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RESEARCH PAPER · Chemistry of Materials · 2017

Phase-Matching in Nonlinear Optical Compounds: A Materials Perspective

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Phase-Matching in Nonlinear Optical Compounds: A Materials PerspectiveOriginalCrystal growth and optical properties of a UV nonlinear optical material KSrCO 3 F73Crystal Growth and Linear and Nonlinear Optical Properties of KIO 3 ·Te(OH) 615Finding the Next Deep-Ultraviolet Nonlinear Optical Material: NH4B4O6F1233Deep-Ultraviolet Nonlinear-Optical Material K3Sr3Li2Al4B6O20F: Addressing the Structural Instability Problem in KBe2BO3F2105CsB 4 O 6 F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units184CsB4O6F: A Congruent‐Melting Deep‐Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units895Noncentrosymmetric quaternary selenide Ba23Ga8Sb2Se38: Synthesis, structure, and optical properties15Viewpoint: Inorganic Materials for UV and Deep-UV Nonlinear-Optical Applications207Li2MnSnSe4: A New Quaternary Diamond‐Like Semiconductor with Nonlinear Optical Response and Antiferromagnetic Property16High-efficiency UV generation at 266 nm in a new nonlinear optical crystal NaSr_3Be_3B_3O_9F_436More than 2017 Reasons We Appreciate Our Authors, Reviewers, and Readers0Ba 2 ZnSc(BO 3 ) 3 and Ba 4 Zn 5 Sc 2 (BO 3 ) 8 : first examples of borates in the Zn–Sc–B–O system featuring special structure configurations15BaLiZn 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 distance16Optimized oriented seed growth and optical properties of high-quality LiInSe 2 crystals13Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials191Cation‐Tuned Synthesis of Fluorooxoborates: Towards Optimal Deep‐Ultraviolet Nonlinear Optical Materials714Virtual Issue: Methods and Protocols Series in Materials Science—20180Virtual Issue: Methods and Protocols Series in Materials Science—20180CaB5O7F3: A Beryllium-Free Alkaline-Earth Fluorooxoborate Exhibiting Excellent Nonlinear Optical Performances192Controlled Growth of Layered Acentric CdTeMoO6 Single Crystals with Linear and Nonlinear Optical Properties50Syntheses, Structures, and Properties of Non-Centrosymmetric Quaternary Tellurates BiMTeO6 (M = Al, Ga)21Two Novel Deep‐Ultraviolet Nonlinear Optical Crystals with Shorter Phase‐Matching Second Harmonic Generation than KBe2BO3F2: A First‐Principles Prediction20Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials95Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates265Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials102The must-have and nice-to-have experimental and computational requirements for functional frequency doubling deep-UV crystals242Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials195Second-order nonlinear optical crystals with mixed anions250Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold59Czochralski Growth and Characterization of a Novel Nonlinear Optical Crystal Te2P2O923Second-order nonlinear optical properties of CuGa In1-Se2 (x = 0.54): Experimental and theoretical investigations4Li2BaSc(BO3)2F and LiBa2Pb(BO3)2F with Layered Structures featuring Special Li−O/F Configurations11A 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 materials98Metal-free perovskites for non linear optical materials70Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation66SrCdGeS4 and SrCdGeSe4: Promising Infrared Nonlinear Optical Materials with Congruent-Melting Behavior74Crystallographic Investigations into the Polar Polymorphism of BaTeW2O9: Phase Transformation, Controlled Crystallization, and Linear and Nonlinear Optical Properties26KLi(HC 3 N 3 O 3 )·2H 2 O: Solvent-drop Grinding Method toward the Hydro-isocyanurate Nonlinear Optical Crystal314Ba10In6Zn7S26-nZnS: An Inorganic Composite System with Interface Phase-Matching Tuned