This application is based upon and claims the benefit of priority of the prior Japanese Patent Application No. 2009-205388, filed on Sep. 5, 2009, the entire contents of which are incorporated herein by reference.
The embodiments described herein relate to a signal converter and a method of manufacturing the same.
Consider a high frequency signal, particularly one in a short wavelength frequency band, such as an extremely high frequency (EHF) wave. When such a signal is to be emitted from or received by an antenna using a transmitter circuit or a receiver circuit, the signal is converted from the transmitter circuit signal format, which is used between the transmitter circuit and the antenna as well as between the receiver circuit and the antenna, to a hollow waveguide signal propagation mode. Alternatively, the signal may be converted from the hollow waveguide signal propagation mode to the receiver circuit signal format. A signal converter is used for such signal conversion.
There exist several proposed structures for coupling a circuit chip or similar device that constitutes the transmitter circuit and receiver circuit with a waveguide. For example, the structure proposed in Japanese Laid-open Patent Publication No. 2003-289201 is provided with a first resonator that connects to a hollow waveguide, and a second resonator that couples with the first resonator. In such a structure, the end of a post-wall waveguide at the first resonator is closed by an array of through conductors, and a coupling window for connecting with the hollow waveguide is provided. The first and second resonators are formed by narrowing the H-plane of the post-wall waveguide at a predetermined interval.
As another example, in the structure proposed in Japanese Laid-open Patent Publication No. 2000-244212, a shorting metal layer is provided on one face of a dielectric substrate, while on the other face there is provided a grounding metal layer in the same shape as the aperture cross-section of a hollow waveguide. Electric potentials are kept equal by the grounding metal layer, the shorting metal layer, and metal embedding the waveguide in the dielectric substrate. In this case, a matching element is installed on the front face of the dielectric substrate enclosed by the grounding metal.
As another example, in the structure proposed in Japanese Laid-open Patent Publication No. 2008-131513, a first ground layer is provided on one face of a dielectric substrate, while a second ground layer is provided on the other face. A hollow waveguide is provided on the side of the first ground layer, and a patch is provided in a notch of the first ground layer.
As another example, in the structure proposed in Japanese Laid-open Patent Publication No. 2006-295891, first and second dielectric substrates are provided, with an hollow coupling conductor for a coplanar strip transmission line installed on the first dielectric substrate, and with a ground conductor installed on the second dielectric substrate.
According to an aspect of the present invention, a signal converter configured to convert a signal between a substrate unit and a hollow waveguide includes a substrate unit, including a first conductor layer formed on one face of a dielectric substrate, and a second conductor layer formed on another face of the dielectric substrate, a plurality of conduction units that penetrate the dielectric substrate and provide conduction between the first conductor layer and the second conductor layer, an waveguide formed by the dielectric substrate, the first and second conductor layers, and the conduction units, and a conversion unit that converts the signal between the waveguide and the hollow waveguide, the conversion unit including a conductor patch having a separator region between itself and the first conductor layer, with the conductor patch being disposed on the substrate unit within an aperture of the hollow waveguide.
The object and advantages of the present invention will be realized and attained by at least the elements, features, and combinations particularly pointed out in the claims.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are not restrictive of the present invention, as claimed.
In the figures, like reference labels refer to like features unless otherwise noted, and dimensions and/or proportions may be exaggerated for clarity of illustration. It will also be understood that when an element is referred to as being “connected to” another element, it may be directly connected or indirectly connected, i.e., intervening elements may also be present. Further, it will be understood that when an element is referred to as being “between” two elements, it may be the only element layer between the two elements, or one or more intervening elements may also be present.
In a structure provided with a plurality of conduction units that constitute a short wall and a coupling window that couples with the hollow waveguide (such as in JP-A-2003-289201 described above), the conduction units are provided with through-holes formed by a laser, drill, or other mechanism. Conductive material is loaded into and formed within such through-holes. The part of the conductor layer that corresponds to the coupling window is formed by cutting out a portion of the conductor layer by etching, for example.
