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RESEARCH PAPER · Chemistry - A European Journal · 2018

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

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Deep‐Ultraviolet Nonlinear Optical Crystal Cs2Al2(B3O6)2O: A Benign Member of the Sr2Be2(BO3)2O Family with [Al2(B3O6)2O]2− Double LayersOriginalBaLiZn 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 distance16BaLiZn3B3O9: a Mixed‐Cation KBe2BO3F2‐Type Zinc‐Borate with a (LiZn3B3O9)∞ Network9Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations11RE(H 2 C 3 N 3 O 3 ) 2 ·(OH)· x H 2 O (RE = La, Y and Gd): potential UV birefringent materials with strong optical anisotropy originating from the (H 2 C 3 N 3 O 3 ) − group31Exploration of New Birefringent Crystals in Bismuth d0 Transition Metal Selenites35Research and Development of Zincoborates: Crystal Growth, Structural Chemistry and Physicochemical Properties20RbNa(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 material69CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Hydroisocyanurates X 2 Y(H 2 C 3 N 3 O 3 ) 4 ·4H 2 O (X = K, Cs; Y = Zn, Cd) with large birefringence stemming from π-conjugated (H 2 C 3 N 3 O 3 ) − anions28Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42Second-order nonlinear optical materials with a benzene-like conjugated π system49Two New Ferroborates with Three‐Dimensional Framework and Wide Transmittance Window2Crystal growth, characterization and theoretical studies of the noncentrosymmetric compound Al3(IO3)9·(HIO3)6·18H2O4Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41Zn(H 2 C 3 N 3 O 3 ) 2 ·3H 2 O: the first single- d 10 transition metal based ultraviolet hydroisocyanurate crystal with large birefringence18π‑Conjugated Trigonal Planar [C(NH2)3]+ Cationic Group: A Superior Functional Unit for Ultraviolet Nonlinear Optical Materials52From K[ZnBP2O8] to K[(Zn0.5Al0.5)2P2O8]: Substitution-Induced Microporous Zincoaluminophosphate with a Congruent-Melting Behavior5From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra10Na 3 AEZn 2 B 3 O 9 (AE = Mg, Ca): two new short-wave ultraviolet beryllium-free Sr 2 Be 2 B 2 O 7 -type zincoborates designed by chemical cosubstitution9Rb5Ba2(B10O17)2(BO2): The formation of unusual functional [BO2]− in borates with deep-ultraviolet transmission window62Deep-ultraviolet nonlinear optical crystals: concept development and materials discovery181NaZnAlP2O8: A New KZnBP2O8‐Type Congruent‐Melting Microporous Zincoaluminophosphate Accessed by Substitution Design Strategy and Molten Salt Method2Design of novel deep-UV nonlinear optical materials with one-dimensional functional module [BO2]∞ chain and fluorine-driven short phase-matching43Perfectly Encoding π‐Conjugated Anions in the RE5(C3N3O3)(OH)12 (RE=Y, Yb, Lu) Family with Strong Second Harmonic Generation Response and Balanced Birefringence91Perfectly Encoding π‐Conjugated Anions in the RE5(C3N3O3)(OH)12 (RE=Y, Yb, Lu) Family with Strong Second Harmonic Generation Response and Balanced Birefringence18CaBO2F: A novel deep-UV structural template with high nonlinear optical performance induced by electron delocalization25Aluminoborates as Nonlinear Optical Materials79Aluminoborates as Nonlinear Optical Materials14Recent advances on the synthesis of Sb(III)-based inorganic ultraviolet nonlinear optical materials47Recent progress in ultraviolet and deep-ultraviolet nonlinear optical aluminoborates17Structural Motif Cosubstitution Strategy for Designing Fluoroaluminoborate with the Sr2Be2B2O7-Type Double-Layered Structure14Cs 2 Mg(H 2 C 3 N 3 S 3 ) 4 ·8H 2 O: An Excellent Birefringent Material with Giant Optical Anisotropy in π-Conjugated Trithiocyanurate19Na4[B6O9 (OH)3](H2O) Cl: A Deep-Ultraviolet Transparent Nonlinear Optical Borate Chloride with {[B6O9 (OH)3]3–}∞ Chains5A deep-ultraviolet nonlinear-optical material with a wide bandgap and large static dielectric polarizability coefficient: Na 6 Si 