EP1592081B1 - Microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board - Google Patents
Microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board Download PDFInfo
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- EP1592081B1 EP1592081B1 EP04425300A EP04425300A EP1592081B1 EP 1592081 B1 EP1592081 B1 EP 1592081B1 EP 04425300 A EP04425300 A EP 04425300A EP 04425300 A EP04425300 A EP 04425300A EP 1592081 B1 EP1592081 B1 EP 1592081B1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P5/00—Coupling devices of the waveguide type
- H01P5/08—Coupling devices of the waveguide type for linking dissimilar lines or devices
- H01P5/10—Coupling devices of the waveguide type for linking dissimilar lines or devices for coupling balanced lines or devices with unbalanced lines or devices
- H01P5/107—Hollow-waveguide/strip-line transitions
Definitions
- the present invention relates to the field of microwave circuits and apparatuses and more precisely to a microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board.
- the invention is referred both to a method for manufacturing the transition and the transition itself.
- Microstrip to waveguide transitions embodied with high-loss dielectric substrates for PCB manufacturing are known in the art.
- the Applicant of the present invention filed on 30-5-2002 an European patent application indicated as Ref.[1] in the REFERENCES listed at the end of the description.
- Ref.[1] the operating frequency range of the transition was extending until to 35 GHz on fibre reinforced glass (FR4) substrates.
- the multilayer board made use of a thick copper layer as second layer of the build-up wafer structure to provide mechanical stiffness to the FR4 substrate for the connection of a rectangular waveguide on the bottom face.
- the copper layer was milled to lay bare the dielectric window of a slot transition and obtain in the meanwhile a sort of flange around it for mounting the waveguide.
- the optimistic value of 80 GHz had been calculated for the only wave propagation along the microstrip without taking into due consideration the effects of microstrip to waveguide transitions.
- Fig.1a shows a metallic layout laid down on the upper face of a dielectric FR4 substrate belonging to a multilayer structure.
- the layout includes a microstrip which extends along the longitudinal symmetry axis of the substrate and terminates with a metal patch.
- the microstrip and the remaining circuitry are encircled by a shielding metallic layout delimiting a rectangular unmetallized window, corresponding to a dielectric window, entered by the patched microstrip.
- the perimetrical metallization of the dielectric window is shaped as a rectangular frame with four unmetallized circle at the four corners in correspondence of threaded holes through the multilayer structure.
- Fig.1b shows a thick copper layer glued to the bottom face of the dielectric substrate to form a metal core giving stiffness to the multilayer structure and constituting a ground plane for the upper microstrip.
- the metal core is milled and completely removed to lay bare the dielectric substrate in correspondence of the dielectric window, so that the patch is visible from the rear due to the semitransparency of the FR4 layer.
- Fig.2a is a cross-section along the axis A-A of fig.1a .
- the figure shows the structure of the multilayer including three dielectric substrates, and the metal core.
- the upper and the lower dielectric substrates are metallized wile the interposed one is used as insulator.
- the end of a rectangular waveguide joins the rectangular window milled in the metal core in correspondence of the dielectric window of the upper substrate, so that the opening in the metal core is a continuation of the waveguide to the dielectric window of the substrate.
- a metallic lid placed upon the frame of the upper face is fixed to the multilayer structure by means of four screws at the corner of the frame penetrating into the upper dielectric substrate, the metal core (flange) and the walls of the rectangular waveguide.
- the metallic lid is a hollow body with a rectangular recess faced to the unmetallized window. In operation, the patched end of the microstrip which comes into the dielectric window acts as an electromagnetic probe for radiating into the closed space around it.
- the dimensions of the patch are calculate so as to transfer the energy from the feeding microstrip to the waveguide efficiently.
- the screwed metallic lid is used as a reflector to prevent propagation from the patch in the opposite direction to the waveguide. To this aim the recess of metallic lid acts as a back short for the signal. From the above considerations it can be conclude that the probe and the dielectric window in communication with the waveguide constitute a microstrip to waveguide transition that transforms the "quasi-TEM" propagation mode of the microstrip into the TE 10 mode of the rectangular waveguide.
- the electromagnetic properties of the transitions are reciprocal, so that the same structure used by the RF transmitter for conveying inside the waveguide a transmission signal from the microstrip is also used by the receiver for conveying a RF reception signal from the waveguide to the microstrip.
- Fig.2b shows a series of metallized through holes (via-holes visible in Fig.2a ) regularly spaced along the frame.
- These via-holes around the transition zone have been introduced successively the filing of Ref.[1] to the aim of improving the performances of the transition at the higher frequencies (35.5 GHz) of the operating range. This statement is possible because the transition at Ref.[1] and the transition of the present invention are both developed in the laboratories of the same Applicant.
- the via-holes supply to the lack of continuity of the waveguide through the thickness of the dielectric substrate around the zone of the transition.
- Fig.3 is a photography of the layout of the transceiver which depicts the real arrangement of via-holes; as it can be noticed, several rows of metallized holes are needed to a satisfactory operation in the SHF range (not in the EHF).
- the European patent application indicated in Ref.[5] discloses a high-frequency package comprising a dielectric substrate, a high-frequency element that operates in a high-frequency region and is mounted in a cavity formed on said dielectric substrate, and a microstrip line formed on the surface or in an inner portion of said dielectric substrate and electrically connected to said high-frequency element, wherein a signal transmission passage of a waveguide is connected to a linear conducting passage or to a ground layer constituting the microstrip line.
- an end of the linear conducting passage is electromagnetically opened, so that the end portion works as a monopole antenna inside the waveguide that is connected.
- the aforementioned high-frequency package has been designed to operate at millimetric waves using costly and rigid substrate materials having a low dielectric constant and small losses (e.g. alumina).
- the complicated structure makes the sealing of the multilayer to the waveguide and the application of an upper closing lid both difficult to obtain. Another difficult arises in correctly terminating the irradiating microstrip inside the waveguide.
