The present invention claims priority under 35 U.S.C. § 119 to Japanese Application No. 2018-189124 filed on Oct. 4, 2018 the entire contents of which are incorporated herein by reference.
The present disclosure relates to a waveguide device and an antenna device.
The specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent Application Publication No. 1 331 688, the specification of U.S. Pat. No. 10,027,032, the specification of U.S. Patent Publication No. 2018/375219, each disclose a waveguide device in which an electromagnetic wave propagates along a ridge that is surrounded by an artificial magnetic conductor. In the waveguide devices disclosed in the specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent Application Publication No. 1 331 688, the specification of U.S. Pat. No. 10,027,032, the specification of US Patent Publication No. 2018/375219, a plurality of electrically conductive rods that are arranged along row and column directions constitute an artificial magnetic conductor. Each of these waveguide devices, as a whole, includes a pair of opposing electrically conductive plates. One of the electrically conductive plates has a ridge that protrudes toward the other electrically conductive plate, and an artificial magnetic conductor that are located on both sides of the ridge. Via a gap, an upper face (which is an electrically-conductive face) of the ridge is opposed to the electrically conductive surface of the other electrically conductive plate. An electromagnetic wave having a wavelength that falls within a propagation-restricted band of the artificial magnetic conductor propagates in a space (gap) between this electrically conductive surface and the upper face of the ridge, in a manner of following along the ridge. A waveguide of this kind will be referred to as a WRG (Waffle-iron Ridge waveguide) or a WRG waveguide.
The specification of U.S. Patent Publication No. 2018/375219 discloses a waveguide device in which two electrically conductive plates opposing each other both have a through hole, such that an electrically-conductive waveguiding wall that surrounds at least a part of the space between such through holes is provided. Through the space surrounded by the waveguiding wall, an electromagnetic wave can be propagated between a plurality of layers.
Example embodiments of the present disclosure provide techniques of improving impedance matching in waveguide devices in each of which an electromagnetic wave is propagated between a plurality of layers.
A waveguide device according to an example embodiment of the present disclosure includes a first electrically conductive member including an electrically conductive surface and a first through hole, a second electrically conductive member including a plurality of electrically conductive rods, each of the first electrically conductive member and the second electrically conductive member including a leading end opposing the electrically conductive surface, and a second through hole which overlaps the first through hole as viewed along an axial direction of the first through hole, and an electrically-conductive waveguiding wall surrounding at least a portion of a space between the first through hole and the second through hole, the waveguiding wall being surrounded by the plurality of electrically conductive rods and allowing an electromagnetic wave to propagate between the first through hole and the second through hole. The waveguiding wall includes a stepped portion or a slope on an inner side.
An antenna device according to an example embodiment of the present disclosure includes a first electrically conductive member including a first electrically conductive surface on a front side, a second electrically conductive surface on a rear side, and a slot extending through and between the first electrically conductive surface and the second electrically conductive surface. The first electrically conductive surface has a shape that defines a horn surrounding the slot. The horn includes a pair of inner wall surfaces extending along a first direction which is perpendicular or substantially perpendicular to an E plane of the slot. A root of each of the pair of inner wall surfaces includes a protrusion extending along the first direction.
An antenna device according to still another example embodiment of the present disclosure includes an electrically conductive member including a first electrically conductive surface on a front side, a second electrically conductive surface on a rear side, and one or more slots extending through and between the first electrically conductive surface and the second electrically conductive surface. The first electrically conductive surface has a shape that defines one or more horns respectively surrounding the one or more slots, and two recesses located on opposite sides of the one or more horns. The one or more horns and the two recesses are arranged side by side in one row, with electrically conductive walls being located therebetween. Each of the electrically conductive walls located between the one or more horns and two recesses includes a central portion and sites on opposite sides of the central portion, the central portion and sites being distanced by two grooves.
According to example embodiments of the present disclosure, impedance matching in waveguide devices in each of which an electromagnetic wave is propagated between a plurality of layers is improved.
The above and other elements, features, steps, characteristics and advantages of the present disclosure will become more apparent from the following detailed description of the example embodiments with reference to the attached drawings.
Hereinafter, specific exemplary constructions according to example embodiments of the present disclosure will be described. Note however that unnecessarily detailed descriptions may be omitted. For example, detailed descriptions on what is well known in the art or redundant descriptions on what is substantially the same constitution may be omitted. This is to avoid lengthy description, and facilitate the understanding of those skilled in the art. The accompanying drawings and the following description, which are provided by the inventors so that those skilled in the art can sufficiently understand the present disclosure, are not intended to limit the scope of claims. In the present specification, identical or similar constituent elements are denoted by identical reference numerals.
In
In the following description, “the front side” means the side at which an electromagnetic wave is radiated or the side at which an electromagnetic wave arrives, whereas “the rear side” means the opposite side to the front side. In the present example embodiment, the front side is the side in the +Z direction, whereas the rear side is the side in the −Z direction.
