The present invention relates to a high-frequency module that transmits, for example, a microwave or millimeter-wave high-frequency signal; and a wiring board for use in the high-frequency module.
Conventionally, a high-frequency module is known in which a wiring board having a line conductor and a waveguide are arranged. Typically, this sort of high-frequency module is provided with a waveguide converter that converts a transmission mode between the line conductor of the wiring board and the waveguide. The waveguide converter is formed in, for example, a plate-shaped wiring board having a line conductor, an antenna pattern, and the like. This sort of wiring board is connected to the waveguide via a brazing filler metal or the like (see Patent Document 1, for example).
However, in the case where the brazing filler metal is peeled away or the like to form a gap in a portion connecting the wiring board and the waveguide, radio waves leak from the gap, which may cause a transmission loss. It is conceivable to apply methods for reducing the gap as much as possible by screwing the wiring board and the waveguide or by providing an additional member such as a gasket between the wiring board and the waveguide, but these methods are problematic, for example, in that the size of the high-frequency module increases and the number of manufacturing steps increases. Thus, there is a demand for a high-frequency module that is as small as possible and that can be easily produced.
Patent Document 1: Japanese Unexamined Patent Publication JP-A 8-139504 (1996)
According to an aspect of the invention, a high-frequency module comprises a wiring board; and a waveguide that is connected to the wiring board. The wiring board includes a dielectric substrate, a line conductor that is formed on a first surface of the dielectric substrate, and a first grounding conductor layer that is formed on a second surface opposed to the first surface of the dielectric substrate, and that has a first opening and a second opening disposed around the first opening. The waveguide is connected to the second surface, and has an opening opposed to the first opening. The waveguide is electromagnetically coupled to the line conductor. The wiring board has a vertical choke portion that at least partially extends from the second opening in a direction perpendicular to the second surface. A horizontal choke portion is formed between the wiring board and the waveguide, along the second surface between the opening of the waveguide and the second opening.
According to an aspect of the invention, a wiring board comprises a dielectric substrate, a line conductor that is formed on a first surface of the dielectric substrate, a first grounding conductor layer that is formed on a second surface opposed to the first surface of the dielectric substrate, and a vertical choke portion that is formed in the dielectric substrate. The first grounding conductor layer has a first opening and a second opening disposed around the first opening. The vertical choke portion extends from the second opening in a direction perpendicular to the second surface.
With the high-frequency module according to the aspect of the invention, a high-frequency module that is small and that can be easily produced can be realized.
With the wiring board according to the aspect of the invention, a high-frequency module that is small and that can be easily produced can be realized using that wiring board.
a) is a see-through view of a high-frequency module according to Embodiment 1 of the invention from a lower face thereof, and
a) is a see-through view of another high-frequency module according to Embodiment 1 of the invention from a lower face thereof, and
a) is a see-through view of a high-frequency module according to Embodiment 2 of the invention from a lower face thereof, and
a) is a see-through view of another high-frequency module according to Embodiment 2 of the invention from a lower face thereof, and
a) is a graph showing frequency characteristics S21 of conventional high-frequency modules having no choke structure, and
a) is a see-through view of a high-frequency module according to Embodiment 4 of the invention from a lower face thereof, and
a) is a see-through view of another high-frequency module according to Embodiment 4 of the invention from an upper face thereof, and
Now referring to the accompanying drawings, embodiments of the invention are described in detail below.
As shown in
Here, the first opening 14 is in the shape of a quadrilateral slit having longer sides perpendicular to the line conductor 12A. The shape and size of the slit are determined such that a signal is efficiently transmitted via the first opening 14 between the waveguide 20 and the line conductor 12A.
The waveguide 20 is connected to the lower face of the wiring board 10 such that an opening thereof is opposed to the first opening 14 of the first grounding conductor layer 13. The wiring board 10 has an internal grounding conductor layer 15 in the shape of a ring having an opening inside the dielectric substrate 11. Here, the edge of the opening of the waveguide 20 substantially matches the edge of the first opening 14 of the first grounding conductor layer 13.
