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This means that when deriving a variant V, if there are receiving events whose sending partners can be changed but are not changed, these unchanged receiving events cannot be changed afterward in any sequences derived from V Recall that it is common for a variant to leave some receiving events unchanged since all combinations of changed and unchanged receiving events are enumerated in the race table Constraint C2 ensures that a particular set of changes occurs in only one variant To illustrate Constraint C2, consider sequence Q0 and its three variants in Fig 731 A variant and the sequence that was collected from it are shown in the same space-time diagram, with the variant above the dashed line and the rest of the sequence below it The SV-graph and spanning tree for these sequences are also shown in Fig 731.

You don't present the data in the raw form as they come from the data source, but in a form that the patterned item wants in the JTree case, TreeModel View information is the rendering part of the pattern Rendering is provided by you, but the patterned item requests the information through a factory class that you must implement TreeCellRenderer You can view the item in several different ways, and so TreeCellEditor is also a view component to this pattern Finally you have the controller part of the pattern The controller is responsible for management tasks and any logic Control actions are provided by the JTree class, because it must hook the listeners of the data model and make the appropriate requests for rendering components, and then arrange for all the right bits to appear on screen.

denote the first- and second-order effects in log-linear parawhere j1 and l1 j1 meterization, respectively. From Equation (21.2), it is apparent that any restriction on conditional probabilities may be equivalently imposed on the log-linear parameters. The specification of a model as the product of conditional probabilities has the advantage of more direct interpretation, whereas log-linear parameterization is more flexible and allows more parsimonious models to be specified. The breakdown of conditional probabilities does imply estimation of the entire set of interaction parameters, while the modified LISREL approach allows us to specify models in which some higher order interactions among variables may be excluded or conveniently constrained.

Jumping ahead just a little here the MVC pattern can be applied to enterprise applications just as much as a GUI API Now, you are looking at a much larger scale The model is the underlying data system, such as the database and the entity beans On the other end of the application are the JSPs and servlets that make up the pages the View portion of the pattern In between you need the control logic to assemble a user's shopping basket, which is the control part of the pattern Almost every enterprise application that has been developed can be broken into these three components, and hence conforms to the MVC pattern..

Notice that the SV-graph contains paths Q0Q2Q3 and Q0Q3, both of which are paths from Q0 to Q3 Constraint C2 excludes path Q0Q2Q3 from the spanning tree To see this, observe that receiving events r2 and r4 exist in Q0 and also in Q3, but the messages they receive in Q0 are different from the messages they receive in Q3 Also observe that edge V2 along the path Q0Q2Q3 only changes the sending partner of r4, leaving the sending partner of r2 unchanged The sending partner of r2 is changed afterward by the edge from Q2 to Q3 Thus, path Q0Q2Q3 violates Constraint C2, which prohibits r2 from being changed in any sequences derived from V2 since r2 could have been changed in V2 but wasn t.

It wasn t until spring 1941 that Feynman accidentally came across a paper by the British physicist Paul Dirac, describing how a very small portion of what Feynman wanted to do could be achieved. In one of his remarkable leaps of intuition, Feynman saw how Dirac s work could be generalized. The result, as often was the case with Feynman, was a very visual approach. This involved considering the possible world lines of a particle. These are graphs where the particle s position in space is plotted against time. If time goes up the page and space across, a particle that is not moving at all will be described by a straight line up the page. One that is moving at a steady speed will be shown as a diagonal straight line. The world line is a map of the history of a particle s existence. Feynman saw that he could fully describe a particle s behaviour by drawing every possible world line linking its starting and nishing position and pulling them together with the probability of such a line occurring. This sounds an impossible task, but ever since Newton and Leibniz had come up with calculus it had been routinely possible to combine an in nite number of components, provided the values got smaller and smaller.