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RESEARCH PAPER · Angewandte Chemie International Edition · 2016

Pb2BO3Cl: A Tailor‐Made Polar Lead Borate Chloride with Very Strong Second Harmonic Generation

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Pb2BO3Cl: A Tailor‐Made Polar Lead Borate Chloride with Very Strong Second Harmonic GenerationOriginalChemInform Abstract: Pb2BO3Cl: A Tailor‐Made Polar Lead Borate Chloride with Very Strong Second Harmonic Generation.0A Polar Titanium–Organic Chain with a Very Large Second-Harmonic-Generation Response5Experimental and ab initio studies of Cd 5 (BO 3 ) 3 Cl: the first cadmium borate chlorine NLO material with isolated BO 3 groups21Explorations of new UV nonlinear optical materials in the Na 2 CO 3 –CaCO 3 system37Syntheses, crystal structures and characterization of three alkaline metal borates7The activity of lone pair contributing to SHG response in bismuth borates: a combination investigation from experiment and DFT calculation28The structural diversity of halogen-centered secondary building units: two new mixed-metal borate halides with deep-ultraviolet cut-off edges16Structural Modulation of Nitrate Group with Cations to Affect SHG Responses in RE(OH)2NO3 (RE = La, Y, and Gd): New Polar Materials with Large NLO Effect after Adjusting pH Values of Reaction Systems151M4Mg4(P2O7)3 (M = K, Rb): Structural Engineering of Pyrophosphates for Nonlinear Optical Applications238Synthesis, second-harmonic generations (SHG), and photoluminescence (PL) properties of Ca 4 Bi 6-x Ln x O 13 (Ln=La and Eu) solid solutions3Design and Synthesis of a Series of Novel Mixed Borate and Carbonate Halides21Two Barium Gold Iodates: Syntheses, Structures, and Properties of Polar BaAu(IO3)5 and Nonpolar HBa4Au(IO3)12 Materials5CsB 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 Units895Acentric La3(IO3)8(OH) and La(IO3)2(NO3): Partial Substitution of Iodate Anions in La(IO3)3 by Hydroxide or Nitrate Anion55K2[B3O3(OH)5]: A new deep-UV nonlinear optical crystal with isolated [B3O3(OH)5]2- anionic groups31Chemical Cosubstitution-Oriented Design of Rare-Earth Borates as Potential Ultraviolet Nonlinear Optical Materials267MBaYB 6 O 12 (M = Rb, Cs): two new rare-earth borates with large birefringence and short ultraviolet cutoff edges42Noncentrosymmetric Cubic Cyanurate K6Cd3(C3N3O3)4 Containing Isolated Planar π-Conjugated (C3N3O3)3– Groups59A beryllium-free deep-UV nonlinear optical material CsNaMgP 2 O 7 with honeycomb-like topological layers53Ba 3 B 10 O 17 Br 2 : a new barium borate halide with B–O layered structure4BaBOF 3 : a new aurivillius-like borate containing two types of F atoms32BaLiZn 3 (BO 3 ) 3 : a new member of the KBe 2 BO 3 F 2 family possessing dense BO 3 triangles and the smallest interlayer distance16Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties78Cs 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 block19Oxyhalides: prospecting ore for optical functional materials with large laser damage thresholds76PbTeGeO 6 : polar rosiaite-type germanate featuring a two dimensional layered structure24Perfect balance harmony in Ba 2 NO 3 (OH) 3 : a beryllium-free nitrate as a UV nonlinear optical material184RbSe 3 B 2 O 9 (OH) and CsSe 3 B 2 O 9 (OH): one dimensional boroselenite-based anionic frameworks with second harmonic generation properties15The first lead fluorooxoborate PbB 5 O 8 F: achieving the coexistence of large birefringence and deep-ultraviolet cut-off edge75The second-harmonic generation intensification derived from localization conjugated π-orbitals in O 2 2−39A Member of Fluorooxoborates: Li2Na0.9K0.1B5O8F2 with the Fundamental Building Block B5O10F2 and a Short Cutoff Edge27Cation‐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 Generation239Pb8M(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) Materials24Recent 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− groups195The relationship between covalent bonds and the optical response in a nonpolar family ATeMoO 6 (A=Mg, Zn, Cd): A Berry-phase investigation14Rb 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 Response42Strong SHG Response via High Orientation of Tetrahedral Functional Motifs in Polyselenide A2Ge4Se10 (A = Rb, Cs)31Li3.366Mg0.317B2O5: The first pyroborate in the Li2O-MgO-B2O3 system1Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects211From LiB3O5 to NaRbB6O9F2: Fluorine‐Directed Evolution of Structural Chemistry33Hydrogen Bonding Assisted Construction of Graphite-like Deep-UV Optical Materials with Two Types