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RESEARCH PAPER · Journal of the American Chemical Society · 2018

Pb 2 GaF 2 (SeO 3 ) 2 Cl: Band Engineering Strategy by Aliovalent Substitution for Enlarging Bandgap while Keeping Strong Second Harmonic Generation Response

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Pb 2 GaF 2 (SeO 3 ) 2 Cl: Band Engineering Strategy by Aliovalent Substitution for Enlarging Bandgap while Keeping Strong Second Harmonic Generation ResponseOriginal“Two in one”: an unprecedented mixed anion, Ba 2 (C 3 N 3 O 3 )(CNO), with the coexistence of isolated sp and sp 2 π-conjugated groups15A rich structural chemistry in π-conjugated hydroisocyanurates: layered structures of A 2 B(H 2 C 3 N 3 O 3 ) 4 · n H 2 O (A = K, Rb, Cs; B = Mg, Ca; n = 4, 10) with high ultraviolet transparency and strong optical anisotropy47Adjustable optical nonlinearity in d 10 cations containing chalcogenides via dp hybridization interaction13Ag 7 TaSe 6 : a new noncentrosymmetric selenide with fascinating “three in one” coordination modes and a strong second harmonic generation response13An energy band engineering design to enlarge the band gap of KTiOPO 4 (KTP)-type sulfates via aliovalent substitution66Cs 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 activity19From 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 crystals26LiMg(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 hydroisocyanurates44M 2 (SeO 3 )F 2 (M = Zn, Cd): understanding the structure directing effect of [SeO 3 ] 2− groups on constructing ordered oxyfluorides14Pb 2 Cd(SeO 3 ) 2 X 2 (X = Cl and Br): two halogenated selenites with phase matchable second harmonic generation27Pb 7 F 12 Cl 2 : a promising infrared nonlinear optical material with high laser damage threshold19Synthesis and structure of a new mixed metal iodate Ba 3 Ga 2 (IO 3 ) 1217Exploration of New Birefringent Crystals in Bismuth d0 Transition Metal Selenites35CsSbF 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 Structure432Cs3Na(H2C3N3O3)4·3H2O: A Mixed Alkali‐Metal Hydroisocyanurate Nonlinear Optical Material Containing π‐Conjugated Six‐Membered‐Ring Units68LiGaP 2 O 7 : A Potential UV Nonlinear-Optical Crystal14Variable Chains Found in Mixed Transition Metal Oxyfluorides with Heterocyclic Ligands9KBiCl2SO4: The First Bismuth Chloride Sulfate Being Second-Order Nonlinear Optical Active44New 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 Properties30Ba2M(C3N3O3)2 (M = Sr, Pb): Band Engineering from p−π Interaction via Homovalent Substitution in Metal Cyanurates Containing Planar π-Conjugated Groups39Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups45Partial Congener Substitution Induced Centrosymmetric to Noncentrosymmetric Transformation Witnessed by K3Ga3(Ge7–xMx)Se20 (M = Si, Sn) and Their Nonlinear Optical Properties51A x Ce 9 (IO 3 ) 36 (A = K, La): the effects of a change in the intermediate valence on the second-harmonic generation response7Ag4Hg(SeO3)2(SeO4): a novel SHG material created in mixed valent selenium oxides by in situ synthesis36First-Principles Design and Simulations Promote the Development of Nonlinear Optical Crystals299K5(W3O9F4)(IO3): An Efficient Mid-Infrared Nonlinear Optical Compound with High Laser Damage Threshold114A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48“Old dog, new tricks”: the lone pair effect inducing divergent optical responses in lead cyanurates containing π-bonds18Li2K4TiOGe4O12: A Stable Mid-Infrared Nonlinear Optical Material69Gd(NO 3 )(Se 2 O 5 )·3H 2 O: