FIELD OF THE INVENTION
[0001] The present invention relates to wireless antenna systems and arrangements, in particular
systems and arrangements including one or more phased array antennas.
BACKGROUND
[0002] Phased array antennas are well known, and are used for example to provide wireless
links. One or more phased array antennas may provide transmission and one or more
phased array antennas may provide reception.
[0003] Signal processing arrangements for modulating and otherwise providing suitable transmission
signals, and for receiving and demodulating received signals, are also well known.
[0004] Phased array antennas and signal processing arrangements are provided in many variations
for many different uses. In many applications, frequencies of less than 10GHz are
employed, requiring relatively large antenna sizes. For a given phased array antenna,
there will be limitations on its useful range (i.e. distance between transmitter and
receiver) of operation. Conventionally, to increase range, antenna size and/or power
must be increased.
SUMMARY OF THE INVENTION
[0005] The present inventors have realised it would be desirable to provide an antenna system
or arrangement that gives a required range of operation by a solution other than that
of increasing antenna size and/or power. The present inventors have realised this
would be particularly desirable in a context of achieving ranges of, say, 100m, with
small equipment sizes, as such a solution could efficiently be deployed in applications
where larger equipment would be less suitable, for example as a wireless communication
system between vehicles, e.g. between vehicles.
[0006] In a first aspect, the present invention provides an antenna system, comprising:
a phased array antenna; and a dielectric lens arrangement; wherein the dielectric
lens arrangement is arranged to magnify the effective aperture of the phased array
antenna.
[0007] The dielectric lens arrangement may be a single solid dielectric lens.
[0008] The solid dielectric lens may comprise a convex surface and a concave surface.
[0009] The convex surface may be substantially spherical.
[0010] The side of the dielectric lens arrangement closest to the phased array antenna may
be positioned within the near field of the phased array antenna.
[0011] The phased array antenna may be adapted to be operated at a frequency greater than
or equal to 50GHz.
[0012] The dielectric lens may be of a material having a dielectric constant greater than
or equal to 2.
[0013] The dielectric lens may be of a material having a dielectric constant greater than
or equal to 5.
[0014] The antenna system may be arranged such that the antenna system retains some ability
to electronically scan the beam provided by and/or being received by the antenna system.
[0015] The antenna system may be adapted to be used as a transmission antenna system.
[0016] The antenna system may be adapted to be used as a reception antenna system.
[0017] In a further aspect, the present invention provides a wireless communication system
comprising, as a transmission antenna system, at least one antenna system according
to any of the above aspects.
[0018] In a further aspect, the present invention provides a wireless communication system
comprising, as a reception antenna system, at least one antenna system according to
any of the above aspects.
[0019] In a further aspect, the present invention provides a wireless communication system
comprising, as a transmission antenna system, at least one antenna system according
to any of the above aspects, and further comprising, as a reception antenna system,
at least one antenna system according to any of the above aspects.
[0020] In a further aspect, the present invention provides a use of one or more antenna
systems according to any of claims 1 to 9 for communication between two vehicles.
BRIEF DESCRIPTION OF THE DRAWINGS
[0021]
Figure 1 is a schematic illustration (not to scale) of a wireless system;
Figure 2 is a schematic illustration (not to scale) showing an antenna system of the
wireless system of Figure 1;
Figure 3 is a schematic illustration (not to scale) showing certain dimensional details
of the antenna system of Figure 2;
Figure 4 is a diagram illustrating aspects of refraction by a spherical lens;
Figure 5 is a schematic illustration (not to scale) of grooves which are provided
at both surfaces of a dielectric lens forming part of the antenna system of Figure
2; and
Figure 6 is a schematic illustration (not to scale) of a phased array antenna 4 forming
part of the antenna system of Figure 2.
DETAILED DESCRIPTION
[0022] Figure 1 is a schematic illustration (not to scale) of a first embodiment of a wireless
system 1. The wireless system 1 comprises two antenna systems 2, which in this embodiment
are the same as each other. Each antenna system 2 comprises a phased array antenna
4 and a dielectric lens 6. The phased array antenna 4 is placed in front of, and spaced
apart, from the dielectric lens 6.
[0023] The phased array antenna 4 of a first of the antenna systems 2 (which may be termed
the transmission antenna system) is electrically coupled to a transmission module
8. The phased array antenna 4 of the other of the antenna systems 2 (which may be
termed the reception antenna system) is electrically coupled to a reception module
10.
