The present invention discloses a passive repeater antenna with a plurality of radiation elements arranged in a first layer or plane, and also comprises a ground plane spaced apart from the radiation elements by a dielectric material.
Operators of wireless systems such as, for example, cellular telephony systems, often wish to increase the capacity of the system in certain areas. In the case of cellular telephony, the operator may wish to increase the system's capacity within certain areas of a cell.
An increase in the system's capacity in a certain area in a cell can be obtained by installing an additional base station to cover that area. Such an additional base station will usually be a so called “micro” or “pico” base station, i.e. a base station with a reduced capacity compared to an ordinary base station, intended to be used to enhance the capacity of an ordinary base station. Naturally, the same effect can also be achieved using an ordinary base station.
The easiest way of connecting such an additional base station to the next higher level in the system, usually the “ordinary” base station of the cell, is usually to use a radio link connection of the “point to point” kind. This means installing one radio link each at the additional base station and the next higher level in the system. In order to make the connection work, Line Of Sight (LOS) is needed between the two radio links. However, operators who wish to make such installations often find that the site at which the additional base station should be installed is not within line of sight (LOS) to higher levels in the system.
One solution to the problem of having two radio links which need LOS but don't have LOS is to install repeater antennas to connect the two radio links to each other. Repeater antennas on the frequency ranges used for cellular telephony, i.e. the microwave range, are usually designed using two parabolic reflectors connected by a waveguide, with the reflectors pointing in different directions.
A repeater antenna which consists of two parabolic reflectors will inherently be clumsy, and thus be difficult to find a suitable installation site for, especially in urban areas, and may also be expensive.
A known alternative repeater antenna consists of a sheet of a reflective material such as metal. In such a repeater antenna, the incident angle and the angle of reflection will be equal, which will limit the usefulness of the reflector.
As described above, there is a need for a repeater antenna which can be used in applications in the microwave range, and which will overcome the drawbacks of the known repeater antennas.
Such a repeater antenna is offered by the present invention in that it discloses a repeater antenna which comprises a plurality of radiation elements arranged in a first layer or plane.
The repeater antenna also comprises a ground plane spaced apart from the radiation elements by a dielectric material, and the radiation elements are each given such an extension and have such a distance between them that an incident electromagnetic wave will reflect from the repeater antenna at an angle that by a predetermined amount will be greater or smaller than the incident angle of the electromagnetic wave.
In a preferred embodiment, the repeater antenna is essentially plane, due to the shape of the conducting plane, the ground plane and the layer of dielectric material. In another preferred embodiment, the repeater antenna is, in addition to being essentially plane, also essentially flat, due to the shape of the conducting plane, the ground plane and the layer of dielectric material.
By means of the invention, a repeater antenna is obtained which can be installed in locations which could previously not be used by repeater antennas with a high degree of directivity and low losses. The antenna of the invention is also less expensive to produce than previous repeater antennas.
The invention will be described in more detail in the following description, with reference to the appended drawings, in which
In
Naturally, the two factors mentioned can also occur in combination, an area with a high concentration of users can be obscured by buildings or other obstacles.
As shown in
As shown in
As can also be seen in
In order to overcome this and other drawbacks in known repeater designs, the invention discloses a repeater antenna in which an incident electromagnetic wave will reflect from the repeater antenna at an angle that will differ from the incident angle, i.e. the angle of reflection will by a predetermined amount be greater or smaller than the incident angle of the electromagnetic wave.
In order to make the choice of installation site for the repeater antenna 130 of the invention as easy as possible, the repeater antenna is essentially plane, due to a number of factors which will be explained in more detail later in this text.
The word “plane” in this context refers to the fact that the thickness of the repeater antenna is significantly less than its width or breadth. Thus, the repeater antenna can be curved while still being plane in the sense that the word is used here, much as a sheet of paper or a sheet of metal can be curved while still being plane. This will further facilitate installation of the antenna, but in one embodiment, the repeater antenna can also be essentially flat, i.e. plane and not curved.
In
In the antenna 200 shown in
The distances mentioned between the radiation elements are in this case predetermined centre distances D12, D23, between radiation elements 210, 220, 230, in neighbouring rows.
As can be seen, the extension in the first direction gradually decreases in the rows from left to right in the repeater antenna, and the pattern is then repeated in a second group of rows 240, 250, 260, these rows being identical to the rows 210, 220, 230, in the first group.
The distance and difference in extensions between the elements of neighbouring rows is such that the phase of the reflected beam, and thus the reflection angle, is controlled to be given the desired difference from the incident angle. Thus, a gradual phase shift in the reflected beam is caused over the surface of the antenna, in this case from left to right, the phase shift in turn causing the reflection angle of the electromagnetic wave to differ from the incident angle of said wave.
This is also the reason that the pattern of the rows is repeated after a certain amount of rows, in this case after three rows: when the phase shift exceeds 360 degrees, or 2π when seen in radians, the pattern will start over again.
In
As can be seen in this cross sectional view, the repeater antenna comprises an electrically conducting ground plane 320 and a layer 310 of a dielectric material is arranged with a first surface facing the ground plane 320.
The radiation elements 210-260 are arranged on a second surface of the layer of dielectric material 310, said second surface facing away from the ground plane 320, so that the dielectric layer will have the function of spacing apart the ground plane 320 and the radiation elements 210-260.
Suitably, the radiation elements are created on the dielectric layer by means of etching of a layer of conducting material which is deposited on the second surface of the dielectric layer. Thus, a layer of electrically conducting material will be, created on the dielectric layer, said conducting layer being the layer of the radiation elements.
If it is desired, the repeater antenna as shown in
However, the repeater antenna can also, in addition to being essentially plane also be essentially flat, which will also be achieved due to the shape of the conducting plane, the ground plane and the layer of dielectric material.
In
As can be seen, the incident angle α1 of the electrical beam with respect to the surface of the antenna differs from the reflection angle α2 of the beam with respect to the same surface, which is exactly the desired effect. The difference between the two angles α1 and α2 can be more or less tailor-made according to the needs of the application by the tailoring the extension of the radiation elements and the distances between them.
In
The difference in angle between the two planes “M” and “B”, shown as β in
The invention can be varied in a large number of ways. For example, if the radiation elements are arranged in rows and columns as shown in
The repeater antenna can also be varied polarization-wise: rows of radiation elements which give a second polarization perpendicular to polarization of the radiation elements 210-260 can be interspersed between the rows of elements 210-260, as shown in
If it is desired to achieve the same difference between incident and reflected angle in the two polarizations, the embodiment of
The radiation elements of the two different polarizations can also be arranged with a second layer of dielectric material between them, in which case they could “cross” each other.
As an alternative, if it is desired to steer the antenna beams in detail and in more than one direction, it would be conceivable to use the antenna of
The invention is not limited to the examples of embodiments described and shown above, but may be freely varied within the scope of the appended claims. For example, although the radiation elements have been shown as elongated elements, they may be embodied in many other forms such as, for example circular, elliptical, or as rectangular patches. They may also be embodied as slits in a conducting plane, instead of as patches around which the rest of the conducting plane has been removed.
Adjacent rows of radiation elements, such as those shown in
Naturally, the repeater antenna of the invention may be used within a wide variety of applications, and is not in any way restricted to the use which is shown in the examples of embodiments shown and described above.
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/SE2005/001077 | 7/4/2005 | WO | 00 | 1/3/2008 |