The first conductive member 110 has a transmission section 116 and a reception section 117 on its face on the front side (i.e., the +Z side). The first conductive member 110 has flat conductive surfaces 110a and 110b, respectively on its face on the front side and the opposite face thereof. The conductive surface 110b on the rear side is opposed to the conductive surface 120a on the +Z side of the second conductive member 120. The second conductive member 120 includes a plurality of electrically conductive rods 124 each having a leading end opposing the conductive surface 110b of the first conductive member 110. The second conductive member 120 also has a conductive surface 120b on its face on the -Z side. The conductive surface 120b is opposed to the conductive surface 130a of the third conductive member 130 on the +Z side. The third conductive member 130 includes a plurality of conductive rods 134 each having a leading end opposing the conductive surface 120b of the second conductive member 120 on the −Z side.
In the reception section 117, the first conductive member 110 includes a plurality of antenna elements 111B that are arranged in a two-dimensional array along the X direction and the Y direction. In the illustrated example, the reception section 117 includes 16 antenna elements 111B that are arranged in 4 rows by 4 columns; however, the number of antenna elements 111B in the reception section 117 is not limited to sixteen. Although the waveguide device 100 of the present example embodiment has both of the transmission section 116 and the reception section 117, it may only have either one of them.
Among the three through holes 113A arranged side by side along the Y direction, the through hole 113A in the middle is surrounded by a waveguiding wall 160. The waveguiding wall 160 is connected to the conductive surface 110b on the rear side. The waveguiding wall 160 may be formed integrally with the first conductive member 110, so as to constitute a part of the first conductive member 110. The waveguiding wall 160 may be produced as an independent member from the first conductive member 110, and thereafter mounted on the first conductive member 110.
The conductive wall 118 being located on either side (regarding the Y direction) of each antenna element 111A and extending along the X direction includes a central portion and grooves 118c which are formed on opposite sides of the central portion. As viewed from the +Z direction, the central portion of the conductive wall 118 is at a position that is shifted along the oscillation direction (i.e., the Y direction) of the electric field from the center of the first through hole 113A. The grooves 118c can be formed by removing portions of the conductive wall 118 by cutting, for example. The top of each conductive wall 118 extending along the X direction is partitioned by the two grooves 118c into a conductive wall 118b (which is the central portion) and conductive walls 118a.
The following effects are attained by providing the grooves 118c, so as to leave a central portion, in the conductive wall 118 being located on either side (regarding the Y direction) of each antenna element 111A and extending along the X direction. First, isolation between electromagnetic waves to be radiated from the three antenna elements 111A is improved. Stated otherwise, electromagnetic waves can be restrained from propagating or leaking in any direction other than the desired direction. Furthermore, the frequency characteristics of the three antenna elements 111A can be stabilized. For example, a stable directivity can be realized even with varying frequencies.
In the present example embodiment, the exposed face of each conductive wall 118a (i.e., the face opposing the side face of the conductive wall 118b) is a curved surface. On the other hand, the conductive wall 118b is cylindrical. The shapes of the conductive walls 118a and 118b are not limited to the illustrated shapes. For example, the shape of the conductive wall 118b may be a prismatic shape, a frustum of a cone, or a frustum of a pyramid. The depth and width of each groove 118c are set to dimensions such that desired radiation characteristics will be provided.
As shown in
In the present example embodiment, the first conductive member 110 is illustrated as including more than one antenna element 111A for transmission purposes; however, the first conductive member 110 may only include a single antenna element 111A. In that case, too, two recesses 119 having an opening of a similar shape to the opening of that antenna element 111A may be provided on both sides of the antenna element 111A. Between each recess 119 and the antenna element 111A, a conductive wall 118 having two grooves 118c as aforementioned may be provided. With such structure, isolation between electromagnetic waves to be radiated can be enhanced, and the frequency characteristics can be improved.
The waveguiding wall 160 does not need to be entirely electrically conductive; it suffices if its end face 165 opposing the conductive surface 120a of the second conductive member 120 is electrically-conductive material.
In the example of
On the inner side, the waveguiding wall 160 has a pair of first inner wall surfaces 164A which are parallel or substantially parallel to the Y direction (i.e., the E plane direction) and a pair of second inner wall surfaces 164B which are parallel or substantially parallel to the X direction (i.e., the H plane direction). Each of the pair of first inner wall surfaces 164A has a stepped portion 162 extending in parallel to the Y direction, the stepped portion 162 constituting a recessed portion of the waveguiding wall 160. The stepped portions 162 serve to expand the rear side (the −Z side) of the first through hole 113A. By thus providing the stepped portions 162 on the inner side of the waveguiding wall 160, impedance matching is improved.
