MICROWAVE DISTRIBUTION NETWORK

Abstract

A microwave distribution network includes stacks of layers, each layer including unit cells. The unit cells have a coaxial input connected to three transmission lines with an angular span of 120°. The layers are configured as a hexagonal lattice formed with replicated unit cells. The coaxial inputs are at the hexagon corners. Each unit cell is connected to three neighbor unit cells. The coaxial inputs of the unit cells and neighbor cells are oriented on a Z-axis of a Cartesian system of axes in which the three transmission lines are on an XY plane, such that the input orientation on the Z-axis is opposite to the former unit cell on the same Z-axis. The distance between coaxial inputs is λ/4, where λ is the wavelength of a microwave distribution network operating frequency. Adjacent layers are interconnected by the coaxial inputs of the unit cells arranged in an opposite direction.

Claims

1. A microwave distribution network, comprising a stacking of a plurality of layers , each of the layers comprising a plurality of unit cells , wherein: the unit cells comprise a coaxial input connected to three transmission lines with an angular span of 120°, the coaxial input being orientated on an Z-axis of a Cartesian system of axes in which the three transmission lines are on an XY plane, the layers are configured as a hexagonal lattice formed with the unit cells by periodical replication, with the coaxial inputs placed at corners of the hexagons, such that each unit cell is connected to three neighbour unit cells, the coaxial inputs of the three neighbour unit cells being oriented on a Z-axis of a Cartesian system of axes in which the three transmission lines are on an XY plane, such that an orientation on the Z-axis is opposite to the an orientation of the coaxial input of the former unit cell on the same Z-axis, a distance between coaxial inputs is λ/4, wherein λ is the wavelength of an operating frequency of the microwave distribution network, and the adjacent layers are interconnected by the coaxial inputs of the unit cells that are arranged in opposite directions.

2. The microwave distribution network, comprising a stacking of a plurality of layers , each of the layers comprising a plurality of unit cells , wherein: the unit cells comprise a coaxial input connected to four transmission lines with an angular span of 90°, the coaxial input being orientated on an Z-axis of a Cartesian system of axes in which the four transmission lines are on an XY plane, the layers are configured as a square or rectangular lattice formed with the unit cells by periodical replication, with the coaxial inputs placed at corners of the square or rectangle, such that each unit cell is connected to four neighbour unit cells, the coaxial inputs of the four neighbour unit cells being oriented on an Z-axis of a Cartesian system of axes in which the four transmission lines are on an XY plane, such that an orientation on the Z-axis is opposite to an orientation of the coaxial input of the former unit cell on the same Z-axis, a distance between coaxial inputs is λ/4, wherein λ is the wavelength of an operating frequency of the microwave distribution network, and the adjacent layers are interconnected by the coaxial inputs of the unit cells that are arranged in opposite directions.

3. The microwave distribution network according to claim 1 , wherein the unit cells comprise a plurality of shielding vias surrounding the transition between the coaxial input and the transmission lines .

4. The microwave distribution network according to claim 1, wherein the unit cells comprise a substrate in which the transmission lines are placed and in which the coaxial input enters.

5. The microwave distribution network according to claim 1, wherein the transmission lines include stubs or width of lines or height of transmission lines or path lines.

6. The microwave distribution network according to claim 1, wherein the transmission coaxial inputs include tuning structures or screws or stubs.

7. An antenna array comprising a microwave distribution network of claim 1.

8. A reflector antenna system comprising a microwave distribution network of claim 1.

9. A lens antenna comprising a microwave distribution network of claim 1.

Description

DESCRIPTION OF FIGURES

[0026] FIG. 1 shows a unit cell.

[0027] FIG. 2 shows a hexagonal lattice formed after periodical replication of the unit cell.

[0028] FIG. 3 shows the periodicity condition and impedance point of view.

[0029] FIG. 4 is a scheme of the current divisor present at the intersection between the coaxial port and the three transmission lines, from the point of view of the transmission line.

[0030] FIG. 5 shows a stacking of layers.

[0031] FIG. 6 is a diagram of a simulated structure with 121 coaxial inputs.

[0032] FIG. 7 shows input port’s reflection, transmission and isolation between input and output ports.

[0033] FIGS. 8 and 9 show an example of power distribution on a 4-layer ODIN with a periodic layer for the ideal case.

DETAILED DESCRIPTION OF THE INVENTION

[0034] A new topology of structure, called Overlapped Distribution Network (ODIN) is proposed. The basic unitary cell of the network is shown in FIG. 1. The proposed structure is a 4-port network, whose dimensions could be tuned in order to guarantee an equal power distribution to each branch. The basic structure consists of a transition from a coaxial port or input to three equal transmission lines placed with an angular span of 120 degrees. The transmission lines can be strip-lines.

