The present disclosure relates to the field of communication devices, and in particular to a dielectric filter unit and a dielectric filter.
When electromagnetic waves propagate in materials with high dielectric constants, their wavelengths can be shortened. Utilizing this theory, dielectric materials can be used instead of traditional metallic materials, allowing for a reduction in the volume of filters while maintaining the same performance criteria. Research on dielectric filters has always been a hot topic in the communication industry. As a crucial component of wireless communication products, dielectric filters have particular significance in the miniaturization of communication devices.
Dielectric filters are typically consisting of multiple resonant cavities. The more resonant cavities there are, the higher the filter order, resulting in better suppression performance. However, this often leads to larger filter sizes. Currently, conventional dielectric filters struggle to balance the requirements of size, multiple resonance modes, and suppression performance, among other factors.
The present disclosure aims to solve at least one of the technical problems in the existing art by providing a dielectric filter unit and a dielectric filter.
In accordance with a first aspect of the present disclosure, in an embodiment provided is a dielectric filter unit. The dielectric filter unit includes a first dielectric resonant cavity and a second dielectric resonant cavity.
The first dielectric resonant cavity is provided with a first frequency hole in an upper end face or a lower end face of the first dielectric resonant cavity. The second dielectric resonant cavity is connected to the first dielectric resonant cavity, and provided with a second frequency hole in an upper end face or a lower end face of the second dielectric resonant cavity.
The dielectric filter unit further includes a coupling slot provided at a joint of the first dielectric resonant cavity and the second dielectric resonant cavity, and a third frequency hole provided at the joint of the first dielectric resonant cavity and the second dielectric resonant cavity.
In accordance with a second aspect of the present disclosure, in an embodiment provided is a dielectric filter including two or more dielectric filter units as described in the above embodiment of the first aspect.
Additional features and advantages of the present disclosure will be set forth in the subsequent description, and in part will become apparent from the description, or may be learned by practice of the present disclosure. The purposes and other advantages of the present disclosure can be realized and obtained by structures particularly noted in the description, the claims and the accompanying drawings.
The accompanying drawings are used to provide further understanding of the technical schemes of the present disclosure and constitute a part of the description. The accompanying drawings are used to explain the technical schemes of the present disclosure together with the embodiments of the present disclosure, and do not constitute a restriction on the technical schemes of the present disclosure.
The present disclosure will be further elaborated hereinafter with reference to the accompanying drawings and embodiments.
In this section, some specific embodiments of the present disclosure will be described in detail, and some preferable embodiments of the present disclosure are shown in the accompanying drawings. The accompanying drawings are used to supplement the text description of the specification with graphic illustrations, so that each technical feature and the overall technical scheme of the present disclosure can be intuitively and vividly understood. However, the accompanying drawings should not be construed as limiting the scope of protection application the present disclosure.
In the description of the present disclosure, the meaning of “several” is one or a plurality; the meaning of “a plurality of” is two or more; “greater than”, “less than”, “more than”, etc. are to be construed as excluding a given figure; and “above”, “below”, “within”, etc. are to be construed as including a given figure. If “first” and “second”, etc. are referred to, it is only for the purpose of distinguishing technical features, and shall not be construed as indicating or implying relative importance or implying the number of the indicated technical features or implying the sequence of the indicated technical features.
In the description of the present disclosure, unless otherwise explicitly defined, the terms such as “arrange”, “install”, and “connect” should be construed in a broad sense, and those skilled in the art can determine the specific meanings of the above terms in the present disclosure in a rational way in conjunction with the specific contents of the technical schemes.
When electromagnetic waves propagate in materials with high dielectric constants, their wavelengths can be shortened. Utilizing this theory, dielectric materials can be used instead of traditional metallic materials, allowing for a reduction in the volume of filters while maintaining the same performance criteria. Research on dielectric filters has always been a hot topic in the communication industry. As a crucial component of wireless communication products, dielectric filters have particular significance in the miniaturization of communication devices.
The significance of cross-coupling lies in the fact that electromagnetic waves undergo a phase polarity inversion after passing through different coupling paths, thereby generating infinitesimal notch points, known as transmission zeros, outside the passband of the filter. Therefore, the out-of-band suppression capability of the filter can be improved without increasing the number of resonant cavities.
The out-of-band zeros are generated on both sides or one side at the high and low ends of the working passband of the filter. When the out-of-band zeros are located on both sides of the passband and have different magnitudes, they are at different distances from the center frequency of the passband. The above characteristics require the design to be flexible and adjustable according to specific out-of-band suppression requirements.
Dielectric filters typically consist of multiple resonant cavities. The more resonant cavities there are, the higher the filter order, resulting in better suppression performance. However, this often leads to larger filter sizes. Currently, conventional dielectric filters struggle to balance the requirements of size, multiple resonance modes, and suppression performance, among other factors.
Embodiments of the present disclosure provide dielectric filter units and dielectric filters that can simultaneously achieve small volumes, multiple resonance modes, and the generation of out-of-band transmission zero points.
The embodiments of the present disclosure will be further explained below with reference to the accompanying drawings.
Referring to
The first dielectric resonant cavity 100 is provided with a first frequency hole 110 in an upper end face or a lower end face of the first dielectric resonant cavity 100.
The second dielectric resonant cavity 200 is connected to the first dielectric resonant cavity 100. The second dielectric resonant cavity 200 is provided with a second frequency hole 210 in an upper end face or a lower end face of the second dielectric resonant cavity 200. A coupling slot 300 is provided at a joint of the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200. A third frequency hole 400 is further provided at the joint of the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200.
