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RESEARCH PAPER · Scientific Reports · 2016

Crystal growth and optical characteristics of beryllium-free polyphosphate, KLa(PO3)4, a possible deep-ultraviolet nonlinear optical crystal

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Crystal growth and optical characteristics of beryllium-free polyphosphate, KLa(PO3)4, a possible deep-ultraviolet nonlinear optical crystalOriginalKPb 2 (PO 3 ) 5 : a novel nonlinear optical lead polyphosphate with a short deep-UV cutoff edge109A New Deep-Ultraviolet Transparent Orthophosphate LiCs 2 PO 4 with Large Second Harmonic Generation Response384Strong Nonlinear-Optical Response in the Pyrophosphate CsLiCdP2O7 with a Short Cutoff Edge69LiRb 2 PO 4 : a new deep-ultraviolet nonlinear optical phosphate with a large SHG response95Study on growth, spectral, optical and thermal characterization of an NLO crystal: 6-Methyl nicotinic acid (6MNA)13Application of the dimensional reduction formalism to Pb 9−x Ba x [Li 2 (P 2 O 7 ) 2 (P 4 O 13 ) 2 ] (x = 0, 2, 6, 7): a series of phosphates with two types of isolated polyphosphate groups13Enhancing optical anisotropy of crystals by optimizing bonding electron distribution in anionic groups236Role of spin–orbit interaction on the nonlinear optical response of CsPbCO 3 F using DFT35Two Phosphates: Noncentrosymmetric Cs6Mg6(PO3)18 and Centrosymmetric Cs2MgZn2(P2O7)255M4Mg4(P2O7)3 (M = K, Rb): Structural Engineering of Pyrophosphates for Nonlinear Optical Applications238A3Sr2P7O21 (A = Rb, Cs): Two Polyphosphates Based on Different Types of P–O Chains and Ring Structures36(H 3 O)Ca 2 Zn 3.5 (PO 4 ) 4 and Ba 2 Cd 3 (PO 4 ) 2 (HPO 4 ) 2 : Syntheses, crystal structures and characterizations of two mixed metal phosphates12Li1.52Na4.48Cd8(PO4)2(P2O7)4: A new mixed-anion diphosphate containing four types of dimensions groups9A Joint Strategy To Evaluate the Microscopic Origin of the Second-Harmonic-Generation Response in Nonpolar ABCO3F Compounds32Recent advances in ultraviolet and deep-ultraviolet second-order nonlinear optical crystals257Deep-ultraviolet nonlinear optical materials: Development trend and innovative exploration16Non-centrosymmetric BaNaP3O9 with a short deep-ultraviolet cutoff edge14Two noncentrosymmetric polyphosphates featuring infinite one-dimensional (PO3)∞ chain, LiMP2O6 (M = Rb, Cs): Synthesis, structure and optical properties8ALiZnP2O7 (A = Rb, Cs): Two Mixed Alkali Zinc Pyrophosphates Featuring a [Li2Zn2P4O20]14– Anionic Skeleton34A Langbeinite-Type Yttrium Phosphate LiCs2Y2(PO4)336Ba2NaClP2O7: Unprecedented Phase Matchability Induced by Symmetry Breaking and Its Unique Fresnoite-Type Structure245Theoretical Investigation of Difluoroboron Complex of Curcuminoid Derivatives with and without Phenyl Substituent (at Meso Position): Linear and Non‐Linear Optical Study9BaPO3Cl: a Metal Phosphate Chloride with Infinite [PO3]∞ Chains25A UV Transmittable NLO crystal Hydrofluoric Acid Mixed Sulphamic acid (FASA) : Synthesis, Growth and Characterization0Experimental characterization and first principles calculations of linear and nonlinear optical properties of two orthophosphates A 3 Al 2 (PO 4 ) 3 (A = Rb, K)36A 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 materials98Growth and theoretical study on the deep-ultraviolet transparent β-CsBa 2 (PO 3 ) 5 nonlinear optical crystal10K 2 SrP 4 O 12 : a deep-UV transparent cyclophosphate as a nonlinear optical crystal79Structural and optical characterization of RbLaP4O12:Ln3+ (Ln3+ = Ce3+, Nd3+, Tm3+, or Yb3+)2Syntheses, crystal structures, and characterizations of three new pyrophosphates CsNaZnP2O7, RbNaZnP2O7, and RbLiMgP2O710Na 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 birefringence49Syntheses, structures and characterization of non-centrosymmetric Rb 2 Zn 3 (P 2 O 