As used herein, the “E plane” is a plane that contains electric field vectors to be created in the central portion of the first through hole 113A (slot), such that the E plane extends through the center of the first through hole 113A and is substantially perpendicular to the conductive surface 110b of the first conductive member 110. The “H plane” is a plane that contains magnetic field vectors to be created in the central portion of the first through hole 113A. In the present example embodiment, the E plane is parallel to the YZ plane, whereas the H plane is parallel to the XZ plane.
Although the stepped portion 162 in the present example embodiment includes a single step, it may alternatively include two or more steps. Moreover, the shape of the stepped portion 162 is not limited to what is shown. So long as impedance matching is achieved, the shape of the stepped portion 162 may be altered as appropriate. Without being limited to a staircase, the shape of the inner side of the waveguiding wall 160 may be an inclined plane, for example. Similar effects can also be obtained by adopting a structure with a pair of slopes that allow the opening to gradually expand in the −Z direction, instead of the stepped portion 162 shown in
On the front side (the +Z side) of the pair of second inner wall surfaces 164B, a pair of protrusions 118d are provided that protrude from the inner wall surface of the first through hole 113A (which is continuous with the pair of second inner wall surfaces 164B) and extend along the X direction.
Details of the structure and possible variants of the waveguiding wall 160 are disclosed in the specification of U.S. Patent Publication No. 2018/375219. The entire disclosure of the specification of U.S. Patent Publication No. 2018/375219 is incorporated herein by reference.
Thus, the waveguiding wall 160 in the present example embodiment includes the pair of first inner wall surfaces 164A which are parallel to the E plane and the pair of second inner wall surfaces 164B which are parallel to the H plane. The waveguiding wall 160 includes one or more stepped portions or one or more slopes on the inner side. The stepped portions or slopes are disposed on the pair of first inner wall surfaces 164A. As viewed from a direction which is perpendicular to the conductive surface 110b of the first conductive member 110, the region that is surrounded by the first and second through holes 113A and 123 and the inner wall surface of the waveguiding wall 160 has an H shape that includes a lateral portion extending along a first direction and a pair of vertical portions extending from both ends of the lateral portion along a second direction which intersects the first direction. The inner wall surface of the waveguiding wall 160 includes a pair of first inner wall surfaces 164A that are parallel to the pair of vertical portions. The stepped portions or slopes are disposed on an edge of the pair of first inner wall surfaces 164A by which the second conductive member 120 is located.
The antenna device according to the present example embodiment includes the first conductive member 110 having the first conductive surface 110a on the front side, the second conductive surface 110b on the rear side, and one or more slots 113A extending through and between the first conductive surface 110a and the second conductive surface 110b. The first conductive surface 110a has a shape that defines one or more horns respectively surrounding the one or more slots 113A. Each horn has a pair of inner wall surfaces 118 extending along a first direction which is perpendicular or substantially perpendicular to the E plane of the slot. The root of each of the pair of inner wall surfaces 118 has a protrusion 118d extending along the first direction.
As shown in
The waveguide device 100 may further include a second conductive member 120 having a third conductive surface 120a opposing the second conductive surface 110b. The second conductive member 120 includes a through hole for allowing an electromagnetic wave to propagate reciprocally between itself and the slot, or a waveguide member defining a ridge waveguide for allowing an electromagnetic wave to propagate reciprocally between itself and the slot.
The first ridge 122A and the second ridge 122B has an upper face (hereinafter referred to as a “waveguide face”) opposing the conductive surface 110b of the first conductive member 110. The waveguide face of each ridge has a plurality of recesses. Each of the first ridge 122A and the second ridge 122B has a port 125 (i.e., a through hole) provided at one end. Although the ports 125 are shown to have an H shape in the illustrated example, its shape is not limited thereto.
A plurality of electrically-conductive rods 124 are provided on the second conductive member 120. The plurality of rods 124 surround the first ridge 122A, the second ridge 122B, the second through holes 123, and the ports 125.
The third rods 124C have their corners significantly chamfered. Each third rod 124C is shaped so that its cross section parallel to the XY plane is gradually pointed. In a cross section taken perpendicular to the axial direction of each third rod 124C, the dimensions of its outer shape decrease from the root toward the leading end of the third rod 124C. As used herein, the axis of a rod refers to a straight line which passes through the centroid of that rod and which is perpendicular to the conductive surface 120a.
At the root of each third rod 124C, a sloped surface is provided which inclines, toward the bottom, outwardly from the center of the axis of the third rod 124C.
Each ridge-side rod 124A has a shape which resembles a quadrangular prism, with its corners being chamfered to a lesser extent, into a curved surface, than are the corners of each third rod 124C. Note that chamfering is optional, and may be omitted.
Regarding the side faces of each ridge-side rod 124A, at least a side face 124d that is opposed to a side face of the ridge 122A, 122B has a right angle, or an angle close to a right angle, with respect to the conductive surface 120a of the second conductive member 120. At the root of any side face of each ridge-side rod 124A that is not opposed to the side face of the ridge 122A, 122B, a sloped surface is provided which inclines, toward the bottom, outwardly from the center of the axis of the ridge-side rod 124A. An “angle which is close to a right angle” means an angle which is closer to a right angle than is the angle between the conductive surface 120a and the side face of at least a rod 124C that is adjacent to the ridge-side rod 124A.