However, due to fabrication inconsistencies, it is difficult to keep the distance that should be kept between the conduction unit array and the coupling window at the desired value. This affects the signal conversion characteristics. In other words, if variation is induced in the distance between the coupling window and the through conductor array, large fluctuations are produced in reflection characteristics for high-frequency signal frequencies. Depending on the frequencies used, waveguide propagation characteristics may also change significantly. In order to improve such characteristics, it is desirable to reduce the frequency dependence of the reflection characteristics.
In addition, depending on the coupling relationship between the hollow waveguide and the part of the substrate constituting the waveguide, higher-order modes or resonances may be produced. Such higher-order modes affect the fundamental resonance mode, and become a factor causing decreases in the signal conversion efficiency in the fundamental resonance mode.
Consequently, one object of the signal converter and manufacturing method disclosed herein is to suppress the effects of fabrication inconsistencies, and improve signal conversion characteristics.
In addition, another object of the signal converter and manufacturing method disclosed herein is to suppress higher-order modes and resonances, and raise the signal conversion efficiency.
In order to achieve the above objects, the signal converter or its manufacturing method disclosed herein involves a signal converter configured to convert a signal between a substrate unit and a hollow waveguide. In the signal converter, a conversion unit is provided on the substrate unit where upon an waveguide is formed. A separator region is provided between the conversion unit and a conductor layer on the substrate unit. A conductor patch is also provided, and disposed on the substrate unit within an aperture of the hollow waveguide. By providing such a configuration, the above objects are achieved.
Thus, in order to achieve the above objects, the signal converter disclosed herein is a signal converter configured to convert a signal between a substrate unit and a hollow waveguide, and is provided with: a substrate unit, a plurality of conduction units, an waveguide, and a conversion unit. In the substrate unit, a first conductor layer is formed on one face of a dielectric substrate, and a second conductor layer is formed on another face of the dielectric substrate. The plurality of conduction units penetrate the dielectric substrate and provide conduction between the first conductor layer and the second conductor layer. The waveguide is formed by the dielectric substrate, the first and second conductor layers, and the conduction units. The conversion unit converts the signal between the hollow waveguide and the waveguide, and is provided with a conductor patch having a separator region between itself and the first conductor layer, with the conductor patch being disposed on the substrate unit within the aperture of the hollow waveguide.
In addition, in order to achieve the above objects, the method of manufacturing a signal converter disclosed herein includes the steps of forming a substrate unit, and joining the substrate unit with a hollow waveguide. In the substrate unit forming step, a substrate unit is formed wherein a first conductor layer is provided on one face of a dielectric substrate, a second conductor layer is provided on another face of the dielectric substrate, and a plurality of conduction units are provided that penetrate the dielectric substrate and provide conduction between the first conductor layer and the second conductor layer. On this substrate unit, there is provided an waveguide formed by the dielectric material portion of the dielectric substrate, and substantially surrounded by the first and second conductor layers as well as the conduction units. A conductor patch is also provided at a conversion unit formed in the waveguide, and a separator region is formed between the conductor patch and the first conductor layer. Subsequently, in the joining step, the substrate unit is joined with a hollow waveguide.
According to the signal converter disclosed herein, advantages like the following are obtained.
(1) Since signal conversion is conducted with a conductor patch installed at the junction between the substrate and the hollow waveguide, the frequency dependence of the signal conversion characteristics is reduced, the effects of fabrication layout errors is alleviated, and signal conversion characteristics can be improved.
(2) Signal conversion characteristics due to fabrication errors at sites that lead signals to the hollow waveguide can be improved.
(3) The production of higher-order modes or resonances can be suppressed, the effects of higher-order modes on the fundamental resonance mode can be reduced, and the signal conversion efficiency in the fundamental resonance mode can be raised.
In addition, according to the method of manufacturing a signal converter disclosed herein, advantages like the following are obtained.
(1) A signal converter with improved signal conversion characteristics can be manufactured.
