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RESEARCH PAPER · Journal of the American Chemical Society · 2019

Uniform Alignment of Non-π-Conjugated Species Enhances Deep Ultraviolet Optical Nonlinearity

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Uniform Alignment of Non-π-Conjugated Species Enhances Deep Ultraviolet Optical NonlinearityOriginalTwo new tin( iv )-containing phosphate fluorides with two types of Sn( iv )–P–O–F frameworks and short cutoff edges0Centrosymmetric Rb2Mg3(SO4)4 and non-centrosymmetric Cs2Mg3(SO4)4 with a phase-matching nonlinear optical response35Facile Growth of an Ultraviolet Hydroisocyanurate Crystal with Strong Nonlinearity and a Wide Phase-Matching Region from π-Conjugated (HC3N3O3)2– Groups45How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates327Recent advances in photofunctional polymorphs of molecular materials96Sn2B5O9Cl: 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 Tin33An Uncommon Hypervalent Fluorooxosilicophosphate5CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Novel cyclic and linearizing cyclic Pd(II) nanohoop-based cordination complexes achieving nonlinear optical activity transparency trade-off optimization6An Effective and Facile Method To Prepare Monofluorophosphates Overcoming the Common Difficulty of Loss of Fluorine and Serious Corrosion: 12 Examples and Their Characterizations and Properties11A new iodate-phosphate Pb 2 (IO 3 )(PO 4 ) achieving great improvement in birefringence activated by (IO 3 ) − groups53A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals48Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43NaRb3B6O9(OH)3(HCO3): A Borate-Bicarbonate Nonlinear Optical Material18Structural Diversity and Giant Birefringence in Cyanates BaCNOX (X = Cl, Br, I, and CNO) Containing Linear π-Conjugated Units: A Combined Experimental and Theoretical Study13[Al(H 2 O) 6 ](IO 3 ) 2 (NO 3 ): a material with enhanced birefringence induced by synergism of two superior functional motifs29Ba 6 BO 3 Cl 9 and Pb 6 BO 4 Cl 7 : structural insights into ortho -borates with uncondensed BO 4 tetrahedra10Helix-constructed polar rare-earth iodate fluoride as a laser nonlinear optical multifunctional material25Hydroisocyanurates 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 ) − anions28K 4 (PO 2 F 2 ) 2 (S 2 O 7 ): first fluorooxophosphorsulfate with mixed-anion [S 2 O 7 ] 2− and [PO 2 F 2 ] − groups14Na 3 Sc 2 (PO 4 ) 2 F 3 : rational design and synthesis of an alkali rare-earth phosphate fluoride as an ultraviolet nonlinear optical crystal with an enlarged birefringence49Polar polymorphism: α- and β-KCsWP 2 O 9 nonlinear optical materials with a strong second harmonic generation response25Second-order nonlinear optical materials with a benzene-like conjugated π system49Three diphosphates, α-Li 2 Na 2 P 2 O 7 , Li 8 Pb 3 Ba(P 2 O 7 ) 4 and Li 7 Rb(P 2 O 7 ) 2 : influences of co-substitution on the crystal structure9Three 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 new ammonium/alkali-rare earth metal difluorophosphates ALa(PO 2 F 2 ) 4 (A = NH 4 and K) with moderate birefringence and short cutoff edges26Effects of P2O7 clusters arrangement on second harmonic generation responses of pyrophosphates14Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320The first rare-earth lead phosphates Pb3AP3O12 (A=Sc, Gd) with remarkable SHG enhancement8Lead 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 Materials55Solid-State Nonlinear Optical Switch with the Widest Switching Temperature Range Owing to Its Continuously Tunable Tc91Enhancement of Second-Order Optical Nonlinearity in a Lutetium Selenite by Monodentate Anion Partial Substitution58Synthesis, characterizations and theoretical analysis of a