Antenna apparatus

The present disclosure relates to antenna apparatuses for forming multiple beams.

In recent years, research and development of satellite communication technology using antenna apparatus have been under way. In order to achieve high-speed communications, it is necessary to use an antenna apparatus with high gain and low interference.

To achieve high gain, antenna apparatuses of a system in which a service area is covered with a plurality of spot beams have been studied. In the system of covering a service area with a plurality of spot beams, it is possible to achieve higher gain than in the case of a general contoured beam antenna.

As to interference, which is generally evaluated by carrier-to-interference ratio (C/I), adjacent beams typically use different frequencies or polarizations to achieve low interference. That is, multiple combinations of frequency and polarization are prepared such that adjacent beams do not use the same combination of frequency and polarization.

As a result, interference between adjacent beams can be suppressed. However, interference may occur between beams using the same combination of frequency and polarization.

In an antenna apparatus disclosed in the following Patent Literature 1, interference waves are reduced by using multiple antenna elements to form one beam and using different excitation coefficients for the multiple antenna elements.

Patent Literature

Patent Literature 1: JP 2009-171308 A

Technical Problem

Since the conventional antenna apparatus are configured as described above, there is a problem that, even though interference can be suppressed between desired two beams out of a plurality of beams having the same combination of frequency and polarization can be suppressed, it is difficult to suppress interference among all the beams having the same combination of frequency and polarization.

Embodiments of the present disclosure have been devised in order to solve the problem as described above, and it is an object of the present disclosure to provide an antenna apparatus capable of suppressing interference among all the beams having the same combination of frequency and polarization.

Solution to Problem

An antenna apparatus according to the present disclosure includes: a plurality of primary radiators for radiating radio waves; and a main reflector for reflecting the radio waves radiated from the plurality of primary radiators, wherein the plurality of primary radiators is classified by combination of frequency and polarization of the radiated radio waves, a plurality of primary radiators belonging to a same class is arranged, in a repeated triangle pattern in which a triangle is arranged repeatedly, at positions corresponding to vertexes of each triangle, and a shape of the main reflector and a shape and arrangement of the repeated triangle pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in the triangle is different from a radiation direction of a sidelobe of a radio wave that is radiated from primary radiators arranged at positions corresponding to the vertexes and is reflected by the main reflector.

Advantageous Effects of Invention

According to the present disclosure, a plurality of primary radiators is classified by combination of frequency and polarization of the radiated radio waves, a plurality of primary radiators belonging to the same class is arranged at positions corresponding to vertexes of one of triangles in a repeated triangle pattern in which a triangular shape is repeated, and a shape of the main reflector and a shape and arrangement of the repeated triangle pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in the triangle is different from a radiation direction of a sidelobe of a radio wave reflected by the main reflector after having been radiated from a primary radiator arranged at a position corresponding to the vertexes. Therefore, the effect of suppressing interference among all the beams having the same combination of frequency and polarization can be obtained.

FIG. 1 is a configuration diagram illustrating an antenna apparatus according to First Embodiment of the present disclosure.

FIG. 2 is a diagram showing an illustrative example of arrangement of primary radiators 1 of the antenna apparatus according to First Embodiment of the present disclosure.

FIG. 3 is an explanatory diagram illustrating an example of combinations of frequency and polarization corresponding to labels.

FIG. 4A is an explanatory diagram illustrating a repeated triangle pattern TR Pattern in which three triangular shapes TR P1 , TR P2 , and TR P3 are arranged in the horizontal direction, FIG. 4B is an explanatory diagram illustrating a repeated triangle pattern TR Pattern in which the two triangular shapes TR p1 and TR P3 are arranged in the horizontal direction and two triangular shapes TR P3 and TR P4 are arranged in the horizontal direction while the two triangular shapes TR P1 and TR P3 are arranged in the vertical direction and two triangular shape patterns TR P2 and TR P4 are arranged in the vertical direction.

FIG. 5 is an explanatory diagram illustrating radiation direction 4 of beams reflected by a main reflector 2 .

FIG. 6A is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflected beam of a primary radiator 1 labeled A 4 , FIG. 6B is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflected beam of a primary radiator 1 labeled B 4 , FIG. 6C is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflected beam of a primary radiator 1 labeled C 2 , and FIG. 6D is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflected beam of a primary radiator 1 labeled D 2 .

FIG. 7 is an explanatory diagram illustrating a simulation result of a radiation pattern of a reflection beam of the primary radiator 1 labeled C 2 .

FIG. 8 is an explanatory diagram illustrating a simulation result of a radiation pattern of the reflection beam of the primary radiator 1 labeled C 2 in the case where an aperture shape of the main reflector 2 is circular.

FIG. 9 is an explanatory diagram showing C/I values in the case where the aperture shape of the main reflector 2 is a parallelogram and in the case where it is circular.

FIG. 10 is a configuration diagram illustrating an antenna apparatus according to Second Embodiment of the present disclosure.

FIG. 11 is a diagram showing an illustrative example of arrangement of primary radiators 1 of the antenna apparatus according to Second Embodiment of the present disclosure.

FIG. 12 is an explanatory diagram illustrating radiation directions θ 1 , θ 2 , and θ 3 of sidelobes of a reflected beam of a primary radiator 1 labeled A 4 .

FIG. 13 is a configuration diagram illustrating an antenna apparatus according to Third Embodiment of the present disclosure.

FIG. 14 is a diagram showing an illustrative example of arrangement of primary radiators 1 of the antenna apparatus according to Third Embodiment of the present disclosure.

FIG. 15 is an explanatory diagram illustrating radiation directions θ 1 , θ 2 , and θ 3 of sidelobes of a reflected beam of a primary radiator 1 labeled C 3 .

FIG. 16 is a configuration diagram illustrating an antenna apparatus according to Fourth Embodiment of the present disclosure.

FIG. 17 is a configuration diagram illustrating an antenna apparatus according to Fifth Embodiment of the present disclosure.

To describe the present disclosure further in detail, embodiments of the present disclosure will be described below with reference to the accompanying drawings.

First Embodiment

FIG. 1 is a configuration diagram illustrating an antenna apparatus according to First Embodiment of the present disclosure.

In FIG. 1 , each of primary radiators 1 is a radio wave irradiation source for radiating a radio wave toward a main reflector 2 .

The primary radiators 1 are arranged such that a spillover of the main reflector 2 is reduced and, in the example of FIG. 1 , are arranged near a focal point of the main reflector 2 .

