WO2016107130A1 - 一种交织极化的多波束天线 - Google Patents

一种交织极化的多波束天线 Download PDF

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Publication number
WO2016107130A1
WO2016107130A1 PCT/CN2015/083722 CN2015083722W WO2016107130A1 WO 2016107130 A1 WO2016107130 A1 WO 2016107130A1 CN 2015083722 W CN2015083722 W CN 2015083722W WO 2016107130 A1 WO2016107130 A1 WO 2016107130A1
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Prior art keywords
group
bridges
bridge
antenna
polarized
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PCT/CN2015/083722
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English (en)
French (fr)
Inventor
赵建平
耿阳
解清明
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华为技术有限公司
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Publication date
Application filed by 华为技术有限公司 filed Critical 华为技术有限公司
Priority to EP15874820.2A priority Critical patent/EP3232510B1/en
Priority to KR1020177021117A priority patent/KR101913294B1/ko
Priority to JP2017534972A priority patent/JP6530074B2/ja
Publication of WO2016107130A1 publication Critical patent/WO2016107130A1/zh
Priority to US15/636,183 priority patent/US10333220B2/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/26Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
    • H01Q3/30Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array
    • H01Q3/34Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by electrical means
    • H01Q3/40Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by electrical means with phasing matrix
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/24Combinations of antenna units polarised in different directions for transmitting or receiving circularly and elliptically polarised waves or waves linearly polarised in any direction
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/29Combinations of different interacting antenna units for giving a desired directional characteristic
    • H01Q21/293Combinations of different interacting antenna units for giving a desired directional characteristic one unit or more being an array of identical aerial elements
    • H01Q21/296Multiplicative arrays
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q25/00Antennas or antenna systems providing at least two radiating patterns
    • H01Q25/001Crossed polarisation dual antennas
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/24Combinations of antenna units polarised in different directions for transmitting or receiving circularly and elliptically polarised waves or waves linearly polarised in any direction
    • H01Q21/26Turnstile or like antennas comprising arrangements of three or more elongated elements disposed radially and symmetrically in a horizontal plane about a common centre

Definitions

  • the present invention relates to the field of communications technologies, and in particular, to an interleaved polarization multi-beam antenna.
  • Multi-beam network is the main technology to realize multi-beam antenna by spatial selectivity.
  • the space-selective method can bring two advantages: one is selective transmission and reception, which can reduce interference to neighbors and be Interference; second, spatial multiplexing is formed between multiple beams.
  • the multi-beam antenna system consists of two parts, one is a dual-polarized array of dual-polarized antenna elements, the other is a Butler matrix, and the dual-polarized array is connected to the Butler matrix.
  • the Butler matrix is a completely passive and reciprocal circuit that includes a number of directional couplers and phase shifting elements, and the Butler matrix is used to generate beams and to generate beams from the Butler matrix through a dual-polarized array.
  • the same beamforming network is used for the two polarization directions, so there are two polarizations in each beam direction (see Fig. 1), and the above multi-beam antenna system becomes simultaneous crossover.
  • a cross-polarized multi-beam antenna system has the effect of performing polarization diversity or multiplexing inside the beam and multiplexing between the beams.
  • Figure 1 is a multi-beam formed by four columns of dual-polarized antennas. Each polarization uses the amplitude and phase of Table 1, both of which point in the same direction.
  • Beam 3 1 ⁇ -270 1 ⁇ -135 1 ⁇ 0 1 ⁇ 135 Beam 4 1 ⁇ 0 1 ⁇ -45 1 ⁇ -90 1 ⁇ -135
  • the cross-polarized multi-beam system belongs to an orthogonal system, that is, the maximum direction of each beam of each polarization is basically the zero or side lob of other beams of the same polarization, and the main problem of the cross-polarized multi-beam system Therefore:
  • the number of multi-beams generally formed in such a system is increased due to the number of multi-beam matrix stages.
  • a three-level network is required, and the increase of the network level will greatly increase the processing difficulty and the network. Loss;
  • the side lobes are not easy to reduce, the Butler class matrix generally has the highest side beam side lobe level, thus increasing the interference between adjacent multiplex beams.
  • An embodiment of the present invention provides an interleaved polarization multi-beam antenna
  • a first aspect of the embodiments of the present invention provides an interleaved polarization multi-beam antenna, including:
  • At least one dual-polarized antenna element comprising a first antenna element polarized at +45 degrees and a second antenna element polarized at -45 degrees;
  • first Butler matrix and a second Butler matrix
  • the first Butler matrix is coupled to the first antenna element such that the first antenna element transmits a first target beam, the first target beam Generating by the first Butler matrix according to the first input signal received by the at least one first beam port, and the orientation of each of the first target beams is different
  • the second Butler matrix and the second antenna The vibrator is connected such that the second antenna element transmits a second target beam, and the second target beam is generated by the second Butler matrix according to the second input signal received by the at least one second beam port, and each The direction of the second target beam is different, wherein one of the second target beams is disposed between any two adjacent first target beams.
  • the interleaved polarized multi-beam antenna includes six of the dual-polarized antenna elements, and the first target beam is received by the first Butler matrix according to the first input of the three first beam ports And generating, by the signal, the second target beam is generated by the second Butler matrix according to the second input signal received by the two second beam ports.
  • the first Butler matrix includes:
  • first set of bridges a first set of bridges, a second set of bridges, and a first set of splitters
  • the first group of bridges generates a total of four signal outputs according to the first input signals of the three channels
  • the second group of bridges is connected with the first group of bridges to receive the output of the first group of bridges.
  • a second signal group wherein the second group of bridges generates a total of four signal outputs according to the four signals output by the first group of bridges, and the second group of bridges generates two signals generated by the second group of bridges. Outputting to the first group of power splitters connected to the second group of bridges, the second group of bridges outputting the other two signals generated by the second group of bridges to two of the bipolar
  • the first antenna element of the antenna element
  • the first group of power splitters is configured to split the two signals input from the second group of bridges into two, and output the formed four signals to the first antenna elements of the four dual-polarized antenna elements. So that six of the first antenna elements emit the first target beam.
  • the first group of bridges includes a first bridge and a second bridge, and the first bridge is a 3 dB 90 degree bridge, and the second bridge is a 3 dB 180 degree bridge;
  • the second group of bridges includes a third bridge and a fourth bridge, and the third bridge and the fourth bridge are both 3 dB 180 degree bridges;
  • the first set of power splitters includes a first power splitter and a second power splitter, and an output power ratio of the first power splitter and the second power splitter is 3:7.
