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Figure 8 2. Lewis s take on the issue of arrays: 1) Avoid the issue altogether, 2) Trust in Dr. Lewis s pragmatic approach and learn a few helpful tricks here and there, or 3) Go to 4 of Dave and Jeff s advanced book and shake hands with the Devil!

= 0

Here is the output information provided by the client:

Adding new products... Here are the products with name=Juice: Carton of apple juice Carton of cranberry juice Here are the products that cost $1: Toasted Sesame Almond Cranberry and Carrot Glass of milk Carton of apple juice Carton of cranberry juice Deleting products added..

= ( 2 0 0 ) = 2 0 0 = 2 0 [( 0 )( )]T = 2 0 0 = 2 0 Now, we use the fact that the metric is symmetric, so 0 = 0 . Adding our two expressions, we get 2 = 2 0 ( + ) 2 We can write + in terms of components and use the fact that the components are anticommuting Grassman numbers to show that the rst term vanishes. First we have = ( + ) = + + + + We also have

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If you re still here and haven t skipped ahead to 9, or put the book away entirely then I am assuming you are willing to go along with the program for this next part of our journey. It is important that I communicate two caveats: You will, at times, think that I m not giving you enough details about arrays. You will, at times, think that I m giving you too many details about arrays. In other words, please show the same awesome flexibility and patience that you have demonstrated up to this point in our give and take partnership. Trust me! Fair enough OK then let s get down to business.

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

= (

Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Sat Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan Jan 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 20 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 13:20:42 EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST EST 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10000] 2007:EntityCMPBean:ejbPostCreate() [primary key=10000] 2007:EntityCMPBean:ejbStore() [primary key=10000] 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10001] 2007:EntityCMPBean:ejbPostCreate() [primary key=10001] 2007:EntityCMPBean:ejbStore() [primary key=10001] 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10002] 2007:EntityCMPBean:ejbPostCreate() [primary key=10002] 2007:EntityCMPBean:ejbStore() [primary key=10002] 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10003] 2007:EntityCMPBean:ejbPostCreate() [primary key=10003] 2007:EntityCMPBean:ejbStore() [primary key=10003] 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10004] 2007:EntityCMPBean:ejbPostCreate() [primary key=10004] 2007:EntityCMPBean:ejbStore() [primary key=10004] 2007:EntityCMPBean:setEntityContext() called. 2007:EntityCMPBean:ejbCreate() [primary key=10005]

This means that 2 0 ( + ) = 0 , and so we are able to write = . Returning to the main thrust of our discussion, in general, space-time coordinates will transform as x x i under a supersymmetry transformation, where are the usual Dirac matrices. Now let s consider the action of the supersymmetry generator on the fermionic or super-worldsheet coordinates. We simply state the result which you can work out in the Quiz:

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