The present invention relates to an antenna device including an antenna coupling element coupled between a plurality of radiating elements and a feeding circuit and also relates to a communication terminal apparatus.
In order to widen the usable frequency range of antenna device or to support a plurality of frequency ranges, an antenna device including two radiating elements directly or indirectly coupled to each other is used. Japanese Patent No. 5505561 discloses an antenna device including two radiating elements and an antenna coupling element that controls power feeding for the two radiating elements.
For example, some communication antennas for mobile phones cover a wide frequency range such as 0.6 GHz to 2.7 GHz. Moreover, for the purpose of implementing carrier aggregation, in which the transmission rate is increased by using a plurality of frequency ranges together, there is a demand for an antenna device that can use a wide range of frequencies together.
The antenna device disclosed in Japanese Patent No. 5505561 is formed by coupling an antenna coupling element, which is configured to implement a transformer, between two radiating elements (a feeding radiating element and a parasitic radiating element) and a feeding circuit. The antenna device having this configuration is very useful in covering a wide range of frequencies together.
However, as functions of communication terminal apparatuses including antenna devices are enhanced, the antenna space is accordingly decreased, and as a result, the feeding radiating element and the parasitic radiating element are arranged close to each other. This arrangement strengthens electric field coupling between the feeding radiating element and the parasitic radiating element.
Such a condition causes a problem in which sufficient radiation efficiency cannot be obtained when the current flowing through the parasitic radiating element due to the antenna coupling element and the current flowing through the parasitic radiating element due to the electric field coupling weaken each other.
When the amount of current flowing through the parasitic radiating element is less than the amount of current that should flow through the parasitic radiating element as described above, the radiation efficiency of the parasitic radiating element is lowered.
Preferred embodiments of the present invention provide antenna devices and communication terminal apparatuses in each of which, in a condition that direct coupling and indirect coupling via an antenna coupling element exist between two radiating elements, a decrease in the radiation efficiency due to currents flowing into a radiating element and canceling each other out is significantly reduced or prevented.
An antenna device according to a preferred embodiment of the present disclosure includes a first radiating element, a second radiating element, a first coil coupled to one of the first radiating element and a feeding circuit, and a second coil coupled to the second radiating element and coupled to the first coil via an electromagnetic field. The first radiating element and the second radiating element are coupled to each other via an electric field. Additionally, the first coil and the second coil define an antenna coupling element. According to a determined direction of coupling between the first coil and the second coil, at a resonant frequency generated by the antenna coupling element and the second radiating element, the absolute value of the phase difference between a current flowing into the second radiating element due to the electromagnetic field of the first coil and the second coil and a current flowing into the second radiating element due to the electric field of the first radiating element and the second radiating element is equal to or less than about 90 degrees.
With the features described above, the current flowing into the second radiating element due to electromagnetic field coupling between the first coil and the second coil and the current flowing into the second radiating element due to electric field coupling between the first radiating element and the second radiating element do not cancel each other.
The preferred embodiments of the present invention provide antenna devices and communication terminal apparatuses in each of which, in a condition that direct coupling due to parasitic capacitance and indirect coupling via an antenna coupling element exist between two radiating elements, a decrease in the radiation efficiency due to currents flowing into the radiating element and canceling each other is significantly reduced or prevented.
The above and other elements, features, steps, characteristics and advantages of the present invention will become more apparent from the following detailed description of the preferred embodiments with reference to the attached drawings.
Conductor patterns L1a, L1b, L2a, and L2b are provided inside the antenna coupling element 20. The conductor pattern L1a and the conductor pattern Lib are coupled to each other via an interlayer connection conductor V1. The conductor pattern L2a and the conductor pattern L2b are coupled to each other via an interlayer connection conductor V2. In
When the antenna coupling element 20 is provided by a resin multilayer substrate, the insulating base layer is preferably, for example, a liquid crystal polymer (LCP) sheet, and the conductor patterns L1a, L1b, L2a, and L2b are preferable provided by, for example, patterning copper foils. When the antenna coupling element 20 is provided by a ceramic multilayer substrate, the insulating base layer is preferably made of, for example, low temperature co-fired ceramics (LTCC), and the conductor patterns L1a, L1b, L2a, and L2b are preferably formed by, for example, applying a copper paste.