a nitrate–selenite nonlinear optical material with a short ultraviolet cutoff edge28Hexagonal tungsten oxides with large bandgaps synthesized by a chemical substitution method31In[Ba 3 Cl 3 F 6 ]: a novel infrared-transparent molecular sieve constructed by halides6Recent progress in selenite and tellurite based SHG materials32Selenite bromide nonlinear optical materials Pb 2 GaF 2 (SeO 3 ) 2 Br and Pb 2 NbO 2 (SeO 3 ) 2 Br: synthesis and characterization20Two-stage evolution from phosphate to sulfate of new KTP-type family members as UV nonlinear optical materials through chemical cosubstitution-oriented design51PbB5O7F3: A High-Performing Short-Wavelength Nonlinear Optical Material120A Series of Chalcogenide Borates RE6Ta2MgQB8O26 (RE = Sm, Eu, Gd; Q = S, Se) Featuring a B4O10 Cluster33MII2M3IIIF3(Te6F2O16) (MII = Pb, Ba; MIII = Al, Ga): New mixed anionic tellurites with isolated Te6 coplanar rings23Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra147Designing Silicates as Deep‐UV Nonlinear Optical (NLO) Materials using Edge‐Sharing Tetrahedra43Enhancement of Second-Order Optical Nonlinearity in a Lutetium Selenite by Monodentate Anion Partial Substitution58BiGa(SeO3)3: A Phase Matchable SHG Material Achieved by Cation Substitution19A6Sb4F12(SO4)3 (A = Rb, Cs): Two Novel Antimony Fluoride Sulfates with Unique Crown-like Clusters50AGa 3 F 6 (SeO 3 ) 2 (A = Rb, Cs): A New Type of Phase-Matchable Hexagonal Tungsten Oxide Material with Strong Second-Harmonic Generation Responses63LiGaF2(IO3)2: A mixed-metal gallium iodate-fluoride with large birefringence and wide band gap39Ba2[MoO3(OH)(IO3)2]IO3: A Promising SHG Material Featuring a Λ-Shaped Functional Motif Achieved by Universal Mono-Site Substitution50A 2 Bi 2 (SeO 3 ) 3 F 2 (A = K and Rb): Excellent Mid-Infrared Nonlinear Optical Materials with Both Strong SHG Responses and Large Band Gaps64Y 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 Response69Nonlinear optical effects in two mercury cyanamide/guanidinium chlorides Hg 3 (NCN) 2 Cl 2 and Hg 2 (C(NH 2 ) 3 )Cl 57Recent Achievements in Lone-Pair Cation-Based Infrared Second-Order Nonlinear Optical Materials95Hydrogen-Bond-Assisted Alignment of [MCu(SeO 3 ) 4 Cl(H 2 O)] 4– (M = Fe, Ga) Anionic Layers to Form Two Polar Oxychlorides: Pb 2 MCu(SeO 3 ) 4 Cl(H 2 O)10[GaF(H 2 O)][IO 3 F]: a promising NLO material obtained by anisotropic polycation substitution42AgBi(SO 4 )(IO 3 ) 2 : aliovalent substitution induces structure dimensional upgrade and second harmonic generation enhancement37Ba 2 [FeF 4 (IO 3 ) 2 ]IO 3 : a promising nonlinear optical material achieved by chemical-tailoring-induced structure evolution8First chiral fluorinated lead vanadate selenite Pb 2 (V 2 O 4 F)(VO 2 )(SeO 3 ) 3 with five asymmetric motifs and large optical properties24From thiophosphate to chalcohalide: mixed-anion AgS x Cl y ligands concurrently enhancing nonlinear optical effects and laser-damage threshold10In situ hydrothermal synthesis of polar second-order nonlinear optical selenate Na 5 (SeO 4 )(HSeO 4 ) 3 (H 2 O) 219NaGaI 3 O 9 F: a new alkali metal gallium iodate combined with IO 3 − and IO 3 F 2− units16Pb 2 TiFO(SeO 3 ) 2 Br: a new polar compound with the strongest second harmonic generation in the selenite bromide family29Rb3In(SO4)3: a defluorinated mixed main-group metal sulfate for ultraviolet transparent nonlinear optical materials with a large optical band gap26Role of fluorine on the structure and second-harmonic-generation property of inorganic selenites and tellurites23Unexpected