Patent Grant
10305194
This application is a National Phase filing under 35 C.F.R. § 371 of and claims priority to PCT Patent Application No.: PCT/FR2015/053220, filed on Nov. 26, 2015, which claims the priority benefit under 35 U.S.C. § 119 of French Application No.: 1461962, filed on Dec. 5, 2014, the contents of which are hereby incorporated in their entireties by reference.
Some embodiments are directed to high-electromagnetic-impedance surface (or HIS, for “High Impedance Surface”) devices.
In some fields, like that of satellite positioning signal receivers for example, surface devices with high electromagnetic impedance are used. The latter can, for example, be used to reduce the electromagnetic couplings between elements in multistandard adaptive networks.
It is recalled that a surface device with high electromagnetic impedance generally comprises a ground plane, at least one dielectric cavity (generally in the form of a substrate), and a printed circuit board (PCB), which is single-layer or multilayer, and comprising a multitude of conductive elements defining patterns arranged periodically and of small size and periodicity compared to the wavelength used.
When there is a desire for the surface device with high electromagnetic impedance to exhibit at least two resonant frequencies, it is possible, for example, to arrange it as described in the patent document U.S. Pat. No. 6,670,932. More specifically, this surface device with high electromagnetic impedance is of mushroom type, that is to say that it comprises a conductive ground plane defining a non-compartmentalized cavity but comprising a matrix of identical conductive pillars, filled with a dielectric material and covered by a printed circuit board bearing metallic patterns, in order to form electromagnetic resonators exhibiting different resonant wavelengths. The size and the periodicity of the elements (or “patches”) defining the patterns is smaller than the resonant wavelengths of the electromagnetic resonators.
Each pattern is intended to capture, at the input of the cavity, an incident electromagnetic wave which is propagated in the ground plane, then to generate, under the pattern, an electric current loop at a determined resonant frequency so as to reflect any incident electromagnetic wave having a frequency in a narrow band centered around this resonant frequency.
The device described offers an interleaving of a first “matrix” of electromagnetic resonators that are identical and that have a first resonant frequency, with a second “matrix” of electromagnetic resonators that are identical and that have a second resonant frequency. This interleaving is obtained by the patterns which are borne by the printed circuit board of fractal or multilayer type, each pattern being centered either on a pillar or between four adjacent pillars.
A drawback with this type of device lies in the fact that the first and second resonant frequencies cannot be adjusted independently of one another and that the reflection bands, of which these resonant frequencies are the center frequencies, are fairly narrow. Furthermore, this type of device proves relatively bulky.
Some embodiments are directed to improve or enhance the situation, and more specifically to make it possible to obtain, in a reduced space, resonant frequencies (or wavelengths) that can be adjusted easily relative to one another and defining the center frequencies (or wavelengths) of reflection bands spectrally wider than in the prior art.
To this end, it notably proposes a high-impedance surface device comprising a set of at least two separate compartments, which are substantially cylindrical, having internal surfaces in an electrically conductive material, and each having, at one end, a single aperture, these apertures of the compartments being oriented on one and the same side and covered by at least one periodic structure of electrically conductive patterns, each compartment being filled with a dielectric material, each compartment thus covered forming at least one electromagnetic resonator, and each electromagnetic resonator exhibiting a resonant wavelength.
In this device:
The device according to some of embodiments can include other features which can be taken separately or in combination, and in particular:
Some embodiments are also directed to a satellite positioning signal receiver, comprising an electric ground plane, at least two radiant elements arranged on this ground plane, and at least one high-impedance surface device of the type of that presented above, arranged on the ground plane between the radiant elements.
Some embodiments are also directed to a method, intended to allow the modification of the impedance over several frequency bands of a high-impedance surface device, and comprising at least one step of modifying electromagnetic properties of at least one compartment of a high-impedance surface device of the type of that presented above.
Some embodiments are also directed to a method, intended to allow the fabrication of a high-impedance surface device which comprises several separate components, which are substantially cylindrical, and a periodic structure of electrically conductive patterns.
This method includes the following steps:
Other features and advantages of the invention will become apparent on examining the following detailed description, and the attached drawings, in which
Some embodiments are directed to a compact, multiband and optionally reconfigurable high-impedance surface device 1, and associated methods.
Hereinbelow, it is considered, by way of nonlimiting example, that the high-impedance surface device 1 forms part of a satellite positioning signal receiver 15, possibly of GNSS (Global Navigation Satellite System) type. However, the invention is not limited to this application. A high-impedance surface device 1, according to the invention, can in fact be used to equip numerous appliances, systems or installations, in civilian or military fields, and notably land, sea, river or air vehicles, transmitting and/or receiving stations, and buildings (possibly of industrial type).