[0024] The phased array antennas 4 are placed close to the respective dielectric lenses
6 so that in operation, in the case of transmission, millimetre waves emitted from
the phased array antenna 4 pass through the dielectric lens 6 before continuing onwards
away from the phased array antenna, and in the case of reception, external millimetre
waves falling on the dielectric lens 6 pass through the dielectric lens 6 before continuing
on to fall on the phased array antenna 4.
[0025] The transmission antenna system is positioned remote from the reception antenna system.
For example, the transmission antenna system may advantageously be placed on a first
vehicle, and the reception antenna system may be placed on a second vehicle. In operation,
when the transmission antenna system and the reception antenna system are sufficiently
aligned, i.e. in effect sufficiently pointed at each other (within angular ranges
that will be described in more detail later below), signals generated/modulated by
the transmission module 8 are transmitted from the transmission antenna system 2,
received by the reception antenna system, and demodulated/otherwise processed by the
reception module 10.
[0026] In other embodiments, only one of the antenna systems, e.g. either the transmission
antenna system or the reception antenna system, is as described above, and the other
antenna system is a conventional antenna system comprising a phased array antenna
but without a dielectric lens.
[0027] In yet further embodiments, either one, or both, of the above described antenna systems
are coupled to both a transmission module and a reception module, and may individually
be used for transmission and/or reception, as opposed to only transmission or only
reception.
[0028] In yet further embodiments, any of the above described arrangements are modified
by using plural antenna systems for either or both of the functions of transmission
and reception.
[0029] It will also be appreciated that, as well as the overall wireless system 1 being
an embodiment of the invention, paired arrangements of one or more transmission antenna
systems with one or more reception antenna systems also represent embodiments of the
present invention; and moreover, a single antenna system 2 (i.e. a phased array antenna
with a dielectric lens 2), with a transmission and/or reception module represents
an embodiment of the present invention; and also a single antenna system 2 (i.e. a
phased array antenna with a dielectric lens 2), without a transmission and/or reception
module represents in itself an embodiment of the present invention.
[0030] Figure 2 is a schematic illustration (not to scale) showing the antenna system 2,
comprising the phased array antenna 4 and the dielectric lens 6, in further detail.
In this embodiment, the dielectric lens 6 is a solid spherical lens, comprising a
convex curved outer surface 12 and a concave curved inner surface 14, where the curved
outer surface 12 is the surface further away from the phased array antenna 4 and the
curved inner surface 14 is the surface closer to the phased array antenna 4. The curved
outer surface 12 is larger than the curved inner surface 14. As a consequence, a further
extent of surface exists between the curved inner surface 14 and the curved outer
surface 12, which for convenience will be termed the remaining inner surface 15.
[0031] In overview, in operation, the dielectric lens 6 effectively acts as a magnifying
lens, in the standard way for such a lens, as follows. (For convenience, certain optical
terminology is used in the following summary of the effect of the lens, and likewise
for convenience certain properties of the millimetre waves employed are simplified
or schematised to allow the effect of the lens to be most readily appreciated.) The
operation will be described in terms of transmission. It will be appreciated that
the reverse operations occur in the case of reception. In operation, the phased array
antenna 4 emits electromagnetic waves (in this embodiment millimetre waves) 16 that
initially, in the so-called near field, may be considered as being nominally parallel
to each other, i.e. providing a nominally parallel beam 18. The curved inner surface
14 of the dielectric lens 6 is positioned relative to the phased array antenna 4 such
that the distance there between is smaller than the extent of the near-field, i.e.
smaller than the Rayleigh distance. Thus the nominally parallel rays 16 of the nominally
parallel beam 18 reach the curved inner surface 14 where they are diverged to provide
diverged rays 20. The diverged rays 20 then pass through the dielectric lens 6 to
reach the outer curved surface 12, where they are converged to be parallel to each
other again and thereby provide a nominally parallel beam 24 exiting the dielectric
lens 6 at the curved outer surface 12. The nominally parallel beam 24 is magnified
compared to the original nominally parallel beam 18 that was emitted by the phased
array antenna 4 and passed into the dielectric lens 6 through the inner curved surface
14, and hence is hereinafter referred to as the magnified nominally parallel beam
24. In other words, the dielectric lens 6 has in effect magnified the effective radiating
aperture of the phased array antenna 4 (in the case of reception the dielectric lens
6 in effect magnifies the effective reception aperture of the phased array antenna
4).
