Page 147 - Photoreactive Organic Thin Films
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126                                             ZOUHEIR SEKKAT AND WOLFGANG KNOLL




                                                           PI-1
                                                        Mean Absorbance
                                                      •o- Dichroic Ratio


                      -P 0.75-

                      c 0.70-
                      C3
                      5
                      4)





                                        100    150   200         300
                                              Time t (hours)
                 FIG. 4.13 Mean absorbance and order parameter, referred to in the figure as dichroic ratio, of PI-1
                 versus time after end of irradiation. After reference 47, redrawn by permission of OSA.













                                                              1.5 2.0  2!5
                                    PI-1
                                                          Time t (hours)
                                  TI =0.1 hours
                                  T 2 = 1.1 hours
                                  %-, = !,6 hours


                                                     10  12   14  16   18
                                                Time t (hours)
                 FIG. 4.14 A logarithmic plot of the long-time cis— Hrans thermal back reaction of PI- 1. The inset
                 shows an expanded view of the first points of the figure. Squares indicate the experimental absorbance,
                 and the solid line indicates a triexponential theoretical fit with the time constants given in the figure.
                 The time t = 0 corresponds to die state of the system approximately 2 minutes after the irradiation is
                 turned off. After reference 47, redrawn by permission of OSA.

                    PI-1 and PI-2 films exhibit dichroic absorbance after polarized irradiation.
                 Figure 4.15 shows polar plots of the absorbance of linearly polarized probe
                 light (at 488 nm) as a function of the angle, \y, between the polarization of
                                                               2
                 the probe and irradiation light (532 nm; 30 mW/cm ). Nonpolar orientation
                 is clearly shown for both PI-1 (left) and PI-2 (right). The highest absorption is
                 observed when the probe and irradiation beams have perpendicular polarizations,
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