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RESEARCH PAPER · Angewandte Chemie International Edition · 2019

CsSbF2SO4: An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO4 (KTP)‐type Structure

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CsSbF2SO4: An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO4 (KTP)‐type StructureOriginalA 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 materials98An 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 arrangement17Centrosymmetric 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 size63Hybridization-activated new deep ultraviolet transparent nonlinear optical material Ba 11 [Al(PO 4 ) 4 ](P 2 O 7 )(PO 4 ) 3 with balanced overall performance and parsimony-forbidden structure23K 2 SrP 4 O 12 : a deep-UV transparent cyclophosphate as a nonlinear optical crystal79LiMg(IO 3 ) 3 : an excellent SHG material designed by single-site aliovalent substitution68LiO 4 tetrahedra lock the alignment of π-conjugated layers to maximize optical anisotropy in metal hydroisocyanurates44Rb 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 design44Tb(HSO 4 )(SO 4 ) – a green emitting hydrogensulfate sulfate with second harmonic generation response21Two low-dimensional metal halides: ionothermal synthesis, photoluminescence, and nonlinear optical properties19Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)28Deep-Ultraviolet Mixed-Alkali-Metal Borates with Induced Enlarged Birefringence Derived from the Structure Rearrangement of the LiB3O545LiGaP 2 O 7 : A Potential UV Nonlinear-Optical Crystal14Dislocations 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 AgGaS2186Prediction 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 Layers24Centrosymmetric Rb2Mg3(SO4)4 and non-centrosymmetric Cs2Mg3(SO4)4 with a phase-matching nonlinear optical response35Two 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)33Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra73Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra18Nontoxic KBBF Family Member Zn2BO3(OH): Balance between Beneficial Layered Structure and Layer Tendency81Cation Modulation on the Crystal Structure and Band Gap of Fluorooxoborates A3B3O3F6 (A = Alkali and Mixed Alkali Metal)17LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO398LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO337[NH4]12[(MoO2)2O(HPO4)2]4[PO4]Cl·0.5H2O: A mixed phosphomolybdate with nonlinear optical properties4Histidinium‐Driven Chirality Control of Self‐Assembled Hybrid Molybdenum Oxyfluorides24RbNa(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 material69Ag4Hg(SeO3)2(SeO4): a novel SHG material created in mixed valent selenium oxides by in situ synthesis36KMg(H 2 O)PO 4 : A Deep-Ultraviolet Transparent Nonlinear Optical Material Derived from KTiOPO 483A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48Synthesis, structure, and third-harmonic generation measurements of a mixed alkali metal iodate, KLi2(IO3)323“Old dog, new tricks”: the lone pair effect inducing divergent optical responses in lead cyanurates containing π-bonds18Alkali-earth metal lead( ii ) oxyhalide Ba 27 Pb 8 O 8 Cl 54 exhibiting interesting [Pb 4 Ba 4 O 4 ] 8+ species8(NH 4 ) 3 [B(OH) 3 ] 2 (COOH) 3 : a graphite-like UV nonlinear optical material with a large birefringence via structural optimization31Ba(B 2 OF 3 (OH) 2 ) 2 with well-ordered OH/F anions and a unique B 2 OF 3 (OH) 2 dimer30Influence of structure-directing polyhedra and heterocyclic ligands on the chain structures and O/F ordering in