of Parallel π-Conjugated Units22Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Ba3Mg3(BO3)3F3 polymorphs with reversible phase transition and high performances as ultraviolet nonlinear optical materials470Second-order nonlinear optical crystals with mixed anions250Synthesis and Characterization of the First Tin Fluoride Borate Sn3[B3O7]F with Second Harmonic Generation Response28The First Examples of Lithium‐Containing Mixed‐Alkali Strontium Borates with Different Dimensional Anionic Architectures and Short Cutoff Edges16Two new mixed metal borates with the large birefringence in borates system confirmed by a disordered crystal optical calculation method6Synthesis, crystal structures and nonlinear optical properties of polymorphism: α- and β-RbHgI3·H2O18Centrosymmetric (NH4)2SbCl(SO4)2 and Non-centrosymmetric (NH4)SbCl2(SO4): Synergistic Effect of Hydrogen-Bonding Interactions and Lone-Pair Cations on the Framework Structures and Macroscopic Centricities89Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations11Na4Yb(CO3)3F: A New UV Nonlinear Optical Material with a Large Second Harmonic Generation Response8BaPO3Cl: a Metal Phosphate Chloride with Infinite [PO3]∞ Chains25Changes of optical transition models caused by crystal structural changes in CaSe2O50A new barium fluorooxoborate BaB 5 O 8 F· x H 2 O with large birefringence and a wide UV transparency window25A new ultraviolet transparent hydra-cyanurate K 2 (C 3 N 3 O 3 H) with strong optical anisotropy from delocalized π-bonds56An energy band engineering design to enlarge the band gap of KTiOPO 4 (KTP)-type sulfates via aliovalent substitution66Ba 3 B 10 O 17 F 2 ·0.1KF: the first mixed alkali/alkaline-earth metal fluorooxoborate with unprecedented double-layered B–O/F anionic arrangement17Ba 4 (BS 3 S) 2 S 4 : a new thioborate with unprecedented [BS 3 -S] and [S 4 ] fundamental building blocks19Centrosymmetric K 2 SO 4 ·(SbF 3 ) 2 and noncentrosymmetric Rb 2 SO 4 ·(SbF 3 ) 2 resulting from cooperative effects of lone pair and cation size63Exploration of the deep-ultraviolet nonlinear optical materials in the derivatives of KBe2BO3F27From centrosymmetric to noncentrosymmetric: cation-directed structural evolution in X 3 ZnB 5 O 10 (X = Na, K, Rb) and Cs 12 Zn 4 (B 5 O 10 ) 4 crystals26Functional layered materials with heavy metal lone pair cations, Pb 2+ , Bi 3+ , and Te 4+90Mg(H 2 O) 6 B 4 O 5 (OH) 4 (H 2 O) 3 : a new hydrated borate with a short DUV cutoff edge9Pb 10 O 4 (BO 3 ) 3 I 3 : a new noncentrosymmetric oxyborate iodide synthesized by the straightforward hydrothermal method6Rb 3 SbF 3 (NO 3 ) 3 : an excellent antimony nitrate nonlinear optical material with a strong second harmonic generation response fabricated by a rational multi-component design44Sr[B(OH) 4 ](IO 3 ) and Li 4 Sr 5 [B 12 O 22 (OH) 4 ](IO 3 ) 2 : two unprecedented metal borate-iodates showing a subtle balance of enlarged band gap and birefringence34Two alkali calcium borates exhibiting second harmonic generation and deep-UV cutoff edges3Two new tin( iv )-containing phosphate fluorides with two types of Sn( iv )–P–O–F frameworks and short cutoff edges0Y 8 O(OH) 15 (CO 3 ) 3 Cl: an excellent short-wave UV nonlinear optical material exhibiting an infrequent three-dimensional inorganic cationic framework61BeO6 Trigonal Prism with Ultralong Be–O Bonds Observed in a Deep Ultraviolet Optical Crystal Li13BeBe6B9O2712Ba4M(CO3)2(BO3)2 (M=Ba, Sr): two borate-carbonates synthesized by open high temperature solution method29Targeting the Next Generation of Deep-Ultraviolet Nonlinear Optical Materials: Expanding from Borates to Borate Fluorides to Fluorooxoborates450CsSbF 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 Structure432[Ge2S5(S2)]4−, A NLO‐Active Unit Leading to an Asymmetric Structure Discovered in Li2Cs4Ge2S5(S2)Cl2: An Experimental and Theoretical study18The first barium lead oxychloride Ba27Pb8O8Cl54 with new isolated [Pb4O4] clusters3Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)28BaB 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 Clusters2K9[B4O5(OH)4]3(CO3)X·7H2O (X = Cl, Br): Syntheses, Characterizations, and Theoretical Studies of Noncentrosymmetric Halogen Borate–Carbonates with Short UV Cutoff Edges16Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS229Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2186[Ln6O8] Cluster‐Encapsulating Polyplumbites as New Polyoxometalate Members and Record Inorganic Anion‐Exchange Materials for ReO4− Sequestration21β‐CsB9O14: A Triple‐Layered Borate with Edge‐Sharing BO4 