As and Epitaxial-Growth MnSi Thin Films - OPUS Würzburg
As and Epitaxial-Growth MnSi Thin Films - OPUS Würzburg
As and Epitaxial-Growth MnSi Thin Films - OPUS Würzburg
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4.2. Test Barrier Material 47<br />
Fig. 4.2: Cubic structure of ABO 3 pervoskite crystals.(for our analysis, A = Sr <strong>and</strong> B = Ti) (a)<br />
shows the (100) AO-terminated plane (e.g. SrO). (b) <strong>and</strong> (c) show the (110) <strong>and</strong> (001) (TiO 2<br />
termination) planes, respectively. Figure reprinted from [Pisk 04]<br />
4.2 Test Barrier Material<br />
For our purposes, we focused on a particular material Strontium Titanate SrTiO 3 to<br />
improve our gating devices’s leakagecurrent characteristics. Reported dielectric constants<br />
for this material is measured to be higher than that of Al x Ga 1−x <strong>As</strong> (where x is Al mole<br />
fraction) <strong>and</strong> Al<strong>As</strong> both at ǫ ≈ 10 - 15ǫ 0 , which comprised the n all-semiconductor gating<br />
barrier used in the previous chapter.[Owen 09]<br />
4.2.1 Strontium Titanate SrTiO 3 (STO)<br />
Strontium Titanate or STO is a prototypical perovskite ferroelectric oxide has been subject<br />
of interest due to its desirable electronic properties (e.g. large electric field-sensitive<br />
permittivity). The perovskite crystal structure is shown in Figure 4.2. It is found to be a<br />
Fig. 4.3: Dielectric constant ǫ for bulk STO measured with temperature. Values at 4K show<br />
constantsintherangeof10000-20000. Thecurvesshowsampleswithdifferentcurrentdirections<br />
(E) <strong>and</strong> stresses (τ for strain <strong>and</strong> σ for thermal strain) Figure reprinted from [Mull 79].