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The border of the current (active) window The caption text of the current (active) window The background color of a multiple-document interface (usually the background color of a document window) The background color (not image) of the desktop The face of button elements The dark shadow area on the edge of 3D button elements The shadow area on the edge of 3D button elements The text of button elements The text in captions, size boxes, and scrollbar arrow boxes Gray (disabled) text Selected item(s) The selected text The border of an inactive window The caption of an inactive window The caption text of an inactive window The background for tooltips The text of tooltips The background of menus The text of menus The gray area of scrollbars The dark shadow for 3D elements The face of 3D elements The highlight color for 3D elements The light color shadow for 3D elements The dark color shadow for 3D elements The window background (for nondocument windows) The window frame The text in windows



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Usually the bulk of text on any Web page is composed of paragraphs. Paragraphs in HTML are denoted by the <p> and </p> pair of tags. When your Web page is processed, the browser formats everything between those two tags as one paragraph and renders it to fit the user s screen, word wrapping as needed at the margins. Any additional line breaks and unnecessary whitespace (beyond one space between words and between sentences) in the HTML code are ignored.





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In other words, the indeterminate a acts like the number This is a result of the fact that multiplication is computed modulo the polynomial g(a) = a2 1: the symbol a is (now by construction) a root of the polynomial g ( x ) . To put it another way, the remainder of a polynomial a2 1 divided by a2 1 is exactly 0. So, by this procedure, any time a2 1 appears in any computation, it may be replaced with 0. Let us take another look at the polynomial multiplication in (5.30):

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In the processes that we wish t o discuss it is no longer adequate t o employ theories that treat quantum-mechanical particles interacting with classical fields In addition, because of processes such as vacuum polarization a singleparticle theory loses its relevance: the quantum fluctuations of the fields create virtual particle-hole pairs and generate an inherently many-body system To remedy the first problem we must consider quantization of classical fields such as the electromagnetic field In the case of the Maxwell (electromagnetic) field the quantization procedure leads to the fruitful picture of a vector quantal field and a massless field particle, the photon Such a theory is extremely well suited t o the description of processes in which photons are emitted or absorbed, because it employs field operators that create or destroy photons.

Sometimes two or more rules can affect the same hypothesis. How would an expert system propagate certainty factors when this occurred Suppose, for example, that we are given the following three rules, which all affect the hypothesis H:

In the case of other fermions and bosons we know how t o find quantum mechanical descriptions both nonrelativistically (Schriidinger equation) and in a Lorentz covariant formulation (Dirac or Klein-Gordon equations) For these cases, however, it turns out to be highly advantageous to quantize the wave equation as if it were a classical field This procedure is called second quantization, the first quantization corresponding to the introduction of the wave equation with appropriate boundary conditions, the second corresponding to quantization of the field that would result from interpreting the wave equation as a classical field equation It is easily demonstrated in second quantization of the Schodinger equation that the second quantization adds no new physics-the first- and secondquantized theories have equivalent physical content.

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However, for particular applications such as many-body theory a second-quantized formalism with creation and annihilation operators automatically satisfying the appropriate quantum statistics is far easier to use than a first-quantized theory A similar situation prevails in the domain of relativistic wave mechanics By analogy with the Maxwell case, the second quantization of the Dirac or Klein-Gordon equations leads to a picture of fields that create and destroy particles (the quanta of the fields), with the interactions in physical systems resulting from the field couplings As we shall see, this is a far more natural.

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