Since the base layer is made of a non-magnetic material (not made of a magnetic ferrite), the antenna coupling element 20 is able to define a transformer have a predetermined inductance and a coupling coefficient in a high frequency range of about 0.6 GHz to about 2.7 GHz, for example.
The conductor patterns L1a, L1b, L2a, and L2b are provided centrally in the middle layer of the multilayer body, and as a result, there is an interval between a ground conductor at the circuit board and a first coil L1 and a second coil L2 in the state in which the antenna coupling element 20 is mounted at the circuit board. Further, if a metal component or element approaches the upper portion of the antenna coupling element 20, an interval still exists between this metal component or element and the first coil L1 and the second coil L2. As a result, the magnetic field of the first coil L1 and the second coil L2 described later is less likely to be affected by the outside environment and stable characteristics are able to be provided.
A feeding circuit 30 is provided at the circuit board 40. Additionally, the antenna coupling element 20 and an inductor L11 are mounted at the circuit board 40.
The first radiating element 11, the second radiating element 12, and the circuit board 40 are enclosed by the housing 50, which has conductivity, when viewed in plan view. The first radiating element 11 is provided at a portion of the housing 50. This portion of the housing is configured to be electrically separated from the other portion of the housing 50. The second radiating element 12 is provided as a conductor pattern at the resin portion in the housing 50 by using the laser-direct-structuring (LDS) process, for example. The second radiating element 12 is not limited to this example and may be provided as a conductor pattern at, for example, a flexible printed circuit (FPC) by using a photoresist process, for example.
The first radiating element connection terminal T1 of the antenna coupling element 20 is coupled to the first radiating element 11 and the second radiating element connection terminal T4 is coupled to the second radiating element 12. The feeding circuit connection terminal T2 is coupled to the feeding circuit 30 and the ground connection terminal T3 is coupled to a ground conductor pattern. With the features described above, the first coil and the second coil of the antenna coupling element 20 shown in
The inductor L11 is coupled between one end of the first radiating element 11 and ground.
The first radiating element 11 operates as a loop antenna in conjunction with the inductor L11 and the ground conductor pattern provided at the circuit board. The second radiating element 12 operates as a monopole antenna.
A parasitic capacitance C12 between radiating elements is generated at a portion PP between a portion of the first radiating element 11 and a portion of the second radiating element 12. In the example shown in
As shown in
The first radiating element 11 resonates in a frequency range of a low band (for example, about 0.60 GHz to about 0.96 GHz). The first radiating element 11 to which the first coil L1 is coupled supports at least a low band. A resonant frequency included in such a low band is a “first resonant frequency”. Additionally, the first radiating element resonates in a frequency range of a high band (for example, about 1.71 GHz to about 2.69 GHz) that is a frequency range higher than the low band. For example, in the case in which the fundamental resonant frequency of the first radiating element 11 to which the first coil L1 is coupled exists in the low band and its third harmonic resonant frequency exists in the high band, the first radiating element 11 resonates in both the low band and the high band.
The second radiating element 12 resonates with the antenna coupling element 20 in the frequency range of the high band (for example, about 1.71 GHz to about 2.69 GHz). The resonant frequency in this case is a “second resonant frequency”, for example, about 2.3 GHz. The second radiating element 12 supports a high band and widens the high band. Thus, the fundamental resonant frequency of the first radiating element to which at least the first coil L1 is coupled is lower than the fundamental resonant frequency of the second radiating element 12 and the antenna coupling element.
The first radiating element 11 is fed with power from the feeding circuit 30 through the first coil L1. The second radiating element 12 is fed with power from the second coil L2 (power is supplied with an induced electromotive force in the second coil L2). For example, when a current i1 flows in the first coil L1, a current i2 is induced in the second coil L2, and as a result, the second radiating element 12 is fed (driven) with power supplied with the current i2. In addition, the second radiating element 12 is coupled to the first radiating element 11 via an electric field by the parasitic capacitance C12. Due to this electric field coupling, a current i12 flows toward the second radiating element 12 side.
