Patent Application
20080198081
In the IEEE Transactions on Antennas and Propagation Vol. 51 No. 7 July 2003 pages 1572-1581 an article has been published titled “Green's function for an Infinite Slot Printed Between Two Homogeneous Dielectrics, Part I: Magnetic Currents”, by Andrea Neto and Stefano Maci. A second part of this article has been published in the IEEE Transactions on Antennas and Propagation Vol. 52 No. 3 March 2004, on pages 666-676. The first article mentions the possibility of building a sub-millimetre wave receiver that is integrated with a dielectric lens and that contains a slot printed on an infinite slab.
The articles describe the properties of electromagnetic waves that travel along a structure with a conductive ground plane that contains a narrow elongated non-conductive slot, when two dielectric media with different dielectric constants ε1 ε2 are present on opposite sides of the ground plane. It is shown that in this configuration a wave travels along the length of the slot, and that part of the wave energy is radiated under a predetermined angle relative to the ground plane.
The articles refer to the possibility of using this phenomenon to realize a leaky wave antenna, but give no details about the structure of such an antenna. In a leaky wave transmission antenna an electromagnetic wave travels along a wave guiding structure so that at successive points along the structure each time a fraction of the wave energy is radiated to the far field. As a result the wave energy gradually decreases along the structure. The travelling wave defines predetermined phase relationships between the radiation from different points along the structure and thereby a direction (if any) in which the radiation from the points leads to coherently radiation, so that the structure acts as an antenna. Usually, leaky wave antennas have a limited bandwidth, which is defined by the characteristic dimensions of the wave guiding structure.
Among others, it is an object of the invention to provide for a broadband antenna.
Among others, it is another object of the invention to provide for a feed structure for a broadband antenna.
Among others, it is a further object of the invention to provide for a multiple frequency feed structure for a broadband antenna.
The antenna according to the invention is set forth in claim 1. According to the invention an antenna with an at least partly conically shaped dielectric body is provided. The conical shape is such that the body has a series of cross-sections shaped like a truncated ellipses. Of the two foci of each ellipse a first one lies on a truncation line along which the truncated ellipse ends. An elongated wave carrying structure, such as a linear non-conductive slot in a conductive ground plane or a conductive track, extends along a focal line through the first foci of the truncated elliptical cross-sections. The second focus lies within the body. The truncation line extends perpendicularly to an axis of the ellipse through the foci. If a conductive ground plane is used, the ground plane adjoins the surface formed by the truncation lines of successive cross-sections.
It has been found that the dielectric body with elliptical cross-sections has the effect that the properties of wave propagation along the elongated wave carrying structure closely resemble the theoretical properties that would apply if a dielectric body that occupy an infinite half-space were used. That is, the speed of propagation hardly depends on wavelength as long as the wavelength is considerably larger than the width of the wave carrying structure. This results in coherent leaky wave radiation in a direction at an angle with respect to the focal line, the angle being substantially wavelength independent, so that broadband antenna behaviour is realized. Preferably the elongated wave carrying structure has a linear straight-line shape, but non-linear shapes, combined with corresponding size variations and offsets of the elliptical cross-sections may be used as an alternative to realize special antenna patterns.
Preferably the main axis of each of the elliptical shapes (the axis through the two foci) coincides with the direction of coherent propagation of the leaky wave. In this way the best approximation of the effect of an infinite dielectric half space is obtained.
Preferably the size of the cross-sections tapers along the cone so that a virtual line, which runs through the points on the perimeters of the elliptical shapes that are furthest from the first focus, is perpendicular to the direction of coherent propagation of the leaky wave. In this way optimal coupling of leaky wave radiation from the dielectric body to the exterior is realized.
Preferably the ellipticity of the elliptical shape is substantially equal to a square root of a relative dielectric constant of the dielectric material. This ellipticity applies to cross-sections in virtual plane that are oriented so that the truncation line is perpendicular to the focal line. This further optimizes the broadband behaviour.
In an embodiment a feed structure is provided integrated on a surface of the body defined by the truncation lines of the elliptical shapes of the cross-sections. This makes it possible to realize a cost-effective efficient feed. As used herein the term “feed” applies to transmission as well as reception with the antenna, that is, both to transfer of field energy to and from the wave carrying structure.
