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57) splits the continuum of external modes into a collection of smaller reservoirs, each having a finite frequency width and coupled to a single-cavity mode Their independency arises from the smallness of the overlap of a given cavity mode with neighboring cavity resonances in the high-Q regime (see Figure 93) Grangier and Poizat [247, 248] have shown that the breakdown of the independent reservoir assumption is essential for the appearance of excess quantum noise in lasers This is a curious phenomenon first found in gain-guided semiconductor lasers by Petermann [491], where a laser has a linewidth larger than the usual SchawlowTownes Iinewidth, as if there were more than one spontaneous emission noise photon per mode Later, Siegman developed a semiclassical theory [561, 562], where excess noise emerges as a consequence of mode nonorthogonality.

10. If you now owe the customer money, click Check Refund to create a refund check. To view your credit memo, choose Activities Create Credit Memos/Refunds. A Create Credit Memos/Refunds screen appears, as shown in Figure 16-9.

Siegman showed that for those lasers the perfect cavity mode expansion of the radiation field breaks down and one must use instead the actual modes of the open laser cavity, which are nonorthogonaL Thus, the breakdown of the Gardiner-Collett Hamiltonian, the need to adopt the.

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Com pared to Boston and San Francisco, Research Triangle Park has an advantage of relatively low land and construction costs, and more afford able labor, given the relatively low cost of living On the West coast, the San Francisco bay area is an intellectual center with three world-class universities the University of California, Berkley; the University of California, San Francisco; and Stanford University fueling biotech innovation Many of the rst biotech companies in the United States emerged in the Bay area in early 1980s, including Genetech, Chiron, and Cetus In addition to the three-decade history of biotech and the ready availability of highly skilled scientists, the San Francisco area bene ts from a permissive regulatory infrastructure For example, Stanford University announced the formation of an institute to study stem cells and human cloning in 2002, despite national pressure against the exploration or use of the technologies.

12Notice that unlike the constant coupling strength advocated by Barnett and Radmore [37] and Gardiner and Collett [225], among others, the frequency-dependent Vn(k) given by (9.57) does not make the phase shift integral in the Fano diagonalization method diverge. Moreover, (9.57) is practically flat (constant) within the cavity resonance peaks but falls off between peaks.

If you process a refund or return but do not issue an immediate refund check to the customer, the customer s account will contain a credit. This credit just sits there until you tell QuickBooks what to do with it. One of the most common ways to spend a customer credit is to apply it to one of the customer s other outstanding invoices. To do this, follow these steps: 1. Choose Customers Receive Payments. The Receive Payments screen appears. 2. Select the customer and job from the Received From list. 3. Click Discounts & Credits, and then the Credits tab. A summary of all applied and unapplied credits for the customer appears as shown in Figure 16-11.

natural cavity modes rather than perfect cavity modes, and the emergence of excess noise in lasers are all connected.

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Figure 16-11: QuickBooks tracks all applied and unapplied credits and allows you to apply them to outstanding customer invoices at the appropriate time.

The informal culture, in which established companies be come incubators for new companies, is credited with the rate of innovation in the area, as measured by the number of biotech patents awarded..

Figure 9.3 Here we show the coupling strength Vn (k) in relation to the cavity resonances. The thin line is a plot of 1 (k)12; the peaks show the cavity resonances corresponding to k o, kl, and k2. The thick dotted line is a plot of sin2 ([k - kIJL)j(k - kI)2 properly scaled to appear in the figure. Notice how VI (k) is practically flat inside the n = 1-mode Iinewidth and falls off as it approaches the next modes. We have used an energy reflectivity Irl2 of 96% (i.e., = 0.2).

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