12.10.2013 Views

PDF (tesi dottorato ROTIROTI) - FedOA - Università degli Studi di ...

PDF (tesi dottorato ROTIROTI) - FedOA - Università degli Studi di ...

PDF (tesi dottorato ROTIROTI) - FedOA - Università degli Studi di ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Materials and Methods: Porous Silicon’ production calibration<br />

Today, the electrochemical etching is a standard method to fabricate nanostructured<br />

porous silicon: a proper choice of the applied current density, the electrolyte<br />

composition, and the silicon doping allow precise control over the morphology and,<br />

consequently, on the physical and chemical properties of the porous silicon structure.<br />

Computer controlled electrochemical etching processes are exploited for the<br />

realization of porous silicon films of controlled thickness and porosity (defined as the<br />

percentage of void in the silicon volume).<br />

Nanoporous, mesoporous and macroporous structures can be achieved, with pore<br />

size ranging from few nanometers up to microns. Moreover, since the etching<br />

process is self-stopping, it is possible to fabricate with a single run process multilayer<br />

stacks made of single layers of <strong>di</strong>fferent porosity. The <strong>di</strong>electric properties of each<br />

PSi layer, and in particular its refractive index n, can be namely modulated between<br />

those of crystalline silicon (n = 3.54, porosity = 0) and air (n= 1, porosity = 100 %); so<br />

that alternating high and low porosity layers, lot of photonic structures, such as<br />

Fabry-Perot interferometers, omni-<strong>di</strong>rectional Bragg reflectors, optical filters based on<br />

microcavities, and even complicated quasi-perio<strong>di</strong>c sequences (Thue-Morse) can be<br />

simply realized, as it is shown in Figure 5.<br />

Reflectivity (a.u)<br />

Reflectivity (a.u)<br />

1,0<br />

0,8<br />

0,6<br />

0,4<br />

0,2<br />

2,0<br />

1,5<br />

1,0<br />

0,5<br />

0,0<br />

600 800 1000 1200 1400 1600<br />

Wavelength (nm)<br />

monolayer<br />

optical microcavity<br />

800 1000 1200 1400<br />

Wavelength (nm)<br />

Reflectivity (a.u.)<br />

600 800 1000 1200 1400 1600<br />

Figure 5. Experimental reflectivity spectra of <strong>di</strong>fferent PSi optical structures.<br />

In this study Fabry-Perot single layer, Bragg mirrors, Thue Morse and optical<br />

microcavities have been used as sensors.<br />

The porous silicon layer was obtained by electrochemical etching in a HF-based<br />

solution at room temperature. The substrate used was a highly doped p + -silicon,<br />

oriented, 0.01 Ω cm resistivity, 400 μm thick. Before ano<strong>di</strong>zation the substrate<br />

was placed in HF solution to remove the native oxide. With this substrate we can<br />

obtain mesoporous layers, with a pore average <strong>di</strong>mension of about 50 nm. In figure 6<br />

SEM images are reported.<br />

1,0<br />

0,8<br />

0,6<br />

0,4<br />

0,2<br />

0,0<br />

Reflectivity (a.u)<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

Bragg<br />

Wavelength (nm)<br />

Thue Morse S6<br />

600 800 1000 1200 1400 1600<br />

Wavelength (nm)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!