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Single-beam experiments at high power showed a central peak instead of a depression By exposing a sample to a gradient two-beam intersection, a lm was inscribed with a continuum of laser intensitites An inphase grating was found in the high power region, and a conventional out-ofphase SRG was found in the low power region The intermediate region clearly showed interdigitation of the peaks from the two regimes, resembling a doubling of grating period observed by others These double-period gratings can be formed in a number of amorphous systems, using the polarization combinations of ( p, p) or (+451, 451), with indications that even the (s, s) and ( p, s) combinations function to a certain extent (Lagugne-Labarthet et al, 2004; Labarthet et al, 2001, 2000; Naydenova et al, 1998a) Observations of a double-frequency orientational grating underneath a normal SRG have also been reported (Schaller et al.



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id := getObjectID() pc := getLifecycleManager(id) pooledSrvt2 := invocationArrived(id) ro := getFreeInstance() removeFromPool(pooledSrvt2)

The statement checks to see if the putwin() function has not returned OK, meaning that the operation has failed.





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, 2003) The double-period SRGs were attributed to interference between the diffracted beams from the primary grating, which gives rise to a light modulation, with double the initial frequency, in the material Whether these double-period gratings are related to the inverted structures observed in high intensity experiments and some LC systems is an open question It is interesting to note that some of the amorphous polymers that exhibit double-frequency behavior have accessible LC phases at a higher temperature These phase behavior results strongly suggest that there are (at least) two mechanisms at play during surface patterning One dominates at low intensity in amorphous systems, whereas another appears to dominate at higher intensity and in LC systems From an applied standpoint,.

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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 23 24 25 26 27 28 29 30 #include <ncurses.h> int main(void) { int y = 0,x = 0, r; initscr(); addstr( You Move The Cursor!\n ); addstr( Enter the Y (row) coordinate: ); refresh(); scanw( %d ,&y); addstr( Enter the X (column) coordinate: ); refresh(); scanw( %d ,&x); r = move(y,x); if(r == ERR) { mvaddstr(3,0, You have moved the cursor! ); move(y,x); } else mvaddstr(3,0, You cannot move the cursor there! ); refresh(); getch(); endwin(); return 0; }

activate() someOperation(x) invocationDone(pooledSrvt2) deactivate() putBackToPool(pooledSrvt2) putBackToPool(pooledSrvt2)

Sample output:

these double-period gratings are of great interest, as they represent a means of generating patterned structures below the usual diffraction limit of far- eld optical lithography. The fact that the optical inscription process is sensitive to both intensity and polarization is of considerable importance (Jiang et al., 1996). Different polarization combinations lead to different amplitudes, h, of the inscribed SRG, as shown in Table 4.1. (The coordinate system is shown in Fig. 4.5.) An optical eld vector component in the direction of light modulation (hence mass transport) appears necessary (Bian et al., 1998). Interestingly, SRGs can even be formed via pure polarization patterns, where the light intensity is uniform over the sample surface (Viswanathan et al., 1999a). In fact, the (s, s) and (RCP, RCP) combinations, which correspond to mainly variations in intensity and little to no polarization contrast, produce very poor SRGs. In contrast, the best gratings are obtained with (+451, 451) and (RCP, LCP) combinations, which involves primarily variation in polarization state across the lm. It should be noted, however, that the exact polarization pattern present inside the material is not known. The pattern TA B L E 4 . 1 . Polarization Patterns at the Sample Surface During SRG Inscription Using a Variety of Polarized Beam Combinations. The Quality of the SRG (as Determined by Grating Height) Is Shown for Comparison

You Move The Cursor! Enter the Y (row) coordinate: 50 Enter the X (column) coordinate: 5 You cannot move the cursor there!

overlay()

Note how the LIFECYCLE MANAGER uses the activate Lifecycle Operation [VSW02] to allow the servant to do some initialization when it is taken from the pool for example to acquire resources. The reverse is done in deactivate, called after the invocation has been handled and just before the servant is put back into the pool. We do not illustrate STATIC INSTANCES for two reasons. First, a STATIC INSTANCE that is not instantiated lazily is trivial, and is implicitly illustrated with many other examples given in the previous chapters: the server application simply instantiates the remote object s servant and registers it with a LIFECYCLE MANAGER for STATIC INSTANCES, which just remembers the servant and forwards invocations to it. Second, when LAZY ACQUISITION is used, the process is basically the same as in the PER-REQUEST INSTANCE example shown above, except that the single servant so created is not destroyed, and can serve subsequent invocations. Specifically this also requires a type-based registration and a proxy, as in the example illustrated above.

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