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Figure 4.15: Absorption coecient spectra of <strong>Si</strong> 3 N 4 and SRSN samples.<br />

tel-00916300, version 1 - 10 Dec 2013<br />

4.4 Summary<br />

<strong>Si</strong>N x materials were grown by two dierent <strong>de</strong>position approaches: Reactive sputtering<br />

and Co-sputtering. Three kinds of <strong>Si</strong>N x layers were grown: N-rich silicon<br />

nitri<strong>de</strong> (NRSN), <strong>Si</strong> 3 N 4 and <strong>Si</strong>-rich silicon nitri<strong>de</strong> (SRSN). It was <strong>de</strong>monstrated that<br />

the refractive in<strong>de</strong>x of the layer is the ruling factor and the <strong>de</strong>position approaches<br />

do not inuence the material properties of these layers.<br />

NRSN:<br />

NRSN material was grown by sputtering <strong>Si</strong> 3 N 4 catho<strong>de</strong> reactively un<strong>de</strong>r N 2 plasma.<br />

FTIR and refractive in<strong>de</strong>x studies conrm this layer is N-rich.<br />

<strong>Si</strong> 3 N 4 :<br />

Stochiometric layer was grown by sputtering <strong>Si</strong> 3 N 4 catho<strong>de</strong> reactively un<strong>de</strong>r N 2<br />

plasma. The refractive in<strong>de</strong>x and FTIR investigations indicate that the grown layer<br />

is <strong>Si</strong> 3 N 4 . The material exhibits low PL emission which increases upon annealing<br />

reaching the highest for 1h-1100°C (CA). The material shows a low absorption that<br />

increases with energies.<br />

SRSN:<br />

SRSN layers with various refractive indices were investigated. It was shown that<br />

by using appropriate r N in the rst <strong>de</strong>position approach orP <strong>Si</strong> in the second one,<br />

we can tune <strong>Si</strong>N x composition close to <strong>Si</strong> 3 N 4 or pure <strong>Si</strong> layers. The SRSN layers<br />

grown by both the <strong>de</strong>position approaches have similar trend in structural and optical<br />

105

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