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a) b - École Polytechnique de Montréal

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organic thin films, a novel and straightforward method was <strong>de</strong>veloped in the last <strong>de</strong>ca<strong>de</strong>(G.<br />

Decher & Hong, 1991a; Nicolau, 1985). It was observed(G. Decher & Hong, 1991a) that<br />

polyelectrolytes with opposite charges could be assembled in an alternating layer by layer<br />

method onto a substrate to generate a sequential multilayer organic thin film(G. Decher, Hong, &<br />

Schmitt, 1992b). The potential utility of this method is to obtain thin, uniform electrically<br />

conductive films on a variety of substrates, as was shown by Rubner and his group(Cheung, Fou,<br />

Ferreira, & Rubner, 1993; Cheung, Fou, & Rubner, 1994; Cheung, Stockton, & Rubner, 1997). It<br />

was found that two consecutive layers are strongly interpenetrated, although some researchers<br />

believe that the layers are locally interpenetrated and diffusion from one polyanion layer to the<br />

neighboring polyanion layer can not occur,(Farhat, Yassin, Dubas, & Schlenoff, 1999) but some<br />

other authors mention that a network of two co-continuous layers is generated(Cheung, et al.,<br />

1997).<br />

In such a film-forming technique, layer-by-layer <strong>de</strong>position of different polyelectrolytes with<br />

opposite charges is involved to fabricate molecularly controlled ultrathin multilayer films(Tse et<br />

al., 2007). Electrostatic interactions are the cause of the adsorption of layers. Kinetic trapping of<br />

charge species from solution on the surface can be <strong>de</strong>scribed as film assembly( Decher, 1997).<br />

Repetitive <strong>de</strong>position steps provi<strong>de</strong> a precise control over the total thickness of the layers in the<br />

range from a few angstroms up to the micrometer range. The LbL technique, unlike other film<br />

fabrication processes such as the Langmuir-Blodgett (LB)(Blodgett, 1934; Zasadzinski,<br />

Viswanathan, Madsen, Garnaes, & Schwartz, 1994) technique, which requires particular<br />

equipment, has no limitation on the type of substrate and charge-bearing species. Consequently,<br />

LbL is a simple method and consi<strong>de</strong>rably more versatile than other techniques.<br />

Decher et al.(G. Decher & Hong, 1991b) <strong>de</strong>veloped the LbL <strong>de</strong>position method since it has been<br />

extensively used to construct thin films of well-<strong>de</strong>fined thicknesses for a wi<strong>de</strong> variety of<br />

applications that can be divi<strong>de</strong>d into two categories(Decher & Schlenoff, 2003): 1) tailoring<br />

surface interactions, such as corrosion protection(Farhat & Schlenoff, 2002), sensors(Decher,<br />

Hong, & Schmitt, 1992a), antibacterial(Rudra, Dave, & Haynie, 2006), antistatic coating for<br />

electrophoresis(Graul & Schlenoff, 1999), and biosensing(Yipeng Sun, 1996), and 2) fabrication<br />

of surface base <strong>de</strong>vices such as electro-optic materials(Fou, Onitsuka, Ferreira, & Rubner, 1996),<br />

<strong>de</strong>vices including nanoreactors(Joly et al., 2000), electrochromic windows(DeLongchamp &<br />

Hammond, 2001), or even in the area of surface patterning for the <strong>de</strong>position of quantum dots<br />

67

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