Furthermore, the high-frequency module 1A has a choke structure 30. The choke structure 30 has a vertical choke portion 31 and a horizontal choke portion 32. Here, the first grounding conductor layer 13 has a second opening 33 around the first opening 14. The vertical choke portion 31 is formed in the wiring board 10, and extends from the second opening 33 in a direction perpendicular to the lower face of the dielectric substrate 11. The vertical choke portion 31 is formed so as to be surrounded by a plurality of first via-conductors 34, a plurality of second via-conductors 35, and the internal grounding conductor layer 15. Here, the plurality of first via-conductors 34 are arranged along the inner periphery of the second opening 33, and connect the first grounding conductor layer 13 and the internal grounding conductor layer 15. The plurality of second via-conductors 35 are arranged along the outer periphery of the second opening 33, and connect the first grounding conductor layer 13 and the internal grounding conductor layer 15.
The horizontal choke portion 32 is disposed between the wiring board 10 and the waveguide 20 in the case where a gap G is formed between the wiring board 10 and the waveguide 20 along the lower face of the dielectric substrate 11 from the opening of the waveguide 20 to the second opening 33, and is formed along the lower face of the wiring board 10 between the outer peripheral edge of the first opening 14 of the first grounding conductor layer 13 and the inner peripheral edge of the second opening 33. As indicated by the broken line in
In this sort of the high-frequency module 1A, a distance L between the outer peripheral edge of the first opening 14 of the first grounding conductor layer 13 and the inner peripheral edge of the second opening 33 in an extension direction X of the line conductor 12A is substantially ¼ the effective wavelength of a high-frequency signal transmitted through the line conductor 12A. Furthermore, a distance H between the first grounding conductor layer 13 and the internal grounding conductor layer 15 is substantially ¼ the effective wavelength of a high-frequency signal transmitted through the line conductor 12A. Here, “effective wavelength” is a wavelength obtained in consideration of a dielectric constant of space through which a high-frequency signal is transmitted. For example, in the case where a high-frequency signal is transmitted through the dielectric substrate 11, the wavelength is shorter than in a vacuum due to the influence of the dielectric constant of the dielectric substrate 11.
When the distances L and H are set in this manner, the electric field strength near the edge of the opening of the waveguide 20 and at the upper end of the vertical choke portion 31 is 0. Furthermore, a point at which the electric field strength is highest is present on the boundary between the vertical choke portion 31 and the horizontal choke portion 32. Accordingly, a resonance occurs in which the gap near the edge of the opening of the waveguide 20 is electromagnetically blocked, and leakage of a high-frequency signal can be suppressed.
Furthermore, in the case where the distance L is set as described above and a width W of the second opening 33 is substantially ¼ to substantially ½ the effective wavelength of a high-frequency signal transmitted, the gap between the first via-conductors 34 and the second via-conductors 35 is wide, and, thus, the electric field generated in the vertical choke portion 31 is smaller than the electric field generated in the horizontal choke portion 32. The reason for this is that, based on the relationship (Electric field)=(Voltage)/(Distance), the electric field is reduced as the distance increases. Accordingly, even at a frequency where ¼ of the effective wavelength does not match the length of the horizontal choke portion 32 and the length of the vertical choke portion 31, the electric field strength near the edge of the opening of the waveguide 20 and at the upper end of the vertical choke portion 31 is 0, and a point at which the electric field strength is highest is present on the boundary between the vertical choke portion 31 and the horizontal choke portion 32. As a result, a resonance occurs in which the gap near the edge of the opening of the waveguide 20 is electromagnetically blocked, and leakage of a high-frequency signal can be suppressed.
Furthermore, in the case where the width W of the second opening 33 is set to be more than 0 and not greater than ½ the effective wavelength of a high-frequency signal transmitted, leakage of a high-frequency signal can be effectively suppressed. That is to say, in the case where the gap between the first via-conductors 33 and the second via-conductors 34 is set to be smaller than ½ the effective wavelength of a high-frequency signal, a vertical electric field in the vertical choke portion 31 can be suppressed, and, as a result, leakage of a high-frequency signal can be suppressed.