Tetrahedra Exhibiting a Short Cutoff Edge and a Large Birefringence30Rb7SrY2(B5O10)3: A Rare-Earth Pentaborate with Moderate Second-Harmonic Response and Interesting Phase-Matching Behavior29Research and Development of Zincoborates: Crystal Growth, Structural Chemistry and Physicochemical Properties20Nontoxic 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 Tin255Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin33Cation Modulation on the Crystal Structure and Band Gap of Fluorooxoborates A3B3O3F6 (A = Alkali and Mixed Alkali Metal)17A high-pressure phase with a non-centrosymmetric crystal structure in the PbSe–PbBr2 system8Designing excellent mid-infrared nonlinear optical materials with fluorooxo-functional group of d0 transition metal oxyfluorides63CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153A new iodate-phosphate Pb 2 (IO 3 )(PO 4 ) achieving great improvement in birefringence activated by (IO 3 ) − groups53Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Al8(BO3)4(B2O5)F8: A F-Containing Aluminum Borate Featuring Two Types of Isolated B–O Groups12(NH 4 ) 3 [B(OH) 3 ] 2 (COOH) 3 : a graphite-like UV nonlinear optical material with a large birefringence via structural optimization31[O 2 Pb 3 ] 2 (BO 3 )I: a new lead borate iodide with 1∞[O 2 Pb 3 ] double chains6Ba 6 BO 3 Cl 9 and Pb 6 BO 4 Cl 7 : structural insights into ortho -borates with uncondensed BO 4 tetrahedra10Gd(NO 3 )(Se 2 O 5 )·3H 2 O: a nitrate–selenite nonlinear optical material with a short ultraviolet cutoff edge28Inorganic planar π-conjugated groups in nonlinear optical crystals: review and outlook145Large nonlinear optical effect in tungsten bronze structures via Li/Na cross-substitutions4Li 2 CdSiS 4 , a promising IR NLO material with a balanced E g and SHG response originating from the effect of Cd with d 10 configuration36Novel ultraviolet (UV) nonlinear optical (NLO) materials discovered by chemical substitution-oriented design302PbSrSiO 4 : a new ultraviolet nonlinear optical material with a strong second harmonic generation response and moderate birefringence37RbB 3 O 4 F 2 : a rubidium fluorooxoborate with an unprecedented [B 3 O 5 F 2 ] 3− functionalized unit and a large birefringence37Synthesis, characterization and crystal structure of a new mixed alkali and alkaline-earth metal borate Rb 9 Ba 24 (BO 3 ) 196Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51Ca 2 B 5 O 9 Cl and Sr 2 B 5 O 9 Cl: Nonlinear Optical Crystals with Deep-Ultraviolet Transparency Windows46A Promising Fluorooxoborate Framework with Flexibile Capability for Diverse Cations to Enhance the Second Harmonic Generation14Infrared Nonlinear Optical Polymorphs α- and β-SrCu 2 SnS 4 Exhibiting Large Second Harmonic Generation Responses with Requisite Phase-Matching Behavior44Noncentrosymmetric Fluorooxoborates A10B13O15F19 (A = K and Rb) with Unexpected [B10O12F13]7– Units and Deep-Ultraviolet Cutoff Edges26PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material120An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses224An Unprecedented Antimony(III) Borate with Strong Linear and Nonlinear Optical Responses42Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320Rational Design of the Nonlinear Optical Response in a Tin Iodate Fluoride Sn(IO3)2F290Designing 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 Materials55Strong Second Harmonic Generation in a Tungsten Bronze Oxide by Enhancing Local Structural Distortion48Aliovalent-substituted synthesis for a non-centrosymmetric phosphate with enhanced nonlinear-optical response5K4Sb(SO4)3Cl: The first apatite-type sulfate ultraviolet nonlinear optical material with sharply enlarged birefringence61A6Sb4F12(SO4)3 (A = Rb, Cs): Two Novel Antimony Fluoride Sulfates with Unique Crown-like Clusters50A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107Li4Ca2B8O16: A Borate with a Unique Fundamental Building Block and a Short Cutoff Edge14Two 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 Effect24Pb 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 Properties29Cs3B3O3F6 with a Deep-Ultraviolet Cutoff Edge and a Suitable Birefringence as the Potential Zero-Order Waveplate Material31Different mechanism of response of asymmetric lone pair electrons around ns2 cations to birefringence and second harmonic generation7Recent Advances in Oxide‐based Nonlinear Optical Materials with Wide Infrared Transparency Beyond 6 μm38Ba3(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 Research140Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups75

