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Generally, a massive particle of integer spin J is associated with an irreducible Lorentz tensor of rank J which has 2 J 1 independent components (see Harris, 1975, $20.4; Ramond, 1981, $1.3). This is modified if the particle is massless. For example, the free photon is a massless vector particle having two, rather than three, states of polarization. We will discuss this in Ch. 2. Fermions constitute a class of objects (of half-integer spin) that transform with well-defined angular momentum properties, but that do not have a Lorentz tensor structure, and hence do not have tensor transformation properties under the Lorentz group (31.5.5). They are called spznors (or bispinors). Although the fermion operators are not Lorentz tensors, certain bilinear combinations have a tensor structure, as we will discuss in $1.5.6.

Using lines and grids for patterns is ideal because they re so easy to create. The key in both types of patterns is the size of the bounding rectangle. You use a grid to draw accurate floor plans or even for drawing perspective scenes. Line patterns are great for creating fences or any repeating linear paths.

n might be a Carmichael number, or The computation could be infeasible if the rst a for which computing a n21 (modulo N ) is not satis ed is too large.

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We can fairly easily describe the interference effects between two mutually coherent light sources in more quantitative and mathematical terms (more sources is much harder!) By mutually coherent, we mean not only that each source is a point source of well-defined frequency, but also that the oscillation of each source is locked into phase with that of the other Typically, this means that the two beams of light came from the same laser, via a system of beamsplitters and mirrors, but we can think of them as two separate sources, S, and S2, that are somehow synchronized (by atomic clocks, etc).

We can imagine that the phase of the emission from one can be adjusted at will, and that the observation point, P , can be freely moved about in space (well, 2-D space in this diagram) to change the time delays between it and either or both of the two sources Each source, Si, emits a spherical wave, which arrives at the observation point, P, after a time delay of z = r,/c This causes a phase delay of @ = ( 2 d A ) rrThe absolute phase of each wave is unobservable, because optical frequencies are so high, but the phase difference between the two waves will determine whether there is no vibration intensity observed at P, a little, or a lot.

The Spry Repeat List object allows you to apply Spry repeat attributes to four different tag options: <ol>, <ul>, <dt>, and <select>. Unlike the Spry Repeat object, the Spry Repeat List object includes an option to select the data column you want to repeat; with the <dt> and <select> tags, you have an ability to select two separate data columns.

If the amplitudes of the two waves are equal at P, and they arrive in phase, they will add together and the total intensity (defined as the average of the square of their sum) will be four times as great as the intensity of either of the waves separately If they arrive out of phase, one will be positive when the other is negative, and they will cancel out exactly, and the total intensity will be zero! This itself is odd enough.

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Consider that if there were one laser death ray headed straight at you, and another (coherent) beam coming in from the side, there supposedly would exist places where there is no total intensity, where it might be safe to stand-but if one of the beams is suddenly blocked, you get fried! The in-between cases, where the waves are not equal in amplitude and the phase difference is somewhere between 0 and n.

(2.24)

When you apply styles and fonts to merge fields, be careful to select the entire field, including the brackets (<< and >>). If you select just part of a merge field when making a style change, FileMaker Pro will ignore it.

111 General Introduction 251 1111 Aim of the 251 1112 Structure and Cells of the Cornea 251 1113 Evidence for Stem Cells in the Cornea 252 1114 Identi cation of Corneal Stem Cells 254 112 Preparation of Media and Reagents 255 1121 PBSA/GASP 255 1122 CMF-Saline G 255 1123 CMF/GASP 256 1124 Trypsin/EDTA 256 1125 DMEM/F-12/GASP 256 1126 LSC Culture Medium 256 1127 DMEM/10FB/GASP 256 1128 Modi ed Jiang Medium (MJM) for Culture of Human Stromal Stem Cells 256 1129 HBSS/2FB 257 11210 DMEM/2FB 257 11211 Keratocyte Differentiation Medium 257 11212 Chondrocyte Differentiation Medium (CDM) 257 11213 Neural Differentiation Medium (NDM) 257 11214 Corneal Endothelial Cell Medium (CECM) 257 11215.

FIGURE 2-17

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