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3Naively. we could think that .;p obeys the boundary condition n 1\ (V1\.;p)ls = O. which can be derived by wrongly inverting (A.24). This inversion is achieved by taking the curl of (A.24) and using (A. 10) to yield x= (VI\.;p)/k. Then as nl\ xis = O. we would deduce that n 1\ (VI\ )ls =: O. The flaw is that (VI\.;p)/k gives only the transverse component ofX. and on the surface of the cavity (only there!) X has a nonvanishing longitudinal compclnent because of the surface charges. 4The same conclusion can be drawn simply by rewriting n . (V I\n) as (nl\ V) . n and noticing that (nl\ V) is perpendicular to n.

to the surface [i.e., from (AS)], it follows that X (V An)ls = O. Using this result in (A34), we conclude that n <t>1 s = 0, so that <t> satisfies the correct boundary condition for the magnetic field. We can now get back to the comparison with Fourier space mentioned at the beginning of this appendix. Instead of (2.46), we have for the cavity fields

Private Sub SaveToolStripMenuItem_Click(ByVal sender As Object, _ ByVal e As SystemEventArgs) _ Handles SaveToolStripMenuItemClick, SaveToolStripButtonClick DirectCast(MeActiveMdiChild, IMDIChild)ProcessSave() End Sub

Effective Java: Programming Language Guide valueOf Returns an instance that has, loosely speaking, the same value as its parameters Static factory methods with this name are effectively type-conversion operators getInstance Returns an instance that is described by its parameters but cannot be said to have the same value In the case of singletons, it returns the sole instance This name is common in provider frameworks

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Thus, (2.91)

This code handles both the Save menu option and the Save toolbar button It calls the ProcessSave method on the active MDI child form if the active MDI child form implements the IMDIChild interface Because it is possible that the active MDI child form does not implement the interface, use a TryCast here to make the code more solid:

y(x, t}

+ 1/2] n1r/ L) sin (fiIvt) sin (fiI [x + ~]) .

Private Sub SaveToolStripMenuItem_Click(ByVal sender As Object, _ ByVal e As SystemEventArgs) _ Handles SaveToolStripMenuItemClick, SaveToolStripButtonClick Dim frmMDIChild As IMDIChild frmMDIChild = TryCast(MeActiveMdiChild, IMDIChild) If frmMDIChild Is Nothing Then MessageBoxShow("You must open a window that supports " _ & " a save before you can save an entry") Else frmMDIChildProcessSave() End If End Sub

You should note that as -L/2 < Xo < L/2, the sine in the denominator of (2.91) never vanishes. Also notice that even though the general solution (2.85) is not necessarily separable, (2.91) is [i.e., (2.91) separates into a spatially dependent factor sin([1r / L]fi[x + L/2]} and a time-dependent factor sin([1r / L]fivt}]. The spatially dependent factor is what we call the mode. So our one-dimensional resonator produces the spatial field pattern (i.e., mode) sin([1r/L]fi[x + L/2]} when its fith resonance Wii = (1r / L }fiv is excited.

The important message for us here is this. In a perfect resonator, not only is the frequency spectrum of the radiation reduced to the discrete cavity resonances, but the fields themselves must be linear combinations of the corresponding mode patterns. So the cavity modes form a complete basis in terms of which any intracavity radiation field can be expanded.

4

This is the staple wine of our free tasting. We will start with field quantization in a perfect cavity because it is easier. Even though the important results of the mode calculation are summarized briefly at the beginning of Section 2.4.1, the reader might find it useful to have a look at Appendix A. After that, we are ready to tackle the free-space case in Section 2.4.2. This is just a bit more sophisticated because it involves continuum modes with lots of delta functions instead of Kronecker deltas and complex canonical variables, but the basic idea is the same of Section 2.4.1. Finally, a disclaimer. We do not talk a lot here about the photon as a particle. In this section it appears simply as the quantum of excitation of the modes of the electromagnetic radiation field. A more vivid description of the photon as a quantum particle is given in 3.

In summary, static factory methods and public constructors both have their uses, and it pays to understand their relative merits Avoid the reflex to provide constructors without first considering static factories because static factories are often more appropriate If you've weighed the two options and nothing pushes you strongly in either direction, it's probably best to provide a constructor simply because it's the norm

The key results of our mode calculation in Appendix A that we will need here are: 1. The orthonormality of the electric field modes (2.92) and of the magnetic field modes (2.93) 2. The expansion of the fields in terms of field modes

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