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shear that may be easily controlled. Chang et al. (2002) raised concern that the amount of phase shift is actually not completely repeatable. It possibly offers the source of error upon introduction of unknown phase shift. Suhara (2002) used a wedge with gap to measure the distribution of the index of refraction in plastic lenses, by additionally performing computational tomography. One very important application of the lateral shearing interferometer incorporating a wedge is in vivo measurement of tears and arti cial tears in human eye. LechnaMarczynska et al. (1999) were the rst to use a simple wedge to perform such measurements. Dubra et al. (2004, 2005) recently took up this work. They used double lateral shearing interferometer, also referred to as a three-dimensional shearing interferometer to pro le tear surface. When the wedge moves in the direction along one of its prismatic surfaces, the optical path of the incident beam changes, that is, the wedge thickness as seen by the ray changes. This feature may be used to introduce the phase change into the wavefront by moving the wedge. The controlled introduction of the phase change

You now have two rectangles, but because you re looking from the top, you see only one. 5. Choose View 3D Views SE Isometric. Now you can see the two rectangles, as shown in Figure 21-8.

Specify start angle or [Parameter]: Use the Endpoint object snap to pick the free endpoint of the line on the right. Specify end angle or [Parameter/Included angle]: Use Endpoint object snap to pick the free endpoint of the line on the left.

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Figure 6.14. SBS re ectivity of a single-mode pump beam focused into the 300-mm-long fused-quartz glass with 300-mm (500-mm) focusing lenses.

>>> db.keys() [ secretCombination ] >>> db.close()

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description of stability requirements for excipients is provided in Section 7.1.2.2. The principles underlying the evaluation of stability data and determination of shelf life (retest dates) for excipients is similar to that described for APIs and drug products in Section 7.1.7.

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The first entry in this file uses the domain keyword to specify the default domain to use when looking up short host names, such as win2k, ubuntu, myserver, and so on. This entry prevents you from always having to specify the name of your local network. In this case, my default domain is vonhagen.org, which means that if I try to contact a host named myserver, the DNS system first attempts to locate the IP address for that name, and then automatically looks for the IP address for the host myserver.vonhagen.org. The remaining entries in this file identify the IP addresses of different name servers that your system should contact when trying to map host names to IP addresses. These name servers are queried in order, and are identified by their IP address because your Linux system would otherwise have to try to use DNS to map names to IP addresses, which would present an interesting bootstrapping problem when trying to find the IP address of the first name server in this file. Like most programs and configuration files in Linux, online help on the contents and format of this file is available using the Linux man command: man resolv.conf.

particles departing the aperture and those remaining in the accelerator For instance, the phase space at the second septum might appear as shown in Figure 46(b) The 90" rotation between the two figures projects the kick of the first septum fully onto the second septum; the orientation of the first ensures that the extracted beam is well displaced from the circulating beam in the second All that remains to be specified are the strength of the resonance driving terms-the integrals A and B above-and the tune difference, 6 v , from resonance Since the ratio of A and B is already set by the orientation of the separatrices at one of the septa, only two quantities remain to be determined There are two conditions to be satisfied.

Body mass index (kg/m2)

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