Study of thermal and optical parameters of ?? glass has been undertaken. Crystallization and glass transition kinetics has been investigated under nonisothermal conditions by DSC technique. Phase separation has been observed in the material and is investigated by taking the XRD of annealed bulk samples. The material possesses good glass forming ability, high value of glass transition temperature about 420?K, and glass stability. Optical band gap and other optical constants such as refractive index and extinction coefficient have been determined. The isoelectronic substitution of Ge with Sn in the glassy system reduces the optical band gap and enhances the thermal properties. 1. Introduction In amorphous semiconductors, among inorganic glassy materials, chalcogenide glasses occupy a unique place in material science towards advancement of technology. Generally these materials are weakly bonded materials than oxide glasses. But in comparison with amorphous silicon, halide glasses, and other group IV tetrahedral bonded semiconductors these materials exhibit the superior properties which can be tailored by varying the composition. The physical properties such as optical band gap, dielectric behavior, and conductivity of chalcogenide glasses mark their strong dependency on lone pair electrons and density of defect states in the band tails [1, 2]. The disorder in amorphous semiconductors causes perturbation in density of state functions resulting in band tails at the edges of the bottom of the conduction band and the top of the valence band [3]. The lone pair orbits have higher energy than the bonding states and hence occupy the top of the valence band. Interactions between lone pair electrons with their local environment and different atoms result in localized states in the band tails [4]. These localized states play crucial role in deciding optical properties of the materials. The better optical and thermal properties of these materials make them of potential use in the technological applications such as in photonics and phase change memories because of higher values of refractive index and lower value of phonon energy of these glasses [5, 6]. The present Investigation on phase change memories (PCM) shows the possibility of obtaining multistate behavior, enhanced ability to withstand thermal cycling, and use of lower voltages for achieving desired phase change response by using the bilayers of Ge-chalcogenide and Sn-chalcogenide [7]. Germanium is a good glass former and has good glass forming region with Se but has the disadvantage that the Ge compositions
References
[1]
S. R. Elliott, C. N. R. Rao, and J. M. Thomas, “The chemistry of the Noncrystalline State,” Angewandte Chemie International Edition, vol. 25, pp. 31–46, 1986.
[2]
R. M. Mehra, A. Ganjoo, and P. C. Mathur, “Electrical and optical properties of amorphous (Se0.7Te0.3)100-xInx system,” Journal of Applied Physics, vol. 75, no. 11, pp. 7334–7339, 1994.
[3]
N. F. Mott and E. A. Davis, Electronic Process in Non-Crystalline Materials, Clarendon, Oxford, UK, 1979.
[4]
M. Kastner, D. Adler, and H. Fritzsche, “Valence-alternation model for localized gap states in lone-pair semiconductors,” Physical Review Letters, vol. 37, no. 22, pp. 1504–1507, 1976.
[5]
C. Meneghini and A. Villeneuve, “As2S3 photosensitivity by two-photon absorption: holographic gratings and self-written channel waveguides,” Journal of the Optical Society of America B: Optical Physics, vol. 15, no. 12, pp. 2946–2950, 1998.
[6]
K. Paivasaari, V. K. Tikhomirov, and J. Turunen, “High refractive index chalcogenide glass for photonic crystal applications,” Optics Express, vol. 15, no. 5, pp. 2336–2340, 2007.
[7]
A. Devasia, S. Kurinec, K. A. Campbell, and S. Raoux, “Influence of Sn Migration on phase transition in GeTe and Ge2Se3 thin films,” Applied Physics Letters, vol. 96, no. 14, Article ID 141908, 2010.
[8]
L. E. McNeil, J. M. Mikrut, and M. J. Peters, “Phase separation in Ge1-xSnxSe2 glasses,” Solid State Communications, vol. 62, no. 2, pp. 101–103, 1987.
[9]
J. M. Mikrut and L. E. McNeil, “Photostructural changes in bulk amorphous Ge1-xSnxSe2,” Journal of Non-Crystalline Solids, vol. 114, no. 1, pp. 127–129, 1989.