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  1. ChemInform Abstract: Pb2BO3Cl: A Tailor‐Made Polar Lead Borate Chloride with Very Strong Second Harmonic Generation.

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  2. A Polar Titanium–Organic Chain with a Very Large Second-Harmonic-Generation Response

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  3. Experimental and ab initio studies of Cd 5 (BO 3 ) 3 Cl: the first cadmium borate chlorine NLO material with isolated BO 3 groups

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  4. Explorations of new UV nonlinear optical materials in the Na 2 CO 3 –CaCO 3 system

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  5. Syntheses, crystal structures and characterization of three alkaline metal borates

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  6. The activity of lone pair contributing to SHG response in bismuth borates: a combination investigation from experiment and DFT calculation

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  7. The structural diversity of halogen-centered secondary building units: two new mixed-metal borate halides with deep-ultraviolet cut-off edges

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  8. Structural Modulation of Nitrate Group with Cations to Affect SHG Responses in RE(OH)2NO3 (RE = La, Y, and Gd): New Polar Materials with Large NLO Effect after Adjusting pH Values of Reaction Systems

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  9. M4Mg4(P2O7)3 (M = K, Rb): Structural Engineering of Pyrophosphates for Nonlinear Optical Applications

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  10. 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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  11. Design and Synthesis of a Series of Novel Mixed Borate and Carbonate Halides

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  12. Two Barium Gold Iodates: Syntheses, Structures, and Properties of Polar BaAu(IO3)5 and Nonpolar HBa4Au(IO3)12 Materials

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

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

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  15. Acentric La3(IO3)8(OH) and La(IO3)2(NO3): Partial Substitution of Iodate Anions in La(IO3)3 by Hydroxide or Nitrate Anion

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

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  17. Chemical Cosubstitution-Oriented Design of Rare-Earth Borates as Potential Ultraviolet Nonlinear Optical Materials

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  18. MBaYB 6 O 12 (M = Rb, Cs): two new rare-earth borates with large birefringence and short ultraviolet cutoff edges

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

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  20. A beryllium-free deep-UV nonlinear optical material CsNaMgP 2 O 7 with honeycomb-like topological layers

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

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  22. BaBOF 3 : a new aurivillius-like borate containing two types of F atoms

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  23. BaLiZn 3 (BO 3 ) 3 : a new member of the KBe 2 BO 3 F 2 family possessing dense BO 3 triangles and the smallest interlayer distance

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  24. Cation-tuned synthesis of the A 2 SO 4 ·SbF 3 (A = Na + , NH 4 + , K + , Rb + ) family with nonlinear optical properties

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

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  26. 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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  27. Oxyhalides: prospecting ore for optical functional materials with large laser damage thresholds

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  28. PbTeGeO 6 : polar rosiaite-type germanate featuring a two dimensional layered structure

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  29. Perfect balance harmony in Ba 2 NO 3 (OH) 3 : a beryllium-free nitrate as a UV nonlinear optical material

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  30. RbSe 3 B 2 O 9 (OH) and CsSe 3 B 2 O 9 (OH): one dimensional boroselenite-based anionic frameworks with second harmonic generation properties

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  31. The first lead fluorooxoborate PbB 5 O 8 F: achieving the coexistence of large birefringence and deep-ultraviolet cut-off edge

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  32. The second-harmonic generation intensification derived from localization conjugated π-orbitals in O 2 2−

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  33. A Member of Fluorooxoborates: Li2Na0.9K0.1B5O8F2 with the Fundamental Building Block B5O10F2 and a Short Cutoff Edge

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

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