As illustrated, this receiver 15 comprises an electric ground plane 16, at least two radiant elements 17k arranged on this ground plane 16, and at least one high-impedance surface device 1 according to the invention, arranged on the ground plane 16 between the radiant elements 17k.
For example, the radiant elements 17k define an adaptive network specifically for receiving navigation signals, for example GNSS signals, in a scrambled environment by modifying the radiation pattern of the receiver in order to generate radiation nulls (or zeros) in the directions of the scrambling interferences. The adaptation of the radiation pattern according to the scramblers is produced through a post-processing of the navigation signals received on each of the radiant elements 17k of the network.
It will be noted that, in the nonlimiting example illustrated in
It is recalled that in an adaptive network, the electromagnetic couplings between radiant elements significantly degrade the performance levels, and in particular the capacity of the signal processing algorithms to accurately locate the angular position of the interferences and consequently to generate radiation nulls in their directions. In such a context, a high-impedance surface device 1 can be charged with stopping the currents which propagate between the radiant elements 17k of the adaptive network in order to reduce the electromagnetic couplings between radiant elements and to optimize the robustness of the GNSS receiver with respect to the electromagnetic interferences.
As illustrated in a nonlimiting manner in
The compartments 2j of the set are separate and substantially cylindrical, have internal surfaces produced in an electrically conductive material, and each have, at one end, a single aperture 3. Furthermore, each compartment 2j is filled with a dielectric material, for example air. For example, the compartments 2j are substantially cylindrical of rectangular or square section.
The apertures 3 of the compartments 2j are all oriented on one and the same side and covered by at least one periodic structure of electrically conductive patterns 4. It will be understood that each aperture 3 can be associated with its own periodic structure of electrically conductive patterns 4, as illustrated in a nonlimiting manner in
It will be noted that each compartment 2j can be covered by a single electrically conductive pattern 4.
It will also be noted that the electrically conductive patterns 4 of each periodic structure can be secured to support means, such as, for example, a printed circuit board (or PCB) 18, of single-layer or multilayer type. For example, the electrically conductive patterns 4 can be printed on this printed circuit board 18. The electrically conductive patterns are arranged periodically and their size and periodicity are small compared to the wavelength used.
In a variant that is not represented, each pattern 4 can be a metal grid ensuring its own support function.
It will also be noted that active elements, such as, for example, varactors, can optionally and beforehand be incorporated on/in the printed circuit board 18 to adjust the capacitive effect of the patterns 4.
It will also be noted that the device 1 can optionally comprise first setting means arranged to set the dielectric permittivity of the support means. The first setting means can be produced in the form of materials whose properties can be electronically controlled, such as for example liquid crystals, plasmas or else ferroelectric materials, and electronic control means for such materials. In a variant, the first setting means can be produced in the form of a metamaterial of adjustable permittivity. The dielectric permittivity acts on the inductance of the compartment 2j. The greater the permittivity, the lower the height of the compartment 2j can be.
Each compartment 2j forms, with the periodic structure of electrically conductive patterns 4 which covers its aperture 3, at least one electromagnetic resonator exhibiting a resonant frequency.
It will also be noted that the wider the compartment 2j, the greater the size of the internal current loop, and therefore the greater the inductance.
The compartments 2j are separated from one another by a distance which is less than the shortest resonant wavelength exhibited by the electromagnetic resonators that they form. Moreover, at least two respective resonant wavelengths of the electromagnetic resonators formed by the covered compartments 2j are different. Furthermore, the periodic structure of electrically conductive patterns 4 exhibits a spatial period which is less than half the shortest resonant wavelength.
The device 1 produces a high-impedance effect at several resonant frequencies (or wavelengths). The number of resonant frequencies (or wavelengths) that can be used is equal to the number of compartments. The high-impedance effect is produced on a hypothetical surface which is situated above the printed circuit board 18, very close and parallel to the printed circuit board 18 and being able to cover a greater or lesser surface depending on the resonant frequency (or wavelength) considered.
The device 1 can be produced according to exemplary embodiments which can be grouped together in at least two families. A first family combines the examples illustrated in
For all the examples of the first family, the device 1 comprises a signal cavity 5 within which each compartment 2j is arranged (or defined). To do this, the cavity 5 comprises at least one vertical partition 6 which is electrically conductive and in contact with a bottom wall 7 and which delimits two compartments 2j. Each vertical partition 6 is preferably substantially planar, and defines a plane substantially at right angles to a plane defined by the bottom wall 7 of the cavity 5. This electrically conductive nature can originate from the material in which the vertical partition 6 is produced or from the fact that the vertical partition 6 is coated on its surfaces with a layer of an electrically conductive material. Moreover, a single periodic structure of electrically conductive patterns 4 covers all the apertures 3 of the different compartments 2j.