The main reflector 2 reflects radio waves radiated from the plurality of primary radiators 1 , and in the example of FIG. 1 the shape of the main reflector 2 is a parabolid.

Reference numeral 3 illustrates an aperture shape when the main reflector 2 is viewed from the front, and in the example of FIG. 1 an aperture shape 3 of the main reflector 2 is a parallelogram.

In First Embodiment, the plurality of primary radiators 1 are classified according to combination of frequency and polarization of radiated radio waves, and a plurality of primary radiators 1 belonging to the same class are arranged at positions corresponding to vertexes of triangles in a repeated triangle pattern in which a triangular shape is repeatedly arranged. Details will be described later.

Furthermore, the shape of the main reflector 2 and the shape and arrangement of the repeated triangle pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in a triangle is different from a radiation direction of a sidelobe of a radio wave that is radiated from primary radiators 1 arranged at positions corresponding to the vertexes and is reflected by the main reflector 2 .

FIG. 2 is a diagram showing an illustrative example of arrangement of the primary radiators 1 of the antenna apparatus according to First Embodiment of the present disclosure.

FIG. 2 illustrates arrangement of the primary radiators 1 as viewed from the front, and in the example of FIG. 2 sixteen primary radiators 1 are arranged. However, this is merely an example, and the number is not limited to sixteen.

An alphabet in the figure is a label representing a combination of frequency and polarization of a radio wave radiated from a primary radiator 1 , and primary radiators 1 labeled with the same alphabet use the same combination of frequency and polarization.

FIG. 3 is an explanatory diagram illustrating an example of combinations of frequency and polarization corresponding to labels.

In FIG. 3 , for example, combinations of two types of polarizations P 1 and P 2 such as vertical polarization and horizontal polarization and two types of frequencies F 1 and F 2 are illustrated, and in FIG. 3 a total of four combinations are described as an example.

The sixteen primary radiators 1 in FIG. 2 are classified according to combination of frequency and polarization of radiated radio waves, and primary radiators 1 labeled A 1 , A 2 , A 3 , and A 4 belong to the same class, and primary radiators 1 labeled B 1 , B 2 , B 3 , and B 4 belong to the same class.

Primary radiators 1 labeled C 1 , C 2 , C 3 , and C 4 belong to the same class, and primary radiators 1 labeled D 1 , D 2 , D 3 , and D 4 belong to the same class.

A plurality of primary radiators 1 belonging to the same class is arranged at positions corresponding to vertexes of triangles in a repeated triangle pattern in which one or more triangular shapes are repeated.

Looking at the four primary radiators 1 labeled A 1 , A 2 , A 3 , and A 4 for example, the three primary radiators 1 labeled A 1 , A 3 , and A 4 are arranged in a triangular shape, and the three primary radiators 1 labeled A 1 , A 2 , and A 4 are also arranged in a triangular shape.

That is, the four primary radiators 1 labeled A 1 , A 2 , A 3 , and A 4 are arranged at positions corresponding to vertexes of triangles in a repeated triangle pattern TR Pattern in which a triangular shape TR P1 and a triangular shape TR P2 are arranged.

The triangular shape TR P1 is an arrangement of the three primary radiators 1 labeled A 1 , A 3 , and A 4 , and the triangular shape TR P2 is an arrangement of the three primary radiators 1 labeled A 1 , A 2 , and A 4 . FIG. 2 illustrates an example in which each of the triangles is an equilateral triangle.

In FIG. 2 , an example of the repeated triangle pattern TR Pattern in which the two triangular shapes TR P1 and TR P2 are arranged in the horizontal direction in the figure is illustrated; however, a repeated triangle pattern TR Pattern in which three or more triangular shapes TR P are arranged in the horizontal direction or a repeated triangle pattern TR Pattern in which a plurality of triangular shapes TR P are arranged in the vertical direction may be employed.

As shown in the example of FIG. 2 , the four primary radiators 1 labeled A 1 , A 2 , A 3 , and A 4 are arranged so as to be in contact with sides of the triangles, and thus the position of the center of each of the primary radiators 1 is apart from the position of a vertex of the triangles. Because the four primary radiators 1 are arranged near the vertexes of the triangles, the four primary radiators 1 are arranged at positions corresponding to the vertexes of the triangles.

Note that it is understood without saying that the position of the center of each of the primary radiators 1 may be arranged so as to coincide with a vertex of the triangles.

FIG. 4 includes explanatory diagrams illustrating examples of a repeated triangle pattern TR Pattern .

FIG. 4A is a diagram illustrating a repeated triangle pattern TR Pattern in which three triangular shapes TR P1 , TR P2 , and TR P3 are arranged in the horizontal direction.

The triangular shape TR P1 is an arrangement of the three primary radiators 1 labeled A 1 , A 3 , and A 4 , the triangular shape TR P2 is an arrangement of the three primary radiators 1 labeled A 1 , A 2 , and A 4 , and the triangular shape TR P3 is an arrangement of the three primary radiators 1 labeled A 2 , A 4 , and A 5 .

FIG. 4B is a diagram illustrating a repeated triangle pattern TR Pattern in which the two triangular shapes TR P1 and TR P2 are arranged in the horizontal direction and the two triangular shapes TR P3 and TR P4 are arranged in the horizontal direction, while the two triangular shapes TR P1 and TR P2 are arranged in the vertical direction and two triangular shapes TR P2 and TR P4 are arranged in the vertical direction.

The triangular shape TR P1 is an arrangement of the three primary radiators 1 labeled A 1 , A 3 , and A 4 , the triangular shape TR P2 is an arrangement of the three primary radiators 1 labeled A 1 , A 2 , and A 4 , the triangular shape TR P3 is an arrangement of the three primary radiators 1 labeled A 3 , A 5 , and A 6 , and the triangular shape TR P4 is an arrangement of the three primary radiators 1 labeled A 3 , A 4 , and A 6 .

As can be seen from FIG. 4 , a repeated triangle pattern TR Pattern of a desired shape can be created by repeating a plurality of triangular shapes TR P in a desired direction.

In the above, the repeated triangle pattern TR Pattern in which one or more triangular shapes are repeated has been described focusing on the four primary radiators 1 labeled A 1 , A 2 , A 3 , and A 4 . In the example of FIG. 2 , arrangements of the primary radiators 1 labeled B 1 , B 2 , B 3 , and B 4 also form a repeated triangle pattern TR Pattern in which the two triangular shapes TR P are arranged in the horizontal direction.