- the main object of the present invention is that to overcome the drawbacks of the known art and indicate a microstrip to waveguide transition obtainable on PCBs arranged for operating at the microwaves with good performances in the nearest EHF range (up to 80 GHz)
- the invention achieves said object by providing a method to manufacture a microstrip to waveguide transition, as disclosed in the method claims.
- Another object of the invention is a microstrip to waveguide transition obtained according to the method, as disclosed in the device claims.
- the transition disclosed at Ref.[1] is now completely redesigned in order to remove almost completely the former dielectric diaphragm from the space of the transition.
- Another fundamental difference from the prior art is that the waveguide now penetrates the dielectric substrate to connect the metallic lid, without breaking the continuity of the metallic walls, except for the two grooves whose effect is completely marginal.
- the frame of via-holes is completely unnecessary to confine the electromagnetic field, and also the drawbacks highlighted at points 1 and 2 are overcome.
- the waveguide part of the transition and the other mechanic part of the transceiver can be obtained by means of numerical control manufacturing techniques starting from a rough metal block.
- Microstrip to waveguide transitions for rectangular waveguides according to the present invention are the easiest to obtain, but the same approach is applicable to obtain transitions for circular or elliptic waveguides.
- a microstrip to waveguide transition, and vice versa, used to connect both the transmitter and the receiver amplifiers to the same antenna by means of a duplexer, is the only part of the transceiver the present invention is concerned with.
- the substrate 1 gives support to a metallic layout including among other things a microstrip 2 placed along the axis of longitudinal symmetry of the figure.
- the microstrip 2 terminates with a small patch 3 nearby the centre of a stripe 4 placed between two symmetric rectangular windows 5 and 6 obtained from the removal of the multilayer by milling (or drilling and sawing) according to the known techniques.
- the area of the two windows 5 and 6 prevails with respect to the area of the central stripe 4 so that the space of the transition is filled prevalently with air.
- a metallization 7 encircles, as a frame, the two symmetric windows 5 and 6 and the central stripe 4, leaving a short passage free for the microstrip 2, but having a finger 7a covering the stripe 4 for a short tract opposite to the patch 3.
- Several metallized thorough holes 8 are regularly spaced along the perimeter of the frame 7. The only purpose of these holes is that of avoiding possible detachments of the upper dielectric layer from the metal core (plate) as a consequence of the milling operation for opening the windows 5 and 6, because of the not perfect physical compatibility at the interface between the two layers.
- a partial top view of the mechanical part 9 of the transceiver is depicted.
- the mechanic is manufactured in a way to include the end of a rectangular waveguide 10.
- the internal cavity 11 of the metallic waveguide10 is filled up with air.
- Two rectangular grooves 12 and 13 are milled for all the thickness of the two longer walls at the extremity of the waveguide 10, along the symmetry axis.
- Four threaded holes 14 are visible at the four corners of the mechanical part 9.
- the dimensions of the two windows 5 and 6 and the width of the stripe 4 are set to accommodate at the same time the stripe 4 into the grooves 12 and 13 at the edge of the waveguide 10 and the edge of the waveguide 10 inside the windows 5 and 6, as far as the depth of the grooves 12 and 13 allows it.
- Fig.4c and fig.4d show the metal core before and after removal, respectively.
- An indication of the real placement of the internal cross-section 11 of the waveguide 10 is added with dashed line in fig.4d . It can be appreciated that the stripe 4 is free from metal in correspondence of the cavity of the microwave 10, so that the tract of the patched microstrip 2, 3 penetrating the cavity 11 is free to radiate as a probe inside the waveguide 10.
- Fig.5a shows a top view of the assembly constituted by the multilayer of fig.4a superimposed to the mechanic of fig.4b so as they can interpenetrate.
- Two axes A-A and B-B are indicated in the figure as reference planes for the cross-sections reported in the successive figure.
- Fig.5b shows the cross-section along the longitudinal symmetry axis A-A of fig.5a .
- the edge of the waveguide 10 emerges from the openings 5 and 6 and a metallic lid 16 is leant on it.
- the lid 16 is fastened to the waveguide 10 by means of screws 17 penetrating the four threaded holes 14 ( fig.4b ).
- the lid 16 includes a central hollow 18 shaped as a very short tract of waveguide 10 closed at the end.
- the lid 16 is now connected to the waveguide without any interposed dielectric layer, so that the metallic continuity of the walls of the waveguide 10 is never interrupted across the transition until the lid is reached. In this way the back currents reflected from the lid reach the ground directly and, as a consequence, via-holes around the transition as in fig.2b are unneeded for the reasons stated before.
- Grooves 12 and 13 have different depths, the first one (12) is deeper than second one (13) to also include the copper finger 15a ( fig.4d ).
- the microstrip 2 stops to be a as such only at the end of the groove 12, whose depth is calculated accordingly.
- the depth of both the grooves 12 and 13 shall be calculated to assure a certain free space between the end of the waveguide 10 and the microstrip 2, and considering that a certain tolerance on the width of the grooves 12 and 13 is foreseen for the insertion of the stripe 4 without problems, as visible in fig.5a , the substrate 1 has to be fixed to the mechanic 1.
- the transition has been designed to operate in the range of 55-60 GHz in accordance with the market request for the transceiver apparatuses.
- the mechanic is worked by a numerical control machine so as to obtain a WR15 (1.88 x 3.76 mm) waveguide.
- the planar circuitry is obtained starting form a multilayer including a dielectric substrate 0.1 mm thick glued to a copper metal plate (core) 2 mm thick is used.
- the electromagnetic coupling between the microstrip 2 and the waveguide 10 is obtained by means of a probe laying on the E-plane of the rectangular waveguide 10 and terminating with the small patch 3. This probe has been obtained as continuation of the microstrip 2 inside the cavity 11 of the waveguide 10 after having removed the ground plane below.