[0035] Some vias surrounding the transition can be placed to provide shielding and facilitate the coupling of the fields to the transmission lines.

[0036] Let P1 be the coaxial port, Z.sub.0 the characteristic impedance of the coaxial line and Z.sub.s the characteristic impedance of the transmission lines. The input impedance observed from P1 is directly obtained by calculating the parallel of the three transmission line impedances. Thus,

[00001]$Z_{in\_coax}=Z_s/3$

If perfect matching is desired, relation (2) is obtained straightforwardly.

[00002]$Z_S=3\cdot Z_0$

[0037] Let us assume now an infinite, periodical replication of the cell, connecting each cell to three neighbours. After this periodical transformation, all the ports of the network will be coaxial lines, working the transmission lines as interconnections between these coaxial ports (FIG. 2).

[0038] It is important to note that, within this replication, neighbour coaxial ports will present different orientations on the Z-axis. This means, if the coaxial port in the original cell is pointing upwards, the three nearest neighbours will point downwards. Following this fashion, their neighbours will point upwards, and so on. The distance between these ports will be now such that it satisfies a quarter of the wavelength conditions. The replication of the cell in the aforementioned manner implies the creation of a hexagonal lattice, as depicted in FIG. 2. Given the periodicity condition, since no end of the lattice is considered, it could be asserted that the impedance seen at the input each transmission line branch is the same, namely Z.sub.in. This impedance will be the result of the mutual influence among every neighbour cell. Each cell will be loaded by the rest of the network. Under the same assumption, the impedance seen at the end of each transmission line, namely Z.sub.A (corresponding to the parallel of the coaxial line and the other two transmission lines, connected to the rest of the network) will also be the same at every intersection. For a clearer perspective from the impedance point of view, refer to FIG. 3. Let Z.sub.0 and Z.sub.s be the characteristic impedance of the coaxial line and the transmission line respectively. Since the length of the transmission line corresponds to a quarter of a wavelength, the transmission lines work as quarter-wave impedance transformers, following the well-known relationship:

[00003]${\text{Z}}_{\text{in}}={\text{Z}}_{{\text{s}}^2}/{\text{Z}}_{\text{A}}$

Where Z.sub.A is calculated as the parallel impedance between one coaxial port and two transmission lines loaded with the rest of the periodical structure.

[00004]$\begin{array}{c}{\text{Z}}_{\text{A}}={\text{Z}}_0//{\text{Z}}_{\text{in}}//{\text{Z}}_{\text{in}}\\ 1/{\text{Z}}_{\text{A}}=1/{\text{Z}}_0+1/{\text{Z}}_{\text{in}}+1/{\text{Z}}_{\text{in}}\\ {\text{Z}}_{\text{A}}={\text{Z}}_0\cdot {\text{Z}}_{\text{in}}/\left(2\cdot {\text{Z}}_0+{\text{Z}}_{\text{in}}\right)\end{array}$

[0039] Given that, in order to ensure impedance matching at the coaxial ports, Z.sub.in=3.Math.Z.sub.0, and substituting (4) in (3), the following relationship between the characteristic impedance of the coaxial lines and the transmission lines is obtained (5).

[00005]${\text{Z}}_{\text{S}}={\text{Z}}_0\cdot \text{sqrt}\left(9/5\right)$

[0040] Furthermore, it can be also checked that:

[00006]${\text{Z}}_{\text{A}}=3\text{/5}\cdot {\text{Z}}_0$

[0041] At this point, since the input impedance seen at each branch is the same, it can be stated that the total power entering the network from an only coaxial input port is divided equally among the three transmission lines. Following this assumption, the power delivered to the neighbour coaxial ports can be calculated as the power delivered to a Z.sub.0 Ω load in a current divisor with three parallel impedances: Z.sub.0 // Z.sub.in // Z.sub.in from the point of view of Z.sub.A. For a clearer idea, refer back to FIG. 2, as well as to FIG. 4. Here, an auxiliary voltage V.sub.A could be defined from the relation between power and voltage (7a). Subsequently, it can be obtained that the power delivered to the load Z.sub.0 corresponds to ⅗ of the power available at the input transmission line. Therefore, it is concluded that the power delivered to each coaxial port, neighbour to the input coaxial, will be:

[00007]$\text{P}=\text{V}\cdot \text{I}={\text{V}}^2\text{/Z}$

[00008]${\text{P}}_{\text{Z0}}={\text{V}}_{\text{A}}{}^2{\text{/Z}}_0={\text{P}}_{\text{A}}\cdot {\text{Z}}_{\text{A}}{\text{/Z}}_0=1\text{/3}{\text{P}}_{\text{T}}\cdot 3\text{/5}=1\text{/5}{\text{P}}_{\text{T}}$

