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of low-molecular-weight azobenzene compound (He et al., 2000), where the contribution of dye bleaching has been suggested. Also, in the sol gel materials, in which some cross-linking of polymer takes place, the ef ciency of polarization recording was minimal (Darracq et al., 1998). The result of holographic irradiation is a modulation of lm thickness that replicates the interference pattern created by the laser beams. This enables the hologram to be encoded as a relief pattern. A weak probe 633-nm laser has been typically used to diffract from this phase hologram. The DE of nth diffracted order may be calculated as Zn In =SIn , where In are the intensities of the nth-order diffracted beams. In the literature, typically the DE of the rst diffraction order has been characterized. Note that it is correct until the recorded gratings are not very deep (that is often the case) and the grating pro le remains sinusoidal. Deep relief gratings have many diffraction orders in Raman Nath regime of diffraction, and their pro les deviate often from sinusoidal form. In this case, the characterization of grating by the total DEs proved to be an advantage. Total DE is determined as the sum of DEs of all nonzero orders, Ztot Z 1 Z 2 . The best-reported example of recording kinetics in ionic complexes is shown in Fig. 2.14 (Kulikovska et al., 2007). The grating was recorded in the material (Methyl Red)/PDADMAC with moderate irradiation intensities of 250 mW/cm2. After 20 min of irradiation, 98% of the probe light was diffracted by the recorded grating. Maximum diffraction of 45% in rst diffraction order was reached after 17 min, whereas maximum of 35% of light diffracted into second diffraction



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var = function([arg(s)])

The value FALSE may be returned by some NCurses functions. Above, the value of var could be either TRUE or FALSE. var is a bool variable type.

Diffraction efficiencies (%)

[Obj97] [OG03]

if( eval == FALSE) while([eval ==] FALSE)

The value FALSE can be used in comparisons, as shown above. Functions that return FALSE can also be used immediately inside comparisons:

0 0 10 20 30 Time (min) 40 50 60

[OL01]

if( function([arg(s)] ) while( function([arg(s)] )

Figure 2.14. Kinetics of the diffraction ef ciencies of the 0th, 1st, and 2nd diffraction orders upon holographic irradiation in (Methyl Red)/PDADMAC lm (Fig. 2.7). Source: Kulikovska et al., 2007. Reprinted with permission from American Chemical Society.





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The logical opposite of FALSE is TRUE. Functions that use or return FALSE can equally use or return TRUE, depending on the situation. Refer to the Notes under the TRUE entry later in this Appendix, for a list of NCurses functions that use the value FALSE.

if(can_change_color())

[OLW98] [OMG04a]

Figure 2.15. AFM image of surface relief grating inscribed in (Methyl Red)/ PDADMAC lm (Fig. 2.7). Source: Kulikovska et al., 2007. Reprinted with permission from American Chemical Society.

Here, if evaluates the results of the can_change_color() function. If FALSE is returned, then the terminal cannot use custom colors for text attributes.

meta(stdscr,FALSE);

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orders after 35 min of irradiation The diffraction behavior reveals a very deep grating An atomic force microscopy (AFM) image of the corresponding grating with a peak-to-valley height of ca 165 mm and a period of 23 mm is presented in Fig 215 One may estimate the recording rate to be as high as 10%/min for this grating Very high modulation depths of relief gratings achieved in these materials are the highest values among the azobenzene-containing materials reported so far In other respects, the inscription of SRG in ionic complex materials was comparable to the azobenzene-functionalized polymers The gratings could be erased, if were irradiated with spatially homogeneous unpolarized UV light, and then recorded again into the same lm Also, the successive recording was demonstrated as a proof of the process reversibility.

[OMG04b]

This function truncates text input from the standard screen to 7-bits wide instead of 8. (See meta().)

In this way, two-dimensional (2-D) cross-gratings consisting of up to 13 linear gratings have been successively inscribed into the lm Figure 216 displays an example of the 2-D grating adopted from Kulikovska et al (2008b) Remarkably, because the induced SRGs are thermally very stable, only heating the samples above 1501C can erase them The thermal stability of the light-induced surface structures in the ionic complex materials is worthy to discuss here in comparison to the stability of gratings in the azobenzene-functionalized polymers It is well established now that SRGs in polymers are stable below the glass transition temperature of the polymers and can be erased if heated above Tg It has been noted that the higher the glass transition temperature, the lower is the SRG formation ef ciency Only shallow, though thermally stable, gratings could be induced in polymers with high Tg of about 1501C (Che et al.

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 #include <ncurses.h> int main(void) { bool tf; initscr(); tf = has_colors(); if( tf == FALSE) addstr( This terminal cannot do colors.\n ); else addstr( This terminal can do colors.\n ); refresh(); getch(); endwin(); return 0; }

Sample output:

[Ope91] [Ope97]

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