With the high-frequency module 1A according to this embodiment, the vertical choke portion 31 is disposed in the dielectric substrate 11, and, thus, the size of the choke structure 30 can be reduced by a wavelength shortening effect. Furthermore, the vertical choke portion 31 can be formed in the dielectric substrate 11 during production of the dielectric substrate 11, and, thus, an increase in the number of steps due to addition of the choke structure 30 can be suppressed.
In the high-frequency module 1A shown in
In a high-frequency module 1B shown in
The vertical choke portion 31 is formed so as to be surrounded by the first via-conductors 34, the second via-conductors 35, and the same plane grounding conductor layer 41. The first via-conductors 34 are arranged along the inner periphery of the second opening 33, and connect the first grounding conductor layer 13 and the same plane grounding conductor layer 41. The second via-conductors 35 are arranged along the outer periphery of the second opening 33, and connect the first grounding conductor layer 13 and the same plane grounding conductor layer 41.
Furthermore, the distance L between the outer peripheral edge of the first opening 14 of the first grounding conductor layer 13 and the inner peripheral edge of the second opening 33 in an extension direction X of the line conductor 12B is substantially ¼ the effective wavelength of a high-frequency signal transmitted through the line conductor 12B. Furthermore, the distance H between the first grounding conductor layer 13 and the same plane grounding conductor layer 41 is substantially ¼ the effective wavelength of a high-frequency signal transmitted through the line conductor 12B.
Here, in
In the high-frequency module 1B, the line conductor 12B, together with the same plane grounding conductor layer 41 and the first grounding conductor layer 13, constitutes a grounded coplanar line. The slots 42 have longer sides in a direction perpendicular to the line conductor 12B. The length of the longer sides is, for example, substantially ½ the effective wavelength of a high-frequency signal transmitted. Furthermore, the length of the shorter sides is determined so as to obtain an optimal impedance that forms electromagnetic coupling via the first opening 14. In the description above, an example is shown in which the front end of the line conductor 12B is short-circuited by the same plane grounding conductor layer 41, but the front end of the line conductor 12B also may be formed as an open end.
The high-frequency module 1B shown in
In both of the two high-frequency modules 1A and 1B, parts for generating or controlling high-frequency waves, such as an RF-IC, a transmitter, an amplifier, or the like, can be mounted on the dielectric substrate 11.
As shown in
Here, in
In the high-frequency module 1C according to Embodiment 2, reflected waves are present that are emitted from the slots 42, that are reflected at the boundary between the dielectric substrate 11 and the waveguide 20, that are again reflected by the internal grounding conductor layer 44, and that return to the boundary between the dielectric substrate 11 and the waveguide 20. Here, in the case where the distance H between the internal grounding conductor layer 44 and the waveguide 20 is substantially ¼ the effective wavelength of a high-frequency signal transmitted to the high-frequency line Ln, a path difference between the above-described reflected waves and direct waves directly transmitted from the slots 42 to the boundary between the dielectric substrate 11 and the waveguide 20 is substantially ½ the effective wavelength of the high-frequency signal, and the phase of the high-frequency signal is reversed when the reflected waves are reflected by the internal grounding conductor layer 44. Thus, such high-frequency signals are intensified each other, and the high-frequency signals transmitted through the wiring board 10 are efficiently transmitted to the waveguide 20.
That is to say, the dielectric substrate 11 that is interposed between the internal grounding conductor layer 44 and the waveguide 20 and that has a thickness set to substantially ¼ the effective wavelength of a high-frequency signal functions as an impedance matching box between the slots 42 and the waveguide 20 having mutually different impedances.
Furthermore, the side face direction of the dielectric substrate 11 is shielded by the first and the second shield conductor portions 43 and 46, and, thus, leakage of a high-frequency signal emitted from the slots 42 to the dielectric substrate 11 and a high-frequency signal reflected at the boundary between the dielectric substrate 11 and the waveguide 20 is suppressed, and a decrease in the conversion efficiency is suppressed.