3 F 181Alkali-metal isocyanurate Cs 3 (H 2 C 3 N 3 O 3 ) 3 (H 3 C 3 N 3 O 3 )·3H 2 O: synthesis and characterization0Ca 3 Al 2 B 8 O 18 : borate with a graphene-like layer featuring two types of topological six-membered rings induced by [AlO 4 ] units7CsAlB 3 O 6 Cl: the rational construction of a KBBF-type structure with aligned 2 ∞ [AlB 3 O 6 Cl] layers via introducing unprecedented [AlO 3 Cl] tetrahedra5Discovery of excellent ultraviolet nonlinear optical materials in chlorates and bromates with highly stereochemically active lone pairs12Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Hierarchical van der Waals Assemblies to Boost Deep‐Ultraviolet Nonlinear‐Optical Capabilities in Boron Phosphate8Toward the ultraviolet (UV) or deep-UV nonlinear optical crystals: The combination of π-conjugated planar [XY3] and tetrahedral [XY4]80A perspective on deep-ultraviolet nonlinear optical materials13Fluorine-driven materials design of novel deep-ultraviolet nonlinear optical crystal materials: Research progress and challenges6Exploiting Deep‐Ultraviolet Nonlinear Optical Material Rb 2 ScB 3 O 6 F 2 Originated from Congruously Oriented [B 3 O 6 ] Groups61Exploiting Deep‐Ultraviolet Nonlinear Optical Material Rb 2 ScB 3 O 6 F 2 Originated from Congruously Oriented [B 3 O 6 ] Groups4Chemical substitution towards a rare-earth borate ultraviolet NLO crystal exhibiting a strong SHG response17K 15 La 7 (BO 3 ) 12 : A KBBF-Like Nonlinear-Optical Material with a Short Cutoff Edge and a Strong Second-Harmonic-Generation Response10“Three functions in one”: multifunctional rare-earth cyamelurates with magnetism, luminescence, and giant optical nonlinearity6[C(NH 2 ) 3 ] 2 [C 2 H 5 (C 2 O 4 )]Cl: rational design of a metal-free UV birefringent crystal through the synergistic assembly of three distinct motifs5Ba 3 Al 2 B 12 O 24 : a beryllium-free member of the Sr 2 Be 2 B 2 O 7 family with a 2 ∞ [B 12 Al 2 O 28 ] double-layered structure4Coordinated assembly of alkali and alkaline earth metals with the perfluorinated [AlF 6 ] group to design deep-ultraviolet zero-order waveplate materials2LiBa 3 Al 2 B 3 O 11 : a deep-ultraviolet transparent optical borate featuring a 2D [Al 2 B 3 O 11 ] ∞ layered structure0层状结构深紫外非线性光学晶体研究进展(特邀)2A Promising Deep Ultraviolet Nonlinear Optical Crystal Activated by the Ordered Structure Design40A Promising Deep Ultraviolet Nonlinear Optical Crystal Activated by the Ordered Structure Design3Review of KBe2BO3F2-like second-order nonlinear optical materials and their structure-performance relationships13Modulation of Crystal Structure and Birefringence: Cation Size Effect in Alkali Metal Fluoroaluminoborates4Promising UV/DUV nonlinear optical materials with X-membered (X = multiples of 6) rings in anhydrous inorganic borates20Recent Progress in the Design and Synthesis of Nonlinear Optical Crystals with Stereochemically Active Lone Pairs8[C(NH2)3]Pb(C2O4)Cl·H2O: A halogen- and lone-pair-tuned UV crystal with large birefringence originated from cooperative π-conjugation6Sr2CdGe3O9: A Potential Zero-Order Waveplate Crystal Featuring an Enlarged Bandgap and Extended Mid-Infrared Transparency1Unlocking Advanced UV NLO Crystals in Rare‐Earth Metal Borate Fluorides via [B 3 O 6 ]‐Mediated Structural Modulation18The condensation of π-conjugated units: a new paradigm for designing high-performance optical crystals4Functional Unit Design of Deep‐UV NLO Crystals With Short Phase‐Matching and Large SHG Response22Toward the vacuum-ultraviolet frontier in nonlinear optical frequency conversion: phase-matching mechanisms across dimensions and architectures2Covalent Interlayer Engineering Enables Ideal Birefringence and Strong SHG in Beryllium‐Free Deep‐UV NLO Borates2Ce(2,2′-bipyridyl)3(SCN)3: Lanthanide Coordination- and Hydrogen-Bond-Directed Binary π-Conjugated Assemblies with Synergistic Large Birefringence and Broad Transparency0Luminescent materials based on aluminoborate compositions: a review0