  • the second Butler matrix includes:
  • the port is connected to receive two channels of the second input signal, and the third group of bridges generates a total of four signals for output according to the second input signal of the two channels,
  • the third group of bridges outputs two signals generated by the third group of bridges to the first group of phase shifters connected to the third group of bridges, and the third group of bridges
  • the other two signals generated by the three sets of bridges are output to the fourth group of bridges connected to the third group of bridges;
  • the fourth group of bridges is connected to the first group of phase shifters, and the fourth group of bridges receives two signals that are output after phase shifting by the first group of phase shifters and the third group Two signals outputted by the bridge to generate four signal outputs, and the fourth group of bridges outputs two signals outputted by the fourth group of bridges to the second antenna elements of the two dual-polarized antenna elements
  • the fourth group of bridges outputs the other two signals output by the fourth group of bridges to the second group of power splitters connected to the fourth group of bridges;
  • the second group of power splitters is configured to divide a 2-way signal input from the fourth group of bridges into two to form a 4-way signal output, and the second group of power splitters divides the second group of power points
  • the two signals output by the device are output to a second group of phase shifters connected to the second group of power splitters, and the second group of phase shifters outputs the two signals after phase shifting to two of the two poles a second antenna element of the antenna element, the second group of power dividers outputting the other two signals output by the second group of power dividers to the second antenna elements of the two dual-polarized antenna elements, And causing 6 of the second antenna elements to emit the second target beam.
  • the third group of bridges includes a fifth bridge and a sixth bridge, and the fifth bridge and the sixth bridge are both 3 dB 90 degree bridges;
  • the fourth group of bridges includes a seventh bridge and an eighth bridge, and the seventh bridge and the eighth bridge are both 3 dB 90 degree bridges;
  • the first group of phase shifters includes a first phase shifter and a second phase shifter, and the phase shifting of the first phase shifter and the second phase shifter are both -45 degrees;
  • the second group of power splitters includes a third power splitter and a fourth power splitter, and the output power ratio of the third power splitter and the fourth power splitter is 3:7;
  • the second group of phase shifters includes a third phase shifter and a fourth phase shifter, and the phase shifting of the third phase shifter and the fourth phase shifter are both -180 degrees.
  • the embodiment of the invention discloses an interleaved polarized multi-beam antenna, comprising: at least one dual-polarized antenna element, the dual-polarized antenna element comprising a first antenna element polarized at +45 degrees and at -45 degrees Extreme a second antenna element; a first Butler matrix and a second Butler matrix, wherein the first Butler matrix is coupled to the first antenna element to generate a first target beam, the second Butler matrix Connected to the second antenna element to generate a second target beam.
  • the polarization characteristics of any two adjacent first target beams and second target beams are different, and each of the first The different directions of a target beam and the different directions of the second target beams can effectively reduce the complexity, loss and cost of the implementation of the Butler matrix, and effectively reduce the interference between adjacent multiplex beams and reduce the interference. Network loss.
  • FIG. 1 is a schematic diagram of a 4-beam formed by a 4-column dual-polarized antenna in the prior art
  • FIG. 2 is a schematic structural diagram of a preferred embodiment of an interleaved polarization multi-beam antenna according to an embodiment of the present invention
  • FIG. 3 is a schematic structural diagram of a preferred embodiment of a first Butler matrix of an interleaved polarized multi-beam antenna according to an embodiment of the present invention
  • FIG. 4 is a schematic structural diagram of a bridge structure of a 3 dB 90-degree bridge according to an embodiment of the present invention
  • FIG. 5 is a schematic structural diagram of a bridge structure of a 3 dB 180-degree bridge according to an embodiment of the present invention.
  • FIG. 6 is a schematic structural diagram of a second preferred embodiment of a second Butler matrix of an interleaved polarized multi-beam antenna according to an embodiment of the present invention
  • FIG. 7 is a schematic diagram of a 5-beam formed by an interleaved polarization multi-beam antenna according to an embodiment of the present invention.
  • the embodiment of the present invention provides an interleaved and polarized multi-beam antenna, which can effectively improve the difficulty of the feed network of the cross-polarized multi-beam system shown in the prior art, and insert Technical problems of large loss, poor sidelobe quality, and large inter-beam interference.
  • the interleaved polarized multi-beam antenna includes:
  • An antenna array 201 comprising at least one dual-polarized antenna oscillator
  • the dual-polarized antenna oscillator includes a first antenna element 2011 polarized at +45 degrees and a second antenna element 2012 polarized at -45 degrees;
  • the first antenna element 2011 and the second antenna element 2012 shown in this embodiment are orthogonally arranged at ⁇ 45 degrees, and are used to form mutually orthogonal linearly polarized electromagnetic waves in space, and each column is bilinearly polarized.
  • the antenna elements of the antenna are arranged linearly, that is, as shown in FIG. 2, and the specific structure and implementation principle of the dual-polarized antenna oscillator are described in the prior art, and are not described in this embodiment.
  • the number of the dual-polarized antenna elements included in the antenna array 201 shown in this embodiment is n, where n is a positive integer, that is, the specific number of the dual-polarized antenna elements is not limited in this embodiment. .
  • the first antenna element 202 is connected to the first antenna element 2011, so that the first antenna element 2011 emits a first target beam;
  • the first target beam is generated by the first input signal received by the first Butler matrix 202 according to the at least one first beam port to be connected by the first butler matrix 202
  • the first antenna element 2011 transmits the first target beam
  • the second target beam is generated by the second Butler matrix 203 according to a second input signal received by the at least one second beam port to pass the connection with the second Butler matrix 203.
  • the second antenna element 2012 transmits the second target beam.
  • one of the second target beams is disposed between any two adjacent first target beams, that is, the poles of any two adjacent first target beams and second target beams Different characteristics.
  • first Butler matrix 202 and the second Butler matrix 203 are not limited in this embodiment, as long as the first Butler matrix 202 generates the first A target beam and the second Butler matrix 203 may generate the second target beam.
  • the first Butler matrix 202 is only connected to the first antenna element 2011 polarized at +45 degrees, so that each of the first target beams generated by the first Butler matrix 202 is made.
  • the second Butler matrix 203 is connected to the second antenna element 2012 which is polarized at -45 degrees, so that the second Butler matrix 203 is generated.
  • Each beam direction of the beam has only a unique negative polarization characteristic, and each of the first target beam and each of the second target beams are alternately arranged, that is, polarization characteristics of any two adjacent beams are different, and each The directions of the beams are different.
  • the interleaved polarized multi-beam antenna shown in this embodiment can effectively reduce the complexity of the implementation of the Butler matrix, because the first target beam and the second target beam are alternately arranged in this embodiment. Degree, loss, and cost, while effectively reducing interference between adjacent multiplex beams.
  • the specific number of the first target beam and the second target beam is not limited, as long as the polarization characteristics of any two adjacent beams are different, and the directions of the beams are different.
  • the specific arrangement manner of the first Butler matrix 202 and the second Butler matrix 203 is not limited, as long as the first Butler matrix 202 and the second Butler matrix 203 are both
  • the antenna array 201 can be connected, because the beam covering the target area is generated by two of the Butler matrices at the same time, thereby reducing the network level of a Butler matrix, thereby greatly reducing the processing difficulty and reducing the network loss. .
  • the first Butler matrix 202 and the second Butler matrix 203 shown in this embodiment may be arranged side by side or may be arranged up and down.
  • the first Butler matrix 202 and The second Butler matrix 203 is exemplified by the upper and lower settings, which has the beneficial effect that the occupied area of the antenna can be saved by the two Butler matrices disposed above and below, thereby facilitating assembly and maintenance.
  • the specific structure of the first Butler matrix 202 is described in detail below with reference to FIG. 3;
  • the first Butler matrix 202 structure shown in FIG. 3 is only a preferred example, and is not a limitation on the specific structure of the first Butler matrix 202, as long as the first Butler matrix 202 is It is sufficient to generate the first target beam that satisfies the above conditions.
