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RESEARCH PAPER · Angewandte Chemie International Edition · 2017

CsB4O6F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units

Xuefei Wang, Ying Wang, Bingbing Zhang, Fangfang Zhang, Zhihua Yang, Shilie Pan

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CsB4O6F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional UnitsOriginalThe First Alkaline‐Earth Fluorooxoborate Ba[B4O6F2]—Characterisation and Doping with Eu2+95Cs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response129Li 8 NaRb 3 (SO 4 ) 6 ·2H 2 O as a new sulfate deep-ultraviolet nonlinear optical material93Perfect balance harmony in Ba 2 NO 3 (OH) 3 : a beryllium-free nitrate as a UV nonlinear optical material184Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials191Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials714Functional Materials Design via Structural Regulation Originated from Ions Introduction: A Study Case in Cesium Iodate System90Non-Centrosymmetric RbNaMgP 2 O 7 with Unprecedented Thermo-Induced Enhancement of Second Harmonic Generation239Pushing Nonlinear Optical Oxides into the Mid-Infrared Spectral Region Beyond 10 μm: Design, Synthesis, and Characterization of La3SnGa5O14145SrB 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 Materials116Effect of Element Substitution on Structural Transformation and Optical Performances in I2BaMIVQ4 (I = Li, Na, Cu, and Ag; MIV = Si, Ge, and Sn; Q = S and Se)63Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials237A 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 Materials356CsSiB3O7: A Beryllium-Free Deep-Ultraviolet Nonlinear Optical Material Discovered by the Combination of Electron Diffraction and First-Principles Calculations58Deep‐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 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 Response207A Fluorooxosilicophosphate with an Unprecedented SiO2F4 Species56Assisting the Effective Design of Polar Iodates with Early Transition-Metal Oxide Fluoride Anions206Designing Deep‐UV Birefringent Crystals by Cation Regulation57Sn[B2O3F2]—The First Tin Fluorooxoborate as Possible NLO Material102Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates265Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials195A review on structure-performance relationship toward the optimal design of infrared nonlinear optical materials with balanced performances252Pb 2 GaF 2 (SeO 3 ) 2 Cl: Band Engineering Strategy by Aliovalent Substitution for Enlarging Bandgap while Keeping Strong Second Harmonic Generation Response178BaB8O12F2: a promising deep-UV birefringent material60Ba3(C3N3O3)2: A New Phase of Barium Cyanurate Containing Parallel π-Conjugated Groups as a Birefringent Material Replacement for Calcite62A 2 Bi 2 (SO 4 ) 2 Cl 4 (A = NH 4 , K, Rb): achieving a subtle balance of the large second harmonic generation effect and sufficient birefringence in sulfate nonlinear optical materials98A 2 SrM IV S 4 (A = Li, Na; M IV = Ge, Sn) concurrently exhibiting wide bandgaps and good nonlinear optical responses as new potential infrared nonlinear optical materials78A new ultraviolet transparent hydra-cyanurate K 2 (C 3 N 3 O 3 H) with strong optical anisotropy from delocalized π-bonds56Rational Design via Synergistic Combination Leads to an Outstanding Deep-Ultraviolet Birefringent Li2Na2B2O5 Material with an Unvalued B2O5 Functional Gene284Two Non-π-Conjugated Deep-UV Nonlinear Optical Sulfates268Targeting the Next Generation of Deep-Ultraviolet Nonlinear Optical Materials: Expanding from Borates to Borate Fluorides to Fluorooxoborates450Module-Analysis-Assisted Design of Deep Ultraviolet Fluorooxoborates with Extremely Large Gap and High Structural Stability109Cs3Na(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 Groups124Sr2LiScB4O10:Ce3+/Tb3+: A Green-Emitting Phosphor with High Energy Transfer Efficiency and Stability for LEDs and FEDs107Prediction 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 Layers99AHgSnQ4 (A = Sr, Ba; Q = S, Se): A Series of Hg-Based Infrared Nonlinear-Optical Materials with Strong Second-Harmonic-Generation Response and Good Phase Matchability76Agar and egg shell derived calcium carbonate and calcium hydroxide nanoparticles: Synthesis, characterization and applications61Nitrate nonlinear optical crystals: A survey on structure-performance relationships146How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates327Nontoxic KBBF Family Member Zn2BO3(OH): Balance between Beneficial Layered Structure and Layer Tendency81Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin255RbNa(HC 3 N 3 O 3 )·2H 2 O exhibiting a strong second harmonic generation response and large birefringence as a new potential UV nonlinear optical material69Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides63KMg(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 