By S. D. Myers
Publication by way of S. D. Myers, J. J. Kelly, R. H. Parrish
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3) S. Yang, C. Stoffers, F. M. K. J. 28 Optoelectronic Materials and Technology Summers, Appl. Phys. Lett. 72 158-160 (1998). Y. L. Zhang, J. K. N. J. Summers, J. Vac. Sei. , B 16 855-857 (1998). 5 ) J. S. H. Holloway, Mat. Res. Soc. Bull. (1999) 51-53. C. A. S. L. H. Holloway, J. Appl. Phys. 83 4578-4583 (1998). 7) J. S. H. Holloway, Mat. Res. Soc. Bull. (1999) 51-53. 8) Y. D. Jiang, Z. L. Wang, J. Mater. Res. 13 2950-2955 (1998). K. H. Jilavi, D. Burgard, R. Nass, H. Schmidt, J. Am. Ceram. Soc.
6. Those spectra as well as all the other presented in this paper have been normalized to the height of the Boson peak for comparison. This choice of reference is the most appropriate because the Boson peak, being at the lowest frequency, also corresponds to the most extended of the modes, and its height is therefore expected to be least sensitive to the particular composition of the glass. This assumption is supported by the fact that a Boson peak is observed in all glasses or amorphous systems, in the same frequency range although not always with the same magnitude .
5) with a comparable and excellent chemical stability. Te0 2 glass also offers a high solubility for rare earth ions, erbium or thullium in particular, and relatively low phonon frequencies. Finally, the multivalent states of Te and the low bonding strength of the Te-0 bond provide compositional flexibility while low glass transition temperatures ensure ease of fabrication. X-ray Photoelectron (XPS) and Raman spectroscopies constitute a particularly powerful combination of techniques for a fundamental study of the structural origin of the vibrational dynamics of Te0 2 glasses.
A Guide to Transformer Maintenance by S. D. Myers