  • the inter-polarized multi-beam antenna shown in FIG. 3 is described by taking the number of the dual-polarized antenna vibrators as six. It should be clarified that the dual-polarized antenna vibrator in this embodiment is used. The number is described as an example and is not limited.
  • the six dual-polarized antenna elements include a first antenna element (M1, M2, M3, M4, M5, and M6) polarized at +45 degrees and a second antenna element polarized at -45 degrees.
  • M1, M2, M3, M4, M5, and M6 polarized at +45 degrees
  • N1, N2 N3, N4, N5, and N6 polarized at -45 degrees
  • the first antenna element M1 and the second antenna element N1 are arranged orthogonally by ⁇ 45 degrees
  • the first antenna element M6 and the second antenna element N6 are orthogonal to ⁇ 45 degrees.
  • One end of the first group of bridges 31 is connected to the first beam port
  • the first group of bridges 31 are connected to the three first beam ports to receive three channels of the first input signal, and the first group of bridges 31 are jointly generated according to the three channels of the first input signals. 4 signal output;
  • the second group of bridges 32 are connected to the first group of bridges 31 to receive four signals output by the first group of bridges 31, and the second group of bridges 32 are according to the first group of bridges.
  • the four output signals of 31 outputs a total of four signal outputs
  • the second group of bridges 32 outputs the two signals generated by the second group of bridges 32 to the connection with the second group of bridges 32.
  • a first set of power splitters 33 the second set of bridges 32 outputting the other two signals generated by the second set of bridges 32 to the first antenna elements of the two dual-polarized antenna elements (M4 and M3);
  • the first group of power dividers 33 is configured to divide the two signals input from the second group of bridges 32 into two, and output the formed four signals to the four of the dual-polarized antenna elements.
  • An antenna element (M2, M6, M1, and M5) is configured to cause the six first antenna elements (M1, M2, M3, M4, M5, and M6) to emit the first target beam.
  • the first beam port for receiving the first input signal shown in FIG. 3 is three (ie, A1, A2, and A3);
  • the first group of bridges 31 of the first Butler matrix specifically includes a first bridge 311 and a second bridge 312, and the first bridge 311 is a 3 dB 90 degree bridge, the The second bridge 312 is a 3 dB 180 degree bridge; the second set of bridges 32 includes a third bridge 321 and a fourth bridge 322, and the third bridge 321 and the fourth bridge 322 Both are 3 decibel 180 degree bridges;
  • the 3-dB 90-degree bridge consists of a four-port power hybrid network.
  • the two outputs 401 and 402 have a phase difference of 90 degrees out of the output signal, and the phase difference between the through-end and the coupled-end is -90°.
  • the phases of the through terminal (401) and the coupling end (402) are -180° and -90°, respectively, and the power ratio of the two ports is 1:1.
  • the phases of the through terminal (402) and the coupling terminal (401) are -90° and -180°, respectively, and the power ratio of the two ports is 1:1.
  • the ⁇ and ⁇ of the 3 dB 180-degree bridge represent the port and the differential port of the 180-degree bridge, respectively.
  • the phase between the through terminal and the coupled terminal is generally -90°
  • the phase shift difference between the two outputs is 0°
  • the difference port ( ⁇ ) is input, the phase of the through terminal and the coupling end are -270°, -90°, respectively, and the phase shift difference between the two outputs is -180°, and the power ratio of the output terminal 501 to the output terminal 502 is It is 1:1.
  • the first bridge 31 which is a 3 dB 90 degree bridge, receives a first input signal from the first beam port A1 and the first beam port A2, and is a 3 dB 180 degree bridge.
  • the sum port of the second bridge 312 is a first beam port A3 for receiving a first input signal, and a difference port of the second bridge 312 is grounded;
  • An output port 3111 of the first bridge 311 and a difference port of the third bridge 321 of the second group of bridges 321 are connected, and an output end 3112 of the first bridge 311 and the second group of electricity a differential port connection of the fourth bridge 322 of the bridge 32;
  • the output end 3121 of the second bridge 312 is connected to the sum port of the third bridge 321 of the second set of bridges 32, and the output end 3122 of the second bridge 312 is connected to the second set of electricity.
  • the fourth bridge 322 in the bridge 32 is connected to the port.
  • the output end 3211 of the third bridge 321 is connected to the first power splitter 331 of the first group of power splitters 33, and the output end 3212 of the third bridge 321 is connected to the first antenna element M4;
  • the output end 3221 of the fourth bridge 322 is connected to the first antenna element M3, and the output end 3222 of the fourth bridge 322 is connected to the second power splitter 332 of the first group of power splitters 33;
  • the output power ratio of the first power splitter 331 and the second power splitter 332 is 3:7.
  • the output power division ratio of the power splitter is described as an example and is not limited.
  • the first power divider 331 is configured to divide the signal input by the third bridge 321 into two, and the output signal has a power division ratio of 3:7, and output the two signals to the first.
  • the second power splitter 332 is configured to divide the signal input by the fourth bridge 322 into two, and the power split ratio of the output signal is 3:7, and output the two signals to the first Antennas M5 and M1 such that the first antenna elements M1, M2, M3, M4, M5, and M6 emit the first target beam;
  • each polarized beam of the first Butler matrix is as shown in Table 2:
  • the second Butler matrix specifically includes:
  • the third group of bridges 61 are connected to the two second beam ports to receive two channels of the second input signal, and the second beam port is connected to each of the second antenna elements;
  • the third group of bridges 61 generates a total of four signal outputs according to the two second input signals, and the third group of bridges outputs the two signals generated by the third group of bridges to the first
  • the first group of phase shifters 62 connected by the three sets of bridges, the third set of bridges 61 outputting the other two signals generated by the third group of bridges 61 to the third set of bridges 61 Connected fourth set of bridges 63;
  • the fourth group of bridges 63 is connected to the first group of phase shifters 62, and the fourth group of bridges 63 receives two signals and outputs that are output after phase shifting by the first group of phase shifters 62.
  • the two signals outputted by the third group of bridges 61 are output to generate four signals, and the fourth group of bridges 63 outputs the two signals output by the fourth group of bridges 63 to the two of the dual polarizations.
  • a second antenna element (N4 and N3) of the antenna element the fourth group of bridges 63 outputting the other two signals output by the fourth group of bridges 63 to the fourth group of bridges 63
  • the second group of power splitters 64 is configured to split the two signals input from the fourth group of bridges 63 into two signals to form a total of four signals, and the second group of power splitters 64 will The two signals output by the two sets of power splitters 64 are output to a second set of phase shifters connected to the second set of power splitters 64;
  • the second group of phase shifters outputs the phase-shifted two signals to the second antenna elements (N1 and N6) of the two dual-polarized antenna elements, and the second group of power splitters 64
  • the other two signals output by the second group of power splitters 64 are output to the second antenna elements (N2 and N5) of the two dual-polarized antenna elements, so that the six of the second antenna elements are emitted.
