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Longitudinal and shear ultrasonic wave velocities were measured in the quaternary compounds CuxAg1¡xInTe2 (0 · x · 1) using pulse echo technique. Measurements were carried out at 4 MHz frequency and at room temperature. Elastic moduli and acoustic impedance have been calculated. Results indicated that these parameters are influenced by the increased addition of copper from x = 0 to 1.
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Czasopismo
Rocznik
Tom
Strony
363--372
Opis fizyczny
Bibliogr. 23 poz., rys., tab.
Twórcy
autor
autor
- Ultrasonic Laboratory, National Institute for Standards, Tersa Str., P.O. Box 136, El-Haram, El-Giza 12211, Egypt, mohamed_s_gaafar@hotmail.com
Bibliografia
- [1] DAVID J., CHEEKE N., Fundamentals and aplications of ultrasonicwaves, CRC Press, Boca Raton, FL, 2002.
- [2] SHAY J.L., WERNICK J.H., Ternary chalcopyrite semiconductors: growth, electronic properties and applications, Pergamon Press, Oxford 1975.
- [3] JAFFE J.E., ZUNGER A., Electronic structure of the ternary chalcopyrite semiconductors CuAlS2, CuGaS2, CuInS2, CuAlSe2, CuGaSe2, and CuInSe2, Phys. Rev. B, 28, 5822 (1983).
- [4] IDEM., ibid., Theory of the band-gap anomaly in ABC2 chalcopyrite semiconductors, 29, 1882 (1984).
- [5] IDEM., ibid., Anion displacements and the band-gap anomaly in ternary ABC2 chalcopyrite semiconductors, 27, 5176 (1983).
- [6] NORMAN F.M. HENRY, KATHLEEN L., International tables for X-ray crystallography, Vol. 1, p. 212, KYNOCH PRESS, Birmingham-England 1969.
- [7] KUROSAKI K., UNEDA H., MUTA H., YAMANAKA S., Thermoelectric properties of thallium antimony telluride, J. Alloys and Compounds, 376, 43 (2004).
- [8] KRIEGER M., SIGG H., REINHART F.K., Elastic constant C11 of AlxGa1¡xAs determined by near infrared Brillouin scattering, Solid State Communications, 88, 267 (1993).
- [9] TSUCHIYA Y., HISAKABE M., Structural changes in molten (GaxIn1¡x)As: Sound velocity measurements, J. Non-Cryst. Solids, 353, 3000 (2007).
- [10] VARSHNEYA A.K., Fundamentals of inorganic glasses, Acad. Press, New York (1994).
- [11] MOUSTAFA A.M., EL-SAYAD E.A., SAKR G.B., Crystal structure refinement of CuxAg1¡xInTe2 bulk material determined from X-ray powder diffraction data using the Rietveld method, Cryst. Res. Technol., 39, 266 (2004).
- [12] KHALIFA F.A., EL-HADI Z.A., MOUSTAFFA F.A., HASSAN N.A., Density and molar volume of some sodium silicate, lead borate and lead silicate glasses, Indian J. Pure Appl. Phys., 27, 279 (1989).
- [13] HOLLEMAN A.F., WIBERG E., WIBERG N., Lehrbuch der Anorganischen Chemie, 91–100 ed., Walter de Gruyter, Berlin 1985.
- [14] MAKISHIMA A., MACKENZIE J.D., Direct calculation of Young’s modulus of glass, J. Non-Cryst. Solids, 12, 35 (1973).
- [15] MAKISHIMA A., MACKENZIE J.D., Calculation of bulk modulus, shear modulus and Poisson’s ratio of glass, J. Non-Cryst. Solids, 17, 147 (1975).
- [16] GRZETA–PLENKOVIC B., SANTIC, Crystal data for CuGaxIn1¡xTe2, J. Appl. Crystallogr., 16, 576 (1983).
- [17] KNIGHT K.S., The crystal structures of CuInSe2 and CuInTe2, Mater. Res. Bull., 27, 161 (1992).
- [18] WOOLLEY J.C., WILLIAMS E.W., Some cross-substitutional alloys of CdTe, J. Electrochem. Soc., 113, 899 (1966).
- [19] RAJENDRAN V., PALANIVELU N., CHAUDHURI B.K., GOSWAMI K., Characterisation of semiconducting V2O5–Bi2O3–TeO2 glasses through ultrasonic measurements, J. Non-Cryst. Solids, 320, 195 (2003).
- [20] BRIDGE B., HIGAZY A., A model of the compositional dependence of the elastic moduli of polycomponent oxide glasses, Phys. Chem. Glasses, 27, 1 (1986).
- [21] BRIDGE B., PATEL N.D., WATERS D.N., On the elastic constants and structure of the pure inorganic glasses, Phys. Stat. Sol. (a), 77, 655 (1983).
- [22] ANDERSON O.L., Physical acoustics, Warren P. Mason ed., Academic Press, New York, (III) B, 45 (1965).
- [23] WANKHEDE D.S., WANKHEDE N.N., LANDE M.K., ARBAD B.R., Densities and ultrasonic velocities of some oxygen containing compounds, Journal of Molecular Liquids, 138, 124 (2008).
Typ dokumentu
Bibliografia
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bwmeta1.element.baztech-article-BATA-0002-0031