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The formation of an SRG is typically monitored via the diffraction of a probe laser beam. One must be careful in analyzing this diffraction ef ciency, however, because a number of simultaneous gratings will be generated in an azo sample during illumination with a light pattern (Fig. 4.6a d). A light intensity pattern will lead to a chemical grating, since illuminated regions will be more cis rich than dark regions. The resultant spatial variation of absorbance and refractive index will lead to various optical effects, including diffraction. This grating is temporary,



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1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 #include <ncurses.h> int main(void) { WINDOW *p; char text[] = Greetings from pad p. ; char *t; initscr(); p = newpad(50,100); /* create a new pad */ if( p == NULL ) { endwin(); puts( Unable to create new pad ); return(1); } t = text; prefresh(p,0,0,0,0,1,25); while(*t) {

24.09.2004 20:59

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Figure 4.6. Schematic of the different gratings that are formed during illumination of an azo sample. (a) SRG. (b) DG. (c) Birefringence (orientational) grating. (d) Chemical (trans/cis) grating. All the gratings contribute to the observed diffraction ef ciency, to varying extents. Gratings (b), (c) and (d) are all refractive-index gratings.

pechochar(p,*t); t++; napms(50);





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Basic Remoting Patterns invocation to the remote object. The REQUESTOR hides the details of the client side distributed object communication from clients.

} wgetch(p); endwin(); return 0; }

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persisting only during irradiation. Simultaneously, a birefringence grating will be inscribed. These birefringence patterns are stable and contribute to the observed nal diffraction ef ciency. An SRG is of course induced if there is any spatial variation in intensity or polarization, and diffraction from this grating is very large, sometimes overwhelming other effects. Lastly, a DG appears to be seeded beneath the material surface, which will also lead to periodic variation of refractive index. The contributions to diffraction due to the surface relief and birefringence gratings can be deconvoluted using a Jones matrix formalism applied to polarized measurements of the rst-order diffracted beams (Helgert et al., 2000; Labarthet et al., 1999, 1998; Naydenova et al., 1998b; Holme et al., 1997). Similarly, scattering theory (Geue et al., 2002b; Pietsch, 2002) was used to t visible light and X-ray diffraction data (Henneberg et al., 2003; Geue et al., 2002c, 2000; Henneberg et al., 2001b) to deconvolute contributions owing to surface relief and density (refractive index) gratings. For scattering from an SRG, the x and z components of the momentum transfer are qx k sin yf sin yi 4:2 qz nk cos yi cos yf where yi and yf are the incident and re ected angles, and k=2p/l. For the visible diffracted peak of order m (i.e., when qx=m2p/L), the scattering intensity was derived to be 2 Ivis % Jm qz h eiqz d Jm qz Dnm d 4:3

Sample output:

where d is the lm thickness, h is the grating height, Dnm is the mth Fourier component of the refractive-index grating, and Jm the mth Bessel function. These Bessel functions can give rise to oscillations in the diffraction signal (Fig. 4.7). Thus, one must be careful not to implicitly assume a linear dependence between grating amplitude and diffraction ef ciency. Clearly, both the DG and SRG contribute to the signal. For the X-ray signal, the scattering amplitude is given by the following: Ax- ray % Jm qz h eiqz d Bm 2 4:4

addch(), newpad(), prefresh()

1) invoke(locationProcessB, Object1 , operationX , arguments)

pnoutrefresh()

where one must now use the qz appropriate for X-rays, and Bm represents the Fourier component of the density modulation (which is presumably identical to the index-modulation). The intensity is not simply the square of A, but can be determined using Fresnel transmission functions. The visible scattering is mostly sensitive to the surface-relief, and the X-ray scattering is due primarily to the density modulation. Using both measurements, the two contributions can of course be determined.

The pnoutrefresh() function is analogous to the wnoutrefresh() function, but for a pad instead of a window. It s used to optimize the updating of multiple pads to the standard screen.

4) operationY()

pnoutrefresh() can best be used when updating several pads on the standard screen. Rather than using prefresh() on each pad, you can use pnoutrefresh() on each pad, then a single doupate() function to perform all the updates at once.

1 0.8 0.6 n

int pnoutrefresh(WINDOW *pad, int pminrow, int pmincol, int sminrow, int smincol, int smaxrow, int smaxcol);

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