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  1. 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

    New Journal of Chemistry · 2018-01-01

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  2. BaLiZn3B3O9: a Mixed‐Cation KBe2BO3F2‐Type Zinc‐Borate with a (LiZn3B3O9)∞ Network

    European Journal of Inorganic Chemistry · 2018-06-20

    Meihong Duan, Mingjun Xia, Rukang K. Li

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

    Chemistry - A European Journal · 2018-09-19

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  4. RE(H 2 C 3 N 3 O 3 ) 2 ·(OH)· x H 2 O (RE = La, Y and Gd): potential UV birefringent materials with strong optical anisotropy originating from the (H 2 C 3 N 3 O 3 ) − group

    Dalton Transactions · 2019-01-01

    Xia Hao, Min Luo, Chensheng Lin, Donghong Lin, Liling Cao, Ning Ye

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  5. Exploration of New Birefringent Crystals in Bismuth d0 Transition Metal Selenites

    Chemistry - A European Journal · 2019-01-13

    Ya-Ping Gong, Chun‐Li Hu, Fang Kong, Jiang‐Gao Mao

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  6. Research and Development of Zincoborates: Crystal Growth, Structural Chemistry and Physicochemical Properties

    Molecules · 2019-07-30

    Yanna Chen, Min Zhang, Miriding Mutailipu, Kenneth Reinhard Poeppelmeier, Shilie Pan

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  7. RbNa(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 material

    Inorganic Chemistry Frontiers · 2019-10-14

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  8. CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability

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  9. Emergent Deep‐Ultraviolet Nonlinear Optical Candidates

    Angewandte Chemie International Edition · 2019-12-10

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  10. Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich

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  11. Hydroisocyanurates X 2 Y(H 2 C 3 N 3 O 3 ) 4 ·4H 2 O (X = K, Cs; Y = Zn, Cd) with large birefringence stemming from π-conjugated (H 2 C 3 N 3 O 3 ) − anions

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  12. Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect

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  13. Second-order nonlinear optical materials with a benzene-like conjugated π system

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  14. Two New Ferroborates with Three‐Dimensional Framework and Wide Transmittance Window

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  15. Crystal growth, characterization and theoretical studies of the noncentrosymmetric compound Al3(IO3)9·(HIO3)6·18H2O

    Journal of Alloys and Compounds · 2020-12-08

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  16. Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials

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  17. Zn(H 2 C 3 N 3 O 3 ) 2 ·3H 2 O: the first single- d 10 transition metal based ultraviolet hydroisocyanurate crystal with large birefringence

    Dalton Transactions · 2021-01-01

    Dandan Wang, Xinyuan Zhang, Fei Liang, Zhanggui Hu, Yicheng Wu

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  18. π‑Conjugated Trigonal Planar [C(NH2)3]+ Cationic Group: A Superior Functional Unit for Ultraviolet Nonlinear Optical Materials

    ACS Omega · 2021-03-23

    Yunxia Song, Min Luo, Donghong Lin, Chensheng Lin, Zujian Wang, Xifa Long, Ning Ye

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  19. From K[ZnBP2O8] to K[(Zn0.5Al0.5)2P2O8]: Substitution-Induced Microporous Zincoaluminophosphate with a Congruent-Melting Behavior

    Inorganic Chemistry · 2021-06-01

    Meihong Duan, Bo Kong, Xu-Kui Yang, Yuxin Li, Peixin Ma, Xinyou An, Tixian Zeng, Da-Bin Qin, Zhi Gang Fang

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  20. From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra

