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3. PHOTO-ORIENTATION BY PHOTOISOMERIZATION                                 £7

               for each, the process of photoisomerization differs. For the photoisomeriz-
               ation of azobenzenes, the free volume needed for inversion is lower than
               what is needed for rotation.
                   Most photo-orientation studies in thin solid films have been
               perforformed on push-pull azobenzene derivatives such as disperse red one
               (DR1; see Figure 3.2). DR1 is a pseudo-stilbene-type azobenzene molecule.
               This means that the n-n* and n-n* transitions overlap each other, a feature
               that leads to a large structureless band in the trans isomer and a strong
               dependence of the maximum of absorption on the polarity of the host
               material, which may be a polymer or a solvent. In thin polymeric films, the
               kinetics of photoisomerization are not of first order, and they represent a
               complex behavior that is a consequence of the chromophore's local free-
               volume distribution in the polymer. The kinetics of isomerization of DR1 in
               films of a poly-methyl-methacrylate (PMMA) polymer are at least biexpo-
               nential. Although this observation could be explained by the dual nature of
               the long wavelength X (k > 400 nm) photochemical transition explained
               above, the multiexponential behavior of the thermal cis—Hrans isomerization
               can be rationalized only by the existence of a distribution of local free
               volumes in the polymer film. In fact, the free volume clearly influences photo-
               isomerization and photo-orientation (vide infra). The thermal cis-~>trans
               isomerization of DR1 in PMMA is monoexponential during the first 10
               seconds; this reaction is fast in both doped (4 s) and functionalized (5 s)
               polymers, as it is for stilbene-like azobenzene molecules. For DR1 in PMMA
               (guest-host), the activation energy is 16 kj/mol, and the photochemical
               quantum yields are  (f> tc = 0.11 ± 0.03 and <fr ct = 0.7 ± 0.1 at room tem-
                       16
               perature.  The experimental and theoretical methods for QY determination,
                                     17
                                               18
               i.e., the methods of Fisher  and Rau,  are summarized in Appendix 3A.







                                         o  DR1 -trans
                                         a  DR1-cis
                                      0.7 p-r^TT^-^T-o-rT-rT-r-r-r-r-m
                                      0-6 b      o ° 0      ~
                                         F       o           :
                                   0>  0.5 -        o        -
                                   e     -      O            -
                                   es  0.4 —        O       —
                                   ja          o
                                   t*
                                                 A
                                   o  0.3 ~    o&.  ^ 0      -
                                   Js          OA   A&      :
                                      0.2 i.  <£•    o       -
                                   ^                         l
                                      0.1  L ***£     °      -
                                       0  L_Sj.., , , ,  1 , ,*, ,CD . , 0, ,\
                                       300  400   500  600 7C
                                                K 1 nm
               FIGURE 3.2  (Top) Trans-DRI. (Bottom) /y>sorption spectra of cis- and trans-DRl.The cis-DRI
               spectrum was determined by Fisher's method.After reference 16, redrawn by permission.
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