stability153Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Li2K4TiOGe4O12: A Stable Mid-Infrared Nonlinear Optical Material69A review of the AI2B II C IV DVI4 family as infrared nonlinear optical materials: the effect of each site on the structure and optical properties59Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material120An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses224BaF 2 TeF 2 (OH) 2 : A UV Nonlinear Optical Fluorotellurite Material Designed by Band-Gap Engineering157Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra147Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials164ZnIO3F: Zinc Iodate Fluoride with Large Birefringence and Wide Band Gap57Enhanced nonlinear optical functionality in birefringence and refractive index dispersion of the deep-ultraviolet fluorooxoborates123Designing a Deep-UV Nonlinear Optical Fluorooxosilicophosphate127A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107New Alkaline-Earth Metal Fluoroiodates Exhibiting Large Birefringence and Short Ultraviolet Cutoff Edge with Highly Polarizable (IO 3 F) 2– Units63Rational Design of the Metal‐Free KBe 2 BO 3 F 2 ⋅(KBBF) Family Member C(NH 2 ) 3 SO 3 F with Ultraviolet Optical Nonlinearity201Two Pyrophosphates with Large Birefringences and Second‐Harmonic Responses as Ultraviolet Nonlinear Optical Materials137Structure-property survey and computer-assisted screening of mid-infrared nonlinear optical chalcohalides113Realizing Deep-Ultraviolet Second Harmonic Generation by First-Principles-Guided Materials Exploration in Hydroxyborates111In Silico Modeling of New “Y-Series”-Based Near-Infrared Sensitive Non-Fullerene Acceptors for Efficient Organic Solar Cells134Finding Optimal Mid-Infrared Nonlinear Optical Materials in Germanates by First-Principles High-Throughput Screening and Experimental Verification79A 3 BBi(P 2 O 7 ) 2 (A = Rb, Cs; B = Pb, Ba): Isovalent Cation Substitution to Sustain Large Second-Harmonic Generation Responses106Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research140Two Mixed-Anion Units of [GeOSe3] and [GeO3S] Originating from Partial Isovalent Anion Substitution and Inducing Moderate Second Harmonic Generation Response and Large Birefringence55Ba(MoO 2 F) 2 (QO 3 ) 2 (Q = Se, Te): Partial Fluorination of MoO 6 Octahedra Enabling Two Polar Solids with Strong and Phase Matchable SHG Response69Giant 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 )57α‐SnF 2 : A UV Birefringent Material with Large Birefringence and Easy Crystal Growth210NaZnCO 3 (OH): A High-Performance Carbonate Ultraviolet Nonlinear Optical Crystal Derived from KBe 2 BO 3 F 2194Borates: A Rich Source for Optical Materials1089Sn2B5O9Br as an Outstanding Bifunctional Material with Strong Second‐Harmonic Generation Effect and Large Birefringence84A review on the recently developed promising infrared nonlinear optical materials103Recent advances of oxyfluorides for nonlinear optical applications69A comprehensive survey on nonlinear optical phosphates: Role of multicoordinate groups106M(NH 2 SO 3 ) 2 (M=Sr, Ba): Two Deep‐Ultraviolet Transparent Sulfamates Exhibiting Strong Second Harmonic Generation Responses and Moderate Birefringence142Theoretical Framework for Encapsulation of Inorganic B12N12 Nanoclusters with Alkaline Earth Metals for Efficient Hydrogen Adsorption: A Step Forward toward Hydrogen Storage Materials81A High Efficiency Trivalent Chromium-Doped Near-Infrared-Emitting Phosphor and Its NIR Spectroscopy Application166Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137LiZn(OH)CO3: A Deep‐Ultraviolet Nonlinear Optical Hydroxycarbonate Designed from a Diamond‐like Structure180Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application167AXHg3P2S8 (A = Rb, Cs; X = Cl, Br): New Excellent Infrared Nonlinear Optical Materials with Mixed‐Anion Chalcohalide Groups of Trigonal Planar [HgS2X]3− and Tetrahedral [HgS3X]5−58K5Mg2La3(BO3)6: An Efficient, Deep-Ultraviolet Nonlinear Optical Material70Fluorine‐Driven Enhancement of Birefringence in the Fluorooxosulfate: A Deep Evaluation from a Joint Experimental and Computational Study139LiB2O3F: A Beryllium-Free Deep-Ultraviolet Nonlinear Optical Material Designed Based on a Boron-Rich Strategy61Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals146Exploring Deep-UV Nonlinear Optical Materials with Enhanced Second Harmonic Generation Response and Birefringence in Fluoroaluminoborate Crystals69Li 4 MgGe 2 S 7 : The First Alkali and Alkaline‐Earth Diamond‐Like Infrared Nonlinear Optical Material with Exceptional Large Band Gap213A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation63Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**175Achieving Short‐Wavelength Phase‐Matching Second Harmonic Generation in Boron‐Rich Borosulfate with Planar [BO3] Units102La 3 Ga 3 Ge 2 S 3 O 10 : An Ultraviolet Nonlinear Optical