1. Field of the Invention
The present invention relates to two-port isolators, and in particular, to a two-port isolator for use in microwave bands, a characteristic adjusting method therefor, and a communication apparatus including a two-port isolator.
2. Description of the Related Art
In general, two-port isolators allow signals to pass through them only in a transmitting direction and prevent the signals from passing through them in a reverse direction. The two-port isolators are used in transmitting circuit portions of mobile communication apparatuses, such as automobile telephones and cellular phones.
The isolator disclosed in Japanese Unexamined Patent Application Publication No. 2003-46307 is a known two-port isolator of the type described above, that is, a type of isolator including first and second center electrodes.
The two-port isolator 300 has an advantage in that a high attenuation is obtained even outside an operating frequency range because the first and second center electrodes 301 and 302 are perpendicular to each other. In the two-port isolator 300, one end of the first center electrode 301 is used as an input port P1, one end of the second center electrode 302 is used as an output port P2, and the other ends (common end) of the first and second center electrodes 301 and 302 are used as a ground port P3. The two-port isolator 300 has a problem in that, when a signal is conveyed from the input terminal 311 to the output terminal 312, the two resonant circuits resonate to produce a large insertion loss.
Accordingly, to eliminate this problem, a low-loss two-port isolator is disclosed in Japanese Unexamined Patent Application Publication No. 9-232818. As
In the two-port isolator 320, one end of the first center electrode 321 is used as an input port P1, one end of the second center electrode 322 is used as a ground port P3, and the other ends of the first and second center electrodes 321 and 322 are used as an output port P2. In the two-port isolator 320, when a signal is conveyed from the input terminal 331 to the output terminal 332, a resonant circuit (defined by the inductor L1 and the matching capacitor C11) between the input port P1 and the output port P2 does not resonate. Only one resonant circuit (defined by an inductor L2 and matching capacitor C12 connected between the output port P2 and the ground port P3) resonates. Thus, in the two-port isolator 320, an insertion loss is reduced.
In general, an input admittance Y12 of a two-port isolator is normally designed to be 0.02 S+0 j S, and its susceptance part is 0 S. In terms of impedance, an input impedance Z12 of the two-port isolator is normally designed to be 50Ω+0 jΩ. However, in the case of mounting the two-port isolator on an actual circuit board of a mobile communication apparatus, the two-port isolator is affected by a pad capacitor on a surface on which the two-port isolator is mounted, lines connected to other components, circuit elements, etc. Accordingly, in relation to an input terminal of the two-port isolator, the susceptance part of the admittance Y11 is not always 0 S. In many cases, it has a positive value (capacitive) or a negative value (inductive).
In addition, in order to enable maximum power to pass in the two-port isolator by reducing a power loss at an input terminal of the isolator, the input admittance Y12 must be matched so as to be a complex conjugate of the admittance Y11. In other words, the susceptance part of the admittance Y12 must be inductive or capacitive in accordance with the susceptance part of the admittance Y11.
In the two-port isolator 300 shown in
Conversely, in the two-port isolator 320 shown in
To overcome the above-described problems, preferred embodiments of the present invention provide a two-port isolator in which matching of the admittance of a first input/output port is adjusted, a characteristic adjusting method therefor, and a communication apparatus including the two-port isolator.
According to a preferred embodiment of the present invention, a two-port isolator includes a permanent magnet, a ferrite member to which a direct-current magnetic field is applied by the permanent magnet, a first center electrode having one end electrically connected to a first input/output port and the other end electrically connected to a second input/output port, the first center electrode being provided on the ferrite member, a second center electrode having one end electrically connected to the second input/output port and the other end electrically connected to a ground port, the second center electrode being arranged on the ferrite member so as to intersect with the first center electrode, with the first center electrode and the second center electrode being electrically insulated from each other, a first matching capacitor electrically connected between the first input/output port and the second input/output port, a resistor electrically connected between the first input/output port and the second input/output port, a second matching capacitor electrically connected between the second input/output port and the ground port, a first input/output terminal electrically connected to the first input/output port, and a second input/output terminal electrically connected to the second input/output port. One of the first input/output port and the second input/output port defines an input port, and the other one defines an output port, and the intersection angle between the first center electrode and the second center electrode is adjusted to be less than about 90 degrees, and the susceptance part of the admittance of the first input/output port is negative in the pass-band center frequency.