(2) Degradation in the signal conversion characteristics of a signal converter due to fabrication errors can be reduced.
Other objects, features, and advantages of the present invention will become more apparent upon consulting the respective embodiments and attached drawings.
The first embodiment is provided with a conductor patch pattern in a signal conversion unit between the substrate and the hollow waveguide. The conductor patch pattern is separated from the conductor layer, and provided in the aperture region of the conductor layer. The signal conversion unit is actually referred to as a line-hollow waveguide converter.
The first embodiment will be described with reference to
As illustrated in
The waveguide 8 is provided with a conversion unit 10 between itself and the hollow waveguide 4. The conversion unit 10 is a signal converting mechanism that converts signals from the waveguide 8 of the waveguide substrate 6 to the hollow waveguide 4 (as indicated by the arrow S1), or alternatively, from the hollow waveguide 4 to the waveguide 8 of the waveguide substrate 6 (as indicated by the arrow S2).
The signal converter 2 will now be described with reference to
As illustrated in
The waveguide substrate 6 is one example of a substrate that constitutes the waveguide 8 described earlier. A dielectric substrate 20 is used for the waveguide substrate 6. A first conductor layer 22 is formed on a first face of the dielectric substrate 20 (such as the front, for example) together to form a dielectric waveguide, while a second conductor layer 24 is formed on its second face (such as the back, for example). The dielectric substrate 20 is one example of a dielectric plate. A dielectric resin, for example, may be used as the dielectric material. However, the dielectric material is not limited to resins, and may also be a material such as ceramic.
Along the lengthwise edges of the waveguide substrate 6, there are disposed first and second conduction through-hole arrays 26 and 28 (as shown, e.g., in
The hollow waveguide 4 is disposed on the top face of the first conductor layer 22 on the waveguide substrate 6. The aperture surface 18 of the hollow waveguide 4 contacts the first conductor layer 22, with the hollow waveguide 4 and the waveguide substrate 6 being joined together. Thus, the conversion unit 10 described earlier is provided on the waveguide substrate 6 at the junction with the hollow waveguide 4.
The conversion unit 10 is provided with a conductor patch 32, and a blocking conduction through-hole array 34 (as shown, e.g., in
The blocking conduction through-hole array 34 (as shown, e.g., in
Consequently, as illustrated in
The length and width of the conductor patch 32, the spacing of the separator region 36, and the distance between the conductor patch 32 and the blocking conduction through-hole array 34 will now be described with reference to
As illustrated in
The junction length of the junction gap formed by the separator region 36 is taken to be L2. This length L2 is the length in the direction of travel along the waveguide 8. This junction length L2 is set so as to be smaller than the thickness L3 of the dielectric substrate 20 (see
In this case, a distance L4 is set from the edge of the conductor patch 32 and extending in the direction of signal travel. The blocking conduction through-hole array 34 is disposed such that a spacing equal to the distance L4 exists between the conductor patch 32 and the blocking conduction through-hole array 34. This distance L4 may be set to a value equal to, or essentially in the vicinity of, an odd multiple of one-fourth the wavelength λ (i.e., λ/4) of a signal propagated by the waveguide substrate 6.
The width of the waveguide 8 is taken to be L5. In order to prevent or at least reduce the production of higher-order modes, the width L5 may be set according to the following Eq. 1.
L5<λ0/√{square root over ((∈γ))} (1)
More preferably, the width L5 may be set according to the following Eq. 2.
Herein, ∈r is the relative permittivity of the dielectric substrate 20, and λ0 is equal to c/f, where c is the speed of light, and f is the frequency. Herein, the guide wavelength λg is expressed in Eq. 3.
If the width L5 of the waveguide 8 is increased, then the guide wavelength λg becomes shorter. In contrast, if the width L5 is decreased, then the guide wavelength λg becomes longer. In Eq. 3, a is the width of the waveguide 8, and is equal to L5.
