An embodiment of the present invention relates to a technique for compensating for variations in the characteristics of a phased array antenna.
In a phased array antenna, a high frequency signal is applied to a portion or all of a plurality of antenna elements. The phased array antenna can control the radiation directivity of the antenna while the direction of the antenna is fixed in one direction by controlling the amplitude and phase of each high frequency signal. The phased array antenna uses phase shifters to control the phase of high frequency signals applied to the antenna elements.
Various methods are employed for the phase shifter, such as a method of physically changing the length of the transmission line to change the phase of the high frequency signal, a method of changing the impedance in the middle of the transmission line to phase the high frequency by reflection, and a method of generating a signal having the desired phase by controlling and combining the gain of the amplifier that amplifies two signals having different phases. In addition, as an example of a phase shifter, a type which utilizes the characteristic properties of a liquid crystal material in which the dielectric constant varies with the applied voltage has been disclosed (Japanese Unexamined Patent Application Publication No. H11-103201).
A phased array antenna according to an embodiment of the present invention includes a plurality of antenna elements, a plurality of phase shifters, each of the plurality of phase shifters is connected to each of the plurality of antenna elements, respectively, a phase control circuit for controlling the amount of phase shift of the plurality of phase shifters, and a temperature sensor for detecting the temperature of the plurality of phase shifters. The phase control circuit is configured to control a voltage applied to the plurality of phase shifters based on the temperature detected by the temperature sensor.
Hereinafter, embodiments of the present invention will be described with reference to the drawings and the like. The present invention may be carried out in various forms without departing from the gist thereof, and is not to be construed as being limited to any of the following embodiments. Although the drawings may schematically represent the width, thickness, shape, and the like of each part in comparison with the actual embodiment in order to clarify the description, they are merely examples and do not limit the interpretation of the present invention. In the present specification and each of the figures, elements similar to those described above with respect to the figures mentioned above are designated by the same reference numerals (or numbers followed by a, b, etc.), and a detailed description thereof may be omitted as appropriate. Furthermore, the characters “first” and “second” appended to each element are convenient signs used to distinguish each element, and have no further meaning unless specifically described.
As used herein, where a member or region is “on” (or “below”) another member or region, this includes cases where it is not only directly on (or just under) the other member or region but also above (or below) the other member or region, unless otherwise specified. That is, it includes the case where another component is included in between above (or below) other members or regions.
The radio waves emitted from each of the plurality of antenna elements 102 have coherency. Therefore, the radio waves emitted from each of the plurality of antenna elements 102 form a phase-aligned wavefront. The phase shifter 104 adjusts the phase of the radio waves emitted from the antenna element 102. The phase shifter 104 controls the phase of the high frequency signal emitted as a radio wave by the phase control circuit 106. Here, the amount of phase shift of the high frequency signal controlled by the phase shifter 104 is referred to as an “amount of phase shift”.
The phased array antenna 100 individually adjusts the phase of the high frequency signal supplied by the phase control circuit 106 to each of the plurality of antenna elements 102 by the phase shifter 104. The direction of travel of the wavefront of radio waves emitted from the plurality of antenna elements 102 can be controlled at any angle. The phased array antenna 100 controls the directivity of the radiating radio waves by controlling the phase of each of the plurality of antenna elements 102.
On the other hand, the phase array antenna device 100 for reception is configured to provide a high frequency amplifier instead of the oscillator 114 to amplify the radio waves received by the plurality of antenna elements 102 and output the signal to a subsequent circuit, such as a demodulator circuit.
The temperature sensor 108 includes a sensing unit 109 and a measuring circuit 110. The sensing unit 109 is implemented by use of a non-contact type temperature sensor for detecting infrared intensity, or a contact type temperature sensor for detecting thermoelectric power, electrical resistance, or a change in magnetism, or the like. For example, a resistance temperature sensor is used in the sensing unit 109. For example, a thermistor or a platinum thin film temperature sensor may be used as the resistance temperature sensor. The sensing unit 109 is disposed such that at least one temperature of the phase shifter 104 is detectable. For example, the sensing unit 109 is disposed in contact with the phase shifter 104. The sensing unit 109 is also located adjacent to or close to the phase shifter 104. In other words, the sensing unit 109 is disposed to sense the temperature of the environment where the phase shifter 104 is located. In either case, the sensing unit 109 may be disposed to directly measure the temperature of the phase shifter 104, or it may be disposed to sense the temperature of the environment in which the plurality of phase shifters 104 are located as a substitute characteristic.
The signal detected by the sensing unit 109 is input to the measurement circuit 110. The measurement circuit 110 converts the signal output from the sensing unit to temperature data and outputs it to the phase control circuit 106. The phase control circuit 106 outputs a control signal for controlling the amount of phase shift to each phase shifter 104. The phase control circuit 106 sets the setting value of the phase control signal according to the temperature so that the amount of phase shift of the phase shifter 104 does not vary with the temperature based on the temperature data input from the measurement circuit 110.
The first electrode 120 is formed of a conductor pattern extending substantially over the first substrate 116. The second electrode 122, on the other hand, is formed of an elongated, strip-like conductor pattern to form a microstrip line. The first electrode 120 is applied with a constant potential. For example, the first electrode 120 is grounded. One longitudinal direction of the second electrode 122 serves as the input terminal of the high frequency signal and the other as the output terminal of the high frequency signal. The liquid crystal layer 124 is provided to fill at least a region between the first electrode 120 and the second electrode 122. Although not shown in
A liquid crystal material is used as the liquid crystal layer 124. As the liquid crystal material, nematic liquid crystal, smectic liquid crystal, cholesteric liquid crystal, discotic liquid crystal, and ferroelectric liquid crystal (for example, chiral smectic liquid crystal) can be used.
