<i>E-k</i> Relation of Valence Band in Arbitrary Orientation/Typical Plane Uniaxially Strained

<table class="table-group" width="800px"><tr class="fig-image" id="a"><td><img alt="686303.fig.005a" src="https://static.hindawi.com/articles/acmp/volume-2014/686303/figures/686303.fig.005a.jpg"/></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(a) </b>(001) plain</td></tr></table></td></tr><tr class="fig-image" id="b"><td><img alt="686303.fig.005b" src="https://static.hindawi.com/articles/acmp/volume-2014/686303/figures/686303.fig.005b.jpg"/></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(b) </b>(101) plain</td></tr></table></td></tr><tr class="fig-image" id="c"><td><img alt="686303.fig.005c" src="https://static.hindawi.com/articles/acmp/volume-2014/686303/figures/686303.fig.005c.jpg"/></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(c) </b>(111) plain</td></tr></table></td></tr></table>

<table>The splitting energy versus stress and angle in uniaxially strained Si.</table>

Advances in Condensed Matter Physics

fig5

Figure 5

Figure 5: <i>E-k</i> Relation of Valence Band in Arbitrary Orientation/Typical Plane Uniaxially Strained 

Advances in Condensed Matter Physics

E-k Relation of Valence Band in Arbitrary Orientation/Typical Plane Uniaxially Strained

Figure 5