In addition, the frequency of the signals converted in the hollow waveguide 4 need to be of a particular frequency band for the system. Consequently, when creating the converter, for example, the converter may be designed to take more than the needed relative bandwidth. One technique for widening the frequency band involves increasing the thickness L3 of the dielectric substrate 20 (see
At this point, consider the thickness L3 of a given dielectric substrate 20. Air exists within the hollow portion 14 of the hollow waveguide 4. The relative permittivity ∈r of this air is equal to 1, while the relative permittivity ∈r of the dielectric substrate 20 is greater than 1. Ordinarily, the relative permittivity ∈r of the resin used as the dielectric material for the dielectric substrate 20 is approximately 3 to 4. Thus, the width L5 of the waveguide 8 should be set narrower than the aperture width L6 (i.e., the long-edge width) of the hollow hollow waveguide 4 (L6>L5).
The spacing L7 between adjacent conduction through-hole units 30 in the conduction through-hole arrays 26 and 28 should be narrow enough so that signals from the waveguide 8 do not leak out. Preferably, the spacing L7 should be significantly smaller than one-fourth the wavelength λ (i.e., λ/4), with a value not more than one-eighth the wavelength λ (i.e., λ/8) being desirable.
The through-hole units 30 will now be described with reference to
As illustrated in
The blocking conduction through-hole array 34 may be similarly made up of blocking conduction through-hole units 38 that penetrate the dielectric substrate 20 and connect the conductor layers 22 and 24 together. In this case, the blocking conduction through-hole units 38 may also be formed by punching or drilling through-holes 40 in the dielectric substrate 20, and then forming a conductor layer 42 on the inner walls of the through-holes 40. Consequently, in each blocking conduction through-hole unit 38, a through-hole 44 is similarly formed in the space enclosed by the conductor layer 42.
A method of manufacturing such a signal converter will now be described with reference to
This manufacturing process is one example of the manufacturing method disclosed herein, and as illustrated in
In the hollow waveguide 4 forming step (step S11), the hollow waveguide 4 described earlier may be formed. As illustrated in
In the waveguide substrate 6 forming step (step S12), the waveguide substrate 6 described earlier may be formed. In the waveguide substrate 6, the conductor layer 22 may be formed on the front surface of the dielectric substrate 20, while the conductor layer 24 may be formed on its back surface. The respective conductor layers 22 and 24 may be formed by a coating method wherein a conductor layer made up of a metal conductor is applied by techniques such as plating or vapor deposition. Alternatively, the respective conductor layers 22 and 24 may be formed by foil pressing (using copper foil, for example). The through-hole units 30 and 38 may be formed by punching the dielectric substrate 20, the conductor layer 22, and the conductor layer 24. The conductor layer 42 may then be disposed inside each of the respective through-hole units 30 and 38. In so doing, the conduction through-hole arrays 26 and 28, as well as the blocking conduction through-hole array 34, are formed. In the waveguide substrate 6 and the conductor layer 22 where the hollow waveguide 4 is disposed, the separator region 36 and the conductor patch 32 may be formed to constitute the conversion unit 10.
In the hollow waveguide 4 and waveguide substrate 6 joining step (step S13), the hollow waveguide 4 is disposed such that the conductor patch 32 on top of the waveguide substrate 6 described earlier fits into the aperture of the hollow waveguide 4 (or in other words, inside the hollow portion 14). In so doing, the signal converter 2 described earlier is obtained.
Modifications and features of the signal converter 2 in accordance with the first embodiment described above are given below.
(1) In the signal converter 2, there is provided a dielectric substrate 20, in addition to conductor layers 22 and 24 as well as conduction through-hole arrays 26 and 28 formed on either side of the dielectric substrate 20. The portion of the dielectric substrate enclosed by the two conduction through-hole arrays 26 and 28 (i.e., conduction post arrays) as well as the conductor layers 22 and 24 is configured to function as the waveguide 8.