Likewise, arrangements of the primary radiators 1 labeled C 1 , C 2 , C 3 , and C 4 also form a repeated triangle pattern TR Pattern in which two triangular shapes TR P are arranged in the horizontal direction, and arrangements of the primary radiators 1 labeled D 1 , D 2 , D 3 , and D 4 also form a repeated triangle pattern TR Pattern in which two triangular shapes TR P are arranged in the horizontal direction.

In the example of FIG. 2 , since there are four combinations of frequency and polarization of radiated radio waves, four repeated triangle patterns TR Pattern each corresponding to one of the combinations are arranged to be combined regularly, and the overall arrangement shape of the sixteen primary radiators 1 has the same parallelogram shape as that of the aperture shape 3 of the main reflector 2 .

Furthermore in the example of FIG. 2 , given vertexes H, I, J, and K of the parallelogram which is the aperture shape 3 of the main reflector 2 , interior angles ∠IHK and ∠IJK of the parallelogram have 60 degrees, which are equal to an interior angle of an equilateral triangle. Moreover, the sixteen primary radiators 1 are arranged such that a radio wave radiated from the primary radiator 1 labeled C 3 is irradiated near the vertex H, a radio wave radiated from the primary radiator 1 labeled D 4 is irradiated near the vertex I, a radio wave radiated from the primary radiator 1 labeled B 2 is irradiated near the vertex J, and a radio wave radiated from the primary radiator 1 labeled A 1 is irradiated near the vertex K.

Also, focusing on the three primary radiators 1 labeled A 1 , B 1 , and D 1 out of the sixteen primary radiators 1 , the three primary radiators 1 are arranged in an equilateral triangle shape without overlapping. This is to arrange beams densely, and the equilateral triangle shape is known as a shape that enables the densest arrangement of a circular aperture.

Next, operations will be described.

The sixteen primary radiators 1 radiate radio waves toward the main reflector 2 . Each of the radio waves radiated from the primary radiators 1 is hereinafter referred to as a beam.

The main reflector 2 reflects beams radiated from the sixteen primary radiators 1 .

FIG. 5 is an explanatory diagram illustrating radiation directions 4 of the beams reflected by the main reflector 2 .

In FIG. 5 , the horizontal axis represents the angle in a horizontal plane, the vertical axis represents the angle in a vertical plane, and a radiation direction 4 of a beam corresponds to a service area of a radio wave.

Furthermore, a label attached to each of the radiation directions 4 of the beams corresponds to a label labeled to each of the primary radiators 1 illustrated in FIG. 2 .

FIG. 6 includes explanatory diagrams illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflection beam of a primary radiator 1 .

Hereinafter, the expression “reflection beam of a primary radiator 1 ” means a beam radiated from the primary radiator 1 and then reflected by the main reflector 2 .

FIG. 6A is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflection beam of the primary radiator 1 labeled A 4 , and FIG. 6B is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflection beam of the primary radiator 1 labeled B 4 .

Furthermore, FIG. 6C is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflection beam of the primary radiator 1 labeled C 2 , and FIG. 6D is an explanatory diagram illustrating radiation directions θ 1 and θ 2 of sidelobes of a reflection beam of the primary radiator 1 labeled D 2 .

The radiation directions θ 1 and θ 2 of sidelobes are determined by the aperture shape 3 of the main reflector 2 , and in a case where the aperture shape 3 of the main reflector 2 is a parallelogram, each of the radiation directions θ 1 and θ 2 is formed in the direction that is perpendicular to associated opposing two sides of the parallelogram.

Looking at the primary radiator 1 labeled A 4 for example, as illustrated in FIG. 6A , sidelobes are formed in a direction θ 1 perpendicular to a line segment HI and a line segment KJ of the parallelogram, while other sidelobes are formed in a direction θ 2 perpendicular to a line segment HK and a line segment IJ of the parallelogram.

Further looking at the primary radiator 1 labeled B 4 , as illustrated in FIG. 6B , sidelobes are formed in a direction θ 1 perpendicular to the line segment HI and the line segment KJ of the parallelogram, while other sidelobes are formed in a direction θ 2 perpendicular to the line segment HK and the line segment IJ of the parallelogram.

Looking at the primary radiator 1 labeled C 2 , as illustrated in FIG. 6C , sidelobes are formed in a direction θ 1 perpendicular to the line segment HI and the line segment KJ of the parallelogram, while other sidelobes are formed in a direction θ 2 perpendicular to the line segment HK and the line segment IJ of the parallelogram.

Further looking at the primary radiator 1 labeled D 2 , as illustrated in FIG. 6D , sidelobes are formed in a direction θ 1 perpendicular to the line segment HI and the line segment KJ of the parallelogram, while other sidelobes are formed in a direction θ 2 perpendicular to the line segment HK and the line segment IJ of the parallelogram.

Looking at the primary radiator 1 labeled A 4 for example, primary radiators 1 having the same combination of frequency and polarization as that of a beam of the primary radiator 1 labeled A 4 are the primary radiators 1 labeled A 1 , A 2 , and A 3 .

Therefore, out of beams reflected by the main reflector 2 , reflection beams of the primary radiators 1 labeled A 1 , A 2 , and A 3 may be interfered by a reflection beam of the primary radiator 1 labeled A 4 .

However, in First Embodiment, since the overall arrangement of the sixteen primary radiators 1 has the same parallelogram shape as that of the aperture shape 3 of the main reflector 2 , the reflection beams of the primary radiators 1 labeled A 1 , A 2 , and A 3 are not interfered by the reflection beam of the primary radiator 1 labeled A 4 .

That is, the primary radiator 1 labeled A 4 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled A 1 and A 2 . Furthermore, the primary radiator 1 labeled A 4 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled A 1 and A 3 .

Suppose the position that corresponds to the vertex of the equilateral triangle(s) at which the primary radiator 1 labeled A 4 is arranged is a base point. Then, directions of line segments passing through the base point and the positions corresponding to the other vertexes of the equilateral triangles are given as a direction α 1 , a direction α 2 , and a direction α 3 as illustrated in FIG. 6A .

Specifically, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement position of the primary radiator 1 labeled A 1 is α 1 , and a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement position of the primary radiator 1 labeled A 2 is α 2 . Moreover, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement position of the primary radiator 1 labeled A 3 is α 3 .

