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RESEARCH PAPER · Angewandte Chemie · 2017

CsB 4 O 6 F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units

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CsB 4 O 6 F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional UnitsOriginalLi 3 Ge 3 Se 6 : the first ternary lithium germanium selenide with interesting ∞ [Ge 6 Se 12 ] n chains constructed by ethane-like [Ge 2 Se 6 ] 6− clusters8The First Alkaline‐Earth Fluorooxoborate Ba[B4O6F2]—Characterisation and Doping with Eu2+95K2[B3O3(OH)5]: A new deep-UV nonlinear optical crystal with isolated [B3O3(OH)5]2- anionic groups31Noncentrosymmetric Cubic Cyanurate K6Cd3(C3N3O3)4 Containing Isolated Planar π-Conjugated (C3N3O3)3– Groups59LiCs 2 La(BO 3 ) 2 and Li 3 K 9 La 3 (BO 3 ) 7 : new mixed alkali metal lanthanum borates with three-dimensional open frameworks and short cut-off edges10NH 4 B 11 O 16 (OH) 2 : a new ammonium borate with wavy-shaped polycyclic 2∞[B 11 O 16 (OH) 2 ] layers27Pb 3 (SeO 3 )Br 4 : a new nonlinear optical material with enhanced SHG response designed via an ion-substitution strategy36Pb4(BO3)2(SO4) and Pb2[(BO2)(OH)](SO4): New lead(II) borate-sulfate mixed-anion compounds with two types of 3D network structures10Pb8M(BO3)6 (M = Mg, Ca): Two new borates with large birefringence activated by the ∞[Pb8B6O18]2- double layers6SrB 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 Materials116Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials237Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials24Ba4B8TeO19: A UV Nonlinear Optical Material41Deep‐Ultraviolet Nonlinear Optical Crystal Cs2Al2(B3O6)2O: A Benign Member of the Sr2Be2(BO3)2O Family with [Al2(B3O6)2O]2− Double Layers70CaB5O7F3: A Beryllium-Free Alkaline-Earth Fluorooxoborate Exhibiting Excellent Nonlinear Optical Performances192Polar Fluorooxoborate, NaB4O6F: A Promising Material for Ionic Conduction and Nonlinear Optics494Polar Fluorooxoborate, NaB4O6F: A Promising Material for Ionic Conduction and Nonlinear Optics67NH4Be2BO3F2 and γ‐Be2BO3F: Overcoming the Layering Habit in KBe2BO3F2 for the Next‐Generation Deep‐Ultraviolet Nonlinear Optical Materials280NH4Be2BO3F2 and γ‐Be2BO3F: Overcoming the Layering Habit in KBe2BO3F2 for the Next‐Generation Deep‐Ultraviolet Nonlinear Optical Materials68Rb 3 VO(O 2 ) 2 CO 3 : A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response207Rb3VO(O2)2CO3: A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response42Combination of d 10 -cations and fluorine anion as active participants to design novel borate/carbonate nonlinear optical materials24Exploring Potential Beryllium-free, Deep-Ultraviolet Optical Crystals in the Rare Earth Fluoride Carbonate–Water System34Rational 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 Properties35From LiB3O5 to NaRbB6O9F2: Fluorine‐Directed Evolution of Structural Chemistry33A Fluorooxosilicophosphate with an Unprecedented SiO2F4 Species56A Fluorooxosilicophosphate with an Unprecedented SiO2F4 Species5Synthesis and electronic structure studies of a novel nonlinear optical crystal L-leucinium squarate monohydrate: A spectroscopic view13Designing Deep‐UV Birefringent Crystals by Cation Regulation57Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102Theoretical study of electronic structure and optical properties of tin doped CuS counter electrode for dye-sensitized solar cells12Cation substitution inducing gap changes and covalent interaction flexibility enhancing second harmonic generation responses in d10 metal chalcogenides11Tailoring nonlinear optical crystal borophosphate through the introduction of transition metal d orbitals for improving optical anisotropy and SHG response: a first-principles investigation1Synthesis and Characterization of the First Tin Fluoride Borate Sn3[B3O7]F with Second Harmonic Generation Response28Effects of transition metals on physical properties of M2BC (M = V, Nb, Mo and Ta): A DFT calculation74PbCdF(SeO 3 )(NO 3 ): A Nonlinear Optical Material Produced by Synergistic Effect of Four Functional Units52Why Some Noncentrosymmetric Borates Do Not Make Good Nonlinear Optical Materials: A Case Study with K3B5O8(OH)222Near infrared broadband emission of a new bismuth-doped Gd0.1Y0.9AlO3 crystal3Structure–Property Relationship and Systematic Study of a Series of Terpyridine Based Nonlinear Optical Compounds: DFT Computation of Interactive