(2) A conversion unit 10 that converts signals is provided in the waveguide 8, with the conversion unit 10 being provided at a position that blocks one end of the waveguide 8. In this conversion unit 10, a conductor patch 32 is provided in an aperture region where the conductor layer 22 is not formed (i.e., in the same planar surface enclosed by the separator region 36). By use of the separator region 36, the conductor patch 32 and the conductor layer 22 are insulated from each other, while also being electromagnetically joined via the separator region 36.
(3) The separator region 36 constitutes a gap such that the conductor patch 32 and the conductor layer 22 do not electrically contact each other. Via this gap, signals in waveguide transmission mode are joined to the conductor patch 32, which acts as a resonator. The resulting frequency characteristics are primarily determined by the size of the conductor patch 32 that acts as a resonator. For this reason, there is reduced dependency on the distance from the conductor layer 22 to the short face of the hollow waveguide 4. As a result, the structure is resilient to the effects of irregularities in the positioning of the conductor patch 32 and the through-holes 40 for the conduction through-hole units 30.
(4) Since the conductor patch 32 is provided, it is possible to improve the signal conversion characteristics of the waveguide 8 constituting the post-wall waveguide, such characteristics being due to fabrication errors at the sites that lead signals to the hollow waveguide 4. In particular, the frequency dependence with respect to the signal conversion characteristics to the hollow waveguide 4 can be improved.
(5) The conductor patch 32 does not contact the conductor layer 22, and is disposed within a planar area equal to the aperture outline of the hollow waveguide 4. The length of this conductor patch 32 in the signal propagation direction may also be set to a value that corresponds to one-half the wavelength λ (i.e., λ/2) of the high-frequency signals to be propagated. In so doing, the signal conversion characteristics can be improved.
(6) The sideways width of the conductor patch 32 is increased with respect to the signal travel direction. For this reason, the spacing between the two conduction through-hole arrays 26 and 28 that constitute the waveguide 8 of the conversion unit 10 can be set wider than the non-waveguide sites in the conversion unit 10. In so doing, the signal conversion characteristics can be improved.
Meanwhile, in some cases, it might be preferable to bring the width of the conductor patch 32 closer to the long-edge width L6 of the hollow waveguide 4, so as to increase the bandwidth. In such cases, the conductor patch 32 might not fit unless the conduction through-hole width L7 (or in other words, the width L5 of the waveguide 8) is increased beyond one-half λ0/∈r1/2 described earlier (see, e.g.,
The second embodiment is configured such that a plurality of conduction through-hole units are provided between the conductor patch 32 and the conductor layer 24 of the first embodiment, with the conductor patch 32 and the conductor layer 24 being connected to each other by the conduction through-hole units.
The second embodiment will be described with reference to
Similarly to the first embodiment, in the signal converter 2 of the present embodiment, the length L8 of the conductor patch 32 in the waveguide mode travel direction (see
According to such a configuration, the conduction through-hole units 46 and 48 are disposed at node positions. For this reason, their effects on the transmission of high-frequency signals is small, higher-order modes can be suppressed, and the fundamental resonance mode can be obtained. In other words, since the conductor patch 32 is shorted along its centerline by the conduction through-hole units 46 and 48, higher-order transmission (i.e., higher-order resonance) between the waveguide 8 (see, e.g.,
In addition, the two conduction through-hole units 46 and 48 in the conductor patch 32 should be spaced apart in the widthwise direction and not in close proximity to each other. The two conduction through-hole units 46 and 48 have an effect equivalent to reducing the width of the waveguide 8, and can increase the higher-order mode suppression effect.
It should also be appreciated that the number of conduction through-hole units 46 and 48 connecting the conductor patch 32 is not limited to one symmetric pair, and that a plurality of such pairs may be disposed, so long as the waveguide width is not made too narrow.
The conduction through-hole units 46 and 48 may be configured similarly to the conduction through-hole units 30, as illustrated in
The third embodiment is configured such that a single conduction through-hole unit is provided between the conductor patch 32 and the conductor layer 24 of the first embodiment, with the conductor patch 32 and the conductor layer 24 being connected to each other by the conduction through-hole unit.