[0032] Figure 3 is a schematic illustration (not to scale) showing certain dimensional details
of the antenna system 2.
[0033] In this embodiment, the curved outer surface is substantially a spherical shaped
surface, with a radius R of approximately 0.035m (35mm). The centre of the emission
surface of the phased array antenna is approximately placed at the centre of the sphere
defining the spherical shaping of the outer curved surface 12.
[0034] In this embodiment, the inner curved surface 14 is substantially elliptical shaped
with a focal point behind the phased array antenna. More details of the functional
effect of this will be described later below with reference to Figure 4. In this embodiment,
the focal point is at a distance of approximately 17mm.
[0035] In this embodiment, the separation s between the centre of the radiating surface
of the phased array antenna and the axially aligned point (i.e. closest point or central
point) on the inner curved surface 14 of the dielectric lens 6 is approximately 0.005m
(5mm).
[0036] In this embodiment, the phased array antenna 4 is approximately square shaped, with
sides of length I approximately equal to 0.015m (15mm).
[0037] In this embodiment, the dielectric lens is made of solid nylon, with a dielectric
constant ε
r approximately equal to 3. However, in other embodiments, other materials with other
dielectric constant values may be used. Preferably a dielectric constant equal to
or greater than 2 is used. For example, PTFE with dielectric constant of approximately
2 may be used. Also for example, in other embodiments a material called "Eccostock"
(trademark) HIK 500F, available from Emerson & Cuming Microwave Products N.V., Nijverheidsstraat
7A, B-2260 Westerlo, Belgium, is used. In this embodiment, this material has a dielectric
constant of approximately 5. The effect of different dielectric constant values of
the material of the dielectric lens 6 will be discussed later below. Other examples
of materials with dielectric constant of approximately ε
r = 5, and which advantageously have relatively low loss at 60GHz, are boron nitride
and a material called "Macor" (trademark) available from Corning Incorporated Lighting
& Materials, Houghton Park CB-08, Corning, New York 14831.
[0038] In other embodiments, other types of lens arrangements (for example multi-lens telescope
arrangements such as a Keplerian refractor or a Galilean telescope arrangement) may
be used instead of the above described dielectric lens of this embodiment. However,
compared to other such possibilities, the use in this embodiment of the dielectric
lens 6 described above, i.e. a single solid lens of a relatively high dielectric material
and with a shape based on a spherical surface, advantageously provides a reasonable
amount of gain i.e. magnification, whilst only requiring a relatively small physical
size.
[0039] The operation of the antenna system 2 of this embodiment, and in particular the operation
of the dielectric lens 6, can further be understood by considering Figure 4, which
is a diagram illustrating aspects of refraction by a spherical lens. Figure 4 shows
a theoretical spherical lens surface (indicated in Figure 4 by reference numeral 40)
of radius R with a centre point indicated in Figure 4 by reference numeral 41, considered
in terms of a reference diameter direction (indicated in Figure 4 by reference numeral
42). For any given point (indicated in Figure 4 by reference numeral 44) on the spherical
lens surface 40, a height from that point to the reference diameter 42 is termed h;
for a ray originating from the centre of the sphere 41 and falling on the surface
point 44, the angle between the original direction of that ray and the output (refracted)
ray is termed θ; the distance between the focal point of the lens (indicated in Figure
4 by reference numeral 46) and the surface point 44, i.e. the focal length, is termed
f; and the angle between the line from the focal point 46 to the surface point 44
and the radius to the surface point 44 is termed ξ.
[0040] A spherical lens of constant dielectric constant brings a bundle of incident rays
to an approximate focus. The location of the focal point for paraxial rays depends
only on the dielectric constant of the sphere (see Figure 4). Using the small angle
approximation, the focal length f is given in terms of the radius of the sphere R
by

. When, for example, the dielectric constant is ε = 4, the focus lies on the circumference.
As the dielectric constant is increased, the focus approaches but never reaches the
centre of the sphere.
[0041] By virtue of the phased array antenna 4 being positioned behind the concave curved
inner surface 14 at the centre of the sphere, the operation is similar to that of
a Galilean telescope, i.e. the rays are approximately directed as illustrated in,
and described above with reference to, Figure 2.
