Patent Grant
9614288
The present invention concerns a device for receiving and/or emitting an electromagnetic wave, a system comprising said device, and a use of such device.
For example, it is known from FR-2 863 109, a device for receiving and/or emitting an electromagnetic wave, comprising a plurality of passive reflective elements. The passive reflective elements are periodically spaced inside the device, and said device uses specific Bragg law electromagnetic properties.
However, the passive reflective elements are spaced from each other of a distance that is a multiple of the wavelength λ. The distance is about λ/2 or greater and such device has a large size.
It is also known from the patent application WO-2008/007024, a device having a reactive type antenna element surrounded by a plurality of metallic diffusers. Thanks to this arrangement, the electromagnetic wave is focused to a point i near the antenna element at a sub wavelength distance. Such device does not near to have a period pattern of metallic diffusers.
However, such device does not have a preferred direction for the electromagnetic wave.
All these devices still need to be improved, in the view of increasing their efficiency and reducing their size.
One object of the present invention is to provide an improved device for receiving and/or emitting an electromagnetic wave.
To this effect, the present invention proposes a device receiving and/or emitting an electromagnetic wave having a free space wavelength λ0 comprised between 1 mm and 10 m, comprising:
Thanks to these features, the device for receiving and/or emitting an electromagnetic wave is small compared to the equivalent known devices of the prior art.
The passive resonant elements are coupled to each others, and the device does not use the Bragg law: the passive resonant elements can be periodic or non periodic inside the medium.
The device uses a band-gap that is known as an hybridization band-gap.
A first region of the device comprising the passive resonant elements is preventing a propagation of electromagnetic waves at the second resonance frequency from the active resonant element through said first region. The device comprises a directivity diagram that is determined by the shape of said first region. The device is able to emit and/or receive an electromagnetic wave according to one or a plurality of predetermined directions.
The electromagnetic energy at the second resonance frequency is concentrated inside a second region around the active resonant element. The device is able to emit and/or receive an electromagnetic wave at a greater distance from itself. The device has a greater sensitivity and is more efficient.
In various embodiments of the device, one and/or other of the following features may optionally be incorporated.
According to another aspect of the invention, the second shape is identical to said first shape, and at least one of the second physical parameters of the second structure is different to a corresponding first physical parameter of the first structure.
According to another aspect of the invention, the first and second physical parameters comprise sizes and materials of the first and second structure, respectively.
According to another aspect of the invention, the first distance and the second distance are lower than λ/10.
According to another aspect of the invention, the passive resonant elements are not periodically disposed inside the medium.
According to another aspect of the invention, the active resonant element is in proximity of a lateral surface of the medium.
According to another aspect of the invention, the active resonant element is at a third distance from the lateral surface, said third distance being lower than the wavelength λ.
According to another aspect of the invention, the device further comprises at least two active resonant elements, said two active resonant elements being separated from each other of a forth distance, and wherein said two active resonant elements have different second resonance frequencies, each of them being comprised inside said band-gap.
The two active resonant elements can therefore emit independent and uncorrelated electromagnetic waves.
According to another aspect of the invention, the forth distance is lower than the wavelength λ, and preferably lower than λ/4.
According to another aspect of the invention, the forth distance is adapted so that at least one passive resonant element is substantially between said two active resonant elements.
According to another aspect of the invention, the two active resonant elements are positioned symmetrically in comparison to a geometrical centre of said device.
According to another aspect of the invention, the device further comprises:
The two active resonant elements can therefore emit independent and uncorrelated electromagnetic waves.
According to another aspect of the invention, the device further comprises:
The two active resonant elements can therefore emit independent and uncorrelated electromagnetic waves.
According to another aspect of the invention, the first and second shapes are wires of electrical conductors, the first resonance frequency depending on a length of said first shape, and the second resonance frequency depending on a length of said second shape.
According to another aspect of the invention, the first and second shapes are split rings of electrical conductors, the first resonance frequency depending on an electric capacitor and an electric inductance of said first shape, and the second resonance frequency depending on an electric capacitor and an electric inductance of said second shape.
According to another aspect of the invention, the first and second shapes are slots on an electrical conductor plate, the first resonance frequency depending on a perimeter length of the slot of said first shape, and the second resonance frequency depending on a length of the slot of said second shape.
Another object of the present invention is to provide a system comprising a device for receiving and/or emitting an electromagnetic wave, wherein the active resonant element is connected to an electronic device for receiving and/or emitting a signal representative to said electromagnetic wave, said electric signal having at least a frequency component substantially equal to the second frequency.
Another object of the present invention is to use a device for receiving and/or emitting an electromagnetic wave having a free space wavelength λ comprised between 1 mm and 1 m, and preferably between 10 cm and 40 cm.