aliovalent cation substitution between two NLO materials LiBa 3 Bi 6 (SeO 3 ) 7 F 11 and Ba 3 Bi 6.5 (SeO 3 ) 7 F 10.5 O 0.518Zn(NH 3 )CO 3 : a “three-in-one” UV nonlinear optical crystal built by a polar molecule bonding strategy18Second-order nonlinear optical property of the ultraviolet transparent alkali metal-rare earth metal carbonate Na3Y(CO3)3.3H2O5A Deep‐UV Nonlinear Optical Borosulfate with Incommensurate Modulations71A Deep‐UV Nonlinear Optical Borosulfate with Incommensurate Modulations13LiZn(OH)CO3: A Deep‐Ultraviolet Nonlinear Optical Hydroxycarbonate Designed from a Diamond‐like Structure180LiZn(OH)CO3: A Deep‐Ultraviolet Nonlinear Optical Hydroxycarbonate Designed from a Diamond‐like Structure10A2MoO2F3(IO2F2) (A = Rb, Cs): Strong Nonlinear Optical Responses and Enlarged Band Gaps through Fluorine Incorporation50A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation22A Congruent‐Melting Mid‐Infrared Nonlinear Optical Vanadate Exhibiting Strong Second‐Harmonic Generation63Giant Second-Harmonic Generation Response and Large Band Gap in the Partially Fluorinated Mid-Infrared Oxide RbTeMo 2 O 8 F149An Effective Strategy for Designing Nonlinear Optical Crystals by Combining the Structure‐Directing Property of Oxyfluorides with Chemical Substitution73An Effective Strategy for Designing Nonlinear Optical Crystals by Combining the Structure‐Directing Property of Oxyfluorides with Chemical Substitution10A new I 3 O 9 3− group constructed from IO 3 − and IO 5 5− anion units in Cs 3 [Ga 2 O(I 3 O 9 )(IO 3 ) 4 (HIO 3 )]4NH4Sb2(C2O4)F5: A novel UV nonlinear optical material synthesized in deep eutectic solvents38Two molybdenyl carbonates with different dimensional structures exhibiting huge differences in band gaps7Complex coordinated functional groups: A great genes for nonlinear optical materials64An excellent lead oxyiodide with a strong second-harmonic generation response and a large birefringence induced by the oriented arrangement of highly distorted [PbO 4 I 2 ] polyhedra13APb 2 (C 7 H 3 NO 4 ) 2 I (A = K, Rb, Cs): rare stable nonlinear optical crystals with second-harmonic generation response and highly distorted lead core coordination polyhedra2Band gap modulation and nonlinear optical properties of quaternary tellurates Li 2 GeTeO 613CaCe(IO 3 ) 3 (IO 3 F)F: a promising nonlinear optical material containing both IO 3 − and IO 3 F 2− anions22Hg 2 (SeO 3 )(SO 4 ): the first sulfate selenite with large birefringence explored from d 10 transition metal compounds36Metal oxyhalides: an emerging family of nonlinear optical materials124Wide bandgaps and strong SHG responses of hetero-oxyfluorides by dual-fluorination-directed bandgap engineering28Lead Tellurite Crystals BaPbTe2O6 and PbVTeO5F with Large Nonlinear-/Linear-Optical Responses due to Active Lone Pairs and Distorted Octahedra20HgSO4: An excellent mid-infrared sulfate nonlinear optical crystal with wide band gap and strong second harmonic generation response19Na 3 Ti 3 O 3 (SeO 3 ) 4 F: A Phase-Matchable Nonlinear-Optical Crystal with Enlarged Second-Harmonic-Generation Intensity and Band Gap20Novel layered heterobimetallic fluorides with large optical band gaps3K3ZrF4(SbF4)(SbF5) and K8(ZrF6)(Sb2Zr2F20): Two Zirconium Fluoroantimonites with Low Dimensional Structures and Wide Transparency Range12Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material51Ultrawide Bandgap and Outstanding Second‐Harmonic Generation Response by a Fluorine‐Enrichment Strategy at a Transition‐Metal Oxyfluoride Nonlinear Optical Material12SrZnGeS 