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2- two peaks at low temperature. 3 kJ mol-1 and has been attributed to a Snoek-type relaxation caused by interstitials hydrogen atoms in the bcc β phase. 2 kJ mol-1) is the same. In isothermal tests the values of Q-1 and E of composite change with an asymptotic trend. These variations depend on diffusion phenomena of interstitial atoms to dislocations that reduces the mean distance between pinning points. Acknowledgments S. Kaciulis and A. Mezzi are grateful for the financial support provided by the ELETTRA synchrotron for the project n.

Lorella Ceschini and Roberto Montanari 35 Experimental depth profiles can be compared with carbon concentration profiles calculated by the 2nd Fick’s law in the case of a semi-infinite solid. 14a. The values of the pre-exponential factor D0 and of the activation energy Q used in the calculation have been taken from ref. [27] and are displayed in Fig. 8a. Carbon diffuses over a distance of about 10 µm, which is about 3 orders of magnitude higher than the experimental one (10 nm) thus the carbon concentration in the interface can not be explained by the process of carbon diffusion in the Ti-α matrix.

Yang: Mater. Sci. Eng. 426 (2006), p. 278. [20] S. Kaciulis: “Spettroscopia elettronica delle superfici”, Tecniche sperimentali per la caratterizzazione dei materiali, ed. 103. F. F. D. A. D. A. A. F. F. F. G. A. [23] R. Donnini, S. Kaciulis, A. Mezzi, R. Montanari and C. Testani: Surf. Interface Anal. Vol. 40 (2008), p. 277. [24] S. Kaciulis, A. Mezzi, R. Donnini, P. Deodati, R. Montanari, N. Ucciardello, M. Amati, M. Kazemian-Abyaneh and C. Testani, Surf. , Vol. 42 (2010) p. 707. [25] M. Kiskinova, K.

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