The third embodiment will be described with reference to
In this embodiment, a single conduction through-hole unit 50 connects the conductor patch 32. The conduction through-hole unit 50 is positioned in the center or near-center of the conductor patch 32, so that the center of the conductor patch 32 becomes a node, and higher-order modes are suppressed. In other words, centerlines m and n are set intersecting the center O of the conductor patch 32, and the conduction through-hole unit 50 is set at the intersection point of the centerlines m and n (i.e., at the center O), or at a position in the vicinity of the intersection point (see, e.g.,
By disposing the conduction through-hole unit 50 in the center of the conductor patch 32 in this way, the basic advantages described earlier are obtained. Furthermore, since the center of the conductor patch 32 is shorted to the conductor layer 24 (see, e.g.,
Herein, the conduction through-hole unit 50 may be configured similarly to the conduction through-hole units 30 illustrated in
The fourth embodiment is configured such that a connection unit is provided between the conductor patch 32 and the conductor layer 22.
The fourth embodiment will be described with reference to
As illustrated in
In this way, the connection unit 52 is a mechanism for connecting the conductor patch 32 with the conductor layer 22, and is formed by a conductor extending from the waveguide 8 (see, e.g.,
In addition, since the connection length and connection width is more finite than the surface conductor outside the conductor patch 32, then in consideration of the phase and the impedance, the connection position is slightly shifted away from the true center position of the conductor patch 32 in the travel direction. Hypothetically, if a connection were made at the near antinode, the connection would be affected by the shortness of the connection length and be changed into a connection point node, which would excite undesired higher-order modes. However, in the present embodiment, such inconveniences may be avoided or at least reduced. As a result, higher-order modes can be suppressed, and a structure resilient to misalignments in the positions of the conduction through-hole units 30 and the position of conductor patch 32 is configured without the use of conduction through-hole units that make conductive connections in order to suppress higher-order modes.
With such a configuration, the basic structure in accordance with the first embodiment is used, with the addition of a conductor patch 32 disposed in connection with the connection unit 52 at the edge of the same planar area as the center of the near edge in the travel direction of waveguide modes within the substrate. The characteristic signal conversion structure is achieved. For this reason, the basic advantages of the first embodiment are obtained, while in addition, higher-order transmission (i.e., higher-order resonance) modes between the waveguide within the substrate and the conductor patch 32 can be suppressed.
Moreover, the above structure is configured such that a portion of the conductor patch 32 is removed, and such that the connection point between the conductor patch 32 and the surrounding conductor layer 22 is moved from the periphery and provided farther inward from the edge of the conductor patch 32. With such a structure, higher-order modes can be suppressed without through-holes for constraining higher-order resonance. Since there are no through-hole units in the center part of the conductor patch 32, positioning of that part can be omitted, thereby making it possible to reduce costs.
The fifth embodiment is configured such that the conductor patch 32 and the conductor layer 22 are connected by two connection units provided between the conductor patch 32 and the waveguide 8 in an intersecting direction, such as orthogonally.
The fifth embodiment will be described with reference to
As illustrated in
With such a configuration, a standing wave node can be maintained at the halfway position of the conductor patch 32 in the travel direction. In other words, the fundamental resonance mode can be maintained, and higher-order modes can be suppressed. In addition, the connecting conductor that makes a connection with the conductor patch 32 in order to suppress higher-order modes is formed by a conductor similar to the conductor layer 22. With such a configuration, it becomes possible to suppress higher-order modes even given misalignment in the position of the conductor patch 32 with respect to the positions of the conduction through-hole units 30. As a result, a structure more resilient to positional misalignments of the conductor patch 32 is realized.
The position on the waveguide 8 where the maximum electric field strength occurs is along the widthwise centerline in the widthwise direction with respect to the travel direction of the waveguide 8 (see, e.g.,
The sixth embodiment is a combination of the fourth and the fifth embodiments.