4 : A Dual‐Waveband Nonlinear Optical Material with a Transparency Spanning UV/Vis and Far‐IR Spectral Regions88SrZnGeS4: A Dual‐Waveband Nonlinear Optical Material with a Transparency Spanning UV/Vis and Far‐IR Spectral Regions12SrAgAsS4: A Noncentrosymmetric Sulfide with Good Infrared Nonlinear Optical Performance Induced by Aliovalent Substitution from Centrosymmetric SrGa2S412PbBi(SeO 3 ) 2 F and Pb 2 Bi(SeO 3 ) 2 Cl 3 : Coexistence of Three Kinds of Stereochemically Active Lone-Pair Cations Exhibiting Excellent Nonlinear Optical Properties57Isoreticular Design of KTiOPO 4 -Like Deep-Ultraviolet Transparent Materials Exhibiting Strong Second-Harmonic Generation68K 3 C 6 N 7 O 3 ·2H 2 O: A Multifunctional Nonlinear Optical Cyamelurate Crystal with Colossal π-Conjugated Orbitals44From Ba3Nb2O2F12(H2O)2 to Ba0.5NbO2F2(H2O): Achieving Balanced Nonlinear Optical Performance by O/F Ratio Regulation18Ce 3 F 4 (SO 4 ) 4 : cationic framework assembly for designing polar nonlinear optical material through fluorination degree modulation23From CdPb 8 (SeO 3 ) 4 Br 10 to Pb 3 (TeO 3 )Br 4 : the first tellurite bromide exhibiting an SHG response and mid-IR transparency21LaAeAl 3 S 7 (Ae = Ca, Sr): Cairo pentagonal layered thioaluminates achieving a good balance between a strong second harmonic generation response and a wide bandgap23Stereochemically active lone-pair-driven giant enhancement of birefringence from three-dimensional CsZn 4 Ga 5 Se 12 to two-dimensional CsZnAsSe 319The first polyanion-substitution-driven centrosymmetric-to-noncentrosymmetric structural transformation realizing an excellent nonlinear optical supramolecule [Cd 4 P 2 ][CdBr 4 ]17Toward Large Second-Harmonic Generation and Deep-UV Transparency in Strongly Electropositive Transition Metal Sulfates112Polar Bismuth Selenite Iodate Oxide BiSeIO6 with Three Types of Lone Pair Cations in One Structure6K2(H2O)WO3F2: A new nonlinear optical material with remarkable second-harmonic generation response and enhanced laser damage threshold9The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO 3 ) 2 and Y 3 F(SeO 3 ) 485The First UV Nonlinear Optical Selenite Material: Fluorination Control in CaYF(SeO3)2 and Y3F(SeO3)47Data Mining and Graph Network Deep Learning for Band Gap Prediction in Crystalline Borate Materials18Efficient Synthesis, Spectroscopic Characterization, and Nonlinear Optical Properties of Novel Salicylaldehyde-Based Thiosemicarbazones: Experimental and Theoretical Studies37Designing a Strong Second-Harmonic Generation Polar Iodate by the Structure-Directing Properties of the “Tumbler-like” [Zn(IO3)(I2O5(OH))] Polyanions20Y(HSeO3)(SeO3)(H2O)·(H2O) and Y2(SeO3)2(SeO4)(H2O)2·(H2O)0.75: Two yttrium selenites with a short UV cut-off edge explored from pure selenite compounds20Advances in aliovalent substitution strategy for the design and synthesis of nonlinear optical materials: d0 transition metal/gallium iodates and selenites70AAl(Te 4 O 10 ) (A = Na, Ag) and K 2 Ga 2 (HTe 6 O 16 )(HTeO 3 ): Three Aluminum/Gallium Tellurites with Large Birefringence and Wide Band Gap21A selenite containing unusual [Ga2F(Se2O5)4(HSeO3)2]5- clusters with the polarization ‘lighted’ by F− anions15Halide-Induced Band Gap Enhancement from Ba2SnSe4 to KBa2SnSe4Cl2A survey of stereoactive oxysalts for linear and nonlinear optical applications40Four UV Transparent Linear and Nonlinear Optical Materials Explored from Pure Selenite Compounds22Stereochemically Active Lone-Pair Containing Metal Substitution in Polar Axis toward a Giant Phase-Matchable