  • the second beam port for receiving the second input signal shown in FIG. 6 is two (ie, B1 and B2);
  • the third set of bridges 61 of the second Butler matrix includes a fifth bridge 611 and a sixth bridge 612, and the fifth bridge 611 and the sixth bridge 612 are both 3 dB 90 degree bridge;
  • the fourth group of bridges 63 includes a seventh bridge 631 and an eighth bridge 632, and the seventh bridge 631 and the eighth bridge 632 are both 3 dB 90 degree bridges;
  • the input end B1 of the fifth bridge 611 is the second beam port, that is, the fifth bridge 611 receives the second input signal through the second beam port B1, the fifth bridge The other input of 611 is grounded;
  • the input end B2 of the sixth bridge 612 is the second beam port, that is, the sixth bridge 612 receives the second input signal through the second beam port B2, and the sixth bridge 612 is another One input is grounded;
  • the output end 6111 of the fifth bridge 611 is connected to the first phase shifter 621 of the first group of phase shifters 62, that is, the first phase shifter 621 receives the output end of the fifth bridge 611. 6111 input signal and phase shifting;
  • phase shifting of the first phase shifter 621 is -45 degrees.
  • phase shifting of the first phase shifter 621 in the embodiment is -45 degrees as an example and is not limited.
  • An output end 6112 of the fifth bridge 611 is connected to an input end 6321 of the eighth bridge 632 of the fourth group of bridges 63;
  • An output end 6121 of the sixth bridge 612 is connected to an input end 6311 of the seventh bridge 631 of the fourth group of bridges 63;
  • the output end 6122 of the sixth bridge 612 is connected to the second phase shifter 622 of the first group of phase shifters 62, that is, the second phase shifter 622 receives the output end of the sixth bridge 612. 6122 input signal and phase shifting;
  • phase shifting of the second phase shifter 622 is -45 degrees.
  • phase shifting of the second phase shifter 622 in this embodiment is -45 degrees as an example and is not limited.
  • the output of the first phase shifter 621 is connected to the input end 6312 of the seventh bridge 631;
  • the output of the second phase shifter 622 is connected to the input end 6322 of the eighth bridge 632;
  • the output end 6313 of the seventh bridge 631 is connected to the input end of the third power splitter 641 of the second group of power splitters 64, and the output end 6314 of the seventh bridge 631 and the second antenna vibrator N4 connection;
  • An output end 6323 of the eighth bridge 632 is connected to the second antenna element N3, an output end 6324 of the eighth bridge 632 and a fourth power divider 642 of the second set of power dividers 64.
  • the third power splitter 641 is configured to divide the signal input by the output end 6313 of the seventh bridge 631 received through the input end thereof into two, one output second antenna element N2, and the other output to the center
  • the fourth power splitter 642 is configured to split the signal input by the output end 6324 of the eighth bridge 632 received through the input end thereof into two, one output second antenna vibrator N5, and the other output to the The fourth phase shifter 652 of the second group of phase shifters;
  • the output power ratio of the third power splitter 641 and the fourth power splitter 642 in the second set of power splitters 64 is 3:7;
  • phase shifting of the third phase shifter 651 and the fourth phase shifter 652 in the second group of phase shifters are both -180 degrees.