7 ) 2 and centrosymmetric Cs 2 M 3 (P 2 O 7 ) 2 (M = Zn and Mg)26Synthesis, structure and characterization of three new Mg-containing phosphates with deep-UV cut-off edges9Tellurium–oxygen group enhanced birefringence in tellurium phosphates: a first-principles investigation4Three 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 edges26Ultraviolet nonlinear optical crystal: (NH4)ZnPO47Synthesis, Crystal Structure, and Characterization of a Noncentrosymmetric Sulfate Cs2Ca2(SO4)320The first rare-earth lead phosphates Pb3AP3O12 (A=Sc, Gd) with remarkable SHG enhancement8Noncentrosymmetric Orthophosphate YM3(PO4)3 (M = Sr, Ba) Crystals: Single Crystal Growth, Structure, and Properties34Synthesis, characterizations and theoretical analysis of a noncentrosymmetric sulfate8KLaP4O12:Tb3+ Nanocrystals for Luminescent Thermometry in a Single-Band-Ratiometric Approach60Single crystal growth, optical absorption and luminescence properties under VUV-UV synchrotron excitation of type III Pr3+:KGd(PO3)49Two 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 Materials29Synthesis, growth and characterization of N, N-dimethyl-4-[2-(2-quinolyl) vinyl] aniline (DADMQ): An SHG material for NLO applications13Bi 32 Cd 3 P 10 O 76 : a new congruently melting nonlinear optical crystal with a large SHG response and a wide transparent region24Nonlinear 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 Birefringence13Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering144Computationally assisted multistage design and prediction driving the discovery of deep-ultraviolet nonlinear optical materials41To improve the key properties of nonlinear optical crystals assembled with tetrahedral functional building units46Ba3Sb2(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 groups106M(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 Birefringence27[C(NH2)3]3PO4·2H2O: A new metal-free ultraviolet nonlinear optical phosphate with large birefringence and second-harmonic generation response70AZn(PO3)3 (A = K, Rb): Deep-Ultraviolet Nonlinear Optical Phosphates Derived from Synergy of a Unique [ZnO6] Octahedron and a [PO3]∞ Chain25Struvite-type AMgPO4·6H2O (A = NH4, K): Two Natural Deep-Ultraviolet Transparent Nonlinear Optical Crystals13Insights into varying dimension structures for deep-UV optical crystals NaBa2Al(P2O7)2 and NaBaAl(PO4)2 constructed separately from unique [Al(P2O7)2] chains and [Al(PO4)2] layers6Recent advances in nonlinear optical rare earth structures63Two Tellurium(IV)-Based Sulfates Exhibiting Strong Second Harmonic Generation and Moderate Birefringence as Promising Ultraviolet Nonlinear Optical Materials28A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**175A General Principle for DUV NLO Materials: π‐Conjugated Confinement Enlarges Band Gap**27Tin(II)-Induced Large Birefringence Enhancement in Metal Phosphates22Recent Development of Non-π-Conjugated Deep Ultraviolet Nonlinear Optical Materials106K 2 (BeS)O 4 F 2 : a novel fluorosulfate with unprecedented 1D [(BeO 3 F)–(SO 3 F)] ∞ chains exhibiting large birefringence10Nain(C2o4)(Hpo4)(H2o)5: An Ultraviolet Transparent Nonlinear Optical Oxalate-Phosphate with Large Birefringence0CsY(SO4)2·4H2O: A Deep-Ultraviolet Birefringent Crystal Induced by an Edge-Sharing Connection26A2BeS2O8 (A = NH4, K, Rb, Cs) Deep Ultraviolet Nonlinear Optical Crystals33Two Metal Phosphate Nonlinear Optical Materials Simultaneously Exhibiting Ultraviolet Transparence and a Large Birefringence50Synthesis, crystal structure, and characterization of two bismuth phosphates Rb2CaBi2P4O15 and Rb3SrBiP4O143From Phosphate Fluoride to Fluorophosphate: Design of Novel Ultraviolet/Deep-Ultraviolet Nonlinear Optical Materials for BePO3F with Optical Property Enhancement34Phosphites: A Nonlinear Optical Materials System with a Wide Band Gap and