Usually, antenna design is easier without a sloped surface being provided on the rods 124. On the other hand, impedance matching is easier to achieve when the rods 124 have a sloped surface. Therefore, in order to promptly design the antenna while achieving impedance matching, in the present example embodiment, among the side faces of each rod 124, those side faces which are not opposed to the side face of the ridge 122A, 122B are sloped. Furthermore, recesses are made in the ridges 122A and 122B for assisting in impedance matching.
The fact that a sloped surface being provided on the rods 124 improves the degree of impedance matching is disclosed in the specification of U.S. Pat. No. 10,027,032. The entire disclosure of the specification of U.S. Pat. No. 10,027,032 is incorporated herein by reference.
A plurality of rods surround the second through hole 123. Also, a plurality of rods surround each port 125. These rods are through hole-side rods 124B.
Each through hole-side rod 124B has a shape resembling a quadrangular prism, and has its corners chamfered to a greater extent, into a curved surface, than are the corners of each third rod 124C. Note that chamfering of the corners is optional, and may be omitted.
Regarding the side faces of each through hole-side rod 124B, at least a side face 124d of the through hole-side rod 124B that is opposed to the through hole has a right angle, or an angle close to a right angle, with respect to the conductive surface 120a of the second conductive member 120. At the root of any side face of the through hole-side rod 124B that is not opposed to the through hole, a sloped surface is provided which inclines, toward the bottom, outwardly from the center of the axis of the through hole-side rod 124B.
Next, a variant of the present example embodiment will be described.
The waveguiding wall 160 may surround at least a part of the space between the first through hole 113A and the second through hole 123, without having to entirely surround this space. With such construction, the waveguiding wall 160 allows an electromagnetic wave to be propagated between the first through hole 113A and the second through hole 123. In
In the example of
Next, a fundamental construction of a waffle-iron ridge waveguide (WRG) that is used in an example embodiment of the present disclosure will be described.
A ridge waveguide which is disclosed in the aforementioned the specification of U.S. Pat. No. 8,779,995, the specification of U.S. Pat. No. 8,803,638, the specification of European Patent Application Publication No. 1331688, the specification of U.S. Pat. No. 10,027,032, the specification of U.S. Patent Publication No. 2018/375219 is provided in a waffle iron structure which is capable of functioning as an artificial magnetic conductor. A ridge waveguide in which such an artificial magnetic conductor is utilized based on the present disclosure is able to realize an antenna feeding network with low losses in the microwave or the millimeter wave band. Moreover, use of such a ridge waveguide allows antenna elements to be disposed with a high density. Such a ridge waveguide may be referred to as a waffle-iron ridge waveguide (WRG) in the present specification. Hereinafter, an exemplary fundamental construction and operation of a waffle-iron ridge waveguide will be described.
An artificial magnetic conductor is a structure which artificially realizes the properties of a perfect magnetic conductor (PMC), which does not exist in nature. One property of a perfect magnetic conductor is that “a magnetic field on its surface has zero tangential component”. This property is the opposite of the property of a perfect electric conductor (PEC), i.e., “an electric field on its surface has zero tangential component”. Although no perfect magnetic conductor exists in nature, it can be embodied by an artificial structure, e.g., an array of a plurality of electrically conductive rods. An artificial magnetic conductor functions as a perfect magnetic conductor in a specific frequency band which is defined by its structure. An artificial magnetic conductor restrains or prevents an electromagnetic wave of any frequency that is contained in the specific frequency band (propagation-restricted band) from propagating along the surface of the artificial magnetic conductor. For this reason, the surface of an artificial magnetic conductor may be referred to as a high impedance surface.
See
On the second conductive member 120, a ridge-like waveguide member 122 is provided among the plurality of conductive rods 124. More specifically, stretches of an artificial magnetic conductor are present on both sides of the waveguide member 122, such that the waveguide member 122 is sandwiched between the stretches of artificial magnetic conductor on both sides. As can be seen from
On both sides of the waveguide member 122, the space between the surface 126 of each stretch of artificial magnetic conductor and the conductive surface 110b of the first conductive member 110 does not allow an electromagnetic wave of any frequency that is within a specific frequency band to propagate. This frequency band is called a “prohibited band”. The artificial magnetic conductor is designed so that the frequency of a signal wave to propagate in the waveguide device 100 (which may hereinafter be referred to as the “operating frequency”) is contained in the prohibited band. The prohibited band may be adjusted based on the following: the height of the conductive rods 124, i.e., the depth of each groove formed between adjacent conductive rods 124; the diameter of each conductive rod 124; the interval between conductive rods 124; and the size of the gap between the leading end 124a and the conductive surface 110b of each conductive rod 124.