a series of zinc vanadium oxyfluorides1M 4 LiBe 4 P 7 O 24 and M 4 Li(Li 3 P)P 7 O 24 (M = Cs, Rb): deep-ultraviolet nonlinear-optical phosphates with a tetrahedra-substituted paracelsian-like framework9Multifunctional Zn( ii )–Yb( iii ) complex enantiomers showing second-harmonic generation, near-infrared luminescence, single-molecule magnet behaviour and proton conduction70Novel ultraviolet (UV) nonlinear optical (NLO) materials discovered by chemical substitution-oriented design302Optimal arrangement of π-conjugated anionic groups in hydro-isocyanurates leads to large optical anisotropy and second-harmonic generation effect42Structural phase transitions coupled with prominent dielectric anomalies and dielectric relaxation in [(CH 3 ) 3 NH] 2 [KCo(CN) 6 ] and mixed [(CH 3 ) 3 NH] 2 [KFe x Co 1−x (CN) 6 ] double perovskite hybrids16Three non-centrosymmetric bismuth phosphates, Li 2 ABi(PO 4 ) 2 (A = K, Rb, and Cs): effects of cations on the crystal structure and SHG response23Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51Band-Gap Modulation of Nonlinear-Optical Fluorooxoborates by Controlling the F/B Ratios4CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework132CsVO2F(IO3): An Excellent SHG Material Featuring an Unprecedented 3D [VO2F(IO3)]− Anionic Framework22Noncentrosymmetric Fluorooxoborates A10B13O15F19 (A = K and Rb) with Unexpected [B10O12F13]7– Units and Deep-Ultraviolet Cutoff Edges26A Series of Chalcogenide Borates RE6Ta2MgQB8O26 (RE = Sm, Eu, Gd; Q = S, Se) Featuring a B4O10 Cluster33Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320Rational Design of the Nonlinear Optical Response in a Tin Iodate Fluoride Sn(IO3)2F290Molecular Construction from AgGaS 2 to CuZnPS 4 : Defect-Induced Second Harmonic Generation Enhancement and Cosubstitution-Driven Band Gap Enlargement96Lead 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 Materials55Unprecedented lattice volume expansion on doping stereochemically active Pb2+ into uniaxially strained structure of CaBa1−xPbxZn2Ga2O726Two New Ferroborates with Three‐Dimensional Framework and Wide Transmittance Window2Enhanced nonlinear optical functionality in birefringence and refractive index dispersion of the deep-ultraviolet fluorooxoborates123Synthesis, characterizations and theoretical analysis of a noncentrosymmetric sulfate8Dimensionality–Band Gap–Third-Harmonic Generation Property Relationship in Novel Main-Group Metal Iodates37Aliovalent-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 birefringence61KInSi1.32Sn0.68Se6: An Infrared Nonlinear Optical Material Containing Three Types of Tetrahedral Units19Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014BiGa(SeO3)3: A Phase Matchable SHG Material Achieved by Cation Substitution19Facile one-step synthesis of 3D hierarchical flower-like magnesium peroxide for efficient and fast removal of tetracycline from aqueous solution59A6Sb4F12(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 polymorphs107Rational 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 Materials29Inherent laws between tetrahedral arrangement pattern and optical performance in tetrahedron-based mid-infrared nonlinear optical materials130Second-order nonlinear optical-active selenide borate Zn8Se2(BO2)12: Experimental and theoretical analysis9K 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 Performance38The study of structure evolvement of KTiOPO4 family and their nonlinear optical properties98Salt-Inclusion Chalcogenide [Ba4Cl2][ZnGa4S10]: Rational Design of an IR Nonlinear Optical