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14.4 WEB SERVER Section 14.3 described the concept of the distributed image le server, which provides easy access to PACS image/data for different applications. In this section we present an image le server design based on the World Wide Web technology that allows easy access to PACS image/data for both inter- and intrahospital applications. 14.4.1 Web Technology In 8 we presented network and communication technology. This section rst reviews the Web technology development over the past years and then presents a Web-based image le server for PACS application. To recap, the Internet was developed by the U.S. government originally for military applications. Through the years its utilization was extended to many other applications. The Internet can be loosely de ned as a set of computers connected by various wiring methods that through TCP/IP transmit information to each other (Section 8.1.2) using a public communication network. The Intranet, on the other hand, is a private Internet that transmits information within an administrative entity

Substituting these expressions in (5.61) yields a system of three equations in a, b, and c. Closer examination reveals that both first equations of this system are linear in a and b and nonlinear in c. The third equation is nonlinear in a, b, and c. Example 5.7 shows that maximum likelihood estimation of a, and y using the likelip, hood equations implies finding all solutions of three nonlinear equations in three unknowns and investigating which solution represents the absolute maximum of the likelihood function. Since the equations to be solved are nonlinear, generally no closed-form solution is available. This is the reason why this kind of estimation problem has to be solved by iterative numerical methods. Usually, the numerical method chosen consists of directly maximizing the log-likelihood function instead of solving the likelihood equations for all possible stationary points and selecting the absolute maximum. Suitable numerical optimization methods are described in 6. On the other hand, the alternative problem of estimating the parameters a and p for a known parameter 7 requires the solution of both first equations only. Since these are two linear equations in two unknowns, the solution is closed-form and, generally, unique. Then, the maximum likelihood estimate of the parameters is computed in one step and no iterations are needed. This attractive closed-form and, typically, unique maximum likelihood estimator occurs whenever the observations are normally distributed and, in addition, the expectation model is linear in the parameters. This important special case will be the subject of Subsection 5.4.3. Finally, we mention that parameters like cr and /3 are usually called linear parameters and parameters like 7 nonlinear parameters.

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3.4.2.2 Number of antenna elements. The dimensions of the rectangular array are determined by N1 and N2. The absolute value of the beamformer angle 80 can be related to the number of elements in the directions n1 and 722 in a way that for 00 = 0" and l6ol = go", a maximum number of antenna elements in the directions

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One can loosely classify the launch trajectories of pellet injection into two categories: HFS (or high- eld side) launch in which the pellet is injected from the inside of the tokamak and LFS (or low- eld side) launch in which the pellet is injected from the outside of the tokamak. It was experimentally observed that the HFS launches of the pellet lead to a signi cantly better fueling ef ciency of the core of the tokamak than the LFS launches. Identifying and quantifying the causal MHD mechanisms in HFS versus LFS pellet launches are the goals of this research. As a frozen pellet of hydrogen or deuterium is injected into the hot plasma tokamak fusion reactor, it is rapidly heated by long mean-free-path electrons streaming along magnetic eld lines, leading to ablation at the frozen pellet surface, with a shield of neutral gas and an ionized high-density plasma cloud around it. This forms a local high- 6 plasmoid, which implies a localized region of high pressure. This can trigger MHD instabilities [26]. Furthermore, the high- plasmoid expands along the magnetic eld lines, and the plasma cloud drifts in the direction of the major radius. This drift was observed in experiments on ASDEX7 Upgrade tokamak, as well as DIII-D8 and JET [16]. Thus, pellets injected on the high- eld side showed a much better penetration and fueling ef ciency than pellets injected on the low- eld side.

Second Normal Form (2NF)

The users then map the SINR in (7.4) and (7.5) to the achievable rate with and without the dominant interference. This pair of rates defines the CSI. The actual mapping between the SINR values and the achievable rates is a function of fading profiles and the available ACM techniques; please refer to 5 for examples of the rate-SINR functions. By defining such a CSI structure, the user s feedback information to BS is reduced to a pair of rates rather than transmitting the signal strength and interference received from A BSs. 4

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