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where d is the ruling s line pitch, y is the angle between the ruling s lines, and a is the rotation angle of the moire pattern (Fig. 17.21). This method is useful for long focal distance lenses (> 1 m). A variant of this method is shown in Figure 17.22 (Glatt and Kafri, 1987). This setup looks for a collimated beam of light that is achieved through the mirror displacement. Under perfect collimation, the mirror position de nes the focal point position. Back focal distance could be measured by measuring the distance between the mirror position and the last lens surface. This new set-up allows the focal distance measurement for a lens of any focal distance, not only long focal distances. (b) Talbot Autoimages. Talbot autoimages are produced by periodic Ronchi rulings in a coherent beam of light (see 9.). Talbot method is done with a coherent collimated beam of light illuminating a periodic amplitude or phase grating. Periodically and equally spaced, an image of the grating will be produced as shown in Figure 17.23. Every Talbot autoimage is considered an object for the lens that produces an image of the same autoimage at the lens image space. Two methods are used to nd the focal lens: One is to put another ronchi ruling coincident with one of the autoimages (Malacara Doblado and Malacara-Hernandez, 1996) (Nakano and Murata, 1985).

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5.4.4 Multimodality 3-D Micro Scanners Software Image Fusion In the animal imaging research center discussed in Section 4.9 and shown in Figures 4.23, 4.24A, B , C , imaging modalities mainly included optical imaging, digital radiography, micro US, micro PET, micro CT, and micro MRI. Some of these imaging modalities are shown in Figure 5.12. Image fusion was also performed on the images from some of these modalities, among them the micro PET-CT image fusion. Because there does not yet exist any hardware image fusion mechanism in the micro imaging domain, the image fusion had to be done with software processing. Figure 5.13 shows some of the results obtained from an animal study with the two separate CT and PET scanners presented in Figure 5.12.

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gather statistics, logging, adding security constraints, and so on. These hooks allow for the runtime manipulation of a flow execution. The FlowExecutionListenerAdapter class is an abstract convenience class for creating your own listeners.

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This section provides a brief introduction to some of the terms you ll encounter in the rest of this chapter. A socket is a network connection endpoint. When your Web browser requests the main Web page of www.python.org, for example, your Web browser creates a socket and instructs it to connect to the Web server hosting the Python Web site, where the Web server is also listening on a socket for incoming requests. The two sides use the sockets to send messages and other data back and forth. When in use, each socket is bound to a particular IP address and port. An IP address is a sequence of four numbers in the range of 0 to 255 (for example, 173.15.20.201); port numbers range from 0 to 65535. Port numbers less than 1024 are reserved for well-known networking services (a Web server, for example, uses port 80); the maximum reserved value is stored in the socket module s IPPORT_RESERVED variable. You can use other port numbers for your own programs, although technically, ports 1024 to 5000 (socket.IPPORT_USERRESERVED) are used for officially registered applications (although nobody will yell at you for using them). Not all IP addresses are visible to the rest of the world. Some, in fact, are specifically reserved for addresses that are never public (such as addresses of the form 192.168.y.z or 10.x.y.z). The address 127.0.0.1 is the localhost address; it always refers to the current computer. Programs can use this address to connect to other programs running on the same machine.

Figure 3.19. Top: Measured pulse energy of an sf-SBS laser as a function of the optical start resonator length for SF6 as SBS material. Every data point is an averaged value over 500 measured single pulse energies. The error bars give the standard deviation. The length of the SBS resonator was 2LB. The two vertical lines indicate the third and fourth resonant start resonator length equal to 3LB and 4LB. Bottom: Measured burst energy for the same laser as a function of the optical start resonator length normalized to the Brillouin length LB of the used SBS materials xenon SF6 and CO2. Each data point is an averaged value over 500 measured burst energies. The error bars give the standard deviation. The lengths of the SBS resonator were 2LB for SF6 and xenon and 3LB for CO2.

DBMS_OUTPUT.PUT_LINE( Not accounting or sales ); END CASE; END;

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