CN112751207B - Lens structure, lens antenna and electronic equipment - Google Patents
Lens structure, lens antenna and electronic equipment Download PDFInfo
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- CN112751207B CN112751207B CN201911056415.XA CN201911056415A CN112751207B CN 112751207 B CN112751207 B CN 112751207B CN 201911056415 A CN201911056415 A CN 201911056415A CN 112751207 B CN112751207 B CN 112751207B
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/02—Refracting or diffracting devices, e.g. lens, prism
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/02—Refracting or diffracting devices, e.g. lens, prism
- H01Q15/04—Refracting or diffracting devices, e.g. lens, prism comprising wave-guiding channel or channels bounded by effective conductive surfaces substantially perpendicular to the electric vector of the wave, e.g. parallel-plate waveguide lens
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q15/00—Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices
- H01Q15/02—Refracting or diffracting devices, e.g. lens, prism
- H01Q15/08—Refracting or diffracting devices, e.g. lens, prism formed of solid dielectric material
Abstract
The application relates to a lens structure, a lens antenna and an electronic device. The lens structure can generate artificial surface plasmon waveguides by utilizing a plurality of pairs of second conducting strips, and the gradual change rule of the number of the second conducting strips of the waveguide structure between layers or in the layers is set, so that the phase delay distribution rule is obtained to realize the wave beam convergence function, and the dielectric loss of electromagnetic waves in the waveguide transmission process is low, so that the lens antenna with smaller loss, higher efficiency and larger broadband can be realized in practical application. In addition, the dielectric layer and the waveguide layer which are alternately arranged in a laminated manner can also realize the assembly preparation of the low-cost lens.
Description
Technical Field
The present application relates to the field of antenna technologies, and in particular, to a lens structure, a lens antenna, and an electronic device.
Background
The lens antenna is an antenna consisting of a lens and a feed source, and can ensure that electromagnetic waves emitted by the feed source are emitted in parallel through the lens by utilizing the convergence characteristic of the lens, or ensure that the electromagnetic waves incident in parallel are converged to the feed source after passing through the lens. Because electromagnetic waves generally need to pass through a plurality of dielectric layers when entering the lens, the introduction of the dielectric will cause the loss of the electromagnetic waves, thereby reducing the efficiency of the lens antenna.
Disclosure of Invention
Accordingly, there is a need for a lens structure, a lens antenna, and an electronic device that can improve the efficiency of the lens antenna.
In order to achieve the purpose of the application, the following technical scheme is adopted:
a lens structure, comprising:
a plurality of dielectric layers;
the multi-waveguide layer is alternately laminated with the dielectric layers along a first direction, and the waveguide layer comprises:
one or more waveguide structures, a plurality of which are spaced and arranged in parallel; the waveguide structure includes a first conductive sheet and at least one pair of second conductive sheets, each pair of the second conductive sheets being symmetrically disposed about a central axis, a plurality of the second conductive sheets on the same side of the central axis being connected to each other through the first conductive sheet;
the waveguide layers are arranged on the same axis, and a first gradual change rule of the number of the second conducting strips is formed among the waveguide structures on the same axis, and/or a second gradual change rule of the number is formed among the waveguide structures; the axis is a straight line passing through any of the waveguide layers and parallel to the first direction.
A lens antenna, comprising:
A feed source array; and
a lens structure as described above arranged parallel to the array of feeds.
An electronic device comprising a lens antenna as described above.
According to the lens structure, the second symmetrical conducting strips are utilized to generate the artificial surface plasmon waveguide, the gradual change rule of the number of the second conducting strips of the waveguide structure between layers or in the layers is set, so that the phase delay distribution rule is obtained to realize the wave beam convergence function, the dielectric loss of electromagnetic waves in the waveguide transmission process is low, and therefore the lens antenna with smaller loss, higher efficiency and larger broadband can be realized in practical application. In addition, the dielectric layer and the waveguide layer which are alternately arranged in a laminated manner can also realize the assembly preparation of the low-cost lens.
The lens antenna comprises the feed source array and the lens structure, and can realize the lens antenna with smaller loss, higher efficiency, larger broadband and lower cost through the symmetrical structure and the gradual change rule of the number of the second conducting strips in the lens structure; the multi-beam emergent and beam scanning can be realized through the arrangement of the feed source array.
The electronic device including the lens antenna has the advantages of smaller loss, higher efficiency, larger broadband and lower cost, and can realize multi-beam emission and beam scanning, so that the electronic device can realize high-efficiency, high-gain and low-cost beam scanning.
Drawings
FIG. 1 is a schematic diagram of a lens structure according to an embodiment;
FIG. 2 is a schematic diagram of a waveguide structure in one embodiment;
FIG. 3 is a schematic structural diagram of a waveguide structure in another embodiment;
FIG. 4 is a schematic structural diagram of a waveguide structure in another embodiment;
FIG. 5 is a schematic structural diagram of a waveguide structure in another embodiment;
FIG. 6 is a schematic structural diagram of a waveguide structure in another embodiment;
FIG. 7 is a schematic structural diagram of a waveguide layer in one embodiment;
FIG. 8 is a schematic structural diagram of a plurality of waveguide structures according to a first tapering rule in an embodiment;
FIG. 9 is a schematic structural diagram of a plurality of waveguide structures according to a second tapering rule in an embodiment;
FIG. 10 is a schematic diagram of a lens structure according to an alternative embodiment;
FIG. 11 is a schematic diagram of a lens structure according to a second alternative embodiment;
FIG. 12 is a schematic diagram of a lens structure according to a third alternative embodiment;
FIG. 13 is a schematic diagram of a lens configuration according to a fourth alternative embodiment;
FIG. 14 is a schematic diagram of a fifth alternative embodiment of a lens construction;
FIG. 15 is a schematic structural view of a waveguide structure in another embodiment;
FIG. 16 is a schematic structural view of a waveguide structure in another embodiment;
FIG. 17 is a schematic view of a waveguide structure in another embodiment;
FIG. 18 is a schematic structural view of a waveguide structure in another embodiment;
FIG. 19 is a schematic diagram of a lens antenna according to an embodiment;
FIG. 20 is a schematic diagram of a feed array in one embodiment;
FIG. 21 is a schematic structural diagram of a lens antenna in another embodiment;
FIG. 22 is a schematic structural diagram of a lens antenna in another embodiment;
FIG. 23 is a diagram illustrating an electronic device according to an embodiment;
FIG. 24 is a beam scanning pattern in one embodiment;
FIG. 25 is a block diagram of an electronic device in an embodiment;
fig. 26 is a schematic structural diagram of an electronic device in an embodiment.