The cavity 5 is delimited by at least one lateral wall 10 and the bottom wall 7. The latter walls 7, 10 are electrically conductive. This electrically conductive nature can originate from the material in which they are produced or from the fact that they are coated with a layer of an electrically conductive material on their internal surfaces.
It will be noted that the cavity 5 can either be added and secured to the ground plane 16, for example by soldering or bonding, or form an integral part of the ground plane 16, for example by stamping and cutting.
In the nonlimiting examples illustrated in
In the nonlimiting example illustrated in
It will be noted that the cavity 5 can comprise any number of compartments 2j, provided that this number is greater than or equal to two.
This cavity 5 with multiple electromagnetic resonators produces capacitive and inductive effects ei which are the source of the high surface impedance. There is in particular a capacitive effect between the ground plane 16 and each pattern 4 which overlaps it, a capacitive effect between patterns 4 which overlap, and an inductive effect ei in each compartment 2j, more specifically in the depth hj of each compartment 2j, thus forming a current loop.
The presence of conductive vertical partition(s) 6 also induces additional capacitive and inductive effects. In particular, additional capacitive effects are present between the “top” ends 11 of the vertical partitions 6 and the patterns 4 which overlap them. These additional capacitive effects are particularly great given that the distances which separate them are small. Additional inductive effects are produced by the multiple current loops which are present in the different compartments 2j.
In this first family, for the first resonant frequency f1 associated with the first compartment 21, the high-impedance effect is located in the zone which extends over all the cavity 5, whereas, for the other resonant frequencies f2, f3, . . . , fn, associated respectively with the other compartments 22, 23, . . . , 2n, the high-impedance effect is located either over all the cavity 5, or in a more restricted zone like above a compartment 2j (j=2 to n), depending on the respective horizontal positions of the vertical partitions 6.
The value of the resonant frequencies depends on the capacitive and inductive effects obtained in the device 1. Consequently, the choice of the resonant frequencies can notably be made by adjusting the respective distances lm (here m=1 to 3 or 1 to 2) which separate the vertical partitions 6 from the lateral wall 10 and/or the respective heights hm of the vertical partitions 6, in other words the vertical distances between the top ends 11 of the vertical partitions 6 and the patterns 4 which overlap them. The vertical distances between the top ends 11 of the vertical partitions 6 and the patterns 4 can be null, the vertical partitions 6 being in this case in contact with the printed circuit board 18.
It will be noted that the resonant frequencies can be set by adjusting both the distances lm and the heights hm. This solution is notably advantageous when the aim is to obtain more than two resonant frequencies because it makes it possible to increase the degrees of freedom to optimize the device 1.
The choice of the resonant frequencies by adjustment of the respective distances lm separating the vertical partitions 6 from the lateral wall 10 is illustrated in
The choice of the resonant frequencies can be the subject either of an initial design or of a prior setting, for example via appropriate setting means for given functions, or of a setting in real time by means of appropriate setting means.
To allow a setting of the distances lm and therefore of the horizontal positions of the vertical partitions 6, each vertical partition 6 can be mobile in a direction which is substantially parallel to a plane defined by the bottom wall 7 of the cavity 5. In this case, the device 1 can comprise setting means arranged to set the horizontal position of each vertical partition 6 in the cavity 5.
To allow a setting of the heights hm, each vertical partition 6 can be mobile in a direction (here vertical) which is substantially at right angles to the plane defined by the bottom wall 7 of the cavity 5. In this case, the device 1 can comprise setting means arranged to set the height of each vertical partition 6 in the cavity 5.
In a variant, and as illustrated in
It will be noted, as illustrated in a nonlimiting manner in
By way of example, to set the resonant frequencies on the desired bands, the following method can be implemented. First of all, a first single-band electromagnetic resonator can be designed on a frequency f1. Then, the number of vertical partitions 6 can be determined to set the number of resonant frequencies f1 to fn. Then, the vertical partitions 6 can be inserted into the cavity 5. The height of the cavity 5 can then be adjusted to obtain the first resonant frequency at the frequency f1. Finally, the distances lm and/or the heights hm can be adjusted to set the frequencies f2 to fn of the other resonant frequencies.
In other words, a method is proposed that is intended to allow the modification of the impedance over several frequency bands of a device 1, and comprising at least one step of modifying electromagnetic properties of at least one compartment 2j of this device 1.