- the edge of the waveguide 10 emerges from the multilayer in the zone of the transition, as far as the depth of grooves 12 and 13 allows it, and joins the edge of the lid 16.
- the top wall of lid 16 acts as a short circuit reflecting back the signal toward the patch 3. The latter has to see an open circuit on its plane for the reflected signal in order to keep it matched to the waveguide 10.
- the required impedance transformation is obtained by milling the length of tract 18 in a way that the distance of the plane of the patch 3 from the short circuit plane internal to lid 16 is about ⁇ /4.
- a first design of the 55-60 GHz transition has been performed roughly calculating the dimensions of its relevant parts with the help of two canonical books cited at Ref.[3] and Ref.[4].
- the design has been refined successively by several simulation sessions performed by means of the electromagnetic simulator 3D AgilentTM HFSS operating on the model shown in fig.6a .
- the goal is that to optimize the probe dimensions, inclusive of patch 3, for operating in the desired band maintaining the bandwidth and matching conditions as far as possible unaffected by mechanical and assembly tolerances.
- fig.6a we see the model including the dielectric stripe 4 leant on the edge of the waveguide 10 transversally to its rectangular cavity 11.
- This model also includes the slot comprised between groove 12 and lid 16, containing the relevant tract of microstrip 2.
- the terminal part of the probe with the patch 3 is modelled inside the cavity 11 and represented with greater details in fig.6b .
- fig.6b we see the microstrip 2 and patch 3 shaped as a T .
- the base of the rectangular patch 3 perpendicular to the microstrip 2 has a length c greater than the height b , but this is not a general rule.
- Labels w and h indicate respectively the longer and the shorter dimensions of the rectangular cavity 11, while label a indicates the length of the microstrip 2 (without copper below) inside the cavity 11 from the internal sidewall 12 to the base of the patch 3; i.e.: the length of the line which carries the signal to the patch 3.
- the simulation results have confirmed that the central frequency of the transition depends on the ratio (a+b)/w, while the adaptation level at the input and the output ports depends on the ratio c/b inside the considered bandwidth.
- the greater the ratio (a+b)/w i.e. the patch nearer to the centre of the cavity) the lower is the central frequency fo of the transition.
- the insertion loss parameter S 21 reported in fig.11 is strongly influenced by the central microstrip which interconnect the two transitions.
- the 20 mm length (about 7 ⁇ ) of the microstrip causes losses of about 1.5 dB, as a consequence each transition contributes to the measure with about 1.25 dB.
- Fig.12 shows a top view of a microstrip to circular waveguide transition, without the upper lid, the embodiment of which is directly achievable from the preceding description of the microstrip to rectangular waveguide transition. The same applies for a microstrip to elliptic waveguide transition (not represented in the figure).
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Abstract
Description
- The present invention relates to the field of microwave circuits and apparatuses and more precisely to a microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board. We remind that "microwaves" is a generic term to indicate several frequency ranges for the air propagation from about 1 GHz up to roughly 3 THz, millimetric waves correspond to the EHF range from 30 to 300 GHz (λ = 10 to 1 mm). The embodiment of the present invention is particularly suitable to the EHF range but there are not limitations to the application in other frequency ranges, for example the SHF one from 3 to 30 GHz (λ = 10 to 1 cm). The invention is referred both to a method for manufacturing the transition and the transition itself.
- Nowadays the manufacturers of microwave transceivers are pressed by an increasing demand of apparatuses operating in the range of millimetric waves, e.g. for applications in: high/medium/low capacity radio links, point-to-multipoint networks, satellite communications, etc. Having recourse to mass manufacturing techniques oriented to achieve cost-effective products like the traditional Printed Circuit Boards (PCB) are problematic in this frequency range, due to the increased dielectric losses of the substrates and the inadequacy of the known designs to interface planar circuits with mechanical waveguides.
- Microstrip to waveguide transitions embodied with high-loss dielectric substrates for PCB manufacturing are known in the art. The Applicant of the present invention filed on 30-5-2002 an European patent application indicated as Ref.[1] in the REFERENCES listed at the end of the description. According to Ref.[1] the operating frequency range of the transition was extending until to 35 GHz on fibre reinforced glass (FR4) substrates. The multilayer board made use of a thick copper layer as second layer of the build-up wafer structure to provide mechanical stiffness to the FR4 substrate for the connection of a rectangular waveguide on the bottom face. The copper layer was milled to lay bare the dielectric window of a slot transition and obtain in the meanwhile a sort of flange around it for mounting the waveguide. Disregarding the transition for the moment, the idea of making use of high-loss substrates to obtain reliable and low-cost microwave circuits suitable to the automatic or semiautomatic assembly techniques, already widely used in the manufacturing of the PCBs, had been inherited from a preceding European patent application filed by the same Applicant on 26/07/2001 and presently indicated as Ref.[2]. This second application was describing a chip-on-board (COB) technology which allowed to integrate on the substrate many parts of the transceiver, in particular it was possible to accommodate on the substrate both the surface mounting components and those in-chip (either discrete or MMIC) with the relevant polarisation circuitry, so as the conventional waveguide transition that constituted the radio interface of the transceiver. The frequency of 80 GHz was the theoretical limit depending on the minimum width Wm of the microstrip and the thickness h of the FR4 layer allowed by the technology. Having considered Wm = 200 µm the width of the microstrip, and λ/Wm = 10 as a good design parameter, then in order to obtain 50 Ω value for the characteristic impedance of the microstrip the thickness of the FR4 layer was h = 100 µm. The optimistic value of 80 GHz had been calculated for the only wave propagation along the microstrip without taking into due consideration the effects of microstrip to waveguide transitions. Because the invention that will be disclosed is referred to an alternative embodiment to the transition of Ref.[1] capable to really operate up to 80 GHz, some details of the embodiment at Ref.[1] are needed in order to appreciate the improvements.
