The present application relates to the field of antennas, in particular to a wideband dual-polarized antenna.
In today's era of frequent use of mobile phones, the market has a huge demand for wideband dual-polarized antennas each year, so that considerable labor and material resources are invested to develop and manufacture simple wideband dual-polarized antennas to meet the market demand in the industry. During practical use, in most cases, a horizontal-plane half-power beamwidth of a dual-polarized antenna is required to be 65 degrees, and the antenna is required to not only has good cross-polar discrimination but also to be well matched with a feed line in a wider band.
Because a horizontal-plane beamwidth of a cross dipole is too wide, a radiator having a complicated structure needs to be used in order to meet the demand on reduction of the beamwidth. A patent document U.S. Pat. No. 5,940,044 describes a dual-polarized antenna having a horizontal-plane half-power beamwidth being about 65 degrees, and the antenna includes a plurality of dipole subarrays, each subarray consisting of four dipoles; two of the dipoles in each subarray are oblique and form a +45-degree angle together with a long side of a ground plate so as to form a polarized radiating element array having the +45-degree angle; and moreover, the other two dipoles form a −45-degree angle with the long side of the ground plate so as to form a polarized radiating element array having the −45-degree angle. The dipoles are arranged in this way, so that a phase center of the dipoles with the +45-degree angle and a member with the −45-degree angle can be aligned with a vertical line parallel to the long side of the ground plate. A few years ago, in the industry, the size of the radiating elements was reduced by a technology optimizing design in which arms of dipoles were bent towards a phase center. Nowadays, most base station antenna arrays employ the radiating element structure.
A modernized multi-input multi-output antenna array includes at least two rows of adjacent radiators. As a result of such a structure configuration, a reflective plate is larger in size, and the wind load is increased accordingly. Therefore, in order to reduce the size of the reflective plate while achieving a structure in which radiators are adjacent to each other, it is necessary to employ a dual-polarized radiating element having a 65-degree horizontal-plane beamwidth and good cross-polar discrimination.
A patent document CN108172978A describes a dual-polarized antenna which has the solution that the dual-polarized antenna includes four dipoles, wherein additional conductive members are arranged on arms of the dipoles, as shown in
An objective of the present application is to provide a wideband dual-polarized antenna with an improved structure for the problems that a beamwidth cannot reach expectations easily and a cross polarization ratio is low in dual-polarized antennas in the prior art.
To achieve the above objective, the present application employs the following technical solution.
The present application discloses a wideband dual-polarized antenna, including a reflective plate and a radiating element mounted on the reflective plate. The radiating element includes four dipoles which are combined to be arranged on the reflective plate; two arms of each dipole are respectively connected to top ends of two conductors, and bottom ends of the conductors are connected to a common base and are placed on the reflective plate; a focusing member with a conical structure is mounted above the radiating element, and includes conductive members and dielectric members; and the conductive members are arranged on the dielectric members in an axisymmetrical manner, are supported by the dielectric members and are arranged above the dipoles.
It should be noted that the wideband dual-polarized antenna of the present application is able to effectively adjust the beamwidth to a desired range by arranging the focusing member with the conical structure above the radiating element, and a cross polarization ratio is relatively low. In an implementation manner of the present application, a half-power beamwidth is 60-65 degrees, and meanwhile, a cross polarization ratio at edges of a +/−60-degree sector is less than −10 dB, and most practical application demands can be met.
Preferably, the focusing member has a conical structure and has a circular, elliptical or polygonal cross section.
It should be noted that the key points of the present application lie in that the focusing member has a conical structure, or may be a cone structure being conical, pyramidal or other polygonal, that is, the cross section of the focusing member is circular or polygonal, depending on the specific design requirements.
Preferably, the radiating element includes four balun-fed folded dipoles tilting for 30-90°.
Preferably, arms of the dipoles are bent towards the central direction of the radiating element.
Preferably, a top of the focusing member with the conical structure is excised in part.
Preferably, in the focusing member, the conductive members have a square, circular, ring-shaped, or other polygonal structure, and the conductive members are placed at an axial portion of the radiating element and are parallel to the reflective plate. The ring-shaped structure may be a circular ring or a polygonal ring; and the ring may be a circular ring or a polygonal ring with an integral structure, or may also be formed by enclosing four segments of straps corresponding to the four dipoles.
Preferably, the conductive members are supported by the dielectric members and are arranged the dipoles respectively; The conductive members are in a shape of a strap, a curved bar, a rectangle, an arc, or a portion of a polygon.
In an implementation manner of the present application, the focusing member has a conical structure formed by enclosing of four dielectric member panels, and the conductive members are in a strap shape, and are attached to the dielectric member panels; the conductive members on the four dielectric member panels are arranged in an axisymmetrical manner; or, the focusing member has a conical frame structure formed by enclosing of four dielectric member posts, and the conductive members in a ring shape are fixed on a dielectric member post frame.
Preferably, in the wideband dual-polarized antenna of the present application, at least two radiating elements and feeding parts are placed on the reflective plate to form a dual-polarized antenna array.
Preferably, the reflective plate is at least provided with two side walls.
Preferably, the wideband dual-polarized antenna is provided with a radome with a circular tube shape.