Next, with reference to
The width (i.e., the size along the X direction and the Y direction) of the conductive rod 124 may be set to less than λm/2. Within this range, resonance of the lowest order can be prevented from occurring along the X direction and the Y direction. Since resonance may possibly occur not only in the X and Y directions but also in any diagonal direction in an X-Y cross section, the diagonal length of an X-Y cross section of the conductive rod 124 is also preferably less than λm/2. The lower limit values for the rod width and diagonal length will conform to the minimum lengths that are producible under the given manufacturing method, but is not particularly limited.
The distance from the root 124b of each conductive rod 124 to the conductive surface 110b of the first conductive member 110 may be longer than the height of the conductive rods 124, while also being less than λm/2. When the distance is λm/2 or more, resonance may occur between the root 124b of each conductive rod 124 and the conductive surface 110b, thus reducing the effect of signal wave containment.
The distance from the root 124b of each conductive rod 124 to the conductive surface 110b of the first conductive member 110 corresponds to the spacing between the first conductive member 110 and the second conductive member 120. For example, when a signal wave of 76.5±0.5 GHz (which belongs to the millimeter band or the extremely high frequency band) propagates in the waveguide, the wavelength of the signal wave is in the range from 3.8934 mm to 3.9446 mm. Therefore, Am equals 3.8934 mm in this case, so that the spacing between the first conductive member 110 and the second conductive member 120 may be less than a half of 3.8934 mm. So long as the first conductive member 110 and the second conductive member 120 realize such a narrow spacing while being disposed opposite from each other, the first conductive member 110 and the second conductive member 120 do not need to be strictly parallel. Moreover, when the spacing between the first conductive member 110 and the second conductive member 120 is less than λm/2, a whole or a part of the first conductive member 110 and/or the second conductive member 120 may be shaped as a curved surface. On the other hand, the conductive members 110 and 120 each have a planar shape (i.e., the shape of their region as perpendicularly projected onto the XY plane) and a planar size (i.e., the size of their region as perpendicularly projected onto the XY plane) which may be arbitrarily designed depending on the purpose.
Although the conductive surface 120a is illustrated as a plane in the example shown in
The distance L2 from the leading end 124a of each conductive rod 124 to the conductive surface 110b is set to less than λm/2. When the distance is λm/2 or more, a propagation mode where electromagnetic waves reciprocate between the leading end 124a of each conductive rod 124 and the conductive surface 110b may occur, thus no longer being able to contain an electromagnetic wave. Note that, among the plurality of conductive rods 124, at least those which are adjacent to the waveguide member 122 do not have their leading ends in electrical contact with the conductive surface 110b. As used herein, the leading end of a conductive rod not being in electrical contact with the conductive surface means either of the following states: there being an air gap between the leading end and the conductive surface; or the leading end of the conductive rod and the conductive surface adjoining each other via an insulating layer which may exist in the leading end of the conductive rod or in the conductive surface.
The interspace between two adjacent conductive rods 124 among the plurality of conductive rods 124 has a width of less than λm/2, for example. The width of the interspace between any two adjacent conductive rods 124 is defined by the shortest distance from the surface (side face) of one of the two conductive rods 124 to the surface (side face) of the other. This width of the interspace between rods is to be determined so that resonance of the lowest order will not occur in the regions between rods. The conditions under which resonance will occur are determined based by a combination of: the height of the conductive rods 124; the distance between any two adjacent conductive rods; and the capacitance of the air gap between the leading end 124a of each conductive rod 124 and the conductive surface 110b. Therefore, the width of the interspace between rods may be appropriately determined depending on other design parameters. Although there is no clear lower limit to the width of the interspace between rods, for manufacturing ease, it may be e.g. λm/16 or more when an electromagnetic wave in the extremely high frequency range is to be propagated. Note that the interspace does not need to have a constant width. So long as it remains less than λm/2, the interspace between conductive rods 124 may vary.
The arrangement of the plurality of conductive rods 124 is not limited to the illustrated example, so long as it exhibits a function of an artificial magnetic conductor. The plurality of conductive rods 124 do not need to be arranged in orthogonal rows and columns; the rows and columns may be intersecting at angles other than 90 degrees. The plurality of conductive rods 124 do not need to form a linear array along rows or columns, but may be in a dispersed arrangement which does not present any straightforward regularity. The conductive rods 124 may also vary in shape and size depending on the position on the second conductive member 120.
The surface 126 of the artificial magnetic conductor that are constituted by the leading ends 124a of the plurality of conductive rods 124 does not need to be a strict plane, but may be a plane with minute rises and falls, or even a curved surface. In other words, the conductive rods 124 do not need to be of uniform height, but rather the conductive rods 124 may be diverse so long as the array of conductive rods 124 is able to function as an artificial magnetic conductor.