Figures 1a, 1b ,2a, 2b , and3 disclose those details. -
Fig.1a shows a metallic layout laid down on the upper face of a dielectric FR4 substrate belonging to a multilayer structure. The layout includes a microstrip which extends along the longitudinal symmetry axis of the substrate and terminates with a metal patch. The microstrip and the remaining circuitry (not visible for simplicity) are encircled by a shielding metallic layout delimiting a rectangular unmetallized window, corresponding to a dielectric window, entered by the patched microstrip. The perimetrical metallization of the dielectric window is shaped as a rectangular frame with four unmetallized circle at the four corners in correspondence of threaded holes through the multilayer structure.Fig.1b shows a thick copper layer glued to the bottom face of the dielectric substrate to form a metal core giving stiffness to the multilayer structure and constituting a ground plane for the upper microstrip. The metal core is milled and completely removed to lay bare the dielectric substrate in correspondence of the dielectric window, so that the patch is visible from the rear due to the semitransparency of the FR4 layer.Fig.2a is a cross-section along the axis A-A offig.1a . The figure shows the structure of the multilayer including three dielectric substrates, and the metal core. The upper and the lower dielectric substrates are metallized wile the interposed one is used as insulator. The end of a rectangular waveguide joins the rectangular window milled in the metal core in correspondence of the dielectric window of the upper substrate, so that the opening in the metal core is a continuation of the waveguide to the dielectric window of the substrate. A metallic lid placed upon the frame of the upper face is fixed to the multilayer structure by means of four screws at the corner of the frame penetrating into the upper dielectric substrate, the metal core (flange) and the walls of the rectangular waveguide. The metallic lid is a hollow body with a rectangular recess faced to the unmetallized window. In operation, the patched end of the microstrip which comes into the dielectric window acts as an electromagnetic probe for radiating into the closed space around it. The dimensions of the patch are calculate so as to transfer the energy from the feeding microstrip to the waveguide efficiently. The screwed metallic lid is used as a reflector to prevent propagation from the patch in the opposite direction to the waveguide. To this aim the recess of metallic lid acts as a back short for the signal. From the above considerations it can be conclude that the probe and the dielectric window in communication with the waveguide constitute a microstrip to waveguide transition that transforms the "quasi-TEM" propagation mode of the microstrip into the TE10 mode of the rectangular waveguide. The electromagnetic properties of the transitions are reciprocal, so that the same structure used by the RF transmitter for conveying inside the waveguide a transmission signal from the microstrip is also used by the receiver for conveying a RF reception signal from the waveguide to the microstrip. -
Fig.2b shows a series of metallized through holes (via-holes visible inFig.2a ) regularly spaced along the frame. These via-holes around the transition zone have been introduced successively the filing of Ref.[1] to the aim of improving the performances of the transition at the higher frequencies (35.5 GHz) of the operating range. This statement is possible because the transition at Ref.[1] and the transition of the present invention are both developed in the laboratories of the same Applicant. The via-holes supply to the lack of continuity of the waveguide through the thickness of the dielectric substrate around the zone of the transition. Thanks to via-holes, the energy is bound inside the parallelepipedal part of the dielectric substrate adjacent to the air cavity of the waveguide, otherwise the propagation through the dielectric substrate outside the zone of the transition would constitute a cause of losses. Furthermore, the via-holes supply the upper lid with ground contacts distributed around the transition, improving the poor contact provided by the screws at the four corners of the frame.Fig.3 is a photography of the layout of the transceiver which depicts the real arrangement of via-holes; as it can be noticed, several rows of metallized holes are needed to a satisfactory operation in the SHF range (not in the EHF). - Despite of the manufacturing simplicity of the transition illustrated in the above figures, any attempts to arrange it to the be used in the EHF range has been concluded with a failure due to unacceptable power loss and distortion introduced by the transition. From the analysis of the main causes of these failures it results that at the millimetric waves:
- 1. Via-holes are not more able to bound the electromagnetic field into the encircled parallelepipedal part of the dielectric substrate. The drawback is due to the fact that diameters and reciprocal distances of the holes are comparable with the used wavelength and can not be further reduced cause unavoidable technological limitations of the via-hole process.
- 2. The thickness of the dielectric substrate is no more completely negligible in comparison with the wavelength of the signal, as a consequence via-holes don't connect to the ground the upper lid efficiently. As a consequence the lid couldn't be considered as a continuation of the waveguide opportunely terminated at the top, and a mismatch between the two sides of the patch may generates unwanted reflections and of spurious resonating modes.
- 3. Losses inside the dielectric part of the transition is excessive due to the poor performances of the semi-valuable substrate.
- The european patent application indicated in Ref.[5] discloses a high-frequency package comprising a dielectric substrate, a high-frequency element that operates in a high-frequency region and is mounted in a cavity formed on said dielectric substrate, and a microstrip line formed on the surface or in an inner portion of said dielectric substrate and electrically connected to said high-frequency element, wherein a signal transmission passage of a waveguide is connected to a linear conducting passage or to a ground layer constituting the microstrip line. In the junction portion of the waveguide, for example, an end of the linear conducting passage is electromagnetically opened, so that the end portion works as a monopole antenna inside the waveguide that is connected.
- The aforementioned high-frequency package has been designed to operate at millimetric waves using costly and rigid substrate materials having a low dielectric constant and small losses (e.g. alumina). Moreover, the complicated structure makes the sealing of the multilayer to the waveguide and the application of an upper closing lid both difficult to obtain. Another difficult arises in correctly terminating the irradiating microstrip inside the waveguide.
- The main object of the present invention is that to overcome the drawbacks of the known art and indicate a microstrip to waveguide transition obtainable on PCBs arranged for operating at the microwaves with good performances in the nearest EHF range (up to 80 GHz)
- The invention achieves said object by providing a method to manufacture a microstrip to waveguide transition, as disclosed in the method claims.