The sixth embodiment will be described with reference to
In the present embodiment, the first connection unit 52 of the fourth embodiment (see
In the present embodiment, the primary resonator is the conductor patch 32, similar to that described in the first embodiment (see
In addition, in the present embodiment, the connection units 52, 54, and 56 that make a connection with the conductor layer 22 are provided on two lateral edges of the conductor patch 32 with respect to the travel direction of waveguide modes within the substrate. For this reason, the conductor layer 22 is connected with the middle regions on the periphery of the conductor patch 32. In this way, by providing short points in the form of the lateral connection units 54 and 56 in addition to the connection unit 52, higher-order transmission (i.e., higher-order resonance) modes between the waveguide 8 and the conductor patch 32 can be suppressed, even if the conductor patch 32 is increased in size.
The seventh embodiment is configured having a plurality of both conduction through-hole arrays as well as blocking conduction through-hole arrays.
The seventh embodiment will be described with reference to
As illustrated in
In this case, the spacing between respective conduction through-hole units 30 or respective blocking conduction through-hole units 38 on individual rows are set substantially identically. In addition, in the spacing portions on each row, another row of conduction through-hole units 30 or blocking conduction through-hole units 38 may be disposed in a staggered configuration. In so doing, advantages are obtained that are equivalent to narrowing the spacing between respective conduction through-hole units 30 or blocking conduction through-hole units 38.
The eighth embodiment is configured such that the through-holes for the conduction through-hole units 30 and the blocking conduction through-hole units 38 are embedded in the conductor layer and configured as through conductors (i.e., conduction posts).
The eighth embodiment will be described with reference to
In this case, the conduction through-hole units 30 are configured as follows. The through-holes 40 are formed penetrating the dielectric substrate 20, and the conductor layer 42 is embedded into the through-holes 40, thereby realizing conduction posts in the form of cylindrical through conductors as a result of the conductor layer 42. Such conduction through-hole units 30 may be used in the conduction through-hole arrays 26 and 28 described earlier (see, e.g.,
In addition, the blocking conduction through-hole units 38 may be similarly configured as follows. The through-holes 40 are formed penetrating the dielectric substrate 20, and the conductor layer 42 is embedded into the through-holes 40, thereby realizing cylindrical through conductors as a result of the conductor layer 42. Besides being cylindrical, the conductor layer 42 may also be a prismoid. Such blocking conduction through-hole units 38 may be used in the blocking conduction through-hole array 34 described earlier (see, e.g.,
The ninth embodiment is configured such that the conduction through-hole arrays 26 and 28 as well as the blocking conduction through-hole array 34 are configured as a conductor wall.
The ninth embodiment will be described with reference to
Since the conduction through-hole arrays 26 and 28 or the blocking conduction through-hole array 34 is a mechanism for realizing a conductor wall, the above arrays are not limited to the conduction through-hole units 30 or the blocking conduction through-hole units 38, and need not be arrays of through-holes. As illustrated in
In the first embodiment, a technique of providing a step portion 33 (see
A comparative example will now be described with reference to
As illustrated in
With such a configuration, a short wall is realized as a result of the blocking conduction through-hole array 134, with the distance L10 from the blocking conduction through-hole array 134 to the coupling window 166 being one-fourth the wavelength (i.e., λ/4) (see, e.g.,
In the fabrication of such a configuration, it is expected that the blocking conduction through-hole array 134 and the coupling window 166 will be formed in separate manufacturing steps. Ordinarily, the blocking conduction through-hole array 134 would be formed by first creating holes by laser or drilling, for example, and then loading conductive material into the holes. Meanwhile, the coupling window 166 would be formed by etching or similar process, wherein a conductive film is formed while leaving a portion corresponding to the coupling window 166.