Material with Superior Comprehensive Performance Derived from AgGaS2134Enhanced Proton Conductivity by Aliovalent Substitution of Cadmium for Indium in Dimethylaminium-Templated Metal Anilicates29CsHgNO3Cl2: A New Nitrate UV Birefringent Material Exhibiting an Optimized Layered Structure49Pb 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 Properties29Anionic Aliovalent Substitution from Structure Models of ZnS: Novel Defect Diamond‐like Halopnictide Infrared Nonlinear Optical Materials with Wide Band Gaps and Large SHG Effects78Anionic Aliovalent Substitution from Structure Models of ZnS: Novel Defect Diamond‐like Halopnictide Infrared Nonlinear Optical Materials with Wide Band Gaps and Large SHG Effects19Recent 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 Evolution10A 3 BBi(P 2 O 7 ) 2 (A = Rb, Cs; B = Pb, Ba): Isovalent Cation Substitution to Sustain Large Second-Harmonic Generation Responses106From S–O–S to B–O–S to B–O–B Bridges: Ba[B(S2O7)2]2 as a Model System for the Structural Diversity in Borosulfate Chemistry28Cs 3 Pb 2 (CH 3 COO) 2 X 5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups75Cs3Pb2(CH3COO)2X5 (X=I, Br): Halides with Strong Second‐Harmonic Generation Response Induced by Acetate Groups22Y 2 (Te 4 O 10 )(SO 4 ): a new sulfate tellurite with a unique Te 4 O 10 polyanion and large birefringence36Ba(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 Response69Noncentrosymmetric K2Mn3(SO4)3F2·4H2O and Rb2Mn3(SO4)3F2·2H2O with pseudo-KTP structures29Sr[B2(SO4)3(S2O7)]: A Borosulfate with an Unprecedented Chain Structure Comprising Disulfate Groups18A new nonlinear optical sulfate of layered structure: Cs2Zn2(SO4)319An Antimony(III) Fluoride Oxalate with Large Birefringence45From silicates to oxonitridosilicates: improving optical anisotropy for phase-matching as ultraviolet nonlinear optical materials47Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”3Reply to the Correspondence on “K2Sb(P2O7)F: Cairo Pentagonal Layer with Bifunctional Genes Reveal Optical Performance”1Sn2B5O9Br as an Outstanding Bifunctional Material with Strong Second‐Harmonic Generation Effect and Large Birefringence84Sb6O7(SO4)2: A Promising Ultraviolet Nonlinear Optical Material with an Enhanced Second‐Harmonic‐Generation Response Activated by SbIII Lone‐Pair Stereoactivity62Ba 3 [Al(PO 4 ) 3 ]: rational design of a promising deep-UV transparent SHG crystal with balanced overall performance originating from the condensation of quartz-type [Al(PO 4 ) 4 ] 9− units16A melamine-based organic–inorganic hybrid material revealing excellent optical performance and moderate thermal stability75An antimony( iii ) borate with large birefringence exhibiting unwonted [B 5 O 11 ] fundamental building blocks and dimeric [Sb 2 O 6 ] clusters26Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering144Centrosymmetric RbSnF 2 NO 3 vs. noncentrosymmetric Rb 2 SbF 3 (NO 3 ) 254Deep-ultraviolet transparent alkali metal–rare earth metal sulfate NaY(SO 4 ) 2 ·H 2 O as a nonlinear optical crystal: synthesis and characterization28From BaCl 2 to Ba(NO 3 )Cl: significantly enhanced birefringence derived from π-conjugated [NO 3 ]14From Ce(IO 3 ) 4 to CeF 2 (IO 3 ) 2 : fluorinated homovalent substitution simultaneously enhances SHG response and bandgap for mid-infrared nonlinear optics26From 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)9In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 219Li 5 Cs(SO 4 ) 3 : a potential zero-order wave plate material with short deep-ultraviolet cutoff