Each conductive rod 124 does not need to have a prismatic shape as shown in the figure, but may have a cylindrical shape, for example. Furthermore, each conductive rod 124 does not need to have a simple columnar shape. The artificial magnetic conductor may also be realized by any structure other than an array of conductive rods 124, and various artificial magnetic conductors are applicable to the waveguide device of the present disclosure. Note that, when the leading end 124a of each conductive rod 124 has a prismatic shape, its diagonal length is preferably less than λm/2. When the leading end 124a of each conductive rod 124 is shaped as an ellipse, the length of its major axis is preferably less than λm/2. Even when the leading end 124a has any other shape, the dimension across it is preferably less than λm/2 even at the longest position.
The height of each conductive rod 124 (in particular, those conductive rods 124 which are adjacent to the waveguide member 122), i.e., the length from the root 124b to the leading end 124a, may be set to a value which is shorter than the distance (i.e., less than λm/2) between the conductive surface 110b and the conductive surface 120a, e.g., λo/4.
The width of the waveguide face 122a of the waveguide member 122, i.e., the size of the waveguide face 122a along a direction which is orthogonal to the direction that the waveguide member 122 extends, may be set to less than λm/2 (e.g. λo/8). If the width of the waveguide face 122a is λm/2 or more, resonance will occur along the width direction, which will prevent any WRG from operating as a simple transmission line.
The height (i.e., the size along the Z direction in the example shown in the figure) of the waveguide member 122 is set to less than λm/2. The reason is that, if the distance is λm/2 or more, the distance between the root 124b of each conductive rod 124 and the conductive surface 110b will be λm/2 or more. Similarly, the height of each conductive rod 124 (in particular, those conductive rods 124 which are adjacent to the waveguide member 122) is also set to less than λm/2.
The distance L1 between the waveguide face 122a of the waveguide member 122 and the conductive surface 110b is set to less than λm/2. If the distance is λm/2 or more, resonance will occur between the waveguide face 122a and the conductive surface 110b, which will prevent functionality as a waveguide. In one example, the distance is λm/4 or less. In order to ensure manufacturing ease, when an electromagnetic wave in the extremely high frequency range is to propagate, the distance is preferably λm/16 or more, for example.
The lower limit of the distance L1 between the conductive surface 110b and the waveguide face 122a and the lower limit of the distance L2 between the conductive surface 110b and the leading end 124a of each conductive rod 124 depends on the machining precision, and also on the precision when assembling the two upper/lower conductive members 110 and 120 so as to be apart by a constant distance. When a pressing technique or an injection technique is used, the practical lower limit of the aforementioned distance is about 50 micrometers (μm). In the case of using an MEMS (Micro-Electro-Mechanical System) to make a product in e.g. the terahertz range, the lower limit of the aforementioned distance is about 2 to about 3 μm.
Next, variants of waveguide structures including the waveguide member 122, the conductive members 110 and 120, and the plurality of conductive rods 124 will be described. The following variants are applicable to the WRG structure in any place in example embodiments of the present disclosure.
The dielectric layer on the outermost surface will allow losses to be increased in the electromagnetic wave propagating through the WRG waveguide, but is able to protect the conductive surfaces 110b and 120a (which are electrically conductive) from corrosion. It also prevents influences of a DC voltage, or an AC voltage of such a low frequency that it is not capable of propagation on certain WRG waveguides.
In the waveguide device 100 of the above-described construction, a signal wave of the operating frequency is unable to propagate in the space between the surface 126 of the artificial magnetic conductor and the conductive surface 110b of the conductive member 110, but propagates in the space between the waveguide face 122a of the waveguide member 122 and the conductive surface 110b of the conductive member 110. Unlike in a hollow waveguide, the width of the waveguide member 122 in such a waveguide structure does not need to be equal to or greater than a half of the wavelength of the electromagnetic wave to propagate. Moreover, the conductive member 110 and the conductive member 120 do not need to be electrically interconnected by a metal wall that extends along the thickness direction (i.e., in parallel to the YZ plane).
On both sides of the waveguide member 122, stretches of artificial magnetic conductor that are created by the plurality of conductive rods 124 are present. An electromagnetic wave propagates in the gap between the waveguide face 122a of the waveguide member 122 and the conductive surface 110b of the conductive member 110.
In the waveguide structure of
For reference,
For reference's sake,
On the other hand, a waveguide device 100 including an artificial magnetic conductor can easily realize a structure in which waveguide members 122 are placed close to one another. Thus, such a waveguide device 100 can be suitably used in an array antenna that includes plural antenna elements in a close arrangement.
Next, an exemplary construction for a slot antenna utilizing the aforementioned waveguide structure will be described. A “slot antenna” means an antenna device having one or plural slots (also referred to as “through holes”) as antenna elements. In particular, a slot antenna having a plurality of slots as antenna elements will be referred to as a “slot array antenna” or a “slot antenna array”.