Optical Nonlinear Silicate Crystal Li 3 (OH)PbSiO 463Optically Anisotropic Mixed-Metal Fluoroiodate Ba2[GaF5(IO3F)] with a Wide Optical Transparent Window and a Moderate Birefringence6Ln 2 F 2 (OH 2 )(MoO 3 ) 2 (SeO 3 ) 2 : Promising Multifunctional Nonlinear Optical Materials Created by Partial Fluorination Strategy under Corrosion Resistant Supercritical Reactions25NaMoO 3 (IO 3 )(H 2 O): water molecule introduction induces strong second harmonic generation response, widened band gap and large anisotropy8A2Hgx(SeO3)y (A = K, Rb, Cs): Three Alkali Metal Mercury Selenites Featuring Unique 1D [HgOm(SeO3)n]∞ Chains13K(NH4)Zn2(PO4)2: a Beryllium-Free Sr2Be2B2O7 Derivative with Enhanced Interlayer Connectivity7A UV non-hydrogen pure selenite nonlinear optical material for achieving balanced properties through framework-optimized structural transformation41Equivalent cation-tuning to realize a new Ce( iv ) fluoride with excellent comprehensive nonlinear optical performances12Hydrogen bonding bolstered head-to-tail ligation of functional chromophores in a 0D SbF 3 ·glycine adduct for a short-wave ultraviolet nonlinear optical material32Noncentrosymmetric tellurite halides created by a depolymerization strategy: toward strong SHG intensity and wide bandgap16Pb 2 Ga 3 F 6 (SeO 3 ) 2 X 3 ·2H 2 O (X = Cl, Br): two new HTO-type members exhibiting large NLO effects mediated by ionic mixing and substitution strategies10Recent advances in rational structure design for nonlinear optical crystals: leveraging advantageous templates153Reconstructing nearly isotropic microstructures to construct a one-dimensional framework causing record birefringence in thiophosphates13Exceptional Optical Anisotropy Enhancement Achieved Through Dual‐Ions Cosubstitution Strategy in Novel Hybrid Bismuth Halides23Guanidinium Vanadate [C(NH2)3]3VO4·2H2O Revealing Enhanced Second-Harmonic Generation and Wide Band Gaps13Hg3Se(SeO3)(SO4): A Mixed-Valent Selenium Compound with Mid-Infrared Transmittance Obtained by In Situ Reaction26Centrosymmetric CaBaMF8 and Noncentrosymmetric Li2CaMF8 (M = Zr, Hf): Dimension Variation and Nonlinear Optical Activity Resulting from an Isovalent Cation Substitution-Oriented Design17A2Pb3[H2N(CH2COO)2]3Cl5 (A = K, Rb): Porous Crystals Constructed on [Pb3Cl5O6] Clusters with Comprehensive Nonlinear Optical Performance3UV-Transparent SHG Material Explored in an Alkali Metal Sulfate Selenite System16Aliovalent Substitution Tunes Physical Properties in a Conductive Bis(dithiolene) Two-Dimensional Metal–Organic Framework15MgHg(SeO3)2(H2O)2: A magnesium mercury selenite with large birefringence6Old tree blossoms anew: Research progress on the structures and optical properties of ultraviolet selenites56Second Harmonic Generation in β-K2TeW3O12: An Acentric Crystal Designed from Centric Phase via Pressure Modulation4La3Ga5M0.5Sn0.5O14, (M = Ge, Si): Design and Synthesis of Two Langasite Nonlinear Optical Materials with Large Second Harmonic Generation and Birefringence Induced by Distorted (Sn/M)O6 Octahedra4Hydrogen bond-derived symmetry transformation in hydroxyborates: Converting the nonlinearity from null to active7Achieving balanced UV SHG responses, optical band gaps and birefringence in rare earth compounds Ln(IO 3 )(SO 4 )·3H 2 O (Ln = Y, Gd, Er, Ho, Dy, Eu)4Different p-block elements induce C 3 [111] octahedral distortion in titanium to generate an intense nonlinear effect14Tuning the band gap and structure from wide gap SrBi 3 O 4 Cl 3 to narrow gap Bi 4 O 4 SeCl 2 by aliovalent anion substitution2

