The present invention relates to a circuit element including a magnetic plate, more particularly to a non-reciprocal circuit device.
A lumped constant non-reciprocal circuit device has long been used as an isolator or circulator in a mobile communication device or mobile communication terminal because it requires less space. An isolator is placed between the power amplifier and antenna in the transmitter of a mobile communication device in order to, for example, prevent unwanted signals from reversely entering the power amplifier from the antenna for a desired frequency band or to stabilize impedance on the load side of the power amplifier; a circulator is used in a transmission/reception branch circuit etc.
As shown in
One end of each of center conductors L1, L2, and L3 projects externally from the rims of ferrite plates F1 and F2 and the projection is connected to a signal input/output port (not shown) and one end of each of matching dielectric board pieces (matching capacitors) C1, C2, and C3. The other end of each of center conductors L1, L2, and L3 and the other end of each of matching dielectric board pieces (matching capacitors) C1, C2, and C3 are grounded electrically. Center conductors L1, L2, and L3 have inductance. When a lumped constant circuit element is used as an isolator, the input/output port of center conductor L3 is connected to one end of a terminator and the other end is grounded electrically to absorb reflected signals.
In a structure as described above, if the matching conditions by matching capacitors, the inductances of the center conductors, and the materials of ferrite plates F1 and F2 are optimized, circulator 100 shows irreversibility in a certain frequency range. That is, circulator 100 has high attenuation characteristics (isolation) for a signal that is input to the input/output port connected to one end of the center conductor L1 and output from the input/output port connected to one end of the center conductor L2, a signal that is input to the input/output port connected to one end of the center conductor L2 and output from the input/output port connected to one end of the center conductor L3, and a signal that is input to the input/output port connected to one end of the center conductor L3 and output from the input/output port connected to one end of center conductor L1; circulator 100 has low attenuation characteristics (or opposite characteristics) for signals that are transmitted in the directions opposite to those. If a terminator R1 is connected to the input/output port of the center conductor L3, the non-reciprocal circuit device functions as an isolator, in the corresponding frequency band, which has high attenuation characteristics for a signal that is input to the input/output port connected to one end of the center conductor L1 and output from the input/output port connected to one end of center conductor L2 and has low attenuation characteristics (or opposite characteristics) for signals that are transmitted in the direction opposite to that.
However, the frequency (operating frequency) bandwidth in which a non-reciprocal circuit device such as a conventional isolator or circulator shows irreversibility is generally narrow. (For example, the frequency bandwidth that gives attenuation with an irreversibility of 20 dB at a center frequency of 2 GHz is several tens of hertz.).
Non-patent literature 1 discloses technology for widening the bandwidth of the operating frequency of an isolator. This known technology achieves a bandwidth ratio of 7.7% at a center frequency of 924 MHz by adding an inductor or capacitor to the input end of an isolator. Non-patent literature 2 discloses an example of increasing the fractional bandwidth to 30 to 60% by adding an inductor or capacitor between a center conductor and the ground. Patent literature 1 discloses technology for widening the bandwidth without increasing insertion loss by providing a capacitor between a ground conductor connected to one end of each of three center conductors and the ground. In the above methods of widening the bandwidth, however, there are limits to the extent to which the bandwidth of operating frequency can be widened due to insertion loss or degradation in isolation characteristics, so it is difficult to use these methods for application in which two frequency bands significantly apart (for example, more than one octave band apart) must be covered.
Patent literature 2 discloses a non-reciprocal circuit device that changes the operating frequency with an RF switch for disconnecting or connecting a capacitor disposed on the input/output port of each center conductor to change the resonance frequency of a resonant circuit. In this structure, however, the operating frequency is toggled with the switch, so concurrent use in a plurality of frequency bands is impossible, thereby disabling its usage in an environment in which a plurality of applications for different frequency bands are implemented concurrently. Patent literature 3 discloses a non-reciprocal circuit device that changes operating frequency bands by changing the reactance of a variable capacitor disposed on mutual connection ends of the three center conductors. Since reactance needs to be changed in this structure, however, it is not applicable to an environment in which a plurality of applications for different frequency bands are implemented concurrently as in the structure in patent literature 2.