Detailed Description
To facilitate an understanding of the present application, the present application will now be described more fully with reference to the accompanying drawings. Preferred embodiments of the present application are illustrated in the accompanying drawings. This application may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete.
It will be understood that, as used herein, the terms "first," "second," and the like may be used herein to describe various elements, but these elements are not limited by these terms. These terms are only used to distinguish one element from another element, and are not to be construed as indicating or implying relative importance or implying any number of technical features indicated. Thus, a feature defined as "first" or "second" may explicitly or implicitly include at least one such feature. In the description of the present application, "plurality" means at least two, e.g., two, three, etc., unless specifically limited otherwise.
Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs. The terminology used herein in the description of the present application is for the purpose of describing particular embodiments only and is not intended to be limiting of the application.
Referring to fig. 1, fig. 1 is a schematic structural diagram of a lens structure in an embodiment.
In the present embodiment, the lens structure 10 is applied to a lens antenna. According to the specific application scenario of the lens antenna, the lens structure 10 has different phase delay distribution laws, so as to realize the function of converging electromagnetic waves. Optionally, the lens structure 10 may operate in a microwave frequency band, and may be adapted to different frequency bands such as millimeter waves and terahertz waves by adjusting structural parameters.
Millimeter waves refer to electromagnetic waves with a wavelength of the order of millimeters, and the frequency of the millimeter waves is about 20GHz to 300 GHz. The 3GP has specified a list of frequency bands supported by 5G NR, the 5G NR spectral range can reach 100GHz, and two frequency ranges are specified: frequency range 1(FR1), i.e. the sub-6 GHz band, and Frequency range 2(FR2), i.e. the millimeter wave band. Frequency range of Frequency range 1: 450MHz-6.0GHz, with a maximum channel bandwidth of 100 MHz. The Frequency range of the Frequency range 2 is 24.25GHz-52.6GHz, and the maximum channel bandwidth is 400 MHz. The near 11GHz spectrum for 5G mobile broadband comprises: 3.85GHz licensed spectrum, for example: 28GHz (24.25-29.5GHz), 37GHz (37.0-38.6GHz), 39GHz (38.6-40GHz) and 14GHz unlicensed spectrum (57-71 GHz). The working frequency bands of the 5G communication system comprise three frequency bands of 28GHz, 39GHz and 60 GHz.
Referring to fig. 1, the lens structure 10 includes a multilayer dielectric layer 100 and a multilayer waveguide layer 200; the waveguide layers 200 and the dielectric layers 100 are alternately stacked in the first direction. The number of layers of the dielectric layer 100 and the waveguide layer 200 is not limited (fig. 1 takes five dielectric layers 100 and four waveguide layers 200 as an example), and meanwhile, the relative area between the dielectric layer 100 and the waveguide layer 200 is not limited and can be adjusted according to the actual application situation.
The dielectric layer 100 is a non-conductive functional layer capable of supporting and fixing the waveguide layer 200, and the dielectric layer 100 and the waveguide layer 200 are alternately stacked to realize the interval distribution of the multilayer waveguide layer 200; meanwhile, the lens structure 10 may be divided into a plurality of regions with discontinuous refractive indexes by the dielectric layer 100, so that the size of the waveguide layer 200 in the first direction only needs to be changed in a small range to achieve the converging effect, thereby achieving the assembly preparation of the low-cost lens. Alternatively, when the thicknesses of the plurality of dielectric layers 100 in the direction of the alternate stacking are equal, the plurality of waveguide layers 200 are equally spaced. Optionally, the material of the dielectric layer 100 is an electrically insulating material.
The plurality of waveguide layers 200 may emit the incident electromagnetic wave in parallel, or converge the incident electromagnetic wave in parallel to a focal point, or diverge the incident electromagnetic wave in parallel. Waveguide layer 200 includes one or more waveguide structures 300. Alternatively, the material of the waveguide layer 200 may be a conductive material, such as a metal material, an alloy material, a conductive silica gel material, a graphite material, and the like, and the material of the waveguide layer 200 may also be a material having a high dielectric constant.
Wherein the waveguide structure 300 comprises a first conductive sheet 301 and at least one pair of second conductive sheets 302, each pair of second conductive sheets 302 being symmetrically disposed about a central axis, the plurality of second conductive sheets 302 on the same side of the central axis being connected to each other through the first conductive sheet 301, the electromagnetic wave being incident to the lens structure 10 along the central axis of the waveguide structure 300. The length direction of the second conductive sheet 302 is substantially perpendicular to the central axis.
In some embodiments, referring to fig. 2-3, each waveguide structure 300 comprises one first conductive sheet 301, with each pair of second conductive sheets 302 disposed on either axial side of the second conductive sheet 302. When the waveguide structure 300 is plural, the plural waveguide structures 300 are spaced and arranged in parallel. Alternatively, the plurality of waveguide structures 300 are equally spaced and arranged side-by-side.
Alternatively, for example as in fig. 2, each pair of second conductive plates 302 is arranged mirror-symmetrically with respect to the central axis a, and each pair of second conductive plates 302 is arranged axially mirror-symmetrically on both sides of the first conductive plate 301. Wherein, the mirror symmetry means that each pair of the second conductive sheets 302 is symmetrical about the axis of the central axis a. Alternatively, for example, fig. 3, each pair of the second conductive sheets 302 is symmetrically disposed in a sliding manner about the central axis a, and each pair of the second conductive sheets 302 is symmetrically disposed in an axial sliding manner on both sides of the first conductive sheet 301. The sliding symmetry means that the two second conductive sheets 302 originally symmetric about the axis slide relatively along the central axis a for a certain distance; the plurality of waveguide structures 300 are independent of each other and similar in shape.
It should be noted that the first conductive plate 301 is not limited to be an independent and integral whole, and may be a conductive plate provided with one or more slits along the axial direction. Taking the first conductive sheet 301 with a slit along the axial direction as an example, the waveguide structure 300 may also be the structure shown in fig. 4.
In some embodiments, referring to fig. 5-6, each waveguide structure 300 comprises two first conductive sheets 301 disposed at intervals; in the same waveguide structure 300, each pair of the second conductive sheets 302 is disposed between the two first conductive sheets 301, and the two second conductive sheets 302 in the same pair are disposed at intervals.
Alternatively, for example, fig. 5, each pair of the second conductive sheets 302 is arranged mirror-symmetrically with respect to the central axis a (a mirror-symmetric slot unit 300A is formed inside the waveguide structure 300, and the slot unit 300A is mirror-symmetric with respect to the central axis a); alternatively, for example, fig. 6, each pair of the second conductive sheets 302 is arranged in a sliding symmetry about the central axis a (thereby, a sliding symmetry slit unit 300A is formed inside the waveguide structure 300, and the slit unit 300A is sliding symmetry about the central axis a).