Design14Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response8Metal-cation substitutions induced the enhancement of second harmonic generation in A 8 BS 6 (A = Cu, and Ag; B = Si, Ge, and Sn)14Multifunctional property exploration: Bi 4 O 5 I 2 with high visible light photocatalytic performance and a large nonlinear optical effect32Pb 10 O 4 (BO 3 ) 3 I 3 : a new noncentrosymmetric oxyborate iodide synthesized by the straightforward hydrothermal method6Crystallographic Investigations into the Polar Polymorphism of BaTeW2O9: Phase Transformation, Controlled Crystallization, and Linear and Nonlinear Optical Properties26Quantum chemical calculations, structural, spectral and nonlinear optical investigations of a novel crystal N,N ′-diphenylguanidinium 3,5-dichlorobenzoate24DFT analysis on spectral and NLO properties of (2E)-3-[4-(dimethylamino) phenyl]-1-(naphthalen-2-yl) prop-2-en-1-one; a d-π-A chalcone derivative and its docking studies as a potent hepatoprotective agent23RbB 11 O 16 (OH) 2 : First Hydroxyl Rubidium Borate with the B‐O 2D Layer Featuring Large Birefringence in the Rb‐B‐O‐H System5BaB 2 O 3 F 2 : A Barium Fluorooxoborate with a Unique [B 2 O 3 F] − Layer and Short Cutoff Edge38Synthesis, Characterization and Optical Properties of Two Metal Borates Containing Two Types of Oxoboron Clusters2Cs3Na(H2C3N3O3)4·3H2O: A Mixed Alkali‐Metal Hydroisocyanurate Nonlinear Optical Material Containing π‐Conjugated Six‐Membered‐Ring Units68Sr 6 Cd 2 Sb 6 O 7 S 10 : Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups124Sr6Cd2Sb6O7S10: Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups22β‐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 Layers24Experiment and First-Principles Calculations of A2Mg2TeB2O10 (A = Pb, Ba): Influences of the Cosubstitution on the Structure Transformation and Optical Properties21Two 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)33Five New Silver Rare‐Earth Iodates, AgLn(IO3)4 (Ln=Pr, Sm, Dy, Er and Tm): Synthesis, Structures and Properties6K5B19O31: A Deep‐Ultraviolet Congruent Melting Compound6Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin255Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin33Synthesis and structure of calcium-tin hybrid microparticles from egg shell and investigation of their thermal behavior and catalytic application13Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Syntheses, structures and characterization of non-centrosymmetric Rb 2 Zn 3 (P 2 O 7 ) 2 and centrosymmetric Cs 2 M 3 (P 2 O 7 ) 2 (M = Zn and Mg)26A Promising Fluorooxoborate Framework with Flexibile Capability for Diverse Cations to Enhance the Second Harmonic Generation14An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses224An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses42Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra147Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra43Lead 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 Materials55Syntheses, characterization and calculations of LimAnM6O15 (A=Rb, Cs; M=Si, Ge; m+n=6)18Rational Design of the Metal‐Free KBe 2 BO 3 F 2 ⋅(KBBF) Family Member C(NH 2 ) 3 SO 3 F with Ultraviolet Optical Nonlinearity201Rational Design of the Metal‐Free KBe2BO3F2⋅(KBBF) Family Member C(NH2)3SO3F with Ultraviolet Optical Nonlinearity31Two 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 Materials29A(H3C3N3O3)(NO3) (A = K, Rb): Alkali-Metal Nitrate Isocyanurates with Strong Optical Anisotropy47Sr5Ga8O3S14: A Nonlinear Optical Oxysulfide with Melilite-Derived Structure and Wide Band Gap48Hierarchical Contribution of Anions to Second Harmonic Generation in A2HgI4 (A = Na, Ag, Cu) Regulated Dramatically by Metal Cations4Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm38A2BBi2(PO4)2(P2O7) (A = K, Rb, B = Pb, Cd): the Effect of Cation Sizes on Structural Evolution10Ba3(BO3)(CO3)F: The First Borate Carbonate Fluoride Synthesized by the High‐Temperature Solution Method19Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research19Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research140Giant 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 )57KSnI 3 ⋅ H 2 O: A New Compound with One‐Dimensional SnI 3 Chains of Pyramidal SnI 5 Polyhedra2M(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 Transition2M3B6O10NO3 (M = K, Rb): Two New Alkali Metal Borate‐Nitrates with Noncentrosymmetric Structures20Prediction 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 Performance6LiZn(OH)CO3: A Deep‐Ultraviolet Nonlinear Optical Hydroxycarbonate Designed from a Diamond‐like Structure180LiZn(OH)CO3: A Deep‐Ultraviolet Nonlinear Optical Hydroxycarbonate Designed from a Diamond‐like Structure10RbMT3(BO3)2O3 (M=Ba, Sr; T=Al, Ga): New Double‐Layered Oxyborates Constructed from [BO3] Triangles and [TO4] Tetrahedra13Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application167Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application18Cs4B4O3F10: First Fluorooxoborate with [BF4] Involving Heteroanionic Units and Extremely Low Melting Point18From Centrosymmetry to Noncentrosymmetry: Tailoring the Structural Arrangements of Carbonates with Strong Nonlinear Optical Response through Partial Anion Substitution33Na2Rb2SrB18O30 with [B9O19]11− fundamental building block consisting of three [B3O7]5− groups5Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals146Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals16The First Mixed Calcium Zinc Borate with a Flexible [B8O17] Fundamental Building Block and Short UV Cutoff Edge7Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials28Li 4 MgGe 2 S 7 : The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap213Li4MgGe2S7: The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap15A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation22A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation63NaRbB3O4F3: A New Fluorooxoborate with a Short UV Cutoff Edge Enriching the Structural Chemistry of Borate7Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate22A 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**27Achieving 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] Units9La 3 Ga 3 Ge 2 S 3 O 10 : An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering63La3Ga3Ge2S3O10: An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering18Strong 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 Modification9A New Nonlinear Optical Material with N(CN)2− Anion2From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra10Na4B8O9F10: A Deep‐Ultraviolet Transparent Nonlinear Optical Fluorooxoborate with Unexpected Short Phase‐Matching Wavelength Induced by Optimized Chromatic Dispersion133Na4B8O9F10: A Deep‐Ultraviolet Transparent Nonlinear Optical Fluorooxoborate with Unexpected Short Phase‐Matching Wavelength Induced by Optimized Chromatic Dispersion13Hierarchical Modulation of Optical Anisotropy Driven by Metal Cation Polyhedra in Fluorooxoborates MIIB4O6F2 (MII=Be, Mg, Pb, Zn, Cd)6[ASr 4 Cl][Ge 3 S 10 ] (A = Na, K) and [KBa 4 Cl][Ge 3 S 10 ]: new salt-inclusion infrared nonlinear optical crystals with zero-dimensional [Ge 3 S 9 ] clusters32Sulfamide: 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] Tetrahedra84LiB5O5F2(OH)4: A new deep-ultraviolet birefringent crystal with [B5O5F2(OH)4] anionic group28Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species6Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species83Realization of Enlarged Birefringence from BaCdBe2(BO3)2F2 to NaMgBe2(BO3)2F via the Cation Size Effect as a Potential Deep-Ultraviolet Birefringent Material18A Theoretical Perspective to Study the Optical Properties of Tetrafluoroborates4Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters9Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters139Design of New Borates with Deep Ultraviolet Transparency Inspired by the Flexibility of Unusual Triple-Layered Frameworks3AgGaSe2-Inspired Nonlinear Optical Materials: Tetrel Selenides of Alkali Metals and Mercury34Broadband 1T-polytype tantalum disulfide saturable absorber for solid-state bulk lasers10[C(NH2)3]2Zn(CO3)2: A Guanidinium-Templated Ultraviolet Nonlinear Optical Material20[Cs6Cl][Ga5GeQ12] (Q = S, Se): two novel porous layered chalcohalides exhibiting two-band emission and ion exchange properties6Ag4SnGe2S7: A Noncentrosymmetric Chalcogenide in I4–II–IV2–VI7 System with Non-Diamond-Like Structure Featuring 1D ∞[SnGe2S8]6– Infinite Chain2Li2PbB2O5: A Pyroborate with Large Birefringence Induced by the Synergistic Effect of Stereochemical Active Lone Pair Cations and π-Conjugated [B2O5] Groups14LiKCuP2O7: Cation substitution application with mixed-alkaline copper-containing pyrophosphate and magnetic properties2Aluminoborates as Nonlinear Optical Materials79Aluminoborates as Nonlinear Optical Materials14Oxychalcogenides: A Promising Class of Materials for Nonlinear Optical Crystals with Mixed‐Anion Groups35