noncentrosymmetric sulfate8Designing a Deep-UV Nonlinear Optical Fluorooxosilicophosphate127Synthesis, crystal structures and optical properties of open-framework gallium phosphates: NaGa3F4(PO4)2(H2O)2 and AGa2P2O7(OH)3(H2O) (A = K, Rb)1A review on phase transition and structure-performance relationship of second-order nonlinear optical polymorphs107New Alkaline-Earth Metal Fluoroiodates Exhibiting Large Birefringence and Short Ultraviolet Cutoff Edge with Highly Polarizable (IO 3 F) 2– Units63Cyclophosphate MBi(P4O12) (M = Cs, Rb): Structure Change Giving Rise to Property Enhancement10K 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 Performance38Zn3B7O13Cl: A New Deep-Ultraviolet Transparency Nonlinear Optical Crystal with Boracite Structure24Pb 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 Properties29Recent 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 Responses106Ba(MoO2F)2(XO3)2 (X = Se and Te): First Cases of Noncentrosymmetric Fluorinated Molybdenum Oxide Selenite/Tellurite Through Unary Substitution for Enlarging Band Gaps and Second Harmonic Generation34Two Mixed-Anion Units of [GeOSe3] and [GeO3S] Originating from Partial Isovalent Anion Substitution and Inducing Moderate Second Harmonic Generation Response and Large Birefringence55Role of Fluorooxo-Functional Units in Symmetry Breaking and Second Harmonic Generation Response Contribution in Fluorooxoborate Nonlinear Optical Crystals15α‐SnF 2 : A UV Birefringent Material with Large Birefringence and Easy Crystal Growth24α‐SnF 2 : A UV Birefringent Material with Large Birefringence and Easy Crystal Growth210Origin of ultra-wide IR transmission and ultra-large birefringence of mercurous halide series with one dimensional chain-like structure: An ab initio study15An Antimony(III) Fluoride Oxalate with Large Birefringence45Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence92Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence13Hydrogen-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)10K 3 B 4 PO 10 and K 2 MB 4 PO 10 (M = Rb/Cs): rare mixed-coordinated borophosphates with large birefringence33Ba 2 [FeF 4 (IO 3 ) 2 ]IO 3 : a promising nonlinear optical material achieved by chemical-tailoring-induced structure evolution8Barium fluoroiodate crystals with a large band gap and birefringence22Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41Deep-ultraviolet transparent alkali metal–rare earth metal sulfate NaY(SO 4 ) 2 ·H 2 O as a nonlinear optical crystal: synthesis and characterization28Na 1.5 Rb 0.5 PO 3 F·H 2 O: synthesis, properties, and stepwise reconstruction of the hydrogen bond network13RbMo 2 P 3 O 14 with large birefringence mainly induced by highly distorted [MoO 6 ] in uncommon [Mo 2 P 3 O 14 ] ∞ layers9Recent advances of oxyfluorides for nonlinear optical applications69The Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal0To improve the key properties of nonlinear optical crystals assembled with tetrahedral functional building units46Zn(NH 3 )CO 3 : a “three-in-one” UV nonlinear optical crystal built by a polar molecule bonding strategy18Ba3Sb2(PO4)4 and Cd3Sb2(PO4)4(H2O)2: Two New Antimonous Phosphates with Distinct [Sb(PO4)2] Structure Types and Enhanced Birefringence37M(NH 2 SO 3 ) 2 (M=Sr, Ba): Two Deep‐Ultraviolet Transparent Sulfamates Exhibiting Strong Second Harmonic Generation Responses and Moderate Birefringence142M(NH 2 SO 3 ) 2 (M=Sr, Ba): Two Deep‐Ultraviolet Transparent Sulfamates Exhibiting Strong Second Harmonic Generation Responses and Moderate Birefringence27Finding Short-Wavelength Birefringent Crystals with Large Optical Anisotropy Activated by π-Conjugated [C(NH2)3] Units45Different mechanism of stereochemical activity and birefringence in post-transition metal halides: A