Sr6 Cd2 Sb6 O7 S10 : Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups.

[1]  K. Fujii,et al.  Function of Tetrahedral ZnS3O Building Blocks in the Formation of SrZn2S2O: A Phase Matchable Polar Oxysulfide with a Large Second Harmonic Generation Response , 2018, Chemistry of Materials.

[2]  C. Zheng,et al.  Observation of High Seebeck Coefficient and Low Thermal Conductivity in [SrO]-Intercalated CuSbSe2 Compound , 2018, Chemistry of Materials.

[3]  Zhihua Yang,et al.  Expanding Frontiers of Ultraviolet Nonlinear Optical Materials with Fluorophosphates , 2018, Chemistry of Materials.

[4]  F. Liang,et al.  Rational Design of the First Lead/Tin Fluorooxoborates MB2O3F2 (M = Pb, Sn), Containing Flexible Two-Dimensional [B6O12F6]∞ Single Layers with Widely Divergent Second Harmonic Generation Effects. , 2018, Journal of the American Chemical Society.

[5]  F. Liang,et al.  M2B10O14F6 (M = Ca, Sr): Two Noncentrosymmetric Alkaline Earth Fluorooxoborates as Promising Next-Generation Deep-Ultraviolet Nonlinear Optical Materials. , 2018, Journal of the American Chemical Society.

[6]  Zhihua Yang,et al.  CsB4 O6 F: A Congruent-Melting Deep-Ultraviolet Nonlinear Optical Material by Combining Superior Functional Units. , 2017, Angewandte Chemie.

[7]  K. Poeppelmeier,et al.  Finding the Next Deep-Ultraviolet Nonlinear Optical Material: NH4B4O6F. , 2017, Journal of the American Chemical Society.

[8]  A. Reshak Spin-polarized Second Harmonic Generation from the Antiferromagnetic CaCoSO Single Crystal , 2017, Scientific Reports.

[9]  Zhihua Yang,et al.  Fluorooxoborates: Beryllium-Free Deep-Ultraviolet Nonlinear Optical Materials without Layered Growth. , 2017, Angewandte Chemie.

[10]  F. Liang,et al.  Mid-Infrared Nonlinear Optical Materials Based on Metal Chalcogenides: Structure–Property Relationship , 2017 .

[11]  Yan-Yan Li,et al.  Tailored synthesis of nonlinear optical quaternary chalcohalides: Ba4Ge3S9Cl2, Ba4Si3Se9Cl2 and Ba4Ge3Se9Cl2. , 2017, Dalton transactions.

[12]  C. Zheng,et al.  Semiconductive K2MSbS3(SH) (M = Zn, Cd) Featuring One-Dimensional ∞1[M2Sb2S6(SH2)]4- Chains. , 2016, Inorganic chemistry.

[13]  Huaidong Jiang,et al.  BaCdSnS4 and Ba3CdSn2S8: syntheses, structures, and non-linear optical and photoluminescence properties. , 2016, Dalton transactions.

[14]  T. McQueen,et al.  Synthesis and Structure of Three New Oxychalcogenides: A2O2Bi2Se3 (A = Sr, Ba) and Sr2O2Sb2Se3 , 2016 .

[15]  G. Guo,et al.  Oxychalcogenide BaGeOSe2: Highly Distorted Mixed-Anion Building Units Leading to a Large Second-Harmonic Generation Response , 2015 .

[16]  Ling Chen,et al.  Noncentrosymmetric inorganic open-framework chalcohalides with strong middle IR SHG and red emission: Ba3AGa5Se10Cl2 (A = Cs, Rb, K). , 2012, Journal of the American Chemical Society.

[17]  Khaled M. Elsabawy,et al.  Infrared spectra, Raman laser, XRD, DSC/TGA and SEM investigations on the preparations of selenium metal, (Sb2O3, Ga2O3, SnO and HgO) oxides and lead carbonate with pure grade using acetamide precursors , 2011 .

[18]  T. K. Bera,et al.  Soluble semiconductors AAsSe2 (A = Li, Na) with a direct-band-gap and strong second harmonic generation: a combined experimental and theoretical study. , 2010, Journal of the American Chemical Society.

[19]  N. N. Petrishchev,et al.  Medical applications of mid-IR lasers. Problems and prospects , 2010 .

[20]  T. K. Bera,et al.  Strong second harmonic generation from the tantalum thioarsenates A3Ta2AsS11 (A = K and Rb). , 2009, Journal of the American Chemical Society.

[21]  T. K. Bera,et al.  Soluble direct-band-gap semiconductors LiAsS2 and NaAsS2: large electronic structure effects from weak As...S interactions and strong nonlinear optical response. , 2008, Angewandte Chemie.

[22]  Yongfang Li,et al.  Controlled Synthesis and Optical Properties of Colloidal Ternary Chalcogenide CuInS2 Nanocrystals , 2008 .

[23]  P. Halasyamani,et al.  Structure and physical properties of the polar oxysulfide CaZnOS. , 2007, Inorganic chemistry.

[24]  J. Aitken,et al.  Phase transitions and second-harmonic generation in sodium monothiophosphate. , 2006, Inorganic chemistry.

[25]  A. Assoud,et al.  Synthesis, Structure, and Electronic Structure of the Ternary Sulfide La7Sb9S24 , 2006 .

[26]  C. Stern,et al.  Examining the out-of-center distortion in the [NbOF5]2- anion. , 2005, Inorganic chemistry.

[27]  P. Maggard,et al.  Alignment of acentric MoO3F33− anions in a polar material: (Ag3MoO3F3)(Ag3MoO4)Cl , 2003 .

[28]  S. Setzler,et al.  Temperature and pulse-duration dependence of second-harmonic generation in CdGeAs2. , 2002, Applied optics.

[29]  A. Fried,et al.  Development of a tunable mid-IR difference frequency laser source for highly sensitive airborne trace gas detection , 2002, Applied physics. B, Lasers and optics.

[30]  Konstantin L. Vodopyanov,et al.  Tunable middle infrared downconversion in GaSe and AgGaS2 , 1998 .

[31]  Ouali Acef,et al.  Absolute value of the d 36 nonlinear coefficient of AgGaS 2 : prospect for a low-threshold doubly resonant oscillator-based 3:1 frequency divider , 1997 .

[32]  G. D. Boyd,et al.  Linear and nonlinear optical properties of some ternary selenides , 1972 .

[33]  G. Boyd,et al.  LINEAR AND NONLINEAR OPTICAL PROPERTIES OF ZnGeP2 AND CdSe , 1971 .

[34]  S. K. Kurtz,et al.  A powder technique for the evaluation of nonlinear optical materials , 1968 .

[35]  W. Braun,et al.  Principles and Techniques of Diffuse‐Reflectance Spectroscopy , 1963 .