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RESEARCH PAPER · Angewandte Chemie · 2018

Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials

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Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical MaterialsOriginalCs 3 VO(O 2 ) 2 CO 3 : an exceptionally thermostable carbonatoperoxovanadate with an extremely large second-harmonic generation response129Synthesis, crystal structure and optical properties of a new fluorocarbonate with an interesting sandwich-like structure7Pb8M(BO3)6 (M = Mg, Ca): Two new borates with large birefringence activated by the ∞[Pb8B6O18]2- double layers6Pb2BO3I: 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 Optics67A strategy for optical properties investigation in ABe 2 BO 3 F 2 (A=K, Rb, Cs) using finite field methods12Li3.366Mg0.317B2O5: The first pyroborate in the Li2O-MgO-B2O3 system1Exploring Potential Beryllium-free, Deep-Ultraviolet Optical Crystals in the Rare Earth Fluoride Carbonate–Water System34MIMIIP3O9 (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 Species5Non-centrosymmetric BaNaP3O9 with a short deep-ultraviolet cutoff edge14Designing Deep‐UV Birefringent Crystals by Cation Regulation57Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates265Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102Cation substitution inducing gap changes and covalent interaction flexibility enhancing second harmonic generation responses in d10 metal chalcogenides11The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges16Intriguing Structural Transition Inducing Variable Birefringences in ABa2MS4Cl (A = Rb, Cs; M = Ge, Sn)32Synthesis, crystal structures and nonlinear optical properties of polymorphism: α- and β-RbHgI3·H2O18Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations11The linear and nonlinear optical response of CsGeX3 (X=Cl, Br, and I): The finite field and first-principles investigation26Ba 4 Bi 2 (Si 8−x B 4+x O 29 ) ( x = 0.09): a new acentric metal borosilicate as a promising nonlinear optical material53A 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 materials78Cs 2 CdV 2 O 6 Cl 2 and Cs 3 CdV 4 O 12 Br: two new non-centrosymmetric oxyhalides containing d 0 and d 10 cations and exhibiting second harmonic generation activity19Metal-cation substitutions induced the enhancement of second harmonic generation in A 8 BS 6 (A = Cu, and Ag; B = Si, Ge, and Sn)14RbSbSO 4 Cl 2 : an excellent sulfate nonlinear optical material generated due to the synergistic effect of three asymmetric chromophores79The first lithium difluorophosphate LiPO 2 F 2 with a neutral polytetrahedral microporous architecture35Theoretical investigation on the promotion of second harmonic generation from chalcopyrite family A I GaS 2 to A II Ga 2 S 47Y 8 O(OH) 15 (CO 3 ) 3 Cl: an excellent short-wave UV nonlinear optical material exhibiting an infrequent three-dimensional inorganic cationic framework61Ba4M(CO3)2(BO3)2 (M=Ba, Sr): two borate-carbonates synthesized by open high temperature solution method29Hierarchy in nonlinear optical responses induced by metal cation tailoring effect in the In-containing chalcogenide compounds4CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure87CsSbF2SO4: An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO4 (KTP)‐type Structure432RbB 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 Edge38Deep-Ultraviolet Mixed-Alkali-Metal Borates with Induced Enlarged Birefringence Derived from the Structure Rearrangement of the LiB3O545β‐CsB9O14: A Triple‐Layered Borate with Edge‐Sharing BO4 Tetrahedra Exhibiting a Short Cutoff Edge and a Large Birefringence30New Members of SHG Active Dugganite Family, A3BC3D2O14 (A = Ba, Pb; B = Te, Sb; C = Al, Ga, Fe, Zn; D = Si, Ge, P, V): Synthesis, Structure, and Materials Properties30Prediction 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 Layers24A new barium-containing alkali metal silicate fluoride NaBa3Si2O7F with deep-UV optical property12Experiment and First-Principles Calculations of A2Mg2TeB2O10 (A = Pb, Ba): Influences of the Cosubstitution on the Structure Transformation and Optical Properties21Agar and egg shell derived calcium carbonate and calcium hydroxide nanoparticles: Synthesis, characterization and applications61Lead titanate-induced abnormal ferroelectric/antiferroelectric phase transitions in Pb(Lu0.5Nb0.5)O3 solid solutions10Nontoxic KBBF Family Member Zn2BO3(OH): Balance between Beneficial Layered Structure and Layer Tendency81K5B19O31: 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 Tin33[NH4]12[(MoO2)2O(HPO4)2]4[PO4]Cl·0.5H2O: A mixed phosphomolybdate with nonlinear optical properties4Synthesis of Co3O4 Nano Aggregates by Co-precipitation Method and its Catalytic and Fuel Additive Applications79Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Rb3Na(H2C3N3O3)4·3H2O with Large Birefringence28Syntheses, characterization, and theoretical calculation of Rb2Mg3(P2O7)2 polymorphs with deep-ultraviolet cutoff edges18Prediction of ternary fluorooxoborates with coplanar triangular units [BO x F 3−x ] x− from first-principles13Second-order nonlinear optical materials with a benzene-like conjugated π system49Tellurium–oxygen group enhanced birefringence in tellurium phosphates: a first-principles investigation4Three non-centrosymmetric bismuth phosphates, Li 2 ABi(PO 4 ) 2 (A = K, Rb, and Cs): effects of cations on the crystal structure and SHG response23A Promising Fluorooxoborate Framework with Flexibile Capability for Diverse Cations to Enhance the Second Harmonic Generation14Designing 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 Materials55Enhanced nonlinear optical functionality in birefringence and refractive index dispersion of the deep-ultraviolet fluorooxoborates123Controllable synthesis and spontaneous phase transition of photonic coordination polymer to produce a