Crystal structure and electrical properties of the mixed valent titanium oxysulfide Sm2Ti2S2O4.5

A new phase Sm₂Ti₂S₂O_4.5 was synthesized and its crystal structure was solved by single-crystal X-ray diffraction. This compound crystallizes in the monoclinic system (C2/m) with lattice constants a=17.9987(11) Å, b=3.71607(14) Å, c=12.6172(8) Å and β=133.645(4)°. The structure is built up from double chains of Ti-centered octahedra between which Sm-polyhedra develop. In spite of very close formulations, the structure of Sm₂Ti₂S₂O_4.5 differs completely from that of the defect Ruddelsden-Popper phase Sm₂Ti₂S₂O₅ previously reported. The title compound presents a mixed valence for titanium with Ti(III) (d¹) and Ti(IV) (d⁰) located in different crystallographic sites. However, conductivity measurements show that this compound is non-metallic.     

Processing and characterization of new oxysulfide glasses in the Ge-Ga-As-S-O system

New oxysulfide glasses have been prepared in the Ge-Ga-As system employing a two-step melting process which involves the processing of the chalcogenide glass (ChG) and its subsequent melting with amorphous GeO₂ powder. Optical characterization of the synthesized oxysulfide glasses has shown that the cut-off wavelength decreases with increasing oxygen content, and this has been correlated to results of Raman and infrared (IR) spectroscopies which show the formation of new oxysulfide structural units. X-ray photoelectron spectroscopy (XPS) analysis to probe the bonding environment of oxygen atoms in the oxysulfide glass network, has revealed the preferred formation of Ga-O and Ge-O bonds in comparison to As-O bonds. This work has demonstrated that melting a ChG glass with GeO₂ leads to the formation of new oxysulfide glassy materials.     

Processing and characterization of new passive and active oxysulfide glasses in the Ge-Ga-Sb-S-O system

New passive and active oxysulfide glasses have been prepared in the Ge-Ga-Sb-S-O system employing a two-step melting process which involves the processing of the chalcogenide glass (ChG) and its subsequent melting with amorphous GeO₂ or Sb₂O₃ powder. Optical characterization of the oxysulfide glasses has shown that the UV cut-off wavelength decreases with increasing oxygen content. Using Raman spectroscopy, correlations have been made between the formation of new Ge- and Sb-based oxysulfide structural units, the Sb content and the O/S ratio. We demonstrate the successful processing of active rare earth doped oxysulfide glasses by melting the chalcogenide glass with Er₂O₃ and Sb₂O₃ and also by melting the Er³⁺ doped chalcogenide glass with Sb₂O₃. Modification of the emission spectra at 1500 nm of Er³⁺ doped samples with the introduction of oxygen revealed that Er³⁺ most likely exists in dual O- and S-neighbor environments. Finally, the photo-response of these new glasses upon near-IR femtosecond laser irradiation has been investigated as a function of Sb content and O/S ratio and shows that the glasses are photo-sensitive to NIR fs laser light with the magnitude of the photo-sensitivity dependent on the glass’ Sb content and O/S ratio.     

Eu<Superscript>3+</Superscript> doped yttrium oxysulfide quantum structures—structural,optical and electronic properties

Small particles of trivalent europium doped yttrium oxysulfide nanocrystals (ϕ ∼ 7 nm) were synthesized using sol–gel polymer thermolysis. The nanocrystals show significant change in the excitation bands corresponding to fundamental absorption and charge transfer absorption bands. The optical spectra essentially comprise of two parts: fundamental absorption (∼260 nm) and Eu³⁺–X²⁻ ligand (O²⁻/S²⁻) charge transfer (∼290 nm) bands. They show significant blue shifts (0.24–0.30 eV), respectively, with respect to the bulk counterpart. These may be explained by considering possible size dependent changes associated with quantum confinement effect in this large bandgap semiconductor system. FT-IR spectra revealed the difference in chemisorbed species between bulk and nanocrystalline samples. The results of the solid-state photo-induced electrical impedance spectroscopy studies are reported.     