for High-Performance Infrared Nonlinear Optical Materials13Module-Analysis-Assisted Design of Deep Ultraviolet Fluorooxoborates with Extremely Large Gap and High Structural Stability109Transformation of the B–O Units from Corner-Sharing to Edge-Sharing Linkages in BaMBO4 (M = Ga, Al)33KBiCl2SO4: The First Bismuth Chloride Sulfate Being Second-Order Nonlinear Optical Active44Highly Polarizable Hg2+ Induced a Strong Second Harmonic Generation Signal and Large Birefringence in LiHgPO4265Untangling electronic, optical and bonding properties of hexagonal bismuth borate SrBi2B2O7 crystal for ultraviolet opto-electronic applications: An ab initio study8Structure and Properties of the Non‐Centrosymmetric Manganese(II) Borate Mn5(BO3)3OH3[NH4]12[(MoO2)2O(HPO4)2]4[PO4]Cl·0.5H2O: A mixed phosphomolybdate with nonlinear optical properties4Crystal Structure and (Non)linear Optical Properties of a Cyanuric Acid Isoniazid <1/1> Co-crystal: Shortcomings of Phase Matching Determination from Powdered Samples12CsAlB 3 O 6 F: a beryllium-free deep-ultraviolet nonlinear optical material with enhanced thermal stability153Nonlinear Optical Crystals for Second Harmonic Generation19Atom-Resolved Analysis of Birefringence of Nonlinear Optical Crystals by Bader Charge Integration55Transformation of Optical Anisotropy Origins in Perovskite-Related Materials: A First-Principles Study23(NH4)Bi2(IO3)2F5: An Unusual Ammonium‐Containing Metal Iodate Fluoride Showing Strong Second Harmonic Generation Response and Thermochromic Behavior92(NH4)Bi2(IO3)2F5: An Unusual Ammonium‐Containing Metal Iodate Fluoride Showing Strong Second Harmonic Generation Response and Thermochromic Behavior11Emergent Deep‐Ultraviolet Nonlinear Optical Candidates324Neue Kandidaten für die nichtlineare Optik im Tief‐UV‐Bereich43Ba 6 In 6 Zn 4 Se 19 : a high performance infrared nonlinear optical crystal with [InSe 3 ] 3− trigonal planar functional motifs22Tellurium–oxygen group enhanced birefringence in tellurium phosphates: a first-principles investigation4Designing Sulfide Borate as a Novel Type of Second-Order Nonlinear-Optical Material91Structure-property relationship in nonlinear optical materials with π-conjugated CO3 triangles146Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320(Na0.60Ba0.70)Ga2Se4: An Infrared Nonlinear Optical Crystal Designed using AgGaSe2 as the Template38Synthesis and Characterization of Two New Second Harmonic Generation Active Iodates: K3Sc(IO3)6 and KSc(IO3)3Cl9Hexagonal In2Se3: A Defect Wurtzite-Type Infrared Nonlinear Optical Material with Moderate Birefringence Contributed by Unique InSe5 Unit75Overcoming the phase-mismatch by fundamental beam modulation1Deep-ultraviolet nonlinear optical crystals by design: A computer-aided modeling blueprint from first principles45Efficient near-infrared laser emission and nonlinear optical properties of a newly developed Yb:LYSB laser crystal10Investigation on the growth rate, crystalline perfection, refractive index, Z-scan and electrical characteristics of Z- cut imidazolium l-tartrate single crystal36Introduction to Optics I: Interaction of Light with Matter1Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )212Giant Optical Anisotropy in the UV‐Transparent 2D Nonlinear Optical Material Sc(IO 3 ) 2 (NO 3 )57AB 11 O 16 (OH) 2 (A = K and Cs): interpenetrating 2D layers with large birefringence7Layered oxide B2S2O9 with a deep-ultraviolet band gap and a strong and robust second-harmonic generation32Phase Matching, Strong Frequency Doubling, and Outstanding Laser-Induced Damage Threshold in the Biaxial, Quaternary Diamond-like Semiconductor Li 4 CdSn 2 S 779Borates: A Rich Source for Optical Materials1089Synergism of multiple functional chromophores significantly enhancing the birefringence in layered non-centrosymmetric chalcohalides20Design and