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Etude par Sonde Atomique Tomographique de la formation de nano ...

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tel-00751814, version 1 - 14 Nov 2012<br />

Chapter 3. Oxi<strong>de</strong> Dispersion Strengthened Steels<br />

Figure 3.4. SEM image of APT sample pre<strong>par</strong>ation by Focused Ion Beam (annu<strong>la</strong>r<br />

milling). Two contrasts are clearly observed indicating that two phases are observed.<br />

b) Evaporation artifacts<br />

In the 3DAP reconstructions of ODS mo<strong>de</strong>l alloy, a shift between Ti and Y atom<br />

positions is observed, as shown in Figure 3.1 (c). It should be mentioned that, the major <strong>par</strong>t<br />

of Y and almost all Ti are <strong>de</strong>tected as molecu<strong>la</strong>r ions. They are bon<strong>de</strong>d with O in the form of<br />

TiO, TiO2 and YO. In addition, CrO, CrO2 and FeO molecu<strong>la</strong>r ions are also observed. Thus,<br />

in or<strong>de</strong>r to study the Y/Ti shift in more <strong>de</strong>tails, concentration profiles showing only YO, TiOx,<br />

FeO and CrOx molecu<strong>la</strong>r ions are shown on Figure 3.5 (a-c).<br />

The YO and TiO+TiO2, FeO, CrO+CrO2 peaks correspond to the Y-Ti-O rich phase on<br />

the concentration profile. The shifts of TiO, TiO2 molecu<strong>la</strong>r ions re<strong>la</strong>tively to YO are clearly<br />

seen in the z direction (direction of analysis). The same observation is done for CrO, CrO2<br />

and FeO molecu<strong>la</strong>r ions.<br />

The shift between these ions is estimated as follow. First, the distance between YO and<br />

TiOx top peaks, d, are <strong>de</strong>termined (as indicated in Figure 3.5 (a)). Then, the width of each<br />

YO, TiO and TiO2 peaks (namely LYO and LTiOx) at half maximum height is estimated and the<br />

difference between these values (LTiOx - LYO) is calcu<strong>la</strong>ted. All these characteristics (d, LYO,<br />

LTiOx and LTiOx -LYO) are summarized in Table 3.2. d varies from 0.2 to 2.1 nm and (LTiOx -LYO)<br />

varies from -0.9 to 0.7 nm. As it can be seen from Figure 3.5 (a), in one case the TiOx peak is<br />

absent in com<strong>par</strong>ison to corresponding YO peak (peak 4 on the figure).<br />

94

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