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orientation also enhances the anisotropy in the irradiated areas, and surprisingly, the polarization dependence remains the same as in the relaxed state, although the diffraction ef ciency increases. Upon UV light exposure, irradiated areas lose the orientation of azobenzene mesogens because of the trans cis photoisomerization, which should initiate the formation of the grating. However, when the lm is relaxed, both irradiated and nonirradiated areas lose the orientation of azobenzene, and irradiated areas recover to the trans-rich state after B10 h at room temperature. In other words, if the refractive index modulation originates only from differences in azobenzene conformation and orientation, it should disappear. Therefore, the stable grating observed in the relaxed lm implies that some permanent structural or morphological changes occurred during the photoisomerization of azobenzene in the irradiated regions. More information on the grating formation mechanisms can be obtained by holographic recording as described later in following text.



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Figure 44-9: IP Fragmentation Figure 44-9 illustrates an example A datagram 4,000 bytes arrives to a router, and this datagram must be forwarded to a link with a MTU of 1500 bytes These implies that the 3,980 data bytes in the original datagram must be allocated to three separate fragments (each of which are also IP datagrams) Suppose that the original datagram is stamped with an identification number of 777 Then the characteristics of the three fragments are as follows: 1st fragment r 1480 bytes in the data field of the IP datagram r identification = 777 r offset = 0 (meaning the data should be inserted beginning at byte 0) r flag = 1 (meaning there is more) 2nd fragment r 1480 byte information field r identification = 777 r offset = 1,480 (meaning the data should be inserted beginning at btye 1,480 r flag = 1 (meaning there is more) 3rd fragment r 1020 byte (=3980-1480-1480) information field





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This example shows two Modular Avionics Units (MAUs); however, it is more typical to use four such units to host all the avionics and utilities functions. It can be seen from this example that the ambitions of Honeywell in wishing to maximise the return on their EPIC investment is driving the levels of system integration in the regional aircraft and business jets to higher levels than the major OEMs such as Boeing and Airbus. A publication which addresses ASCB and compares it with other data buses is at reference [9]. This reference contains much useful data regarding the certi cation of data bus systems. For an example of a fuel system integrated into the EPIC system see the paper at reference [10] which describes the integration of the Hawker Horizon fuel system into the Honeywell EPIC system.

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Instead of using a UV lamp and a grating photomask, an interference pattern generated by two coherent beams of a UV laser (krypton, l = 350 nm) can be used to write a grating on a stretched ATE lm. While placing the probe light (633 nm) at the same exposed area, the grating formation dynamics can be monitored by measuring the change in diffraction ef ciency. The authors used such an optical setup to get more insight into the mechanism of grating formation. In the experiments, the two recording beams producing the interference pattern were

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both linearly polarized perpendicular to the SD (s s geometry), with the crossing angle adjusted to yield various periods The holographic gratings recorded were in the Raman Nath diffraction regime, the fringes were perpendicular to the SD, and the polarization of the probe light was parallel to it Again, since azobenzene mesogens are oriented along the SD in the lm before the exposure, the grating a priori should be a grating whose spatial modulation of refractive index arises mainly from the difference between oriented trans-azobenzene in nonirradiated regions and disordered cis-azobenzene in irradiated regions The dynamic process of grating formation was monitored for a series of lms stretched to various degrees to reveal the role of deformation Figure 1112 presents the results (the recording beams were switched on at the zero time).

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