Furthermore, the vertical choke portion 31 is disposed in the dielectric substrate 11, and, thus, the size of the choke structure 30 can be reduced by a wavelength shortening effect. Furthermore, the choke structure 30 can be formed in the dielectric substrate 11 during production of the dielectric substrate 11, and, thus, an increase in the number of steps due to addition of the choke structure 30 can be suppressed.
Furthermore, the length H of the vertical choke portion 31 formed in the dielectric substrate 11 is substantially ¼ the effective wavelength of a high-frequency signal, and is the same as the distance H between the internal grounding conductor layer 44 and the waveguide 20. Thus, it is not necessary for the thickness of the dielectric substrate 11 to be increased for addition of the choke structure, and a high-frequency module having a thin choke structure can be realized.
Furthermore, in the high-frequency module 1C according to Embodiment 2, it is preferable that, on a face passing through the center of the first opening 14 and perpendicular to the longitudinal direction of the first opening 14 (a cross-section taken along line C-C), the distance L between the edge of the first opening 14 and the inner peripheral edge of the second opening 33 is substantially ¼ the wavelength of a high-frequency signal transmitted, and that the width W of the second opening 33 is substantially ¼ to substantially ½ the effective wavelength of a high-frequency signal transmitted. In other words, it is preferable that, when seen through from above, the distance L between the edge of the first opening 14 and the inner peripheral edge of the second opening 33 in the line direction of the line conductor 12B (the longitudinal direction of the line conductor 12B in the shape of a straight line) is substantially ¼ the effective wavelength of a high-frequency signal transmitted, and that the width W of the second opening 33 is substantially ¼ to substantially ½ the effective wavelength of a high-frequency signal transmitted.
When the distances L and W are set in this manner, the electric field strength near the edge of the opening of the waveguide 20 and at the upper end of the vertical choke portion 31 is 0, and a point at which the electric field strength is highest is present on the boundary between the vertical choke portion 31 and the horizontal choke portion 32. Accordingly, a resonance occurs in which the gap near the edge of the opening of the waveguide 20 is electromagnetically blocked, and leakage of a high-frequency signal can be suppressed.
Furthermore, when the distances L and W are set as described above, the gap between the first via-conductors 34 and the second via-conductors 35 is wide, and, thus, the electric field generated in the vertical choke portion 31 is smaller than the electric field generated in the horizontal choke portion 32, as seen from the relationship (Electric field)=(Voltage)/(Distance) indicating that the electric field is reduced as the distance increases. Accordingly, even at a frequency where substantially ¼ of the effective wavelength of a high-frequency signal does not match the length of the horizontal choke portion 32 and the length of the vertical choke portion 31, the electric field strength near the edge of the opening of the waveguide 20 and at the upper end of the vertical choke portion 31 is 0, and a point at which the electric field strength is highest is present on the boundary between the vertical choke portion 31 and the horizontal choke portion 32. As a result, a resonance occurs in which the gap near the edge of the opening of the waveguide 20 is electromagnetically blocked, and leakage of a high-frequency signal can be suppressed.
Here, in the case where the width W of the second opening 33 is set to be more than 0 and not greater than ½ the effective wavelength of a high-frequency signal transmitted, leakage of a high-frequency signal can be effectively suppressed. That is to say, in the case where the gap between the first via-conductors 34 and the second via-conductors 35 is set to be smaller than ½ the effective wavelength of a high-frequency signal, a vertical electric field in the vertical choke portion 31 can be suppressed, and, as a result, leakage of a high-frequency signal can be suppressed.
Here, as shown in
Next, the characteristics of the high-frequency module 1C according to Embodiment 2 will be described. Whether or not the function of a high-frequency module can be obtained can be investigated based on transmission characteristics S21 between the high-frequency line Ln and the waveguide 20. This value is required to be as high as possible in order to transmit a high-frequency signal from the high-frequency line Ln to the waveguide 20 at a high conversion efficiency. Here, A of
As shown in
Next, C of
As indicated by C of
However, since the dielectric constant of the dielectric substrate 11 of the vertical choke portion 31 is different from the dielectric constant of air present in a gap formed between the dielectric substrate 11 and the waveguide 20, a high-frequency signal is reflected at the boundary between the dielectric substrate 11 of the choke structure 30 and the air, the effect of suppressing leakage of a high-frequency signal is reduced, and the frequency band of a high-frequency signal in which leakage of a high-frequency signal can be suppressed is narrowed by 3.1 GHz or more.