edge20Rb3In(SO4)3: a defluorinated mixed main-group metal sulfate for ultraviolet transparent nonlinear optical materials with a large optical band gap26Recent advances of oxyfluorides for nonlinear optical applications69The tin sulfates Sn(SO 4 ) 2 and Sn2(SO4)3: crystal structures, optical and thermal properties10Ba3Sb2(PO4)4 and Cd3Sb2(PO4)4(H2O)2: Two New Antimonous Phosphates with Distinct [Sb(PO4)2] Structure Types and Enhanced Birefringence37A comprehensive survey on nonlinear optical phosphates: Role of multicoordinate groups106Na 6 MQ 4 (M=Zn, Cd; Q=S, Se): Promising New Ternary Infrared Nonlinear Optical Materials24Halonitrides Zn 2 NX (X=Cl,Br): Novel Mid-Infrared Nonlinear Optical Materials30Second-order nonlinear optical and photoelectric properties of Zn4B6O12S20[C(NH2)3]3PO4·2H2O: A new metal-free ultraviolet nonlinear optical phosphate with large birefringence and second-harmonic generation response70Large Second-Harmonic Response and Giant Birefringence of CeF 2 (SO 4 ) Induced by Highly Polarizable Polyhedra248Second-order nonlinear optical property of the ultraviolet transparent alkali metal-rare earth metal carbonate Na3Y(CO3)3.3H2O5Bi2[B2(SeO3)6]: A Metal Boroselenite with a Unique Zero-Dimensional [B2(SeO3)6]6– Anionic Group and Large Birefringence31Titanium Iodates with a Second-Harmonic-Generation Response8Molecular Engineering toward an Enlarged Optical Band Gap in a Bismuth Sulfate via Homovalent Cation Substitution26UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate196UV Solar‐Blind‐Region Phase‐Matchable Optical Nonlinearity and Anisotropy in a π‐Conjugated Cation‐Containing Phosphate28Te(CS(NH2)2)4SO4·2H2O: A Three-in-One Semiorganic Nonlinear Optical Crystal with an Unusual Quadrilateral (TeS4)6– Chromophore14α-Ca2CdP2 and β-Ca2CdP2: Two Polymorphic Phosphide-Based Infrared Nonlinear Crystals with Distorted NLO-Active Tetrahedral Motifs Realizing Large Second Harmonic Generation Effects and Suitable Band Gaps30Synthesis, Crystal Structures, and Thermal Analyses of Two New Antimony Tellurite Sulfates: [Sb2(TeO4)](SO4) and [Sb2(TeO3)2](SO4)10Tin Chloride Sulfates A3Sn2(SO4)3–xCl1+2x (A = K, Rb, Cs; x = 0, 1) as Multifunctional Optical Materials33Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response130Be2(BO3)(IO3): The First Anion‐mixed Van der Waals Member in the KBe2BO3F2 Family with a Very Strong Second Harmonic Generation Response8High-Performance Second-Harmonic-Generation (SHG) Materials: New Developments and New Strategies323Sr2Pb(BeB5O10)(BO3): An Excellent Ultraviolet Nonlinear-Optical Beryllium Borate by the Pb-Modified Construction of a Conjugated System and Lone-Pair Effect14KCs2[Pb2Br5(HCOO)2]: A Polar 3D Lead‐Bromide Framework Exhibiting Strong Second‐Harmonic Generation Response10[Ag(NH 3 ) 2 ] 2 SO 4 : A Strategy for the Coordination of Cationic Moieties to Design Nonlinear Optical Materials**6[Ag(NH3)2]2SO4: A Strategy for the Coordination of Cationic Moieties to Design Nonlinear Optical Materials**85Linear and Nonlinear Optical Properties of Centrosymmetric Sb 4 O 5 SO 4 and Noncentrosymmetric Sb 4 O 4 (SO 4 )(OH) 2 Induced by Lone Pair Stereoactivity55Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials28Noncentrosymmetric Rb3(COOH)3(H3BO3)2 vs Centrosymmetric Cs3(COOH)3(H3BO3)2142D van der Waals Layered [C(NH2)3]2SO3S Exhibits Desirable UV Nonlinear-Optical Trade-Off47Tourmaline with ultraviolet optical nonlinearity: Emergent material discovery from mineral5Achieving 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 Modification9

