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RESEARCH PAPER · Angewandte Chemie International Edition · 2017

Beryllium‐Free β‐Rb2Al2B2O7 as a Possible Deep‐Ultraviolet Nonlinear Optical Material Replacement for KBe2BO3F2

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Beryllium‐Free β‐Rb2Al2B2O7 as a Possible Deep‐Ultraviolet Nonlinear Optical Material Replacement for KBe2BO3F2OriginalTwo deep-ultraviolet nonlinear optical alkaline-earth metal borates based on different types of oxoboron clusters56Extending Unique 1D Borate Chains to 3D Frameworks by Introducing Metallic Nodes44Synthesis, second-harmonic generations (SHG), and photoluminescence (PL) properties of Ca 4 Bi 6-x Ln x O 13 (Ln=La and Eu) solid solutions3Tanabe Prize in Acid–Base Catalysis and Robert B. Anderson Catalysis Award: B. M. Weckhuysen / MRS Outstanding Young Investigator Award: J. A. Dionne and J. M. Rondinelli / VAAM Research Prize: T. J. Erb2Tanabe‐Preis für Säure‐Base‐Katalyse und Robert B. Anderson Catalysis Award: B. M. Weckhuysen / MRS Outstanding Young Investigator Award: J. A. Dionne und J. M. Rondinelli / VAAM‐Forschungspreis: T. J. Erb2Finding the Next Deep-Ultraviolet Nonlinear Optical Material: NH4B4O6F1233Na2(H2en)[B5O8(OH)]2[B3O4(OH)]2 and Na3(HCOO)[B5O8(OH)]: Two Borates Co‐Templated by Inorganic Cations and Organic Compounds20CsB 4 O 6 F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units184CsB4O6F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units895Syntheses, crystal structure and luminescent properties of polyborates PbLnB7O13 (Ln = Gd, Sm) with a 2D [B7O13]∞ framework13K2[B3O3(OH)5]: A new deep-UV nonlinear optical crystal with isolated [B3O3(OH)5]2- anionic groups31Structural and spectroscopic properties of new noncentrosymmetric self-activated borate Rb3EuB6O12 with B5O10 units182From a Metastable Layer to a Stable Ring: A Kinetic Study for Transformation Reactions of Li2Mo3TeO12 to Polyoxometalates12Ba 3 B 10 O 17 Br 2 : a new barium borate halide with B–O layered structure4Cs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response129K 11 RbB 28 O 48 : a new triple-layered borate with an unprecedented [B 28 O 57 ] fundamental building block19RbSe 3 B 2 O 9 (OH) and CsSe 3 B 2 O 9 (OH): one dimensional boroselenite-based anionic frameworks with second harmonic generation properties15Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials191Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials714Non-Centrosymmetric RbNaMgP 2 O 7 with Unprecedented Thermo-Induced Enhancement of Second Harmonic Generation239A new luminescent host material K3GdB6O12: synthesis, crystal structure and luminescent properties activated by Sm3+7SrB 5 O 7 F 3 Functionalized with [B 5 O 9 F 3 ] 6− Chromophores: Accelerating the Rational Design of Deep‐Ultraviolet Nonlinear Optical Materials738SrB5O7F3 Functionalized with [B5O9F3]6− Chromophores: Accelerating the Rational Design of Deep‐Ultraviolet Nonlinear Optical Materials116A Series of Rare-Earth Borates K 7 MRE 2 B 15 O 30 (M = Zn, Cd, Pb; RE = Sc, Y, Gd, Lu) with Large Second Harmonic Generation Responses103M2B10O14F6 (M = Ca, Sr): Two Noncentrosymmetric Alkaline Earth Fluorooxoborates as Promising Next-Generation Deep-Ultraviolet Nonlinear Optical Materials356Recent advances in ultraviolet and deep-ultraviolet second-order nonlinear optical crystals257The role of cations in second-order nonlinear optical materials based on π-conjugated [BO 3 ] 3− groups195Deep‐Ultraviolet Nonlinear Optical Crystal Cs2Al2(B3O6)2O: A Benign Member of the Sr2Be2(BO3)2O Family with [Al2(B3O6)2O]2− Double Layers70Polar Fluorooxoborate, NaB4O6F: A Promising Material for Ionic Conduction and Nonlinear Optics494Polar Fluorooxoborate, NaB4O6F: A Promising Material for Ionic Conduction and Nonlinear Optics67Beryllium-Free Nonlinear-Optical Crystals A 3 Ba 3 Li 2 Ga 4 B 6 O 20 F (A = K and Rb): Members of the Sr 2 Be 2 (BO 3 ) 2 O Family with a Strong Covalent Connection between the ∞ 2 [Li 2 Ga 4 B 6 O 20 F] 9– Double Layers27Anisotropy of nonlinear optical properties in monoclinic SmxY1-xCa4O(BO3)3 crystals12From Sr2Nb2O7to CaxSr2–xNb2O7: An Effective Enhancement of Nonlinear Optical Activity by a Simple Way of Cation Substituting11Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges16Removal of A-Site Alkali and Alkaline Earth Metal Cations in KBe2BO3F2-Type Layered Structures To Enhance the Deep-Ultraviolet Nonlinear Optical Capability46Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response8BaPO3Cl: a Metal Phosphate Chloride with Infinite [PO3]∞ Chains25Growth, Crystal Structures, and Characteristics of Li 5 ASrMB 12 O 24 (A = Zn, Mg; M = Al, Ga) with [MB 12 O 24 ] Frameworks12Ba 3 Ca 4 (BO 3 ) 3 (SiO 4 )Cl: a new non-centrosymmetric complex alkaline-earth metal borosilicate chloride with a deep-ultraviolet cut-off edge19Ca 2 GeB 2 O 7 and Ca 1.78 Cd 0.22 GeB 2 O 7 : two acentric borogermanates with a melilite-like structure and