quencies are given by 3.02, 2.90, and 2.80 GHz, respectively. Note that the resonant frequency approaches the predicted value of 2.71 GHz as the superstrate thickness is increased. The result is expected because it has been assumed that the whole upper half-plane is filled with the superstrate mater
Use of PML boundary conditions for wireless telephone simulations
โ Scribed by Cynthia Furse; Yan Cui; Gianiuca Lazzi; Om Gandhi
- Publisher
- John Wiley and Sons
- Year
- 1997
- Tongue
- English
- Weight
- 109 KB
- Volume
- 15
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
โฆ Synopsis
Figure 5 Transmission curves T versus with p s 1.5, p s 2, and p s 2.5 for the Lagrangian formulation required input peak power is easily evaluated with this varia-ลฝ . tional approach Figure 4 . Finally, for a given input peak power, the transmission coefficient, as shown in Figure 5, does not always decrease when the XPM parameter is increased.
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