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  21. Na 3 AEZn 2 B 3 O 9 (AE = Mg, Ca): two new short-wave ultraviolet beryllium-free Sr 2 Be 2 B 2 O 7 -type zincoborates designed by chemical cosubstitution

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  22. Rb5Ba2(B10O17)2(BO2): The formation of unusual functional [BO2]− in borates with deep-ultraviolet transmission window

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  23. Deep-ultraviolet nonlinear optical crystals: concept development and materials discovery

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  24. NaZnAlP2O8: A New KZnBP2O8‐Type Congruent‐Melting Microporous Zincoaluminophosphate Accessed by Substitution Design Strategy and Molten Salt Method

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  25. Design of novel deep-UV nonlinear optical materials with one-dimensional functional module [BO2]∞ chain and fluorine-driven short phase-matching

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  26. Perfectly Encoding π‐Conjugated Anions in the RE5(C3N3O3)(OH)12 (RE=Y, Yb, Lu) Family with Strong Second Harmonic Generation Response and Balanced Birefringence

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  28. CaBO2F: A novel deep-UV structural template with high nonlinear optical performance induced by electron delocalization

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  30. Aluminoborates as Nonlinear Optical Materials

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  31. Recent advances on the synthesis of Sb(III)-based inorganic ultraviolet nonlinear optical materials

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  32. Recent progress in ultraviolet and deep-ultraviolet nonlinear optical aluminoborates

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  33. Structural Motif Cosubstitution Strategy for Designing Fluoroaluminoborate with the Sr2Be2B2O7-Type Double-Layered Structure

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  34. Cs 2 Mg(H 2 C 3 N 3 S 3 ) 4 ·8H 2 O: An Excellent Birefringent Material with Giant Optical Anisotropy in π-Conjugated Trithiocyanurate

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  35. Na4[B6O9 (OH)3](H2O) Cl: A Deep-Ultraviolet Transparent Nonlinear Optical Borate Chloride with {[B6O9 (OH)3]3–}∞ Chains

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  36. A deep-ultraviolet nonlinear-optical material with a wide bandgap and large static dielectric polarizability coefficient: Na 6 Si 3 F 18

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  37. Alkali-metal isocyanurate Cs 3 (H 2 C 3 N 3 O 3 ) 3 (H 3 C 3 N 3 O 3 )·3H 2 O: synthesis and characterization

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  38. Ca 3 Al 2 B 8 O 18 : borate with a graphene-like layer featuring two types of topological six-membered rings induced by [AlO 4 ] units

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  39. CsAlB 3 O 6 Cl: the rational construction of a KBBF-type structure with aligned 2 ∞ [AlB 3 O 6 Cl] layers via introducing unprecedented [AlO 3 Cl] tetrahedra

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  40. Discovery of excellent ultraviolet nonlinear optical materials in chlorates and bromates with highly stereochemically active lone pairs

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  41. Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates

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  42. Hierarchical van der Waals Assemblies to Boost Deep‐Ultraviolet Nonlinear‐Optical Capabilities in Boron Phosphate

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  43. Toward the ultraviolet (UV) or deep-UV nonlinear optical crystals: The combination of π-conjugated planar [XY3] and tetrahedral [XY4]

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  44. A perspective on deep-ultraviolet nonlinear optical materials

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  45. Fluorine-driven materials design of novel deep-ultraviolet nonlinear optical crystal materials: Research progress and challenges

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  46. Exploiting Deep‐Ultraviolet Nonlinear Optical Material Rb 2 ScB 3 O 6 F 2 Originated from Congruously Oriented [B 3 O 6 ] Groups

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  47. Exploiting Deep‐Ultraviolet Nonlinear Optical Material Rb 2 ScB 3 O 6 F 2 Originated from Congruously Oriented [B 3 O 6 ] Groups

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  48. Chemical substitution towards a rare-earth borate ultraviolet NLO crystal exhibiting a strong SHG response

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  49. K 15 La 7 (BO 3 ) 12 : A KBBF-Like Nonlinear-Optical Material with a Short Cutoff Edge and a Strong Second-Harmonic-Generation Response

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  50. “Three functions in one”: multifunctional rare-earth cyamelurates with magnetism, luminescence, and giant optical nonlinearity

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