Mobile communication systems support multiband/multimode operation, which requires several bandpass filters and which becomes inevitably bulky with conventional cavity type resonators. The base station as well as the remote radio head now requires compact multiband bandpass filters with high performance. This high performance and compactness of the bandpass filters can be accomplished by replacing conventional cavity resonators with ceramic resonators, which have been widely used in satellite communication systems. This paper examines the use of these ceramic resonators in mobile communication systems.
The conventional dielectric resonator used for satellite transponders is a dielectric disk in which the two resonant modes are degenerate. A bandpass filter made with this resonator has good stability against temperature variations and has been applied to many satellite communication systems [1-3]. In 1997, a triple-mode dielectric rod resonator was proposed to reduce the size of the bandpass filter . Since this resonator has triple modes, a 3-pole bandpass filter can be designed by one triple-mode resonator. Using two triplemode resonators, a 6-pole elliptic function bandpass filter was successfully demonstrated for a satellite transponder in .
The ceramic resonators analyzed in this paper are dielectric spheres and rods in which triple modes exist. The resonant characteristics are essential to the design of bandpass filter. The electromagnetic fields in these resonators are well known ; therefore, only their resonant characteristics, including the tuning method, will be discussed.
Triple modes can also be supported in a dielectric cube. However, because of the Q values, two types-sphere and rod-will be discussed. The dielectric resonator must be placed inside the metallic housing or cavity; therefore, the dimensions of the metallic cavities and mounts for the dielectric sphere and rod are determined in such a way that they do not affect the resonant characteristics of dielectric resonators very much.
As illustrated in Fig. 1, a spherical dielectric resonator with radius
We can introduce the circumferential chamfering of the sphere as shown in Fig. 3, so that the resonant frequency of the TE01δZ mode is shifted upward, while that of the other two modes are not affected. The sphere surface along the z-axis is chamfered, so the radius is reduced from
εras = 9, aas = 13 mm, bas = 20 mm, tas = 5 mm.
The corresponding resonant frequencies are
The cylindrical dielectric rod shown in Fig. 5 can also support triple resonant modes. However, in this structure, only two TE01δX mode and TE01δY mode are degenerate. The third mode, TE01δZ mode, which has a very similar electric field distribution along the cross section, has different resonant frequencies depending on the length
Resonant frequency (MHz) variations as a function of rod length H
The dielectric sphere, as well as the dielectric rod, was fabricated in the metal housing as shown in Fig. 7. The calculated Q values of the resonant dielectric sphere lie between 27,000 and 29,000, depending on the modes, while those of dielectric rod resonator are between 24,000 and 27,000. The quality factors, Q, were measured as in . The measured resonant frequencies and their behaviors are not much different from the simulated results. Measured Q values of the dielectric sphere are over 27,000 depending on the input/ output coupling structures within the metal housing. Chamfering the sides of the sphere permits easy separation of the resonant frequencies of TE01δX and TE01δZ modes. The measured resonant frequencies, including the cross coupling in the dielectric rod resonator, are 855.19MHz (TE01δX mode), 855.24MHz (TE01δy mode), and 855.86MHz (TE01δz mode); the inhomogeneity of the dielectric can introduce a small discrepancy from the simulated results. However, separation of the resonant frequency of degenerate mode TE01δX and TE01δY modes for 3-pole bandpass filter applications requires other decoupling schemes. The internal cross coupling can create the transmission zero. For the dielectric rod, the Q values are over 24,000 when it is evaluated from the measured results shown in Fig. 8. The dimension of the dielectric rod for the simulation is given in Fig. 9, where the three modes are separated as in Fig. 8. The resonant frequency of the TE01δZ mode in the dielectric rod can be moved upward by adjusting its length along the z-direction compared to its diameter. As is the case for the sphere, separation of the resonant frequency of TE01δX mode and TE01δY mode needs other decoupling structures because the separation of the resonant frequency of the degenerate mode is not sufficiently large for the design of a bandpass filter. We obtained very similar behavior in the frequency response for the dielectric sphere as discussed in the simulated results.
Novel triple-mode high-Q spherical dielectric loaded cavity resonators are analyzed for application to bandpass filters for mobile communication systems. Two types of dielectric resonators-spheres and rods-are analyzed and simulated in order to obtain their resonant characteristics. The frequency responses of the two types of resonators behave in the similar way when the resonant frequencies of triple modes are concerned. We also studied the change in the resonant frequencies as a function of the structural parameters of the resonators so that we can use them in the design of bandpass filters.