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diminished performance of grating The conditions for recording holographic gratings remain to be optimized It is expected that using more ef cient visible light photoinitiators for faster photopolymerization may improve the segregation between the azobenzene polymer and the LC 11523 What Determines the Switching Performance Using the preceding design of materials, the diffraction ef ciency and switching performance in terms of speed and stability could be improved by choosing appropriate materials and adjusting the preparation conditions First, the nematic LC should have a large birefringence with its no equal to np, given a good planar alignment This will give rise to large index modulation and thus high diffraction ef ciency for the grating and no or negligible diffraction when an electric eld or UV light is applied Second, upon photopolymerization, the polymer should segregate as thoroughly as possible from the LC to form the periodic grating structure.

=<t>(X,Y,Re,Sc)

When deciding between switch modules and pass-through connections to external switches, investigate whether you have any special features on your current switches that may not be available in the switch module that runs in your chassis. Also check for compatibility between switch vendors (of switch modules and your existing external switches).

For the investigated system, there is a small amount of azobenzene polymer that remained in the LC regions, which, as argued, is responsible for the optical switching based on photoinduced nematic isotropic phase transition However, it is likely that even with complete separation of the polymer from the LC, mesogenic azobenzene groups in the interface between the two regions could accomplish the optical switching While ensuring the optical switching of diffraction, the absence of azobenzene polymer in the LC regions is desirable because homogeneous LC orientation can be induced by rubbed surfaces, which determines the high diffraction state, and the electric eld induced reorientation of LC molecules can develop without interaction with the polymer, allowing the electrical switching of diffraction to be governed by the behavior of pure nematic LC.

(2.7.28)

143 Experimental measurements yield the mean value of the material flux JY, independent of the coordinates X and Y. If a further dimensionless parameter, the Sherwood number, is introduced,

Third, experimental conditions can be optimized by taking into account several factors that were found to affect the grating formation and switching performance: (1) Polymerization in the isotropic phase generally results in a better grating, probably because of the high uidity that favors the diffusion or transport of the monomer and thus the segregation between polymer and LC (2) Long polymerization time (1 2 h) is necessary to complete the reaction with the used visible light photoinitiator, whereas photoinitiators absorbing longer wavelengths may afford faster polymerization by reducing the interference of azobenzene monomers and polymer (3) With the used materials, a concentration of 15% 20% for the azobenzene monomer is necessary.

For I/O to storage devices, most blade chassis offer the option to use on-blade storage and/or to connect to a SAN or NAS. Diskless blades were introduced by Egenera in the very early days of blades and now are being implemented more frequently across all blade-vendor chassis. Q Do you have a requirement for local disk storage on each/all blade(s), or can you configure your blades to have shared access to storage on a SAN

then Eqs (2.7.1) and (2.7.28) yield the criterial equation Sh = F(Sc, Re) For the thickness of the Nernst layer we have (cf. Eq. 2.7.2) (2.7.30)

At higher concentrations, the segregation between polymer and LC is not thorough and the polymer remained in LC regions is too much to allow good surface alignment for the LC, whereas at lower concentrations, the amount of polymer in irradiated areas is not suf cient to have large polymer strips..

( 73) 2 1

With the boot-from-SAN option, using diskless (also known as anonymous) blades eliminates state from the blade, allowing simpler provisioning/reprovisioning since you don t have to worry about how to access (or back up) the information on the on-blade storage.

In all the studies discussed, the grating is transmission-type, with the grating vector lying in the sample plane. Using azobenzene-containing polymer-stabilized and polymer-dispersed LCs (PSLCs and PDLCs), Bunning and coworkers

In convective diffusion to a rotating disk, the characteristic velocity Vo is given by the product of the disk radius r, as a characteristic dimension of the system, and the radial velocity a>, so that the Reynolds number is given by the equation Re = (2.7.32)

demonstrated the preparation of re ection gratings that can be switched by light (Urbas et al, 2004a,b) By lling a photosensitive LC/monomer mixture in an ITO-coated cell, they succeeded in using an interference pattern to record a grating structure whose vector is perpendicular to the sample plane In this case, the periodic modulation of refractive index goes along the plane normal and the grating acts as a Bragg re ector exhibiting wavelength selective re ectivity With the LC host doped with an LC azobenzene compound, the reversible trans cis photoisomerization can be used to optically change the orientational state of the LC and thus the modulation of index, making it possible to switch on and off the re ected (diffracted) light In one case (Urbas et al.