CN112216995B - Single beam design method based on 1Bit reconfigurable reflection array - Google Patents
Single beam design method based on 1Bit reconfigurable reflection array Download PDFInfo
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/29—Combinations of different interacting antenna units for giving a desired directional characteristic
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/0087—Apparatus or processes specially adapted for manufacturing antenna arrays
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/06—Arrays of individually energised antenna units similarly polarised and spaced apart
- H01Q21/061—Two dimensional planar arrays
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q3/00—Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
- H01Q3/26—Arrangements 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
- H01Q3/30—Arrangements 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
- H01Q3/34—Arrangements 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
- H01Q3/36—Arrangements 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 variable phase-shifters
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Abstract
The invention discloses a single-beam design method based on a 1Bit reconfigurable reflective array, which mainly solves the problem that the 1Bit reconfigurable reflective array cannot obtain an ideal single beam. The method comprises the steps of determining a theta scanning range of a main beam of a reconfigurable reflector array; calculating the compensation phase of the main beam in the center of the scanning range, and encoding the compensation phase to obtain Bit (i, j); selecting the type of the metal radiation unit at the (i, j) coordinate position according to the coding matrix to obtain a reflection array formed by two types of metal radiation units; calculating the compensation phase of the required main beam theta, and encoding the compensation phase to obtain an encoded matrix Bitc(i, j); and controlling the on-off of PIN tubes of the metal radiation units at each position of the reflection array according to the matrix to realize beam reconstruction. The invention can obtain ideal single wave beam without increasing cost, optimizes the antenna performance, and can be used for indoor signal blind-filling and wave beam scanning of the L-shaped corridor.
Description
Technical Field
The invention belongs to the technical field of antennas, and particularly relates to a single-beam design method which can be used for indoor signal blind-filling and beam scanning of an L-shaped corridor.
Background
With the development of modern communications, there is an increasing demand for functional diversity and adaptability of antennas, especially in radar communications and public communications networks. One of the most important advantages of the reconfigurable reflective array is that beam scanning can be realized, and unlike the conventional phased array which uses complicated T/R components, the required function can be realized by using a low-loss phase converter. The reconfigurable reflective array for realizing beam scanning is the 1Bit reconfigurable reflective array which is applied most. 180-degree phase difference between the units is realized by controlling the PIN tube, so that two states of 0 and 1 are presented, and then compensation phases required by the reflective array units are quantized, so that beam scanning is realized.
Hirokazu Kamoda, Toru Iwasaki et al proposed a 1Bit Reconfigurable reflective array antenna of a millimeter wave imaging system working at 60GHz in an article "60-GHz Electronically configurable Large reflecting Using Single-Bit Phase Shifter" in 2011. According to the design principle, the PIN tube is loaded on a phase delay line at the tail end of a microstrip patch to control on-off, the electrical length of a unit is changed, and therefore the reflection phase of the unit is changed, and finally +/-25-degree beam scanning is achieved. However, when 1-Bit coding is used, two beams of symmetry must occur, which is inherent to 1-Bit itself. Such two symmetric beams are applicable when the application scenario requires exactly two beams, e.g. a T-corridor. However, if only a single beam is required for the reflectarray application scenario, the excess beam is wasted and the main beam is reduced by 3 dB.
Schlemma, Xuxu Shenheng et al proposed a Design of Ku band reconfigurable reflective array unit in 2015 article "Design of a 2-bit reconfigurable reflective array element using two MEMS switches". The design is to load two MEMS switches on one unit to realize 2Bit phase reconfigurability. 1Bit has two states of 0 and 1, and the corresponding phase precision is 180 degrees; however, 2Bit can realize four states of "00", "01", "10" and "11", corresponding to a phase precision of 90 °. Increasing the phase accuracy from 180 ° to 90 ° allows the desired single beam to be obtained, but this increases the cost of the antenna and the complexity of the dc bias circuit.
