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4.4.2 Single Photon Emission CT (SPECT) There are several designs for SPECT, but only the rotating gamma camera system is discussed here (see Fig. 4.11) because it is commercially available. In a rotating camera system the gamma camera is rotated around the object, and the multiple 2-D images series are reconstructed and stored for postprocessing. The camera is composed of a large scintillation crystal of diameter 30 to 50 cm and a number of photomultiplier tubes (PMTs) attached to the opposite surface of the crystal. When a -ray photon interacts with the crystal, the light generated from the photoelectric effect is uniformly distributed among the neighboring PMTs. By measuring the relative signal of each PMT, the camera can locate the interactive position for each event. The drawback of this system is the dif culty of maintaining a uniform speed of rotation with the rather heavy camera. Figure 4.11 shows the schematic of a SPECT. Since a typical tomographic study takes 15 to 20 minutes to accomplish, it is important to maintain patient immobilization. To provide the best sensitivity and resolution, it is desirable to have the camera as close to the patient as possible. Since the dimension of body width is greater than body thickness, an elliptical orbit of rotation of the camera tends to produce a higher resolution image. Different collimators are used for different applications. In general, the reconstruction algorithm must be modi ed and the attenuation values corrected for each type of collimator. For example, a single-plane converging collimator will need a fan-beam reconstruction algorithm, and a parallel collimator will need a parallel-beam algorithm.

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the SBS cell, the four beams again split and follow separate paths through their respective ampli ers and are rejoined in the output beam of the laser Just as with the single-channel long-pulse laser system, a permanent-magnet Faraday rotator located in each ampli er arm isolates the high-energy output pulses from the injected input beam Figure 527 takes on the slightly more daunting task of showing the actual beam paths and component placements used in the phase-locked laser system Although an initial impression might be one of signi cant complexity, a careful comparison of this optical layout to that of the single-channel system shown in Fig 514 easily reveals the direct correlation between the two designs However, there are several unique features to note in the four-beam system 552.

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1 Injection laser mechanical isolation The long-range illumination application for which this laser system is intended demands very high beam point stability As previously discussed for the single-channel system, phase conjugation effectively removes effects of vibration, thermal distortion, and component alignment drift in the ampli er section However, any disturbances transmitted to the injection laser translate directly into the high-power output beam For this reason, the optical bench supporting the injection laser system and that for the highenergy ashlamp-pumped ampli ers are physically separated The injection laser is housed in a separate room and is mounted to a large isolated concrete slab along with the high-precision laser beam director The larger ampli er optical bench is located in an adjacent room.

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Dave Glick - Using ASP.NET MVC and Razor To Generate PDF Files
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Export ASP.Net MVC View to PDF in 3 Quick steps | Rami Vemula
22 Jan 2014 ... Export ASP.Net MVC View to PDF in 3 Quick steps. Step 1 – Create an ASP.Net MVC5 Solution using VS 2013. Create the following model and controller action in the solution. Step 2 – Download Rotativa PDF nuget. Step 3 – Test the application. Press F5 and start the application, navigate to /Home/GeneratePDF.

Beam transport to and from the ampli ers through the adjoining wall is via a 2-m-long 1:1 relay-imaging telescope, providing a high degree of mechanical isolation from the ashlamp percussion and any vibration introduced by the high- ow cooling water through the ampli ers No active alignment is needed between the two benches This would not be possible except for the SBS wavefront correction and rigorous relay-imaging built into the laser system which fully compensate for relative optical bench motion caused by vibration or long-term mechanical drift between the isolated oor slabs The net result is a high-power, 100-J/pulse laser system directly attached to the experimental apparatus that exhibits the spatial footprint and thermal and vibrational signature of the low-power injection laser system (see Fig 528) 552.

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2 The four-beam optical transport system The goal of the design of the optical beam train for the phase-locked ampli er system was to use shared optical components, as possible, to reduce the parts count and overall complexity of the system The 1:1 image-relay telescopes inside the multipass regenerative ampli er train as well as the polarizing beam splitters that couple the beams in and out of the ring are shared by all four extraction beams As can be seen in Fig 527, it is only at the ampli er end of the telescopes that individual beams are picked off and directed through separate zigzag ampli ers The output beam from the oscillator/ preampli er injection system is expanded to a 30-mm round beam before it passes through a 45-mm clear-aperture permanent-magnet Faraday rotator.

The beam is then anamorphically expanded by a factor of four in the horizontal dimension using.

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