Oxysulfide Designed by Anion‐Directed Band Gap Engineering63Strong SHG Responses in a Beryllium‐Free Deep‐UV‐Transparent Hydroxyborate via Covalent Bond Modification89Complex coordinated functional groups: A great genes for nonlinear optical materials64Na4B8O9F10: A Deep‐Ultraviolet Transparent Nonlinear Optical Fluorooxoborate with Unexpected Short Phase‐Matching Wavelength Induced by Optimized Chromatic Dispersion133Guanidinium Fluorooxoborates as Efficient Metal-free Short-Wavelength Nonlinear Optical Crystals140Ball milling induced strong polarization electric fields in Cu3B2O6 crystals for high efficiency piezocatalysis90Rational design of a promising oxychalcogenide infrared nonlinear optical crystal60Potential optical functional crystals with large birefringence: Recent advances and future prospects322Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra84Crystal‐Field Engineering Control of an Ultraviolet–Visible‐Responsive Near‐Infrared‐Emitting Phosphor and Its Applications in Plant Growth, Night Vision, and NIR Spectroscopy Detection123The Combination of Structure Prediction and Experiment for the Exploration of Alkali‐Earth Metal‐Contained Chalcopyrite‐Like IR Nonlinear Optical Material104Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species83Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters139Enhancement of Birefringence in Borophosphate Pushing Phase-Matching into the Short-Wavelength Region150All-small-molecule organic solar cells with high fill factor and enhanced open-circuit voltage with 18.25 % PCE: Physical insights from quantum chemical calculations78(NH4)3B11PO19F3: a deep-UV nonlinear optical crystal with unique [B5PO10F]∞ layers142Deep-ultraviolet nonlinear optical crystals: concept development and materials discovery181An excellent deep-ultraviolet birefringent material based on [BO2]∞ infinite chains185Achieving Large Second Harmonic Generation Effects via Optimal Planar Alignment of Triangular Units64Exploring Short-Wavelength Phase-Matching Nonlinear Optical Crystals by Employing KBe2BO3F2 as the Template95AIB3IIC3IIIQ8VI: A New Family for the Design of Infrared Nonlinear Optical Materials by Coupling Octahedra and Tetrahedra Units152Rb 2 CdSi 4 S 10 : novel [Si 4 S 10 ] T2-supertetrahedra-contained infrared nonlinear optical material with large band gap79Rb 3 B 11 P 2 O 23 : Materials Design of a New Chemically Benign Deep-Ultraviolet Nonlinear Optical Material58Aluminoborates as Nonlinear Optical Materials79Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181NaRb 6 (B 4 O 5 (OH) 4 ) 3 (BO 2 ) Featuring Noncentrosymmetry, Chirality, and the Linear Anionic Group BO 2 –100Recent Development of Sn II , Sb III ‐based Birefringent Material: Crystal Chemistry and Investigation of Birefringence130Target‐Driven Design of Deep‐UV Nonlinear Optical Materials via Interpretable Machine Learning125Birefringence Regulation by Clarifying the Relationship Between Stereochemically Active Lone Pairs and Optical Anisotropy in Tin‐based Ternary Halides56Cs 3 [(BOP) 2 (B 3 O 7 ) 3 ]: A Deep-Ultraviolet Nonlinear Optical Crystal Designed by Optimizing Matching of Cation and Anion Groups169Zn 2 HgP 2 S 8 : A Wide Bandgap Hg‐Based Infrared Nonlinear Optical Material with Large Second‐Harmonic Generation Response75Breaking the Inherent Interarrangement of [B3O6] Clusters for Nonlinear Optics with Orbital Hybridization Enhancement142Deep‐Ultraviolet Transparent Mixed Metal Sulfamates with Enhanced Nonlinear Optical Properties and Birefringence75Fluorination Strategy Towards Symmetry Breaking of Boron‐centered Tetrahedron for Poly‐fluorinated Optical Crystals70Fluorination strategy toward chemical and functional modification65Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Toward the ultraviolet (UV) or deep-UV nonlinear optical crystals: The combination of π-conjugated planar [XY3] and tetrahedral [XY4]80Covalently bonded fluorine optimizing deep-ultraviolet nonlinear optical performance of fluorooxoborates56Assembly of π‐Conjugated [B3O6] Units by Mer‐Isomer [YO3F3] Octahedra to Design a UV Nonlinear Optical Material, Cs2YB3O6F297Enhanced UV Nonlinear Optical Properties in Layered Germanous Phosphites through Functional Group Sequential Construction116Review on birefringence in borates based on birefringence-active functional groups and arrangements57Sulfate Derivatives with Heteroleptic Tetrahedra: New Deep‐Ultraviolet Birefringent Materials in which Weak Interactions Modulate Functional Module Ordering61Functional Modules Map of Unexplored Chemical Space: Guiding the Discovery of Giant Birefringent Materials76Exploiting Deep‐Ultraviolet Nonlinear Optical Material Rb 2 ScB 3 O 6 F 2 Originated from Congruously Oriented [B 3 O 6 ] Groups61Looking Back the Nonlinear Optical Crystals in a Functionalized Unit's Perspective109Vacuum ultraviolet second-harmonic generation in NH4B4O6F crystal73