In summary, there is a contradiction in realizing single beam scanning by the current 1Bit reconfigurable reflective array. A 1Bit would necessarily waste unwanted symmetric beams and would increase the antenna cost if a 2Bit were used.
Disclosure of Invention
The invention aims to provide a single-beam design method based on a 1Bit reconfigurable reflection array aiming at the defects of the prior art so as to obtain an ideal single beam without increasing the cost of an antenna.
In order to achieve the purpose, the technical scheme of the invention is as follows:
a single beam design method based on a 1Bit reconfigurable reflection array is characterized in that the 1Bit reconfigurable reflection array is an M multiplied by N1 Bit reconfigurable reflection array formed by two types of metal radiation units, M, N are positive integers more than or equal to 2, and the two types of metal radiation units are loaded with a PIN diode through a phase delay line; the first type of metal radiation unit realizes phase shift of 0 degree and 180 degrees by controlling the on-off of the PIN tube; the second metal radiation unit realizes 90-degree and 270-degree phase shift by controlling the on-off of the PIN tube;
the single beam design based on the 1Bit reconfigurable reflection array comprises the following steps:
1) determining the theta scanning range of the main beam of the reconfigurable reflector array as thetaS≤θ≤θ F0 is not more than thetaS<60,0<θF≤60;
2) Calculating the main beam theta of the center of the scanning rangeM=(θS+θF) Compensated phase of/2Coding the compensation phase to obtain a coding matrix Bit (i, j);
3) selecting the type (1) or (2) of the metal radiation unit at the coordinate position of (i, j) according to the coding matrix Bit (i, j), and obtaining a specific 1Bit reconfigurable reflection array (3);
4) calculating the compensation phase of the main beam theta required by the reconfigurable reflection array (3)For the compensation phaseCoding by a conventional 1Bit coding method to obtain a coded matrix BitcAnd (i, j), controlling the PIN tube of the metal radiation unit at each position of the 1Bit reconfigurable reflection array (3) to be switched on and switched off according to the matrix to realize beam reconfiguration, and obtaining an ideal single beam.
Compared with the prior art, the invention has the following advantages:
firstly, two types of metal radiation units are arranged on a 1Bit reconfigurable reflection array, a natural 90-degree phase difference is introduced, and on the basis, 1Bit coding is used to enable four states with the 90-degree phase difference to appear in the reflection array.
Secondly, the invention obtains ideal single wave beam without increasing PIN tube, which saves cost.
Drawings
FIG. 1 is a diagram of a 1Bit reconfigurable reflective array system of the present invention;
FIG. 2 is a flow chart of an implementation of the present invention;
FIG. 3 is a normalized pattern for a beam of the present invention with a scan selected at 0;
FIG. 4 is a normalized pattern for a beam of the present invention with a scan selected at 10;
FIG. 5 is a normalized pattern for a beam of the present invention with a scan selected at 20;
FIG. 6 is a normalized pattern for a beam of the present invention with a scan selected at 30;
FIG. 7 is a normalized pattern for a beam of the present invention with a scan selected at 40;
FIG. 8 is a normalized pattern for a beam of the present invention with a scan selected at 45;
FIG. 9 is a normalized pattern for a beam of the present invention at a scan selected of 50;
FIG. 10 is a normalized pattern for a 55 scan selection for a beam of the present invention;
fig. 11 is a normalized pattern of the inventive beam when the scan is selected to be 60.
Detailed Description
The invention is described in further detail below with reference to the attached drawing
Referring to fig. 1, a 1Bit reconfigurable reflective array system 3 of the present example includes a first metal radiation unit 1 and a second metal radiation unit 2.
The first type of metal radiation unit is characterized in that a section of phase delay line 4 is loaded on the basis of a conventional reflective array unit, a PIN (personal identification number) tube 5 is loaded in the phase delay line, when the PIN tube is closed, a signal does not pass through the whole phase delay line, and the phase shift is 0 degree; when the PIN tubes are communicated, signals reach the terminal through the phase delay line and are reflected back to the unit patch, and the phase shift is 180 degrees;
the second metal radiating unit is obtained by changing the length of the phase delay line on the basis of the first metal radiating unit, and the length l of the phase delay line and the phase delayThe relation of (A) is as follows:
where k is the wavenumber, and a suitable l is chosen according to the equation such that when the PIN is closed, the phase shift is 90 °; when the PIN tubes are connected, the phase shift is 270 °.