A control signal is applied to the second electrode 122 from the phase control circuit 106. The control signal is a DC or AC voltage signal. Preferably, the DC voltage signal is a polarity reversing signal which has a polarity that is reversed over time. When the control signal is applied to the second electrode 122, the liquid crystal layer 124 changes the orientation of the liquid crystal molecule according to the potential difference between the first electrode 120 and the second electrode 122. Since the liquid crystal molecule is a polar molecule, the dielectric constant of the liquid crystal layer 124 varies depending on the orientation of the liquid crystal molecule. That is, the phase shifter 104 can vary the dielectric constant by the voltage applied to the second electrode 122.
The dielectric constant of the liquid crystal material varies depending on the temperature. Accordingly, the phase shifter using a liquid crystal material changes the amount of phase shift depending on temperature. Thus, the challenge is to vary the directivity of the phased array antenna in response to changes in temperature.
In order to overcome these problems and precisely control the amount of phase shift of the high frequency signal propagated by the phase shifter 104, it is preferred that the control signal applied to the second electrode 122 be compensated for according to the temperature characteristics of the liquid crystal layer 124. The phased array antenna 100 has the function of detecting the temperature of the phase shifter 104 by the temperature sensor 108, as described with reference to
As described above, since the liquid crystal molecules are polar molecules and have dielectric constant anisotropy, the dielectric constant varies depending on the orientation state.
The second dielectric constant (ε//) is larger than the first dielectric constant (ε⊥) (ε⊥<ε//). This is because the liquid crystal molecules 126 in the second state are oriented in the direction perpendicular to the main surfaces of the first substrate 116 and the second substrate 118. The phase shifter 104 can vary the phase of the high frequency signal flowing through the second electrode 122 by changing the dielectric constant of the liquid crystal layer 124. For example, when the dielectric constant of the liquid crystal layer 124 increases, the phase velocity of the high frequency signal is slowed. Specifically, the phase shifter 104 changes from the first state to the second state, thereby delaying the phase of the high frequency signal propagating through the second electrode 122. Thus, it is possible to control the amount of phase shift of the high frequency signal by changing the voltage (DC voltage) applied to the second electrode 122.
Since the dielectric constant of the liquid crystal layer 124 is changed by the polarization of the liquid crystal molecules 126, the dielectric constant can be changed by applying an AC voltage to the second electrode 122 and changing its frequency. For example, when the frequency of the AC voltage applied to the second electrode 122 increases, the liquid crystal molecule 126 cannot follow the frequency and becomes non-polarized. Accordingly, the dielectric constant of the liquid crystal layer 124 can be varied by changing the frequency of the AC voltage applied to the second electrode 122. In this case, when the frequency of the AC voltage is high and the polarization of the liquid crystal molecule 126 cannot follow the frequency, this corresponds to the first state described above, and when the frequency of the AC voltage is low and the polarization of the liquid crystal molecule 126 can follow the frequency, this corresponds to the second state described above. In this manner, the phase shifter 104 can control the phase of the high frequency signal by applying an AC voltage to the second electrode 122 and varying its frequency.
The dielectric constant of the liquid crystal layer 124 varies depending on the temperature. Table 1 shows an example of a temperature-dependent dielectric constant in a nematic liquid crystal. The dielectric constant of the first dielectric constant (ε⊥) in the first state does not vary in the range of 20° C., 40° C., and 60° C., whereas the second dielectric constant (ε//) in the second state varies in the same temperature range. Table 1 also shows that the dielectric constant varies with the frequency (1 kHz, 20 GHz) of the AC voltage applied to the liquid crystal layer.
As shown in Table 1, the dielectric constant of the liquid crystal layer 124 is constant with respect to temperature, whereas the first dielectric constant (ε⊥) is constant with respect to temperature, and the second dielectric constant (ε//) is varied with respect to temperature. Accordingly, it is possible to compensate for the temperature of the dielectric constant by adjusting the value of the control signal VLC controlling the orientation state of the liquid crystal layer 124. Here, to perform temperature compensation for the dielectric constant of the liquid crystal layer 124, it is sufficient to control the tunability (τeff) defined in Eq. (1) to be constant.
τeff=(ε//−ε⊥)/ε// (1)
Although the dielectric constant of the liquid crystal layer 124 varies due to a change in the orientation of the liquid crystal molecule 126, the capacitance formed between the first electrode 120 and the second electrode 122 also changes with a concomitant change. That is, the capacitance formed between the first electrode 120 and the second electrode 122 is greater in the second state than in the first state. Such characteristics can also be used to vary the resonant frequency of the antenna. That is, the resonant condition of the antenna can be variable.
Although the above shows the case where the control signal VLC is a DC voltage, the same applies to the case where the AC control signal VLC is applied. In this case, the output signal setting unit 136 sets the frequency fLC of the control signal VLC based on the temperature compensation data.
The phased array antenna 100 according to one embodiment of the present invention includes the phase control circuit 106 that outputs a control signal for controlling the amount of phase shift of the phase shifter 104. The phase control circuit 106 outputs a control signal based on the temperature of the phase shifter 104 sensed by the temperature sensor 108. Accordingly, radio waves with a precisely controlled phase from the antenna element array 103 can be stably output regardless of the ambient temperature.
Number | Date | Country | Kind |
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2019-019239 | Feb 2019 | JP | national |
This application is a Continuation of International Patent Application No. PCT/JP2019/045859, filed on Nov. 22, 2019, which claims priority to Japanese Patent Application No. 2019-019239, filed on Feb. 6, 2019, the disclosures of which are incorporated herein by reference for all purposes as if fully set forth herein.
Number | Date | Country | |
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Parent | PCT/JP2019/045859 | Nov 2019 | US |
Child | 17394951 | US |