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  1. A 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 materials

    Journal of Materials Chemistry C · 2019-01-01

    Kaichuang Chen, Yi Jin Yang, Guang Peng, Shunda Yang, Tao Yan, Huixin Fan, Zheshuai Lin, Ning Ye

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  2. An energy band engineering design to enlarge the band gap of KTiOPO 4 (KTP)-type sulfates via aliovalent substitution

    Journal of Materials Chemistry C · 2019-01-01

    Fei Yang, Lijuan Huang, Lijuan Huang, Xiaoyu Zhao, Ling Huang, Ling Huang, Daojiang Gao, Jian Bi, Xin Wang, Guohong Zou

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  3. Ba 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 arrangement

    Chemical Communications · 2019-01-01

    Yahui Li, Hongwei Yu, Guopeng Han, Hao Li, Zhihua Yang, Shilie Pan

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  4. Centrosymmetric 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 size

    Inorganic Chemistry Frontiers · 2019-01-01

    Qian Wang, Lei Wang, Xiaoyu Zhao, Ling Huang, Daojiang Gao, Jian Bi, Xin Wang, Guohong Zou

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  5. Hybridization-activated new deep ultraviolet transparent nonlinear optical material Ba 11 [Al(PO 4 ) 4 ](P 2 O 7 )(PO 4 ) 3 with balanced overall performance and parsimony-forbidden structure

    Journal of Materials Chemistry C · 2019-01-01

    Zhi Gang Fang, Bing‐Ping Yang, Chun‐Li Hu, Jiang‐Gao Mao

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  6. K 2 SrP 4 O 12 : a deep-UV transparent cyclophosphate as a nonlinear optical crystal

    Chemical Communications · 2019-01-01

    Zhiyong Bai, Lehui Liu, Lizhen Zhang, Yisheng Huang, Feifei Yuan, Zhoubin Lin

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  7. LiMg(IO 3 ) 3 : an excellent SHG material designed by single-site aliovalent substitution

    Chemical Science · 2019-01-01

    Jin Chen, Chun‐Li Hu, Fei‐Fei Mao, Xiaohan Zhang, Bing‐Ping Yang, Jiang‐Gao Mao

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  8. LiO 4 tetrahedra lock the alignment of π-conjugated layers to maximize optical anisotropy in metal hydroisocyanurates

    Inorganic Chemistry Frontiers · 2019-01-01

    Xianghe Meng, Fei Liang, Jian Tang, Kaijin Kang, Wenlong Yin, Tixian Zeng, Bin Kang, Zheshuai Lin, Mingjun Xia

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  9. Rb 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 design

    Dalton Transactions · 2019-01-01

    Lei Wang, Fei Yang, Xiaoyu Zhao, Ling Huang, Daojiang Gao, Jian Bi, Xin Wang, Guohong Zou

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  10. Tb(HSO 4 )(SO 4 ) – a green emitting hydrogensulfate sulfate with second harmonic generation response

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  11. Two low-dimensional metal halides: ionothermal synthesis, photoluminescence, and nonlinear optical properties

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  12. Synthesis, characterization, and theoretical analysis of three new nonlinear optical materials K7MRE2B15O30 (M= Ca and Ba, RE= La and Bi)

    Science China Materials · 2019-03-22

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  13. Deep-Ultraviolet Mixed-Alkali-Metal Borates with Induced Enlarged Birefringence Derived from the Structure Rearrangement of the LiB3O5

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  14. LiGaP 2 O 7 : A Potential UV Nonlinear-Optical Crystal

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  15. Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2

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  16. Dislocations that Decrease Size Mismatch within the Lattice Leading to Ultrawide Band Gap, Large Second‐Order Susceptibility, and High Nonlinear Optical Performance of AgGaS2

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  17. Prediction 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 Layers

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  18. Prediction of Fluorooxoborates with Colossal Second Harmonic Generation (SHG) Coefficients and Extremely Wide Band Gaps: Towards Modulating Properties by Tuning the BO3/BO3F Ratio in Layers

    Angewandte Chemie · 2019-07-01

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  19. Centrosymmetric Rb2Mg3(SO4)4 and non-centrosymmetric Cs2Mg3(SO4)4 with a phase-matching nonlinear optical response

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  20. Two 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)

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  21. Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra

    Angewandte Chemie International Edition · 2019-08-26

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  22. Cs2Bi2O(Ge2O7) (CBGO): A Larger SHG Effect Induced by Synergistic Polarizations of BiO5 Polyhedra and GeO4 Tetrahedra

    Angewandte Chemie · 2019-08-29

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  23. Nontoxic KBBF Family Member Zn2BO3(OH): Balance between Beneficial Layered Structure and Layer Tendency

    Advanced Science · 2019-09-16

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  24. Cation Modulation on the Crystal Structure and Band Gap of Fluorooxoborates A3B3O3F6 (A = Alkali and Mixed Alkali Metal)

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  25. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  26. LiMII(IO3)3 (MII=Zn and Cd): Two Promising Nonlinear Optical Crystals Derived from a Tunable Structure Model of α‐LiIO3

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  27. [NH4]12[(MoO2)2O(HPO4)2]4[PO4]Cl·0.5H2O: A mixed phosphomolybdate with nonlinear optical properties

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