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RESEARCH PAPER · Inorganic Chemistry · 2011

Structure Change Induced by Terminal Sulfur in Noncentrosymmetric La 2 Ga 2 GeS 8 and Eu 2 Ga 2 GeS 7 and Nonlinear-Optical Responses in Middle Infrared

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Structure Change Induced by Terminal Sulfur in Noncentrosymmetric La 2 Ga 2 GeS 8 and Eu 2 Ga 2 GeS 7 and Nonlinear-Optical Responses in Middle InfraredOriginalOxygen, sulfur, selenium, tellurium and polonium0Solvothermal syntheses and characterizations of lanthanide(iii)/SbS43− complexes associated by a dien ligand: A detailed study based on the lanthanide contraction effect18The first μ-Ge2Se8 ligand to lanthanide(iii) centers: solvothermal syntheses and characterizations of lanthanide selenidogermanate complexes with a pentadentate polyamine as a co-ligand14ChemInform Abstract: Structure Change Induced by Terminal Sulfur in Noncentrosymmetric La2Ga2GeS8 and Eu2Ga2GeS7 and Nonlinear‐Optical Responses in Middle Infrared.0Disconnection Enhances the Second Harmonic Generation Response: Synthesis and Characterization of Ba23Ga8Sb2S38247Syntheses, Structures, Optical and Magnetic Properties of Ba2MLnSe5(M = Ga, In;Ln= Y, Nd, Sm, Gd, Dy, Er)54Sulfides with Strong Nonlinear Optical Activity and Thermochromism: ACd4Ga5S12 (A = K, Rb, Cs)172Ba3LnInS6 (Ln = Pr, Sm, Gd, Yb) and Ba2LnGaS5 (Ln = Pr, Nd): Syntheses, Structures, and Magnetic and Optical Properties35Syntheses, Structures, Physical Properties, and Electronic Structures of Ba2MLnTe5(M = Ga and Ln = Sm, Gd, Dy, Er, Y; M = In and Ln = Ce, Nd, Sm, Gd, Dy, Er, Y)38Molecular Germanium Selenophosphate Salts: Phase-Change Properties and Strong Second Harmonic Generation85Oxygen, sulfur, selenium, tellurium and polonium3Heterometallic Clusters [CuSn3S9]5− and [Cu6Sn6S20]10−: Solvothermal Synthesis and Characterization of 4f–3d Thiostannates26Synthesis, Crystal Structure, Magnetic Property, and Electronic Structure of Ba2YbInSe56Syntheses, Structures, and Nonlinear Optical Properties of Quaternary Chalcogenides: Pb4Ga4GeQ12 (Q = S, Se)60Functionalization Based on the Substitutional Flexibility: Strong Middle IR Nonlinear Optical Selenides AXII4XIII5Se12219Konsequenzen der modernen Germaniumchemie1Ba8Sn4S15: A Strong Second Harmonic Generation Sulfide with Zero-Dimensional Crystal Structure106New Quaternary Rare-Earth Chalcogenides BaLnSn2Q6 (Ln = Ce, Pr, Nd, Q = S; Ln = Ce, Q = Se): Synthesis, Structure, and Magnetic Properties30Synthesis, Structure and Bonding, Optical Properties of Ba4MTrQ6 (M=Cu, Ag; Tr=Ga, In; Q=S, Se)18Solvothermal syntheses of lanthanide thiogermanates displaying three new structural moieties17Syntheses, Structures, and Nonlinear-Optical Properties of Metal Sulfides Ba2Ga8MS16 (M = Si, Ge)94A series of new lanthanoid thioarsenates: insights into the influence of lanthanide contraction on the formation of new lanthanoid thioarsenates25PbGa2MSe6 (M = Si, Ge): Two Exceptional Infrared Nonlinear Optical Crystals131Second Harmonic Generation Response Optimized at Various Optical Wavelength Ranges through a Series of Cubic Chalcogenides Ba6Ag2.67+4δSn4.33−δS16–xSex41Synthesis and Characterization of Mid-Infrared Transparency Compounds: Acentric BaHgS2 and Centric Ba8Hg4S5Se752Syntheses, crystal structures, and NLO properties of the