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

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

Measured concentration Ti, Y, O (at,%)<br />

20<br />

18<br />

16<br />

14<br />

12<br />

10<br />

8<br />

6<br />

4<br />

2<br />

0<br />

Figure 2.7. Com<strong>par</strong>ison of chemical composition estimated for <strong>nano</strong><strong>par</strong>ticles in ODS<br />

steel by Laser-Assisted Tomographic Atom Probe (LATAP) and Wi<strong>de</strong> Angle Laser-Assisted<br />

Tomographic Atom Probe (LAWATAP).<br />

II.4. Particu<strong>la</strong>r case of ODS and NDS materials<br />

a) Determination of experimental <strong>par</strong>ameters<br />

In or<strong>de</strong>r to get reproducible and reliable results during APT analysis, it is important to set<br />

correctly experimental conditions. Temperature, Laser wavelength and pulse fraction are<br />

important <strong>par</strong>ameters influencing results.<br />

LATAP<br />

LAWATAP<br />

core TAP<br />

core LAWATAP<br />

Ti Y O<br />

Laser wavelength. Two different Laser wavelengths were avai<strong>la</strong>ble on LATAP and<br />

LAWATAP at the beginning of this work: λ=1030 nm (infrared) and λ=515 nm (green). It is<br />

clearly established that for ferritic materials, green Laser pulses give <strong>la</strong>rgely better mass<br />

resolution than infrared. Thus, 515 nm wavelengths were used in all experiments.<br />

Temperature effect. The temperature of the sample during analysis may have different<br />

consequences. First, the risk of sample breaking increases when the temperature <strong>de</strong>creases.<br />

However, by increasing the temperature, mass resolution and spatial resolution are affected<br />

and additional effect such as preferential evaporation 2 may bias the chemical composition<br />

2 This effect happens when elements have different field of evaporation. If the standing voltage of the<br />

specimen is too high, elements with lower field of evaporation will preferentially evaporate during the<br />

time between the pulses. This effect can be avoi<strong>de</strong>d by increasing the pulse fraction (which results in a<br />

<strong>de</strong>crease of standing voltage) or <strong>de</strong>creasing the temperature (differences in evaporation fields are<br />

normally <strong>de</strong>creases with <strong>de</strong>creasing of the temperature).<br />

60

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