Multiphonon absorption in As2S3As2Se3 glasses

Multiphonon absorption in As₂S₃ and As₂Se₃ glasses is well explained by a molecular model in terms of combination bands of high frequency vibrational modes of pyramidal AsY₃ and bent AsYAs groups (Y = SorSe). Multiphonon absorption coefficients in mixed As₂S₃As₂Se₃ glasses are nearly additive in terms of the pure components, suggesting a high degree of non-random mixing.     

Infrared properties of AsχTe1−χ glasses

Infrared reflection and transmission measurements in As_χTe_1?χ glasses (45?×?55) show well-defined Gaussian vibrational absorption peaks. Comparisons with spectra observed in crystalline and glassy As₂S₃ and As₂Se₃ indicate that the local order in As_χTe_1?χ glasses is not like that found in crystalline As₂Te₃, but rather it consists primarily of AsTe₃ pyramids which are probably linked together in a fashion similar to that found in As₂S₃ and As₂Se₃.     

Urbach tails and the structure of chalcogenide glasses

A novel analysis of optical absorption tails of inorganic network glasses is shown to provide important information on the structure of the glass. The anomalous composition and temperature dependence of absorption tails in Ge_xSe_1?x and As_xSe_1?x systems indicate that these glasses retain locally layered structures at particular stoichiometries corresponding to GeSe₂ and As₂Se₃, and a reversible structural change is taking place well below the glass transition temperature. A phenomenological model for the absorption tail slope of glasses is proposed, analogous to the Urbach rule for crystalline materials.     

Highly nonlinear chalcogenide fibres for all-optical signal processing

Chalcogenide glasses offer many attractive properties for all-optical signal processing including large Kerr nonlinearity (up to 500 × silica glass), an intrinsic ultrafast response time and low to moderate two-photon absorption (TPA). These properties together with the convenience of a fibre format allow us to achieve all-optical signal processing at low peak power and in a very compact form. In this paper, several nonlinear processing functions will be demonstrated including: femto-second pedestal free, pulse compression; all-optic wavelength conversion; and all-optical regenerator. In addition, we show enhanced nonlinearity for more efficient signal processing by tapering the As₂Se₃ fibre. These applications show chalcogenide glass fibres are very promising candidate materials for nonlinear all-optic signal processing.     

Optical absorption edge of As<Subscript>40–<Emphasis Type="Italic">x</Emphasis></Subscript>Sb<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>S<Subscript>60</Subscript> glassy alloys

The fundamental absorption edge of glassy alloys of an As–Sb–S system was studied in the temperature range 77–300 K. The spectral and thermal behavior of the fundamental absorption edge of As_40–x Sb_xS₆₀ glasses was shown to be described by an exponential function of phonon energy. The temperature and concentration behavior of the optical band gap in the studied glasses was established. The well-known Varshni relationship was used to describe the temperature dependence of the optical band gap.     

ESR in X-irradiated As2O3 glass

X-irradiation of glassy As₂O₃ at 77K or 300K produces an unusually large density (～5×10¹⁸ cm^-3) of paramagnetic centers which are stable at 300K. The average spin-Hamiltonian parameters (g = 1.998, g_⊥ = 1.984, A₆ = 243G, A_⊥ = 114G) indicate that these centers are analogous to those previously observed in As₂Se₃ and As₂S₃ glasses and that they consist of unpaired electrons localized on a non-bonding 4p orbital of an As atom. Unlike the results obtained for As₂Se₃ and As₂S₃, the concommitant holes in As₂O₃ are trapped on Fe²⁺ impurity sites which become Fe³⁺ and not on non-bonding oxygen p orbitals. The radiation induced ESR is also accompanied by a stable optical absorption tail which lies within the band gap and increases exponentially with energy. This absorption can be partially bleached with the application of sub-band-gap light.     

Optical properties of chalcogenide glasses in the terahertz spectral region

Optical properties of chalcogenide glasses of three different compositions (As₂S₃, As₂S₃ × As₂Se₃, and As₂Se₃) are studied via terahertz pulsed spectroscopy. Absorption coefficients and refractive indices are measured in a frequency range of 0.2–1.6 THz. The results show that the phonon modes of the studied materials vary with the composition of the glasses.     