According to another preferred embodiment of the present invention, a two-port isolator includes a permanent magnet, a ferrite member to which a direct-current magnetic field is applied by the permanent magnet, a first center electrode having one end electrically connected to a first input/output port and the other end electrically connected to a second input/output port, the first center electrode being provided on the ferrite member, a second center electrode having one end electrically connected to the second input/output port and the other end electrically connected to a ground port, the second center electrode being arranged on the ferrite member so as to intersect with the first center electrode, with the first center electrode and the second center electrode being electrically insulated from each other, a first matching capacitor electrically connected between the first input/output port and the second input/output port, a resistor electrically connected between the first input/output port and the second input/output port, a second matching capacitor electrically connected between the second input/output port and the ground port, a first input/output terminal electrically connected to the first input/output port, and a second input/output terminal electrically connected to the second input/output port. One of the first input/output port and the second input/output port defines an input port, and the other one defines an output port, and the intersection angle between the first center electrode and the second center electrode is adjusted to be greater than about 90 degrees, and the susceptance part of the admittance of the first input/output port is positive in the pass-band center frequency.
Preferably, the admittance of the first input/output port has a complex conjugate relationship with an external circuit.
The two-port isolator may further include a capacitor electrically connected in series between the first input/output port and the first input/output terminal.
The two-port isolator may further include an inductor electrically connected in series between the first input/output port and the first input/output terminal.
The two-port isolator may further include an inductor having one end electrically connected to the first input/output port and the other end electrically connected to the first input/output terminal, and a capacitor shunt-connected to the other end of the inductor.
The two-port isolator may further include a capacitor electrically connected between the first input/output port and the ground.
According to another preferred embodiment of the present invention, a two-port isolator includes a permanent magnet, a ferrite member to which a direct-current magnetic field is applied by the permanent magnet, a first center electrode having one end electrically connected to a first input/output port and the other end electrically connected to a second input/output port, the first center electrode being provided on the ferrite member, a second center electrode having one end electrically connected to the second input/output port and the other end electrically connected to a ground port, the second center electrode being arranged on the ferrite member so as to intersect with the first center electrode, with the first center electrode and the second center electrode being electrically insulated from each other, a first matching capacitor electrically connected between the first input/output port and the second input/output port, a resistor electrically connected between the first input/output port and the second input/output port, a second matching capacitor electrically connected between the second input/output port and the ground port. One of the first input/output port and the second input/output port defines an input port, and the other one defines an output port, and the intersection angle between the first center electrode and the second center electrode is an angle other than 90 degrees.
According to another preferred embodiment of the present invention, a communication apparatus including a two-port isolator as described above is provided.
According to another preferred embodiment of the present invention, a characteristic adjusting method for a two-port isolator is provided. The two-port isolator includes a permanent magnet, a ferrite member to which a direct-current magnetic field is applied by the permanent magnet, a first center electrode having one end electrically connected to a first input/output port and the other end electrically connected to a second input/output port, the first center electrode being provided on the ferrite member, a second center electrode having one end electrically connected to the second input/output port and the other end electrically connected to a ground port, the second center electrode being arranged on the ferrite member so as to intersect with the first center electrode, with the first center electrode and the second center electrode being electrically insulated from each other, a first matching capacitor electrically connected between the first input/output port and the second input/output port, a resistor electrically connected between the first input/output port and the second input/output port, a second matching capacitor electrically connected between the second input/output port and the ground port, a first input/output terminal electrically connected to the first input/output port, and a second input/output terminal electrically connected to the second input/output port. One of the first input/output port and the second input/output port defines an input port, and the other one defines an output port, and the susceptance part of the admittance of the first input/output port is adjusted by changing the intersection angle between the first center electrode and the second center electrode.
According to preferred embodiments of the present invention, by adjusting the intersection angle between the first and second center electrodes to be less than about 90 degrees, the susceptance part of the admittance of the first input/output port is set to be negative in the band-pass center frequency. Alternatively, by adjusting the intersection angle between the first and second center electrodes to be greater than about 90 degrees, the susceptance part of the admittance of the first input/output port is set to be positive in the band-pass center frequency. This easily enables the admittance of the first input/output port to have a complex conjugate relationship with an external circuit. Therefore, adjustment of the admittance of the first input/output port is facilitated. As a result, a two-port isolator in which matching of the admittance of a first input/output port is adjusted, and a communication apparatus including the two-port isolator are obtained.