Other features and advantages of the invention will be apparent from the following detailed description of three of its embodiments given by way of non-limiting examples, with reference to the accompanying drawings. In the drawings:
In the various figures, the same reference numbers indicate identical or similar elements. The direction Z is a vertical direction. A direction X or Y is a horizontal or lateral direction.
This device comprises:
The medium 11 has a refractive index nd.
The space may be air. In that case, its refractive index is equal to one.
The free space wavelength λ0 corresponds to a wavelength λ inside the medium 11 with the following well-known relation: nd·λ=λ0.
The medium 11 is for example a parallelepiped, comprising a first surface S1 and a second surface S2, the second surface S2 being opposite to said first surface along the vertical direction Z. The first and second surfaces S1, S2 are substantially parallel planes. A direction D is substantially a straight line perpendicular to said surfaces and parallel to the vertical direction Z. The first and second surfaces S1, S2 are distant of a height value H.
The medium 11 has an electric permeability of εd.
In present description, we consider that the passive resonant elements 12 have a first structure comprising at least a first shape and first physical parameters.
In case of the first embodiment of the invention:
The length Lw1 of each passive resonant element is for example equal to the height value H of the medium 11.
In other words, each passive resonant element 12 of the first embodiment are electrical conductive wires having a diameter a and extending along the direction D according to a length Lw1 between a first end 12a above the first surface S1 and a second end 12b above second surface S2.
In this first embodiment the passive resonant elements 12 form on the first surface S1 or any plane XY perpendicular to said vertical direction Z a regularly spaced square grid. The passive resonant elements 12 are parallel to each other along the vertical direction Z.
The passive resonant elements 12 have at least one resonance frequency f1, a first resonance frequency.
The passive resonant elements 12 are spaced from each other along the direction X or Y of a first distance dl lower than λ/4, and preferably lower than λ/10. This sub-wavelength first distance dl is the step of said grid.
The passive resonant elements 12 are therefore electromagnetically coupled to each other.
Thanks to this feature, a hybridization band-gap is created around the first resonance frequency f1. In the present case of electrical conductive wires, the band-gap will be above the resonance frequency of a single wire.
The passive resonant elements 12 form on
On
A first resonance wavelength λ1 is determined by:
λ1/2=Lw1*
where Lw1* is a first electrical length corresponding to said first geometrical length Lw1 of the passive resonant element 12.
In fact, the length Lw1 generates a plurality of first resonance frequencies f1, each of them being multiple of the first one. But, the present description will only refer to the first one of them for simplicity.
The first resonance frequency f1 is:
f1=c/λ1,
i.e.: f1=c/(2·Lw1*),
where c is the speed of a wave (light) in the vacuum space.
On
Such passive resonant element comprises a plurality of geometrical lengths:
Each of these geometrical lengths Lwi, i being an index representing a wire portion of the passive resonant element 12, is related to an electrical length Lwi*, to a first resonance wavelength λ11, and to a first resonance frequency f1i.
A wavenumber ki corresponding to a wave is a number defined as the number of wavelengths per unit distance, i.e. ki=2π/λi.
The passive resonant element 12 has a plurality of resonance frequencies f1i that can be represented, for the plurality of all of them, in a wavenumber-frequency diagram as shown on
The passive resonant elements 12 can be incorporated inside the medium 11 according to a periodic pattern. The device has a simple geometry, and the device electromagnetic properties (sensitivity, directivity, performance or efficiency) can be more easily computed and predicted before fabrication.
The passive resonant elements 12 can be incorporated inside the medium 11 according to a non periodic pattern. The device is less sensitive to fabrication uncertainties concerning the positions of the passive resonant elements 12 inside the medium 11. Such problem is well known for Bragg band-gap materials or metamaterials.
One or several active resonant elements 13 are also incorporated inside the medium 11 between the passive resonant elements 12.
The active resonant elements 13 are coupled or connected to an electronic device 14 for receiving or emitting a signal.
The active resonant elements 13 can be fed with a single electric signal S to emit or receive a single electromagnetic wave W, or they may be fed with a plurality of electric signals (one different signal for each active element) to emit or receive simultaneously the plurality of signals through a plurality of independent electromagnetic waves.
The active resonant elements 13 are close to the passive resonant elements 12. The active resonant element 13 is spaced apart from a passive resonant element 12 belonging to the plurality of resonant passive elements of a second distance d2 that is lower than λ2, and eventually lower than λ/10.
The active resonant element 13 is preferably positioned inside the medium 11, in proximity of a periphery of said medium that is to say in proximity of lateral surface LS.
For example, the distance between the active resonant element 13 and the proximal lateral surface from said active resonant element is lower than a third distance d3. Between said active resonant element 13 and said proximal lateral surface there is no or only one passive resonant element 12. The active resonant element 13 is therefore able to emit an electromagnetic wave W laterally from said lateral surface LS (
The third distance d3 is lower than the wavelength λ, and preferably lower than λ/4. The active resonant element 13 is near the proximal lateral surface LS.