Each waveguide structure 300 is formed with one slot unit 300A. When the waveguide structure 300 is plural, the plural waveguide structures 300 are disposed in parallel. Alternatively, two first conductive sheets 301 adjacent to two adjacent waveguide structures 300 are connected to each other (see fig. 7, fig. 7 exemplifies 5 waveguide structures 300 and a second conductive sheet 302 arranged mirror-symmetrically with respect to the central axis a).
When electromagnetic waves are incident to the lens structure 10 along the central axis a of the waveguide structure 300, in the length direction of the second conductive sheets 302, an artificial surface plasmon waveguide (hereinafter abbreviated as a waveguide) can be generated at the edge of each second conductive sheet 302 or at the edge of each slot unit 300A, a plurality of pairs of mirror-symmetric second conductive sheets 302 can generate mirror-symmetric waveguide pairs, and each waveguide structure is formed by linearly arranging a plurality of waveguides; the pairs of the second conductive sheets 302 can generate pairs of waveguides with symmetrical sliding, and each waveguide structure is composed of a plurality of waveguides arranged linearly. Alternatively, in each waveguide structure 300, the plurality of second conductive sheets 302 located on the same side of the central axis a are arranged in parallel and have the same center distance p, and the lengths h of the plurality of second conductive sheets 302 are the same, so that the edges of each second conductive sheet 302 in the length direction in the plurality of waveguide structures 300 can generate the same waveguide. Wherein the center distance p may be understood as the distance between the geometric centers of two adjacent second conductive sheets 302.
When the electromagnetic wave is incident to the lens structure along the central axis a of the waveguide structure 300, the electromagnetic wave can continue to propagate along the waveguide, and the propagation constant is larger than the free space, that is, the equivalent refractive index larger than 1 is realized, and the convergence function is realized. Since most of the energy of the electromagnetic wave concentrates on the edge of the second conductive sheet 302 in the length direction of the waveguide structure 300, only a small amount of the energy enters the medium, and thus the electromagnetic wave is hardly affected by the loss of the medium, and thus a lens antenna with less loss and higher efficiency can be realized in practical application. When each pair of the second conductive sheets 302 is axially and symmetrically slid, the equivalent refractive index changes less with frequency, so that a lens antenna with a larger bandwidth can be realized in practical application.
In some embodiments, there is a first tapering rule of the number of the second conductive layers 302 between the plurality of waveguide structures 300 of the plurality of waveguide layers 200 on the same axis, and/or there is a second tapering rule of the number of the second conductive layers 302 between the plurality of waveguide structures 300 of the waveguide layers 200. Wherein the axis is a straight line passing through any of the waveguide layers 200 and parallel to the first direction.
When the electromagnetic wave is incident to the lens structure 10 along the central axis a of the waveguide structure 300, the lens structure 10 having the first gradual change rule can realize the converging effect of the electromagnetic wave beam in the first direction, and the lens structure 10 having the second gradual change rule can realize the converging effect of the electromagnetic wave beam in the second direction. Wherein the second direction is substantially perpendicular to both the first direction and the axial direction of the first conductive sheet 301, i.e. parallel to the length direction of the second conductive sheet 302.
Specifically, referring to fig. 8, the first gradual change rule is that the number of the second conductive layers 302 decreases symmetrically from the central position of the same axis to the waveguide structures 300 on both sides, i.e. decreases symmetrically from the waveguide structure 300 on the central layer of the plurality of waveguide layers 200 to the waveguide structures 300 on both sides (fig. 8 takes the waveguide structure 300 in the embodiment of fig. 3 as an example, and only shows the waveguide structure 300 on the axis a of each waveguide layer 200 at the same time It is intended that the number of the second conductive sheets 302 of the intermediate layer waveguide structure 300 is denoted by T 3A Two layers on one side are respectively marked as T 2A And T 1A And the two layers on the other side are respectively marked as T 4A And T 5A ，T 3A ＞T 4A ＝T 2A ＞T 1A ＝T 5A ) (ii) a Referring to fig. 9, the second gradual change rule is that the number of the second conductive sheets 302 decreases from the arrangement center of the waveguide structures 300 of the waveguide layer 200 to both sides symmetrically, that is, the number of the second conductive sheets 302 decreases from the waveguide structure 300 at the center of the layer to the waveguide structures 300 at both sides of the layer symmetrically (fig. 9 takes the waveguide structure 300 in the embodiment of fig. 3 as an example, and only shows the waveguide structure 300 of a certain waveguide layer 200, and the number of the paired second conductive sheets 302 at the center of the layer is marked as T C One side of the layer center is marked as T B And T A The other side of the layer center is marked as T D And T E ，T C ＞T B ＝T D ＞T A ＝T E ). When the structural size of the second conductive sheets 302 of the plurality of waveguide structures 300 is the same, the larger T, the larger the phase delay value.
It should be noted that the decrement may be a linear decrement or a non-linear decrement, for example, the linear decrement may be understood as decreasing according to an equal ratio series, a gradient of an equal difference series or according to a specific rule.
Specifically, when the number of the waveguide layers 200 is at least three, a first gradual change rule of the number of the second conductive sheets 302 is provided between the plurality of waveguide structures 300 on the same axis in the plurality of waveguide layers 200; and/or when the number of the waveguide structures 300 of the waveguide layer 200 is at least three, the plurality of waveguide structures 300 of the waveguide layer 200 have a second gradient rule of the number of the second conductive layers 302. When the number of the waveguide layer 200 is one or two, the waveguide layer includes at least three waveguide structures 300, and a second gradual change rule of the number of the second conductive layers 302 is provided between the plurality of waveguide structures 300 of the waveguide layer 200.
