Embodiments herein relate to filters. In particular, they relate to integrated low-pass and band-pass filter unit formed by sheet metal coated with dielectric material.
In the 5th Generation (5G) communication, two types of frequency ranges have been defined, Frequency Range-1, i.e. Sub-6 GHZ, which is less than 6 GHZ, and Frequency Range-2, i.e. millimeter wave, which is above 24 GHz. With the development of the 5G communication, multiple-input and multiple-output (MIMO) technology is widely used in Sub-6 GHz base station product, in which amount of filter unites (FUs) need to be integrated with antenna unit (AU) or radio unit (RU). Considering cost and space saving, FUs are usually soldered onto radio unit mother board, Low-Pass Filter (LPF) board or antenna power splitter board, which means smaller and lighter FUs are quite in demand.
In traditional base station solutions, metal cavity FUs are most recommended because of their high Quality (Q) value and power handling performance. For 5G advanced radio system, the size and weight of FUs become critical issues. Ceramic waveguide (CWG) filters especially CWGs are one of the preferred FU solutions for 5G, due to their high performance, light weight, small size and easy integration. However, there are so many limitations of CWG FU, e.g., the Q value of a CWG filter is lower than a metal cavity filter, the size of a CWG filter needs to be limited to reduce the risk of being cracked when it is soldered onto a board since the ceramic material is easy to break if the size is too big, the high frequency suppression, i.e. the out of band frequency attenuation performance is relatively poor, etc. Due to those limitations, radio products which can use CWG filters are limited.
As a part of developing embodiments herein, problems and limitations with traditional CWG filters and metal FUs will further be discussed.
Traditional metal FUs have good performance and reliability. However, they have big size or volume and higher cost and are not a good solution for MIMO system.
One of the problems of the current CWG filters is bandwidth limitation. While a wideband radio product demands for wideband filters.
The Q value of a CWG filter is lower. To increase the Q value, the size of the cavity must be increased, and this contradicts with the basic design desire of smaller size.
CWG FUs also have limitation factors in production, which cannot be used in complex radio systems. They are also unreliable during long-term radio work progress. A CWG FU is always soldered with a Printed Circuit Board (PCB) LPF to get better out of band attenuation, the LPF will bring much loss and extra coupling from two near paths on the PCB.
Sheet metal FUs have good reliability in production, but they have worser power handling capacity and bigger size compared to CWG FUs. Sheet metal band pass filter (BPF) is usually combined with a sheet metal LPF to get better out of band attenuation, the sheet metal LPF has smaller insertion loss compared with the PCB LPF.
It is therefore an object of embodiments herein to provide a filter unit with improved radio performance, power handling capacity and reliability, and at the same time with reduced size and weight.
According to one aspect, the object is achieved by an integrated low-pass and band-pass filter unit. The integrated low-pass and band-pass filter unit comprises an inner cavity formed by a shell of conductive materials. The integrated low-pass and band-pass filter unit further comprises one or more low-pass resonators and two or more band-pass resonators comprised in the inner cavity. The low-pass and band-pass resonators are integrally formed by electroplated sheet metal material. A part of each of the low-pass and band-pass resonators is coated with dielectric material. The two or more band-pass resonators are arranged at two sides of the inner cavity such that at least two resonators are aligned to face each other.
The integrated low-pass and band-pass filter unit further comprises a first separator of electroplated sheet metal arranged in the inner cavity between the low-pass resonators and band-pass resonators and a second separator of electroplated sheet metal arranged in the inner cavity between the band-pass resonators at the two sides of the inner cavity.
The integrated low-pass and band-pass filter unit further comprises an input port to receive a signal to be filtered and an output port to output a filtered signal.
According to some embodiments herein, the integrated low-pass and band-pass filter unit may further comprise a first coupling structure of the dielectric material. The first coupling structure is arranged between the two resonators facing each other and the first coupling structure may be connected to the dielectric material coated part of the one resonator or to the dielectric material coated parts of both resonators.
In other words, according to the embodiments herein, to solve the contradiction between the high Q-factor and small size of a filter, an integrated low-pass and band-pass filter unit formed by sheet metal coated with dielectric material is provided.
The integrated low-pass and band-pass filter unit according to embodiments herein have some advantages, for examples:
Therefore, embodiments herein provide a filter unit with improved radio performance, power handling capacity and reliability, and at the same time with reduced size and weight.
Examples of embodiments herein are described in more detail with reference to attached drawings in which:
According to embodiments herein, to solve the contradiction between the Q-factor and size of a filter, an integrated low-pass and band-pass filter unit with low-pass and band-pass function formed by sheet metal materials and parts of the sheet metal materials being dielectric material-coated is provided.
The integrated low-pass and band-pass filter unit according to the embodiments herein comprises a main body comprising a low-pass filter comprising one or more low-pass resonators and a band-pass filter comprising two or more band-pass resonators. The low-pass and band-pass resonators are integrally formed by electroplated sheet metal material. To reduce the size of the main body, parts of the metal sheet resonators can be coated with dielectric material.
The flat metal sheet of the low-pass and band-pass filters LP 110, BP 120 is bent to form the main body of the integrated low-pass and band-pass filter unit. For example, the flat metal sheet of the low-pass and band-pass resonators 111, 112, 113, 121, 122, 123, 124, 125, 126 may be bent at the positions 131, 132, 133 shown in
The bending positions may be chosen at other places than what are shown in
For the same Q value, the lower the frequency, the larger the volume of a single cavity of a resonator. The resonant frequency of a resonator is the frequency at which the energy of the stored electric field equals that of the stored magnetic field. The plastic-coated high dielectric material makes the electric field energy and magnetic field energy mostly concentrated near the resonator and equal to the electromagnetic field energy at lower frequencies. Therefore using the dielectric material coated sheet metal resonators can effectively reduce the resonance frequency of the resonator in order to reduce the size of the resonator. As a result, the size of a single cavity of a resonator and in turn, the size of the whole filter unit composed of several single cavities can be reduced.