Because the directions α 1 , α 2 , and α 3 of the line segments are different from the radiation directions θ 1 and θ 2 of the sidelobes, reflection beams of the primary radiators 1 labeled A 1 , A 2 , and A 3 are not interfered by the reflection beam of the primary radiator 1 labeled A 4 .

Looking at the primary radiator 1 labeled C 2 for example, primary radiators 1 having the same combination of frequency and polarization as that of a beam of the primary radiator 1 labeled C 2 are the primary radiators 1 labeled C 1 , C 3 , and C 4 .

Therefore, out of beams reflected by the main reflector 2 , reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 may be interfered by a reflection beam of the primary radiator 1 labeled C 2 .

However, in First Embodiment, since the overall arrangement of the sixteen primary radiators 1 has the same parallelogram shape as that of the aperture shape 3 of the main reflector 2 , the reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 are not interfered by the reflection beam of the primary radiator 1 labeled C 2 .

That is, the primary radiator 1 labeled C 2 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled C 1 and C 4 .

Suppose the position that corresponds to the vertex of the equilateral triangle at which the primary radiator 1 labeled C 2 is arranged is a base point. Then, directions of line segments passing through the base point and the positions corresponding to the other vertexes of the equilateral triangle are given as a direction α 3 and a direction α 2 as illustrated in FIG. 6C .

Specifically, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled C 2 and the arrangement position of the primary radiator 1 labeled C 1 is α 3 , and a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled C 2 and the arrangement position of the primary radiator 1 labeled C 4 is α 2 .

Although the primary radiator 1 with label C 2 and the primary radiator 1 labeled C 3 are not located at positions corresponding to vertexes of the same equilateral triangle, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled C 2 and the arrangement position of the primary radiator 1 labeled C 3 is α 4 .

Because the directions α 2 , α 3 , and α 4 of the line segments are different from the radiation directions θ 1 and θ 2 of the sidelobes, reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 are not interfered by the reflection beam of the primary radiator 1 labeled C 2 .

Looking at the primary radiator 1 labeled B 4 , a similar relation to the case of looking at the primary radiator 1 labeled A 4 applies, and reflection beams of the primary radiators 1 labeled B 1 , B 2 , and B 3 are not interfered by a reflection beam of the primary radiator 1 labeled B 4 .

In addition, looking at the primary radiator 1 labeled D 2 , a similar relation to the case of looking at the primary radiator 1 labeled C 2 applies, and reflection beams of the primary radiators 1 labeled D 1 , D 3 , and D 4 are not interfered by a reflection beam of the primary radiator 1 labeled D 2 .

FIG. 7 is an explanatory diagram illustrating a simulation result of a radiation pattern of a reflection beam of the primary radiator 1 labeled C 2 .

In FIG. 7 , the horizontal axis represents the angle in a horizontal plane, and the vertical axis represents the angle in a vertical plane. Since the aperture shape 3 of the main reflector 2 is a parallelogram, sidelobes due to the reflection beam of the primary radiator 1 labeled C 2 are formed in two directions.

However, as described above, it is understood that the reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 are not interfered by the reflection beam of the primary radiator 1 labeled C 2 since the directions α 2 , α 3 , and α 4 of the line segments are different from the radiation directions θ 1 and θ 2 of the sidelobes.

FIG. 8 is an explanatory diagram illustrating a simulation result of a radiation pattern of the reflection beam of the primary radiator 1 labeled C 2 in the case where the aperture shape of the main reflector 2 is circular.

In FIG. 8 , the horizontal axis represents the angle in a horizontal plane, and the vertical axis represents the angle in a vertical plane.

In the case where the aperture shape of the main reflector 2 is circular, sidelobes due to the reflection beam of the primary radiator 1 labeled C 2 are concentrically formed around the direction of the main beam. It can be understood that as a result of the above the sidelobes due to the reflection beam of the primary radiator 1 labeled C 2 arrive at service areas of reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 , and thus the reflection beams of the primary radiators 1 labeled C 1 , C 3 , and C 4 are interfered by the reflection beam of the primary radiator 1 labeled C 2 .

Note that, in the case where the aperture shape of the main reflector 2 is rectangular, sidelobes are formed in directions each perpendicular to two opposing sides of the rectangle. Therefore, the reflection beams of the primary radiators 1 labeled C 3 and C 4 are not interfered by the reflection beam of the primary radiator 1 labeled C 2 ; however, the reflection beam of the primary radiator 1 labeled C 1 is interfered by the reflection beam of the primary radiator 1 labeled C 2 since the sidelobes due to the reflection beam of the primary radiator 1 labeled C 2 arrive at the service area of the reflection beam of the primary radiator 1 labeled C 1 .

FIG. 9 is an explanatory diagram showing C/I values in the case where the aperture shape of the main reflector 2 is a parallelogram and in the case where it is circular.

A C/I in the case where the aperture shape 3 of the main reflector 2 is a parallelogram is −28.5 dB, and a C 1 in the case where the aperture shape of the main reflector is circular is −23.2 dB, and therefore the C/I is improved by 5.3 dB in the case where the aperture shape 3 of the main reflector 2 is a parallelogram than in the case where the aperture shape is circular.

As is apparent from the above, according to First Embodiment, the plurality of primary radiators 1 is classified by combination of frequency and polarization of the radiated radio waves, a plurality of primary radiators belonging to the same class is arranged at positions corresponding to vertexes of one of triangles in a repeated triangle pattern TR Pattern , and the shape of the main reflector 2 and the shape and arrangement of the repeated triangle pattern TR Pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in the triangle is different from a radiation direction of a sidelobe of a radio wave reflected by the main reflector 2 after having been radiated from a primary radiator 1 arranged at a position corresponding to the vertexes. Therefore, the effect of suppressing interference among all the beams having the same combination of frequency and polarization can be obtained.

According to First Embodiment, the aperture shape 3 of the main reflector 2 is a parallelogram, and one or more triangular shapes are repeated such that the repeated triangle pattern TR Pattern has the same shape as that of the aperture shape 3 of the main reflector 2 , and thus a major part of radio waves radiated from the plurality of primary radiators 1 is reflected by the main reflector 2 , thereby enabling mitigation of radio waves not reflected by the main reflector 2 . Therefore, the utilization rate of radio waves is increased, and the gain of the antenna apparatus can be increased.

