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PhD Thesis Arne Lüker final version V4 - Cranfield University

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Sol-Gel derived Ferroelectric Thin Films for Voltage Tunable Applications<br />

temperature, make the results of these measurements vulnerable. But still, a peak in the<br />

permittivity is a peak. As a reference the permittivity vs. temperature curve of bulk<br />

BaTiO3 was measured, Fig. 3.6, and compared with the well known results from Merz,<br />

Fig. 2.6.<br />

Permittivity [nF]<br />

1,5<br />

1,4<br />

1,3<br />

1,2<br />

1,1<br />

1<br />

0,9<br />

0,8<br />

-20<br />

Fig. 3.6: Permittivity vs Temperature of bulk BaTiO3. Measured in the Poling Rig.<br />

The result shows that the peaks in permittivity are in the right position compared to<br />

Merz measurements. Therefore this method can be used to measure the transition<br />

temperature qualitative without doubts.<br />

3.2.6 Auger Emission Spectroscopy (AES)<br />

-10<br />

dow n up<br />

orthorhombic tetragonal<br />

Auger Emission Spectroscopy (AES), or Auger Analysis, is a technique used in the<br />

identification of elements present on the surface of the sample. AES involves the<br />

bombardment of the sample with an energetic primary beam of electrons. This process<br />

generates, among other things, a certain class of electrons known as Auger electrons.<br />

The mechanism by which an Auger electron is released starts with an electron being<br />

ejected by the primary electron beam from its shell, say, the K-shell. Another electron<br />

from an outer shell (say, the L1-level) of the same atom emits energy in the form of a<br />

0<br />

Temperature [°C]<br />

10<br />

20<br />

77

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