In a variant, a method can be intended to allow the fabrication of a high-impedance surface device 1 which comprises several separate compartments 2j, which are substantially cylindrical, and a periodic structure of electrically conductive patterns 4.
This variant method comprises the following steps:
It will be noted, surprisingly, that the variation of the width of the first compartment 21, and therefore the variation of the distance l1, hardly varies the first resonant frequency f1 but varies the second resonant frequency f2.
A modal analysis makes it possible to understand the unexpected effect resulting from the invention. In effect, the resonant frequency f1 remains stable as a function of the distance l1 because the mode generated in the device 1 is derived from a resonance in which the magnetic field moves vertically in the cavity 5 in phase balance. This resonant mode is that which is observed when the first vertical partition 6 is not present in the cavity 5 (case where l1=0). Through the nature of this resonant mode, the variation of the distance l1 does not in any way affect the resonant frequency f1. Conversely, the magnetic field in the device 1 at the resonant frequency f2 has a different mapping. The vertical partition 6 in effect interacts with the electromagnetic field, and therefore the field is cancelled on a vertical line in the vicinity of the vertical partition 6 and produces a mode of higher order than that observed at the resonant frequency f1. The distance l1 therefore conditions this resonant mode and affects the value of the resonant frequency f2.
For all the examples of the second family, the device 1 comprises at least two unconnected cavities 5j each forming (or defining) one of the compartments 2j. The number of resonant frequencies (or wavelengths) is therefore here defined by the number of cavities 5j.
In the examples illustrated in a nonlimiting manner in
The cavities 5j, and therefore the electromagnetic resonators, share one and the same ground plane 16 and, as indicated above, are spaced apart from one another by a distance which is less than the shortest resonant wavelength.
This family of exemplary embodiments has the particular feature of producing successive high-impedance effects for distinct resonant frequencies. Each electromagnetic resonator is characterized by its own resonant frequency. The high-impedance effect is produced on a hypothetical surface located above the or each printed circuit board 18 and very close, and parallel, to the or each printed circuit board 18.
For each electromagnetic resonator, the resonant frequency depends primarily on the height hm (here m=j) of the associated cavity 5j, on the dielectric material filling this cavity 5j, and on the transmission and reflection characteristics of the printed circuit board 18. In effect, in a representation of “LC circuit” type, the height hm of a cavity 5j and the type of dielectric material in the cavity 5j directly impact the inductance value, whereas the printed circuit board 18 has a tendency to impact the capacitance value.
The multi-resonant nature obtained also with this family of exemplary embodiments proves unexpected, in as much as it was logical to think that the frequencies higher than the resonant frequency of the first cavity 51 would not be able to pass through the latter cavity 51 and reach the adjacent cavities 5j (with j≠1).
It will be noted, as illustrated in a nonlimiting manner in
This option requires the device 1 to comprise setting means arranged to set the position (here vertical) of each horizontal partition 9j within its cavity 5j, and therefore its compartment 2j.
It will also be noted that the device 1 can optionally comprise second setting means arranged to set the magnetic permeability of the material filling each compartment 2j. The second setting means can be produced in the form of a magnetic material of adjustable magnetic permeability, such as, for example, a ferromagnetic material or a metamaterial. As a nonlimiting example, the second setting means can be produced in the form of a ferrite whose magnetic permeability changes under the influence of a magnetic field. The reflection band in fact increases with the increase in the magnetic permeability of the material. An adjustable magnetic permeability makes it possible to adjust the inductance.
By virtue of the invention, a high-impedance surface device is made available that is compact because it comprises a reduced number of cavities. There is also made available a high-impedance surface device that is multiband, optionally reconfigurable, and suited to reflection bands that are spectrally wider than in the prior art.
| Number | Date | Country | Kind |
|---|---|---|---|
| 14 61962 | Dec 2014 | FR | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/FR2015/053220 | 11/26/2015 | WO | 00 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2016/087749 | 6/9/2016 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 4042935 | Ajioka | Aug 1977 | A |
| 6670932 | Diaz et al. | Dec 2003 | B1 |
| 9843099 | Legay | Dec 2017 | B2 |
| Entry |
|---|
| International Search Report issued in PCT/FR2015/053220 dated Feb. 26, 2016 (with English translation). |
| Written Opinion issued in PCT/FR2015/053220 dated Feb. 26, 2016. |
| Dan Sievenpiper et al., “High-Impedance Electromagnetic Surfaces with a Forbidden Frequency Band”, IEEE Transactions on Microwave Theory and Techniques, IEEE Service Center, vol. 47, No. 11, Nov. 1, 1999, p. 2059. |
| Number | Date | Country | |
|---|---|---|---|
| 20170365931 A1 | Dec 2017 | US |
