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The Effect of Zr-Doping and Crystallite Size on the Mechanical ...

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I. Introducti<strong>on</strong><br />

temperatures [11]. Up<strong>on</strong> decompressi<strong>on</strong> at ambient temperatures, <strong>the</strong> transformati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

OII to MI was found at 20 GPa, <strong>the</strong> cubic phase could be followed to below 9 GPa <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

below 7 GPa MI transforms to a mixture <str<strong>on</strong>g>of</str<strong>on</strong>g> TiO2II <str<strong>on</strong>g>and</str<strong>on</strong>g> rutile [18]. <str<strong>on</strong>g>The</str<strong>on</strong>g> pressures <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

phase transformati<strong>on</strong>s are different for compressi<strong>on</strong> <str<strong>on</strong>g>and</str<strong>on</strong>g> decompressi<strong>on</strong> <str<strong>on</strong>g>and</str<strong>on</strong>g> vary in<br />

different studies. <str<strong>on</strong>g>The</str<strong>on</strong>g> reas<strong>on</strong> for that is most likely that in many cases phase<br />

transformati<strong>on</strong>s to <strong>the</strong> <strong>the</strong>rmodynamically stable phase were hindered kinetically <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

<strong>on</strong>ly <strong>the</strong> metastable phases were observed. <str<strong>on</strong>g>The</str<strong>on</strong>g> apparent pressure-temperature phase<br />

diagram <str<strong>on</strong>g>of</str<strong>on</strong>g> TiO2 is presented in Figure 1, c<strong>on</strong>taining transformati<strong>on</strong> pressures as well as<br />

pressure ranges in which <strong>the</strong> phases were observed.<br />

In <strong>the</strong> following chapters, <strong>the</strong> phases anatase, rutile, TiO2II <str<strong>on</strong>g>and</str<strong>on</strong>g> MI will play an<br />

important role <str<strong>on</strong>g>and</str<strong>on</strong>g> <strong>the</strong>ir structures are described in more detail in <strong>the</strong> following (Figure<br />

2). In anatase, each Ti is surrounded by an octahedr<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> six oxygen atoms. Four edges<br />

per octahedr<strong>on</strong> are shared, building a “zig-zag” chain parallel to a as well as b. <str<strong>on</strong>g>The</str<strong>on</strong>g><br />

chains are stacked antiparallel to <strong>the</strong> c axis. Rutile c<strong>on</strong>sists <str<strong>on</strong>g>of</str<strong>on</strong>g> TiO6 octahedra <str<strong>on</strong>g>and</str<strong>on</strong>g> two<br />

opposing edges <str<strong>on</strong>g>of</str<strong>on</strong>g> each octahedr<strong>on</strong> are shared, forming linear chains parallel to <strong>the</strong> cdirecti<strong>on</strong>.<br />

In <strong>the</strong> a-b-plane, <strong>the</strong> chains are linked via corner-sharing oxygen atoms. In<br />

TiO2II, <strong>the</strong> octahedra make up a network similar to rutile but are distorted. <str<strong>on</strong>g>The</str<strong>on</strong>g> structure<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> MI can be seen as an even fur<strong>the</strong>r distorted versi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> TiO2II, exhibiting a seven-fold<br />

coordinati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> Ti-atom.<br />

Figure 2: Elementary cells <str<strong>on</strong>g>and</str<strong>on</strong>g> polyhedra <str<strong>on</strong>g>of</str<strong>on</strong>g> TiO2 anatase, rutile, TiO2II <str<strong>on</strong>g>and</str<strong>on</strong>g> MI. Oxygen atoms are shown<br />

in red, titanium atoms <str<strong>on</strong>g>and</str<strong>on</strong>g> polyhedra are shown in blue.<br />

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