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  1. Li 3 Ge 3 Se 6 : the first ternary lithium germanium selenide with interesting ∞ [Ge 6 Se 12 ] n chains constructed by ethane-like [Ge 2 Se 6 ] 6− clusters

    Dalton Transactions · 2017-01-01

    Guangmao Li, Ni Zhen, Yu Chu, Zhongxiang Zhou

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  2. The First Alkaline‐Earth Fluorooxoborate Ba[B4O6F2]—Characterisation and Doping with Eu2+

    Chemistry - A European Journal · 2017-11-03

    Stephan G. Jantz, Florian Pielnhofer, Leo van Wüllen, Richard Weihrich, Martin J. Schäfer, Henning A. Höppe

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  3. K2[B3O3(OH)5]: A new deep-UV nonlinear optical crystal with isolated [B3O3(OH)5]2- anionic groups

    Journal of Alloys and Compounds · 2017-11-16

    Qian Wang, Chensheng Lin, Guohong Zou, Mengjiao Liu, Daojiang Gao, Jian Bi, Ling Huang

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  4. Noncentrosymmetric Cubic Cyanurate K6Cd3(C3N3O3)4 Containing Isolated Planar π-Conjugated (C3N3O3)3– Groups

    Inorganic Chemistry · 2017-12-13

    Mingjun Xia, Molin Zhou, Fei Liang, Xianghe Meng, Jiyong Yao, Zheshuai Lin, Rukang K. Li

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  5. LiCs 2 La(BO 3 ) 2 and Li 3 K 9 La 3 (BO 3 ) 7 : new mixed alkali metal lanthanum borates with three-dimensional open frameworks and short cut-off edges

    Dalton Transactions · 2018-01-01

    Ruru Ma, Yun Mo Yang, Cong Hu, Xiaoyu Dong, Zhihua Yang, Shilie Pan

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  6. NH 4 B 11 O 16 (OH) 2 : a new ammonium borate with wavy-shaped polycyclic 2∞[B 11 O 16 (OH) 2 ] layers

    New Journal of Chemistry · 2018-01-01

    Chunmei Huang, Fangfang Zhang, Bingbing Zhang, Zhihua Yang, Shilie Pan

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

    Dalton Transactions · 2018-01-01

    Xiaoxiao Wang, Xingxing Jiang, Hongming Liu, Lei Yang, Zheshuai Lin, Zhanggui Hu, Xiang‐Gao Meng, Xingguo Chen, Jingui Qin

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  8. Pb4(BO3)2(SO4) and Pb2[(BO2)(OH)](SO4): New lead(II) borate-sulfate mixed-anion compounds with two types of 3D network structures

    Journal of Solid State Chemistry · 2018-01-30

    Tingting Ruan, Wenwen Wang, Chun‐Li Hu, Xiang Xu, Jiang‐Gao Mao

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  9. Pb8M(BO3)6 (M = Mg, Ca): Two new borates with large birefringence activated by the ∞[Pb8B6O18]2- double layers

    Journal of Alloys and Compounds · 2018-02-22

    Chen Zhou, Hui Zhang, Jianian Cheng, Hongyi Li, Sadeh Beysen

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  10. SrB 5 O 7 F 3 Functionalized with [B 5 O 9 F 3 ] 6− Chromophores: Accelerating the Rational Design of Deep‐Ultraviolet Nonlinear Optical Materials

    Angewandte Chemie International Edition · 2018-03-02

    Miriding Mutailipu, Min Zhang, Bingbing Zhang, Liying Wang, Zhihua Yang, Xin Hua Zhou, Shilie Pan

