Films minces à base de Si nanostructuré pour des cellules ...

Films minces à base de Si nanostructuré pour des cellules ... Films minces à base de Si nanostructuré pour des cellules ...

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properties. The increasing Si incorporation with refractive indices is reected in all the characterization techniques. Based on the investigations, the results on SRSN can be summarized under two categories: (a) n 1.95eV ≤ 2.4 ˆ There is no formation of nanocrystals. For samples with low refractive indices (n 1.95eV =2.0-2.2) the absence of nanocrystals is attributed to the low Si excess and to the low D Si in SRSN as compared to SiO 2 . For samples with refractive indices between 2.3-2.4, this may be attributed to the low power density provided during thermal annealing, which does not favour crystallization. tel-00916300, version 1 - 10 Dec 2013 ˆ The material exhibits photoluminescence depending on the applied laser power density. ˆ With increasing refractive indices (Si excess), the emission decreases and the absorption coecient increases. (b) n 1.95eV ≥ 2.4 ˆ The threshold of refractive index for forming nanocrystals in SRSN matrix is demonstrated. XRD and Raman measurements conrm the presence of nanocrystals. ˆ No emission is observed from PL measurements whatever be the annealing, while from Raman measurements emission is witnessed. This emission is quenched after 1h-1100°C annealing. Correlation between formation of nanocrystals and quenching of PL suggest that nanocrystals might have a detrimental eect on emission in SRSN materials. ˆ The absorption coecient decreases with increasing sample thickness. 4.5 SRSO/SRSN multilayer The microstructural and optical analyses of SRSO/SRSN MLs grown by RF sputtering technique is demonstrated in the following sections. It was seen in chapter 3 that the best material properties in SRSO/SiO 2 MLs (formation of nanocrystals, emission, absorption etc.) are obtained after CA (1h-1100°C annealing). Hence the SRSO/SRSN ML is also subjected to CA for initial investigations. The material properties of CA sample are compared with those obtained from their as-grown MLs. 106

A multilayer composed of 100 patterns of 3.5 nm-SRSO and 5 nm-SRSN, (which will be referred as 100(3.5/5)) is chosen as a typical example for these initial investigations. The SRSN sublayers in this sample are grown using reactive sputtering approach. 4.5.1 Ellipsometry The total thickness, roughness and pattern thickness of the 100(3.5/5) ML were analyzed using ellipsometry. Figures 4.16 and 4.17 show the results of ellipsometry simulations of the as grown and CA samples. The ts were performed assuming the SRSO/SRSN multilayer to be a constant refractive index homogenous layer. tel-00916300, version 1 - 10 Dec 2013 (a) Figure 4.16: As-grown 100(3.5/5) ML. (a)Fitting of the ellipsometric functions (Is & Ic as a function of photon energy). The circles relate to experimental spectra and the lines to the tting, and (b) The dispersion curves, n eV & k eV of the real and imaginary parts of refractive indices respectively; n 1.95 eV = 2.137 is highlighted in the gure. (b) It can be noticed in the results obtained from as-grown and CA 100(3.5/5) MLs (Fig. 4.16a and 4.17a) that with such an approximation the theoretical spectra well t the measured ones. Moreover, the 832 nm thickness of the as grown sample deduced from ellipsometry closely relates to the expected thickness of 850 nm [(100 pattern x 3.5 tSRSO ) + (100 pattern x 5 tSRSN )]. As highlighted in gures 4.16b and 4.17b, the refractive index of the as-grown sample, n 1.95eV =2.13 increases to 2.34 after CA. This increase is also accompanied by a reduction in thickness of the CA sample to 777 nm (as-grown sample = 832 nm) thereby indicating a densication process favoured by annealing. 107

A multilayer composed of 100 patterns of 3.5 nm-SRSO and 5 nm-SRSN, (which<br />

will be referred as 100(3.5/5)) is chosen as a typical example for these initial investigations.<br />

The SRSN sublayers in this sample are grown using reactive sputtering<br />

approach.<br />

4.5.1 Ellipsometry<br />

The total thickness, roughness and pattern thickness of the 100(3.5/5) ML were<br />

analyzed using ellipsometry. Figures 4.16 and 4.17 show the results of ellipsometry<br />

simulations of the as grown and CA samples. The ts were performed assuming the<br />

SRSO/SRSN multilayer to be a constant refractive in<strong>de</strong>x homogenous layer.<br />

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

(a)<br />

Figure 4.16: As-grown 100(3.5/5) ML. (a)Fitting of the ellipsometric functions (Is & Ic<br />

as a function of photon energy). The circles relate to experimental spectra and the lines<br />

to the tting, and (b) The dispersion curves, n eV & k eV of the real and imaginary parts<br />

of refractive indices respectively; n 1.95 eV = 2.137 is highlighted in the gure.<br />

(b)<br />

It can be noticed in the results obtained from as-grown and CA 100(3.5/5) MLs<br />

(Fig. 4.16a and 4.17a) that with such an approximation the theoretical spectra<br />

well t the measured ones. Moreover, the 832 nm thickness of the as grown sample<br />

<strong>de</strong>duced from ellipsometry closely relates to the expected thickness of 850 nm<br />

[(100 pattern x 3.5 tSRSO ) + (100 pattern x 5 tSRSN )]. As highlighted in gures 4.16b and<br />

4.17b, the refractive in<strong>de</strong>x of the as-grown sample, n 1.95eV =2.13 increases to 2.34<br />

after CA. This increase is also accompanied by a reduction in thickness of the CA<br />

sample to 777 nm (as-grown sample = 832 nm) thereby indicating a <strong>de</strong>nsication<br />

process favoured by annealing.<br />

107

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