- Other object of the invention is a microstrip to waveguide transition obtained according to the method, as disclosed in the device claims.
- According to the invention, the transition disclosed at Ref.[1] is now completely redesigned in order to remove almost completely the former dielectric diaphragm from the space of the transition. Prevalently air fills up the propagation space of the electromagnetic waves in the new transition; with that the drawback highlighted at
point 3 is overcome. Another fundamental difference from the prior art is that the waveguide now penetrates the dielectric substrate to connect the metallic lid, without breaking the continuity of the metallic walls, except for the two grooves whose effect is completely marginal. In other words, the frame of via-holes is completely unnecessary to confine the electromagnetic field, and also the drawbacks highlighted atpoints - Advantageously, the waveguide part of the transition and the other mechanic part of the transceiver can be obtained by means of numerical control manufacturing techniques starting from a rough metal block. Microstrip to waveguide transitions for rectangular waveguides according to the present invention are the easiest to obtain, but the same approach is applicable to obtain transitions for circular or elliptic waveguides.
- Being all causes of losses and misoperation imputable to the only transition removed, the upper frequency limit due to the microstrip on PCBs technique, for example 80 GHz, is now fully exploitable from the transceiver.
- The features of the present invention which are considered to be novel are set forth with particularity in the appended claims. The invention and its advantages may be understood with reference to the following detailed description of an embodiment thereof taken in conjunction with the accompanying drawings given for purely non-limiting explanatory purposes and wherein:
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figures 1a to 3 , already described, show a microstrip to waveguide transition according to the prior art mentioned at Ref.[1]; -
figures 4a to 4d show some manufacturing steps of the multilayer and the waveguide according to the method of the invention; -
figures 5a to 5d show a top view, a longitudinal, and transversal cross section views of the transition according to the invention; -
figures 6a and 6b show a perspective simulation model and relevant parameters of the transition according to the invention; -
figures 7 and 8 show the S11 and S21 parameters of the simulated model; -
fig. 9a shows a top view of two transition back-to-back used for measures; -
fig. 9b shows a photography of the back-to-back transition offig.9a ; -
figures 10. and 11 show the S11 and S21 parameters really measured at the ends of the back-to-back arrangement offig.9a ; -
fig. 12 shows a top view of a microstrip to circular waveguide transition, without the upper lid. - As a description rule, in the several figures of the drawings like referenced numerals identify like elements. Besides, the various elements represented in the figures are not a scaled reproduction of the original ones. With reference to
fig.4a we see a partial upper face of adielectric substrate 1 belonging to a known multilayer structure presently used to obtain the circuitry of a transceiver operating nearby 60 GHz (EHF range) employing traditional PCB techniques. The multilayer structure is a simpler version of the one disclosed at Ref.[1] limited to include a thindielectric substrate 1, characterized by high dielectric losses in comparison with alumina or Gallium Arsenide substrates traditionally used for EHF applications, made adherent to a thick copper plate giving the needed stiffness to the planar structure. A microstrip to waveguide transition, and vice versa, used to connect both the transmitter and the receiver amplifiers to the same antenna by means of a duplexer, is the only part of the transceiver the present invention is concerned with. Thesubstrate 1 gives support to a metallic layout including among other things amicrostrip 2 placed along the axis of longitudinal symmetry of the figure. Themicrostrip 2 terminates with asmall patch 3 nearby the centre of astripe 4 placed between two symmetricrectangular windows windows central stripe 4 so that the space of the transition is filled prevalently with air. Ametallization 7 encircles, as a frame, the twosymmetric windows central stripe 4, leaving a short passage free for themicrostrip 2, but having afinger 7a covering thestripe 4 for a short tract opposite to thepatch 3. Several metallizedthorough holes 8 are regularly spaced along the perimeter of theframe 7. The only purpose of these holes is that of avoiding possible detachments of the upper dielectric layer from the metal core (plate) as a consequence of the milling operation for opening thewindows - In
fig.4b a partial top view of themechanical part 9 of the transceiver is depicted.
The mechanic is manufactured in a way to include the end of arectangular waveguide 10. Theinternal cavity 11 of the metallic waveguide10 is filled up with air. Tworectangular grooves waveguide 10, along the symmetry axis. Four threadedholes 14 are visible at the four corners of themechanical part 9. The dimensions of the twowindows stripe 4 are set to accommodate at the same time thestripe 4 into thegrooves waveguide 10 and the edge of thewaveguide 10 inside thewindows grooves figures 4c and 4d , before this accommodation takes place part of the metal core must be removed from thestripe 4.Fig.4c and fig.4d show the metal core before and after removal, respectively. An indication of the real placement of theinternal cross-section 11 of thewaveguide 10 is added with dashed line infig.4d . It can be appreciated that thestripe 4 is free from metal in correspondence of the cavity of themicrowave 10, so that the tract of the patchedmicrostrip cavity 11 is free to radiate as a probe inside thewaveguide 10. -
Fig.5a shows a top view of the assembly constituted by the multilayer offig.4a superimposed to the mechanic offig.4b so as they can interpenetrate. Two axes A-A and B-B are indicated in the figure as reference planes for the cross-sections reported in the successive figure.Fig.5b shows the cross-section along the longitudinal symmetry axis A-A offig.5a . With reference tofig.5b , the edge of thewaveguide 10 emerges from theopenings metallic lid 16 is leant on it. Thelid 16 is fastened to thewaveguide 10 by means ofscrews 17 penetrating the four threaded holes 14 (fig.4b ). Thelid 16 includes a central hollow 18 shaped as a very short tract ofwaveguide 10 closed at the end. By comparison with the prior art offig.2a , thelid 16 is now connected to the waveguide without any interposed dielectric layer, so that the metallic continuity of the walls of thewaveguide 10 is never interrupted across the transition until the lid is reached. In this way the back currents reflected from the lid reach the ground directly and, as a consequence, via-holes around the transition as infig.2b are unneeded for the reasons stated before.Grooves copper finger 15a (fig.4d ). The highlighted dissymmetry on the two depths is a consequence of the dissymmetric layout on thestripe 4, which bears