In a further embodiment the feed structure that comprises a coplanar wave guide with a pair of parallel non conductive feed slots in the ground plane with a tongue of conductive material in between. The coplanar wave-guide extends transverse to and across the antenna slot in the ground plane, and is terminated so that a short-circuit impedance arises in a coplanar waveguide at a position where the coplanar waveguide crosses the antenna slot. In this way optimal coupling is realized between the feed structure and the antenna slot. Preferably a part of the antenna slot extends beyond the point where the coplanar waveguide crosses the antenna slot. This part of the antenna slot extends so far that at an operation frequency waves excited in said part are reflected in phase back to the point where the coplanar waveguide crosses the antenna slot. In another embodiment a plurality of coplanar wave guides are used as feed structures for different frequencies, arranged so that fields of each frequency are presented with open-circuit impedance at the crossing points of all but one of the coplanar wave guides. In this way optimal isolation between the feed structures is realized.
Similar feed structures can be realized when a conductive track is used as wave carrying line.
The antenna may be used in combination with transmission and/or reception apparatus that is arranged successively and/or simultaneously to supply and/or receive the signals with mutually different frequencies that are far apart in frequency, for example at least a factor of two apart or even more. Efficient antenna behaviour (i.e. with well defined main lobes) for all these frequencies is realized with a single cone shaped antenna structure. Even transmitter and/or receptor equipment that handles signals with frequencies that are further apart may be used with effective antenna behaviour for all these frequencies.
These and other objects and advantageous aspects of the invention will be described by non-limitative examples using the following figures.
Operation of the antenna is based on the fact that the propagation speed of waves along a slot 14 in a conductive ground plane 12 is substantially independent of the wavelength of the wave, if ground plane 12 is bounded by two infinite half-spaces of mutually different dielectric constant, provided that the slot width is substantially smaller than the wavelength (smaller than a quarter of the wavelength). This means that such a slot will act as a leaky wave antenna, which radiates into one of the half-spaces in a direction that is independent of the wavelength of the radiation.
In practice infinite half spaces of dielectric material are of course impossible. This means that finite bodies of material must be used, but normally the finite size of the body affects the speed of propagation of the waves along antenna slot 14 in a wavelength dependent way. This wavelength dependence limits the antenna bandwidth, and makes the direction of radiation wavelength dependent.
In the present antenna, the wavelength dependence is minimized by the use of a dielectric body 10 with truncated elliptical cross-sections with one focus at the position of the antenna slot 14. Preferably, cross-sections through plane parallel to the direction of propagation of the leaky wave through the dielectric have this shape and have their first focus at the antenna slot 14. As will be appreciated this direction depends on the speed of wave propagation along antenna slot 14, which in turn depends on the dielectric constants of the dielectric material of body 10 and the surrounding space. The required direction can be determined theoretically, by means of simulation or by means of analytical solutions, or experimentally, by observing the direction of propagation in the dielectric body.
The half-space below ground plane 12 is formed by air (or a vacuum, or by some other gas or fluid). The upper half-space is approximated by the dielectric body 10. Because of the elliptical cross-sections radiation from the antenna slot 14 can only react back on the antenna slot 14 after two reflections on the perimeter of the dielectric body 10. This minimizes the effect of the finite size of dielectric body 10, with the result that the wavelength independent propagation speed for an infinite half space is closely approximated. Preferably, the elliptical cross-sections are shaped so that their eccentricity substantially equals the square root of the relative dielectric constant of the dielectric body 10 with respect to that of the surrounding space.
The result is that radiation leaks from antenna slot 14, giving rise to wavefronts 30 at an angle φ to ground plane 12, the angle φ being determined by the speed of propagation along antenna slot 14, which is a function of the dielectric constant of the dielectric body but is substantially independent of the wavelength. In the case of the example where the dielectric constant is 3.27 the angle φ equals approximately forty degrees.
In the embodiment of the figures the size of the elliptical cross-sections tapers towards the end of the antenna structure so that, at least on the main axes 22 of the ellipses, the wave-fronts 30 of equal phase run parallel to the top line surface 32 at the top of the ellipse (where the main axes 22 cross the surface of the ellipse) toward which the wave-fronts 30 travel. As a result, the wave has normal incidence on top line surface 32 and proceeds with wave-fronts in the same direction after leaving the dielectric body. This arrangement with a tapering so that top line surface 32 is substantially perpendicular to the direction of propagation of the radiated wave is preferred to minimize reflections. However, without deviating from the invention top line surface 32 may be at an angle with respect to the wave-fronts 30, as long as the angle is kept so small that no total reflection occurs this merely results in breaking of the direction of radiation when the radiation leaves dielectric body 10, with some increased loss due to reflections.