  • the fourth phase shifter 652 outputs the phase-shifted signal to the second antenna element N1, and the third phase shifter 651 outputs the phase-shifted signal to the second antenna element N6, so that The second antenna elements N1, N2, N3, N4, N5, and N6 emit the second target beam;
  • each polarized beam of the second Butler matrix is as shown in Table 3:
  • N1 N2 N3 N4 N5 N6 B1 0.54 ⁇ 0 0.84 ⁇ -45 1 ⁇ -90 1 ⁇ -135 0.84 ⁇ -180 0.54 ⁇ -225 B2 0.54 ⁇ -225 0.84 ⁇ -180 1 ⁇ -135 1 ⁇ -90 0.84 ⁇ -45 0.54 ⁇ 0
  • the beam emitted by the antenna array is as shown in FIG. 7, and the interleaved polarized multi-beam antenna shown in this embodiment is used.
  • the utility model can effectively reduce the complexity, loss and cost of the implementation of the Butler matrix and reduce the interference between adjacent multiplexed beams.
  • the multi-beam antenna with the interleaved polarization formed by the five beams is taken as an example, which is not limited, that is, the number of beams that can be formed by the multi-beam antenna of the interleaved polarization is not limited in this embodiment, as long as the first The target beam and the second target beam are spaced apart, and the orientation and polarization of any two adjacent beams are different.
  • the disclosed systems, devices, and methods may be implemented in other ways.
  • the device embodiments described above are merely illustrative.
  • the division of the unit is only a logical function division.
  • there may be another division manner for example, multiple units or components may be combined or Can be integrated into another system, or some features can be ignored or not executed.
  • the mutual coupling or direct coupling or communication connection shown or discussed may be an indirect coupling or communication connection through some interface, device or unit, and may be in an electrical, mechanical or other form.

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Abstract

本发明实施例公开了一种交织极化的多波束天线,包括:至少一个双极化天线振子,所述双极化天线振子包括呈+45度极化的第一天线振子和呈-45度极化的第二天线振子;第一巴特勒矩阵以及第二巴特勒矩阵,所述第一巴特勒矩阵与所述第一天线振子连接,以使所述第一天线振子发射第一目标波束;所述第二巴特勒矩阵与所述第二天线振子连接,以使所述第二天线振子发射第二目标波束。因本实施例中的所述第一目标波束和所述第二目标波束之间呈交错设置,任意相邻的两个第一目标波束和第二目标波束的极化特性不同,则能够有效的减少巴特勒矩阵实现的复杂度,损耗以及成本,同时有效的减少相邻复用波束之间的干扰。

Description

一种交织极化的多波束天线
本申请要求于2014年12月30日提交中国专利局、申请号为201410857222.5、发明名称为“一种交织极化的多波束天线”的中国专利申请的优先权,其全部内容通过引用结合在本申请中。
技术领域
本发明涉及通信技术领域,尤其涉及的是一种交织极化的多波束天线。
背景技术
随着移动通信系统的不断升级,对天线提出新的指标要求,如多波束、小型化等成为现代天线设计的主要因素。多波束网络是利用空间选择性实现多波束天线的主要技术,利用空间选择性的方法可以带来两个方面的好处:一是进行选择性发射和接收,这样可以降低对于邻区的干扰和被干扰;二是多波束之间形成空间复用。
多波束天线系统有两部分组成,一部分是由双极化天线单元构成的双极化阵列,另外一部分是巴特勒(Butler)矩阵,且该双极化阵列连接到巴特勒矩阵。巴特勒矩阵是一个完全无源的和互易的电路,该电路包括若干定向耦合器以及相移元件,且该巴特勒矩阵用于产生波束,并通过双极化阵列将巴特勒矩阵产生的波束发射出去。目前多波束天线系统应用中,对于两个极化方向采用相同的波束形成网络,因此在每个波束方向上都是有两个极化存在(见图1),上述多波束天线系统成为同时交叉极化的多波束天线系统,这样的交叉极化多波束天线系统效果是在波束内部进行极化分集或者复用,而在波束之间实现复用。
图1是一个由4列双极化天线形成的多波束,每个极化都采用表1的幅度和相位,两个极化都指向同样的方向。
表1
  列1 列2 列3 列4
波束1 1∠-225 1∠-180 1∠-135 1∠-90
波束2 1∠45 1∠-90 1∠-225 1∠0
波束3 1∠-270 1∠-135 1∠0 1∠135
波束4 1∠0 1∠-45 1∠-90 1∠-135
同时交叉极化的多波束系统属于一种正交系统,即每个极化的每个波束最大值方向基本是同极化其它波束的零点或旁瓣,同时交叉极化的多波束系统主要问题在于:第一、这种系统一般形成的多部束数目较多时候由于多部束矩阵级数增加,比如要形成6波束需要采用三级网络,网络级数增加将大幅度增加加工难度和网络损耗;第二、旁瓣不容易降低,Butler类矩阵一般最边两个波束旁瓣电平较高,因而增加了相邻复用波束之间的干扰。
发明内容
本发明实施例提供了一种交织极化的多波束天线;
本发明实施例第一方面提供了一种交织极化的多波束天线,包括:
至少一个双极化天线振子,所述双极化天线振子包括呈+45度极化的第一天线振子和呈-45度极化的第二天线振子;
第一巴特勒矩阵以及第二巴特勒矩阵,其中,所述第一巴特勒矩阵与所述第一天线振子连接,以使所述第一天线振子发射第一目标波束,所述第一目标波束由所述第一巴特勒矩阵根据至少一个第一波束端口接收的第一输入信号所产生的,且各所述第一目标波束的指向不同;所述第二巴特勒矩阵与所述第二天线振子连接,以使所述第二天线振子发射第二目标波束,所述第二目标波束由所述第二巴特勒矩阵根据至少一个第二波束端口接收的第二输入信号所产生的,且各所述第二目标波束的指向不同,其中,任意相邻的两个所述第一目标波束之间设置有一个所述第二目标波束。
结合本发明实施例第一方面,本发明实施例第一方面的第一种实现方式中,