Referring to fig. 2 and 7, in this embodiment, based on the above-mentioned single beam design method of the 1Bit reconfigurable reflective array, the implementation steps are as follows:
step 1, determining a reconfigurable reflection array main beam theta scanning range to be 0-60 degrees, taking but not limited to the example of theta 40 degrees and theta 60 degreesS=0、θF=60。
Step 2, calculating the compensation phase at 30 DEGThe compensated phase is encoded to obtain an encoding matrix Bit (i, j).
2.1) calculating the compensation phase at 30 DEG from the actual incident wave angle and the required reflected wave angle by the following equation
WhereinIs the angle of the incident wave and,is the angle of the reflected wave, (x)i,yi,zi) Is the coordinate of the ith passive reflective array unit, and lambda is the wavelength;
2.2) compensating the phase of each unitApproximately four states, and according toAnd carrying out quantization coding on the phase range:
Wherein: encoding "00" means that a 0 ° phase shift is achieved; encoding "01" means achieving a 90 ° phase shift; encoding "10" means that a 180 ° phase shift is achieved; encoding "11" means that a 270 ° phase shift is achieved.
And 3, selecting the type of the metal radiation unit at the coordinate position of (i, j) according to the coding matrix Bit (i, j), and obtaining a specific 1Bit reconfigurable reflection array 3.
3.1) when the coding matrix Bit (i, j) is 00 and 10, placing the first type metal radiation unit 1 under the (i, j) coordinate position;
3.2) when the coding matrix Bit (i, j) is 01 and 11, radiating the metal 2 by a second type at the (i, j) coordinate position to obtain a 1Bit reconfigurable reflection array 3.
Step 4, calculating the compensation phase of the main beam theta required by the reconfigurable reflection array 3For the compensation phaseCoding by a conventional 1Bit coding method to obtain a coded matrix Bitc(i,j)。
4.1) calculating the compensation phase of the most central main beam theta of the scanning range according to the angle of the actual incident wave and the required angle of the reflected wave by the following formula
WhereinIs the angle of the incident wave and,is the angle of the reflected wave, (x)i,yi,zi) Is the coordinate of the ith passive reflective array unit, and lambda is the wavelength;
4.2) compensating the phaseCarry out coding whenThen, at (i, j) position code equals 0; when in useThen, the code is equal to 1 at the (i, j) position, and the resulting coded matrix Bitc(i, j) wherein:refers to the phase of the metal radiation unit when the PIN tube is disconnected under the (i, j) position coordinate system,the phase position refers to the phase position of the metal radiation unit when the PIN tube is communicated under the position coordinates of (i, j);
The effect of the invention can be further illustrated by the following simulation examples:
simulation 1: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 0 °, and the result is shown in fig. 3.
It can be seen from fig. 3 that the method of the present invention can obtain the required main beam in the 0 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
Simulation 2: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 10 °, and the result is shown in fig. 4.
It can be seen from fig. 4 that the method of the present invention can obtain the required main beam in the 10 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
Simulation 3: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 20 °, and the result is shown in fig. 5.
Fig. 5 shows that the method of the present invention can obtain the required main beam in the 20 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
And (4) simulation: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 30 °, and the result is shown in fig. 6.
Fig. 6 shows that the method of the present invention can obtain the required main beam in the 30 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
And (5) simulation: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 45 °, and the result is shown in fig. 8.
Fig. 8 shows that the method of the present invention can obtain the required main beam in the 45 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
And (6) simulation: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 50 °, and the result is shown in fig. 9.
It can be seen from fig. 9 that the method of the present invention can obtain the required main beam in the 50 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
And (7) simulation: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° ≦ θ ≦ 60 °, and the main beam angle θ of the reflection array is 55 °, and the result is shown in fig. 10.