As shown, ground plane 12 extends substantially over the full width of the truncations, but no further. This is convenient for mechanical purposes, but not essential for radiative purposes: without deviating from the invention the ground plane may extend beyond the elliptical cross-sections or cover only part of the truncation. Preferably the width of the ground plane 12 away from the slot is so selected large that it contains the area wherein the majority of the electric current flows according to the theoretical solution in the case of an infinite ground plane, for example so that the ground plane 12 extends over at least one wavelength on either side of the slot 14 and preferably over at least three to four wavelengths.
A conductive track may be used instead of non-conductive antenna slot 14 that is shown in the figures, when the conductive ground plane 12 is omitted or replaced by a non-conductive ground plane. Like the antenna slot 14, such a conductive track that extends through one of the foci of successive cross-sections gives rise to substantially wavelength independent propagation speed and leaky wave radiation that provides an antenna effect.
Typically a single non-conductive slot or conductive track extends through the focal line. In the case of the slot this leads to a propagating field structure with electric field lines from one half of the ground plane to the other and magnetic field lines through the slot, transverse to the ground plane. Preferably no additional slot is provided in parallel with the slot. However, a similar propagating field may be realized with one or more additional slots in parallel to the slot, provided that these slots are excited in phase with the excitation of the slot, or at least not excited completely in phase opposition to the excitation of the slot. Out of phase (but not opposite phase) excitation of different slots may be used to redirect the antenna beam.
Similar considerations hold for the conductive track, except that the role of magnetic and electric fields is interchanged. Preferably a single conductive track is used, but more than one track may be used, provided that the tracks are preferably not excited in mutual phase opposition.
Although the invention is illustrated for the case of transmission of radiation, it will be realized that, owing to the principle of reciprocity, the antenna also operates to receive radiation from the direction in which it can be made to radiate, i.e. from a substantially wavelength independent direction.
The feed structure makes use of magnetic field excitation, which excites a wave in antenna slot 14 by means of a magnetic field in the slot with field lines substantially perpendicular to ground plane 12. Such a magnetic field can be induced with a conductor that crosses the antenna slot, such as the tongue between feed slots 40.
Because the coplanar wave guide ends in a short-circuit at antenna slot 14, a current maximum is created (and therefore a magnetic field maximum) at the position of antenna slot 14. Thus maximum excitation of waves in antenna slot 14 is realized. Antenna slot 14 extends over the length of the antenna in one direction and for a finite length 44 beyond the point where feed slots 40 end in antenna slot 14 in the other direction. The finite length 44 preferably corresponds to a quarter wavelength of the waves (optionally plus an integer number of half wavelengths), so that waves that are reflected at the end of finite length are in phase with the directly excited wave. At the end of feed slots 40 opposite to antenna slot 14 a feed connection 42 to a transmitter or receiver circuit (not shown) is provided. Feed connection 42 is arranged to apply a symmetric field from a central portion of ground plane 12 between feed slots to the parts of the ground plane on either side of feed slots 40. Optionally, conductive bridges 46 couple the parts of the ground plane on either side of feed slots 40 to suppress anti-symmetric modes.
It should be noted that the length of the various slots of the feed structure limit the bandwidth of the antenna. Typically a useful frequency bandwidth of 50% of the central frequency can be reached.
It will be realized that feed slots 40 may extend through antenna slot 14 instead of terminating at antenna slot 14. In this case the feed slots 40 may extend for an integer number of half wavelengths, the tongue being connected to the ground plane at the end, so that a short-circuit impedance is realized in the coplanar waveguide at the position where it crosses antenna slot 14. Alternatively, the tongue may end in an open-circuit, in which case the feed slots 40 preferably extend for a quarter wavelengths (plus any number of integer wavelengths) to realize a short-circuit impedance in the coplanar waveguide at the position where it crosses antenna slot 14. Due to impedance effects of the way the tongue is terminated a slight deviation from these lengths may be required to create a short-circuit impedance at the position where it crosses antenna slot 14.
Isolating structures 54, 56 serve to suppress cross-coupling between the feed connections 42, 52. In operation fields of respective, mutually different frequencies are applied to the feed connections 42, 52. Cross-coupling is realized by minimizing the magnetic field coupling at the point where a particular feed structure crosses antenna slot 14 for all applied frequencies but the frequency of the field that is applied by the feed connection 42, 52 of the particular feed structure (in the example of the figure the magnetic field couplings at the respective crossings each needs to be minimized only for one respective frequency). The magnetic field coupling is realized by providing an open-circuit impedance at the point where a feed connection 42, 52 supplies the field to antenna slot 14 for the non-coupling frequency (or frequencies).