Due to the adoption of the above technical solution, the present application has the following beneficial effects:
in the wideband dual-polarized antenna of the present application, the beamwidth is adjusted by arranging the focusing member with the conical structure above the radiating element so that the wideband dual-polarized antenna has the beamwidth reaching the desired range, the low cross polarization ratio and can better meet the practical application demands.
An existing dual-polarized antenna, for example, a dual-polarized antenna described in the patent document CN108172978A, as shown in
Therefore, the present application inventively provides that a focusing member with a conical structure is installed above a radiating element, as shown in
Compared with the existing technical solution, the dual-polarized antenna of the present application has the reduced half-power beamwidth, and the antenna having the focusing member with the conical structure obtains higher gains. In addition, the dual-polarized antenna of the present application can increase the cross polarization ratio at the edges of the +/−60-degree sector, and by employing the design that the focusing member has the conical structure, the difference of the beamwidths of an E plane and an H plane is reduced; the dielectric members and the conductive members that jointly constitute the focusing member with the conical structure can change the radiation characteristics of the dual-polarized antenna, and thus, the cross polarization ratio of the antenna can be increased by adjusting the sizes of these components. The dual-polarized antenna of the present application is capable of reducing coupling interference between adjacent antennas. Specifically, the focusing member with the conical structure can focus radiation waves from the arms of the dipoles, and meanwhile, can reduce radiation interference generated by the reflective plate the surface of which is provided with adjacent antennas to increase the overall performance of the antenna.
The present application is further described in detail below by way of specific embodiments and drawings. The following embodiments are only for further illustrating the present application and should not be construed as limiting the present application.
A wideband dual-polarized antenna of the embodiment includes a reflective plate and a radiating element mounted on the reflective plate. The radiating element, as shown in
Compared with a structural form of a focusing conductive member of an existing antenna, the design of the focusing member 5 with the conical structure in the embodiment can more efficiently focus radiation from the arms of the dipoles, making beams produced by the dual-polarized antenna of the present application narrower. Alternatively, in the case that beamwidths are the same, the size of the reflective plate of the antenna of the present invention may be smaller. In addition, compared with the existing technical solution, the dual-polarized antenna of the present application can increase the cross polarization ratio at the edges of the +/−60-degree sector, and the employed focusing member with the conical structure can reduce the difference of the beamwidths of the E plane and the H plane. The focusing member with the conical structure is constituted by the dielectric members and the conductive elements jointly, can change the radiation characteristics of the antenna, and thus, in practical use, the cross polarization ratio of the antenna can be increased by adjusting the sizes of the components.
A wideband dual-polarized antenna of the embodiment is similar to that in the embodiment 1, and has the differences that the focusing member with the conical structure specifically employs a pyramid structure. As shown in
The conductive members in the embodiment, for example, sheet-like conductive members, are placed on an axis part of the radiating element, or bent conductive members in a strap-shaped structure are placed above the arms of the dipoles, and can promote the focusing effect of the focusing member with the conical structure.
Therefore, in the case that the focusing member with the conical structure and multiple layers of conductive members is employed, by changing the dielectric properties of the dielectric members, or optimizing the shape or structure of the conductive members, the dual-polarized antenna can acquire a direction diagram meeting requirements in a wider band range, and good matching between the radiating element and a feed line is achieved. For example, the dielectric members placed at different layers of the focusing member with the conical structure need to be reduced in dielectric constants, and may be considered to be fabricated by using different materials including porous foam-like materials. With such a multilayer focusing member with the conical structure and having conductive members arranged inside, it is possible to obtain a desired radiation direction diagram according to the practical use demands and to reduce the height of the focusing member. Therefore, for the antenna including the focusing member with the conical structure in the embodiment, the usage amount of dielectric materials can be reduced, meanwhile, the size of a radome is reduced, the design and fabrication are simplified, the space is saved, and the cost is lowered.
A wideband dual-polarized antenna in the embodiment is similar to that in the embodiment 1, and has the differences that as shown in
A wideband dual-polarized antenna in the embodiment is similar to that in the embodiment 1, and has the differences that as shown in
In the embodiment, an antenna array is formed by employing the wideband dual-polarized antenna in the embodiment 4. As shown in
In the embodiment, an antenna array is formed by employing the wideband dual-polarized antenna in the embodiment 3, and is placed entirely within a circular tube-shaped radome 28. As shown in
In addition, in the embodiment, the antenna array as shown in
The above content is for further detailed description of the present application in combination with the specific embodiments, and cannot be construed that the specific embodiments of the present application are only limited to these descriptions. Those of ordinary skill in the art can make a plurality of simple derivations and substitutions without departing from the concept of the present application.
Number | Date | Country | Kind |
---|---|---|---|
201910184207.1 | Mar 2019 | CN | national |
The present application is a Continuation Application of PCT Application No. PCT/CN2019/113043 filed on Oct. 24, 2019, which claims the benefit of Chinese Patent Application No. 201910184207.1 filed on Mar. 12, 2019. All the above are hereby incorporated by reference in their entirety.
Number | Date | Country | |
---|---|---|---|
Parent | PCT/CN2019/113043 | Oct 2019 | US |
Child | 17474026 | US |