strong second-harmonic generation response25K4Sb(SO4)3Cl: The first apatite-type sulfate ultraviolet nonlinear optical material with sharply enlarged birefringence61Synthesis, crystal structures and optical properties of open-framework gallium phosphates: NaGa3F4(PO4)2(H2O)2 and AGa2P2O7(OH)3(H2O) (A = K, Rb)1Syntheses, characterization and calculations of LimAnM6O15 (A=Rb, Cs; M=Si, Ge; m+n=6)18Deep-ultraviolet nonlinear optical crystals by design: A computer-aided modeling blueprint from first principles45Two 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 Anisotropy47Synthesis of monetite micro particles from egg shell waste and study of its environmental applications: Fuel additive and catalyst11K 2 Sb(P 2 O 7 )F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance297K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance38Sr5[BO2(OH)]3(OH)3F: First hydroxyborate fluoride with the [BO2(OH)]2− unit2Pb 18 O 8 Cl 15 I 5 : A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties165Pb18O8Cl15I5: A Polar Lead Mixed Oxyhalide with Unprecedented Architecture and Excellent Infrared Nonlinear Optical Properties29In Silico Modeling of New “Y-Series”-Based Near-Infrared Sensitive Non-Fullerene Acceptors for Efficient Organic Solar Cells134Recent 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 Evolution10Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research19Series of Crystals with Giant Optical Anisotropy: A Targeted Strategic Research140Y 2 (Te 4 O 10 )(SO 4 ): a new sulfate tellurite with a unique Te 4 O 10 polyanion and large birefringence36KSnI 3 ⋅ H 2 O: A New Compound with One‐Dimensional SnI 3 Chains of Pyramidal SnI 5 Polyhedra2Ba 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 -borate34Barium fluoroiodate crystals with a large band gap and birefringence22Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2From BaCl 2 to Ba(NO 3 )Cl: significantly enhanced birefringence derived from π-conjugated [NO 3 ]14From 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)9RbMo 2 P 3 O 14 with large birefringence mainly induced by highly distorted [MoO 6 ] in uncommon [Mo 2 P 3 O 14 ] ∞ layers9Recent advances of oxyfluorides for nonlinear optical applications69SrTi(IO 3 ) 6 ·2H 2 O and SrSn(IO 3 ) 6 : distinct arrangements of lone pair electrons leading to large birefringences11The Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal0To improve the key properties of nonlinear optical crystals assembled with tetrahedral functional building units46Two deep-ultraviolet nonlinear optical monolayers obtained by a template-optimized design strategy2Ultraviolet nonlinear optical crystals A 3 SrBi(P 2 O 7 ) 2 (A = K, Rb) with large second harmonic generation responses15New Polymorphism for Ba3Zn2(BO3)3F with Two Polymorphs Exhibiting Anomalous Phase Transition2Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials24Prediction 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 Performance6RbMT3(BO3)2O3 (M=Ba, Sr; T=Al, Ga): New Double‐Layered Oxyborates Constructed from [BO3] Triangles and [TO4] Tetrahedra13Vibrational and optical studies of a nonlinear optical crystal, Cs2Bi2O(Ge2O7)3Cs4B4O3F10: 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 Substitution33Fluorine‐Driven Enhancement of Birefringence in the Fluorooxosulfate: A Deep Evaluation from a Joint Experimental and Computational Study139Na2Rb2SrB18O30 with [B9O19]11− fundamental building block consisting of three [B3O7]5− groups5BaYOBO3: A deep-ultraviolet rare-earth oxy-borate with a large second harmonic generation response45The First Mixed Calcium Zinc Borate with a Flexible [B8O17] Fundamental Building Block and Short UV Cutoff Edge7Heterobimetallic Cluster‐Based Coordination Polymers: Assembly, Structures and Third‐Order Nonlinear Optical Properties4NaRbB3O4F3: 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 Phosphate22Tetragonal Silicene and Germanene Quantum Dots: Candidates for Enhanced Nonlinear Optical and Photocatalytic Activity26La 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 Engineering18An Overview on Recent Trends in Deep‐Ultraviolet (DUV) and Ultraviolet (UV) Nonlinear Optical Crystals25Syntheses, Structures and Properties of Alkali and Alkaline Earth Metal Diamond-Like Compounds Li2MgMSe4 (M = Ge, Sn)12A New Nonlinear Optical Material with N(CN)2− Anion2A first-principle investigate about the different response of birefringence and SHG from AB3O6 (A = Bi, Sb) compounds5From 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 substitution11Na4B8O9F10: 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)6KF·B(OH) 3 : a KBBF-type material with large birefringence and remarkable deep-ultraviolet transparency33Large optical anisotropy-oriented construction of a carbonate-nitrate chloride compound as a potential ultraviolet birefringent material44Linear unit BN 2 : a novel birefringence-enhanced fundamental module with sp orbital hybridization9Mg(H 2 O) 6 [(IO 2 (OH)) 2 (IO 3 )] 2 : a new iodate with a very large band gap and optical anisotropy13Rational design of a promising oxychalcogenide infrared nonlinear optical crystal60Unprecedented mid-infrared nonlinear optical materials achieved by crystal structure engineering, a case study of (KX)P 2 S 6 (X = Sb, Bi, Ba)59Sulfamide: 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] Tetrahedra84Rb5Ba2(B10O17)2(BO2): The formation of unusual functional [BO2]− in borates with deep-ultraviolet transmission window62Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal9The 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 Species6Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species83A 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] Clusters139(NH4)3B11PO19F3: a deep-UV nonlinear optical crystal with unique [B5PO10F]∞ layers142From CsKTaF7 to CsNaTaF7: Alkali Metal Cations Regulation to Generate SHG Activity**22