Raman spectra and structure of As40−xS60Ix glasses

The Raman spectra of bulk As_40?xS₆₀I_x glasses with 0?x?20 have been studied. The obtained spectra can be successfully explained assuming the structure of these glasses to be composed of As₂S_3.45 polymer network matrix with dissolved AsBr₃ and S₈ molecules.     

Study of As-Sb-Se chalcogenide glasses by NQR and EPR spectroscopy methods

In this paper experimental results obtained by both ⁷⁵As NQR and EPR spectroscopy are presented for the three-component system As-Sb-Se. The ⁷⁵As NQR spectra of glasses of structures (As₂Se₃)_0.78 (Sb₂Se₃)_0.22, (As₂Se₃)_0.75 (Sb₂Se₃)_0.25, (As₂Se₃)_0.5 (Sb₂Se₃)_0.5 have broad lines with two Sb-NQR lines (corresponding to the Sb₂Se₃ units) and two ⁷⁵As-NQR lines (corresponding to the As₂Se₃ units). Differences in the EPR spectra of the different glasses arise because of the different amounts of arsenic and antimony in their structure.     

The absorption edge of amorphous As2S3

The absorption constantK of amorphous As₂S₃ was determined at the absorption edge in the range 1 to 10⁵ cm^–1. It is shown that at low energy levels up to about 10³ cm^–1 K depends exponentially on the photon energy; at higher absorption levels the energy dependence ofK is quadratic. The significance of these results is discussed. When sulphur is added to As₂S₃ the absorption edge has similar properties but is shifted towards lower energies.     

Reversible photo-induced volume changes in evaporated As2S3 and As4Se5Ge1 films

Reversible photo-induced volume changes have been observed accompanying reversible optical absorption edge shift produced by successive cycles of band gap illumination and annealing for well-annealed evaporated As₂S₃ and As₄Se₅Ge₁ films. The As₂S₃ film shows an increase in its volume by illumination, while As₄Se₅Ge₁ film shows a decrease. Qualitative discussion has been given in connection with pressure-induced optical constant change.     

Optical limiting in fullerenes, colloidal metal solutions, and semiconductors in the field of pico-and nanosecond pulses of an Nd:YAG laser

Optical limiting of pico-and nanosecond pulsed radiation of a Nd:YAG laser (λ=1064 and 532 nm) is studied in solutions of fullerenes (C₆₀ and C₇₀), semiconductor crystals and films (GaAs, As₂S₃, As₂₀S₈₀, 2As₂S₃/As₂Se₃, and 3As₂S₃/As₂Se₃), and colloidal solutions of metals (Au, Ag, Pt, and Cu). The effect of the particle aggregation in silver solutions on the optical limiting is considered. Optical limiting mechanisms, specifically, reverse saturable absorption, two-photon absorption, and self-action effects, are discussed. Nonlinear absorption coefficients of the studied materials are measured.     

Ionic conduction pathways in noble metal chalcohalide glasses

High-energy X-ray diffraction, neutron diffraction and extended X-ray absorption fine structure experiments have been carried out for (MI)_x(As₂Se₃)_1−x glasses (M: Ag or Cu). The addition of a large amount of MI does not significantly affect short-range orderings of the host network matrix. The interatomic distance of M–I pairs is very similar to the case of crystalline MI. However, the coordination number of M–I pairs in the present glasses seems to be somewhat smaller than that in the crystalline MI, suggesting a heavy distortion of tetrahedral coordinates of MI units or structural disorder of the I–I sub-cages in the glass state. It would be predictable that the structure model for MI–As₂Se₃ glasses is proposed to be a pseudobinary mixture of the As(Se_1/2)₃ network matrix and MI-related conduction pathways.     

Reversible photostructural change in melt-quenched As2S3 glass

Reversible phtodarkening and photostructural change accomplished by repeated cycles of band-gap illumination and annealing have been observed in melt-quenched As₂S₃ glass for the first time. The magnitudes of photo-induced shift of optical absorption edge as well as the fraction of photo-expansion observed in melt-quenched As₂S₃ glass coincide quantitatively with those observed in well-annealed evaporated As₂S₃ glass. The experimental data involving results of crystalline As₂S₃ demonstrate that the reversible photostructural change is “unique” to amorphous state and is not affected by the difference in disordered structure originated from preparation technique.     