Since the dielectric constant of the dielectric material, e.g., plastic, is higher than air, a part of the electric field generated by a resonator is constraint within the plastic boundary. Therefore, the maximum electric field intensity of a single cavity containing the resonators is relatively lower, which can significantly improve the power handling capacity of the filter unit.
Materials with the dielectric constant of 1.8˜10 are preferred. In actual use, materials with Dielectric Loss Angle lower than one thousandth are preferred based on the insertion loss characteristics of the filter. Dielectric Loss Angle is the phase difference between the electric field vector and the electric displacement in a dielectric material. This phase difference is caused by energy losses in the dielectric.
The main body 300 is placed in a shell to form a complete filter.
The integrated low-pass and band-pass filter unit 400 according to the embodiments herein comprises the inner cavity 401, one or more low-pass resonators 411, 412, 413 and two or more band-pass resonators 421, 422, . . . 426 comprised in the inner cavity 401. The low-pass and band-pass resonators 411, 412, 413, 421, . . . 426 are integrally formed by electroplated sheet metal material. A part of each of the low-pass and band-pass resonators 411, 412, 413, 421, . . . 426 is coated with dielectric material.
The two or more band-pass resonators 421, . . . 426 are arranged at two sides of the inner cavity 401 such that at least two resonators, e.g. band-pass resonators 422, 425, are aligned to face each other.
The integrated low-pass and band-pass filter unit 400 further comprises a first separator 430 of electroplated sheet metal arranged in the inner cavity 401 between the low-pass resonators 411, 412, 413 and band-pass resonators 421, . . . 426 to separate the spatial between the low-pass resonators 411, 412, 413 and band-pass resonators 421, . . . 426.
The integrated low-pass and band-pass filter unit 400 further comprises a second separator 440 of electroplated sheet metal arranged in the inner cavity 401 between the band-pass resonators at the two sides of the cavity 401 to separate the spatial between the two sides of the band-pass resonators.
The integrated low-pass and band-pass filter unit 400 further comprises an input port 450 to receive a signal to be filtered and an output port 460 to output a filtered signal.
According to embodiments herein, a negative coupling structure may be introduced in the integrated low-pass and band-pass filter unit 400. For example, the upper half of the two plastic-coated resonators facing each other may be filled with plastic to form strong negative coupling.
Therefore, according to some embodiments herein, the integrated low-pass and band-pass filter unit 400 may further comprise a first coupling structure 470 of the dielectric material. The first coupling structure 470 may be arranged between two BP resonators facing each other, e.g. between the BP resonators 422 and 425. The first coupling structure 470 may be connected to the dielectric material coated parts of both resonators, as shown in
The first coupling structure 470 may also be connected only to the dielectric material coated part of one of the two facing BP resonators, e.g. the first coupling structure 470 is only connected to the BP resonator 425, as shown in
The negative coupling occurs at the top of the resonators. Therefore, the first coupling structure 470 is a negative coupling structure. The negative coupling changes with the size and shape of the coupling structure 470. Thus, the negative coupling may be adjusted freely by adjusting the size and/or the shape of the coupling structure 470. The negative coupling may also be adjusted by a loading screw 480 placed at the middle of the coupling structure 470 as shown in
The first coupling structure 470 of the dielectric material is paced at the top of the two resonators facing each other such that a negative coupling between the two resonators is achieved as a result of directions of the electric fields generated by the two resonators being opposite.
When positive coupling occurs between two resonators, the direction of electric field in one single cavity of one resonator will generally be the same as that in another single cavity of another resonator. When the plastic-coated position is at the bottom of the two resonators, the coupling of the resonators will produce positive coupling, and the coupling strength varies with the change of the coupling window.
Therefore, according to some embodiments herein, the integrated low-pass and band-pass filter unit 400 may further comprises a second coupling structure 611. The second coupling structure 611 may be paced at the bottom of two resonators such that a positive coupling between the two resonators is achieved as a result of directions of electric fields generated by the two resonators being the same.
The positive coupling may be achieved by a coupling structure between two resonators facing each other or any two neighbor resonators at the same side of the inner cavity 401. Generally, between the bottom and upper of a resonator, For examples, an open window structure 611, a coupling structure of dielectric material, a direct metal bar connection etc. all are positively couplings.
The integrated low-pass and band-pass filter unit 400 according to the embodiments herein may be employed in various electronic devices or any devices or apparatus where filtering radio frequency signals is needed.
One or more integrated low-pass and band-pass filter units 400 may also form a multiband filter unit and employed in various electronic devices or any devices or apparatus where filtering radio frequency signals is needed.
To summarize, according to the embodiments herein, an integrated low-pass and band-pass filter unit 400 formed by sheet metal coated with dielectric material is provided and has some advantages, for examples:
The word “comprise” or “comprising”, when used herein, shall be interpreted as non-limiting, i.e. meaning “consist at least of”.
The embodiments herein are not limited to the above described preferred embodiments. Various alternatives, modifications and equivalents may be used. Therefore, the above embodiments should not be taken as limiting the scope of the invention, which is defined by the appended claims.
Number | Date | Country | Kind |
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PCT/CN2021/118317 | Sep 2021 | WO | international |
Filing Document | Filing Date | Country | Kind |
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PCT/SE2022/050401 | 4/26/2022 | WO |