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Because the i (the functions being solved for) are part of B, the solution is obtained iteratively [453]: 1. A set of i are initially guessed, from which Bi is computed. 2. The Fock operator is then used to solve for a new i, which is used to compute a new Bi. This process is repeated until i becomes constant. The molecular orbitals are constructed from a basis set of one-electron atomic orbitals, . The electrons can be assigned to the molecular orbitals in various ways [e.g., 1s(1) 1s(2) 2s(3) 2s(4), 1s(1) 1s(2) 2s(3) 2p(4), etc.]. The LCAO method is used to approximate i, with the molecular orbital coe cients, cij, calculated via linear variation where i is now calculated using the Fock operator. Hence, each iteration involves solving for a new

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account for distortion because of a large voltage amplitude, and, therefore, the rise of the second-harmonic component does not show up in the analysis. From what has been said, it is clear that stability may be a concern in the design of a frequency doubler. As a rst approach, small-signal stability circles at either frequencies are a useful indication of potentially dangerous terminations [20, 33]. However, a more convenient formal approach can be done by means of the nonlinear scattering functions (see 3) [43], which relate small incremental perturbations of the largesignal waves by means of a linear matrix, in a similar way as the scattering parameters relate small perturbations of a large DC bias signal ( 2). The need for the use of incremental parameters from a large-signal regime is based on the fact that a device under compression does not have the same gain properties as in small-signal conditions (Figure 6.30(a)), and that frequency conversion within the device creates paths for the signal that could induce a positive feedback across different frequencies (Figure 6.30(b)). It can be seen that critical situations can take place even when the linear parameters indicate a stable design [44]. So far, only frequency doublers have been considered with full-nonlinear analysis. For higher-order frequency multipliers (triplers, etc.), similar considerations can be made, leading to a similar design approach [26, 27, 45 47].

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Figure 6.11. SBS re ectivity of a single-mode pump beam as a function of an incident energy focused into a fused-silica glass at a repetition rate of 10 Hz.

(9.28)

On the CD-ROM The drawing used in the following exercise, ab10-g.dwg, is in the Drawings folder on the CD-ROM.

50 43 65 95 40 95

Frequency (MHz)

To add cardinality information, ER diagrams add one or more of three symbols to the lines leading in and out of entity sets. The three symbols are: ring: A ring (or circle or ellipse) means zero. line: A short line (or dash or bar) means one. crow s foot: A crow s foot (or teepee or whatever you call it) means many.

Optical Shop Testing, Third Edition Edited by Daniel Malacara Copyright # 2007 John Wiley & Sons, Inc. 219

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When the second development effort (that is, the second iteration) ensues, the developer is confident that he or she will intersect his or her effort with the first development effort because all development efforts are being driven from the data model. Each succeeding development effort builds on the preceding one. The result is that the different development efforts are done under a unifying data model. And because they are built under a single data model, the individual iterative efforts produce a cohesive and tightly orchestrated whole, as shown in Figure 3-24. When the different iterations of development are done with no unifying data model, there is much overlap of effort and much separate, disjoint development. Figure 3-25 illustrates this cacophonous result.

(b) Spectrum of (a)

Following are some key points discussed in this chapter:

f (x,)

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