These and various other features, elements, steps, characteristics and advantages of the present invention will become more apparent from the following detailed description of preferred embodiments thereof with reference to the attached drawings.
Two-port isolators, a characteristic adjusting method therefor, and a communication apparatus according to preferred embodiments of the present invention are described below with reference to the accompanying drawings.
The lower metal case portion 8 includes right and left side walls 8b and 8a. The lower metal case portion 8 is integrally molded with the resin case 3 preferably by insertion molding. A bottom wall 8b of the lower metal case portion 8 has a pair of opposite sides. From one side, two ground terminals 16 extend (two ground terminals from the other side are not shown). For providing a magnetic circuit, the upper metal case portion 4 and the lower metal case portion 8 are preferably made of ferromagnetic material, such as soft iron, and their surfaces are plated with Ag or Cu.
In the center electrode assembly 13, the center electrodes 21 and 22 are arranged to intersect with each other above the ferrite member 20, which is disk-shaped and made of microwave ferrite, with an insulating layer (not shown) provided therebetween. The intersection angle θ between the center electrodes 21 and 22 is adjusted to be different from 90 degrees. In the first preferred embodiment of the present invention, the center electrodes 21 and 22 are two lines whose outermost widths are parallel. However, the center electrodes 21 and 22 may include one line, or three or more lines, and may have nonparallel or curved shapes. Opposite ends 21a and 21b of the first center electrode 21 and opposite ends 22a and 22b of the second center electrode 22 extend to a bottom surface of the ferrite member 20. The ends 21a to 22b are spaced from one another.
The center electrodes 21 and 22 may be wound around the ferrite member 20 using copper foil, or may be formed by printing silver paste on or inside the ferrite member 20. Alternatively, the center electrodes 21 and 22 may be formed by a laminated base, as described in Japanese Unexamined Patent Application Publication No. 9-232818. However, by using the printing of silver paste, the center electrodes 21 and 22 have high positional accuracy, such that connection to the laminated base 30 is stable. In particular, when connection is made by using minute connecting electrodes 51 to 54 for center electrodes, the formation of the center electrodes 21 and 22 by printing produces outstanding reliability and usability.
As shown in
The laminated base 30 is produced in the following manner. The dielectric sheets 41 to 43 are formed of low temperature sintering dielectric material which includes a principal component of Al2O3 and which includes, as a second component, one or more of SiO2, SrO, CaO, PbO, Na2O, K2O, MgO, BaO, CeO2, and B2O3.
Next, contraction preventing sheets 46 and 47 are produced. The contraction preventing sheets 46 and 47 are not burnt in burning conditions (particularly a burning temperature of 1000 degrees Centigrade or below) of the laminated base 30, and prevent burning contraction in base-plane directions (X and Y directions) of the laminated base 30. The material used for the contraction preventing sheets 46 and 47 is a mixture of alumina powder and stabilized zirconia powder. The sheets 41 to 43, 46, and 47 have thicknesses of about 10 μm to about 200 μm.
The electrodes 51 to 54 and 56 to 58 are formed on reverse surfaces of the sheets 41 to 43, 46, and 47. As the material for the electrodes 51 to 54, and 56 to 58, a material, such as Ag, Cu, or Ag—Pd, which has a low resistivity and which can be burnt simultaneously with the dielectric sheets 41 to 43, is used.
The resistor 27 is formed on a reverse surface of the dielectric sheet 41 by a method such as pattern printing. As the material for the resistor 27, cermet, carbon, ruthenium, or other suitable material, may be preferably used. The resistor 27 may be arranged on an upper surface of the laminated base 30, or may be formed as a chip resistor.
Via holes 60 and via holes 65 are formed by making holes for via holes beforehand using a method such as laser beam machining or punching, and filling the holes with conductive paste.
The capacitor electrode 57 opposes the ground electrode 58, with the dielectric sheet disposed therebetween. The capacitor electrode 57 and the ground electrode 58 define a matching capacitor 26. The matching capacitors 25 and 26, the resistor 27, the electrodes 51 to 54, and the via holes 60 and 65 define an electrical circuit in the laminated base 30.