Alternatively, when the first direction of the waveguide layer 200 and the dielectric layer 100 is perpendicular to the polarization direction of the lens antenna in the practical application scenario, the plurality of waveguide structures 300 are configured as: a first gradual change rule of the number of the second conductive sheets 302 is provided among the plurality of waveguide structures 300 on the same axis in the plurality of waveguide layers 200; at this time, if the number of the second conductive sheets 302 of the plurality of waveguide structures 300 in the waveguide layer 200 is the same (see the first alternative embodiment and the second alternative embodiment), the lens structure 10 only realizes the electromagnetic wave convergence in the first direction; if the second gradual change law of the number of the second conductive layers 302 exists between the waveguide structures 300 in the same waveguide layer 200 (see the third alternative embodiment), the lens structure 10 can achieve the electromagnetic wave convergence in the first direction and the second direction at the same time. Specifically (illustrated by the waveguide structure 300 of the embodiment of fig. 3):
the first alternative embodiment: referring to fig. 10, fig. 10 illustrates five waveguide layers 200, each waveguide layer 200 having only one waveguide structure 300 (the number of the second conductive sheets 302 of the waveguide structure 300 in the nth waveguide layer 200 is denoted by T) n ) At this time, there is a first gradual change law of the number of the second conductive sheets 302 between the five waveguide structures 300: t is a unit of 3 ＞T 4 ＝T 2 ＞T 5 ＝T 1 That is, the T value decreases from the waveguide structure 300 of the waveguide layer 200 located at the center to the waveguide structures 300 of the two side layers, so that the phase retardation value of the lens structure 10 decreases from the middle layer to the two side layers, and the lens structure 10 realizes the convergence of the electromagnetic wave in the first direction (y direction in the drawing).
An alternative embodiment two: referring to fig. 11, fig. 11 illustrates the five-layer waveguide layer 200 and each waveguide layer 200 includes two waveguide structures 300, where a first gradual change rule of the number of the second conductive sheets 302 is defined between the waveguide structures 300 on the same axis in the five-layer waveguide layer 200, and the number of the second conductive sheets 302 of the two waveguide structures 300 in the waveguide layer 200 is the same. Specifically, the method comprises the following steps: the gradual change situation of the number is as follows: t is 3A ＝T 3B ＞T 4A ＝T 4B ＝T 2A ＝T 2B ＞T 5A ＝T 5B ＝T 1A ＝T 1B (wherein, the plurality of waveguide structures 300 in the A-axis are respectively located in the A-region of the waveguide layer 200, and the number of the second conductive sheets 302 of the waveguide structures 300 in the A-region of the nth waveguide layer 200 is denoted by T nA (ii) a In the B axisThe waveguide structures 300 are respectively located in the B region of the waveguide layer 200, and the number of the second conductive layers 302 of the waveguide structures 300 located in the B region of the nth waveguide layer 200 is marked as T nB ) That is, the T value decreases from the middle layer to the two side layers, so that the phase retardation value of the lens structure 10 decreases from the middle layer to the two side layers, and the lens structure 10 realizes the convergence of the electromagnetic waves in the first direction.
The third alternative embodiment: referring to fig. 12, fig. 12 illustrates the five-layer waveguide layer 200 and three waveguide structures 300 per layer of waveguide layer 200, where a first gradient rule of the number of the second conductive layers 302 exists among the waveguide structures 300 on the same axis in the five-layer waveguide layer 200, and a second gradient rule of the number of the second conductive layers 302 exists among the waveguide structures 300 in the same waveguide layer 200. Specifically, the method comprises the following steps: the number of second conductive strips 302 of the waveguide structure 300 situated in the axis a of the different waveguide layers 200 (corresponding to the a region of the waveguide layer 200, the a region of the nth waveguide layer 200 being designated T) nA ) The first gradual change law of the number of the second conductive sheets 302 is provided between the five waveguide structures 300: t is 3A ＞T 4A ＝T 2A ＞T 5A ＝T 1A The number of second conductive strips 302 of the waveguide structure 300 situated along the axis B of the different waveguide layer 200 (corresponding to the B region of the waveguide layer 200, the B region of the nth waveguide layer 200 is denoted T nB ) The first gradual change law of the number of the second conductive sheets 302 is provided between the five waveguide structures 300: t is 3B ＞T 4B ＝T 2B ＞T 5B ＝T 1B The number of second conductive strips 302 of the waveguide structure 300 situated along the axis C of the different waveguide layers 200 (corresponding to the C region of the waveguide layer 200, the C region of the nth waveguide layer 200 is denoted T) nC ) The first gradual change law of the number of the second conductive sheets 302 is provided between the five waveguide structures 300: t is a unit of 3C ＞T 4C ＝T 2C ＞T 5C ＝T 1C And, the number in each waveguide layer 200 is a second gradual change law: t is A ＝T C ＜T B . Thus, the phase retardation value of the lens structure 10 decreases from the middle layer to both side layers, and decreases from the center position in the layers to both side positions, and the lens structure 10 can be formedSo as to realize the convergence of the electromagnetic waves in the first direction and the second direction (i.e. the x direction in the figure) at the same time.
Alternatively, when the first directions of the waveguide layer 200 and the dielectric layer 100 are parallel to the polarization direction of the lens antenna in the practical application scenario, the plurality of waveguide structures 300 are configured as: a second gradual change law of the number of the second conductive strips 302 exists among the plurality of waveguide structures 300 in the waveguide layer 200; at this time, if the number of the second conductive sheets 302 of the plurality of waveguide structures 300 on the same axis in different waveguide layers 200 is the same (see the fourth alternative embodiment), the lens structure 10 only realizes the electromagnetic wave convergence in the second direction; if the first gradual change rule of the number of the second conductive layers 302 is provided between the waveguide structures 300 on the same axis in different waveguide layers 200 (see the fifth alternative embodiment), the lens structure 10 can achieve the electromagnetic wave convergence in the second direction and the first direction at the same time. Specifically (illustrated by the waveguide structure 300 of the embodiment of fig. 3):
An alternative embodiment is four: referring to fig. 13, in fig. 13, three layers of waveguide layers 200 are taken as an example, and each layer of waveguide layer 200 includes five waveguide structures 300, at this time, a second gradient rule of the number of the second conductive layers 302 exists among the plurality of waveguide structures 300 in the waveguide layer 200, and the number of the plurality of waveguide structures 300 on the same axis in different waveguide layers 200 is the same. Specifically, the method comprises the following steps: the first gradual change law of the number of the second conductive strips 302 is provided between the five waveguide structures 300 of the same waveguide layer 200: t is C ＞T B ＝T D ＞T A ＝T E That is, the value T decreases from the waveguide structure 300 at the layer center position to the waveguide structures 300 on both sides, so that the phase retardation value of the lens structure 10 decreases from the layer center position to both sides, and the lens structure 10 realizes the convergence of the electromagnetic wave in the second direction.