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  11. SrB5O7F3 Functionalized with [B5O9F3]6− Chromophores: Accelerating the Rational Design of Deep‐Ultraviolet Nonlinear Optical Materials

    Angewandte Chemie · 2018-03-02

    Miriding Mutailipu, Min Zhang, Bingbing Zhang, Liying Wang, Zhihua Yang, Xin Hua Zhou, Shilie Pan

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  12. Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials

    Angewandte Chemie International Edition · 2018-03-07

    Hongwei Yu, Nathan Z. Koocher, James M. Rondinelli, P. Shiv Halasyamani

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  13. Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials

    Angewandte Chemie · 2018-03-07

    Hongwei Yu, Nathan Z. Koocher, James M. Rondinelli, P. Shiv Halasyamani

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  14. Ba4B8TeO19: A UV Nonlinear Optical Material

    Inorganic Chemistry · 2018-04-03

    Lili Liu, Joshua Young, Manuel Smeu, P. Shiv Halasyamani

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  15. Deep‐Ultraviolet Nonlinear Optical Crystal Cs2Al2(B3O6)2O: A Benign Member of the Sr2Be2(BO3)2O Family with [Al2(B3O6)2O]2− Double Layers

    Chemistry - A European Journal · 2018-04-15

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  16. CaB5O7F3: A Beryllium-Free Alkaline-Earth Fluorooxoborate Exhibiting Excellent Nonlinear Optical Performances

    Inorganic Chemistry · 2018-04-17

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

    Angewandte Chemie International Edition · 2018-04-17

    Zhizhong Zhang, Ying Wang, Bingbing Zhang, Zhihua Yang, Shilie Pan

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

    Angewandte Chemie · 2018-04-17

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  19. NH4Be2BO3F2 and γ‐Be2BO3F: Overcoming the Layering Habit in KBe2BO3F2 for the Next‐Generation Deep‐Ultraviolet Nonlinear Optical Materials

    Angewandte Chemie International Edition · 2018-05-12

    Guang Peng, Ning Ye, Zheshuai Lin, Lei Kang, Shilie Pan, Min Zhang, Chensheng Lin, Xifa Long, Min Luo, Yu Chen, Yu‐Huan Tang, Feng Xu, Tao Yan

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  20. NH4Be2BO3F2 and γ‐Be2BO3F: Overcoming the Layering Habit in KBe2BO3F2 for the Next‐Generation Deep‐Ultraviolet Nonlinear Optical Materials

    Angewandte Chemie · 2018-05-12

    Guang Peng, Ning Ye, Zheshuai Lin, Lei Kang, Shilie Pan, Min Zhang, Chensheng Lin, Xifa Long, Min Luo, Yu Chen, Yu‐Huan Tang, Feng Xu, Tao Yan

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  21. Rb 3 VO(O 2 ) 2 CO 3 : A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response

    Angewandte Chemie International Edition · 2018-05-15

    Guohong Zou, Hongil Jo, Seong‐Ji Lim, Tae‐Soo You, Kang Min Ok

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  22. Rb3VO(O2)2CO3: A Four‐in‐One Carbonatoperoxovanadate Exhibiting an Extremely Strong Second‐Harmonic Generation Response

    Angewandte Chemie · 2018-05-15

    Guohong Zou, Hongil Jo, Seong‐Ji Lim, Tae‐Soo You, Kang Min Ok

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  23. Combination of d 10 -cations and fluorine anion as active participants to design novel borate/carbonate nonlinear optical materials

    Journal of Alloys and Compounds · 2018-05-18

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  24. Exploring Potential Beryllium-free, Deep-Ultraviolet Optical Crystals in the Rare Earth Fluoride Carbonate–Water System

    Crystal Growth & Design · 2018-05-20

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  25. Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects

    Journal of the American Chemical Society · 2018-05-21

    Min Luo, Fei Liang, Yunxia Song, Dan Zhao, Ning Ye, Zheshuai Lin

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  39. Why Some Noncentrosymmetric Borates Do Not Make Good Nonlinear Optical Materials: A Case Study with K3B5O8(OH)2

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  40. Near infrared broadband emission of a new bismuth-doped Gd0.1Y0.9AlO3 crystal

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  43. Metal-cation substitutions induced the enhancement of second harmonic generation in A 8 BS 6 (A = Cu, and Ag; B = Si, Ge, and Sn)

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