From a transmission circuit not shown, an electromagnetic wave is supplied to a waveguide extending between the waveguide face 122a of each waveguide member 122 and the conductive surface 110b of the conductive member 110. Among the plurality of slots 112 arranged along the Y direction, the distance between the centers of two adjacent slots 112 is designed so as to be equal in value to the wavelength of an electromagnetic wave propagating in the waveguide, for example. As a result of this, electromagnetic waves with an equal phase can be radiated from the six slots 112 arranged along the Y direction.
The antenna device 200 shown in
Next, an example embodiment of another antenna device that includes a waveguide device and at least one antenna element (radiating element) which is connected to a waveguide inside the waveguiding wall of the waveguide device will be described. To be “connected to a waveguide inside the waveguiding wall” means either being directly connected, or being indirectly connected via another waveguide (e.g., the aforementioned WRG), to the waveguide inside the waveguiding wall. The at least one antenna element has at least one of: the function of radiating into space an electromagnetic wave which has propagated through the waveguide inside the waveguiding wall; and the function of allowing an electromagnetic wave which has propagated in space to be introduced into the waveguide inside the waveguiding wall. That is, the antenna device according to the present example embodiment is used for at least one of transmission and reception of signals.
This antenna device further includes a conductive member 110 that covers the waveguide members 122U and the conductive rods 124U in the first waveguiding layer 10a. The conductive member 110 has 16 slots (apertures) 112 that are arrayed in four rows and four columns. On the conductive member 110, side walls 114 surrounding each slot 112 are provided. For each slot 112, the side walls 114 constitute a horn for adjusting the directivity of the slot 112. The number and arrangement of slots 112 in this example are only an example. The orientation and shape of each slot 112 are not limited to the example shown. For example, H-shaped slots may be used. Likewise, what is shown in the figures should not be seen as a limitation as to whether the side walls 114 of the horn are sloped or not, angles thereof, or the horn shape. Instead of the horn as illustrated, the horn structure in Example embodiment 1 may be adopted, for example.
In the example shown in
Via a port (through hole) 145L in the third conductive member 230, the waveguide member 122L may couple to an external waveguide device or radio frequency circuit (electronic circuit). As one example,
Note that a structure for connecting an electronic circuit to a waveguide is disclosed in, for example, U.S. Patent Publication No. 2018/0351261, U.S. Patent Publication No. 2019/0006743, U.S. Patent Publication No. 2019/0139914, U.S. Patent Publication No. 2019/0067780, U.S. Patent Publication No. 2019/0140344, and International Patent Application Publication No. 2018/105513. The entire disclosure of these publications is incorporated herein by reference.
The conductive member 110 shown in
In the antenna array of this example, as can be seen from
With the waveguide member 122L shown in
Note that it is not necessary for all slots 112 functioning as antenna elements to radiate electromagnetic waves in the same phase. The network patterns of the waveguide members 122 in the excitation layer and the distribution layer may be arbitrary, and each waveguide member 122 may be configured to independently propagate a mutually different signal.
Although the waveguide members 122U on the first conductive member 210 according to the present example embodiment lacks branching portions and bends, portions thereof that function as the excitation layer may include at least one of a branching portion(s) and a bend(s). As described earlier, it is not necessary for all conductive rods in the waveguide device to have similar shapes.
According to the present example embodiment, between the through holes 211 in the first conductive member 210 and the through holes 221 in the second conductive member 220, electromagnetic waves can be directly propagated via the electrically-conductive waveguiding walls 203. Since unwanted propagation does not occur on the second conductive member 220, structures such as other waveguides, circuit boards, or a camera may be disposed on the second conductive member 220. Thus, the device enjoys an improved design freedom. Although the present example embodiment illustrates that the waveguiding walls are disposed between the first conductive member 210 and the second conductive member 220, the waveguiding walls may be disposed in other positions.
When constructing an excitation layer and a distribution layer, various circuit elements in waveguides can be utilized. Examples thereof are disclosed in U.S. Pat. No. 10,042,045, U.S. Pat. No. 10,090,600, U.S. Pat. No. 10,158,158, International Patent Application Publication No. 2018/207796, International Patent Application Publication No. 2018/207838, and U.S. Patent Publication No. 2019/0074569, for example. The entire disclosure of these publications is incorporated herein by reference.
While each slot 112 in
The further conductive member 150 has four further slots 111, each slot 111 communicating with the cavity 180. A signal wave which is radiated from the slot 112 into the cavity 180 is radiated toward the front side of the further conductive member 150 via the four further slots 111. A structure may also be adopted where a horn is provided on the front side of the further conductive member 150, such that the further slots 111 open at the bottom of that horn. In this case, a signal wave which is radiated from the slot 112 is radiated via the cavity 180, the further slots 111, and the horn.
Next, variants of the shape of each through hole (slot or port) according to example embodiments of the present disclosure will be described. A cross section that is taken perpendicular to the axis of the through hole may have shapes as described in the following, for example. The variants presented below are similarly applicable to any example embodiment of the present disclosure.