所述交织极化的多波束天线包括6个所述双极化天线振子,所述第一目标波束由所述第一巴特勒矩阵根据3个所述第一波束端口接收的所述第一输入信号所产生的,所述第二目标波束由所述第二巴特勒矩阵根据2个所述第二波束端口接收的所述第二输入信号所产生的。
结合本发明实施例第一方面的第一种实现方式,本发明实施例第一方面的第二种实现方式中,
所述第一巴特勒矩阵包括:
第一组电桥,第二组电桥和第一组功分器,其中,所述第一组电桥与3个所述第一波束端口相连以接收3路所述第一输入信号,所述第一组电桥根据3路所述第一输入信号共生成4路信号输出,所述第二组电桥与所述第一组电桥连接以接收所述第一组电桥输出的4路信号,所述第二组电桥根据所述第一组电桥输出的4路信号共生成4路信号输出,所述第二组电桥将所述第二组电桥生成的2路信号输出至与所述第二组电桥连接的所述第一组功分器,所述第二组电桥将所述第二组电桥生成的另2路信号输出至2个所述双极化天线振子的第一天线振子;
所述第一组功分器用于将从所述第二组电桥输入的2路信号一分为二,将形成的4路信号输出至4个所述双极化天线振子的第一天线振子,以使6个所述第一天线振子发射出所述第一目标波束。
结合本发明实施例第一方面的第二种实现方式,本发明实施例第一方面的第三种实现方式中,
所述第一组电桥包括第一电桥和第二电桥,且所述第一电桥为3分贝的90度电桥,所述第二电桥为3分贝的180度电桥;
所述第二组电桥包括第三电桥和第四电桥,且所述第三电桥和所述第四电桥均为3分贝的180度电桥;
所述第一组功分器包括第一功分器和第二功分器,且所述第一功分器和所述第二功分器的输出功分比为3:7。
结合本发明实施例第一方面的第一种实现方式,本发明实施例第一方面的第四种实现方式中,
所述第二巴特勒矩阵包括:
第三组电桥、第四组电桥、第一组移相器、第二组功分器以及第二组移相器,其中,所述第三组电桥与2个所述第二波束端口相连以接收2路所述第二输入信号,所述第三组电桥根据2路所述第二输入信号共生成4路信号输出,所述 第三组电桥将所述第三组电桥生成的2路信号输出至与所述第三组电桥连接的所述第一组移相器,所述第三组电桥将所述第三组电桥生成的另2路信号输出至与所述第三组电桥连接的第四组电桥;
所述第四组电桥与所述第一组移相器连接,且所述第四组电桥接收经所述第一组移相器移相后输出的2路信号以及所述第三组电桥输出的2路信号以生成4路信号输出,所述第四组电桥将所述第四组电桥输出的2路信号输出至2个所述双极化天线振子的第二天线振子,所述第四组电桥将所述第四组电桥输出的另2路信号输出至与所述第四组电桥连接的第二组功分器;
所述第二组功分器用于将从所述第四组电桥输入的2路信号一分为二共形成4路信号输出,所述第二组功分器将所述第二组功分器输出的2路信号输出至与所述第二组功分器连接的第二组移相器,所述第二组移相器将移相后的两路信号输出至2个所述双极化天线振子的第二天线振子,所述第二组功分器将所述第二组功分器输出的另2路信号输出至2个所述双极化天线振子的第二天线振子,以使6个所述第二天线振子发射出所述第二目标波束。
结合本发明实施例第一方面的第四种实现方式,本发明实施例第一方面的第五种实现方式中,
所述第三组电桥包括第五电桥和第六电桥,且所述第五电桥和所述第六电桥均为3分贝的90度电桥;
所述第四组电桥包括第七电桥和第八电桥,且所述第七电桥和所述第八电桥均为3分贝的90度电桥;
所述第一组移相器包括第一移相器和第二移相器,且所述第一移相器和所述第二移相器的移相均为-45度;
所述第二组功分器包括第三功分器和第四功分器,且所述第三功分器和所述第四功分器的输出功分比为3:7;
所述第二组移相器包括第三移相器和第四移相器,且所述第三移相器和所述第四移相器的移相均为-180度。
本发明实施例公开了一种交织极化的多波束天线,包括:至少一个双极化天线振子,所述双极化天线振子包括呈+45度极化的第一天线振子和呈-45度极 化的第二天线振子;第一巴特勒矩阵以及第二巴特勒矩阵,其中,所述第一巴特勒矩阵与所述第一天线振子连接以生成第一目标波束,所述第二巴特勒矩阵与所述第二天线振子连接,以生成第二目标波束。因本实施例中的所述第一目标波束和所述第二目标波束之间呈交错设置,任意相邻的两个第一目标波束和第二目标波束的极化特性不同,各所述第一目标波束的指向不同以及各所述第二目标波束的指向不同,则能够有效的减少巴特勒矩阵实现的复杂度,损耗以及成本,同时有效的减少相邻复用波束之间的干扰以及降低了网络损耗。
附图说明
图1为现有技术由4列双极化天线形成的4波束示意图;
图2为本发明实施例所提供的交织极化的多波束天线的一种较佳实施例结构示意图;
图3为本发明实施例所提供的交织极化的多波束天线的第一巴特勒矩阵的一种较佳实施例结构示意图;
图4为本发明实施例所提供的3分贝的90度电桥的电桥原理结构示意图;
图5为本发明实施例所提供的3分贝的180度电桥的电桥原理结构示意图;
图6为本发明实施例所提供的交织极化的多波束天线的第二巴特勒矩阵的一种较佳实施例结构示意图;
图7为本发明实施例所提供的交织极化的多波束天线所形成的一种5波束示意图。
具体实施方式
本发明实施例提供了一种交织极化的多波束天线,该交织极化的多波束天线能够有效的改善现有技术中所示的交叉极化的多波束系统的馈电网络实现难度、插损大、副瓣质量差以及相邻波束间干扰大的技术问题。
以下结合图2所示对本实施例所示的交织极化的多波束天线的具体结构进行详细说明:
所述交织极化的多波束天线包括:
天线阵列201,该天线阵列201包括至少一个双极化天线振子;
其中,所述双极化天线振子包括呈+45度极化的第一天线振子2011和呈-45度极化的第二天线振子2012;
本实施例所示的第一天线振子2011和所述第二天线振子2012成±45度正交布置,其用于在空间形成相互正交的线极化电磁波,且每一列双线性极化天线的天线振子呈线性排列,即如图2所示,且所述双极化天线振子的具体结构和实现原理请见现有技术,在本实施例中不做赘述。
本实施例所示的天线阵列201所包括的所述双极化天线振子的个数为n,其中,n为正整数,即本实施例对所述双极化天线振子的具体个数不作限定。
第一巴特勒矩阵202以及第二巴特勒矩阵203;
其中,所述第一巴特勒矩阵202与所述第一天线振子2011连接,以使所述第一天线振子2011发射第一目标波束;
具体的,所述第一目标波束由所述第一巴特勒矩阵202根据至少一个第一波束端口接收的第一输入信号所产生的,以通过与所述第一巴特勒矩阵202连接的所述第一天线振子2011发射所述第一目标波束;
具体的,所述第二目标波束由所述第二巴特勒矩阵203根据至少一个第二波束端口接收的第二输入信号所产生的,以通过与所述第二巴特勒矩阵203连接的所述第二天线振子2012发射所述第二目标波束。
更具体的,任意相邻的两个所述第一目标波束之间设置有一个所述第二目标波束,即任意相邻的两个所述第一目标波束和所述第二目标波束的极化特性不同。
需明确的是,本实施例对所述第一巴特勒矩阵202和所述第二巴特勒矩阵203具体所包含的器件以及具体结构不作限定,只要所述第一巴特勒矩阵202产生所述第一目标波束以及所述第二巴特勒矩阵203产生所述第二目标波束即可。
因本实施例中,所述第一巴特勒矩阵202只与呈+45度极化的第一天线振子2011连接,则使得所述第一巴特勒矩阵202所产生的第一目标波束的每个波束方向上只有唯一的正极化特性,又因所述第二巴特勒矩阵203只与呈-45度极化的第二天线振子2012连接,则使得所述第二巴特勒矩阵203所产生的第二目标 波束的每个波束方向上只有唯一的负极化特性,而且各所述第一目标波束和各所述第二目标波束呈交错设置,即任意相邻的两个波束的极化特性不同,且各波束的指向不同。
因本实施例中的所述第一目标波束和所述第二目标波束之间呈交错设置,则使得本实施例所示的交织极化的多波束天线能够有效的减少巴特勒矩阵实现的复杂度,损耗以及成本,同时有效的减少相邻复用波束之间的干扰。
本实施例对所述第一目标波束和所述第二目标波束的具体个数不作限定,只要任意相邻的两个波束的极化特性不同,以及各波束的指向不同即可。
本实施例中,对所述第一巴特勒矩阵202以及所述第二巴特勒矩阵203的具体设置方式不作限定,只要所述第一巴特勒矩阵202以及所述第二巴特勒矩阵203均与所述天线阵列201连接即可,因同时通过两个所述巴特勒矩阵产生覆盖目标区域的波束,则减少了一个巴特勒矩阵的网络级数,则大大减少了加工的难度以及降低了网络损耗。
本实施例所示的所述第一巴特勒矩阵202以及所述第二巴特勒矩阵203可并列设置或可上下对应设置,较佳的,本实施例中,所述第一巴特勒矩阵202以及所述第二巴特勒矩阵203以呈上下设置为例,其带来的有益效果为因通过呈上下设置的两个巴特勒矩阵能够节省天线的占用面积,从而便于装配和维护。