[0042] The concave curved inner surface 14 is preferably designed to convert the cone of
rays from the convex outer surface 12 to a parallel bundle. The magnification m available
for such an arrangement is

and therefore depends only on the dielectric constant. For example, (as per one preferred
embodiment) a magnification of 2.236 is achieved by the use of the above mentioned
material with a dielectric constant equal to 5. By providing a magnification of 2.236
(in both azimuth and elevation), the useful range of the antenna system 2 is, to a
first approximation, increased by a factor of 2.236
2 i.e. approximately 5. Thus, in approximate terms, although using a phased array antenna
with a useful range of approximately 20m (as is the case for the phased array antenna
4 of this embodiment, which will be described in more detail later below with reference
to Figure 6), the overall antenna system 2 provides a useful range of approximately
100m. (Note each lens increases the effective aperture in both azimuth and elevation
dimensions.)
[0043] In other embodiments, the radius R of the lens can be freely chosen within reason,
but preferably it should be larger than the magnified image of the array. However,
if it is too small, diffraction may dominate.
[0044] By using a spherical shape for the convex outer curved surface 12 of the dielectric
lens 6, distortion or deviation arising from the different swept angles involved in
the operation of the phased array antenna 4 is reduced or avoided. However, in other
embodiments, this advantage may be traded off with improved gain at specific angles
by using shapes other than spherical, for example by using elliptical or hyperbolic
shaped surfaces. It will also be appreciated that the whole of the outer surface need
not be fully in compliance with the basic operational shape of the surface. For example,
the surface may be truncated with a cylinder shape at the rear to aid mounting of
the lens. Also for example, grooves or notches or ridges (in addition to the grooves
to be described later below with reference to Figure 5) may be included for the purposes
of fixing the dielectric lens mechanically to clamps or the like. Depending on their
positions or size, such variations may degrade performance but only to a limited extent
compared to the overall magnification and uniformity achieved by the lens, or may,
if located sufficiently radially distant from the magnified image of the antenna,
have no, or at least negligible, interplay with the magnification process.
[0045] By using an elliptical shape for the concave inner curved surface 14, "optical" performance
tends to be optimised. However, since a shallow curvature is preferable, the exact
details of the curved surface shape are not very significant, i.e. in other embodiments
other shapes may be used for the concave curved inner surface.
[0046] In this embodiment the inner curved surface 14 and the outer curved surface 12 are
both provided with (i.e. the surfaces comprise a further detail of shaping) with concentric
grooves for the purpose of providing, at least to some extent, impedance matching,
i.e. the grooves function as an anti-reflection measure. The grooves represent a way
of minimising the mismatch between the high dielectric constant of the lens and that
of free space. Figure 5 is a schematic illustration (not to scale) of the grooves
which are provided at both surfaces. The dotted line indicated by reference numeral
52 represents a hypothetical smooth form of the respective curved surfaces. The grooves
50 are provided by virtue of troughs 54 and ridges 56. The grooves are preferably
at less than half-wavelength pitch, which in the case of operation at 60GHz means
a pitch of 2.5mm or less is desirable. In this embodiment, a pitch of 1.5mm is provided,
with the ridges 56 and the troughs 54 each being 0.75mm wide. The height or depth
of the grooves is 0.85mm. The optimum values depend upon the intended frequency to
be used.
[0047] In other embodiments, anti-reflection properties may instead be provided by the use
of antireflection coatings applied to the curved surfaces, or by any other appropriate
means.
[0048] In the above described embodiments, the shape of the dielectric lens 6 may be provided
by any suitable manufacturing process, for example by machining a solid block of the
material or by casting.
[0049] Further details of the phased array antenna 4 of this embodiment will now be described.
Figure 6 is a schematic illustration (not to scale) of the phased array antenna 4.
In this embodiment the phased array antenna 4 comprises a total of fifty-two dipole-like
antenna elements 60 arranged in eight alternating columns of six and seven elements.
The overall size of the antenna is approximately 0.015m x 0.015m (15mm x 15mm). The
phased array antennas 4 of this embodiment provide thirty-six beams with wide elevation
and azimuth scan angular ranges to allow for non line of sight operation. These are
commercial units sold by AboCom Systems Inc. (trademark) of No.77, Yu-Yih Road, Chu-Nan
Chen, Miao-Lih Hsuan, Taiwan, R.O.C. that are provided for the WirelessHD standard
market (i.e. digital video data).
[0050] In this embodiment the phased array antenna is operated in the frequency range of
57 to 66GHz.
