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93 99 The choice of lead precursor has been found to have an effect on growth rate, particle size, and orientation of the PbS lm The growth rate was slowest with lead nitrate solution Use of lead acetate solution as a precursor increased the growth rate up to 006 nm/cycle, and its complexation with triethanolamine resulted in a growth rate of 012 nm/cycle The complexation of lead acetate had no effect on the grain size Use of a nitrate solution, on the other hand, resulted in a reduced grain size The PbS thin lms grown by SILAR were polycrystalline (ie, cubic) with different degrees of preferred orientation The most preferred orientation occurred when a complexed lead acetate solution was used as a precursor (Fig 88) According to RBS analysis, the PbS thin lm grown with the triethanolaminecomplexed lead acetate solution was stoichiometric.

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MONTE CARLO SIMULATION FOR X-RAY FLUORESCENCE SPECTROSCOPY for Z,s and fi,j are taken from Krause (Krause, 1979). In the case of Auger electron production, the trajectory is terminated; for simplicity, it is assumed that the X-ray production due to Auger and photoelectrons is negligible compared to that by direct uorescence. Alternatively, in the trajectory calculation, the photon path can be simply continued along a random direction ( i , i ). The probability of a uorescent line l originating from a shell s of atom Z can be written as: PZ sl = Z,S Z,s pZ sl Z (6.1.7)

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In addition, 6 to 8 at% of light impurities (such as H, C, N, and O) were detected10,91 99 Multilayer CdS PbS lms have been grown using different cycles for CdS and PbS The XRD patterns showed that the double-layer components were.

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where Gp and Gv are the power and voltage gains respectively. 18.2.6 Cascaded Equations of Power Gain In the system analysis for multiple RF blocks or an RF subsystem, the system power gain is contributed by the gain of individual RF blocks, which can be calculated in terms of so-called cascaded equation of power gain. . Let us derive the cascaded equation for power gain of a system containing only two blocks as shown in Figure 18.5. Gk = GT,k = Gk +1 = GT,k +1 = PL,k , PS ,k PL,k +1 , PS ,k +1 (18.46) (18.47)

117. Qi, P.; Vermesh, O.; Grecu, M.; Javey, A.; Wang, Q.; Dai, H.; Peng, S.; Cho, K. J. 2003. Toward large arrays of multiplex functionalized carbon nanotube sensors for highly sensitive and selective molecular detection. Nano Lett. 3:347 351. 118. Snow, E. S.; Perkins, F. K.; Houser, E. J.; Badescu, S. C.; Reinecke, T. L. 2005. Chemical detection with a single-walled carbon nanotube capacitor. Science 307:1942 1945.

The Pierce sketch relation is the only sketch relation that applies to a 3D out-of-plane edge or curve without projecting the edge or curve into the sketch plane. It acts as if the 3D curve is a length of thread and the sketch point is the eye of a needle where the thread pierces the needle eye. The Pierce relation is most important in the Sweep feature when it is applied in the profile sketch between endpoints, centerpoints, or sketch points and the out-of-plane guide curves. This is because the Pierce relation determines how the profile sketch will be solved when it is moved down the sweep path to create intermediate profiles. Figure 7.17 illustrates the function of the Pierce relation in a sweep with guide curves. The dark section on the left is the sweep section that is sketched. The lighter sketches to the right represent the intermediate profiles that are automatically created behind the scenes, and are used internally to create the loft.

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