The active resonant element 13 is preferably at the periphery. The device has a small size.
The active resonant element 13 has a second structure comprising a second shape and second physical parameters.
In case of the first embodiment of the invention:
In the particular first embodiment, the second shape of the active resonant element is identical to the first shape of the passive resonant element. The active resonant element 13 differs from the passive resonant element 12 only by the length Lw2 that is shorter than the length Lw1. The passive and active resonant elements 12, 13 only differ by their physical parameters. The second structure of the active resonant element is therefore different to the first structure of the passive resonant element.
The active resonant element 13 has a resonance frequency, named a second resonance frequency f2. The second resonance frequency f2 is comprised between fΔ1 and fΔ2, i.e. inside the band-gap Δf of the plurality of passive resonant elements 12.
The electrical length of the wire of the active resonant element 13 is for example reduced compared to the electrical length of the wire of the passive resonant element 12: The second resonance frequency f2 of the active resonant element 13 is higher than the first frequency f1 of the passive resonant elements 12, and said second resonance frequency f2 can fall inside the band-gap Δf.
However, the plurality of passive resonant elements 12 does not propagate waves belonging to said band-gap Δf.
An emitted wave W emitted form the active resonant element 13 is attenuated in the direction of the plurality of passive resonant elements 12. The device behaves such as having a first region R1 comprising most of the passive resonant elements 12, and a second region R2 comprising the active resonant elements 13, the first and second region R1, R2 excluding each other and being separated by a boundary 19 (
The device is therefore able to emit or to receive an electromagnetic wave W according to a predetermined direction or several predetermined directions, said predetermined directions being defined by the shapes of the first and second regions R1, R2.
Thanks to these predetermined directivity diagram of each active resonant element 13, the device can emit a different signal from each active resonant element 13 for a multi-input multi-output (MIMO) application.
Additionally, a signal having a frequency component substantially equal to the second frequency f2 can be efficiently emitted or received.
The device can emit or receive an electromagnetic wave in the far field, with an improved sensitivity compared with a device wherein the second frequency f2 of the active resonant element 13 is not inside the band-gap Δf of the plurality of passive resonant elements 12.
The shapes of the active resonant elements 13 are preferably identical to the shape of the passive resonant element 12. At least one of the physical parameters of the active resonant elements 13 is different than physical parameters of the passive resonant elements 12. The active resonant element 13 can have a second resonance frequency f2 inside the band-gap Δf of the plurality of passive resonant elements 12.
The device of
In case of emission, the electric signals of the plurality of active resonant elements 13 can be different from each other. In case of reception, the electric signals of the plurality of active resonant elements 13 can be different and uncorrelated to each other.
These active resonant elements 13 may be used independently from each other and may be used in a MIMO configuration of the device.
This device comprising a plurality of active resonant elements 13 is an extremely compact array of antenna.
Moreover, two active resonant elements (131, 132) are separated from each other of a forth distance d4.
The forth distance d4 between two active resonant elements 13 is preferably higher than the second distance d2 between an active resonant element 13 and a neighbour passive resonant element 12. At least one passive resonant element 12 is for example between two active resonant elements 13. The active resonant elements 13 belonging to the plurality are not coupled to each other.
The forth distance d4 is for example lower than the wavelength in the medium 11, and preferably lower than λ/4. The device comprising a plurality of active resonant elements 13 is small.
The electric signals of the plurality of active resonant elements 13 are therefore more uncorrelated to each other, so that they can be used independently.
The two active resonant elements (131, 132) may also have different second physical parameters, so that the first active resonant element 131 has a second resonant frequency f21 that is different than the second resonant frequency f22 of the second active resonant element 132.
The two active resonant elements (131, 132) are then not coupled to each other, and the signals of the active resonant elements 13 are again more uncorrelated.
The passive resonant elements 12 are conductive wires of approximately 30 mm length, with first half portion in direction Z and second half portion in direction Y. The first resonance frequency f1 corresponds to the above lengths of the passive resonant elements 12 conductive wires. In that case, the first resonance frequency f1 is approximately of 2.2 GHz.
The active resonant element 13 is a conductive wire of approximately 25 mm length, with first portion in direction Z and second portion in direction Y above the second half portions of the passive resonant elements 12. The second resonance frequency f2 corresponds to the above length of the active resonant element 13 conductive wire. In that case, the second resonance frequency f2 is approximately of 2.45 GHz.
The different portions of wires that are parallel to each other are distant of 2 mm.
