- Nano Express
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Optical and Vibrational Spectra of CsCl-Enriched GeS2-Ga2S3 Glasses
© Klym et al. 2016
- Received: 30 November 2015
- Accepted: 1 March 2016
- Published: 9 March 2016
Optical and FTIR spectroscopy was employed to study the properties of 80GeS2-20Ga2S3-CsCl chalcohalide glasses with CsCl additives in a temperature range of 77–293 K. It is shown that CsCl content results in the shift of fundamental absorption edge in the visible region. Vibrational bands in FTIR spectra of (80GeS2-20Ga2S3)100 − х (СsCl) x (x = 5, 10, and 15) are identified near 2500 cm−1, 3700 cm−1,, around 1580 cm−1, and a feature at 1100 cm−1. Low energy shifts of vibrational frequencies in glasses with a higher amount of CsCl can be caused by possible thermal expansion of the lattice and nanovoid agglomeration formed by CsCl additives in the inner structure of the Ge-Ga-S glass.
- Chalcohalide glass
- Optical spectra
- Vibrational properties
Modern IR photonics emphasizes a significant importance of glassy functional materials with improved exploitation characteristics [1–3]. Among the promising media for applications of photonics are specific glasses, such as non-oxide glassy-like materials with a high content of chalcogens (S, Se, Te), which are also widely known as the chalcogenide glasses (ChGs) [4, 5]. Main developments concerning the preparation of such materials include different methods of their technological and post-technological structural modification using external influences, such as thermal annealing, high-energy irradiation, and laser beam treatment [5–8]. Technical possibilities of these modification methods, however, are, to a large extent, restricted by peculiarities of a vitreous state with characteristic effects of natural physical aging, functional non-reproducibility, and thermodynamic instability in view of high affinity to chemical reactivity.
That is why the commonly used optimization of ChG is connected with traditional chemical compositional modification based on doping possibilities with additional components introduced into the glass matrix to attain new, sometimes unusual, properties. The principal functionality of ChG is determined by their excellent IR transparency. A wide range including both commercially important atmospheric telecommunication windows at 3–5 and 8–12 μm up to a space telecommunication domain at 20–25 μm can be effectively combined with the transparency of halide compounds in a visible range by developing mixed chalcogenide-halogenide glasses such as Ge-Ga-S-CsCl systems [9, 10]. The mix of unique optical properties with high flexibility in composition and fabrication methodology makes these ChG systems compelling for IR photonics . The exceptional IR transparency associated with suitable viscosity/temperature dependence creates a good opportunity for developing ChG-based molded optics for IR devices.
In [12, 13], we studied the influence of CsCl amount on an atomic-deficit sub-system (void- or pore-type structure formed due to the lack of atoms at some of glassy network sites) in Ge-Ga-S-CsCl chalcohalide composition. In this work, we analyze the CsCl effect on the optical and vibrational properties of (80GeS2-20Ga2S3)100 − x (CsCl) x glasses with x = 5, 10, and 15.
GeS2-Ga2S3-CsCl chalcogenide glasses were sintered from Ge, Ga, S, and CsCl compounds (99.999 % purity), as described in details elsewhere [14–16]. Raw materials were melted at 850 °C in a silica tube for several hours. The (80GeS2-20Ga2S3)100 − х (СsCl) x (x = 5, 10, and 15) glasses were annealed at 15 °C below a glass transition temperature (T g) for each of the glasses  to minimize inner strains. Such amount of CsCl additives is optimal in order to modify Ge-Ga-S glasses before future doping of these materials by rare-earth ions. For the purpose of convenience, the obtained glasses of (80GeS2-20Ga2S3)100(СsCl)0, (80GeS2-20Ga2S3)95(СsCl)5, (80GeS2-20Ga2S3)90(СsCl)10, and (80GeS2-20Ga2S3)85(СsCl)15 hereafter are referred to as (CsCl)0, (CsCl)5, (CsCl)10, and (CsCl)15, respectively.
Optical spectra were measured using a Cary5 (Varian) short-wavelength spectrophotometer. A Bruker Vector 22 instrument was exploited to record the spectra in the mid and far-infrared regions . IR spectroscopy at different temperatures was carried out at the infrared beamline SINBAD of the Daphne Light synchrotron IR facility [17–21]. The infrared transmission spectra were collected using a Vertex 70V FTIR spectrometer equipped with a Janis ST-100-FTIR (Janis Research Company, LLC, Woburn, MA) continuous flow cryostat and a room temperature DTGS detector. The outer cryostat windows were made of CaF2. The temperature points (293, 220, 150, and 77 K) were set with a LakeShore 331 temperature controller and kept constant, controlling the flux of liquid nitrogen and heating power during the necessary measurement procedure. The heating/cooling rate in experiments was set to 10 K min−1. The transmission spectra were acquired in the vacuum between 4500 and 900 cm−1 with a spectral resolution of 4 cm−1, performing 128 scans.
The vibrational spectra of (80GeS2-20Ga2S3)100 − х (СsCl) x (x = 5, 10, and 15) glasses collected at different temperatures for each composition are shown in Fig. 3. It can be observed that the bands located near 1580 cm−1 appear for all glasses and show no shifts. In the (CsCl)5 and (CsCl)10 ChG samples, there is a very slight shift of the S–H absorption band located near 2500 cm−1 at elevating temperatures. However, the temperature shift of vibrational frequencies towards lower energies for (CsCl)15 glasses is detected for the S–H vibrational band and O–H-related peaks also shift with the increase of temperature from 77 to 293 K. We tend to think that this effect may be due to the differences in water absorption in the structure at higher temperatures. All transformations of vibrational modes of (80GeS2-20Ga2S3)85(СsCl)15 glasses are related to the excessive amount of CsCl additive, resulting in the damage to the inner structure of the host material.
The CsCl addition effects on the optical and vibrational spectra for GeS2-Ga2S3-CsCl glasses are investigated. It is demonstrated that the transmission in the visible region increases with a CsCl concentration from 60 % in (CsCl)0 to 80 % in (CsCl)10 and (CsCl)15. A sharp peak at 4000 nm for a base (CsCl)0 glass is attributed to S–H stretching and is considerably damped for samples with CsCl in the mid-IR spectra. There are also features at 6300 nm corresponding to H2O, in which 6700 and 2900 nm are related to O–H stretching vibrations. The intensity of absorption bands associated with water increased with the CsCl amount, confirming the hygroscopicity of CsCl. It is established that for each measured temperature (77, 150, 220, and 293 K), the intensities of the observed vibrational bands increase with the CsCl amount in the 80GeS2-20Ga2S3 ChG. The principal vibrational bands centered near 1100, 1580, 2500, and 3700 cm−1 in (CsCl)15 glasses are slightly shifted to lower energies between 77 and 150 K. The shift is more pronounced between 220 and 293 K. Such temperature shifts of vibrational frequencies can be caused by possible thermal expansion of the lattice and agglomeration of nanovoids formed by CsCl additives. Temperature dependences of FTIR spectra also indicate the lower-energy shift of vibrational frequency of the S–H-related band for (CsCl)15 glasses and the shift of O–H-related peaks at elevating temperatures.
The FTIR experiments at INFN-LNF were supported by the European Community in the frame of CALIPSO program under FP7 – Transnational Access to Research Infrastructures (TARI), Contract No. 312284. H. Klym thank the Lviv Polytechnic University under Doctoral Program and support via the Project DB/KIBER (No. 0115U000446), A.I. Popov thanks the VBBKC L-KC-11-0005 project Nr. KC/126.96.36.199.1/10/01/006, 5.4 for the funding.
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