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3 Click a property in the Data Sources window The property item changes to a drop-down control list 4 Drop down the control list and select the desired control type Select Customize from the list to select a control type that is not on the list You can select just about any type of control, including third-party and custom controls

For a discussion on the shortcomings of Dirac's formalism in quantum mechanics, see [231] Even though position was represented by an operator in Section 21, time was only a parameter There have been attempts to promote time to an operator, too [10,85] But the modem approach in quantum field theory is to make position also a parameter, as in Section 24 The lack of a time operator implies that the time-energy uncertainty relation does not have the same status as the positionmomentum uncertainty relation in nonrelativistic quantum mechanics, for it cannot be derived from fundamental commutation relations [649] We will get back to this issue in 3 Some of the key papers on the old quantum theory are collected in [591] Key papers on QED can be found in [544].

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NOTE: Before a third-party control can be added as a control type in the Data Sources window, it must first be added to the Forms Designer toolbox

For the early history of QED and a nice description of Born and Jordan's seminal work [68], see [447] Key papers from the early days of quantum optics can be found in [359] The latter reference also has a very pedagogical introduction to field quantization Two very good introductions to Feynman's version of quantum mechanics are the marvelous book by Feynman and Hibbs [204] and the very interesting paper [430] For a popular version of Feynman's approach to QED, see [201] (another interesting popular book related to this chapter is Podolny's book about the vacuum [493]) For a more detailed account of Feynman's approach to QED, see [203] If you would like to know more about Green's functions, reference [642] gives a brief elementary account of them For a more complete account, see Barton's excellent book [40].

22 of [2061 shows how cavities can be seen as the high-frequencycounterparts of ordinary electronic lumped-circuit oscillators (eg, LC oscillators) For a detailed calculation of perfect cavity modes, see Appendix A and also 2 of Haus's book [276] The formal analogy between Poisson brackets and commutators can also be used to do calculations in classical electrodynamics very similar to the way they are done in quantum electrodynamics (ie, with mode expansions and using the harmonic oscillator Poisson brackets satisfied by the expansion coefficients) This field oscillator approach is described and applied in [90, 233]..

Effective Java: Programming Language Guide // HORRIBLE PROGRAM - uses busy-wait instead of Objectwait! public abstract class WorkQueue { private final List queue = new LinkedList(); private boolean stopped = false; protected WorkQueue() { new WorkerThread()start(); } public final void enqueue(Object workItem) { synchronized (queue) { queueadd(workItem); } } public final void stop() { synchronized (queue) { stopped = true; } } protected abstract void processItem(Object workItem) throws InterruptedException; private class WorkerThread extends Thread { public void run() { final Object QUEUE_IS_EMPTY = new Object(); while (true) { // Main loop Object workItem = QUEUE_IS_EMPTY; synchronized (queue) { if (stopped) return; if (!queueisEmpty()) workItem = queueremove(0); } if (workItem != QUEUE_IS_EMPTY) { try { processItem(workItem); } catch (InterruptedException e) { return; } } } } } }

When you drag the control from the Data Sources window to the Forms Designer, Visual Studio renders the type of control you selected as the default control type for the property The property retains its default control type in the Data Sources window

If you have trouble following the various manipulations of vector expressions involving \l in Section 2.2 and in Appendix A, have a look at Appendix E.

Milonni's book [451] offers a quite comprehensive pedagogical account of the Casimir effect, including a discussion of the curious model that Casimir proposed for the electron. Most of the important literature on the Casimir force is listed in [377], with key advances discussed in detail in the recent review [66]. For a recent measurement of the Casimir force, see [97]. For a calculation of the fluctuations around the expected value of the Casimir force (i.e., variances), see the chapter by Barton in [49] . For more on the vacuum catastrophe, see [5, 316, 483, 511, 629].

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