mid‐Infrared Nonlinear Optical Crystal2A Band‐Orientation Co‐Anchoring Strategy for the Design of a High‐Performance Mid‐Infrared Nonlinear Optical Crystal12Unlocking Advanced UV NLO Crystals in Rare‐Earth Metal Borate Fluorides via [B 3 O 6 ]‐Mediated Structural Modulation18Shape‐Topology‐Driven Design of Deep Ultraviolet Nonlinear Optical Crystals: Engineering [CH 3 PO 3 ]–Metal‐Oxo Layered Frameworks for Enhanced SHG, DUV Transparency3Constructing Deep‐Ultraviolet Nonlinear Optical Crystals via Synergistic Combination of Fluorinated Polyhedra and Polymerized BO 3 Units15Topology-symmetry analysis and structure prediction in nonlinear optical AB4O6F (A = Na, K, Rb, Cs, NH4) and AAlB3O6F (A = K, Rb, Cs) polytypes1Charge Compensation via Heterovalent Cation Disorder for Birefringence Modulation to Design UV Nonlinear Optical Crystal0A Lithium Calcium Borate Nonlinear Optical Crystal with Deep-UV Cutoff Edge and Moderate Second-Harmonic Generation Response1Toward the vacuum-ultraviolet frontier in nonlinear optical frequency conversion: phase-matching mechanisms across dimensions and architectures2Covalent Interlayer Engineering Enables Ideal Birefringence and Strong SHG in Beryllium‐Free Deep‐UV NLO Borates2

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  2. Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich

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  3. Helix-constructed polar rare-earth iodate fluoride as a laser nonlinear optical multifunctional material

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

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  5. K2Na(IO3)2(I3O8) with Strong Second Harmonic Generation Response Activated by Two Types of Isolated Iodate Anions

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  7. Li4Ca2B8O16: A Borate with a Unique Fundamental Building Block and a Short Cutoff Edge

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  35. A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**

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