development of near-infrared, visible and ultraviolet LIDAR echo emulator for HgCdTe avalanche photodiode characterisation0Distinctive modulation of optical anisotropy by halogens in α/β-Cd–P–X (X = Cl, Br, and I)2Finding Short-Wavelength Birefringent Crystals with Large Optical Anisotropy Activated by π-Conjugated [C(NH2)3] Units45[C(NH2)3]3PO4·2H2O: A new metal-free ultraviolet nonlinear optical phosphate with large birefringence and second-harmonic generation response70π‑Conjugated Trigonal Planar [C(NH2)3]+ Cationic Group: A Superior Functional Unit for Ultraviolet Nonlinear Optical Materials52Toward the Enhancement of Critical Performance for Deep-Ultraviolet Frequency-Doubling Crystals Utilizing Covalent Tetrahedra137Discovery 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 Application18AXHg3P2S8 (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]5−58Bulk crystal growth, crystalline perfection and optical homogeneities of 2AP4N single crystals for second and third order frequency conversion and terahertz (THz) device applications31Temperature dependent refractive index, thermo-optic coefficient and birefringence of negative biaxial imidazolium l-tartrate non-linear optical crystal8Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals146Hydroxyfluorooxoborate Na[B3O3F2(OH)2]⋅[B(OH)3]: Optimizing the Optical Anisotropy with Heteroanionic Units for Deep Ultraviolet Birefringent Crystals16Exploring Deep-UV Nonlinear Optical Materials with Enhanced Second Harmonic Generation Response and Birefringence in Fluoroaluminoborate Crystals69Centrosymmetric or Noncentrosymmetric? Transition Metals Talking in K 2 TGe 3 S 8 (T = Co, Fe)25Calculating properties of non-collinear phase matching in two different polarization for KDP crystal2Achieving 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] Units9Structure Tuning, Strong Second Harmonic Generation Response, and High Optical Stability of the Polar Semiconductors Na1–xKxAsQ234A New Nonlinear Optical Material with N(CN)2− Anion2Superalkali-based alkalides Li3O@[12-crown-4]M (where M= Li, Na, and K) with remarkable static and dynamic NLO properties; A DFT study53Giant Non‐Resonant Infrared Second Order Nonlinearity in γ ‐NaAsSe229Synergistic Effect of π-Conjugated [C(NH 2 ) 3 ] Cation and Sb(III) Lone Pair Stereoactivity on Structural Transformation and Second Harmonic Generation58Near-infrared, visible, and ultraviolet lidar echo emulator1Na4B8O9F10: 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 Dispersion13A 2 P 2 S 6 (A = Ba and Pb): a good platform to study the polymorph effect and lone pair effect to form an acentric structure28Growth and Characterizations of a New Nonlinear Optical Crystal for 266 Nm Laser Generation: Lisr3be3b3o9f41Metal oxyhalides: an emerging family of nonlinear optical materials124Na 3 B 6 O 10 (HCOO): an ultraviolet nonlinear optical sodium borate-formate33Nonlinear optics with structured light148Phase matching achieved by isomorphous substitution in IR nonlinear optical material Ba 2 SnSSi 2 O 7 with an undiscovered [SnO 4 S] functional motif47Phase Matching3Review of Heteroleptic Tetrahedra as Birefringent or Nonlinear Optical Motifs17Ba6(CuxZy)Sn4S16 (Z = Mg, Mn, Zn, Cd, In, Bi, Sn): High Chemical Flexibility Resulting in Good Nonlinear-Optical Properties12Phase Relations in the CaO-B2O3-Sc2O3 Ternary System1Infrared nonlinear optical performances of a new sulfide β-PbGa2S415Advances in second-order nonlinear optical sulfates38Hydrothermal single crystal growth and structural investigation of the stuffed tridymite family as NLO materials6Enhanced Second-Harmonic-Generation Efficiency and Birefringence in Melillite Oxychalcogenides Sr2MGe2OS6 (M = Mn, Zn, and Cd)97Crystal Growth and Physical Properties of the Nonlinear Optical Crystal KLi(HC3N3O3)·2H2O15SnP2S6: A