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The slk_attron() function applies the standard text attributes to the soft labels. It is the soft label key equivalent of the attron() function.

Figure 5.15. Typical SEM image of the colloids after they are irradiated by two laser beams with orthogonally polarized directions, each for 10 min. Source: From Li et al., 2006b.

int slk_attron(const chtype attrs); int slk_attr_on(attr_t attrs, void* opts);

Location Forwarder Therefore:

attrs is a chtype variable representing one or more attribute constants as defined in NCURSES.H. NULL is used in the slk_attr_on() function as a placeholder for the undefined opts value.



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The differentiation between the irradiation effects of the polarized laser single beam and the interfering p-polarized laser beams can be observed by using 2-D arrays of the colloidal spheres as the testing samples. The samples were prepared by the vertical deposition method, which is discussed in Section 5.5. By this method, the hexagonally close-packed structure of the colloid spheres can be obtained. Different deformation behavior can be observed after irradiating the colloidal array with the polarized laser single beam for 15 min or the p-polarized interfering laser beams for 20 min. For the former, the colloidal spheres are uniformly stretched along the polarization direction of the laser beam. As the restraint of the neighboring colloids, the deformation degree of the colloids in the array is less than that of the isolated colloids. Changing the relative direction of the polarization to the array assembly direction shows no in uence on the stretching effect. On the contrary, after being irradiated with the interfering laser beams, only the colloids in bright regions of the interference fringes are changed, whereas those in the dark regions are almost unaffected. The exact mechanism of the deformation induced by the laser single beam is still not clear. In the experiment, the light intensity of the spatially ltered and collimated laser beam (1.5 cm in diameter) should be uniform in submicrometer size. This phenomenon has been further con rmed in another type of colloid composed of well-de ned polymeric chains (Lambeth and Moore, 2007). Such observations cannot be directly explained by using the gradient force of the laser irradiation. More investigations, both through theoretical and experimental approaches, seem to be required to understand this unusual photoresponsive effect.





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As with attron(), the slk_attron() function merely adds attributes to those already set. Setting a new attribute does not affect previous attributes applied to the soft labels. Soft label keys are normally displayed with the A_STANDOUT attribute applied. Multiple attributes can be applied by using more than one NCurses attribute constant separated by a logical OR in the slk_attron() statement.

For remote objects that the INVOKER cannot resolve locally, make a LOCATION FORWARDER forward invocations to the remote object in another server applications. The LOCATION FORWARDER looks up the actual location of the remote object based on its OBJECT ID. The result of this lookup is an ABSOLUTE OBJECT REFERENCE of another remote object. The LOCATION FORWARDER has two options: either it sends the client-side distributed object middleware an update notification about the new location, so that the client can retry the invocation on the new location, or it transparently forwards the invocation to the new location.

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Refer to Table A-1 (in the attrset() entry) for a list of NCurses attribute constants. COLOR_PAIR(n) can be specified as a text attribute, where n is a color pair number defined by an init_pair() function earlier in the program. Also see the slk_color() function. Individual labels can be assigned unique attributes by using slk_attron() or slk_attrset() and then issuing a slk_set() function to update one or more labels. The updated labels show the newly applied attributes.

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