Patent literature 4 discloses a structure in which two isolators are placed in series with two ferrite plates for dual-band support using an installation area of the size equivalent to that for a single band isolator. However, application to portable terminals is difficult because the height is increased in this structure.
The present invention addresses the above problems with the object of providing a dual-band-capable non-reciprocal circuit device that can solely obtain irreversibility concurrently in two frequency bands significantly apart even though the circuit element has a size equivalent to that of a single-band-capable lumped constant non-reciprocal circuit device in order to achieve multiband/multimode terminals.
A non-reciprocal circuit device of the present invention comprises a magnetic plate; a plurality of center conductors, each of which has a first end and a second end, the plurality of center conductors being mutually insulated and disposed so as to intersect on the magnetic plate; a plane conductor disposed facing the plurality of center conductors with the magnetic plate placed between the plane conductor and the plurality of center conductors, the plane conductor being connected to the first ends of all of the plurality of center conductors; a plurality of matching capacitors, each of which has a first end and a second end, the first end being grounded electrically, the second end being connected to the second end of corresponding one of the plurality of center conductors; a plurality of first matching circuits, each of which has a first and a second end, the first end being connected to the second end of corresponding one of the plurality of center conductors, the second end being an input/output port; and a second matching circuit having a first end and a second end, the first end being connected to or integrated with the plane conductor, the second end being grounded electrically.
The non-reciprocal circuit device of the present invention can solely obtain irreversibility concurrently in two frequency bands significantly apart even though the circuit element has a size equivalent to that of a single-band-capable lumped constant non-reciprocal circuit device.
Preferred embodiments of the present invention will be described below with reference to the drawings. In the embodiments, the present invention is applied to a lumped constant circulator, which is an exemplary non-reciprocal circuit device, but the invention is not limited to the following embodiments.
A first embodiment of the present invention will be described below.
<Outer Structure>
As shown in
The plane conductor P1 is a disc-shaped conductor integrated with the center conductors L1, L2, and L3; the first ends of the center conductors L1, L2, and L3 are connected to the three points dividing the rim of the plane conductor P1 into three equal parts. The first ends of the center conductors L1, L2, and L3 are mutually short-circuited and each of the second ends has two parallel lines connected to the rim of the plane conductor P1. The disc-shaped ferrite plate F1 is placed on one surface (top surface in
The surface (bottom surface in
Projection ends S1, S2, and S3 (opposite to the ends connected to the plane conductor P1) of the center conductors L1, L2, and L3 project externally from the rim of the ferrite plate F1. The projection ends S1, S2, and S3 are connected to the first ends of the inductors L11, L12, and L13, respectively. Matching dielectric board pieces C1, C2, and C3 are further attached on the surfaces of the projection ends S1, S2, and S3, which face the ground conductor, to form matching capacitors between each of the projection ends S1, S2, and S3 and the ground conductor G. Reference characters C1, C2, and C3 for matching dielectric board pieces are also used below as the reference characters of these matching capacitors. The second ends of the inductors L11, L12, and L13 configure input/output ports SS1, SS2, and SS3, respectively, and are connected to the first ends of the capacitors C11, C12, and C13, respectively. The second ends of the capacitors C11, C12, and C13 are grounded electrically. Pairs of an inductor and a capacitor, (L11, C11), (L12, C12), and (L13, C13), constitute the first matching circuits M11, M12, and M13, respectively.
A chip inductor, a line with a certain length, etc. can be used to implement each of the inductors L11 to L13. A chip capacitor, a varactor such as a PIN diode, etc. can be used or a dielectric having one end grounded can be sandwiched to implement each of the capacitors C11 to C13. A permanent magnet for magnetizing the ferrite plate F1 is actually disposed facing the ferrite plate F1, but the permanent magnet is not shown in the figure.