An alternative embodiment five: referring to fig. 14, in fig. 14, three layers of waveguide layers 200 are taken as an example, and each layer of waveguide layer 200 includes five waveguide structures 300, at this time, a second gradient rule of the number of the second conductive layers 302 exists among the plurality of waveguide structures 300 in the waveguide layer 200, and a first gradient rule of the number of the second conductive layers 302 exists among the plurality of waveguide structures 300 on the same axis in different waveguide layers 200. Specifically, the method comprises the following steps: The first gradual change law of the number of the second conductive strips 302 is provided between the five waveguide structures 300 of the same waveguide layer 200: t is C ＞T B ＝T D ＞T A ＝T E That is, the T value decreases from the waveguide structure 300 at the layer center position to the waveguide structures 300 at both sides, and there is a first gradual change law of the number of the second conductive sheets 302 between the three waveguide structures 300 in the a region in different waveguide layers 200: t is 2A ＞T 1A ＝T 3A The three waveguide structures 300 in the B region of different waveguide layers 200 have a first gradual change law of number: t is a unit of 2B ＞T 1B ＝T 3B The first gradual change law of the number of the second conductive strips 302 exists between the three waveguide structures 300 in the C region of different waveguide layers 200: t is 2C ＞T 1C ＝T 3C . Therefore, the equivalent refractive index of the lens structure 10 decreases from the center of the layer to the two sides, and at the same time, the equivalent refractive index decreases from the middle layer to the two sides, so that the lens structure 10 realizes the convergence of the electromagnetic waves in the second direction and the first direction.
Further, in some embodiments, referring to fig. 15-16, when each waveguide structure 300 includes one first conductive sheet 301, each pair of second conductive sheets 302 is disposed on both axial sides of the first conductive sheet 301: each waveguide structure 300 is provided with a first region 3001, a second region 3002, and a third region 3003 in the axial direction, the second conductive sheet is provided in the second region 3002, and at least one of the first region 3001 and the third region 3003 is provided with a first matching unit. Wherein, the first region 3001 is an incident region of the waveguide structure 300, and the third region 3003 is an emergent region of the waveguide structure 300; alternatively, the first region 3001 is an exit region of the waveguide structure 300, and the third region 3003 is an entrance region of the waveguide structure 300.
The first matching unit comprises at least one pair of first matching sections 303 which are symmetrical about a central axis, and two first matching sections 303 in the same pair are respectively arranged on two sides of the first conductive plate 301; in the length direction, the length of the first matching section 303 of the same waveguide structure 300 is smaller than that of the second conductive sheet 302 (fig. 15 exemplifies that only the first region 3001 is provided with the first matching units and the first matching sections 303 are two pairs, and fig. 16 exemplifies that the first region 3001 and the third region 3003 are provided with the first matching units and each first matching section 303 is two pairs).
Wherein the structure of the first matching sections 303 is similar to that of the second conductive sheet 302, optionally, each pair of first matching sections 303 is mirror symmetric about the central axis a, that is, each pair of first matching sections 303 is axially mirror symmetric arranged on both sides of the first conductive sheet 301; alternatively, each pair of first matching sections 303 is slidably symmetric about the central axis a, that is, each pair of first matching sections 303 is axially slidably symmetric disposed on both sides of the first conductive sheet 301 (fig. 15-16 exemplify that the second conductive sheet 302 is slidably symmetric and the first matching sections 303 are mirror images). The first matching section 303 has conductivity, and optionally, the material of the first matching section 303 is the same as that of the second conductive sheet 302.
Since the length of the first matching section 303 is smaller than that of the second conductive sheet 302, when the electromagnetic wave is incident to the first matching section 303 through the second conductive sheet 302, the refractive index gradually decreases; when the first connection region is the incident region of the waveguide structure 300 (taking fig. 15 as an example), the first matching section 303 can implement impedance matching between the incident region of the electromagnetic wave of the lens structure 10 and the free space, so as to reduce the energy loss of the electromagnetic wave; when the first connection region is the exit region of the waveguide structure 300, the first matching section 303 can respectively implement impedance matching between the exit region of the electromagnetic wave of the lens structure 10 and the free space, so as to reduce energy loss of the electromagnetic wave, thereby increasing the transmission distance of the electromagnetic wave and improving the efficiency of the lens antenna.
A third gradient rule is provided between the pairs of first matching sections 303, and the third gradient rule is that the lengths of the pairs of first matching sections 303 decrease from the side of the first area 3001 close to the second area 3002 to the side of the first area 3001 far away from the second area 3002, and/or decrease from the side of the third area 3003 close to the second area 3002 to the side of the third area 3003 far away from the second area 3002. The number of pairs of the first matching segments of the first area 3001 and the second area 3002 may be the same or different. In fig. 16, the length of the first matching section 303 is divided into two pairs, for example, the first area 3001 and the second area 3002 are respectively provided with two pairs of first matching sections 303, and each pair of the second conductive sheets 302 and each pair of the first matching sections 303 are arranged in mirror symmetry Is given by h 1 And h 2 ，h 1 And h 2 Is tapered with respect to h (h is the length of the second conductive sheet 302), i.e., h>h 1 >h 2 P (p is the distance between the geometric centers of two adjacent first matching segments 303) remains unchanged.
Since the lengths of the pairs of first matching segments 303 decrease from the side of the first region 3001 close to the second region 3002 to the side of the first region 3001 far from the second region 3002, and/or decrease from the side of the third region 3003 close to the second region 3002 to the side of the third region 3003 far from the second region 3002, the refractive indexes at the two ends of the waveguide can be gradually reduced, the impedance mismatch between the lens structure 10 and the free space can be further reduced, the energy loss of the electromagnetic wave can be more effectively reduced, and the lens antenna efficiency can be more effectively improved.
Alternatively, the spacing between two adjacent second conductive sheets 302 on the waveguide structure is equal to the spacing between two adjacent first matching sections 303, so that the impedance matching is more uniformly distributed in space.
Further, in some embodiments, referring to fig. 17-18, each waveguide structure 300 comprises two first conductive sheets 301 disposed at intervals; in the same waveguide structure 300, each pair of the second conductive sheets 302 is disposed between the two first conductive sheets 301, and when the two second conductive sheets 302 in the same pair are disposed at intervals: each waveguide structure is provided with a fourth region 3004, a fifth region 3005 and a sixth region 3006 along the axial direction, the fifth region 3005 is provided with the second conductive sheet 302, and at least one of the fourth region 3004 and the sixth region 3006 is provided with the second matching unit. Here, when the fourth area 3004 or the sixth area 3006 is not provided with the second matching unit, the second conductive sheet 302 may be separately provided.