On the relation between the gap,the transformation temperature and the average heat of atomization of As2Te3 glasses

The average heat of atomization of semiconducting glasses on the As₂Te₃ base, containing silicon, germanium and thallium is calculated from the heats of atomization of constituting elements. The average heat of atomization is correlated with the intrinsic energy gap and the transformation temperature of the studied glasses. The linear dependence between the energy gap, the transformation temperature and the average heat of atomization is found for As₂Te₃ glasses with silicon, germanium and thallium and is correlated with the binding energy between the constituting atoms.     

129I-Mössbauer spectroscopic study of iodide-containing chalcogenide glasses

¹²⁹I-Mössbauer spectroscopy was used to study the short-range order in I-containing chalcogenide glasses. It was found that AsXI glasses, where X=S or Se, are molecular solids composed from molecular units of arsenic iodide and arsenic chalcogenide. The local environment of iodide ions in ternary superionic conducting glasses AgI?Ag₂S?As₂S₃ is similar to that in the crystalline superionic conductor Ag₃SI and differs distinctly from iodide local order in binary vitreous alloys AgI?As₂S₃ and crystalline AgI.¹²⁹I-Mössbauer spectra of all glasses were fitted satisfactory, when a distribution of the electric-quadrupole coupling constant is taken into account.     

The structural, optical, and dielectric spectroscopy studies of novel ZnO–As2O3 glass system with Sb2O3 as additive

ZnO–As₂O₃–Sb₂O₃ glasses of varying concentrations of Sb₂O₃ with ZnO (ranging from 5 to 45 mol%) are prepared. A number of studies, including differential thermal analysis, and study of spectroscopic properties (viz., optical absorption and IR spectra) and dielectric properties (constant ε′, loss tan δ and ac conductivity σ_ac) over a wide range of frequency and temperature of these glasses are carried out. Analyses of the results of these investigations have indicated that the glasses containing higher concentrations of Sb₂O₃ are more suitable for non-linear optical (NLO) applications.     

The optical,structural and thermal optimizations of Ge-As-Se-S-Te glasses

The optical, structural and thermal optimizations of Ge₃₃As₁₂Se₅₅ glass were the aim of this study. In this regards, Ge₃₃As₁₂Se₄₅M₁₀ (M = Se, Te, S and S_0.5Te_0.5) glasses were synthesized by conventional melt quenching technique in quartz ampule. The prepared samples were characterized using X-ray diffraction (XRD), scanning electron microscopy (SEM), differential scanning calorimetry (DSC) and Fourier transform infrared spectroscopy (FTIR). The fundamental absorption edge for prepared samples was also analyzed in terms of the theory proposed by Davis and Mott. The addition of S and Te elements to melting batch has deleterious effects on optical properties of Ge₃₃As₁₂Se₅₅ glass. Mg and Al can act as gettering elements for reduction of the intensity of oxide absorption bands from FTIR spectra (without any effects on optical properties of Ge₃₃As₁₂Se₅₅ glass). The precipitation of GeSe phase, during crystallization process, has negligible effects on optical properties of Ge₃₃As₁₂Se₅₅ glass.     

Optical band gap studies and estimation of two photon absorption coefficient in alkali bismuth borate glasses

The optical absorption spectra of the glasses with composition xBi₂O₃·(30???x)R₂O·70B₂O₃ (R?Li, Na, K) and xBi₂O₃·(70???x)B₂O₃·30Li₂O (0?≤?x?≤?20) have been recorded in the wavelength range 350–650?nm. The glass samples were prepared by the normal melt–quench technique. The fundamental absorption edge for all the series of glasses is analyzed using the theory of Davis and Mott. The position of absorption edges and the values of optical band gap are dependent on the mol% of Bi₂O₃. The absorption in these glasses is associated with indirect transitions. The values of Urbach's energy and band tailing parameters are reported. The two photon absorption coefficient, β, in these glasses has also been estimated from the optical band gap and its value ranges from 1.3 to 11.6?cm/GW. The relationship between β and glass composition has also been discussed in terms of the electronic structure of the glass system.     

Interaction of surface plasmons with interference modes in thin-film nanostructures

In Au/As₂S₃ metal-semiconductor surface composite structures, anomalous absorption of light beyond the fundamental absorption edge of the semiconductor is observed. This absorption is caused by the interaction of the near field of surface plasmons in metal nanoparticles with interference (virtual) modes of the Fabry-Perot cavity formed by the semiconductor film.