The above-described dielectric sheets 41 to 43 are stacked. The stacked dielectric sheets 41 to 43 are vertically arranged between the contraction preventing sheets 46 and 47. The integrated body is burnt. This produces a sintered body. After that, by using ultrasonic cleaning, wet honing, or other suitable method, unburnt portions of the contraction preventing sheets 46 and 47 are removed, such that the laminated base 30 in
As shown in
The above-described component parts are assembled in the following manner. As shown in
The laminated base 30 is accommodated in the resin case 3 integrated with the lower metal case portion 8. The ground electrode 58 provided on the laminated base 30 is fixedly connected to the bottom wall 8b by soldering. Similarly, the two via holes 65 on an end surface of the laminated base 30 are fixedly connected to the input extraction electrode 14a and the output extraction electrode by soldering.
The lower metal case portion 8 and the upper metal case portion 4 are joined by soldering to form the metal case. The metal case also functions as a yoke. In other words, the metal case generates a magnetic path surrounding the permanent magnet member 9, the center electrode assembly 13, and the laminated base 30. The permanent magnet member 9 applies a DC magnetic field to the ferrite member 20.
In the above-described manner, the two-port isolator 1 shown in
Differently from the two-port isolator 320 (in
As shown in
The following Table 1 shows values of the input admittance Y2 (pass-band center frequency: 926.5 MHz) of the input port P1 when the intersection angle θ between the center electrodes 21 and 22 of the two-port isolator 1 are variously changed. For comparison, Table 1 also shows the input admittance Y12 of the two-port isolator 320 (shown in
In addition,
The mutual inductance between the center electrodes 21 and 22 decreases when the intersection angle θ is increased, and increases when the intersection angle θ is decreased. Accordingly, a change in intersection angle θ shifts not only the input admittance Y2 of the input port P1 but also the resonant frequency (see
Table 1 and
Conversely, in Examples 4 to 6, by setting the intersection angle θ to be greater than about 90 degrees, the susceptance part of the admittance Y2 of the input port P1 can be set to be positive (capacitive) in the pass-band center frequency. At this time, the greater the intersection angle θ, the greater the absolute value of the susceptance. In addition, when the intersection angle θ is 90 degrees, the susceptance is zero.
As described above, by changing the intersection angle θ between the center electrodes 21 and 22, the susceptance can be changed without substantially changing the conductance. The ferrite member 20 has tensor permeability and its elements are complex numbers. Thus, the self-inductances and mutual inductance of the center electrodes 21 and 22 are represented by complex numbers. In addition, a change in intersection angle θ between the center electrodes 21 and 22 changes the mutual inductance of the center electrodes 21 and 22 and changes the input admittance Y2. In the case of the two-port isolator 300 of the related art in
In the first preferred embodiment, although a change in intersection angle θ changes the mutual inductance similarly to that of the two-port isolator 300, only the susceptance part of the admittance Y2 changes and the conductance does not change. This is because, when viewed from the input port P1, the center electrodes 21 and 22 are connected in series so as to offset a change in real part of the mutual inductance.
Therefore, by changing the intersection angle θ between the center electrodes 21 and 22, the admittance Y2 of the input port P1 is easily set to have a complex conjugate relationship with an external circuit. As a result, matching of the admittance Y2 of the input port P1 is easily adjusted, thus reducing a power loss caused by mismatching. In addition, when the intersection angle θ is small, the size of the capacitors C1 and C2 of the two-port isolator 1 is reduced, thus reducing the size of the two-port isolator 1.
It is preferable for the intersection angle θ to be in the range of about 60 to about 87 degrees, and about 93 to about 120 degrees. This is because, when the intersection angle θ is too close to 90 degrees, it is not effective because the susceptance can be changed only to a too small degree, while, when the intersection angle θ is too far from the intersection angle θ, it is not practical because the susceptance is changed to a excessive degree.
As
The following Table 2 shows values of the input admittance Y2′ (viewed from the input terminal 14) (pass-band center frequency: 926.5 MHz) when the intersection angle θ between the center electrodes 21 and 22 of the two-port isolator 1A is increased to greater than about 90 degrees. Since the intersection angle θ is set to be greater than about 90 degrees, the susceptance part of input admittance Y2 at the input port P1 is positive in the pass-band center frequency (see Examples 4 to 6 in Table 1). The susceptance part of the input admittance Y2′ of the input terminal 14 is approximately zero.