In First Embodiment, the example has been illustrated in which two interior angles of the parallelogram which is the aperture shape 3 of the main reflector 2 , that is, the ∠IHK and the ∠IJK are 60 degrees, which are equal to the interior angles of an equilateral triangle; however, even in the case where the ∠IHK and the ∠IJK of the parallelogram deviate from 60 degrees by about 20%, interference among all the beams having the same combination of frequency and polarization can be suppressed. That is, even in the case where the aperture shape 3 of the main reflector 2 is not a perfect parallelogram, interference among all the beams having the same combination of frequency and polarization can be suppressed.

In First Embodiment, the example in which the three primary radiators 1 are arranged in a triangular shape has been illustrated; however depending on a required service area, one or two primary radiators 1 may be thinned out from those in a triangular shape TR P from among a plurality of triangular shapes TR P .

Furthermore, it is only required that an arrangement of the repeated triangle pattern TR Pattern is in conformity with the arrangement of FIG. 2 for example, and the shape of the repeated triangle pattern TR Pattern is not required to be a parallelogram as a result of thinning out some of the primary radiators 1 .

In First Embodiment, the example in which there are four combinations of frequency and polarization has been illustrated; however, this is merely an example, and the number of combinations of frequency and polarization may be three or seven, for example.

In First Embodiment, the aperture shape 3 of the main reflector 2 is a parallelogram; however, vertexes of the parallelogram are not required to be angular and may be, for example, rounded or chamfered.

Second Embodiment

In Embodiment 1, the aperture shape 3 of the main reflector 2 is a parallelogram. In Second Embodiment, an example in which an aperture shape of the main reflector is a hexagon will be described.

In the case where the aperture shape 3 of the main reflector 2 is a parallelogram, for example when the antenna apparatus is mounted on a satellite, useless space is created, and the space cannot be effectively used, which may deteriorate mountability to the satellite.

Accordingly, in Second Embodiment, an example will be described in which a hexagon is used as a shape that enables more effective use of the space.

FIG. 10 is a configuration diagram illustrating an antenna apparatus according to Second Embodiment of the present disclosure. In FIG. 10 , the same reference numeral as that in FIG. 1 represents the same or a corresponding part and thus descriptions thereon are omitted.

A main reflector 5 is a reflector which reflects radio waves radiated from a plurality of primary radiators 1 .

Reference numeral 6 denotes an aperture shape of the main reflector 5 when viewed from the front, and in the example of FIG. 10 , an aperture shape 6 of the main reflector 5 is a hexagon.

In Second Embodiment, it is assumed that the aperture shape 6 of the main reflector 5 is a regular hexagon.

FIG. 11 is a diagram showing an illustrative example of arrangement of the primary radiators 1 of the antenna apparatus according to Second Embodiment of the present disclosure.

FIG. 11 illustrates an arrangement of the primary radiators 1 as viewed from the front, and in the example of FIG. 11 nineteen primary radiators 1 are arranged. However, this is merely an example, and the number is not limited to nineteen.

An alphabet in the figure is a label representing a combination of frequency and polarization of a radio wave radiated from a primary radiator 1 , and primary radiators 1 labeled with the same alphabet use the same combination of frequency and polarization.

The nineteen primary radiators 1 in FIG. 11 are classified by combinations of frequency and polarization of radiated radio waves, and primary radiators 1 labeled A 1 , A 2 , A 3 , A 4 , A 5 , A 6 , and A 7 belong to the same class, and primary radiators 1 labeled B 1 , B 2 , B 3 , and B 4 belong to the same class.

Primary radiators 1 labeled C 1 , C 2 , C 3 , and C 4 belong to the same class, and primary radiators 1 labeled D 1 , D 2 , D 3 , and D 4 belong to the same class.

A plurality of primary radiators 1 belonging to the same class is arranged at positions corresponding to vertexes of each of triangles in a repeated triangle pattern in which one or more triangular shapes are repeated.

Looking at the four primary radiators 1 labeled C 1 , C 2 , C 3 , and C 4 for example, the three primary radiators 1 labeled C 1 , C 2 , and C 3 are arranged in a triangular shape, and the three primary radiators 1 labeled C 2 , C 3 , and C 4 are also arranged in a triangular shape.

That is, the four primary radiators 1 labeled C 1 , C 2 , C 3 , and C 4 are arranged at positions corresponding to vertexes of each of triangles in a repeated triangle pattern TR Pattern in which a triangular shape TR P1 and a triangular shape TR P2 are arranged.

The triangular shape TR P1 is an arrangement of the three primary radiators 1 labeled C 1 , C 2 , and C 3 , and the triangular shape TR P2 is an arrangement of the three primary radiators 1 labeled C 2 , C 3 , and C 4 . FIG. 11 illustrates an example in which each of the triangles is an equilateral triangle.

In FIG. 11 , an example of the repeated triangle pattern TR Pattern in which the two triangular shapes TR P1 and TR P2 are arranged in the horizontal direction in the figure is illustrated; however, a repeated triangle pattern TR Pattern in which three or more triangular shapes TR P are arranged in the horizontal direction or a repeated triangle pattern TR Pattern in which a plurality of triangular shapes TR P are arranged in the vertical direction may be employed.

Next, operations will be described.

The nineteen primary radiators 1 radiate beams toward the main reflector 5 .

The main reflector 5 reflects the beams radiated from the nineteenth primary radiators 1 .

FIG. 12 is an explanatory diagram illustrating radiation directions θ 1 , θ 2 , and θ 3 of sidelobes of a reflection beam of the primary radiator 1 labeled A 4 .

The radiation directions θ 1 , θ 2 , and θ 3 of the sidelobes are determined by the aperture shape 6 of the main reflector 5 , and in the case where the aperture shape of the main reflector 5 is a regular hexagon, the sidelobes are formed in directions each perpendicular to two sides of the regular hexagon opposing each other.

That is, sidelobes are formed in the direction θ 1 perpendicular to both a line segment LM and a line segment OP of the regular hexagon, sidelobes are formed in the direction θ 2 perpendicular to both a line segment MN and a line segment PQ of the regular hexagon, and sidelobes are formed in the direction θ 3 perpendicular to both a line segment NO and a line segment QL of the regular hexagon.