As shown in
The polarity of the coupling between the first coil L1 and the second coil L2 is determined such that the current i2 and the current i12 do not weaken each other at the second resonant frequency described above. In other words, the first coil L1 and the second coil L2 are coupled to each other such that, at the second resonant frequency defined by the second radiating element 12 and the antenna coupling element 20 defined by the first coil L1 and the second coil L2, the absolute value of the phase difference between the current i12 flowing into the second radiating element 12 due to electromagnetic field coupling between the first coil L1 and the second coil L2 and the current i2 flowing into the second radiating element 12 due to electric field coupling is equal to or less than about 90 degrees.
As a result, the relationship between the direction of the magnetic field created by the first coil L1 when a current flows from the first coil L1 to the first radiating element 11 and the direction of the magnetic field created by the second coil L2 when a current flows from the second coil L2 to the second radiating element 12 is changed between the equal or substantially equal relationship and the opposite or substantially opposite relationship in accordance with the position of electric field coupling in the antenna, but the coupling relationship described above is not changed. For example, depending on the position of electric field coupling in the antenna, in the antenna coupling element 20, the terminal T3 may be a second radiating element connection terminal and the terminal T4 may be a ground connection terminal. Accordingly, the first coil L1 and the second coil L2 provide a direction of the magnetic field created by the first coil L1 when a current flows from the first coil L1 to the first radiating element 11 that is opposite or substantially opposite to a direction of the magnetic field created by the second coil L2 when a current flows from the second coil L2 to the second radiating element 12.
Due to the relationship described above, the current i12 and the current i2 do not weaken each other, and thus, the radiation efficiency in the high band is significantly improved. Furthermore, in the case in which the absolute value of the phase difference between the current i12 and the current i2 is less than about 90 degrees, the currents strengthen each other, and thus, the radiation efficiency in the high band is further significantly improved.
The polarity of coupling between the first coil L1 and the second coil L2 of the antenna coupling element 20 of the antenna device of the comparative example is opposite or substantially opposite to the polarity of the coupling between the first coil L1 and the second coil L2 of the antenna coupling element 20 included in the antenna device 101 according to the present preferred embodiment. In the antenna device of the comparative example, as shown in
In the present preferred embodiment, as seen from
By using the electromagnetic field coupling described above, the phase of the current i12 flowing into the second radiating element 12 is able to be determined by measuring, for example, with the use of a network analyzer or the like, the phase of the current flowing between the second radiating element and the second coil L2 at the second resonant frequency in the state in which the first radiating element 11 and the second radiating element 12 are physically sufficiently spaced apart from each other in the structure of the antenna device 101 as shown in
However, it is in practice difficult to directly measure the phase of the current without bringing a current probe adjacent to or in a vicinity of the object. Accordingly, the phase of the current i12 is determined, for example, as follows: firstly, 2×2 S (Scattering) parameters of two input ends, which are an input end of the first radiating element 11 (an end on the power supply side of the first radiating element 11) and an input end of the second radiating element 12 (an end on the ground side of the second radiating element 12), are measured and 4×4 S parameters of only the antenna coupling element 20 having four terminals of the terminals T1 to T4 are also measured; and subsequently, by including the circuitry of the antenna device 101 and the S parameters described above, the current flowing between the second radiating element 12 and the second coil L2 is determined by performing a calculation on a circuit simulator. Furthermore, for example, the structure of the antenna device 101 as shown in
The feeding circuit 30 shown in
Next, an example is described in which, regardless of the polarity of coupling between the first coil L1 and the second coil L2 of the antenna coupling element 20, the current i12 flowing into the second radiating element 12 due to electromagnetic field coupling between the first coil L1 and the second coil L2 and the current i2 flowing into the second radiating element 12 due to electric field coupling do not weaken each other at the second resonant frequency.
The antenna devices shown in
Thus, under the condition that the current i12 flowing into the second radiating element 12 due to electromagnetic field coupling between the first coil L1 and the second coil L2 and the current i2 flowing into the second radiating element 12 due to electric field coupling do not cancel each other out at the second resonant frequency, the antenna coupling element 20 shown in
Two kinds of the antenna coupling elements 20 that are different from each other with respect to the polarity of coupling between the first coil L1 and the second coil L2 are previously prepared and one antenna coupling element 20 of a predetermined polarity of coupling may be used in accordance with the condition to which the antenna coupling element 20 is applied. Alternatively, in the example shown in
Next, some examples of an antenna device including features of individual portions different from those of the antenna devices described above will be provided.