In
In
In
In
An antenna device according to an example embodiment of the present disclosure can be suitably used in a radar device or a radar system to be incorporated in moving entities such as vehicles, marine vessels, aircraft, robots, or the like, for example. A radar device would include an antenna device according to an example embodiment of the present disclosure and a microwave integrated circuit that is connected to the antenna device. A radar system would include the radar device and a signal processing circuit that is connected to the microwave integrated circuit of the radar device. The signal processing circuit may perform a process of estimating the azimuth of an arriving wave based on a signal that is received by a microwave integrated circuit, for example. For example, the signal processing circuit may be configured to execute the MUSIC method, the ESPRIT method, the SAGE method, or other algorithms to estimate the azimuth of the arriving wave, and output a signal indicating the estimation result. Furthermore, the signal processing circuit may be configured to estimate the distance to each target as a wave source of an arriving wave, the relative velocity of the target, and the azimuth of the target by using a known algorithm, and output a signal indicating the estimation result.
In the present disclosure, the term “signal processing circuit” is not limited to a single circuit, but encompasses any implementation in which a combination of plural circuits is conceptually regarded as a single functional part. The signal processing circuit may be realized by one or more System-on-Chips (SoC). For example, a part or a whole of the signal processing circuit may be an FPGA (Field-Programmable Gate Array), which is a programmable logic device (PLD). In that case, the signal processing circuit includes a plurality of computation elements (e.g., general-purpose logics and multipliers) and a plurality of memory elements (e.g., look-up tables or memory blocks). Alternatively, the signal processing circuit may be a set of a general-purpose processor(s) and a main memory device(s). The signal processing circuit may be a circuit which includes a processor core(s) and a memory device(s). These may function as the signal processing circuit.
An antenna device according to an example embodiment of the present disclosure includes a multilayered WRG structure which permits downsizing, and thus allows the area of the face on which antenna elements are arrayed to be significantly reduced, as compared to a construction in which a conventional hollow waveguide is used. Therefore, a radar system incorporating the antenna device can be easily mounted in a narrow place such as a face of a rearview mirror in a vehicle that is opposite to its specular surface, or a small-sized moving entity such as a UAV (an Unmanned Aerial Vehicle, a so-called drone). Note that, without being limited to the implementation where it is mounted in a vehicle, a radar system may be used while being fixed on the road or a building, for example.
An antenna device according to an example embodiment of the present disclosure can also be used in a wireless communication system. Such a wireless communication system would include an antenna device according to any of the above example embodiments and a communication circuit (a transmission circuit or a reception circuit) connected to the antenna device. For example, the transmission circuit may be configured to supply, to a waveguide within the antenna device, a signal wave representing a signal for transmission. The reception circuit may be configured to demodulate a signal wave which has been received via the antenna device, and output it as an analog or digital signal.
An antenna device according to an example embodiment of the present disclosure can further be used as an antenna in an indoor positioning system (IPS). An indoor positioning system is able to identify the position of a moving entity, such as a person or an automated guided vehicle (AGV), that is in a building. An antenna device can also be used as a radio wave transmitter (beacon) for use in a system which provides information to an information terminal device (e.g., a smartphone) that is carried by a person who has visited a store or any other facility. In such a system, once every several seconds, a beacon may radiate an electromagnetic wave carrying an ID or other information superposed thereon, for example. When the information terminal device receives this electromagnetic wave, the information terminal device transmits the received information to a remote server computer via telecommunication lines. Based on the information that has been received from the information terminal device, the server computer identifies the position of that information terminal device, and provides information which is associated with that position (e.g., product information or a coupon) to the information terminal device.
Application examples of radar systems, communication systems, and various monitoring systems that include a slot array antenna having a WRG structure are disclosed in the specifications of U.S. Pat. No. 9,786,995 and U.S. Pat. No. 10,027,032, for example. The entire disclosure of these publications is incorporated herein by reference. A slot array antenna according to the present disclosure is applicable to each application example that is disclosed in these publications.
A waveguide device according to the present disclosure is usable in any technological field that utilizes electromagnetic waves. For example, it is available to various applications where transmission/reception of electromagnetic waves of the gigahertz band or the terahertz band is performed. In particular, they may be suitably used in onboard radar systems, various types of monitoring systems, indoor positioning systems, wireless communication systems, etc., where downsizing is desired.
This application is based on Japanese Patent Applications No. 2018-189124 filed on Oct. 4, 2018, the entire contents of which are hereby incorporated by reference.
While example embodiments of the present disclosure have been described above, it is to be understood that variations and modifications will be apparent to those skilled in the art without departing from the scope and spirit of the present disclosure. The scope of the present disclosure, therefore, is to be determined solely by the following claims.
Number | Date | Country | Kind |
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2018-189124 | Oct 2018 | JP | national |