[0051] Beam-forming electronics are used to drive the array to produce a fixed set of beams
using phase shifters. These may be positioned directly behind the radiating array,
or may be provided in a separate module, for example being provided as part of the
transmission module 8. (In the case of reception, the corresponding electronics serves
to perform the receive signal amplification and beamforming function). This reception
electronics may be positioned directly behind the radiating array, or may be provided
in a separate module, for example being provided as part of the reception module 10.)
[0052] In this embodiment, as mentioned above, the phased array antenna 4 operating on its
own, i.e. without the dielectric lens 6, can generate a beam that covers a wide azimuth
and elevation scan angular range. The angular range of the antenna system 2, i.e.
the effect of the dielectric lens 6, is that the angular output range is reduced.
In this embodiment, the reduction in angular range is related to the reduction in
the beamwidth. In general the improvement in distance range is at a cost of angular
range. However, there are many applications where such a trade-off is either irrelevant
or at least bearable, for example in a vehicle to vehicle communications application
as mentioned earlier. Also, in some applications the relative positioning and directionality
between the transmission antenna system and the reception antenna system can be fixed,
in which case relatively narrow angular range can be tolerated (and may even be advantageous).
In yet further embodiments, the achievable azimuth angle can be traded off with the
achievable elevation angle, for example by use of asymmetrical lens shapes.
[0053] It will be appreciated that an advantage of the above described embodiments is that
increased distance range is achieved whilst retaining at least a significant extent
of the ability to electronically scan the beam.
[0054] In the above described embodiments the phased array antenna is operated at a frequency
between 57 to 66GHz. By using such a relatively high frequency, the physical size
of the dielectric lens can be kept small. Thus, in preferred embodiments, the phased
array antenna is operated at frequencies greater than or equal to 50GHz. However,
in other embodiments other frequencies may be used.
[0055] In the above described embodiments the phased array antenna is as described with
reference to Figure 6. However, this need not be the case, and in other embodiments
other implementations or details of phased array antenna may be used instead, for
example different sizes, different angular output, different numbers of antenna elements,
different numbers of beams, different beam properties, and so on.
[0056] Likewise, some or all of the various dimensions of the various elements employed
in the above described embodiments, e.g. sizes of the dielectric lens and the phased
array antenna, and spacing between the various elements employed in the above described
embodiments, may be different in other embodiments.
1. An antenna system, comprising:
a phased array antenna (4); and
a dielectric lens arrangement (6);
wherein the dielectric lens arrangement (6) is arranged to magnify the effective aperture
of the phased array antenna (4).
2. An antenna system according to claim 1, wherein the dielectric lens arrangement (6)
is a single solid dielectric lens (6).
3. An antenna system according to claim 2, wherein the solid dielectric lens (6) comprises
a convex surface (12) and a concave surface (14).
4. An antenna system according to claim 3, wherein the convex surface (12) is substantially
spherical.
5. An antenna system according to any of claims 1 to 4, wherein the side (14) of the
dielectric lens arrangement (6) closest to the phased array antenna (4) is positioned
within the near field of the phased array antenna (4).
6. An antenna system according to any of claims 1 to 5, wherein the phased array antenna
(4) is adapted to be operated at a frequency greater than or equal to 50GHz.
7. An antenna system according to any of claims 2 to 6, wherein the dielectric lens (6)
is of a material having a dielectric constant greater than or equal to 2.
8. An antenna system according to claim 7, wherein the dielectric lens (6) is of a material
having a dielectric constant greater than or equal to 5.
9. An antenna system according to any of claims 1 to 8, arranged such that the antenna
system retains some ability to electronically scan the beam provided by and/or being
received by the antenna system.
10. An antenna system according to any of claims 1 to 9, adapted to be used as a transmission
antenna system.
11. An antenna system according to any of claims 1 to 10, adapted to be used as a reception
antenna system.
12. A wireless communication system comprising, as a transmission antenna system, at least
one antenna system according to any of claims 1 to 9.
13. A wireless communication system comprising, as a reception antenna system, at least
one antenna system according to any of claims 1 to 9.
14. A wireless communication system comprising, as a transmission antenna system, at least
one antenna system according to any of claims 1 to 9, and further comprising, as a
reception antenna system, at least one antenna system according to any of claims 1
to 9.
15. Use of one or more antenna systems according to any of claims 1 to 9 for communication
between two vehicles.