The dielectric filter unit includes the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200, and the coupling slot 300 is arranged between the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200, such that a certain amount of coupling between the two resonant cavities is enabled. Further, the third frequency hole 400 is arranged at the joint of the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200, and configured to cooperate with the coupling slot 300, thereby enabling a third resonance mode within the dual-cavity structure. This configuration enables the dielectric filter to achieve three transmission modes by using the physical form and volume dimensions of only two cavities, thus achieving the performance of a third-order filter, and also enables generation of out-of-band transmission zeros, providing high adjustability and producibility.
It can be seen that in the embodiment shown in
It should be noted that the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200 may have various shapes, for example, a polygonal shape or an irregular cuboid shape. Both the first dielectric resonant cavity 100 and the second dielectric resonant cavity 200 in this embodiment are designed as rectangular cuboids.
As shown in
The first frequency hole 110 and the second frequency hole 210 are located in the same end face of the dielectric filter unit, for example, both are located in the upper end face or the lower end face of the dielectric filter unit. As in the embodiment shown in
It can be understood that the first frequency hole 110 and the second frequency hole 210 may also be located in different end faces of the dielectric filter unit, i.e., the first frequency hole 110 and the second frequency hole 210 may be respectively located in the upper end face and the lower end face of the dielectric filter unit. For example, referring to
In addition, when the first frequency hole 110 and the second frequency hole 210 are located in different end faces of the dielectric filter unit, the dielectric filter unit may also be provided with a fourth frequency hole. The fourth frequency hole is located in another end face of the first dielectric resonant cavity opposite to the end face in which the first frequency hole is located or in another end face of the second dielectric resonant cavity opposite to the end face in which the second frequency hole is located. In the embodiment shown in
The first frequency hole 110, the second frequency hole 210, and the fourth frequency hole 220 are all blind holes with a cross-sectional shape that may be circular, rectangular, regular polygonal, or irregular polygonal.
It should be noted that the coupling slot 300 is located in a region between the two dielectric resonant cavities, and the coupling slot 300 may be a through slot extending from the upper end face to the lower end face of the dielectric filter unit or a non-through blind slot. In addition, the number of coupling slots 300 in the dielectric filter unit may be only one or more than one. In the embodiment shown in
In addition, the coupling slot 300 may be formed by recessing from a surface of the dielectric filter unit or may be completely embedded in the dielectric filter unit. The embodiment shown in
Referring to
When the number of the coupling slots 300 is more than one, the coupling window 310 refers to the sum of the projection areas of all the coupling slots 300. Furthermore, when there is a non-overlapping area between projection areas of any two coupling slots 300, the coupling window 310 also includes the non-overlapping area between the projections.
It should be noted that the number of the third frequency holes 400 in the dielectric filter unit may be only one as shown in
Referring to
It should be noted that the term “dielectric” in the context of the dielectric filter unit refers to a material with a certain dielectric constant, such as ceramics with a dielectric constant of 20, 40, 60, etc. It can be understood that the dielectric filter unit can be made of either a single material with a specific dielectric constant or a combination of materials with different dielectric constants.
In addition, in an embodiment of a second aspect of the present disclosure provided is a dielectric filter, including two or more dielectric filter units as described in the above embodiments of the first aspect. Now referring to
The transmission zero in a dielectric filter is generated by the superposition of signals with opposite phases from a cross-coupling path of non-adjacent cavities and a main coupling path, which causes the signal to be attenuated at specific frequencies outside the passband, resulting in the creation of a theoretical infinitesimal notch, known as the transmission zero.
Referring to
Referring to
With the dielectric filter unit provided by the embodiments of the present disclosure, the out-of-band suppression performance of the filter is increased by generating a third resonance mode, i.e., adding an additional resonant cavity, without increasing the volume; or the volume is significantly reduced while maintaining the same number of cavities. The dielectric filter unit generates a transmission zero, thereby further improving the out-of-band suppression performance in the filter transmission response. The third resonant mode of the dielectric filter unit can be independently adjustable, and the associated transmission zero is also independently adjustable, making it highly producible. The quality factor Q of the dielectric filter unit is not compromised by the generation of the third resonance mode. The dielectric filter unit is easy to process and form, and allows for lower material cost and lighter weight compared to filters of the same order.
The present disclosure includes the embodiments of dielectric filter units and dielectric filters. According to the schemes provided in the embodiments of the present disclosure, the dielectric filter unit includes a first dielectric resonant cavity and a second dielectric resonant cavity. The coupling slot is arranged between the first dielectric resonant cavity and the second dielectric resonant cavity such that a certain amount of coupling between the two resonant cavities is enabled. In addition, the third frequency hole is arranged at the joint of the first dielectric resonant cavity and the second dielectric resonant cavity, and configured to cooperate with the coupling slot, thereby enabling a third resonance mode within the dual-cavity structure. This configuration enables the dielectric filter to achieve three transmission modes using the physical form and volume dimensions of only two cavities, thus achieving the performance of a third-order filter, and also enables generation of out-of-band transmission zeros, providing high adjustability and producibility. The dielectric filter units and dielectric filters provided can simultaneously achieve small volumes, multiple resonance modes, and the generation of out-of-band transmission zero points.
Although the embodiments of the present disclosure have been described in detail above with reference to the accompanying drawings, the present disclosure is not limited to the above embodiments, and various changes may be made within the knowledge of those of ordinary skill in the art without departing from the purpose of the present disclosure.
| Number | Date | Country | Kind |
|---|---|---|---|
| 202111130983.7 | Sep 2021 | CN | national |
This application is a national stage filing under 35 U.S.C. § 371 of international application number PCT/CN2022/112564, filed Aug. 15, 2022, which claims priority to Chinese patent application No. 202111130983.7, filed Sep. 26, 2021. The contents of these applications are incorporated herein by reference in their entirety.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/CN2022/112564 | 8/15/2022 | WO |