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x: s : s + + /2

The overlay() function takes text from one window and places that text into the blank portions of another window.

int overlay(const WINDOW *srcwin, WINDOW *dstwin);

+ /2 + /4 0 0 /2 /4 /2



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More examples of POOLING, especially POOLING of persistent, stateful remote objects, are shown at the end of 7, Extended Infrastructure Patterns, to illustrate the LIFECYCLE MANAGER and CONFIGURATION GROUP patterns. The diagrams that follow illustrate CLIENT-DEPENDENT INSTANCES in more detail. The next diagram shows how a client accesses a CLIENTDEPENDENT INSTANCE using a factory remote object. Here the factory is used to create the CLIENT-DEPENDENT INSTANCE, and the instance is explicitly destroyed by the client after a number of invocations.

srcwin is a WINDOW pointer representing the source window, from which text is copied. dstwin is a WINDOW pointer representing the destination, the window where text from srcwin is pasted.

+45 : 45





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With the overlay() function, only the blank parts of the destination window are over-written with text from the source window. Text from srcwin will not replace text in dstwin, neither will text attributes be copied to the dstwin. srcwin and dstwin do not need to be the same size. However:

The two windows must overlap. It is only the overlapping portion of the windows that is overlaid. When the two windows do not overlap, overlay() returns ERR.

someOperation(x) someOtherOperation(x) destroy() delete()

Figure 4.5. Coordinate system used to describe SRG inscription, with x running along the direction of light modulation. The two incident beams have their polarization state controlled. The s polarization is parallel to the surface, whereas the p state is parallel to the plane-of-incidence.

overlay(first,second);

After the statement, locations where window first overlaps window second will be changed; any blank spots in window second will be filled by overlapping text from window first.

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impinging on the sample is readily calculated from knowledge of the input polarizations, yet in the bulk of the material the light pattern will be redirected and repolarized on the basis of the detailed three-dimensional structure of the surface, refractive index, and birefringence. The optical erasure of an SRG, performed by homogenous irradiation, is also polarization-dependent (LagugneLabarthet et al., 2002; Jiang et al., 1998). Thus, the gratings possess a memory of the polarization state during inscription, encoded in the orientational distribution of chromophores at various grating positions. Typically, gratings inscribed with highly favorable polarization combinations will be optically erased more quickly. The s-polarization state, which produces poor gratings, is generally optimal for performing the erasure. These results are obviously related to the orientational distribution of chromophores after surface patterning and their subsequent interaction with the erasing polarization.

The more interesting tasks happen under the hood of the distributed object middleware, of course. The next sequence diagrams tries to illustrate this. First, we have to initialize the respective LIFECYCLE MANAGER

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 #include <ncurses.h> int main(void) { WINDOW *alpha,*beta; int x; initscr(); start_color(); init_pair(1,COLOR_WHITE,COLOR_BLUE); init_pair(2,COLOR_WHITE,COLOR_RED); /* create and color two side-by-side windows */ alpha = newwin(5,30,0,0); wbkgd(alpha,COLOR_PAIR(1)); beta = newwin(5,30,1,2); wbkgd(beta,COLOR_PAIR(2)); /* populate the windows with text */ for(x=0;x<75;x++) { wprintw(alpha, O ); wprintw(beta, X ); } wrefresh(alpha); wrefresh(beta); getch(beta); /* copy from window beta to window alpha */ overlay(beta,alpha); wrefresh(alpha); wrefresh(beta); wgetch(beta); endwin(); return 0; }

In a typical inscription experiment, a sinusoidally varying light pattern is generated at the sample surface. What results is a sinusoidal surface pro le: an SRG. This is the pattern most often reported in the literature, because it is conveniently generated (by intersecting two coherent beams) and easily monitored (by recording the diffraction intensity at a nonabsorbing wavelength, usually using a HeNe laser at 633 nm). However, it must be emphasized that the azo surface mass transport can produce arbitrary patterns. Essentially, the lm encodes the impinging light pattern as a topography pattern. Both the intensity

Sample output: Two windows appear, one blue with Os and another red with Xs. The two windows overlap for all but one row and column. Pressing Enter copies the Xs from the red window to the blue.

10, copywin(), overwrite(), dupwin()

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