short ultraviolet cutoff edge14Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F27Fluoroborophosphates: a family of potential deep ultraviolet NLO materials43Rational Design via Synergistic Combination Leads to an Outstanding Deep-Ultraviolet Birefringent Li2Na2B2O5 Material with an Unvalued B2O5 Functional Gene284Zeolitic Open-Framework Borates with Noncentrosymmetric Structures and Nonlinear Optical Properties24Two Non-π-Conjugated Deep-UV Nonlinear Optical Sulfates268Module-Analysis-Assisted Design of Deep Ultraviolet Fluorooxoborates with Extremely Large Gap and High Structural Stability109Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)28Two Deep Ultraviolet Hydrated Borate Crystals: Centrosymmetric LiRbB5O8(OH)·H2O and Non-Centrosymmetric K2B5O8(OH)·2H2O8First-principle study on structural, linear and nonlinear optical properties of selenocyanate complex ZnCd(SeCN)4 crystal6β‐CsB9O14: A Triple‐Layered Borate with Edge‐Sharing BO4 Tetrahedra Exhibiting a Short Cutoff Edge and a Large Birefringence30Mixed Transition Metal (Oxy)fluoride Paramagnet Chains: Synthesis, Structure, and Characterization11Prediction 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 Layers24Research and Development of Zincoborates: Crystal Growth, Structural Chemistry and Physicochemical Properties20Histidinium‐Driven Chirality Control of Self‐Assembled Hybrid Molybdenum Oxyfluorides24KMg(H 2 O)PO 4 : A Deep-Ultraviolet Transparent Nonlinear Optical Material Derived from KTiOPO 483CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Syntheses and structures of a new 2D layered borate and a novel 3D porous-layered aluminoborate17Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Gd(NO 3 )(Se 2 O 5 )·3H 2 O: a nitrate–selenite nonlinear optical material with a short ultraviolet cutoff edge28Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320Two New Ferroborates with Three‐Dimensional Framework and Wide Transmittance Window2Designing a Deep-UV Nonlinear Optical Fluorooxosilicophosphate127Aliovalent-substituted synthesis for a non-centrosymmetric phosphate with enhanced nonlinear-optical response5Hydrogen-Bond-Assisted Reinforcement of Interlayer Connections in Zn2BO3X·H2O (X = Cl, Br): Two UV Nonlinear Optical Crystals with KBBF-Type Structure9Two 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 Materials29Gadolinium-Rich Borate Gd 17.33 (BO 3 ) 4 (B 2 O 5 ) 2 O 16 Exhibiting a Magnetocaloric Effect24Zn3B7O13Cl: A New Deep-Ultraviolet Transparency Nonlinear Optical Crystal with Boracite Structure24Nonlinear-Optical Crystal Rb3YB6O12 with Condensed B5O10 Blocks That Exhibits an Intriguing Structural Arrangement and a Short Ultraviolet Absorption Edge26Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )212Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )57Cs 2 AlB 5 O 10 : a short-wavelength nonlinear optical crystal with moderate second harmonic generation response12Ba 3 [Al(PO 4 ) 3 ]: rational design of a promising deep-UV transparent SHG crystal with balanced overall performance originating from the condensation of quartz-type [Al(PO 4 ) 4 ] 9− units16Ba 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 -borate34Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41Deep-ultraviolet transparent alkali metal–rare earth metal sulfate NaY(SO 4 ) 2 ·H 2 O as a nonlinear optical crystal: synthesis and characterization28Pb 2 TiFO(SeO 3 ) 2 Br: a new polar compound with the strongest second harmonic generation in the selenite bromide family29Ultraviolet nonlinear optical crystals A 3 SrBi(P 2 O 7 ) 2 (A = K, Rb) with large second harmonic generation responses15M(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 Birefringence27New Polymorphism for Ba3Zn2(BO3)3F with Two Polymorphs Exhibiting Anomalous Phase Transition2Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance43Prediction of Novel van der Waals Boron Oxides with Superior Deep‐Ultraviolet Nonlinear Optical Performance6Second-order nonlinear optical property of the ultraviolet transparent alkali metal-rare earth metal carbonate Na3Y(CO3)3.3H2O5A Deep‐UV Nonlinear Optical Borosulfate with Incommensurate Modulations71A Deep‐UV Nonlinear Optical Borosulfate with Incommensurate Modulations13Borosilicate Crystal LaBSiO5: A New Promising Ultraviolet Quasiphase Matching Material31UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate196UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate28RbMT3(BO3)2O3 (M=Ba, Sr; T=Al, Ga): New Double‐Layered Oxyborates Constructed from [BO3] Triangles and [TO4] Tetrahedra13Large Magnetocaloric Effect in Li3K9Gd3(BO3)7 Crystal Featuring Sandwich-Like Three-Dimensional Framework22Cs4B4O3F10: First Fluorooxoborate with [BF4] Involving Heteroanionic Units and Extremely Low Melting Point18Expanding the chemistry of borates with functional [BO2]− anions200K5Mg2La3(BO3)6: An Efficient, Deep-Ultraviolet Nonlinear Optical Material70Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials282D