Fig. 10 shows that the method of the present invention can obtain the required main beam in the 55 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
And (8) simulation: the HFSS software is used to simulate the normalized directional diagram of the present invention when the scanning range is 0 ° < theta > 60 °, and the main beam angle θ of the reflection array is 60 °, and the result is shown in fig. 11.
Fig. 11 shows that the method of the present invention can obtain the required main beam in the 60 ° direction of the main beam required by the reflector array, and no higher side lobes appear in the other directions.
In conclusion, the invention can realize different main beam directions within the beam scanning range of 0-60 degrees, and obtain the required ideal single beam.
Claims (6)
1. A single beam design method based on a 1Bit reconfigurable reflection array is characterized by comprising the following steps:
the 1Bit reconfigurable reflection array is an M multiplied by N1 Bit reconfigurable reflection array (3) formed by two types of metal radiation units (1, 2), M, N are positive integers more than or equal to 2, and the two types of metal radiation units are loaded with a PIN diode (5) through a phase delay line (4); the first-class metal radiation unit (1) realizes phase shift of 0 degree and 180 degrees by controlling the on-off of the PIN diode; the second metal radiation unit (2) realizes 90-degree and 270-degree phase shift by controlling the on-off of the PIN tube; the single beam design based on the 1Bit reconfigurable reflection array comprises the following steps:
1) determining the theta scanning range of the main beam of the reconfigurable reflector array as thetaS≤θ≤θFWherein 0 is not more than thetaS<60,0<θF≤60;
2) Calculating the main beam theta of the center of the scanning rangeM=(θS+θF) Compensated phase of/2Coding the compensation phase to obtain a coding matrix Bit (i, j);
3) selecting a first type metal radiation unit (1) or a second type metal radiation unit (2) at the (i, j) coordinate position according to the coding matrix Bit (i, j) to obtain a specific 1Bit reconfigurable reflection array (3);
4) calculating the compensation phase of the main beam theta required by the 1Bit reconfigurable reflection array (3)For the compensation phasePerforming conventional 1Bit encodingObtaining the coded matrix Bit by the method codingcAnd (i, j), controlling the on-off of PIN diodes of metal radiation units at each position of the 1Bit reconfigurable reflection array (3) according to the matrix to realize beam reconfiguration, and obtaining an ideal single beam.
2. The method of claim 1, wherein 2) the scan range centermost main beam θ is calculatedM=(θS+θF) Compensated phase of/2Is calculated by the following formula:
3. The method of claim 1, wherein the compensating phase in 2)The coding matrix Bit (i, j) obtained by coding is expressed as follows:
wherein: encoding "00" means that a 0 ° phase shift is achieved; encoding "01" means achieving a 90 ° phase shift; encoding "10" means that a 180 ° phase shift is achieved; encoding "11" means that a 270 ° phase shift is achieved.
4. The method according to claim 1, wherein the first type of metal radiating elements (1) or the second type of metal radiating elements (2) at the (i, j) coordinate position are selected in 3) according to the coding matrix Bit (i, j) as follows:
when the codes are 00 and 10, the position is provided with a first metal radiation unit (1);
when encoded as 01 and 11, the position places a second type of metal radiating element (2).
5. The single beam design method based on the 1Bit reconfigurable reflective array according to claim 1, characterized in that, in 4), the compensation phase is compensatedCoded matrix Bit obtained by codingc(i, j), as follows:
6. The method for designing the single beam based on the 1Bit reconfigurable reflective array according to claim 1, wherein the coded matrix Bit in 4)c(i, j) controlling the on-off of PIN diodes of metal radiating units at each position of the 1Bit reconfigurable reflective array (3) at BitcWhen (i, j) is 0, the PIN at the (i, j) coordinate position is dipolarThe pipe (5) is disconnected; at BitcWhen (i, j) is 1, the PIN diode (5) at the position coordinate of (i, j) is connected.
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