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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 />

Concentration Concentration (at,%) (at,%)<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

λ<br />

λ λFe+Cr Fe<br />

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

λY-Ti-O λ YTiO<br />

Fe-Cr phase Y-Ti-O phase<br />

0 5 10 15 20 25 30 35 40 45 50 55 60<br />

Distance (at,%)<br />

Figure 3.2. Profile generated from a volume in Figure 3.1 (b). Characteristic lengths<br />

of Y-Ti-O – λY-Ti-O and Fe-Cr-rich phases and Fe-rich phases – λFe+Сr are shown. Fe, Cr, Mn,<br />

Si, C, W species are associated with Fe-Cr-rich phase while Y, YO, O/O2, Ti, TiOx, FeO,<br />

CrOx with Y-Ti-O phase. Profile is 12×12×60 nm 3 with step of 0.2 nm.<br />

A simi<strong>la</strong>r two-phase microstructure was also observed in a different analysis (LATAP<br />

analyse, see Figure 3.6) while a one phase structure, corresponding to Fe-Cr-rich phase has<br />

been observed in the <strong>la</strong>st experiment, Figure 3.3. This non homogeneous microstructure can<br />

be exp<strong>la</strong>ined simply looking at the microstructure observed during APT tip pre<strong>par</strong>ation in<br />

SEM / FIB (Figure 3.4). Different contrasts (bright and dark) clearly reveal that a two phase<br />

structure is present. The shape of both phases is not well <strong>de</strong>fined and irregu<strong>la</strong>r. From SEM<br />

picture it is clear that, the dimensions of these phases vary between tens of <strong>nano</strong>metres to<br />

several micrometers. So, the dimensions of these phases, can exp<strong>la</strong>in the different<br />

microstructures observed by 3DAP.<br />

Fe<br />

Cr<br />

W<br />

10×10×70 nm 3<br />

Figure 3.3. 3D reconstruction of ODS mo<strong>de</strong>l alloy analysed by LATAP. Fe, Cr, W are<br />

shown. No presence of Y-Ti-O-rich phase is observed. Analyzed volume is 10×10×70 nm 3 .<br />

93

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