Scattering parameters of microstrip ring resonators with ) and without slits that are either edge or side coupled to the feedlines are simulated by the FDTD method. The strip conductors on the de¨ice can either be infinitely thin or finite in thickness. The simulations predict the occurrence of reso
Modeling of nonlinear optical media with the TLM-based finite-difference–time-domain method
✍ Scribed by Zhizhang Chen; Jian Xu; Jun-Ming Chuang
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 488 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
✦ Synopsis
setup. T h e use of YBa,Cu,O, thin film does not change the antenna design and resonance frequency when compared to a normal metal. At 80 K, the improvement of efficiency was 1.2 d B over a silver counterpart working at the same temperature. This result may be even better at lower temperatures that a r e now easily obtainable with Stirling closed circuit cryogenerators well adapted to this purpose. T h e improvement of the superconducting antenna is essentially because the reduction of ohmic losses in the feeding line. In order to decrease the losses still more, we try t o reduce the surface resistance by an accurate control of the amount of intergrain weak links (e.g., high angle grain boundaries in the case of YBa,Cu,O, films grown on (100) MgO [lo]). A t present, we are working on an antenna array composed of several patches. As the ohmic losses increase rapidly with the length of the feeding lines, we hope that the use of a superconducting distribution network increases the efficiency substantially.
📜 SIMILAR VOLUMES
Two different types of source excitation for finite-difference ( ) time-domain FDTD simulations, i.e., electric and magnetic field types, are in¨estigated in this work for configurations that ha¨e no ground planes. This paper shows that the electric field excitation introduces errors in the computed
and is divided into five uniform segments. For the explicit scheme, the time sample was chosen as 0.053 LM. The Ž . current at the location 0.0; y0.1 is shown in Figure 4. Again, the agreement is good, and it is seen that for the implicit scheme, one can make ⌬ t large and violate the Courant stabil