The device can then emit and receive wave at a central frequency of approximately 2.45 GHz corresponding to the second resonance frequency f2, and with a frequency bandwidth of approximately 100 MHz, said frequency bandwidth being comprised inside the frequency band-gap (Δf) of the passive resonant elements. The central frequency corresponds to a free space wavelength λ0 between 20 cm and 12 cm. In this example, the first and second distances (d1, d3) are lower than λ/10.
The size of the device in the Y and Z directions of this variant is therefore smaller than in the device of
These passive and active resonant elements 12, 13 are in the form of a split ring element extending in a plane XY above the first surface S1. Their structure also uses electrical conductive elements.
Such second embodiment of the invention is smaller in the direction Z compared to the first embodiment of the invention.
The first shape and the second shape are small loops having at least one opening, like a C letter. The loop behaves like an electric inductance L. The opening behaves like an electric capacitor C. The passive or active resonant element 12, 13 behaves like a small electric circuit having a resonance frequency fc that is substantially equal to
The passive resonant element 12 has a first resonance frequency f1 depending on an electric capacitor C1 and an electric inductance L1. The active resonant element 13 has a second resonance frequency f2 depending on an electric capacitor C2 and an electric inductance L2.
The plurality of passive resonant elements 12 has a band-gap Δf. The active resonant element 13 is designed to have a second resonance frequency inside the band-gap.
The other features for this embodiment of the invention are similar. And, it provides the same advantages.
All the optional variants are also possible.
Such device is small and efficient to emit or receive an electromagnetic wave W from or to far field.
The two second resonance frequencies can be positioned inside the frequencies band-gap Δf of the passive resonant elements 12.
Thanks to such a device having two active resonant elements 13, two waves can be emitted or received simultaneously, without interference, since the signal from them are uncorrelated because of the plurality of passive resonant elements 12 creating a band-gap.
The passive resonant elements 12 are slots in an electric conductive plate of 24 mm length and 0.5 mm width. The first resonance frequency f1 corresponds to the above length and width (perimeter) of the passive resonant elements 12 slots. In that case, the first resonance frequency fl is approximately of 2.2 GHz.
The active resonant element 13 is a slot of 19 mm length and 0.5 mm width. The second resonance frequency f2 corresponds to the above length and width of the active resonant element 13 slot. In that case, the second resonance frequency f2 is approximately of 2.45 GHz.
The slots are distant from each other of 2 mm.
The device can then emit and receive wave at a central frequency of approximately 2.45 GHz corresponding to the second resonance frequency f2, and with a frequency bandwidth of approximately 100 MHz, said frequency bandwidth being comprised inside the frequency band-gap (Δf) of the passive resonant elements.
In this example, the first and second distances (d1, d3) are also lower than λ/10.
The size of this device in Y direction is twice lower than the size of
According to all the embodiments of the invention, the device for receiving and/or emitting an electromagnetic wave is small compared to the equivalent known devices of the prior art.
Such device has a high efficiency to emit or receive an electromagnetic wave, so that data can be transmitted to a great distance from the device.
Moreover, the device can be designed to provide a predetermined directivity diagram that is determined by the first and second region shapes (region with passive resonant elements and region with active resonant element).
Additionally, the device can comprise a plurality of active resonant elements that are isolated from each other by the passive resonant elements 12 band-gap. The device can be used for MIMO application with very low correlation between the channels.
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/IB2011/002453 | 5/6/2011 | WO | 00 | 10/31/2013 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2012/153164 | 11/15/2012 | WO | A |
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| 7242368 | Thevenot et al. | Jul 2007 | B2 |
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| 7522105 | LaComb | Apr 2009 | B1 |
| 7636070 | De Lustrac et al. | Dec 2009 | B2 |
| 20070080891 | De Lustrac | Apr 2007 | A1 |
| Number | Date | Country |
|---|---|---|
| 2801428 | May 2001 | FR |
| 2830131 | Mar 2003 | FR |
| 2854735 | Nov 2004 | FR |
| 2854738 | Nov 2004 | FR |
| 2863109 | Jun 2005 | FR |
| WO 0171774 | Sep 2001 | WO |
| WO 2008003991 | Jan 2008 | WO |
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| Entry |
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| Llombart, N. et al. “1-D scanning Arrays on Dense Dielectrics Using PCS-EBG Technology” IEEE Transactions on Antennas and Propagation, vol. 55, No. 1, Jan. 2007. |
| Abstract and English Machine Translation for French Patent No. FR 2801428. |
| Abstract and English Machine Translation for French Patent No. FR 2830131. |
| Abstract and English Machine Translation for French Patent No. FR 2854735. |
| Abstract and English Machine Translation for French Patent No. FR 2854738. |
| Abstract and English Machine Translation for French Patent No. FR 2863109. |
| Number | Date | Country | |
|---|---|---|---|
| 20140062821 A1 | Mar 2014 | US |