以下结合图3所示对所述第一巴特勒矩阵202的具体结构进行详细说明;
需明确的是,图3所示的第一巴特勒矩阵202结构仅仅为一种较佳的示例,不是对所述第一巴特勒矩阵202具体结构的限定,只要所述第一巴特勒矩阵202能够产生满足上述条件的第一目标波束即可。
其中,图3所示的所述交织极化的多波束天线以所述双极化天线振子的数量为6个为例进行说明,需明确的是,本实施例对所述双极化天线振子的数量为举例进行说明,不作限定。
具体的,即6个所述双极化天线振子包括呈+45度极化的第一天线振子(M1、M2、M3、M4、M5和M6)和呈-45度极化的第二天线振子(N1、N2、 N3、N4、N5和N6),即第一天线振子M1和第二天线振子N1成±45度正交布置,以此类推,第一天线振子M6和第二天线振子N6成±45度正交布置。
本实施例所示的第一巴特勒矩阵包括:
第一组电桥31、第二组电桥32以及第一组功分器33;
所述第一组电桥31的一端连接到第一波束端口;
其中,所述第一组电桥31与3个所述第一波束端口相连以接收3路所述第一输入信号,所述第一组电桥31根据3路所述第一输入信号共生成4路信号输出;
所述第二组电桥32与所述第一组电桥31连接以接收所述第一组电桥31输出的4路信号,所述第二组电桥32根据所述第一组电桥31输出的4路信号共生成4路信号输出,所述第二组电桥32将所述第二组电桥32生成的2路信号输出至与所述第二组电桥32连接的所述第一组功分器33,所述第二组电桥32将所述第二组电桥32生成的另2路信号输出至2个所述双极化天线振子的第一天线振子(M4和M3);
所述第一组功分器33用于将从所述第二组电桥32输入的2路信号一分为二,将形成的4路信号输出至4个所述双极化天线振子的第一天线振子(M2、M6、M1以及M5),以使6个所述第一天线振子(M1、M2、M3、M4、M5和M6)发射出所述第一目标波束。
以下对所述第一巴特勒矩阵内部具体结构进行详细说明:
图3所示的用于接收第一输入信号的第一波束端口为3个(即A1、A2和A3);
所述第一巴特勒矩阵的所述第一组电桥31具体包括第一电桥311和第二电桥312,且所述第一电桥311为3分贝的90度电桥,所述第二电桥312为3分贝的180度电桥;所述第二组电桥32包括第三电桥321和第四电桥322,且所述第三电桥321和所述第四电桥322均为3分贝的180度电桥;
以下结合图4所示对所述3分贝的90度电桥的电桥原理进行详细说明:
3分贝的90度电桥由四端口的功率混合网络构成,其两输出端401和402具有输出信号相位差90度的特性,其直通端和耦合端的相位间差-90°。
即当信号从403输入时,直通端(401)和耦合端(402)的相位分别为-180°、-90°,两端口的功率比为1:1。当信号从404输入时,直通端(402)和耦合端(401)的相位分别为-90°、-180°,两端口的功率比为1:1。
以下结合图5所示对所述3分贝的180度电桥的电桥原理进行详细说明:
3分贝的180度电桥的Σ、△分别代表180度电桥的和端口与差端口。对3dB180°电桥来说,当和端口(Σ)输入时,直通端和耦合端的相位一般都为-90°,两输出端的相移差为0°,输出端501与输出端502的功率比为1:1;当差端口(△)输入时,直通端和耦合端的相位分别为-270°、-90°,两输出端相移差为-180°,输出端501与输出端502的功率比为1:1。
以下3分贝的90度电桥和3分贝的180度电桥的电桥原理请参见图4和图5所示,不再赘述。
进一步参见图3所示,为3分贝的90度电桥的所述第一电桥311由第一波束端口A1和第一波束端口A2接收第一输入信号,为3分贝的180度电桥的所述第二电桥312的和端口为用于接收第一输入信号的第一波束端口A3,所述第二电桥312的差端口接地;
所述第一电桥311的输出端3111和所述第二组电桥32中的第三电桥321的差端口连接,所述第一电桥311的输出端3112与所述第二组电桥32的第四电桥322的差端口连接;
所述第二电桥312的输出端3121与所述第二组电桥32中的第三电桥321的和端口连接,所述第二电桥312的输出端3122与所述第二组电桥32中的第四电桥322的和端口连接。
所述第三电桥321的输出端3211与第一组功分器33中的第一功分器331连接,所述第三电桥321的输出端3212与第一天线振子M4连接;
所述第四电桥322的输出端3221与第一天线振子M3连接,所述第四电桥322的输出端3222与所述第一组功分器33中的第二功分器332连接;
具体的,所述第一功分器331和所述第二功分器332的输出功分比为3:7。
本实施例对功分器的输出功分比为举例进行说明,不作限定。
所述第一功分器331用于将所述第三电桥321输入的信号一分为二,且输出信号的功分比为3:7,且将输出的两路信号分别输出至第一天线振子M2和M6;
所述第二功分器332用于将所述第四电桥322输入的信号一分为二,且输出信号的功分比为3:7,且将输出的两路信号分别输出至第一天线振子M5和M1,以使第一天线振子M1、M2、M3、M4、M5以及M6发射出所述第一目标波束;
具体的,所述第一巴特勒矩阵各极化波束的幅度和相位如表2所示:
表2
  M1 M2 M3 M4 M5 M6
A1 0.54∠90 0.84∠0 1∠-90 1∠-180 0.84∠90 0.54∠0
A2 0.54∠180 0.84∠-90 1∠0 1∠90 0.84∠180 0.54∠-90
A3 0.54∠0 0.84∠0 1∠0 1∠0 0.84∠0 0.54∠0
以下结合图6所示对第二巴特勒矩阵的具体结构进行详细说明:
所述第二巴特勒矩阵具体包括:
第三组电桥61、第四组电桥63、第一组移相器62以及第二组移相器以及第二组功分器64;
所述第三组电桥61与2个所述第二波束端口相连以接收2路所述第二输入信号,且所述第二波束端口连接到各所述第二天线振子;
所述第三组电桥61根据2路所述第二输入信号共生成4路信号输出,所述第三组电桥将所述第三组电桥生成的2路信号输出至与所述第三组电桥连接的所述第一组移相器62,所述第三组电桥61将所述第三组电桥61生成的另2路信号输出至与所述第三组电桥61连接的第四组电桥63;
所述第四组电桥63与所述第一组移相器62连接,且所述第四组电桥63接收经所述第一组移相器62移相后输出的2路信号以及所述第三组电桥61输出的2路信号以生成4路信号输出,所述第四组电桥63将所述第四组电桥63输出的2路信号输出至2个所述双极化天线振子的第二天线振子(N4和N3),所述第四组电桥63将所述第四组电桥63输出的另2路信号输出至与所述第四组电桥63连接的第二组功分器64;
所述第二组功分器64用于将从所述第四组电桥63输入的2路信号一分为二共形成4路信号输出,所述第二组功分器64将所述第二组功分器64输出的2路信号输出至与所述第二组功分器64连接的第二组移相器;
所述第二组移相器将移相后的两路信号输出至2个所述双极化天线振子的第二天线振子(N1和N6),所述第二组功分器64将所述第二组功分器64输出的另2路信号输出至2个所述双极化天线振子的第二天线振子(N2和N5),以使6个所述第二天线振子发射出所述第二目标波束。
以下对所述第二巴特勒矩阵内部具体结构进行详细说明:
图6所示的用于接收第二输入信号的第二波束端口为2个(即B1和B2);
所述第二巴特勒矩阵的所述第三组电桥61包括第五电桥611和第六电桥612,且所述第五电桥611和所述第六电桥612均为3分贝的90度电桥;
所述第四组电桥63包括第七电桥631和第八电桥632,且所述第七电桥631和所述第八电桥632均为3分贝的90度电桥;
具体的,所述第五电桥611的输入端B1为所述第二波束端口,即所述第五电桥611通过所述第二波束端口B1接收第二输入信号,所述第五电桥611的另一输入端接地;
所述第六电桥612的输入端B2为所述第二波束端口,即所述第六电桥612通过所述第二波束端口B2接收第二输入信号,所述第六电桥612的另一输入端接地;
所述第五电桥611的输出端6111与所述第一组移相器62的第一移相器621连接,即所述第一移相器621接收所述第五电桥611的输出端6111输入的信号,并进行移相;
本实施例中,所述第一移相器621的移相为-45度。
需明确的是,本实施例所述第一移相器621的移相为-45度为举例进行说明,不作限定。