On the other hand, as indicated by D of
The reason for this is that the gap between the first via-conductors 34 and the second via-conductors 35 is as wide as 0.68 mm, and, thus, the electric field generated in the vertical choke portion 31 is smaller than the electric field generated in the horizontal choke portion 32, as seen from the relationship (Electric field)=(Voltage)/(Distance) indicating that the electric field is reduced as the distance W increases. Accordingly, even at a frequency where ¼ of the effective wavelength of a high-frequency signal does not match the length L of the horizontal choke portion 32 and the length H of the vertical choke portion 31, the electric field strength near the edge of the opening of the waveguide 20 and at the upper end of the vertical choke portion 31 is 0, a point at which the electric field strength is highest is present on the boundary between the vertical choke portion 31 and the horizontal choke portion 32, and, as a result, a resonance occurs in which the gap near the edge of the opening of the waveguide 20 is electromagnetically blocked, and leakage of a high-frequency signal can be suppressed. As a result, the frequency band of a high-frequency signal in which leakage of a high-frequency signal can be suppressed can be made wider.
Here, in the case where the width W of the second opening 33 is set to be more than 0 and not greater than ½ the effective wavelength of a high-frequency signal transmitted, leakage of a high-frequency signal can be effectively suppressed. That is to say, in the case where the gap between the first via-conductors 34 and the second via-conductors 35 is set to be smaller than ½ the effective wavelength of a high-frequency signal, a vertical electric field in the vertical choke portion 31 can be suppressed, and, as a result, leakage of a high-frequency signal can be suppressed.
As described above, the high-frequency module according to Embodiment 2 can realize broadband characteristics in which S21 is −0.5 dB or more over a frequency range of 12.6 GHz. Accordingly, the high-frequency module according to Embodiment 2 of the invention has excellent characteristics around a frequency band used for a vehicle-mounted collision-preventing radar (76 GHz band), and, thus, can be sufficiently applied as a high-frequency module for a vehicle-mounted collision-preventing radar.
As shown in
According to the high-frequency module 1E according to Embodiment 3, even in the case where an unwanted resonance occurs at a frequency corresponding to the length of the second openings 33 when the high-frequency module 1E is viewed from above, the length of the second openings 33 can be easily adjusted, and, thus, the frequency of such an unwanted resonance occurring at the vertical choke portion 33 can be more easily set to a frequency that does not affect transmission of a high-frequency signal.
A high-frequency module 1F shown in
The high-frequency module 1F according to this embodiment has internal grounding conductor layers 44 and 51 that are formed inside the dielectric substrate 11. The internal grounding conductor layer 44 has the opening 45 that is opposed to the first opening 14 and an opening 52 that is opposed to the second opening 33. Furthermore, the internal grounding conductor layer 51 is disposed between the internal grounding conductor layer 44 and the same plane grounding conductor layer 41, and has an opening 53 that is opposed to the first opening 14 and the opening 45. Here, the opening 53 disposed in the internal grounding conductor layer 51 functions as a transmission opening.
The wiring board 10 has the plurality of first via-conductors 34 that are arranged along the inner periphery of the second opening 33 and that connect the first grounding conductor layer 13 and the internal grounding conductor layer 44, and the plurality of second via-conductors 35 that are arranged along the outer periphery of the second opening 33 and that connect the first grounding conductor layer 13 and the internal grounding conductor layer 44. Furthermore, the wiring board 10 has a plurality of third via-conductors 54 that are arranged along the inner periphery of the opening 52 and that connect the internal grounding conductor layer 44 and the internal grounding conductor layer 51, and a plurality of fourth via-conductors 55 that are arranged along the outer periphery of the opening 52 and that connect the internal grounding conductor layer 44 and the internal grounding conductor layer 51.
