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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 />

Appendixes<br />

Appendix 3. 3DAP data treatment methods<br />

The procedure for the data treatment is simi<strong>la</strong>r for all materials and consists of several<br />

steps. The assumption of a random distribution of solute atoms is tested by methods discussed<br />

below.<br />

a) Statistical tests<br />

3DAP technique is used to check fine scale variations of composition in materials. If there<br />

are slight variations of chemical compositions, the so called frequency distribution (FD) may<br />

reveal microstructural features that are not visible (by eyes) on 3D pictures.<br />

When atoms are randomly distributed a binomial distribution (BD) of the local<br />

concentrations is expected. If precipitation, clustering or segregation occurs in the material, the<br />

FD becomes broa<strong>de</strong>r than the BD or even shows well se<strong>par</strong>ated peaks corresponding to<br />

different phases.<br />

In or<strong>de</strong>r to construct the FD, the APT data are divi<strong>de</strong>d into blocks, usually containing<br />

equal number of atoms (Nbox), called the sampling block size (typically 50…500 atoms).<br />

However, the shape of the FD may vary with the chosen block size. For those cases, data<br />

should be analysed in a more careful way.<br />

A convenient and straightforward test is suggested by Thuvan<strong>de</strong>r et al [5]. It is usually<br />

used when small variations of composition or or<strong>de</strong>ring are of interest. The random or non<br />

random distribution of solute atoms is tested by com<strong>par</strong>ing the value of the standard error (s)<br />

calcu<strong>la</strong>ted from experimental data and standard <strong>de</strong>viation (σ) of the binomial distribution<br />

calcu<strong>la</strong>ted from the experimental data set.<br />

The mean concentration, c0, of element A is calcu<strong>la</strong>ted using the experimental data. Then<br />

the standard error, s, is calcu<strong>la</strong>ted for every block size in a range, typically 100-500 atoms,<br />

using the expression:<br />

1 ��<br />

n<br />

2<br />

b<br />

2<br />

s � ( c � c )<br />

(1)<br />

i 0<br />

n �1<br />

i 1<br />

b<br />

where nb is the total number of blocks and ci is the concentration of element A in block i. With<br />

increasing of block size, s generally <strong>de</strong>creases. The experimentally obtained s is com<strong>par</strong>ed with<br />

the standard <strong>de</strong>viation, σ, of the BD:<br />

200

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