quaternary sulfides RE3Sb0.33SiS7 (RE=La, Pr)24Na4MgM2Se6 (M = Si, Ge): The First Noncentrosymmetric Compounds with Special Ethane-like [M2Se6]6– Units Exhibiting Large Laser-Damage Thresholds56Crystal and electronic structures, and photoluminescence and photocatalytic properties of α-EuZrS 326Pb 5 Ga 6 ZnS 15 : a noncentrosymmetric framework with chains of T2-supertetrahedra41(Cs6Cl)6Cs3[Ga53Se96]: A Unique Long Period-Stacking Structure of Layers Made from Ga2Se6 Dimers via Cis or Trans Intralayer Linking12Synthesis of heterometallic chalcogenides containing lanthanide and group 13–15 metal elements94Syntheses and structural characterization of non-centrosymmetric Na2M2M'S6 (M, M′=Ga, In, Si, Ge, Sn, Zn, Cd) sulfides36Recent achievements on middle and far-infrared second-order nonlinear optical materials433Ba 6 Li 2 CdSn 4 S 16 : lithium substitution simultaneously enhances band gap and SHG intensity44Two new phases in the ternary RE–Ga–S systems with the unique interlinkage of GaS 4 building units: synthesis, structure, and properties16Mid-Infrared Nonlinear Optical Materials Based on Metal Chalcogenides: Structure–Property Relationship338Structure of rare-earth chalcogenide glasses by neutron and x-ray diffraction6Na2ZnSn2S6: A mixed-metal thiostannate with large second-harmonic generation response activated by penta-tetrahedral [ZnSn4S14]10− clusters10Na 6 Zn 3 MIII2Q 9 (M III = Ga, In; Q = S, Se): four new supertetrahedron-layered chalcogenides with unprecedented vertex-sharing T 3 -clusters and desirable photoluminescence performances31NaBaM III Q 3 (M III = Al, Ga; Q = S, Se): first quaternary chalcogenides with isolated edge-sharing (MIII2Q 6 ) 6− dimers8A Series of Lanthanide Selenidogermanates: The First Coexistence of Three Types of Selenidogermanate Units in the Same Architecture10BaB2S4: An Efficient and Air-Stable Thioborate as Infrared Nonlinear Optical Material with High Laser Damage Threshold85Two rare-earth-based quaternary chalcogenides EuCdGeQ 4 (Q = S, Se) with strong second-harmonic generation66Effect of S and Se replacement on electronic and thermoelectric features of BaCu2GeQ4 (Q = S, Se) chalcogenide crystals27A highly distorted HgS 4 tetrahedron-induced moderate second-harmonic generation response of EuHgGeS 462New quaternary chalcogenide Ba 4 HgAs 2 S 10 originating from the combination of linear [HgS 2 ] 2− and tetrahedral [AsS 4 ] 3− modules8Quaternary rare-earth sulfide LaSnGa3S7: Synthesis, structure, thermal and optical properties5Crystal chemistry, second-order nonlinear optical, and magnetic properties of Eu8Sn4Se2014EuHgGeSe 4 and EuHgSnS 4 : Two Quaternary Eu-Based Infrared Nonlinear Optical Materials with Strong Second-Harmonic-Generation Responses55Applying band gap engineering to tune the linear optical and nonlinear optical properties of noncentrosymmetric chalcogenides La 4 Ge 3 Se x S 12− x ( x = 0, 2, 4, 6, 8, 10)21Breaking through the “3.0 eV wall” of energy band gap in mid-infrared nonlinear optical rare earth chalcogenides by charge-transfer engineering145Unique Unilateral-Chelated Mode-Induced d–p−π Interaction Enhances Second-Harmonic Generation Response in New Ln3LiMS7 Family41Recent advances in nonlinear optical rare earth structures63Rational combination of multiple structural groups on regulating nonlinear optical property in hexagonal Ln3MGeS7 