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So what, if anything, are finalizers good for There are two legitimate uses One is to act as a safety net in case the owner of an object forgets to call the explicit termination method that you provided per the advice in the previous paragraph While there's no guarantee that the finalizer will get invoked promptly, it's better to free the critical resource late than never, in those (hopefully rare) cases when the client fails to hold up its end of the bargain by calling the explicit termination method The three classes mentioned as examples of the explicit

" It was Paul Dirac (who had a first degree in electrical engineering and was an admirer of Heaviside's writings) who took the idea of magnetic monopoles seriously and showed in 1931 [157] that the existence of a single magnetic monopole would explain the quantization of charge (see 4 of Jackson's book [314] and [545]) The existence of magnetic monopoles has been inferred theoretically by 't Hooft [598] and Polyakov [494], but their predicted energies have so far proved to be too high for experimental confirmation (see eg, [1]) Recently, Zhong Fang and collaborators [188] have found experimental evidence for effective monopoles at much lower energies in the ground state of crystals (see also [421]) But these are only effective monopoles that have no meaning outside such ground states.

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4 De ne the appropriate information to log into the selected database server 5 Select the database name The databases in the selected database server instance are listed in the drop-down The resulting dialog appears similar to Figure 84

For an extensive list of references on magnetic monopoles, see the resource letter published in the American Journal of Physics [239] Kobe [364] also uses the Sttickelberg-Wheeler-Feynman idea to solve the negative-energy-photon problem and interpret the antiphoton However, he does not do a parity transformation He considers antiphotons to be negativeenergy states which go backward in time rather than in space-time As a result, his antiphotons turn out to be photons of the opposite helicity The American Journal of Physics has published some excellent pedagogical papers on light polarization and the spin of the photon You might wish to have a look specially at [46] and [277] Recently, the de Broglie wavelength of a two-photon wave packet has been measured [219].

Ole Keller holds the view that the question of the localizability of the photon cannot be separated from that of how a photon is born, say, out of an atom or molecule So he considers the interaction with matter and near-fields explicitly See, for instance, [342-350] Chan et al [98, 99] have recently followed a similar idea in which they dealt explicitly with the entanglement between the atom and the emitted photon using a Schmidt decomposition (for a pedagogical account of the use of the Schmidt decomposition for dealing with entangled systems, see [185}) But notice that their use of the dipole approximation in.

Figure 84 The Add Connection dialog allows you to de ne a connection to a database and then test that connection

the analysis in principle rules out the possibility of investigating localization of the photon to a region smaller than the typical size of an atom. Jauch and Piron [322] dropped Newton's and Wigner's [464] assumption that position measurements should be compatible (commute) with one another and obtained a position operator for the photon. Since then, this idea of dropping the commonsense ideas adopted in [464] of what a position measurement is and what localized states are has lead to a cottage industry of papers on alternative photon position operators. See, for example, [278-280]. For a review of Proca equations and the experimental search for an upper limit to the photon's mass, see [238,367]. See also Sec. 12.9 of Jackson's book [314] and the paper by Bass and SchrOdinger [44]. Crandall wrote a nice pedagogical paper in the American Journal of Physics [128] describing an undergraduate experiment to put an upper limit on the photon's mass. Those curious about quaternions should read Appendix C (they are used actively nowadays in computer animation, robotics, and in field theory). The following references should also be quite readable for the average physicist: [2, 67, 95, 96, 146, 179, 180,244,256,257,263,264,266,291], 9 of[386], and [506,566,567,588]. For a discussion on the localization of relativistic particles in the context of the consistent histories interpretation of quantum mechanics, see [471J. The consistent histories approach has been used to resolve [254] some apparent paradoxes related to localization of relativistic particles [286-288]. See also von Zuben's analysis of these paradoxes [621].

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