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under the symmetry operation. But, since the system can actually exist in only one of these states, the symmetry appears to be broken. This phenomenon, that the ground state of the system does not possess the symmetry of the Hamiltonian, is called "spontaneous symmetry breaking." We have encountered the simplest manifestation of spontaneous symmetry breaking in the two-dimensional Ising model. The total energy is invariant under a simultaneous sign change of all the spins. Yet, the lowest-energy configuration is that in which all spins are aligned. In this case the symmetry is expressed through the fact that the spins could also have aligned themselves along the opposite direction. A more subtle example is the nonvanishing of the superfluid order parameter, as discussed in 12. When a continuous symmetry is spontaneously broken in a quantum mechanical system, interesting consequences follow. In this case, there is a noncountable infinity of ground states (with energy taken to be zero) orthogonal to one another. The system must choose one of these. As a consequence of the degeneracy, there emerges a type of excited state in which the local ground state changes very gradually over space, so as to form a "wave" of very long wavelength. Such a state is orthogonal to anyone ground state, with an energy approaching zero when the wavelength approaches infinity. This is called a "Goldstone excitation." The underlying symmetry is said to be realized in the "Goldstone mode." Familiar examples of Goldstone excitations include phonons in a crystal lattice, which expresses the broken translational invariance, and spin waves in a ferromagnetic, which realizes the basic rotational invariance. A new twist occurs when the system is coupled to a zero-mass vector field such as the photon field. In this case the Goldstone mode gives way to the" Higgs

aFor a discussion of broken symmetry in condensed matter physics, see P. W. Anderson, Basic Notions of Condensed Matter Physics (Benjamin-Cummings, Menlo Park, CA, 1984), 2. For its role in particle physics, see K. Huang, Quarks, Leptons, and Gauge Fields (Wodd Scientific, Singapore, 1982), s 3,4. bWeinberg-Salam model of unified electro-weak interactions. cQuantum chromodynamics with massless quarks.

The deployer role focuses on configuring and installing an application assembled by the assembler onto an application server This typically involves resolving external dependencies, configuring resources required by the application such as databases and mail services, configuring the application for transactions and security, and so on, and deploying the application to the app server

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mode," wherein the "photon" acquires a mass dynamically, and the would-be Goldstone excitation becomes the longitudinal degree of freedom of the massive "photon." An example of this is the Meissner effect in superconductivity, in which the photon mass corresponds to the inverse penetration depth. We offer a list of broken symmetry phenomena in condensed matter physics and particle physics in Table 16.5. In defining spontaneously broken symmetry, we have assumed that a system can exist in only one ground state, even if it possesses many equivalent ones. This is obvious in classical mechanics, but not in quantum mechanics. In the latter case one can legitimately ask, "Why can't the system exist in a linear combination of different ground states " The answer is that, to make a transition from one ground state to another. one needs an operator that simultaneously changes the states of all the particles in the system. Such an operator does not exist in the thermodynamic limit, when the number of particles tends to infinity. In this limit, therefore, the different ground states generate separate Hilbert spaces, and transitions among them are forbidden. One says that there is a "super selection rule" insulating the ground states from one another. If a superposition is made of two different ground states, then no physical measurement can determine the relative phase of the two states; one would have two separate systems that can never communicate with each other. Thus, such a superposition does not correspond to any experimental situation.

If you want to display a larger full-screen map, click the Big Map button at the top right of the map.

(11.131)

where v'(N)

Assembly can be carried out manually or with the help of assembly and deployment tools Deployment involves using a deployment tool that generates container-specific classes to enable the container to provide the required runtime services to the enterprise application

r=::---1

(-I~r~+I)

(11.132)

Sometimes you want to see the area just outside a given map but don t neces sarily want to zoom out the entire map. Instead you want to re-center the map. Again, there are two ways to do this. You can re-center via the point-and-clicking method by selecting the Re-Center option below the map. With this option selected, when you click a point on the map, the map will be redrawn, with your click point as the new center point. Another option is to use the North, East, South, and West controls along the sides of the map. Click the North control to pan the map north; use the East con trol to pan the map east; and so on.

Figure 15-10

kT{ v [

~ (1 + r )] -

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J2EE components utilize eXtensible Markup Language (XML)-based deployment descriptors for communication between the component developer, the application assembler, and the deployer

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