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Metal. , 21A: 2419–2429, 1990. 49. J. Harvey, P. G. Partridge, and C. L. Snooke, J. Mater. , 20, 1009–1014, 1985. 50. S. L. Semiatin and H. R. Piehler, Metall. , 10A: 85–96, 1979. 51. A. Wisbey and P. G. Partridge, Mater. Sci. , 9: 441–444, 1993. 337 52. T. S. Baker and P. G. Partridge, in R. ), Diffusion Bonding, Cranfield, England: SIS, 1987, pp. 73–89. 53. J. L. Alcaraz, J. M. Martı´nez-Esnaola, and J. Gil-Sevillano, Int. J. Solid Structures, 33: 2075–2093, 1996. 54. J. L. Alcaraz, J. M. Martı´nez-Esnaola, and J.

46. D. V. Dunford and P. G. Partridge, in R. ), Diffusion Bonding, Cranfield, England: SIS, 1987, pp. 17–32. 47. J. Pilling and N. Ridley, Mater. , 3: 353–359, 1987. 48. A. G. , Metal. , 21A: 2419–2429, 1990. 49. J. Harvey, P. G. Partridge, and C. L. Snooke, J. Mater. , 20, 1009–1014, 1985. 50. S. L. Semiatin and H. R. Piehler, Metall. , 10A: 85–96, 1979. 51. A. Wisbey and P. G. Partridge, Mater. Sci. , 9: 441–444, 1993. 337 52. T. S. Baker and P. G. Partridge, in R. ), Diffusion Bonding, Cranfield, England: SIS, 1987, pp.

4 Ȑm wide is also clearly observed, which corresponds to a possible FeTi2 intermetallic phase. However, both crystallographic structures and chemical analyses are also compatible with the Fe2Ti4O phase. The oxygen necessary to form this phase probably comes from the initial interface. 3 Ȑm) rich in Si and Zr is present. These particles (trapped during the polishing on emery at the free surface of the austenitic 316L stainless steel) indicate the evolution of the original interface showing the occurrence of the Kirkendall effect (45).

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