Looking at the primary radiator 1 labeled A 4 for example, primary radiators 1 having the same combination of frequency and polarization as that of a beam of the primary radiator 1 labeled A 4 are the primary radiators 1 labeled A 1 , A 2 , A 3 , A 5 , A 6 , and A 7 .

Thus, out of beams reflected by the main reflector 5 , reflection beams of the primary radiators 1 labeled A 1 , A 2 , A 3 , A 5 , A 6 , and A 7 may be interfered by a reflection beam of the primary radiator 1 labeled A 4 .

However, in Second Embodiment, since the overall arrangement of the nineteen primary radiators 1 has the same regular hexagon shape as that of the aperture shape 6 of the main reflector 5 , the reflection beams of the primary radiators 1 labeled A 1 , A 2 , A 3 , A 5 , A 6 , and A 7 are not interfered by the reflection beam of the primary radiator 1 labeled A 4 .

That is, the primary radiator 1 labeled A 4 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled A 1 and A 2 , for example. Furthermore, the primary radiator 1 labeled A 4 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled A 1 and A 3 .

Directions of line segments passing through a base point of the position corresponding to the vertex of the equilateral triangles, in which the primary radiator 1 labeled A 4 is arranged, and the positions corresponding to the other vertexes of the equilateral triangles are given as a direction α 1 , a direction α 2 , and a direction α 3 as illustrated in FIG. 12 .

Specifically, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement positions of the primary radiators 1 labeled A 1 and A 7 is α 1 , and a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement positions of the primary radiators 1 labeled A 2 and A 6 is α 2 . Moreover, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled A 4 and the arrangement positions of the primary radiators 1 labeled A 3 and A 5 is α 3 .

Because the directions α 1 , α 2 , and α 3 of the line segments are different from the radiation directions θ 1 , θ 2 , and θ 3 of the sidelobes, reflection beams of the primary radiators 1 labeled A 1 , A 2 , A 3 , A 5 , A 6 , and A 7 are not interfered by the reflection beam of the primary radiator 1 labeled A 4 .

As is apparent from the above, according to Second Embodiment, the plurality of primary radiators 1 is classified by combination of frequency and polarization of the radiated radio waves, a plurality of primary radiators belonging to the same class is arranged at positions corresponding to vertexes of one of triangles in a repeated triangle pattern TR Pattern and the shape of the main reflector 5 and the shape and arrangement of the repeated triangle pattern TR Pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in the triangle is different from a radiation direction of a sidelobe of a radio wave reflected by the main reflector 5 after having been radiated from a primary radiator 1 arranged at a position corresponding to the vertexes. Therefore, the effect of suppressing interference among all the beams having the same combination of frequency and polarization can be obtained.

Furthermore, according to Second Embodiment, the aperture shape 6 of the main reflector 5 is a regular hexagon, and one or more triangular shapes are repeated such that the repeated triangle pattern TR Pattern has the same shape as that of the aperture shape 6 of the main reflector 5 , and thus a major part of radio waves radiated from the plurality of primary radiators 1 is reflected by the main reflector 5 , thereby enabling mitigation of radio waves not reflected by the main reflector 5 . Therefore, the utilization rate of radio waves is increased, and the gain of the antenna apparatus can be increased. In addition, mountability to a satellite can be enhanced for example compared to First Embodiment.

In Second Embodiment, the example has been illustrated in which interior angles of the hexagon which is the aperture shape 6 of the main reflector 5 are 120 degrees; however, even in the case where the interior angles deviate from 120 degrees by about 20%, interference among all the beams having the same combination of frequency and polarization can be suppressed. That is, even in the case where the aperture shape 6 of the main reflector 5 is not a perfect regular hexagon, interference among all the beams having the same combination of frequency and polarization can be suppressed.

In Second Embodiment, the example in which the three primary radiators 1 are arranged in a triangular shape has been illustrated; however depending on a required service area, one or two primary radiators 1 may be thinned out from those in a triangular shape TR P from among a plurality of triangular shapes TR P .

Furthermore, it is only required that an arrangement of the repeated triangle pattern TR Pattern is in conformity with the arrangement of FIG. 11 for example, and the shape of the repeated triangle pattern TR Pattern is not required to be a regular hexagon as a result of thinning out some of the primary radiators 1 .

In Second Embodiment, the example in which there are four combinations of frequency and polarization has been illustrated; however, this is merely an example, and the number of combinations of frequency and polarization may be three or seven, for example.

In Second Embodiment, the aperture shape 6 of the main reflector 5 is a regular hexagon; however, vertexes of the regular hexagon are not required to be angular and may be, for example, rounded or chamfered.

Third Embodiment

In First Embodiment, the aperture shape 3 of the main reflector 2 is a parallelogram. In Third Embodiment, an example in which an aperture shape of the main reflector is triangular will be described.

FIG. 13 is a configuration diagram illustrating an antenna apparatus according to Third Embodiment of the present invention. In FIG. 13 , the same reference numeral as that in FIG. 1 represents the same or a corresponding part and thus descriptions thereon are omitted.

A main reflector 7 is a reflector which reflects radio waves radiated from a plurality of primary radiators 1 .

Reference numeral 8 denotes an aperture shape of the main reflector 7 when viewed from the front, and in the example of FIG. 13 , the aperture shape 8 of the main reflector 7 is triangular.

In Third Embodiment, it is assumed that the aperture shape 8 of the main reflector 7 is an equilateral triangle.

FIG. 14 is a diagram showing an illustrative example of arrangement of the primary radiators 1 of the antenna apparatus according to Third Embodiment of the present disclosure.

FIG. 14 illustrates arrangement of the primary radiators 1 as viewed from the front, and in the example of FIG. 14 fifteen primary radiators 1 are arranged. However, this is merely an example, and the number is not limited to fifteen.

An alphabet in the figure is a label representing a combination of frequency and polarization of a radio wave radiated from a primary radiator 1 , and primary radiators 1 labeled by the same alphabet use the same combination of frequency and polarization.

The fifteen primary radiators 1 in FIG. 14 are classified by combination of frequency and polarization of radiated radio waves, and primary radiators 1 labeled A 1 , A 2 , A 3 , A 4 , A 5 , and A 6 belong to the same class, and primary radiators 1 labeled B 1 , B 2 , and B 3 belong to the same class.

Primary radiators 1 labeled C 1 , C 2 , and C 3 belong to the same class, and primary radiators 1 labeled D 1 , D 2 , and D 3 belong to the same class.