polar crystals10Pb 4 SeBr 6 : A Congruently Melting Mid‐Infrared Nonlinear Optical Material with Excellent Comprehensive Performance39Heteroanionic Melilite Oxysulfide: A Promising Infrared Nonlinear Optical Candidate with a Strong Second-Harmonic Generation Response, Sufficient Birefringence, and Wide Bandgap65First-principles investigations of metal chalcogenides Tl2Hg3X4(X=S,Se,Te) for advanced optoelectronic and thermoelectric applications20Eu 2 P 2 S 6 : The First Rare‐Earth Chalcogenophosphate Exhibiting Large Second‐Harmonic Generation Response and High Laser‐Induced Damage Threshold144Eu2P2S6: The First Rare‐Earth Chalcogenophosphate Exhibiting Large Second‐Harmonic Generation Response and High Laser‐Induced Damage Threshold7Enlightening the stability and optoelectronic properties of Ba2MLnSe5 (M = Ga, In; Ln = Y, Nd, Sm, Gd, Dy, Er) semiconductors: A first-principles study3Rational Design of a Rare‐Earth Oxychalcogenide Nd3[Ga3O3S3][Ge2O7] with Superior Infrared Nonlinear Optical Performance64Synthesis, Structure, and optical properties of Y3GaGe0.5S7: A new member in the polar R3MTQ7 family4Rare-earth-based chalcogenides and their derivatives: an encouraging IR nonlinear optical material candidate70Evaluation and prospect of Mid-Infrared nonlinear optical materials in f0 rare earth (RE = Sc, Y, La) chalcogenides45LaMg6Ga6S16: a chemical stable divalent lanthanide chalcogenide70Exploring the electronic, optical, and thermoelectric features of BaXCu 3 Se 4 (X = In, Tl) quaternary chalcogenides: first-principles study10A Rare Earth Chalcogenide Nonlinear Optical Crystal KLaGeS4: Achieving Good Balance among Band Gap, Second Harmonic Generation Effect, and Birefringence13Insights into the optoelectronic, thermodynamic, and thermoelectric properties of novel BaYCuX3 (X = Se, Te) semiconductors from first-principles investigation3First-Principles Study of Novel BaLnAgSe3 (Ln = Er, Gd) Active UV-reflecting Materials for Optoelectronic and Thermoelectric Applications5Realizing Excellent Infrared Nonlinear Optical Performance in Eu-Based Chalcogenides via Rational Cross Substitution Strategy26The electronic structure, optical, and transport properties of novel SrScCu3M4 (M = Se, Te) semiconductors4Cationic substitution engineering induces a new quaternary chalcogenide in the A–M IIIA –M IVA –Q system for optical crystal applications1Non-centrosymmetric Y3FeGaSe7 and Y3Mn0·5SiSe7 with extremely low thermal conductivities2Doubling Polarizability Anisotropy of The Tetrahedral Motifs to Achieve Phase Matching for Melilite-Type Compound2From Centrosymmetric Eu 2 Ga 2 S 5 to Noncentrosymmetric EuMg 6 Ga 6 S 16 via Introduction of Distorted MgS 6 Octahedron: Featuring Wide Bandgap and Nonlinear Optical Activity3Ba 10 Zn 7 Ga 6 S 26 : Promising Infrared Nonlinear Optical Crystal Exhibiting a High Laser Damage Threshold0Antibonding States Drive Anharmonicity and Low Thermal Conductivity in Edge-Sharing Metal Chalcogenides4Mixed chalcogenidogermanates: solvothermal synthesis of tetranuclear oxotellurogermanate clusters and photocatalytic performance0Salt-Inclusion Rare-Earth Chalcogenides: Exploring Infrared Nonlinear Optical Crystals via a Guest-Framework Modulation Strategy0EuMn6Ga6S16: A Wide Bandgap Europium-Based Nonlinear Optical Sulfide0

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