van der Waals Layered [C(NH2)3]2SO3S Exhibits Desirable UV Nonlinear-Optical Trade-Off47Achieving 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] Units9Strong 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 Modification9Unusual ferroelectric-dependent birefringence in 2D trilayered perovskite-type ferroelectric exploited by dimensional tailoring63Structure and Origin of the Second-Harmonic Generation Response of Nonlinear Optical Material Sr2Be2B2O713AAl3P6O20 (A = Rb, Cs): Two deep-ultraviolet transparent nonlinear optical materials designed by aliovalent substitution11Halogen-Ion-Induced Structural Phase Transition Giving a Polymorph of HgBr2 with Balanced Nonlinear Optical Properties8Ba 2 Zn 2 B 6 O 13 : coplanar [B 2 O 5 ] in unnoted U-shaped [B 6 O 13 ] groups achieving large birefringence6KF·B(OH) 3 : a KBBF-type material with large birefringence and remarkable deep-ultraviolet transparency33Na 3 AEZn 2 B 3 O 9 (AE = Mg, Ca): two new short-wave ultraviolet beryllium-free Sr 2 Be 2 B 2 O 7 -type zincoborates designed by chemical cosubstitution9Nain(C2o4)(Hpo4)(H2o)5: An Ultraviolet Transparent Nonlinear Optical Oxalate-Phosphate with Large Birefringence0Pb 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 groups4PO(CH 2 CH 2 CF 3 ) 3 : an organic ultraviolet nonlinear optical material without any anionic group3α-LiMB 9 O 15 (M = Sr, Pb): flexible [B 3 O 7 ] units leading to the low temperature phase of β-LiMB 9 O 15 (M = Sr, Pb)11MM′B3O4F3 (M = K; M′ = Na, K, Cs): Alkali-Metal Fluorooxoborates with ∞1[B3O4F3] Chains and Deep-Ultraviolet Cutoff Edges12“Removing Center”─An Effective Structure Design Strategy for Nonlinear Optical Crystals37Advances in second-order nonlinear optical sulfates38Ba2B10O16(OH)2·(H3BO3)(H2O): A Possible Deep-Ultraviolet Nonlinear-Optical Barium Borate36Strong 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)2212A2BeS2O8 (A = NH4, K, Rb, Cs) Deep Ultraviolet Nonlinear Optical Crystals33[C4H4O4]⋅[C6H13N] as a nonlinear optical co-crystal with spike-like dielectric anomalies0Deep-ultraviolet nonlinear optical crystals: concept development and materials discovery181Decentering the Symmetry via Docking B and F in the KBe2BO3F2-Family Structure0Achieving Large Second Harmonic Generation Effects via Optimal Planar Alignment of Triangular Units64Phosphites: A Nonlinear Optical Materials System with a Wide Band Gap and Moderate Second-Harmonic Generation Effect27Exploring Short-Wavelength Phase-Matching Nonlinear Optical Crystals by Employing KBe2BO3F2 as the Template95Aluminoborates as Nonlinear Optical Materials79Aluminoborates as Nonlinear Optical Materials14A promising ultraviolet nonlinear optical crystal: Rb 3 Ba 3 Li 2 Al 4 B 6 O 20 F—crystal growth, physical properties, and 266 nm laser generation17Constructing ultraviolet nonlinear optical crystals with large second harmonic generation and short absorption edges by using polar tetrahedral S 2 O 3 groups14KMB 4 O 6 F 3 (M = Co, Fe): two-dimensional magnetic fluorooxoborates with triangular lattices directed by triangular BO 3 units16Recent advances on the synthesis of Sb(III)-based inorganic ultraviolet nonlinear optical materials47Three new aluminoborates: from 1D tube to 3D framework9BaB2P2O8F2: A Fluoroborophosphate with [B2P2O8F2]∞ Layers and Deep-Ultraviolet Cutoff Edge4Two Acentric Aluminoborates Incorporated d10 Cations: Syntheses, Structures, and Nonlinear Optical Properties24Fluorooxoborates: A precious treasure of deep-ultraviolet nonlinear optical materials24Recent advances of inorganic phosphates with UV/DUV cutoff edge and large second harmonic response7Recent progress in ultraviolet and deep-ultraviolet nonlinear optical aluminoborates17Recent advances in non-π-conjugated nonlinear optical sulfates with deep-UV absorption edge53An interlinked prediction-experiment paradigm discovering deep-ultraviolet fluorooxoborates with desired optical nonlinearity and birefringence76Two Mixed-Alkali-Metal Selenates as Short-Wave Ultraviolet Nonlinear-Optical Materials10Design Principles for Noncentrosymmetric Materials23Ultraviolet Crystal with Strong Optical Nonlinearity by Creating Halogen-Centered Secondary Building Blocks15A Non‐π‐Conjugated Molecular Crystal with Balanced Second‐Harmonic Generation, Bandgap, and Birefringence10Tailored Synthesis of Two Metal Borates KSrM3B2O9 (M = Al and Ga) Exhibiting Wide Ultraviolet Transparency4Ultrashort Phase‐Matching Wavelength and Strong Second‐Harmonic Generation in Deep‐UV‐Transparent Oxyfluorides by Covalency Reduction33Ultrashort Phase‐Matching Wavelength and Strong Second‐Harmonic Generation in Deep‐UV‐Transparent Oxyfluorides by Covalency Reduction3K(NH4)Zn2(PO4)2: a Beryllium-Free Sr2Be2B2O7 Derivative with Enhanced Interlayer Connectivity7A bifunctional primitive strategy induces enhancements of large second harmonic generation and wide UV transmittance in rare-earth borates containing [B 5 O 10 ] groups22

