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power to the hard disk and the case front fan and controls We also coiled up the 12" SATA interface cable (again, we got one each with the drive and the motherboard, both a bit too long for the local layout) to keep things neat None of the cables proved difficult to route, and only one access issue popped up, one that was easily resolved The Fan 3 pin block sits immediately to one side of the secondary IDE connector on the motherboard By the time we realized we had to insert one of the case fan connectors into that block, we d already seated the IDE cable But the pull tab on that particular cable made it easy to remove, which we did to make room for our fingers to steer that fan connector into position After that, we replaced the IDE connector without incident.

In this self-starting geometry demonstrated at 514 nm with CW illumination, the twopump beams were derived from the incident beam itself using beam-fanning and total internal re ection on the crystal faces In the following sections, this geometry is called internal loop geometry In 1984, various self-pumped phase conjugate mirrors were proposed, modeled, and experimentally tested [2] Among them, the linear phase conjugate mirror requires two additional mirrors that form a linear resonator providing the two counterpropagating pump beams [2] This phase conjugate mirror, along with its semilinear version (only one additional mirror), has been used in laser cavities as end mirrors [6] One major drawback of this geometry is that coherence length is required to provide ef cient phase conjugation In the case of a Q-switched Nd:YAG laser, it is about 1 cm.

We also had to route the PSU fan cable all the way over to the other side of the motherboard to plug it into the Fan 2 pin block (which also took a while to find, as we scanned the motherboard s pin-out diagram) But because Seasonic s cable was more than long enough to reach, this was no big deal Clear labeling on case cable headers made installing them a snap We didn t even have to consult a manual for the interface connections, only for the on/off and reset buttons Our final power-on test produced a healthy POST, so we were done with the initial build at this point.

Other than the round IDE cable we used to connect the optical drive to the motherboard, we didn t have to buy any additional cables or other items for this build, nor did it require any special tools (or cause us to break much of a sweat, either)..

This is why linear phase conjugate mirrors are not used for the application discussed in this chapter The ring phase conjugate mirror [2] uses two additional mirrors, which form a loop and feed the transmitted beam back to the photorefractive crystal These two geometries (internal loop and ring) are often used for the improvement of laser sources such as laser diode injection and spectral narrowing [8] or self-corrected oscillators [34] These two kinds of self-pumped phase conjugate mirrors with BaTiO3:Rh are also currently developed for the application to dynamic wavefront correction of nanosecond Nd:YAG lasers at 106 mm [35, 36] They are discussed in the following sections..

bandwidth obtained is 74 MHz (2426 2500 MHz), or about 3.0% referenced to the center frequency at 2463 MHz. The obtained impedance bandwidth of the higher operating band is close to the bandwidth requirement of the ISM band at 2.45 GHz. Radiation patterns at the center frequency of the lower and upper operating bands were also measured. Results are presented in Figure 3.3. Large cross-polarization is

C r = - -3 =

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Note: LOQ is expressed as concentration or amount of analyte, which is derived from measured signal Lowest signal: xL = xbl + 10sbl Lowest concentration/ amount: LOQ = qL(cL) = xL/S = 10sbl/S Note: a signal of 10 times SDblanco corresponds to % RSD of 10%

The Layers and Properties toolbars make it easy to tell an object s layer, linetype, and color. Remember that when you select an object, its layer, linetype, lineweight, color, and plot style appear in these toolbars.

The Poisson distribution Suppose that p ( w ;0) is the parametric family of Poisson probability functions (3.42). This expression is equivalent to (3.84) Thus, this family of Poisson probability functions parametric in 0 is exponential with