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Also, it is possible to have the piece of work executed in the context of a transaction imported by the resource adapter, rather than the context associated with the current thread. The third parameter is an optional ExecutionContext.

} public class UcnyWorkJob implements Work {

Therefore the Polyakov action is invariant under a Weyl transformation. Since Eq. (3.12) is dependent on the space-time coordinates ( , ) of the worldsheet, it is a local symmetry.

#import "helloWorld_005ViewController.h"

void run() { // HERE IS WHERE THE WORK ACTUALLY TAKES PLACE } }

Gauge freedom can be used to simplify the worldsheet metric. What this means is that we can use the symmetries of the action (i.e., utilize the transformations that leave the action and hence the physics unchanged) to write the worldsheet metric in a more convenient form, that is sometimes called the ducial metric h ( ). Here we consider a worldsheet with a vanishing Euler characteristic (a cylinder is relevant to our interest). The worldsheet has only two coordinates ( , ), and this means that h is a 2 2 matrix: h00 h = h10 h01 h11 (3.13)

void release() { WHEN WE FINISH THE WORK WE RELEASE THE RESOURCES } }

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This is going to make things particularly easy for us. We immediately nd that there are only three independent components of the worldsheet metric. This is because, in general, the metric tensor g is symmetric, so that g = g The fact that the metric is just 2 2 means that the symmetry requirement xes the off-diagonal components: h01 = h10

@implementation helloWorld_005ViewController @synthesize label, uiImageView; - (IBAction)buttonPressed:(id) sender{ label.text = @"Hello World, I'm back!"; UIImage *imageSource = [UIImage imageNamed: @"kera.png"]; uiImageView.image = imageSource; }

These two characteristics are combined, but they can be separated, because at times it is useful to describe the structure and behavior separately.

So, this means that we only have to specify three components of h . The choice can be simpli ed by using two of the local symmetries of the Polyakov action. From the previous section we recall that these are Reparameterization invariance Weyl transformations The rst case, reparameterization invariance, that is, a coordinate transformation, can be used to take the metric into a form that is proportional to the two-dimensional at Minkowski metric as follows: 1 0 h e ( , ) = e ( , ) 0 1 (3.14)

FIGURE 3-14

Collaboration diagrams can be enhanced by the inclusion of the dynamic behavior of the message sequences exchanged among objects to accomplish a specific purpose. This is called an interaction, and it helps in understanding the dynamics of the system and its participating objects.

This form happens to be particularly useful, because now we can apply a Weyl transformation to get rid of the exponential factor. The end result is that it is possible to use the local symmetries of the Polyakov action to take the worldsheet metric into the at Minkowski metric: 1 0 h = 0 1 (3.15)

If this doesn t quite make sense at the moment, that s OK. There sure are a lot of entities with image as part of their name, object, or association, and it is confusing. We ll be examining this topic more thoroughly in 7, so, right now, don t lose any sleep over it! Figure 5 8 illustrates how your code should appear at this point.

Objects have state or status. The state of an object depends on the current activity or condition. A state diagram illustrates the states of the object and the input and transitions that cause changes in the state. The state diagram shows the sequences of states that an object passes through during its lifetime. They correspond to prompts for input coupled with the responses and actions. A state machine is a diagram of states and transitions that describe the response of an object of a given class to the receipt of external stimuli, and it is generally attached to a class or a method. A state diagram represents a state machine: a state being a condition during the life of an object or an interaction during which it

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