In the example, one frequency is twice the other frequency. The slots of the isolating structure 54 that face the highest frequency feed connection 42 end in a short-circuit and have a length of half a wavelength for that frequency, and consequently, a quarter of a wavelength for the lower frequency of the other feed connection 52. This results in a short-circuit impedance at the position antenna slot for the high frequency and an open-circuit impedance at that position for the low frequency. As a result there is maximum coupling between the feed structure and antenna slot 14 for the highest frequency and minimum coupling for the lowest frequency.
The slots of the isolating structure 54 that face the lowest frequency feed connection 52 end in an open-circuit and also have a length of half a wavelength for the highest frequency, and consequently, a quarter of a wavelength for the lower frequency. This results in a short-circuit impedance at the position antenna slot for the low frequency and an open-circuit impedance at that position for the high frequency. As a result there is maximum coupling between the feed structure and antenna slot 14 for the lowest frequency and minimum coupling for the highest frequency.
Due to impedance effects of the way the tongues are terminated slight deviations from these lengths may be required to create short-circuit and open-circuit impedance at the position where it crosses antenna slot 14.
Preferably, the length of the slot between the feed structures and the finite length 44 are a quarter wavelength of the lower frequency. Thus, waves that are reflected back into antenna slot 14 from the end of finite length 44 are in phase with directly excited waves for both frequencies.
It should be appreciated that the actual antenna structure with antenna slot 14 is suitable for an extremely broad band of frequencies. The frequencies of the example, which are a factor two apart easily fit into this broadband. In the example only the feed structure limits the bandwidth. In practice a dual band antenna is realized which can be operated in two bands of about 30% bandwidth (width divided by central frequency).
Although the feed structure has been described for the example of excitation with two frequencies, of which one is twice the other, it should be appreciated that different feed structures are possible for different combinations of frequencies, or for a greater number of frequencies. In this case more complicated isolating structures may be required to provide substantially open-circuit impedances for “other” frequencies at the points where fields are fed to antenna slot 14. Also for example antenna slot 14 may be split into branching slots in the feed structure to accommodate several frequencies.
As another example measures to suppress cross-coupling may be taken in the transmission and/or receiver apparatus 60 that is connected to the feed connections. Furthermore, it should be understood that, instead of integrated coplanar waveguides, other types of feed structures could be used, such as external waveguides that interface with antenna slot 14.
When a conductor track is used instead of antenna slot 14, feed structures may be used that are the dual of the feed structure for antenna slot, i.e. wherein conductive parts are replaced by non-conductive parts and vice versa. In this case, instead of the coplanar wave guides bifilar feed structures are used, composed of a pair of adjacent conductors.
By now it will be appreciated that an extremely broadband antenna structure is realized by means of an antenna structure with a dielectric body of truncated elliptical cross-section, with a ground plane with a slot that extends through the foci of the elliptical cross-sections or a conductor that extends through the foci. Transmitter and/or receiver equipment 60 may be attached to the antenna structure to supply and/or receive fields of widely different frequency simultaneously and/or successively to the antenna structure for effective transmission and/or reception. Various feed structures may be used to excite or receive waves from the antenna slot. In an embodiment the feed structures may be integrated in the ground plane. Typically, the feed structures are selected dependent on the frequency or frequencies at which the transmitter and/or receiver equipment 60 uses the antenna structures. Although specific feed structures have been shown, it should be appreciated that other feed structures are possible, such as a waveguide that debouches at some position in the slot, or along a range or series of positions. If the antenna is used at widely different frequencies respective feed structures for such different frequencies may be used. Especially when these frequencies are far apart (e.g. a factor of ten) it is not very difficult to ensure that different feed structures for the respective frequencies do not interfere with each other.
Although a preferred antenna structure has been shown which is conical along its entire length with a straight line through the focal points, it should be appreciated that without deviating from the invention only part of the antenna may be conically shaped and that the line through the focal points may be curved. In the former case the conically shaped part provides for a directional behaviour of the antenna beam. A curved line (and therefore a curved slot or conductor track) results in locally varying directions of propagation of the leaky wave. By varying the size of the ellipses in a corresponding way it can be ensured that leaky waves from different parts of the focal line through the focal points interfere coherently after leaving dielectric body. Also multiple antenna lobes may be realized for example by using slots containing different parts at an angle with respect to one another and/or truncated elliptical cross-sections that taper in different ways at different points along the conical body.
| Number | Date | Country | Kind |
|---|---|---|---|
| 04077132.1 | Jul 2004 | EP | regional |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/NL05/00513 | 7/15/2005 | WO | 00 | 4/30/2008 |