first-principles investigation1[C(NH2)3]3PO4·2H2O: A new metal-free ultraviolet nonlinear optical phosphate with large birefringence and second-harmonic generation response70Second-order nonlinear optical property of the ultraviolet transparent alkali metal-rare earth metal carbonate Na3Y(CO3)3.3H2O5Discovery of NLO Semiorganic (C 5 H 6 ON) + (H 2 PO 4 ) − : Dipole Moment Modulation and Superior Synergy in Solar-Blind UV Region270Two Lead Halides with Strong SHG Response Obtained by the Isovalent Substitutions of Alkali Metal Cation and Halogen Anion22Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137UV 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 Phosphate28Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application167Discovery of First Magnesium Fluorooxoborate with Stable Fluorine Terminated Framework for Deep‐UV Nonlinear Optical Application18Te(CS(NH2)2)4SO4·2H2O: A Three-in-One Semiorganic Nonlinear Optical Crystal with an Unusual Quadrilateral (TeS4)6– Chromophore14AXHg3P2S8 (A = Rb, Cs; X = Cl, Br): New Excellent Infrared Nonlinear Optical Materials with Mixed‐Anion Chalcohalide Groups of Trigonal Planar [HgS2X]3− and Tetrahedral [HgS3X]5−58Fluorine‐Driven Enhancement of Birefringence in the Fluorooxosulfate: A Deep Evaluation from a Joint Experimental and Computational Study139Tetrafluoroborate-Monofluorophosphate (NH4)3[PO3F][BF4]: First Member of Oxyfluoride with B–F and P–F Bonds16Non-π-Conjugated Deep-Ultraviolet Nonlinear Optical Crystal K2Zn3(SO4)(HSO4)2F437Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate212Sn2PO4I: An Excellent Birefringent Material with Giant Optical Anisotropy in Non π‐Conjugated Phosphate22A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**175Synthesis, Crystal Structure, and Nonlinear Optical Property of an Anhydrous Sulfate KTb(SO4)216A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**272D van der Waals Layered [C(NH2)3]2SO3S Exhibits Desirable UV Nonlinear-Optical Trade-Off47An 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 Substitution10Tourmaline with ultraviolet optical nonlinearity: Emergent material discovery from mineral5NiCoP with Dandelion-like Arrays Anchored on Nanowires for Electrocatalytic Overall Water Splitting15H{[Na(H2O)3]6F}(PO4)2 ⋅ 2(H2O): A New Polycation‐Type Phosphate with Deep Ultraviolet Transparency0Polymorphic Pb14O8I12 and Pb7O4I6 oxyhalides featuring unprecedented [O8Pb14] clusters with broad IR transparency20From β‐Na2B6O10 to Na3AlB8O15 and Na3Al2B7O15: Structural Tuning of Anionic‐Group Architectures by Substitution of [BO4] by [AlO4] Covalent Tetrahedra10Complex coordinated functional groups: A great genes for nonlinear optical materials64Pushing KTiOPO4-like Nonlinear Optical Sulfates into the Deep-Ultraviolet Spectral Region19Hybrid organic–inorganic triguanidine arsenate dihydrate for ultraviolet nonlinear optical application15Na4B8O9F10: A Deep‐Ultraviolet Transparent Nonlinear Optical Fluorooxoborate with Unexpected Short Phase‐Matching Wavelength Induced by Optimized Chromatic Dispersion133Na4B8O9F10: A Deep‐Ultraviolet Transparent Nonlinear Optical Fluorooxoborate with Unexpected Short Phase‐Matching Wavelength Induced by Optimized Chromatic Dispersion13Recent Development of Non-π-Conjugated Deep Ultraviolet Nonlinear Optical Materials106(N 2 H 6 )[HPO 3 F] 2 : maximizing the optical anisotropy of deep-ultraviolet fluorophosphates33[C 3 N 6 H 7 ] 2 [B 3 O 3 F 4 (OH)]: a new hybrid birefringent crystal with strong optical anisotropy induced by mixed functional units85A flexible functional module to regulate ultraviolet optical nonlinearity for achieving a balance between a second-harmonic generation response and birefringence43From oxides to oxysulfides: the mixed-anion GeS 3 O unit