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 ...
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
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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