A plurality of primary radiators 1 belonging to the same class is arranged at positions corresponding to vertexes of each of triangles in a repeated triangle pattern in which one or more triangular shapes are repeated.

Looking at the six primary radiators 1 labeled A 1 , A 2 , A 3 , A 4 , A 5 , and A 6 for example, the three primary radiators 1 labeled A 1 , A 2 , and A 3 are arranged in a triangular shape, and the three primary radiators 1 labeled A 2 , A 4 , and A 5 are also arranged in a triangular shape. The three primary radiators 1 labeled A 2 , A 3 , and A 5 are arranged in a triangular shape, and the three primary radiators 1 labeled A 3 , A 5 , and A 6 are arranged in a triangular shape.

That is, the six primary radiators labeled A 1 , A 2 , A 3 , A 4 , A 5 , and A 6 are arranged at positions corresponding to vertexes of each of triangles in a repeated triangle pattern TR Pattern in which a triangular shape TR P1 , a triangular shape TR P2 , a triangular shape TR P3 , and a triangular shape TR P4 are arranged.

The triangular shape TR P1 is an arrangement of the three primary radiators 1 labeled A 1 , A 2 , and A 3 , the triangular shape TR P2 is an arrangement of the three primary radiators 1 labeled A 2 , A 4 , and A 5 , the triangular shape TR P3 is an arrangement of the three primary radiators 1 labeled A 2 , A 3 , and A 5 , and the triangular shape TR P4 is an arrangement of the three primary radiators 1 labeled A 3 , A 5 , and A 6 . FIG. 14 illustrates an example in which each of the triangles is an equilateral triangle.

In FIG. 14 , an example of the repeated triangle pattern TR Pattern in which the three triangular shapes TR P2 , TR P3 , and TR P4 are arranged in the horizontal direction in the figure and the triangular shapes TR P1 , TR P2 , TR P3 , and TR 4 are arranged in the vertical direction in the figure is illustrated; however, the present invention is not limited thereto, and the number of repetitive patterns in the horizontal direction and the vertical direction may be any number.

Next, operations will be described.

The fifteen primary radiators 1 radiate beams toward the main reflector 7 .

The main reflector 7 reflects the beams radiated from the fifteenth primary radiators 1 .

FIG. 15 is an explanatory diagram illustrating radiation directions θ 1 , θ 2 , and θ 3 of sidelobes of a reflection beam of the primary radiator 1 labeled C 3 .

The radiation directions θ 1 , θ 2 , and θ 3 of the sidelobes are determined by the aperture shape 8 of the main reflector 7 , and in the case where the aperture shape 8 of the main reflector 7 is an equilateral triangle, the sidelobes are formed in directions each perpendicular to one side of the equilateral triangle.

That is, sidelobes are formed in the direction θ 1 perpendicular to a line segment TR of the equilateral triangle, sidelobes are formed in the direction θ 2 perpendicular to a line segment RS of the equilateral triangle, and sidelobes are formed in the direction θ 3 perpendicular to a line segment ST of the equilateral triangle.

Looking at the primary radiator 1 labeled C 3 for example, primary radiators 1 having the same combination of frequency and polarization as that of a reflection beam of the primary radiator 1 labeled C 3 are the primary radiators 1 labeled C 1 and C 2 .

Thus, out of beams reflected by the main reflector 7 , reflection beams of the primary radiators 1 labeled C 1 and C 2 may be interfered by a reflection beam of the primary radiator 1 labeled C 3 .

However, in Third Embodiment, because the overall arrangement of the fifteen primary radiators 1 has the same equilateral triangle shape as that of the aperture shape 8 of the main reflector 7 , the reflection beams of the primary radiators 1 labeled C 1 and C 2 are not interfered by the reflection beam of the primary radiator 1 labeled C 3 .

That is, the primary radiator 1 labeled C 3 is arranged at a position corresponding to a vertex of the same equilateral triangle as that of the primary radiators 1 labeled C 1 and C 2 .

Directions of line segments passing through a base point of the position corresponding to the vertex of the equilateral triangle, in which the primary radiator 1 labeled C 3 is arranged, and the positions corresponding to the other vertexes of the equilateral triangle are given as a direction α 1 and a direction α 2 as illustrated in FIG. 15 .

Specifically, a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled C 3 and the arrangement position of the primary radiator 1 labeled C 1 is α 1 , and a direction of a line segment passing through the arrangement position of the primary radiator 1 labeled C 3 and the arrangement position of the primary radiator 1 labeled C 2 is α 2 .

Here, because the directions α 1 and α 2 of the line segments are different from the radiation directions θ 1 , θ 2 , and θ 3 of the sidelobes, the reflection beams of the primary radiators 1 labeled C 1 and C 2 are not interfered by the reflection beam of the primary radiator 1 labeled C 3 .

As is apparent from the above, according to Third Embodiment, the plurality of primary radiators 1 is classified by combinations of frequency and polarization of the radiated radio waves, a plurality of primary radiators belonging to the same class is arranged at positions corresponding to vertexes of one of triangles in a repeated triangle pattern TR Pattern , and the shape of the main reflector 7 and the shape and arrangement of the repeated triangle pattern TR Pattern are determined such that a direction of a line segment passing through positions corresponding to two vertexes in the triangle is different from a radiation direction of a sidelobe of a radio wave reflected by the main reflector 7 after having been radiated from a primary radiator 1 arranged at a position corresponding to the vertexes. Therefore, the effect of suppressing interference among all the beams having the same combination of frequency and polarization can be obtained.

Furthermore, according to Third Embodiment, the aperture shape 8 of the main reflector 7 is a equilateral triangle, and one or more triangular shapes are repeated such that the repeated triangle pattern TR Pattern has the same shape as that of the aperture shape 8 of the main reflector 7 , and thus a major part of radio waves radiated from the plurality of primary radiators 1 is reflected by the main reflector 7 , thereby enabling mitigation of radio waves not reflected by the main reflector 7 . Therefore, the utilization rate of radio waves is increased, and the gain of the antenna apparatus can be increased.

In Third Embodiment, the example has been illustrated in which interior angles of the triangle which is the aperture shape 8 of the main reflector 7 are 60 degrees; however, even in the case where the interior angles deviate from 60 degrees by about 20%, interference among all the beams having the same combination of frequency and polarization can be suppressed. That is, even in the case where the aperture shape 8 of the main reflector 7 is not a perfect equilateral triangle, interference among all the beams having the same combination of frequency and polarization can be suppressed.