a microstrip on the left part wile the right part is bare. More precisely, themicrostrip 2 stops to be a as such only at the end of thegroove 12, whose depth is calculated accordingly. Moreover the depth of both thegrooves waveguide 10 and themicrostrip 2, and considering that a certain tolerance on the width of thegrooves stripe 4 without problems, as visible infig.5a , thesubstrate 1 has to be fixed to themechanic 1. Twoholes 19, visible infig.5a , are part of a number of them drilled in the multilayer and themechanic 9 to align the planar circuit with respect to thewaveguide 10 and fasten them to the mechanic.Figures 5c and 5d show the cross-sections along the transversal symmetry axis B-B and C-C offig.5a , respectively. The observation of these figures further clarifies the arguments already developed in the description of the preceding ones and not additional description is needed. - In the operation, the transition has been designed to operate in the range of 55-60 GHz in accordance with the market request for the transceiver apparatuses. The mechanic is worked by a numerical control machine so as to obtain a WR15 (1.88 x 3.76 mm) waveguide. The planar circuitry is obtained starting form a multilayer including a dielectric substrate 0.1 mm thick glued to a copper metal plate (core) 2 mm thick is used. The selected dielectric substrate is known with its commercial name Roger™ 4350, having losses measured by a tanδ = 0.037 at 10 GHz, as declared by the manufacturer; this value clearly increases in the operating frequency range of the transition. Roger™ is similar to FR4 or "vetronite"™ used to manufacture the transition cited at Ref.[1], to say, a material made of glass fibres impregnated with epoxy resin having tanδ from 0,025 to 0,05. These values of tanδ are typical for PCBs but not immediately for microwave circuits where alumina imposes with a tan δ = 0,0001. The electromagnetic coupling between the
microstrip 2 and thewaveguide 10 is obtained by means of a probe laying on the E-plane of therectangular waveguide 10 and terminating with thesmall patch 3. This probe has been obtained as continuation of themicrostrip 2 inside thecavity 11 of thewaveguide 10 after having removed the ground plane below. The edge of thewaveguide 10 emerges from the multilayer in the zone of the transition, as far as the depth ofgrooves lid 16. The top wall oflid 16 acts as a short circuit reflecting back the signal toward thepatch 3. The latter has to see an open circuit on its plane for the reflected signal in order to keep it matched to thewaveguide 10. The required impedance transformation is obtained by milling the length oftract 18 in a way that the distance of the plane of thepatch 3 from the short circuit plane internal tolid 16 is about λ/4. To complete the analysis of the transition, the effect of two slots delimited bylid 16 and eithergrooves - A first design of the 55-60 GHz transition has been performed roughly calculating the dimensions of its relevant parts with the help of two canonical books cited at Ref.[3] and Ref.[4]. The design has been refined successively by several simulation sessions performed by means of the
electromagnetic simulator 3D Agilent™ HFSS operating on the model shown infig.6a . The goal is that to optimize the probe dimensions, inclusive ofpatch 3, for operating in the desired band maintaining the bandwidth and matching conditions as far as possible unaffected by mechanical and assembly tolerances. With reference tofig.6a , we see the model including thedielectric stripe 4 leant on the edge of thewaveguide 10 transversally to itsrectangular cavity 11. This model also includes the slot comprised betweengroove 12 andlid 16, containing the relevant tract ofmicrostrip 2. The terminal part of the probe with thepatch 3 is modelled inside thecavity 11 and represented with greater details infig.6b . With reference tofig.6b , we see themicrostrip 2 andpatch 3 shaped as a T. The base of therectangular patch 3 perpendicular to themicrostrip 2 has a length c greater than the height b, but this is not a general rule. Labels w and h indicate respectively the longer and the shorter dimensions of therectangular cavity 11, while label a indicates the length of the microstrip 2 (without copper below) inside thecavity 11 from theinternal sidewall 12 to the base of thepatch 3; i.e.: the length of the line which carries the signal to thepatch 3. The simulation is carried out considering a WR15 (1.88 x 3.76 mm) waveguide; with that: h = 0.5w. The simulation results have confirmed that the central frequency of the transition depends on the ratio (a+b)/w, while the adaptation level at the input and the output ports depends on the ratio c/b inside the considered bandwidth. Generally speaking, the greater the ratio (a+b)/w (i.e. the patch nearer to the centre of the cavity) the lower is the central frequency fo of the transition. Besides, once w (3.76 mm) is selected in accordance with standard design rules for rectangular waveguides operating in the proximity of the desired central frequency fo (58 GHz), and (a+b)/w is set to obtain the exact fo, then b (and hence a) and c are optimized in the desired frequency band independently of the exact fo previously set. For the operating band of 55-60 GHz, the values of (a+b)/w = 0,18 and c/b = 2.22 are found to be optimal. The results of simulations are reported infigures 7 and 8 which concern the scattering parameters S11 and S21 versus frequency, respectively. With reference tofig.7 , we see that the reflection coefficient S11 never falls below 20 dB in the considered band, while infig.8 the maximum insertion loss S21 is about 0.1 dB. - In order to check the soundness of simulations and the actual performances of the transition, a prototype with two transitions connected back-to-back by a central microstrip has been realized, as the one depicted in
fig.9a photographed infig.9b . The left part offig.9a is a mirror image of the transition offig.5a . The adaptation at one input port of the double structure is measured after having closed the other port on a matched load, therefore the measure concerns the whole matching of the two transitions. The measured scattering parameters S11 and S21 versus frequency are reported infigures 10 and 11 , respectively. With reference tofig.10 , we see that the reflection coefficient S11 is never worse than 10 dB in the considered band. The insertion loss parameter S21 reported infig.11 is strongly influenced by the central microstrip which interconnect the two transitions. In fact, the 20 mm length (about 7λ) of the microstrip causes losses of about 1.5 dB, as a consequence each transition contributes to the measure with about 1.25 dB. -
Fig.12 shows a top view of a microstrip to circular waveguide transition, without the upper lid, the embodiment of which is directly achievable from the preceding description of the microstrip to rectangular waveguide transition. The same applies for a microstrip to elliptic waveguide transition (not represented in the figure). -
- [1]
EP 02425349.4 1367668 ) - [2]
EP 01830497.2 1280392 ). - [3] "Microwave Filters, Impedance-Matching Networks, and Coupling Structures"; G.L.Matthaei, L. Yong and E. M. T. Jones; Artech House Books; 1980.
