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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 2. Materials, experimental and simu<strong>la</strong>tion techniques<br />

(c) Deconvolution of over<strong>la</strong>p between 64CrN 2+ and 64TiN 2+ is conducted due to<br />

natural abundances of Cr and Ti in agreement with the procedure discussed above<br />

(for 64TiO 2+ /64TiN 2+ or 54Cr 2+ /54 Fe 2+ ).<br />

Figure 2.13. Mass spectrum of nitri<strong>de</strong>d NDS steel after annealing at 700°C/1h by<br />

LAWATAP. Interval from 23 to 36 amu is shown.<br />

c) Methods for APT data treatment<br />

The data treatment procedure, in general, is simi<strong>la</strong>r for all materials and consists of<br />

several steps:<br />

Number of atoms<br />

3000<br />

2500<br />

2000<br />

1500<br />

1000<br />

500<br />

(a) Measurement of the global chemical composition of the analysed volume;<br />

(b) Investigation of solute distributions in analysed volumes. If clusters are not visible<br />

(simply by eyes), then statistical tests are used. The assumption of a random distribution of<br />

solute atoms (Cr, Ni, Mn, W, Si, etc.) is tested using the statistical test <strong>de</strong>scribed in Appendix<br />

3-a. Two results are possible:<br />

0<br />

(i) Statistical test confirms that the distribution of solute atoms in the analysed<br />

volume is random. In this case the analysed volume is consi<strong>de</strong>red as a <strong>par</strong>t of<br />

matrix.<br />

48Ti 2+<br />

50Cr 2+ -50Ti 2+<br />

52Cr 2+<br />

53Cr 2+<br />

54Cr 2+ - 54Fe 2+<br />

55Mn 2+<br />

56Fe 2+<br />

57Fe 2+<br />

58Fe 2+ - 58Ni 2+<br />

23 24 25 26 27 28 29 30 31 32 33 34 35 36<br />

Mass-over-charge ratio (amu)<br />

60TiN 2+ - 60Ni 2+<br />

61TiN 2+ - 61Ni 2+<br />

62TiN 2+ - 62Ni 2+<br />

63TiN 2+<br />

64CrN 2+<br />

66CrN 2+<br />

67CrN 2+<br />

68CrN 2+<br />

69

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