The second matching unit comprises at least two pairs of second conducting plates 302 and at least one pair of second matching sections 304 which are symmetrical about the central axis, the two second matching sections 304 in the same pair are respectively arranged on different first conducting plates 301, and each second matching section is arranged between every two adjacent second conducting plates 302 and is connected with every two adjacent second conducting plates 302; in the length direction, the length of the second matching section 304 of the same waveguide structure 300 is smaller than that of the second conductive sheet 302, and the length direction is perpendicular to the axial direction (fig. 17 exemplifies that only the fourth region 3004 is provided with the second matching units and the second matching sections 304 are two pairs, and fig. 18 exemplifies that the fourth region 3004 and the sixth region 3006 are simultaneously provided with the second matching units and each second matching section 304 is two pairs).
Wherein the structure of the second matching segments 304 is similar to that of the second conductive sheet 302, optionally, each pair of the second matching segments 304 has mirror symmetry about the central axis a; optionally, each pair of second matching sections 304 is slip-symmetric about the central axis a (fig. 17-18 take the example of the second conductive sheet 302 being mirror-symmetric and the second matching sections 304 being mirror-symmetric). The second matching section 304 is electrically conductive, optionally the material of the second matching section 304 is the same as the material of the second conductive strip 302.
Since the length of the second matching section 304 is smaller than that of the second conductive sheet 302, the length of the first slot a1 of the slot unit 300A formed by the waveguide structure 300 is larger than that of the second slot a2, and when electromagnetic waves are incident to the edge of the second slot a2 through the edge of the first slot a1, the refractive index gradually decreases; when the fourth region is the incident region of the waveguide structure 300 (taking fig. 17 as an example), the second matching section 304 can implement impedance matching between the incident region of the electromagnetic wave of the lens structure 10 and the free space, so as to reduce the energy loss of the electromagnetic wave; when the fourth region is the exit region of the waveguide structure 300, the second matching section 304 can respectively implement impedance matching between the exit region of the electromagnetic wave of the lens structure 10 and the free space, so as to reduce energy loss of the electromagnetic wave, thereby increasing the transmission distance of the electromagnetic wave and improving the efficiency of the lens antenna.
The fourth gradient rule is that the lengths of the pairs of second matching sections 304 increase from the side of the fourth area 3004 close to the fifth area 3005 to the side of the fourth area 3004 far from the fifth area 3005, and/or increase from the side of the sixth area 3006 close to the fifth area 3005 to the side of the sixth area 3006 far from the fifth area 3005. The number of pairs of the second matching segments of the fourth area 3004 and the sixth area 3006 may be the same or different. Fig. 17 is provided with two pairs of first matching pairs in the fourth area 3004 and the sixth area 3006, respectively Segment 303, and each pair of second conductive plates 302 and each pair of second matching segments 304 are arranged in mirror symmetry as an example, the lengths of the second matching segments 304 are h 3 And h 4 ，h 3 And h 4 Is less than h (h is the length of the second conductive sheet 302) and h 3 And h 4 Is gradually increased, i.e. h>h 4 >h 3 P (p is the distance between the geometric centers of two adjacent second matching segments 304) remains unchanged.
Since the lengths of the pairs of second matching sections 304 increase from the side of the fourth area 3004 close to the fifth area 3005 to the side of the fourth area 3004 far from the fifth area 3005, and/or increase from the side of the sixth area 3006 close to the fifth area 3005 to the side of the sixth area 3006 far from the fifth area 3005, the refractive indexes at the two ends of the waveguide can be gradually reduced, the impedance mismatch between the lens structure 10 and the free space can be further reduced, the energy loss of the electromagnetic wave can be more effectively reduced, and the lens antenna efficiency can be more effectively improved.
The lens structure provided by the embodiment can generate the artificial surface plasmon waveguide by utilizing the multiple pairs of symmetrical second conducting strips, obtains the phase delay to realize the wave beam convergence function by setting the gradual change rule of the number of the waveguide structures between layers or in the layers, and has low dielectric loss in the transmission process of electromagnetic waves along the waveguide, so that the lens antenna with smaller loss, higher efficiency and larger broadband can be realized in practical application. Furthermore, by arranging a plurality of pairs of first matching sections or second matching sections at two ends of each waveguide structure, the impedance mismatch between the lens structure and the free space can be reduced, the energy loss of electromagnetic waves can be reduced more effectively, and the efficiency of the lens antenna in practical application can be improved. In addition, the dielectric layer and the waveguide layer which are alternately arranged in a laminated manner can also realize the assembly preparation of the low-cost lens.
Referring to fig. 19, fig. 19 is a schematic structural diagram of the lens antenna 1 in an embodiment.
In this embodiment, the lens antenna 1 includes the lens structure 10 and the feed array 20 as described in the above embodiments.
The lens structure 10 is described in the above embodiments, and will not be described herein.
Wherein the array of feed sources 20 is arranged parallel to the lens structure 10. The feed array 20 includes a plurality of feed elements. Optionally, please refer to fig. 20 (in the figure, 5 feed units are taken as an example), a plurality of feed units 20a are arranged in a line shape, and the centers of the line shape arrangement are located at the foci of the lens structure 10, so that the feed array 20 can realize multi-beam emission; different beam directions can be obtained by feeding different feed source units of the feed source array 20, thereby realizing beam scanning and being suitable for the application of millimeter wave lens antennas. It can be understood that the feed array 20 in this embodiment may be a radiating element array disposed on the millimeter wave integrated module, and the feed unit 20a may be a radiating element in multiple forms, for example, radiation patches in different forms, such as a rectangle, a ring, and a cross.
The lens antenna provided by the embodiment comprises a feed source array and a lens structure, and the lens antenna with smaller loss, higher efficiency, larger broadband and lower cost can be realized through the symmetrical structure and the gradual change rule of the number of the second conducting strips in the lens structure; the multi-beam emergent and beam scanning can be realized through the arrangement of the feed source array.
Referring to fig. 21 and 22, fig. 21 and 22 are schematic structural views of a lens antenna 1 in another embodiment.
In this embodiment, the lens antenna 1 includes the lens structure 10 and the feed array 20 as described in the above embodiments, a first metal plate 30, and a second metal plate 40 spaced apart from the first metal plate 20. The lens structure 10 and the feed array 20 are disposed between a first metal plate 30 and a second metal plate 40, respectively.
The lens structure 10 and the feed source array 20 are described in the above embodiments, and are not described in detail here. Also, according to the above-described embodiment, different arrangement situations of the first direction of the lens structure 10 by the waveguide layer 200 and the dielectric layer 100 can be applied to application scenarios with different polarization directions.