Further provided are a plurality of fifth via-conductors 56 that surround the opening 53 and the opening 45 and that connect the internal grounding conductor layer 44 and the internal grounding conductor layer 51 along the edges of the opening 53 and the opening 45, and a plurality of sixth via-conductors 57 that are formed around the first opening 14 and that connect the first grounding conductor layer 13 and the internal grounding conductor layer 44.
Here, the second via-conductors 35 and the fourth via-conductors 55 are arranged vertically and electrically connected via the internal grounding conductor layer 44. Furthermore, in the direction in which the line conductor 12B extends, the third via-conductors 54 is positioned farther away from the opening 52 than the first via-conductors 34.
The vertical choke portion 31 is formed so as to be surrounded by the first via-conductors 34, the second via-conductors 35, the third via-conductors 54, the fourth via-conductors 55, and the internal grounding conductor layer 51. The vertical choke portion 31 has a cross-section in the shape of an inverted L.
In the high-frequency module 1F shown in
Furthermore, in the case where the length of the vertical choke portion, that is, the distance from the portion P connecting the first waveguide portion 31A and the horizontal choke portion 32 to a point Q farthest from the portion P on the wall face of the terminal end of the second waveguide portion 31B is substantially ¼ the effective wavelength λ of a high-frequency signal transmitted, in other words, in the case where the length of a path that extends along the wall face of the first waveguide portion 31A closer to the wall of the waveguide, and then diagonally passes through the second waveguide portion 31B from the point connecting the first waveguide portion 31A and the second waveguide portion 31B, to the point Q on the wall face of the terminal end of the second waveguide portion 31B, which is farthest from the connecting point (the sum of a height Hb of the first waveguide portion 31A and a length of a broken line R diagonally passing through the second waveguide portion 31B) is substantially λ/4, the voltage is highest at the portion P connecting the horizontal choke portion 32 and the vertical choke portion 31, the current is highest at the wall face of the terminal end of the second waveguide portion 31B, and the choke effect can be obtained.
Here, in
In the case where the vertical choke portion 31 includes the first waveguide portion 31A and the second waveguide portion 31B in this manner, the height of the wiring board can be lower than that of the vertical choke portion 31 in the shape of a straight line, and a high-frequency module with a reduced height can be realized.
Furthermore, in the case where the distance L is substantially λ/4, and the width Wb of the second opening 33 is substantially λ/4 to substantially λ/2, and in the case where the width Wb of the second opening 33 is set to be more than 0 and not greater than λ/2, an effect as in Embodiment 1 can be obtained.
Furthermore, as shown in
Here, in
Examples of a dielectric material for forming the dielectric substrate 11 include a ceramic material mainly containing aluminum oxide, aluminum nitride, silicon nitride, mullite, or the like, a glass, a glass ceramic material formed by firing a mixture of glass and ceramic fillers, an organic resin-based material such as epoxy resin, polyimide resin, and fluorine-based resin (typically, tetrafluoroethylene resin), and an organic resin-ceramic (also including glass) composite material.
Examples of a material for forming conductor portions in the wiring board 10, such as the line conductors 12A and 12B, the same plane grounding conductor layer 41, the internal grounding conductor layers 44 and 51, the first grounding conductor layer 13, the first and the second shield conductors 43 and 46, and the first to the sixth via-conductor portions 34, 35, and 54 to 57, include a metallization material mainly containing tungsten, molybdenum, gold, silver, copper, or the like, and a metal foil mainly containing gold, silver, copper, aluminum, or the like.
In particular, in the case where the waveguide converter is contained in the wiring board 10 on which a high-frequency part is mounted, it is desirable that the dielectric substrate 11 is made of a dielectric material that has a small dielectric loss tangent and that can realize a hermetic seal. Examples of a particularly desirable dielectric material include at least one inorganic material selected from the group consisting of aluminum oxide, aluminum nitride, and glass ceramic material. It is preferable that the dielectric substrate 11 is made of such a hard material, because the dielectric loss tangent is small and the mounted high-frequency part can be hermetically sealed, which improves the reliability of the mounted high-frequency part. In this case, it is desirable that, as the conductor material, a metallization conductor that can be fired at the same time as the dielectric material is used, in view of hermetic seal properties and productivity.