Promising Infrared Nonlinear Optical Crystal with Strong Nonresonant Second Harmonic Generation and Phase-Matchability32Double‐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] Clusters139Ba2MAsQ5 (Q = S and Se) Family of Polar Structures with Large Second Harmonic Generation and Phase Matchability23RbBiP2S6: A Promising IR Nonlinear Optical Material with a Giant Second-Harmonic Generation Response Designed by Aliovalent Substitution80(NH4)3B11PO19F3: a deep-UV nonlinear optical crystal with unique [B5PO10F]∞ layers142Orientation-Controlled Anisotropy in Single Crystals of Quasi-1D BaTiS326Two Metal Phosphate Nonlinear Optical Materials Simultaneously Exhibiting Ultraviolet Transparence and a Large Birefringence50Observation of a triangular-lattice pattern in nonlinear wave mixing with optical vortices34Heteroanionic Control of Exemplary Second-Harmonic Generation and Phase Matchability in 1D LiAsS2–xSex43Role of coordination site in governing the structural, electronic and optical properties of Ca-doped strontium barium niobate5From Phosphate Fluoride to Fluorophosphate: Design of Novel Ultraviolet/Deep-Ultraviolet Nonlinear Optical Materials for BePO3F with Optical Property Enhancement34Finding a Deep‐UV Borate BaZnB4O8 with Edge‐sharing [BO4] Tetrahedra and Strong Optical Anisotropy20Direction dependent crystalline perfection, Z-scan studies and fabrication of Type-I and Type-II SHG elements using imidazolium L-tartrate crystals for optical modulator applications7CaBO2F: A novel deep-UV structural template with high nonlinear optical performance induced by electron delocalization25Exploring Short-Wavelength Phase-Matching Nonlinear Optical Crystals by Employing KBe2BO3F2 as the Template95NaHSO4·H2O: A Promising Deep-Ultraviolet Nonlinear-Optical Bisulfate with Large Birefringence and a Second-Harmonic-Generation Effect16LiNaB6O9F2: A Promising UV NLO Crystal Having Fluorine‐Directed Optimal Performances and Double Interpenetrating 3[B6O9F2]∞ Networks33Large birefringence in the quasi-one-dimensional material Sb2Se3: A DFT investigation of electronic and optical anisotropy19Stabilization of the Polar Structure and Giant Second‐Order Nonlinear Response of Single Crystal γ‐NaAs0.95Sb0.05Se219d6versus d10, Which Is Better for Second Harmonic Generation Susceptibility? A Case Study of K2TGe3Ch8 (T = Fe, Cd; Ch = S, Se)18Enhancement of birefringence and refractive index dispersion optimization from iodates to fluorooxoiodates1Evaluating refractive index and birefringence of nonlinear optical crystals: Classical methods and new developments45Large-size high-quality CdSe-OPO component for far IR laser output prepared by directional crystal growth technique8Recent progress in borate-based short-wavelength nonlinear optical crystals with boron–oxygen skeleton modification28Searching for silicate nonlinear optical materials by combining calculation and experiment17Two UV optical crystals with strong optical anisotropy, large band gaps and an α-BBO type structure7Visualizing the alignment of lone pair electrons in La 3 AsS 5 Br 2 and La 5 As 2 S 9 Cl 3 to form an acentric or centrosymmetric structure10Noncentrosymmetric γ-Cs2I4O11 Obtained from IO4 Polyhedral Rearrangements in the Centrosymmetric β-Phase16Rational Design of a Rare‐Earth Oxychalcogenide Nd3[Ga3O3S3][Ge2O7] with Superior Infrared Nonlinear Optical Performance64Recent advances of inorganic phosphates with UV/DUV cutoff edge and large second harmonic response7Target‐Driven Design of Deep‐UV Nonlinear Optical Materials via Interpretable Machine Learning125Sr6Ge3OSe11: A Rationally Designed Noncentrosymmetric Oxyselenide with Polar [GeOSe3] Building Blocks16Enhancement of second-order optical nonlinearities and nanoscale periodic domain patterning in ferroelectric boron-substituted aluminum nitride thin films16

