30.07.2015 Views

Déformation photoinduite dans les films minces contenant des ...

Déformation photoinduite dans les films minces contenant des ...

Déformation photoinduite dans les films minces contenant des ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

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

Chapter 3. Microscopic mechanisms at the origin of the photo-induced deformation inazobenzene-containing thin <strong>films</strong> 60Defining ɛ pi the pre-irradiation light dose and ɛ int the interfering beam light dose wecan <strong>des</strong>cribe the photodeformation obtained in the pre-irradiation experiments of Figure3.2(c) as:a(ɛ int , ɛ pi ) = a(ɛ int , 0) − a pl (ɛ pi ) (3.3)pastel-00527388, version 1 - 19 Oct 2010where a pl (ɛ pi ) is the plastic deformation induced by the pre-irradiation. The deformationamplitude a(ɛ int , ɛ pi ) obtained under exposure to the interfering beam dose ɛ int aftera pre-irradiation dose ɛ pi is equal to the photodeformation amplitude a(ɛ int , ɛ pi = 0)obtained under exposure to the interference pattern without pre-irradiation diminishedof the plastic photoexpansion a pl (ɛ pi ) due to the pre-irradiation dose ɛ pi . By takinginto account only the saturation deformation amplitu<strong>des</strong> observed in Figure 3.2(c)we obtain the curve in Figure 3.2(d) relative to the matrix photoexpansion, whichrepresents:a(ɛ int = ∞, ɛ pi ) = a(∞, 0) − a pl (ɛ pi ) (3.4)This allows to deduce the saturation plastic deformation amplitude:a pl (ɛ pi ) = a(∞, 0) − a(∞, ɛ pi ) (3.5)which can be simply rewritten:a pl (ɛ) = a(∞, 0) − a(ɛ) (3.6)The experimental variation of a pl (ɛ) is plotted in Figure 3.3(a). By using eq. 3.2, wecan easily obtain the amplitude of the elastic part of the photodeformation:a el (ɛ) = a(ɛ) − a pl (ɛ) (3.7)In Figure 3.3(b-c) we show the variation of a el (ɛ) deduced from the experimental dataobtained with two different interference power densities, 4 mW/mm 2 and 1.5 mW/mm 2respectively.The behavior of a pl (ɛ) and a el (ɛ) indicates that the plasticity of the photodeformationgrows with the irradiation dose, reaching a maximum amplitude of about 4 nm atɛ pi ≃ 10 mJ. On the other hand, the elastic deformation amplitude exhibits a transientfeature for low doses and beyond reaches a plateau.We note that the amplitude of a el (ɛ) at saturation is slightly larger for 4 mW/mm 2irradiation power density (b) than for 1.5 mW/mm 2 irradiation power density (c). Thisis coherent with the stress-strain model for an elastic deformation. However, we are

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

Saved successfully!

Ooh no, something went wrong!