<Circuit Configuration>
As shown in
In addition, the first ends of the first matching circuits M11, M12, and M13 are connected to the projection ends S1, S2, and S3 of the center conductors L1, L2, and L3, respectively; the second ends of the first matching circuits M11, M12, and M13 constitute input/output ports SS1, SS2, and SS3, respectively. The first matching circuit M11 has a pair of, for example, inductor L11 and capacitor C11 as shown in
<Principle of Operation>
The first frequency band (higher frequency side) of the dual-band is determined mainly by the center conductors L1, L2, and L3, the matching capacitors C1, C2, and C3, and the inductances and capacitances of the first matching circuits M11, M12, and M13. The second frequency band (lower frequency side) of the dual-band is determined mainly by the inductances and capacitances of the first matching circuits M11, M12, and M13 and the inductance and capacitance of the second matching circuit M2. If the capacitances of the matching capacitors C1, C2, and C3 are increased, the interval between the two frequency bands (first frequency band and second frequency band) is reduced. If fine tuning is performed by the first matching circuits M11, M12, and M13 and the second matching circuit M2, high isolation can be achieved with low transmission loss. In addition, if the capacitances of the first matching circuits M11, M12, and M13 are increased and the inductances are reduced, the operating frequency bands can be shifted to the lower side; if the capacitances are reduced and the inductances are increased, the operating frequency bands can be shifted to the higher side. The insertion loss and degradation in isolation characteristics depend on the characteristics (such as the size and saturation magnetization) of the ferrite plate F1 or the external magnetic field strength. The lower limit of the second operating frequency band shifted by adjustment of the inductance or capacitance depends on these characteristics. Accordingly, if the size and properties (characteristics) of the ferrite plate F1 are selected appropriately, the second operating frequency band can be shifted to a lower side. A shift to a lower side is achieved by, for example, increasing the diameter of the ferrite plate, selecting a ferrite with a lower saturation magnetization, or reducing the external magnetization strength.
<Characteristic Data>
Transmission characteristics data will be shown below to clarify the effect of the invention. In the following description, reference characters L1, L2, and L3 for the center conductors also indicate their line lengths, reference characters L11, L12, and L13 for the inductors also indicate their inductances, and reference characters C1, C2, and C3 for the capacitors also indicate their capacitances.
Next, an example of how the transmission characteristics depend on difference in inductances L11 to L13 and capacitances C11 to C13 in first matching circuits M11, M12, and M13.
A comparison of characteristics data in
The first matching circuits with the structure shown in
In addition, the number of combinations of LC resonant circuits is increased, so the number of bands in which irreversibility can be obtained is increased.
The structure including the capacitor C31 shown in
The present invention is not limited to the above three embodiments. For example, the present invention is applied to a lumped constant circulator, which is an exemplary non-reciprocal circuit device, in the above embodiments, but the invention may be applied to a lumped constant isolator. In this case, a terminator R1 is added to input/output port SS3 described in the first embodiment. It will be appreciated that various modifications may be made as appropriate without departing from the scope of the invention.
The non-reciprocal circuit device of the present invention is particularly applicable to an isolator or circulator in wide-band communication devices such as mobile phone terminals for dual-band use.
Number | Date | Country | Kind |
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2008-039118 | Feb 2008 | JP | national |
2008-318725 | Dec 2008 | JP | national |
Number | Name | Date | Kind |
---|---|---|---|
3605040 | Knerr et al. | Sep 1971 | A |
3836874 | Maeda et al. | Sep 1974 | A |
5977845 | Kitahara | Nov 1999 | A |
6020793 | Makino et al. | Feb 2000 | A |
Number | Date | Country |
---|---|---|
2 251 701 | May 1974 | DE |
0 959 520 | Nov 1999 | EP |
1 041 664 | Oct 2000 | EP |
9-93003 | Apr 1997 | JP |
11-234003 | Aug 1999 | JP |
2001-119210 | Apr 2001 | JP |
Number | Date | Country | |
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20090206942 A1 | Aug 2009 | US |