Moderate Second-Harmonic Generation Effect27Cadmium phosphates with two types of fundamental building units and a wide ultraviolet transparency window1Anisotropic structure building unit involving diverse chemical bonds: a new opportunity for high-performance second-order NLO materials181Co-substitution design: a new glaserite-type rare-earth phosphate K 2 RbSc(PO 4 ) 2 with high structural tolerance6Enhancing birefringence of non-π-conjugated sulfate systems through rare-earth metal-centered polyhedra10New Ultraviolet Nonlinear Optical Crystal Rb3Hg2(SO4)3Cl3Recent advances of inorganic phosphates with UV/DUV cutoff edge and large second harmonic response7Spatial Frequency Manipulation of a Quartz Crystal for Phase‐Matched Second‐Harmonic Vacuum Ultraviolet Generation16Design Principles for Noncentrosymmetric Materials23Novel LiCa(PO3)3 and LiSr(PO3)3 microwave dielectric ceramics38Deep‐Ultraviolet Transparent Mixed Metal Sulfamates with Enhanced Nonlinear Optical Properties and Birefringence11Deep‐Ultraviolet Transparent Mixed Metal Sulfamates with Enhanced Nonlinear Optical Properties and Birefringence75NH4Y(SO4)2·H2O and NH4YSO4F2: Two New Ammonium‐Rare Earth Metal Sulfates with Enhanced Optical Anisotropy and Deep Ultraviolet Transmission3Investigation on Physicochemical Properties of Nonlinear Optical (NLO) Single Crystal: Rubidium Hydrogen Fumarate5K0.9Rb2.1B8PO16: Design and Synthesis of a Deep-Ultraviolet Nonlinear Optical Crystal with Balanced Performance Derived from π-Conjugated and Non-π-Conjugated Groups11Structure and optical properties of alkali rare-earth double phosphates of M3RE(PO4)2 (M = K, Rb; RE = Y, La, and Lu)4Deep‐Ultraviolet Transparent Nonlinear Optical Phosphates: A New Alternative to Conventional Borates9A 3 Sc(PO 4 ) 2 (A = Li, Na): rare earth cations effectively regulate phosphate structures for enhanced birefringence4Four noncentrosymmetric molybdophosphates discovered by a chemical substitution strategy4Chiral-Unit-Oriented Design of Non-π-Conjugated Noncentrosymmetric Phosphates with Short Absorption Edges4Na3Y2F3P2O8 and K4Y3F5P4O14: [YOF] Polyhedra Inducing Birefringence Enhancement in Non-π-Conjugated Phosphate Systems3Designing a 3‐Hydroxypropane‐1‐Sulfonate Deep‐Ultraviolet Nonlinear Optical Crystal9(NH4)Na3Zn4(PO4)4:An open-framework zincophosphate exhibiting well-balanced optical and thermal performance1The Layered Structure–Induced Enhanced Birefringence of LiMgPO 4 : A First‐Principles Investigation1Tuning the Anionic Configuration in ASc2(P2O7)2 (A = Ba, Pb) through A-Site Cationic Coordination Engineering0Ba 3 (MoO 2 F 3 )PO 4 F 2 : Rational Design and Synthesis of an Alkaline-Earth Phosphate Fluoride as a Birefringent Crystal1Sn 4+ /Sn 2+ Aliovalent Substitution: A Strategy for Local Structure Engineering to Enhance Birefringence and Trigger Structural Symmetry Transition0Potential Deep Ultraviolet Phosphate With Y‐Based: 1 [(PO 3 ) 4 ] ∞ Chains AYP 4 O 12 (A = K, NH 4 ) and the First [P 3 O 10 ] Anionic Framework KLiYP 3 O 100

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  48. Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence

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    Xinyuan Zhang, Lei Kang, Pifu Gong, Zheshuai Lin, Yicheng Wu

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  49. Nonlinear Optical Oxythiophosphate Approaching the Good Balance with Wide Ultraviolet Transparency, Strong Second Harmonic Effect, and Large Birefringence

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  50. Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering

    Materials Horizons · 2021-01-01

    Dajiang Mei, Wangzhu Cao, Naizheng Wang, Xingxing Jiang, Jun Zhao, Weikang Wang, Junhui Dang, Shiyan Zhang, Yuandong Wu, Pinhua Rao, Zheshuai Lin

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