Table 2 indicates that, by setting the intersection angle θ between the center electrodes 21 and 22 to be greater than about 90 degrees, only connection of one inductor 28 to the input port P1 increases the input admittance Y2′ (viewed from the input terminal 14) to greater than about 0.02 S. Conversely, in the case of the two-port isolator 320 (see
As
The following Table 3 shows values of the input admittance Y2′ (viewed from the input terminal 14) (pass-band center frequency: 926.5 MHz) when the intersection angle θ between the center electrodes 21 and 22 of the two-port isolator 1B is reduced to less than about 90 degrees. Since the intersection angle θ is set to be less than about 90 degrees, the susceptance part of the input admittance Y2 the input port P1 is negative in the pass-band center frequency (see Examples 1 to 3 in Table 1). The susceptance part of the input admittance Y2′ of the input terminal 14 is approximately zero.
Table 3 indicates that, by setting the intersection angle θ between the center electrodes 21 and 22 to be less than about 90 degrees, only connection of the capacitor 29 to the input port P1 increases the input admittance Y2′ (viewed from the input terminal 14) to greater than about 0.02 S. As a result, the size and cost of the two-port isolator 1B are greatly reduced. In addition, the number of connecting positions between elements is reduced, so that the reliability of the two-port isolator 1B is improved. The total capacitance of the capacitors C1, C2, and C3 can be set to be less than the total capacitance of the capacitors C1 and C2 of the two-port isolator 1A according to the second preferred embodiment. Thus, the sized of the two-port isolator 1B according to the third preferred embodiment is reduced as compared to the two-port isolator 1A according to the second preferred embodiment.
As
The following Table 4 shows values of attenuation in the second harmonic and the third harmonic when the intersection angle θ between the center electrodes 21 and 22 is set to be greater than about 90 degrees. For comparison, Table 4 also shows attenuation in harmonics of the two-port isolator 320 (in
Table 4 and
As
In this case, in order to set the susceptance part of the input admittance Y2′ of the input terminal 14 to be approximately zero, the capacitor 29 is set such that the capacitance C3 of the capacitor 29 satisfies the expression:
C3=−B/ω
where ω represents an angular frequency, and B represents one of the susceptances in Examples 1 to 3 in Table 1.
The following Table 5 shows values of the capacitance C3 which are determined as described above. The frequency is 926.5 MHz. Since the intersection angle θ is set to be less than about 90 degrees, the susceptance part of the admittance Y2 of the input port P1 is negative in the pass-band center frequency.
Table 5 indicates that the total capacitance of the capacitances C1, C2, and C3 in Examples 16 to 18 is reduced as compared to the total capacitance (see the Related Art in Table 1) of the two-port isolator of the related art. Therefore, by setting the intersection angle θ between the center electrodes 21 and 22 to be less than about 90 degrees, and connecting the capacitor 29 in parallel to the input port P1, the total capacitance is reduced as compared to that of the two-port isolator of the related art, such that the size of the two-port isolator 1D is reduced.
A communication apparatus according to a sixth preferred embodiment of the present invention is described below, with a cellular phone as an example of the communication apparatus.
Each of the two-port isolators 1, 1A, 1B, 1C, and 1D according to the first to fifth preferred embodiments can be used as the transmitting isolator 231. By mounting each of these two-port isolators, a cellular phone having improved electrical characteristics and high reliability is achieved.
The present invention is not limited to the foregoing preferred embodiments, but may be variously modified. For example, by inverting the N pole and S pole of the permanent magnet 9, the input port P1 and the output port P2 are switched. However, when using the port P2 as an input port, and the port P1 as an output port, an input return loss has a relatively narrow band and an output return loss has a relatively wide band.
It should be understood that the foregoing description is only illustrative of the present invention. Various alternatives and modifications can be devised by those skilled in the art without departing from the present invention. Accordingly, the present invention is intended to embrace all such alternatives, modifications and variations that fall within the scope of the appended claims.
Number | Date | Country | Kind |
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2003-312689 | Sep 2003 | JP | national |
2004-178057 | Jun 2004 | JP | national |
Number | Date | Country | |
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20080174381 A1 | Jul 2008 | US |
Number | Date | Country | |
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Parent | 10909605 | Aug 2004 | US |
Child | 12050365 | US |