Y2O2S:Eu nanocrystals, a strong quantum-confined luminescent system

Trivalent europium-doped yttrium oxysulfide nanocrystals synthesized using sol-gel thermolysis show significant blue shifts in the excitation bands corresponding to fundamental absorption, charge-transfer absorption. A significant blue shift observed in the fundamental absorption edge for the nanocrystals having an average crystallite size (φ) in the range 9-15 nm indicates a strong quantum confinement with a Bohr exciton radius of 5-13 nm. Also, the diffuse reflectance spectra and the corresponding Kubelka-Munk plot indicate the possibility of profound decrease in the absorption coefficient of Eu³⁺-ligand charge-transfer species necessitating further studies in this wide-gap semiconductor nanocrystalline system.     

Sr6Cd2Sb6O7S10: Strong SHG Response Activated by Highly Polarizable Sb/O/S Groups

A new nonlinear optical (NLO) oxysulfide, Sr₆Cd₂Sb₆O₇S₁₀, which contains the functional groups [SbO_xS_5?x]^7? (x=0, 1) with a 5s² electron configuration, is synthesized by a solid‐state reaction. This compound displays a phase‐matchable second harmonic generation (SHG) response four times stronger than AgGaS₂ (AGS) under laser irradiation at 2.09 μm. Single‐crystal‐based optical measurements reveal a SHG intensity that can be tuned by temperature and novel photoluminescence properties. Theoretical analyses demonstrate that tetragonal [SbOS₄]^7? and [SbS₅]^7? pyramids make the predominant contribution to the enhanced SHG effect. Among those, the [SbOS₄]^7? units with mixed anions make a larger contribution. This work proposes that oxysulfide groups with an ns² electron configuration can serve as new functional building units in NLO materials and opens a new avenue for the design of other optoelectronic materials.     

Synthesis and electrochemical characteristics of oxysulfide spinel material for lithium secondary batteries

Oxysulfide spinel LiMn₂O_3.98S_0.02 powders with monodispersed, and highly homogeneous particles were synthesized by a sol-gel method using an aqueous solution of metal acetates and sulfide containing glycolic acid as a chelating agent. The oxysulfide spinel, LiMn₂O_3.98S_0.02 electrode initially delivers 80 mAh g⁻¹, steadily increases during cycling, and reaches 99 mAh g⁻¹ at the 20th cycle. The substitution of a small amount S for O in LiMn₂O₄ spinel helps to maintain structural integrity during cycling, which then overcomes the Jahn–Teller distortion in the spinel Mn phase in the 3 V region.     

Photoexpansion and photobleaching effects in oxysulfide thin films of the GeS2+Ga2O3 system

Oxysulfide systems undergo structural transformations upon illumination with laser light of near bandgap energy, as well as chalcogenide materials (glasses and films). In this paper, photoinduced effects such as photoexpansion and photobleaching were observed in GeS₂+Ga₂O₃ (GGSO) films synthesized by electron beam evaporation. A surface expansion of the thin films and a shift to shorter wavelengths of the optical absorption edge were observed as a result of UV laser irradiation (wavelength of 351 nm) and they are dependent on laser power density, exposure time and film composition. These parameters were varied to evaluate and enhance the observed effects. In addition, the irradiated GGSO samples exhibited a decrease in refractive index, measured with a prism-coupling technique, which makes these films suitable candidates for applications as gratings and waveguides in integrated optics.     

Solution preparation of the amorphous molybdenum oxysulfide MoOS2 and its use for catalysis

Acid condensation of aqueous MoO₂S₂²⁻ anion yields amorphous MoOS₂ oxysulfide. This compound possesses tubular morphology and when freshly precipitated is soluble in polar organics such as acetone and ethanol. The ensemble of characterizations (IR, UV-visible, EXAFS spectroscopy) suggests that it contains cyclic or short linear oligomers of neutral molybdenum (V) oxysulfide MoOS₂ core. Thermal decomposition of MoOS₂ under inert atmosphere leads to the formation of a mixture of MoO₂ and MoS₂ phases. Promotion of MoOS₂ with cobalt followed by sulfidation leads to highly active HDS catalysts.