induces huge improvement in the nonlinear optical effect and optical anisotropy for potential nonlinear optical materials19Inducing large birefringence by enhancing asymmetric electron distribution of Y–O polyhedra21K 2 (BeS)O 4 F 2 : a novel fluorosulfate with unprecedented 1D [(BeO 3 F)–(SO 3 F)] ∞ chains exhibiting large birefringence10Large optical anisotropy differentiation induced by the anion-directed regulation of structures29Large optical anisotropy-oriented construction of a carbonate-nitrate chloride compound as a potential ultraviolet birefringent material44Metal oxyhalides: an emerging family of nonlinear optical materials124Mg(H 2 O) 6 [(IO 2 (OH)) 2 (IO 3 )] 2 : a new iodate with a very large band gap and optical anisotropy13Nain(C2o4)(Hpo4)(H2o)5: An Ultraviolet Transparent Nonlinear Optical Oxalate-Phosphate with Large Birefringence0PNO: a promising deep-UV nonlinear optical material with the largest second harmonic generation effect17Rational design of a promising oxychalcogenide infrared nonlinear optical crystal60Synergistic effect of 2 [V 2 P 2 O 14 ] ∞ layers and hydrogen bonds inducing large birefringence in M(VO) 2 (PO 4 ) 2 ·4H 2 O (M = Ca, Sr, Ba) systems4Wide bandgaps and strong SHG responses of hetero-oxyfluorides by dual-fluorination-directed bandgap engineering28High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence21High‐Performance Sulfate Optical Materials Exhibiting Giant Second Harmonic Generation and Large Birefringence199Crystal Structure and Theoretical Analysis of Cs2Ca3(SO4)47Potential optical functional crystals with large birefringence: Recent advances and future prospects322Advances in second-order nonlinear optical sulfates38Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra9Sulfamide: A Promising Deep‐Ultraviolet Nonlinear Optical Crystal Assembled from Polar Covalent [SO2(NH2)2] Tetrahedra84CsY(SO4)2·4H2O: A Deep-Ultraviolet Birefringent Crystal Induced by an Edge-Sharing Connection26Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)212Strong Nonlinearity Induced by Coaxial Alignment of Polar Chain and Dense [BO3] Units in CaZn2(BO3)2212Sr3[SnOSe3][CO3]: A Heteroanionic Nonlinear Optical Material Containing Planar π‐conjugated [CO3] and Heteroleptic [SnOSe3] Anionic Groups78Sr3[SnOSe3][CO3]: A Heteroanionic Nonlinear Optical Material Containing Planar π‐conjugated [CO3] and Heteroleptic [SnOSe3] Anionic Groups7Ultrawide 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 Material12A deep ultraviolet transparent birefringent monofluorophosphate: Cd2.5(NH4)2(PO3F)3Cl ⋅ 2H2O4Balance of Deep-Ultraviolet Transparency and Large Second Harmonic Generation Response in a Silicate Crystal9Maximizing the linear and nonlinear optical responses of alkaline tricyanomelaminate28Crystal Growth and Physical Properties of the Nonlinear Optical Crystal KLi(HC3N3O3)·2H2O15Alkali metal sulfate: A new non-π-conjugated deep-ultraviolet quasi-phase matching crystal27Lone Pair-Driven Enhancement of Birefringence in Polar Alkali Metal Antimony Phosphates46Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species6Promising Deep‐Ultraviolet Birefringent Materials via Rational Design and Assembly of Planar π‐Conjugated [B(OH)3] and [B3O3(OH)3] Functional Species83An Optimized KBe2BO3F2‐Like Structure: The Unity of Deep‐Ultraviolet Transparency, Nonlinear Optical Property, and Ferroelectricity22Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters9Double‐Modification Oriented Design of a Deep‐UV Birefringent Crystal Functionalized by [B12O16F4(OH)4] Clusters139(NH4)3B11PO19F3: a deep-UV nonlinear optical crystal with unique [B5PO10F]∞ layers142Yin–Yang Complementarity Strategy Achieving Giant Optical Anisotropy in a Metal-free Birefringent Material C(NH2)3(HC4O4)14