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

    Chemical Science · 2018-01-01

    Guohong Zou, Zhien Lin, Hongmei Zeng, Hongil Jo, Seong‐Ji Lim, Tae‐Soo You, Kang Min Ok

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  2. Synthesis, crystal structure and optical properties of a new fluorocarbonate with an interesting sandwich-like structure

    Dalton Transactions · 2018-01-01

    Changcheng Tang, Xingxing Jiang, Shu Hai Guo, Mingjun Xia, Lijuan Liu, Xiaoyang Wang, Zheshuai Lin, Chuangtian Chen

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  3. 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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  4. 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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  5. Pb2BO3I: A Borate Iodide with the Largest Second‐Harmonic Generation (SHG) Response in the KBe2BO3F2 (KBBF) Family of Nonlinear Optical (NLO) Materials

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  6. Ba4B8TeO19: A UV Nonlinear Optical Material

    Inorganic Chemistry · 2018-04-03

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

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

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

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

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  12. Li3.366Mg0.317B2O5: The first pyroborate in the Li2O-MgO-B2O3 system

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

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    Qian Wang, Fangfang He, Ling Huang, Daojiang Gao, Jian Bi, Guohong Zou

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  14. 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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  15. From LiB3O5 to NaRbB6O9F2: Fluorine‐Directed Evolution of Structural Chemistry

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  16. A Fluorooxosilicophosphate with an Unprecedented SiO2F4 Species

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  17. A Fluorooxosilicophosphate with an Unprecedented SiO2F4 Species

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  18. Non-centrosymmetric BaNaP3O9 with a short deep-ultraviolet cutoff edge

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  19. Designing Deep‐UV Birefringent Crystals by Cation Regulation

    Chemistry - A European Journal · 2018-06-25

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  20. Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates

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  21. Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials

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  22. Cation substitution inducing gap changes and covalent interaction flexibility enhancing second harmonic generation responses in d10 metal chalcogenides

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  23. The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges

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  24. Intriguing Structural Transition Inducing Variable Birefringences in ABa2MS4Cl (A = Rb, Cs; M = Ge, Sn)

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  25. Synthesis, crystal structures and nonlinear optical properties of polymorphism: α- and β-RbHgI3·H2O

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  26. Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations

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  27. The linear and nonlinear optical response of CsGeX3 (X=Cl, Br, and I): The finite field and first-principles investigation

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  28. Ba 4 Bi 2 (Si 8−x B 4+x O 29 ) ( x = 0.09): a new acentric metal borosilicate as a promising nonlinear optical material

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  29. A 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 materials

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  30. Cs 2 CdV 2 O 6 Cl 2 and Cs 3 CdV 4 O 12 Br: two new non-centrosymmetric oxyhalides containing d 0 and d 10 cations and exhibiting second harmonic generation activity

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

    New Journal of Chemistry · 2019-01-01

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  32. RbSbSO 4 Cl 2 : an excellent sulfate nonlinear optical material generated due to the synergistic effect of three asymmetric chromophores

    Journal of Materials Chemistry C · 2019-01-01

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  33. The first lithium difluorophosphate LiPO 2 F 2 with a neutral polytetrahedral microporous architecture

    Chemical Communications · 2019-01-01

    Guopeng Han, Ying Wang, Hao Li, Zhihua Yang, Shilie Pan

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  34. Theoretical investigation on the promotion of second harmonic generation from chalcopyrite family A I GaS 2 to A II Ga 2 S 4

    RSC Advances · 2019-01-01

    Alimujiang Yalikun, Ming‐Hsien Lee, Mamatrishat Mamat

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