For this reason, due to fabrication irregularities in each manufacturing step, it is difficult to accurately set the desired value for the distance that should be secured between the blocking conduction through-hole array 134 and the coupling window 166. Taking L to be the distance between the coupling window 166 and the blocking conduction through-hole array 134, consider the case where signal converters 102 are manufactured with three different values for L10: the distances La, Lb, and Lc (where La≠Lb≠Lc). In such as case, the characteristics of signal conversion to the waveguide 104 vary, as illustrated in
As demonstrated by these signal conversion characteristics (see
In contrast with the above comparative example, such inconveniences do not exist in the foregoing embodiments. The distance between the conductor patch 32 and the blocking conduction through-hole array 34 that acts as a short wall is set to an odd multiple of one-fourth the wavelength λ (i.e., λ/4) of the signal propagated along the waveguide substrate 6. As a result, a standing wave is produced. Since a conductor patch 32 is present before the signal reaches the short wall, and since the junction gap formed by the separator region 36 is comparative narrow, direct leakage is small. Instead, the one-half wavelength (λ/2) conductor patch 32 strongly resonates, and the signal to be transmitted can be led to the hollow waveguide 4. The halfway position of the conductor patch 32 in the travel direction of the waveguide 8 corresponds to a node of the standing wave, and the conductor patch 32 induces resonance such that the antinodes of the standing wave are produced at the near and far edges of the conductor patch 32 in the travel direction. Consequently, the primary resonance length becomes the length of the conductor patch 32 in the transmission direction, and the relative influence is lowered for the standing wave produced in the distance (i.e., gap) between the short wall made up of the blocking conduction through-hole array 34, and the edge of the gap on the far side of the conductor patch 32 in the travel direction of the waveguide 8. As a result, the influence exerted by the distance to the short wall on the conversion characteristics is significantly reduced. Thus, in the foregoing embodiments, the precision of the positioning can be mitigated in the two manufacturing steps described in the comparative example, the effects on the conversion characteristics due to the error in the single manufacturing step for pattern formation of the conductor layer 22 and the conductor patch 32 can be reduced, and the conversion characteristics can be improved.
The signal converter or the manufacturing method disclosed herein can be used for a high-frequency wave module having a waveguide connection unit for a frequency band such as that of microwaves and EHF waves. For example, the signal converter and manufacturing method disclosed herein can be broadly utilized in technologies such as EHF wave communication systems and automotive radar transceivers.
All examples and conditional language recited herein are intended for pedagogical purposes to aid the reader in understanding the principles of the present invention and the concepts contributed by the inventor to furthering the art, and are to be construed as being without limitation to such specifically recited examples and conditions, nor does the organization of such examples in the specification relate to a showing of the superiority and inferiority of the present invention. Although the embodiment(s) of the present invention(s) has (have) been described in detail, it should be understood that the various changes, substitutions, and alterations could be made hereto without departing from the spirit and scope of the present invention.
Number | Date | Country | Kind |
---|---|---|---|
2009-205388 | Sep 2009 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
6580335 | Iizuka et al. | Jun 2003 | B1 |
7148765 | Tahara et al. | Dec 2006 | B2 |
7586386 | Takahashi | Sep 2009 | B2 |
20040119554 | Tahara et al. | Jun 2004 | A1 |
20050200424 | Takeda et al. | Sep 2005 | A1 |
20070052504 | Fujita | Mar 2007 | A1 |
20070085626 | Lee et al. | Apr 2007 | A1 |
20070182505 | Fujita et al. | Aug 2007 | A1 |
20080309427 | Kim et al. | Dec 2008 | A1 |
Number | Date | Country |
---|---|---|
2000-244212 | Sep 2000 | JP |
2003-273612 | Sep 2003 | JP |
2003-289201 | Oct 2003 | JP |
2006-295891 | Oct 2006 | JP |
2007-12710 | Jan 2007 | JP |
2008-131513 | Jun 2008 | JP |
Entry |
---|
Japanese Office Action mailed Sep. 10, 2013 for corresponding Japanese Application No. 2009-205388, with Partial English-language Translation. |
Number | Date | Country | |
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20110057743 A1 | Mar 2011 | US |