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  1. Crystal growth and optical properties of a UV nonlinear optical material KSrCO 3 F

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  2. Crystal Growth and Linear and Nonlinear Optical Properties of KIO 3 ·Te(OH) 6

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  3. Finding the Next Deep-Ultraviolet Nonlinear Optical Material: NH4B4O6F

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  4. Deep-Ultraviolet Nonlinear-Optical Material K3Sr3Li2Al4B6O20F: Addressing the Structural Instability Problem in KBe2BO3F2

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

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

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  7. Noncentrosymmetric quaternary selenide Ba23Ga8Sb2Se38: Synthesis, structure, and optical properties

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  8. Viewpoint: Inorganic Materials for UV and Deep-UV Nonlinear-Optical Applications

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  9. Li2MnSnSe4: A New Quaternary Diamond‐Like Semiconductor with Nonlinear Optical Response and Antiferromagnetic Property

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  10. High-efficiency UV generation at 266 nm in a new nonlinear optical crystal NaSr_3Be_3B_3O_9F_4

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  11. More than 2017 Reasons We Appreciate Our Authors, Reviewers, and Readers

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  12. Ba 2 ZnSc(BO 3 ) 3 and Ba 4 Zn 5 Sc 2 (BO 3 ) 8 : first examples of borates in the Zn–Sc–B–O system featuring special structure configurations

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

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  14. Optimized oriented seed growth and optical properties of high-quality LiInSe 2 crystals

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

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  19. CaB5O7F3: A Beryllium-Free Alkaline-Earth Fluorooxoborate Exhibiting Excellent Nonlinear Optical Performances

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  20. Controlled Growth of Layered Acentric CdTeMoO6 Single Crystals with Linear and Nonlinear Optical Properties

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  21. Syntheses, Structures, and Properties of Non-Centrosymmetric Quaternary Tellurates BiMTeO6 (M = Al, Ga)

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  22. Two Novel Deep‐Ultraviolet Nonlinear Optical Crystals with Shorter Phase‐Matching Second Harmonic Generation than KBe2BO3F2: A First‐Principles Prediction

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  23. Advantageous Units in Antimony Sulfides: Exploration and Design of Infrared Nonlinear Optical Materials

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  24. Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates

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  25. Fluorooxoborates: Ushering in a New Era of Deep Ultraviolet Nonlinear Optical Materials

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  26. The must-have and nice-to-have experimental and computational requirements for functional frequency doubling deep-UV crystals

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  27. Module-Guided Design Scheme for Deep-Ultraviolet Nonlinear Optical Materials

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  28. Second-order nonlinear optical crystals with mixed anions

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  29. Adduct-Type IR Nonlinear-Optical Crystal SbI 3 ·(S 8 ) 3 with a Large Second-Harmonic Generation and a High Laser-Induced Damage Threshold

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  30. Czochralski Growth and Characterization of a Novel Nonlinear Optical Crystal Te2P2O9

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  31. Second-order nonlinear optical properties of CuGa In1-Se2 (x = 0.54): Experimental and theoretical investigations

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

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  34. Metal-free perovskites for non linear optical materials

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  35. Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation

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  36. SrCdGeS4 and SrCdGeSe4: Promising Infrared Nonlinear Optical Materials with Congruent-Melting Behavior

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  37. Crystallographic Investigations into the Polar Polymorphism of BaTeW2O9: Phase Transformation, Controlled Crystallization, and Linear and Nonlinear Optical Properties

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  38. KLi(HC 3 N 3 O 3 )·2H 2 O: Solvent-drop Grinding Method toward the Hydro-isocyanurate Nonlinear Optical Crystal

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  39. Ba10In6Zn7S26-nZnS: An Inorganic Composite System with Interface Phase-Matching Tuned for High-Performance Infrared Nonlinear Optical Materials

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  40. Module-Analysis-Assisted Design of Deep Ultraviolet Fluorooxoborates with Extremely Large Gap and High Structural Stability

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  41. Transformation of the B–O Units from Corner-Sharing to Edge-Sharing Linkages in BaMBO4 (M = Ga, Al)

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