[10]
E. A. Kislitskaya and V. F. Kokorina, “Effect of the replacement of germanium by tin on glass formation and the physicochemical properties of glasses in the antimony-germanium-selenium system,” Zhurnal Prikladnoi Khimii, vol. 44, pp. 646–648, 1971, Translated.
[11]
M. M. Wakkad, E. Kh. Shokr, and Sh. Mohamed, “Crystallization kinetics and some physical properties of as-prepared and annealed Ge-Sb-Se chalcogenide glasses,” Physica Status Solidi A: Applications and Materials, vol. 183, pp. 399–411, 2001.
[12]
G. Mathew, K. N. Madhusudanan, and J. Philip, “Characteristics of photoconductivity in amorphous GexSb10Se90-x thin films,” Physica Status Solidi A: Applications and Materials, vol. 168, pp. 239–248, 1998.
[13]
N. B. Maharjan, K. Singh, and N. S. Saxena, “Calorimetric studies in Se75Te25-xSnx chalcogenide glasses,” Physica Status Solidi A: Applications and Materials, vol. 195, no. 2, pp. 305–310, 2003.
[14]
G. Kaur and T. Komatsu, “Crystallization behavior of bulk amorphous Se-Sb-In system,” Journal of Materials Science, vol. 36, no. 18, pp. 4531–4533, 2001.
[15]
M. S. Kamboj and R. Thangaraj, “Calorimetric studies of bulk Se-Te-Pb glassy system,” The European Physical: Journal Applied Physics, vol. 24, no. 1, pp. 33–36, 2003.
[16]
J. Bicerano and S. R. Ovshinsky, “Chemical bond approach to the structures of chalcogenide glasses with reversible switching properties,” Journal of Non-Crystalline Solids, vol. 74, no. 1, pp. 75–84, 1985.
[17]
M. Lasocka, “The effect of scanning rate on glass transition temperature of splat-cooled Te85Ge15,” Materials Science and Engineering, vol. 23, no. 2-3, pp. 173–177, 1976.
[18]
H. E. Kissinger, “Variation of peak temperature with heating rate in differential thermal analysis,” Journal of Research of the National Bureau of Standards, vol. 57, pp. 217–221, 1956.
[19]
H. E. Kissinger, “Reaction kinetics in differential thermal analysis,” Analytical Chemistry, vol. 29, no. 11, pp. 1702–1706, 1957.
[20]
K. White, R. L. Crane, and J. A. Snide, “Crystallization kinetics of As2-xSbxS3 glass in bulk and thin film form,” Journal of Non-Crystalline Solids, vol. 103, no. 2-3, pp. 210–220, 1988.
[21]
C. T. Moynihan, A. J. Easteal, J. Wilder, and J. Tucker, “Dependence of the glass transition temperature on heating and cooling rate,” Journal of Physical Chemistry, vol. 78, no. 26, pp. 2673–2677, 1974.
[22]
J. A. Augis and J. E. Bennett, “Calculation of the Avrami parameters for heterogeneous solid state reactions using a modification of the Kissinger method,” Journal of Thermal Analysis, vol. 13, no. 2, pp. 283–292, 1978.
[23]
J. C. Manifacier, J. Gasiot, and J. P. Fillard, “A simple method for the determination of the optical constants n, k and the thickness of a weakly absorbing thin film,” Journal of Physics E: Scientific Instruments, vol. 9, no. 11, pp. 1002–1004, 1976.
[24]
R. Swanepoel, “Determination of the thickness and optical constants of amorphous silicon,” Journal of Physics E: Scientific Instruments, vol. 16, no. 12, pp. 1214–1222, 1983.
[25]
J. Tauc, The Optical Properties of Solids, pp. 171–180, North-Holland Publishing, Amsterdam, The Netherlands, 1970.
[26]
A. Ganjoo and H. Jain, “Millisecond kinetics of photoinduced changes in the optical parameters of a-As2S3 films,” Physical Review B—Condensed Matter and Materials Physics, vol. 74, no. 2, Article ID 024201, 11 pages, 2006.
[27]
M. M. Wakkad, E. K. Shokr, and S. H. Mohamed, “Optical and calorimetric studies of Ge-Sb-Se glasses,” Journal of Non-Crystalline Solids, vol. 265, no. 1, pp. 157–166, 2000.