Dielectric resonator antenna

Details Dielectric resonator antenna Dielectric resonator antenna

1999-08-06

2001-11-27

Wong, Don (Department: 2821)

Communications: radio wave antennas

Antennas

With grounding structure

C343S785000, C343S789000, C343S873000

Reexamination Certificate

active

06323824

ABSTRACT:

FIELD OF THE INVENTION
The invention relates to a dielectric resonator antenna (DRA) having an electrically conducting layer in a plane of symmetry.
Furthermore, the invention relates to a transmitter and a receiver having a dielectric resonator antenna with an electrically conducting layer in a plane of symmetry and also to a mobile radiotelephone with such an antenna.
BACKGROUND OF THE INVENTION
Dielectric resonator antennas (DRA) are known as miniaturized antennas of ceramics or another dielectric medium for microwave frequencies. In a dielectric resonator whose dielectric medium ∈
r
>>1 is surrounded by air, this dielectric medium has a discrete spectrum of self-frequencies and self-modes. Contrary to a resonator, which has a very high quality when radiation losses are avoided, the radiation of power is in the forefront in the resonator antenna. Since no conducting structures are used as a radiating element, the skin effect can have no detrimental consequences. Therefore, such antennas have low-ohmic losses at high frequencies. When materials having a high dielectric constant are used, furthermore a compact, miniaturized structure may be achieved.
FIG. 1
shows such a DR antenna
1
in the basic form regarded as an example. In addition to the form of a parallelepiped, also other forms are possible, such as for example, cylindrical or spherical geometries. Dielectric resonator antennas are resonant elements which operate only in a narrow band around one of the their resonant frequencies. The problem of the miniaturization of an antenna is equivalent to lowering the operating frequency with given antenna dimensions. As a result, the lowest resonance (TE
z
111
-mode) is used. This mode has a plane, which is called plane of symmetry
2
, in which the tangential component of the electric field disappears. When the antenna is halved in the plane of symmetry
2
and an electrically conducting surface
3
is deposited (for example, a metal plate), the resonant frequency continues to be equal to the resonant frequency of an antenna having the original dimensions. This is represented in
FIG. 2. A
further miniaturization with this antenna can be achieved by means of a dielectric medium having a high dielectric constant ∈
r
. For this purpose, preferably a material having minor dielectric losses is chosen.
Such a dielectric resonator antenna is described in the article “Dielectric Resonator Antennas—A review and general design relations for resonant frequency and bandwidth”, Rajesh K. Mongia and Prakash Barthia, Intern. Journal of Microwave and Millimeter-Wave Computer-aided Engineering, vol. 4, no. 3, 1994, pp. 230-247. The article gives an overview of the modes and radiation characteristic for various shapes, such as cylindrical, spherical and rectangular DRAs. For different shapes the possible modes and planes of symmetry are shown (see FIGS. 4, 5, 6 and page 240, left column, lines 1-21). Particularly a parallelepiped-shaped dielectric resonator antenna is described in the FIG. 9 and the associated description. By means of a metal surface in the x-z plane with y=0, or in the y-z plane with x=0, the original structure may be halved without modifying the field distribution or other resonance characteristics for the TE
z
111
-mode (page 244, right column, lines 1-7). The DRA is excited via a microwave transmission line in that it is inserted into the stray field in the neighborhood of a microwave line (for example, a microstrip line or the end of a coaxial line).
With this type of coupling of the power, the impedance matching of the dielectric resonator antenna with the transmission line, necessary for a good efficiency, is hard, because the matching strongly depends on the position of the antenna relative to the transmission line. The deviation of the relative position of the transmission line, however, strongly varies especially in the case of automatic production.
SUMMARY OF THE INVENTION
It is an object of the invention to provide a better coupling of the dielectric resonator antenna to a transmission line.
The object is achieved in that in the plane of symmetry at least one electrical contact, insulated from the electrically conducting layer, is provided and in that the electric layer and the electrical contact are used for connecting the dielectric resonator antenna to at least one transmission line for a signal to be transmitted or received. In this manner, two electrical contacts evolve that are fixedly connected to the dielectric resonator antenna, which contacts may be connected to the DRA for coupling the power. An antenna according to the invention may be mounted with other components onto a printed circuit board (PCB) in the known SMD technique (soldering onto the surface of the printed circuit board). This DRA allowing of SME may be fixedly soldered with the transmission lines onto the printed circuit board, so that a distinctly better coupling is achieved than when a transmission line is inserted into the leakage field. The impedance matching depends considerably less on the exact positioning of the antenna on the printed circuit board, than when inserted into the leakage field, for which case the matching strongly depends on the distance from the antenna to the transmission line.
In an advantageous embodiment, a metallic layer is provided for forming the electrically conducting layer in the plane of symmetry and for forming the electrical contact. Based on their good manufacturing properties and electrical conductivity, metallic layers are highly suitable for realizing the connection to a transmission line.
In a further embodiment, a metallic layer is provided on a side of the DRA adjacent the plane of symmetry for connection to the electrical contact in the plane of symmetry. In this manner, the extension by the metallic layer achieves a very good excitation of the dielectric resonator antenna. For example, with a parallelepiped-shaped antenna and the plane of symmetry as a base, the electrical contact may be arranged on an adjacent head-end. The metallic layer is then continued over the edge to the base, so that a soldering point develops in the plane of symmetry, which point may be used for the surface mounting. This soldering point is naturally insulated from the electrically conducting layer, which is preferably done by skipping a small area when the plane of symmetry is metallized. Preferably, a silver paste is used for forming the metallic layer by burning into the material of the DRA.
In a preferred further embodiment, a ceramic of (Ba,Nd,Gd)TiO
3
is provided as a material for the dielectric resonator antenna. This ceramic material has all the important properties for the dielectric resonator antenna such as a high dielectric constant, a low dielectric losses and a low dielectric temperature coefficient.
Further advantageous embodiments are contained in the further claims.
Besides, the object of the invention is further achieved by a transmitter and a receiver and a mobile radiotelephone in which in the plane of symmetry of the antenna at least one electrical contact is provided insulated from the electrically conducting layer and the electrical layer and the electrical contact are provided for connecting the dielectric resonator antenna to at least one transmission line for a signal to be transmitted or received.
These and other aspects of the invention are apparent from and will be elucidated with reference to the embodiments described hereinafter.


REFERENCES:
patent: 5453754 (1995-09-01), Fray
patent: 5581262 (1996-12-01), Kawahata et al.
patent: 5923305 (1999-07-01), Sadler et al.
patent: 5940036 (1999-08-01), Oliver et al.
patent: 5952972 (1999-09-01), Ittipiboon et al.
patent: 6052087 (2000-04-01), Ishikawa et al.
patent: 3509014 (1986-09-01), None
patent: 0790663A1 (1997-08-01), None
patent: 0767510A1 (1997-04-01), None
By Rajesh K. Mongia & Prakash Barthis, “Dielectric Resonator Antennas—A Review and General Design Relations for Resonant Frequency and Bandwith”, Intern. Journal of Microwave and Millimeter-Wave Compu

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