所述第五电桥611的输出端6112与所述第四组电桥63的所述第八电桥632的输入端6321连接;
所述第六电桥612的输出端6121与所述第四组电桥63的所述第七电桥631的输入端6311连接;
所述第六电桥612的输出端6122与所述第一组移相器62的第二移相器622连接,即所述第二移相器622接收所述第六电桥612的输出端6122输入的信号,并进行移相;
本实施例中,所述第二移相器622的移相为-45度。
需明确的是,本实施例所述第二移相器622的移相为-45度为举例进行说明,不作限定。
所述第一移相器621的输出端连接至所述第七电桥631的输入端6312;
所述第二移相器622的输出端连接至所述第八电桥632的输入端6322;
所述第七电桥631的输出端6313与第二组功分器64中的第三功分器641的输入端连接,所述第七电桥631的输出端6314与所述第二天线振子N4连接;
所述第八电桥632的输出端6323与所述第二天线振子N3连接,所述第八电桥632的输出端6324与所述第二组功分器64中的第四功分器642的输入端连接;
所述第三功分器641用于将通过其输入端接收到的所述第七电桥631的输出端6313输入的信号一分为二,一路输出第二天线振子N2,另一路输出至所述第二组移相器中的第三移相器651;
所述第四功分器642用于将通过其输入端接收到的所述第八电桥632的输出端6324输入的信号一分为二,一路输出第二天线振子N5,另一路输出至所述第二组移相器中的第四移相器652;
具体的,所述第二组功分器64中的所述第三功分器641和所述第四功分器642的输出功分比为3:7;
所述第二组移相器中的所述第三移相器651和所述第四移相器652的移相均为-180度。
所述第四移相器652将移相后的信号输出至所述第二天线振子N1,所述第三移相器651将移相后的信号输出至所述第二天线振子N6,以使第二天线振子N1、N2、N3、N4、N5以及N6发射出所述第二目标波束;
具体的,所述第二巴特勒矩阵各极化波束的幅度和相位如表3所示:
表3
  N1 N2 N3 N4 N5 N6
B1 0.54∠0 0.84∠-45 1∠-90 1∠-135 0.84∠-180 0.54∠-225
B2 0.54∠-225 0.84∠-180 1∠-135 1∠-90 0.84∠-45 0.54∠0
采用本实施例所示的第一巴特勒矩阵以及第二巴特勒矩阵,所述天线阵列所发射出的波束如图7所示,可见,采用本实施例所示的交织极化的多波束天线,能够有效的减少巴特勒矩阵实现的复杂度,损耗以及成本,减小相邻复用波束之间的干扰。
本实施例以形成有5波束的交织极化的多波束天线为例,不作限定,即本实施例对交织极化的多波束天线具体可形成的波束个数不作限定,只要满足所述第一目标波束和所述第二目标波束间隔设置,且任意相邻的两个波束的指向以及极化不相同即可。
所属领域的技术人员可以清楚地了解到,在本申请所提供的几个实施例中,应该理解到,所揭露的系统,装置和方法,可以通过其它的方式实现。例如,以上所描述的装置实施例仅仅是示意性的,例如,所述单元的划分,仅仅为一种逻辑功能划分,实际实现时可以有另外的划分方式,例如多个单元或组件可以结合或者可以集成到另一个系统,或一些特征可以忽略,或不执行。另一点,所显示或讨论的相互之间的耦合或直接耦合或通信连接可以是通过一些接口,装置或单元的间接耦合或通信连接,可以是电性,机械或其它的形式。
以上所述,以上实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的精神和范围。

Claims (6)

  1. 一种交织极化的多波束天线,其特征在于,包括:
    至少一个双极化天线振子,所述双极化天线振子包括呈+45度极化的第一天线振子和呈-45度极化的第二天线振子;
    第一巴特勒矩阵以及第二巴特勒矩阵,其中,所述第一巴特勒矩阵与所述第一天线振子连接,以使所述第一天线振子发射第一目标波束,所述第一目标波束由所述第一巴特勒矩阵根据至少一个第一波束端口接收的第一输入信号所产生的,且各所述第一目标波束的指向不同;所述第二巴特勒矩阵与所述第二天线振子连接,以使所述第二天线振子发射第二目标波束,所述第二目标波束由所述第二巴特勒矩阵根据至少一个第二波束端口接收的第二输入信号所产生的,且各所述第二目标波束的指向不同,其中,任意相邻的两个所述第一目标波束之间设置有一个所述第二目标波束。
  2. 根据权利要求1所述的交织极化的多波束天线,其特征在于,所述交织极化的多波束天线包括6个所述双极化天线振子,所述第一目标波束由所述第一巴特勒矩阵根据3个所述第一波束端口接收的所述第一输入信号所产生的,所述第二目标波束由所述第二巴特勒矩阵根据2个所述第二波束端口接收的所述第二输入信号所产生的。
  3. 根据权利要求2所述的交织极化的多波束天线,其特征在于,所述第一巴特勒矩阵包括:
    第一组电桥,第二组电桥和第一组功分器,其中,所述第一组电桥与3个所述第一波束端口相连以接收3路所述第一输入信号,所述第一组电桥根据3路所述第一输入信号共生成4路信号输出,所述第二组电桥与所述第一组电桥连接以接收所述第一组电桥输出的4路信号,所述第二组电桥根据所述第一组电桥输出的4路信号共生成4路信号输出,所述第二组电桥将所述第二组电桥生成的2路信号输出至与所述第二组电桥连接的所述第一组功分器,所述第二组电桥将所述第二组电桥生成的另2路信号输出至2个所述双极化天线振子的第一天线振子;
    所述第一组功分器用于将从所述第二组电桥输入的2路信号一分为二,将形成的4路信号输出至4个所述双极化天线振子的第一天线振子,以使6个所述第一天线振子发射出所述第一目标波束。
  4. 根据权利要求3所述的交织极化的多波束天线,其特征在于,
    所述第一组电桥包括第一电桥和第二电桥,且所述第一电桥为3分贝的90度电桥,所述第二电桥为3分贝的180度电桥;
    所述第二组电桥包括第三电桥和第四电桥,且所述第三电桥和所述第四电桥均为3分贝的180度电桥;
    所述第一组功分器包括第一功分器和第二功分器,且所述第一功分器和所述第二功分器的输出功分比为3:7。
  5. 根据权利要求2所述的交织极化的多波束天线,其特征在于,所述第二巴特勒矩阵包括:
    第三组电桥、第四组电桥、第一组移相器、第二组功分器以及第二组移相器,其中,所述第三组电桥与2个所述第二波束端口相连以接收2路所述第二输入信号,所述第三组电桥根据2路所述第二输入信号共生成4路信号输出,所述第三组电桥将所述第三组电桥生成的2路信号输出至与所述第三组电桥连接的所述第一组移相器,所述第三组电桥将所述第三组电桥生成的另2路信号输出至与所述第三组电桥连接的第四组电桥;
    所述第四组电桥与所述第一组移相器连接,且所述第四组电桥接收经所述第一组移相器移相后输出的2路信号以及所述第三组电桥输出的2路信号以生成4路信号输出,所述第四组电桥将所述第四组电桥输出的2路信号输出至2个所述双极化天线振子的第二天线振子,所述第四组电桥将所述第四组电桥输出的另2路信号输出至与所述第四组电桥连接的第二组功分器;
    所述第二组功分器用于将从所述第四组电桥输入的2路信号一分为二共形成4路信号输出,所述第二组功分器将所述第二组功分器输出的2路信号输出至与所述第二组功分器连接的第二组移相器,所述第二组移相器将移相后的两路信号输出至2个所述双极化天线振子的第二天线振子,所述第二组功分器将所 述第二组功分器输出的另2路信号输出至2个所述双极化天线振子的第二天线振子,以使6个所述第二天线振子发射出所述第二目标波束。
  6. 根据权利要求5所述的交织极化的多波束天线,其特征在于,
    所述第三组电桥包括第五电桥和第六电桥,且所述第五电桥和所述第六电桥均为3分贝的90度电桥;
    所述第四组电桥包括第七电桥和第八电桥,且所述第七电桥和所述第八电桥均为3分贝的90度电桥;
    所述第一组移相器包括第一移相器和第二移相器,且所述第一移相器和所述第二移相器的移相均为-45度;
    所述第二组功分器包括第三功分器和第四功分器,且所述第三功分器和所述第四功分器的输出功分比为3:7;
    所述第二组移相器包括第三移相器和第四移相器,且所述第三移相器和所述第四移相器的移相均为-180度。
PCT/CN2015/083722 2014-12-30 2015-07-10 一种交织极化的多波束天线 WO2016107130A1 (zh)

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