[0042] Where P.sub.T stands for the total input power coming from the first coaxial port. Until now, it has determined: the amount of power delivered to each branch from the coaxial port (one third each) and the amount of power delivered to each neighbour port (three-fifths of the available power at each branch, namely one-fifth of the total power). From these results, it can be deduced that six-fifteenths of the total power (one per transmission line branch) are being delivered to the rest of the network. As stated in (7b), three-fifths of the power will be delivered to the coaxial port (⅟25 of the total power, namely -14 dB), which will be the nominal isolation between in-plane consecutive coaxial ports (this means, consecutive coaxial ports with the same orientation in the Z-axis).

[0043] Up to this point, the main features and behaviour of the network have been presented and its properties under a periodicity condition have been discussed. The next step involves the stacking of several layers of the hexagonal lattice, as sketched in FIG. 5. With this regard, it is important to note that it was stated that the coaxial ports are arranged with alternately directions. This feature will allow the interconnection of the layers and the longitudinal propagation of the energy across the structure.

[0044] Reference is made to to FIGS. 8 and 9 to see an example representation of the power distribution of an N=4 scenario (this means, one third of the power is delivered to each neighbour port). Here, dark circles represent the power inputs at each layer, while light circles represent the output ports at each layer. Smaller light circles represent coaxial lines pointing downwards and smaller dark circles correspond to the ones pointing upwards at N=1. For N=2,3... their orientation shall be exchanged alternatively at each layer, in order to follow an upward propagation. The power is distributed within each layer, concentrating its most part at the central position with respect to the input port at Layer 1. As it can be seen, since the side of the hexagon corresponds to a quarter of a wavelength, the distance between consecutive radiating elements is lower than half a wavelength.

[0045] In order to provide an example of the performance of the network, as single, finite layer of the structure, as depicted in FIG. 6 was simulated in a circuital simulator software. The coaxial ports were modelled by lumped ports with Z.sub.0 = 50 Ω. The L- Band was chosen as the band of operation and a reference frequency f.sub.0 of 1.5 GHz was chosen to design the quarter wave transformers. The fact that the topology is composed of resonant elements infers the resonant behaviour of the network. Since simulating an infinitely periodical structure was unfeasible, a reasonably large structure with 121 ports was simulated. It was observed that the transmission to a neighbour port (for example, from Port 1 to Ports 2, 6 and 10 in FIG. 6) was around -6.5 dB and the isolation between consecutive ports to roughly -16 dB.

[0046] Regarding non-consecutive ports, we can distinguish between two types of non-consecutive ports: the ones located at the centred normal-axes of the three symmetry axis (ports 17, 21, 25, 29, 33 and 37), and the ones which are not (15, 19, 23, 27, 31 and 35) - See FIG. 6 for a clearer view. It has been seen that the isolation between port 1 and ports of the first type present a higher isolation (below 35 dB) than the rest (below 20 dB). All these parameters are represented in FIG. 7.

[0047] In FIG. 8 it can be seen that the signal that enters through one of the inputs, placed in one of the six corners of a hexagon, will distribute the power mainly through the three nearest coaxial outputs to the upper layer, and these in turn will do the same to the next, so that the signal is distributed over an increasingly wide area. The signal is radiated by all the radiating elements that receive a significant part of the introduced signal.

[0048] FIGS. 8 and 9 show an example of power distribution on a 4-layer ODIN with a periodic layer for the ideal case. Dark circles represent the sources on each layer. Light circles with a number represent the receiving nodes (output ports) on each layer. In this scenario of four layers, the power division given by the network could be used to feed an hexagonal array of 19 radiating elements.

[0049] Several layers of the structure could be appropriately stacked in order to increment the number of radiating elements, thus defining a bigger radiating area for each one of the beams, which could be highly overlapped while sufficiently isolated from each other.

[0050] The transmission lines 3 may include stubs or width of lines or height of transmission lines or path lines. The transmission coaxial inputs 2 may include tuning structures or screws or stubs.

[0051] Another possibility is to obtain a square or rectangular lattice after the periodical replication of unit cells 1 that comprise a coaxial input 2 connected to four transmission lines 3 with an angular span of 90°, the coaxial input 2 being orientated on an Z-axis of a Cartesian system of axes in which the four transmission lines 3 are on an XY plane.

[0052] Although the present invention has been fully described in connection with preferred embodiments, it is apparent that modifications can be made within the scope, not considering this as limited by these embodiments, but by the content of the following claims.