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  1. “Two in one”: an unprecedented mixed anion, Ba 2 (C 3 N 3 O 3 )(CNO), with the coexistence of isolated sp and sp 2 π-conjugated groups

    Dalton Transactions · 2019-01-01

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

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  2. A rich structural chemistry in π-conjugated hydroisocyanurates: layered structures of A 2 B(H 2 C 3 N 3 O 3 ) 4 · n H 2 O (A = K, Rb, Cs; B = Mg, Ca; n = 4, 10) with high ultraviolet transparency and strong optical anisotropy

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  3. Adjustable optical nonlinearity in d 10 cations containing chalcogenides via dp hybridization interaction

    Dalton Transactions · 2019-01-01

    Jianian Cheng, Bing‐Hua Lei, Chen Zhou, Shilie Pan, Zhihua Yang

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  4. Ag 7 TaSe 6 : a new noncentrosymmetric selenide with fascinating “three in one” coordination modes and a strong second harmonic generation response

    Journal of Materials Chemistry C · 2019-01-01

    Zhuang Li, Shengzi Zhang, Wenlong Yin, Kaijin Kang, Yangwu Guo, Wenhao Xing, Zheshuai Lin, Jiyong Yao, Yicheng Wu

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  5. 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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  6. 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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  7. From 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 crystals

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

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  10. M 2 (SeO 3 )F 2 (M = Zn, Cd): understanding the structure directing effect of [SeO 3 ] 2− groups on constructing ordered oxyfluorides

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  11. Pb 2 Cd(SeO 3 ) 2 X 2 (X = Cl and Br): two halogenated selenites with phase matchable second harmonic generation

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  12. Pb 7 F 12 Cl 2 : a promising infrared nonlinear optical material with high laser damage threshold

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  13. Synthesis and structure of a new mixed metal iodate Ba 3 Ga 2 (IO 3 ) 12

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

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  15. CsSbF 2 SO 4 : An Excellent Ultraviolet Nonlinear Optical Sulfate with a KTiOPO 4 (KTP)‐type Structure

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

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  17. Cs3Na(H2C3N3O3)4·3H2O: A Mixed Alkali‐Metal Hydroisocyanurate Nonlinear Optical Material Containing π‐Conjugated Six‐Membered‐Ring Units

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

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  19. Variable Chains Found in Mixed Transition Metal Oxyfluorides with Heterocyclic Ligands

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  20. KBiCl2SO4: The First Bismuth Chloride Sulfate Being Second-Order Nonlinear Optical Active

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  21. New 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 Properties

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  22. Ba2M(C3N3O3)2 (M = Sr, Pb): Band Engineering from p−π Interaction via Homovalent Substitution in Metal Cyanurates Containing Planar π-Conjugated Groups

    Inorganic Chemistry · 2019-07-15

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  23. Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups

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  24. Partial Congener Substitution Induced Centrosymmetric to Noncentrosymmetric Transformation Witnessed by K3Ga3(Ge7–xMx)Se20 (M = Si, Sn) and Their Nonlinear Optical Properties

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  25. A x Ce 9 (IO 3 ) 36 (A = K, La): the effects of a change in the intermediate valence on the second-harmonic generation response

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  26. Ag4Hg(SeO3)2(SeO4): a novel SHG material created in mixed valent selenium oxides by in situ synthesis

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  27. First-Principles Design and Simulations Promote the Development of Nonlinear Optical Crystals

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  28. K5(W3O9F4)(IO3): An Efficient Mid-Infrared Nonlinear Optical Compound with High Laser Damage Threshold

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