- [4] "Foundation for Microwave Engineering"; R. E. Collin; McGraw-Hill 2nd Edition; © 1992.
- [5]
EP 0874415 A2 , title: "HIGH-FREQUENCY PACKAGE". Applicant: KYOCERA CORPORATION. (Published on 28/10/1998).
Claims (16)
- Method to manufacture a microstrip to waveguide transition, wherein the transition comprises:- a multilayer structure comprising at least a dielectric substrate (1) of the type usable in the technology of printed circuits boards;- the multilayer substrate is provided on a rigid metal plate (15);- a metallic layout (2, 3, 7) is supported by the dielectric substrate (1);- wherein the metallic layout (2, 3, 7) includes: a microstrip (2) terminating with a patch (3) acting as a probe for coupling the microstrip (2) to a waveguide (10) through the dielectric substrate (1); and two windows (5, 6) symmetric to a longitudinal axis of the metallic layout (2, 3, 7), separated to each other by a central strip (4) bearing the probe;
the method includes the steps of:- removing the multilayer (1), the rigid metal plate (15) and the metallic layout (2, 3, 7) in correspondence to the two windows (5, 6);- removing the rigid metal plate placed below the strip (4) at least in the region between the windows; milling two rectangular grooves (12, 13) of given depth for all the thickness of two opposite walls at the extremity of the waveguide (10) along the symmetry axis;- the dimensions of the two windows (5,6) and the width of the strip (4) are set to accommodate at the same time the strip (4) into the grooves (12,13) at an edge of the waveguide (10) and said edge of the waveguide (10) inside the windows (5,6), as far as the depth of the grooves (12,13) allows it;- fastening a metallic lid (16) to the edge of the waveguide (10) emerging from the two sides (5, 6) of the strip (4) for reflecting back to the waveguide (10) the power radiated by the probe (3) in the opposite direction. - The method of claim 1, characterized in that the whole area of the two windows (5, 6) at the two side of the stripe (4) prevails with respect to the area of the central stripe (4), so that the space of the transition is filled up prevalently with air.
- The method of claim 1 or 2, characterized in that includes the step of aligning the metallic layout (2, 3, 7) with respect to the waveguide (10) and fastening the multilayer to a metallic support body (9) which has been worked to obtain the waveguide (10).
- The method of any claim from 1 to 3, characterized in that includes the step of removing the rigid metal plate (15) from said stripe (4) at least in correspondence of the cavity (11) of the waveguide (1 0) crossed by the stripe (4).
- The method of claim 4, characterized in that includes the step of milling in the body of said lid (16) a central hollow (18) shaped as a short tract of said waveguide (10) with a depth of about λ/4.
- The method of any claim from 1 to 5, characterized in that before opening said windows (5, 6) in the multilayer (1,15), a drilling and a metallizing step are performed to encircle said windows (5,6) and the stripe (4) with metallized through holes (7,8) to avoid possible detachments between the dielectric layer (1) and the rigid metal plate (15).
- The method of any preceding claim, characterized in that said windows (5, 6) opened in the multilayer (1, 15) have rectangular shape.
- The method of any claim from 1 to 7, characterized in that includes the step of setting the central frequency of the transition by fixing a corresponding value of the ratio (a+b)/w, were: w is the longer cavity dimension of a rectangular waveguide whose shorter dimension holds known ratio with w, a is the length of the line which carries the signal to the patch (3), and b is the base of the patch (3) shaped as a rectangle perpendicular to the microstrip (2).
- The method of claim 8, characterized in that includes the step of optimizing the adaptation at the input and the output ports inside the desired frequency band by fixing the ratio c/b, where c is the height of the rectangular patch inside the considered bandwidth; wherein the desired frequency band spans 55 to 60 GHz; wherein a dielectric layer (1) with relative dielectric constant εr of approximately 3.54 is used and wherein the thickness is about 100 µm, the value of (a+b)/w is about 0,18 and the value of c/b is about 2.22.
- Microwave to waveguide transition manufactured with the method according to any of the claims 1 to 9.
- The transition of claim 10, characterized in that the two opposite grooves (12, 13) have different depths and the deeper one includes the microstrip (2) inclusive of the rigid metal plate (1 5).
- The transition of claim 11, characterized in that the two opposite grooves (12,13) have transversal dimensions such they behave as two under-cut waveguides in the desired frequency range of the transition able to confine the electromagnetic field in the volume of the transition.
- The transition of any claim from 10 to 12, characterized in that said waveguide (10) is rectangular.
- The transition of any claim from 10 to 12, characterized in that said waveguide (10) is circular.
- The transition of any claim from 10 to 12, characterized in that said waveguide (10) is elliptic.
- The transition of any claim from 10 to 15, characterized in that includes a crown of metallized through holes (7, 8) which contains the edge of the waveguide (10) at the two sides of the stripe (4) to avoid possible detachments between the dielectric layer (1) and the rigid metal plate (15).