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  1. Two deep-ultraviolet nonlinear optical alkaline-earth metal borates based on different types of oxoboron clusters

    Dalton Transactions · 2017-01-01

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  2. Extending Unique 1D Borate Chains to 3D Frameworks by Introducing Metallic Nodes

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  3. Synthesis, second-harmonic generations (SHG), and photoluminescence (PL) properties of Ca 4 Bi 6-x Ln x O 13 (Ln=La and Eu) solid solutions

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  4. Tanabe Prize in Acid–Base Catalysis and Robert B. Anderson Catalysis Award: B. M. Weckhuysen / MRS Outstanding Young Investigator Award: J. A. Dionne and J. M. Rondinelli / VAAM Research Prize: T. J. Erb

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  5. Tanabe‐Preis für Säure‐Base‐Katalyse und Robert B. Anderson Catalysis Award: B. M. Weckhuysen / MRS Outstanding Young Investigator Award: J. A. Dionne und J. M. Rondinelli / VAAM‐Forschungspreis: T. J. Erb

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  6. Finding the Next Deep-Ultraviolet Nonlinear Optical Material: NH4B4O6F

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  12. Structural and spectroscopic properties of new noncentrosymmetric self-activated borate Rb3EuB6O12 with B5O10 units

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  14. Ba 3 B 10 O 17 Br 2 : a new barium borate halide with B–O layered structure

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  15. Cs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response

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  16. K 11 RbB 28 O 48 : a new triple-layered borate with an unprecedented [B 28 O 57 ] fundamental building block

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  30. Polar Fluorooxoborate, NaB4O6F: A Promising Material for Ionic Conduction and Nonlinear Optics

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  31. Beryllium-Free Nonlinear-Optical Crystals A 3 Ba 3 Li 2 Ga 4 B 6 O 20 F (A = K and Rb): Members of the Sr 2 Be 2 (BO 3 ) 2 O Family with a Strong Covalent Connection between the ∞ 2 [Li 2 Ga 4 B 6 O 20 F] 9– Double Layers

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  32. Anisotropy of nonlinear optical properties in monoclinic SmxY1-xCa4O(BO3)3 crystals

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