In Third Embodiment, the example in which the three primary radiators 1 are arranged in a triangular shape has been illustrated; however depending on a required service area, one or two primary radiators 1 may be thinned out from those in a triangular shape TR P from among a plurality of triangular shapes TR P .

Furthermore, it is only required that an arrangement of the repeated triangle pattern TR Pattern is in conformity with the arrangement of FIG. 14 for example, and the shape of the repeated triangle pattern TR Pattern is not required to be a equilateral triangle as a result of thinning out some of the primary radiators 1 .

In Third Embodiment, the example in which there are four combinations of frequency and polarization has been illustrated; however, this is merely an example, and the number of combinations of frequency and polarization may be three or seven, for example.

In Third Embodiment, the aperture shape 8 of the main reflector 7 is an equilateral triangle; however, vertexes of the equilateral triangle are not required to be angular and may be, for example, rounded or chamfered.

Fourth Embodiment

In First to Third Embodiments, each of the primary radiators 1 radiates one beam to the main reflectors 2 , 5 , and 7 ; however, a plurality of radiating elements may radiate one beam to the main reflector 2 , 5 , or 7 .

FIG. 16 is a configuration diagram illustrating an antenna apparatus according to a fourth embodiment of the present disclosure. In FIG. 16 , the same reference numeral as that in FIG. 1 represents the same or a corresponding part and thus descriptions thereon are omitted.

Each of primary radiators 1 includes a plurality of radiating elements 9 .

In the antenna apparatus of FIG. 16 , for simplicity of explanation, an example in which three primary radiators are mounted is illustrated. However, in practice, a plurality of primary radiators 1 for radiating radio waves having the same combination of frequency and polarization is mounted, and a plurality of primary radiators 1 for radiating radio waves having different combinations of frequency and polarization is also mounted. Thus, also in the antenna apparatus of FIG. 16 , sixteen primary radiators 1 are mounted for example like the antenna apparatus of FIG. 1 according to First Embodiment.

However, the number of primary radiators 1 and the number of radiating elements included in each of the primary radiators 1 may be any number.

A beam forming circuit 10 is a feeding circuit for exciting a plurality of radiating elements 9 in the primary radiators 1 .

The beam forming circuit 10 excites four radiating elements 9 such that radio waves having the same combination of frequency and polarization are radiated from the four radiating elements 9 belonging to the same primary radiator 1 while exciting each group of four radiating elements 9 belonging to the three primary radiators 1 such that combinations of frequency and the polarization of radio waves radiated from the three primary radiators 1 are different.

In the beam forming circuit 10 , an excitation coefficient is designed for each of the radiating elements 9 , and in the case where the direction of beams radiated from the three primary radiators 1 are fixed, a signal capable of implementing the excitation coefficient is fed to the radiating element 9 .

In the case where the direction of beams radiated from the three primary radiators 1 is variable, the beam forming circuit 10 includes phase shifters for adjusting the phase of a signal output to each of the plurality of radiating elements 9 and a variable gain amplifier(s) for adjusting the amplitude of a signal output to the plurality of radiating elements 9 , to adjust excitation coefficients of the radiating elements 9 with the phase shifters and the variable gain amplifier(s).

As a result, the radiation direction of a beam reflected by the main reflector 2 , a range of a service area of the beam, and the like can be variable.

As is clear from the above, according to Fourth Embodiment, since the beam forming circuit 10 for exciting the plurality of radiating elements 9 is included, the effect of suppressing interference among all the beams having the same combination of frequency and polarization can be obtained like in First Embodiment described above as well as the effect of enhancing the degree of freedom of the radiation direction or other features of the beam.

In Fourth Embodiment, the plurality of radiating elements 9 and the beam forming circuit 10 are used for the antenna apparatus of First Embodiment in which the aperture shape 3 of the main reflector 2 is a parallelogram; however, the plurality of radiating elements and the beam forming circuit 10 may be used for the antenna apparatus in which the aperture shape 6 of the main reflector 5 is a regular hexagon as in Second Embodiment or the antenna apparatus in which the aperture shape 8 of the main reflector 7 is an equilateral triangle as in Third Embodiment.

Fifth Embodiment

In First to Fourth Embodiments, the plurality of primary radiators 1 radiate beams to the main reflectors 2 , 5 , and 7 ; however, the beams radiated from the plurality of primary radiators 1 may be radiated toward the main reflector 2 , 5 , or 7 via a secondary reflector.

FIG. 17 is a configuration diagram illustrating an antenna apparatus according to Fifth Embodiment of the present disclosure. In FIG. 17 , the same reference numeral as that in FIG. 1 represents the same or a corresponding part and thus descriptions thereon are omitted.

A secondary reflector 11 is a reflector which reflects radio waves radiated from a plurality of primary radiators 1 toward a main reflector 2 , and in the example of FIG. 17 , the secondary reflector 11 is a Cassegrain type reflector having a mirror surface of a hyperboloid of revolution.

Even in the case where the secondary reflector 11 reflects the beams radiated from the plurality of primary radiators 1 toward the main reflector 2 , interference among all the beams having the same combination of frequency and polarization can be suppressed like in First Embodiment described above.

Here, the secondary reflector 11 of a Cassegrain type having a mirror surface of a hyperboloid of revolution is described as an example; however, a secondary reflector 11 of a Gregorian type having a mirror surface of an ellipsoid of revolution may be used. Alternatively, a secondary reflector 11 having a flat mirror surface may be used.

Moreover, the secondary reflector 11 may include a plurality of reflectors.

In Fifth Embodiment, the secondary reflector 11 is used for the antenna apparatus of First Embodiment; however, the secondary reflector 11 may be used for the antenna apparatuses of Second to Fourth Embodiments described above.

Note that, within the scope of the present invention, Embodiments may be combined freely, modifications may be made to any component of Embodiments, or omission of any component in Embodiments may be made.

Antenna apparatuses disclosed in the present disclosure is suitable for antenna apparatuses with high gain and low interference.

1 : Primary radiator, 2 : Main reflector, 3 : Aperture shape of the main reflector, 4 : Radiation direction of beam, 5 : Main reflector, 6 : Aperture shape of main reflector, 7 : Main reflector, 8 : Aperture shape of main reflector, 9 : Radiating element, 10 : Beam forming circuit, 11 : Secondary reflector.