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  33. K3B6O9F3: A New Fluorooxoborate with Four Different Anionic Units

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  34. 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

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

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  36. Effect of Element Substitution on Structural Transformation and Optical Performances in I2BaMIVQ4 (I = Li, Na, Cu, and Ag; MIV = Si, Ge, and Sn; Q = S and Se)

    Inorganic Chemistry · 2018-03-06

    Leyan Nian, Kui Wu, Guijie He, Zhihua Yang, Shilie Pan

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  37. 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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  38. 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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  39. A 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 Responses

    Chemistry of Materials · 2018-03-08

    Zhiqing Xie, Miriding Mutailipu, Guijie He, Guopeng Han, Ying Wang, Zhihua Yang, Min Zhang, Shilie Pan

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  40. M2B10O14F6 (M = Ca, Sr): Two Noncentrosymmetric Alkaline Earth Fluorooxoborates as Promising Next-Generation Deep-Ultraviolet Nonlinear Optical Materials

    Journal of the American Chemical Society · 2018-03-08

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

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  41. CsSiB3O7: A Beryllium-Free Deep-Ultraviolet Nonlinear Optical Material Discovered by the Combination of Electron Diffraction and First-Principles Calculations

    Chemistry of Materials · 2018-03-26

    Zhengyang Zhou, Yi Qiu, Fei Liang, Lukáš Palatinus, Morgane Poupon, Tao Yang, Rihong Cong, Zheshuai Lin, Junliang Sun

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  42. Crystal structures and theoretical studies of polyphosphate LiZnP3O9 for nonlinear optical applications

    Journal of Solid State Chemistry · 2018-03-29

    Zhiqing Xie, Xin Su, Hanqin Ding, Hongyi Li

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  43. 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

    Zhi Gang Fang, Xingxing Jiang, Meihong Duan, Zhanyu Hou, Changcheng Tang, Mingjun Xia, Lijuan Liu, Zheshuai Lin, Feidi Fan, Lei Bai, Chuangtian Chen

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

    Angewandte Chemie · 2018-04-17

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

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  46. 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

    Inorganic Chemistry · 2018-04-20

    Xianghe Meng, Fei Liang, Mingjun Xia, Zheshuai Lin

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  47. A strategy for optical properties investigation in ABe 2 BO 3 F 2 (A=K, Rb, Cs) using finite field methods

    Physica B Condensed Matter · 2018-04-26

    Hahaer Mushahali, Baoxia Mu, Qian Wang, Mamatrishat Mamat, Haibin Cao, Guang Yang, Qun Jing

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  48. Growth and characterization of nonlinear optical crystal Gamma glycine by the additive of lithium bromide

    Optics & Laser Technology · 2018-05-03

    M. Esthaku Peter, T. Gurumurthi, Zerihun Tadele, Bayou Aboye, Mubarik Awel Hussan

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  49. 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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  50. 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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