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE602004024169T DE602004024169D1 (en) | 2004-04-29 | 2004-04-29 | Microstrip waveguide transition for millimeter plate formed in a multilayer circuit board |
EP04425300A EP1592081B1 (en) | 2004-04-29 | 2004-04-29 | Microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board |
ES04425300T ES2334566T3 (en) | 2004-04-29 | 2004-04-29 | TRANSITION FROM MICROCINTA TO WAVE GUIDE FOR MILIMETRIC WAVES INCORPORATED IN A MULTI-PAPER PRINTED CIRCUIT CARD. |
AT04425300T ATE449434T1 (en) | 2004-04-29 | 2004-04-29 | MICRO STRIP CONDUCT WAVE CONDUCT JUNCTION FOR MILLIMETER BOARD FORMED IN A MULTILAYER CIRCUIT BOARD |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP04425300A EP1592081B1 (en) | 2004-04-29 | 2004-04-29 | Microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board |
Publications (2)
Publication Number | Publication Date |
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EP1592081A1 EP1592081A1 (en) | 2005-11-02 |
EP1592081B1 true EP1592081B1 (en) | 2009-11-18 |
Family
ID=34932465
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP04425300A Expired - Lifetime EP1592081B1 (en) | 2004-04-29 | 2004-04-29 | Microstrip to waveguide transition for millimetric waves embodied in a multilayer printed circuit board |
Country Status (4)
Country | Link |
---|---|
EP (1) | EP1592081B1 (en) |
AT (1) | ATE449434T1 (en) |
DE (1) | DE602004024169D1 (en) |
ES (1) | ES2334566T3 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
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RU2557472C1 (en) * | 2014-01-21 | 2015-07-20 | Общество с ограниченной ответственностью "КВЧ-Комплекс" | Waveguide adapter from metal waveguide to dielectric waveguide |
CN112736394A (en) * | 2020-12-22 | 2021-04-30 | 电子科技大学 | H-plane waveguide probe transition structure for terahertz frequency band |
Families Citing this family (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2007054355A1 (en) | 2005-11-14 | 2007-05-18 | Vega Grieshaber Kg | Waveguide junction |
WO2008060047A1 (en) * | 2006-11-17 | 2008-05-22 | Electronics And Telecommunications Research Institute | Apparatus for transitioning millimeter wave between dielectric waveguide and transmission line |
KR100846872B1 (en) | 2006-11-17 | 2008-07-16 | 한국전자통신연구원 | Apparatus for the transition of dielectric waveguide and transmission line in millimeter wave band |
JP4365852B2 (en) | 2006-11-30 | 2009-11-18 | 株式会社日立製作所 | Waveguide structure |
JP4648292B2 (en) * | 2006-11-30 | 2011-03-09 | 日立オートモティブシステムズ株式会社 | Millimeter-wave transceiver and in-vehicle radar using the same |
JP5115026B2 (en) | 2007-03-22 | 2013-01-09 | 日立化成工業株式会社 | Triplate line-waveguide converter |
US8723616B2 (en) | 2009-02-27 | 2014-05-13 | Mitsubishi Electric Corporation | Waveguide-microstrip line converter having connection conductors spaced apart by different distances |
US9496593B2 (en) | 2011-02-21 | 2016-11-15 | Siklu Communication ltd. | Enhancing operation of laminate waveguide structures using an electrically conductive fence |
US9270005B2 (en) | 2011-02-21 | 2016-02-23 | Siklu Communication ltd. | Laminate structures having a hole surrounding a probe for propagating millimeter waves |
US10135147B2 (en) | 2016-10-18 | 2018-11-20 | At&T Intellectual Property I, L.P. | Apparatus and methods for launching guided waves via an antenna |
CN112310587B (en) * | 2020-10-27 | 2022-02-01 | 华东光电集成器件研究所 | Waveguide output bearing device |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS592402A (en) * | 1982-06-28 | 1984-01-09 | Hitachi Ltd | Converter of waveguide-microstrip line |
JPH10126114A (en) * | 1996-10-23 | 1998-05-15 | Furukawa Electric Co Ltd:The | Feeder converter |
DE69835633T2 (en) | 1997-04-25 | 2007-08-23 | Kyocera Corp. | High-frequency assembly |
JP2001177312A (en) * | 1999-12-15 | 2001-06-29 | Hitachi Kokusai Electric Inc | High-frequency connection module |
ATE379958T1 (en) | 2001-07-26 | 2007-12-15 | Siemens Spa Italiana | CIRCUIT BOARD AND CORRESPONDING PRODUCTION PROCESS FOR INSTALLING MICROWAVE CHIPS UP TO 80 GHZ |
EP1367668A1 (en) | 2002-05-30 | 2003-12-03 | Siemens Information and Communication Networks S.p.A. | Broadband microstrip to waveguide transition on a multilayer printed circuit board |
-
2004
- 2004-04-29 ES ES04425300T patent/ES2334566T3/en not_active Expired - Lifetime
- 2004-04-29 AT AT04425300T patent/ATE449434T1/en not_active IP Right Cessation
- 2004-04-29 DE DE602004024169T patent/DE602004024169D1/en not_active Expired - Lifetime
- 2004-04-29 EP EP04425300A patent/EP1592081B1/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2557472C1 (en) * | 2014-01-21 | 2015-07-20 | Общество с ограниченной ответственностью "КВЧ-Комплекс" | Waveguide adapter from metal waveguide to dielectric waveguide |
CN112736394A (en) * | 2020-12-22 | 2021-04-30 | 电子科技大学 | H-plane waveguide probe transition structure for terahertz frequency band |
CN112736394B (en) * | 2020-12-22 | 2021-09-24 | 电子科技大学 | H-plane waveguide probe transition structure for terahertz frequency band |
Also Published As
Publication number | Publication date |
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EP1592081A1 (en) | 2005-11-02 |
ATE449434T1 (en) | 2009-12-15 |
ES2334566T3 (en) | 2010-03-12 |
DE602004024169D1 (en) | 2009-12-31 |
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