Optionally, referring to fig. 21, the first directions of the waveguide layer 200 and the dielectric layer 100 are respectively parallel to the first metal plate 30 and the second metal plate 40 (taking the waveguide layer 200 as a waveguide structure 300 and each pair of the second conductive sheets 302 is symmetrically disposed in a sliding manner, the first direction is perpendicular to the paper surface in the drawing), so that the lens structure 10 can be suitable for a vertical polarization application scenario, and the polarization directions of the lens antenna 1 are respectively perpendicular to the first metal plate 30 and the second metal plate 40.
Optionally, referring to fig. 22, the first directions of the waveguide layer 200 and the dielectric layer 100 are perpendicular to the first metal plate 30 and the second metal plate 40, respectively (the first direction is parallel to the paper in the drawing), so that the lens structure 10 can be suitable for a horizontally polarized application scenario, and the polarization directions of the lens antenna 1 are parallel to the first metal plate 30 and the second metal plate 40, respectively.
The first metal plate 30 and the second metal plate 40 can be used for reflecting internal electromagnetic waves and shielding external interference. By placing the lens structure 10 and the feed array 20 between the first metal plate 30 and the second metal plate 40, leakage of electromagnetic waves radiated by the feed can be reduced, thereby improving the efficiency of the lens antenna 1 and improving the structural strength of the lens antenna 1. Alternatively, the first flat metal plate 30 and the second flat metal plate 40 are made of super-hard aluminum plate, but may be made of other metal materials such as stainless steel.
The lens antenna provided by the embodiment comprises a first metal flat plate, a second metal flat plate, a feed source array and a lens structure, and on one hand, the lens antenna with smaller loss, higher efficiency, larger broadband and lower cost can be realized through the symmetrical structure and the gradual change rule of the number of the second conducting plates in the lens structure; on the other hand, leakage of electromagnetic waves radiated by the feed source can be reduced through the arrangement of the first metal flat plate and the second metal flat plate, so that the efficiency of the antenna is improved, and meanwhile, the structural strength of the antenna is improved; moreover, multi-beam emergent and beam scanning can be realized through the arrangement of the feed source array.
The application also provides an electronic device 2, the electronic device 2 includes the lens antenna 1 as the above embodiment, because the loss of the lens antenna 1 is less, the efficiency is higher, the broadband is bigger and the cost is lower, and can realize multi-beam emergence and beam scanning, therefore the electronic device 2 can realize high efficiency, high gain, low-cost beam scanning, can be applicable to the receiving and dispatching of 5G communication millimeter wave signals, simultaneously, the focal length of the lens antenna 1 is short, the size is small, easily integrate in the electronic device 2, can reduce the occupation space of the lens antenna 1 in the electronic device 2 simultaneously.
Optionally, referring to fig. 23, the electronic device 2 further comprises a detection module 160, a switch module 161, and a control module 162.
The detecting module 160 is configured to obtain a beam signal strength of the electromagnetic wave radiated by the lens antenna 1 when the feed unit 20a is in an operating state, and also may be configured to detect and obtain parameters such as power, an electromagnetic wave Absorption ratio or a Specific Absorption Rate (SAR) of the electromagnetic wave received by the lens antenna 1 when the feed unit 20a is in the operating state.
And a switch module 161 connected to the switch module 161 for selectively conducting a connection path with any one of the feed source units 20 a. Alternatively, the switch module 161 may include an input terminal connected to the control module 162 and a plurality of output terminals connected to the plurality of feed source units 20a in a one-to-one correspondence. The switch module 161 may be configured to receive a switching instruction sent by the control module 162, so as to control on and off of each switch in the switch module 161, and thus control on and off connection between the switch module 161 and any one of the feed source units 20a, so that any one of the feed source units 20a is in a working (on) state.
And the control module 162 is respectively connected with the detection module 160 and the switch module 161, and controls the switch module 161 according to the beam signal strength, so that the feed source unit 20a corresponding to the strongest beam signal strength is in a working state.
Therefore, any one of the feed source units 20a can work through the detection module 160, the switch module 161 and the control module 162 to obtain different beam directions, so that beam scanning is realized, and the method can be applied to the millimeter wave lens antenna; moreover, the beam scanning process does not need a shifter and an attenuator, so that the cost is greatly reduced.
Taking the feed source array 20 including five feed source units as an example, the detection module 160 may correspondingly obtain five beam signal strengths, and screen out the strongest beam signal strength from the five beam signal strengths, and use the feed source unit 20a corresponding to the strongest beam signal strength as a target feed source unit, and the switching instruction sent by the control module 162 controls the conductive connection between the switch module 161 and the target feed source unit, so that the target feed source unit is in a working (conductive) state. The simulation resulted in a beam scanning pattern as shown in figure 24. According to the simulation result, the mobile phone can realize the high-efficiency, high-gain and low-cost beam scanning of the 6G millimeter wave of the mobile phone by arranging the two lens antennas 1.
Optionally, the electronic device 2 includes a plurality of lens antennas 1, and the plurality of lens antennas 1 are distributed on different sides of a middle frame of the electronic device 2. Optionally, referring to fig. 25 for assistance, the middle frame of the electronic device 2 includes a first side 181 and a third side 183 that are disposed opposite to each other, and a second side 182 and a fourth side 184 that are disposed opposite to each other, where the second side 182 is connected to one ends of the first side 181 and the third side 183, and the fourth side 184 is connected to the other ends of the first side 181 and the third side 183. At least two sides of the first side 181, the second side 182, the third side 183, and the fourth side 184 are respectively provided with the lens antenna 1.
Taking the example that the electronic device 2 includes two lens antennas 1, optionally, referring to fig. 26, the two lens antennas 1 are disposed on two long sides (for example, the first side 181 and the third side 183) of the mobile phone, that is, the two long sides can cover spaces on two sides of the mobile phone.
It should be noted that the electronic device 2 in the above embodiments includes, but is not limited to, any product and component with an antenna transceiving function, such as a mobile phone, a tablet computer, a display, a smart watch, and the like. The division of each unit in the electronic device 2 is only used for illustration, and in other embodiments, the electronic device 2 may be divided into different modules as needed to complete all or part of the functions of the electronic device 2.
The technical features of the embodiments described above may be arbitrarily combined, and for the sake of brevity, all possible combinations of the technical features in the embodiments described above are not described, but should be considered as being within the scope of the present specification as long as there is no contradiction between the combinations of the technical features.
The above-mentioned embodiments only express several embodiments of the present application, and the description thereof is more specific and detailed, but not construed as limiting the scope of the invention. It should be noted that, for a person skilled in the art, several variations and modifications can be made without departing from the concept of the present application, which falls within the scope of protection of the present application. Therefore, the protection scope of the present patent shall be subject to the appended claims.