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  1. Two new tin( iv )-containing phosphate fluorides with two types of Sn( iv )–P–O–F frameworks and short cutoff edges

    New Journal of Chemistry · 2019-01-01

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

    Inorganic Chemistry Communications · 2019-07-22

    Meng Wang, Dequan Wei, Lanju Liang, Xin Pei Yan, Kaikai Lv

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

    Inorganic Chemistry · 2019-08-15

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

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  4. How To Maximize Birefringence and Nonlinearity of π-Conjugated Cyanurates

    Journal of the American Chemical Society · 2019-09-12

    Jing Lu, Yu‐Kun Lian, Lin Xiong, Qianru Wu, Min Zhao, Ke-Xin Shi, Ling Chen, Li‐Ming Wu

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  5. Recent advances in photofunctional polymorphs of molecular materials

    Chinese Chemical Letters · 2019-09-17

    Bo Lu, Shuya Liu, Dongpeng Yan

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  6. Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin

    Angewandte Chemie International Edition · 2019-09-17

    Jingyu Guo, Abudukadi Tudi, Shujuan Han, Zhihua Yang, Shilie Pan

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  7. Sn2B5O9Cl: A Material with Large Birefringence Enhancement Activated Prepared via Alkaline‐Earth‐Metal Substitution by Tin

    Angewandte Chemie · 2019-09-17

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  8. An Uncommon Hypervalent Fluorooxosilicophosphate

    Chemistry - An Asian Journal · 2019-10-17

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

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  10. Novel cyclic and linearizing cyclic Pd(II) nanohoop-based cordination complexes achieving nonlinear optical activity transparency trade-off optimization

    Organic Electronics · 2019-11-16

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  11. An Effective and Facile Method To Prepare Monofluorophosphates Overcoming the Common Difficulty of Loss of Fluorine and Serious Corrosion: 12 Examples and Their Characterizations and Properties

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  12. A new iodate-phosphate Pb 2 (IO 3 )(PO 4 ) achieving great improvement in birefringence activated by (IO 3 ) − groups

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  13. A new family of quaternary thiosilicates SrA 2 SiS 4 (A = Li, Na, Cu) as promising infrared nonlinear optical crystals

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  14. Emergent Deep‐Ultraviolet Nonlinear Optical Candidates

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

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  16. NaRb3B6O9(OH)3(HCO3): A Borate-Bicarbonate Nonlinear Optical Material

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  17. Structural Diversity and Giant Birefringence in Cyanates BaCNOX (X = Cl, Br, I, and CNO) Containing Linear π-Conjugated Units: A Combined Experimental and Theoretical Study

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  18. [Al(H 2 O) 6 ](IO 3 ) 2 (NO 3 ): a material with enhanced birefringence induced by synergism of two superior functional motifs

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  19. Ba 6 BO 3 Cl 9 and Pb 6 BO 4 Cl 7 : structural insights into ortho -borates with uncondensed BO 4 tetrahedra

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  20. Helix-constructed polar rare-earth iodate fluoride as a laser nonlinear optical multifunctional material

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  21. 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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  22. K 4 (PO 2 F 2 ) 2 (S 2 O 7 ): first fluorooxophosphorsulfate with mixed-anion [S 2 O 7 ] 2− and [PO 2 F 2 ] − groups

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  23. Na 3 Sc 2 (PO 4 ) 2 F 3 : rational design and synthesis of an alkali rare-earth phosphate fluoride as an ultraviolet nonlinear optical crystal with an enlarged birefringence

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  24. Polar polymorphism: α- and β-KCsWP 2 O 9 nonlinear optical materials with a strong second harmonic generation response

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

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  26. Three diphosphates, α-Li 2 Na 2 P 2 O 7 , Li 8 Pb 3 Ba(P 2 O 7 ) 4 and Li 7 Rb(P 2 O 7 ) 2 : influences of co-substitution on the crystal structure

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  27. Three non-centrosymmetric bismuth phosphates, Li 2 ABi(PO 4 ) 2 (A = K, Rb, and Cs): effects of cations on the crystal structure and SHG response

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  28. Two new ammonium/alkali-rare earth metal difluorophosphates ALa(PO 2 F 2 ) 4 (A = NH 4 and K) with moderate birefringence and short cutoff edges

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  29. Effects of P2O7 clusters arrangement on second harmonic generation responses of pyrophosphates

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  30. Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)3

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  31. The first rare-earth lead phosphates Pb3AP3O12 (A=Sc, Gd) with remarkable SHG enhancement

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  32. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

    Angewandte Chemie International Edition · 2020-03-11

    Xinglong Chen, Hongil Jo, Kang Min Ok

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  33. Lead Mixed Oxyhalides Satisfying All Fundamental Requirements for High‐Performance Mid‐Infrared Nonlinear Optical Materials

    Angewandte Chemie · 2020-03-11

    Xinglong Chen, Hongil Jo, Kang Min Ok

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  34. Solid-State Nonlinear Optical Switch with the Widest Switching Temperature Range Owing to Its Continuously Tunable Tc

    Journal of the American Chemical Society · 2020-03-11

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