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The idiom takes advantage of the guarantee that a class will not be initialized until it is used [JLS, 1241] When the getFoo method is invoked for the first time, it reads the field FooHolderfoo, causing the FooHolder class to get initialized The beauty of this idiom is that the getFoo method is not synchronized and performs only a field access, so lazy initialization adds practically nothing to the cost of access The only shortcoming of the idiom is that it does not work for instance fields, only for static fields In summary, whenever multiple threads share mutable data, each thread that reads or writes the data must obtain a lock Do not let the guarantee of atomic reads and writes deter you from performing proper synchronization Without synchronization, there is no guarantee as to which, if any, of a thread's changes will be observed by another thread Liveness and safety failures can result from unsynchronized data access Such failures will be extremely difficult to reproduce They may be timing dependent and will be highly dependent on the details of the JVM implementation and the hardware on which it is running The use of the volatile modifier constitutes a viable alternative to ordinary synchronization under certain circumstances, but this is an advanced technique Furthermore, the extent of its applicability will not be known until the ongoing work on the memory model is complete

Cavities are no exception. A real cavity is always dissipative. In this chapter we consider this dissipation from a fundamental perspective and address some key conceptual questions related to it. For concreteness and simplicity, we neglect absorption at the cavity walls and consider the leakage of electromagnetic radiation out of the cavity as the only source of dissipation. In that case, a first approximation to the problem is to quantize the field inside the cavity and outside as if the cavity is perfect (Le., completely closed by perfectly reflecting walls) and then deal with the transmissivity losses by including an ad hoc coupling term in the Hamiltonian of the total system. This coupling term annihilates a photon in one of the discrete cavity modes and creates another in one of the outside continuum of modes. It should also do the reverse2 (otherwise, it will not be Hermitian). To make it even simpler, we can assume that the coupling strength V with which a cavity mode couples to the outside is a constant (Le., the same for all cavity mode~xtemal mode pairs). The Hamiltonian is then given by

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4

tually any physical system for which he could write down Hamilton's equations just by replacing the Poisson brackets by commutators multiplied by a certain constant. Here is how the analogy between Poisson brackets and commutators comes about. 5 The Poisson bracket of any two dynamical variables, U and v, in classical mechanics is defined by (2.1) where qn and Pn are any set of canonical coordinates and momenta that describe the system. In terms of Poisson brackets, the classical equation of motion of any dynamical variable 7} is given simply by

To implement a Print Preview feature: 1 Ensure that there is a way for the user to select a Print Preview This is most logically de ned near the Print option 2 Add the PrintPreviewDialog control to the form from which the user initiates the Print Preview process This is normally the same form containing the PrintDocument control Give the PrintPreviewDialog control a logical name, such as PTPrintPreview 3 In the event handler for the control that initiates the Print Preview, write the code required to display the Print Preview dialog The code requires two simple steps: associate the appropriate PrintDocument control with the Print Preview dialog and then show the dialog as follows:

i] =

(7},

PTPrintPreviewDocument = PTPrintDocument PTPrintPreviewShowDialog()

(2.2)

where H is the Hamiltonian. From (2.1) it follows that Poisson brackets satisfy the identity (U, (v, w)) + (v, (w, u)) + (w, (u, v)) = 0 (2.3) and have the following properties:

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