The feeding circuit 30 is provided at the circuit board 40. Additionally, the antenna coupling element 20 and the inductor L11 are mounted at the circuit board 40.
The first radiating element 11, the second radiating element 12, and the third radiating element 13 are provided as conductor patterns at the resin portion in the housing 50 by using the laser-direct-structuring (LDS) process or the like, for example. The first radiating element 11, the second radiating element 12, and the third radiating element 13 are not limited to this example and may be provided at the circuit board 40 or provided as conductor patterns at a flexible printed circuit (FPC) by employing a photolithography process or the like, for example. In the case in which all the radiating elements are provided inside the housing as described above, the housing 50 may be provided of an insulating member without conductivity, for example, a glass member or a resin member.
The first radiating element connection terminal T1 of the antenna coupling element 20 is coupled to the first radiating element 11 and the second radiating element connection terminal T4 is coupled to the second radiating element 12. The feeding circuit connection terminal T2 is coupled to the feeding circuit 30 and the ground connection terminal T3 is coupled to a ground conductor pattern.
The inductor L11 is coupled between one end of the first radiating element 11 and ground.
The first radiating element 11 defines and functions as a loop antenna in conjunction with the inductor L11 and the ground conductor pattern provided at the circuit board. The second radiating element 12 operates as a monopole antenna. The third radiating element 13 is, for example, a GPS antenna and is coupled to a feeding circuit different from the feeding circuit 30.
Other features, components, and elements are the same as or similar to those of the antenna devices shown in
The first radiating element 11 is provided at a portion of the housing. This portion of the housing is electrically separated from the other portion of the housing. The circuit board 40 includes a ground region GZ in which a ground conductor pattern 42 is provided and a non-ground region NGZ in which the ground conductor pattern 42 is not provided. The second radiating element 12 is provided in the non-ground region NGZ.
The second radiating element 12 is provided as a linear conductor pattern including a folded portion 12FB in a midpoint. Since the second radiating element 12 is provided as a linear conductor pattern including a folded portion in a midpoint as described above, the second radiating element 12 is able to be provided in a reduced space. Moreover, in this example, the second radiating element 12 includes a first linear conductor pattern 12A extending from the antenna coupling element 20 and a second linear conductor pattern 12B provided by folding the second radiating element 12 to the side apart from the first radiating element 11. With this structure, the portion close to the first radiating element 11 is relatively short and the first radiating element 11 and the second radiating element 12 extend in opposite or substantially opposite directions, and thus, actual electric field coupling with the first radiating element 11 is relatively small.
The line width of the second linear conductor pattern 12B is greater than the line width of the first linear conductor pattern 12A, and thus, the resonance band width of the resonance circuit including the second radiating element 12 is able to be widened.
The inductors Lila and L11b have different inductances and the capacitors C11a and C11b have different capacitances. The resonant frequency of the first radiating element 11 is able to be changed in accordance with a particular one selected from the reactance elements Lila, L11b, C11a and C11b. Other features, components, and elements are the same as or similar to those shown in
The preferred embodiments of the present invention are also able to be applied to an antenna device in which the first radiating element 11 is an inverted F antenna or PIFA.
The preferred embodiments of the present invention are also able to be applied to an antenna device including an inverted F antenna or PIFA including the features described herein.
While preferred embodiments of the present invention have been described above, it is to be understood that variations and modifications will be apparent to those skilled in the art without departing from the scope and spirit of the present invention. The scope of the present invention, therefore, is to be determined solely by the following claims.
Number | Date | Country | Kind |
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2018-084210 | Apr 2018 | JP | national |
This application claims the benefit of priority to Japanese Patent Application No. 2018-084210 filed on Apr. 25, 2018 and is a Continuation Application of PCT Application No. PCT/JP2019/012058 filed on Mar. 22, 2019. The entire contents of each application are hereby incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2019/012058 | Mar 2019 | US |
Child | 16992197 | US |