The above-described wiring board 10 is produced as follows. For example, in the case where an aluminum oxide-based sintered body is used as the dielectric material, first, an appropriate organic solvent or another solvent is added to and mixed with a material powder of aluminum oxide, silicon oxide, magnesium oxide, calcium oxide, or the like to form a slurry, this slurry is shaped into sheets using a conventionally well known doctor blade method or calender roll method, and, thus, ceramic green sheets are produced. Furthermore, an appropriate organic solvent or another solvent is added to and mixed with a material powder of a high-melting-point metal such as tungsten or molybdenum, and, thus, a metallization paste is produced.
Next, the ceramic green sheets are processed using a processing method or the like, and, thus, through-holes for forming through conductors as the first and the second shield conductor portions 43 and 46, and the first to the sixth via-conductor portions 34, 35, and 54 to 57 are formed. Next, using a printing method or the like, the formed through-holes are filled with the metallization paste, and the metallization paste is printed in the shape of the line conductors 12A and 12B, the same plane grounding conductor layer 41, the internal grounding conductor layers 44 and 51, and the first grounding conductor layer 13. In the case where the dielectric substrate 11 has a layered structure including a plurality of dielectric layers, ceramic green sheets in which these conductors are embedded and printed are layered, pressure-bonded through application of a pressure, and fired at a high temperature (approximately 1600° C.). Furthermore, the conductors exposed on the surface, such as the line conductors 12A and 12B, the same plane grounding conductor layer 41, the first grounding conductor layer 13, or the like may be surface-treated so as to be nickel plated and gold plated.
The through conductors forming the first and the second shield conductor portions 43 and 46, and the first to the sixth via-conductor portions 34, 35, and 54 to 57 may be so-called via-conductors in which the through-holes are filled with a conductor, or may be so-called through-hole conductors in which a conductor layer is attached to the inner wall of the through-holes. Furthermore, the shield conductor portions 46, and the second and the fourth via-conductor portions 35 are 55 may be side-face conductors formed on the side face of the dielectric substrate 11, or castellation conductors.
Here, in the above-described example of the high-frequency modules 1B to 1F, the high-frequency line 1 has a coplanar line configuration, but may have a grounded coplanar line configuration in which another dielectric layer is layered on the dielectric substrate 11, and an upper-face grounding conductor layer is disposed on the upper face of this dielectric layer so as to cover the line conductor 12B. Also in this case, an effect as in the high-frequency modules 1B to 1F can be obtained by providing the dielectric substrate 11 with a choke structure.
There is no particular limitation on the shape of the waveguide 20. For example, when a WR series standardized as a square waveguide is used, a variety of calibration kits for measurement can be used, and, thus, various characteristics can be easily evaluated, but a square waveguide can be also used that is made smaller within the range in which cut-off of the waveguide is not generated, in order to reduce the size and weight of the system according to the frequency of a high-frequency signal used. Furthermore, a circular waveguide also can be used.
The waveguide 20 is preferably made of a metal, and the inner wall of the waveguide is preferably coated with a noble metal such as gold, silver, or the like in order to reduce a conductor loss or to prevent corrosion due to current. Furthermore, the waveguide 20 may be formed by shaping a resin into a desired waveguide shape, and the inner wall of the waveguide may be coated with a noble metal such as gold, silver, or the like as in the case of a metal. The waveguide 20 may be attached to the high-frequency line-waveguide converter by fixing using a conductive brazing filler metal, by screwing, or the like.
Here, the invention is not limited to the examples of the foregoing embodiments, and various changes are possible within the range not departing from the gist of the invention.
Number | Date | Country | Kind |
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2007-252428 | Sep 2007 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2008/067688 | 9/29/2008 | WO | 00 | 3/29/2010 |