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Very often authors of programming books do the same old thing. They first present a very simple, ubiquitous Hello World application and then throttle the user with intense code that loses a great many readers and students straight away. Utilizing Objective-C (being run in Cocoa) along with the iPhone and iPad SDK, I ve had to really rethink this introductory process. I have identified three challenges here. Teaching you Hello World and then going into advanced technologies and APIs would be counter-productive. It makes no sense to randomly choose one of the many ways to say Hello to the world from your iPhone or iPad. They are all going to be necessary to have in your toolkit at a later date. Trying to write a simple Hello World application in Objective-C is more involved than the beginner is ready for, unless we break up the process into stages or layers. My solution to overcoming these issues is simple. I ll show you how to say Hello to the world from your iPhone/iPad in not one, not two, but quite a few different ways. Each time, we ll go a little bit deeper, and we ll have a blast as we do so. Each time you travel down the road into the land of Xcode, you are immediately asked what type of vehicle you d like to drive. A Jeep A race car A convertible By focusing on basics, I am going to show you how to drive in Xcode. The objective here will be to gain competence and confidence in whatever style of vehicle we must access. So, let s take a look at exactly what these different vehicles have to offer. Here I would like you to follow along with me.

(p ) (p )

Here is the output information provided by the client:

(8.27)

This is a message from a stateless session bean!

Assuming that you have already downloaded the SDK and installed Interface Builder, Xcode, and the iPhone/iPad Simulator, open up your Mac and click the Xcode icon on your dock. Your screen should look similar to Figure 1 9. Up pops the Welcome to Xcode window; it includes all your iPhone and iPad resources.

and subtracting Eqs. (8.21) from (8.20) gives N R N L = nK (8.28)

Here is the output information provided by the client and the application server console:

So notice we have extra terms in the formulas for mass [Eq. (8.27)] and the level matching condition [Eq. (8.28)] as compared to the formulas introduced for the

...when the jar is deployed to the server... Sat Jan 20 12:58:55 EST 2007:SLSessionBean:4536570 ejbCreate()

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Figure 1 9. After clicking the Xcode icon, you will see the Welcome to Xcode screen. Keep the Show at Launch option checked.

20 12:58:55 EST 2007:SLSessionBean:2076276 the client application is executed... 20 12:59:15 EST 2007:SLSessionBean:2076276 the server is shut down... 20 13:01:33 EST 2007:SLSessionBean:2076276 20 13:01:33 EST 2007:SLSessionBean:4536570

bosonic string in Chap. 2. The extra terms are due to two components, the KaluzaKlein excitations and the winding states of the string. The Kaluza-Klein excitations can be regarded as particles and so cannot be thought of as due to strings in a general sense. However the winding excitations can only come from strings, because only strings can wrap around a compacti ed extra dimension. Now let s look at the mass formula in Eq. (8.27) together with the relations for the momenta in Eqs. (8.22) and (8.25). Our task here is to consider limiting behavior. First we consider the case where R . In this limit, the momentum goes to the continuum limit and the Kaluza-Klein excitations disappear. It is simple to show that pL = pR and hence the winding state w= 1 25 25 p pR 0 2 L

ejbCreate() getMsg() ejbRemove() ejbRemove()

The center of mass momentum Eq. (8.8) returns to the nonquantized, continuous momentum of the noncompacti ed case. Now let s think about the opposite limit where R 0. You might also expect that this is like returning to the noncompacti ed case. After all, taking the limit R 0 is like making the extra dimension go away. In quantum eld theory we might expect the elds to completely decouple from that unseen extra dimension. However, things don t quite work this way in string theory. As R 0, we nd that the Kaluza-Klein modes become in nitely massive and decouple from the theory. Since these can be regarded as particle states, maybe this isn t so surprising. What s left behind for the center of mass momentum are the winding states. First note that as R 0 we obtain p R = pL Hence p 25 0 but the winding term behaves in the following way: w= 1 25 25 25 pL pR pL 2

When a client calls an EJB, the ultimate goal is to gain the benefits derived from executing the business methods on a bean class. Before the EJB can get access to these methods, it must first find the EJBHome interface necessary to make an instance of the EJB class. The first step in the process of finding the EJBHome starts with creating an InitialContext class.

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