Claims (23)
1. A lens structure, comprising:
a plurality of dielectric layers;
the multilayer waveguide layer, the waveguide layer with the dielectric layer sets up along the alternative stromatolite of first direction, the waveguide layer includes:
one or more waveguide structures, a plurality of which are spaced and arranged in parallel; the waveguide structure includes a first conductive sheet and at least one pair of second conductive sheets, each pair of the second conductive sheets being symmetrically disposed about a central axis, a plurality of the second conductive sheets on the same side of the central axis being connected to each other through the first conductive sheet;
A first gradual change rule of the number of the second conducting strips is arranged among a plurality of waveguide structures on the same axis in the plurality of waveguide layers, and/or a second gradual change rule of the number is arranged among the plurality of waveguide structures in the plurality of waveguide layers; the axis is a straight line which passes through any waveguide layer and is parallel to the first direction;
the first gradual change rule is that the number decreases symmetrically from the central position of the axis to the waveguide structures at both sides, and the second gradual change rule is that the number decreases symmetrically from the arrangement center of the plurality of waveguide structures of the waveguide layer to both sides.
2. The lens structure of claim 1, wherein when the number of waveguide layers is at least three, the first gradient rule exists among a plurality of waveguide layers on the same axis; and/or when the waveguide structures of the waveguide layer are at least three, the second gradient rule is formed among a plurality of waveguide structures of the waveguide layer;
when the number of the waveguide layers is one or two, the waveguide layers comprise at least three waveguide structures, and the second gradual change rule is formed among a plurality of waveguide structures of the waveguide layers.
3. A lens structure according to claim 2, wherein said first law of progression is applied between a plurality of said waveguide layers lying on the same axis:
said number of said plurality of waveguide structures in said waveguide layer is the same; or the second gradient rule is formed among a plurality of waveguide structures in the waveguide layer.
4. The lens structure of claim 2, wherein the second grading law is applied between a plurality of the waveguide structures in the waveguide layer:
the number of the waveguide structures on the same axis in the waveguide layers is the same; and the first gradual change rule is formed among a plurality of waveguide structures on the same axis in the waveguide layers.
5. The lens structure of claim 1, wherein each pair of the second conductive sheets is arranged mirror-symmetrically about the central axis; or, each pair of the second conducting strips is arranged in a sliding symmetry mode around the central shaft.
6. The lens structure of claim 1, wherein the plurality of second conductive sheets on the same side of the central axis in the waveguide structure are equally spaced and arranged in parallel, and the second conductive sheets have the same length.
7. A lens structure according to any one of claims 1 to 6, wherein each said waveguide structure comprises one said first conducting strip, each said pair of second conducting strips being disposed axially on either side of said first conducting strip.
8. The lens structure according to claim 7, wherein each waveguide structure is provided with a first region, a second region and a third region along the axial direction, the second conductive sheet is provided in the second region, and at least one of the first region and the third region is provided with a first matching unit;
the first matching unit comprises at least one pair of first matching sections which are symmetrical about the central axis, and two first matching sections in the same pair are respectively arranged on two sides of the first conducting strip;
in the length direction, the length of the first matching section of the same waveguide structure is smaller than that of the second conducting strip, and the length direction is perpendicular to the axial direction.
9. The lens structure of claim 8, wherein the lengths of the pairs of first matching sections decrease from a side of the first region near the second region to a side of the first region away from the second region, and/or decrease from a side of the third region near the second region to a side of the third region away from the second region.
10. The lens structure of claim 8, wherein each pair of the first matching segments is mirror symmetric about the central axis; alternatively, each pair of the first matching segments is slip-symmetric about the central axis.
11. The lens structure of claim 8, wherein a spacing between two adjacent second conductive strips on the waveguide structure is equal to a spacing between two adjacent first matching segments.
12. A lens structure according to any one of claims 1 to 6, wherein each waveguide structure comprises two spaced apart first conductive sheets; in the same waveguide structure, each pair of the second conducting strips is arranged between the two first conducting strips, and the two second conducting strips in the same pair are arranged at intervals.
13. The lens structure according to claim 12, wherein each waveguide structure is provided with a fourth region, a fifth region and a sixth region along the axial direction of the first conductive sheet, the fifth region is provided with the second conductive sheet, and at least one of the fourth region and the sixth region is provided with a second matching unit;
the second matching unit comprises at least two pairs of second conducting strips and at least one pair of second matching sections which are symmetrical about the central axis, the two second matching sections in the same pair are respectively arranged on different first conducting strips, and each second matching section is arranged between and connected with two adjacent second conducting strips;
In the length direction, the length of the second matching section of the same waveguide structure is smaller than that of the second conducting strip, and the length direction is perpendicular to the axial direction.
14. The lens structure of claim 13, wherein the length of the plurality of pairs of second matching segments increases from a side of the fourth region closer to the fifth region to a side of the fourth region farther from the fifth region, and/or increases from a side of the sixth region closer to the fourth region to a side of the sixth region farther from the fourth region.
15. The lens structure according to claim 13, characterized in that each pair of second matching segments is mirror symmetric about the central axis; alternatively, each pair of the second matching sections is in sliding symmetry about the central axis.
16. A lens antenna, comprising:
a feed source array; and
a lens structure as claimed in any one of claims 1 to 15 arranged in parallel with the array of feeds.
17. The lens antenna of claim 16, further comprising:
a first metal plate;
the second metal flat plate is parallel to the first metal flat plate and is arranged at intervals;
Wherein the lens structure and the feed array are respectively arranged between the first metal flat plate and the second metal flat plate.
18. The lens antenna of claim 17, wherein the first direction is parallel to the first metal plate and the second metal plate, respectively.
19. The lens antenna of claim 18, wherein the polarization directions of the lens antenna are perpendicular to the first metal plate and the second metal plate, respectively.
20. The lens antenna of claim 17, wherein the first direction is perpendicular to the first and second metal plates, respectively.
21. The lens antenna of claim 20, wherein the polarization directions of the lens antenna are parallel to the first metal plate and the second metal plate, respectively.
22. An electronic device comprising a lens antenna according to any one of claims 16-21.
23. The electronic device of claim 22, wherein the feed array comprises a plurality of feed units, the electronic device further comprising:
the detection module is used for acquiring the beam signal intensity of the lens antenna when the feed source unit is in a working state;
The switch module is connected with the feed source array and used for selectively conducting a connecting path with any one feed source unit;
and the control module is respectively connected with the detection module and the switch module and is used for controlling the switch module according to the beam signal intensity so as to enable the feed source unit corresponding to the strongest beam signal intensity to be in a working state.
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