JP2020024165A - Radiated power estimation method - Google Patents

Radiated power estimation method Download PDF

Info

Publication number
JP2020024165A
JP2020024165A JP2018149490A JP2018149490A JP2020024165A JP 2020024165 A JP2020024165 A JP 2020024165A JP 2018149490 A JP2018149490 A JP 2018149490A JP 2018149490 A JP2018149490 A JP 2018149490A JP 2020024165 A JP2020024165 A JP 2020024165A
Authority
JP
Japan
Prior art keywords
power
electric power
measuring
transmitting antenna
angle
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP2018149490A
Other languages
Japanese (ja)
Other versions
JP7016303B2 (en
Inventor
福田 敦史
Atsushi Fukuda
敦史 福田
浩司 岡崎
Koji Okazaki
浩司 岡崎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NTT Docomo Inc
Original Assignee
NTT Docomo Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NTT Docomo Inc filed Critical NTT Docomo Inc
Priority to JP2018149490A priority Critical patent/JP7016303B2/en
Publication of JP2020024165A publication Critical patent/JP2020024165A/en
Application granted granted Critical
Publication of JP7016303B2 publication Critical patent/JP7016303B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

To provide a radiated power estimation technology capable of estimating total radiated power efficiently and highly accurately in a short time.SOLUTION: A radiated power estimation method is provided for finding total radiated power of a transmitting antenna in a measuring system comprising a base station device, a transmitting antenna, a turntable for rotating the transmitting antenna, a receiving antenna for receiving a radio wave coming from the transmitting antenna, and an electric power measuring instrument for measuring electric power of the received radio wave. The radiated power estimation method has: Step S1 of the electric power measuring instrument measuring electric power in a portion in a bandpass of a signal that is transmitted by the transmitting antenna and received by the receiving antenna in each of predetermined angle samples, while the turntable continuously rotates; Step S2 of the electric power measuring instrument specifying an angle sample having a ratio of the electric power obtained in each angle sample to the maximum value of the electric power of equal to or more than a predetermined threshold; Step S3 of the electric power measuring instrument measuring the electric power at the whole signal bandwidth with a specified angle sample; and Step S4 for estimating the total radiated power from the electric power obtained in Step S3.SELECTED DRAWING: Figure 4

Description

本発明は、空間に放射された電波の全放射電力を推定する放射電力推定技術に関する。   The present invention relates to a radiation power estimation technique for estimating the total radiation power of radio waves radiated into space.

特定方向において強い放射強度となる指向性を持たせるアレーアンテナシステムでは、アンテナと送信機が一体化されたアクティブアンテナが用いられる場合がある。アクティブアンテナにおいて送信機の出力端子にモニタ用のコネクタが装備されていない場合、送信電力測定はアンテナから空間に放射された全放射電力を測定することによって行われる。空間に放射された全放射電力を測定する方法はOver The Air(OTA)測定法と呼ばれ、OTA測定システムが用いられる。例えば非特許文献1にOTA測定システムが開示されている。   2. Description of the Related Art In an array antenna system having a directivity having a strong radiation intensity in a specific direction, an active antenna in which an antenna and a transmitter are integrated may be used. When the output terminal of the transmitter is not equipped with a connector for monitoring in the active antenna, the transmission power measurement is performed by measuring the total radiated power radiated from the antenna to the space. A method of measuring the total radiated power radiated into the space is called an Over The Air (OTA) measurement method, and an OTA measurement system is used. For example, Non Patent Literature 1 discloses an OTA measurement system.

図1を参照して、基地局装置91の送信電力を測定する従来のOTA測定システム900および測定方法を説明する。OTA測定システム900は、基地局装置91と、基地局装置91に接続されている送信アンテナ92と、送信アンテナ92が載せられた回転台96(この例では基地局装置91も回転台96に載せられている)と、送信アンテナ92から所定の距離だけ離れた位置に設置されている受信アンテナ93と、受信アンテナ93が受信した電波の電力を測定する電力測定器95を含む。   With reference to FIG. 1, a conventional OTA measurement system 900 for measuring the transmission power of the base station device 91 and a measurement method will be described. The OTA measurement system 900 includes a base station apparatus 91, a transmission antenna 92 connected to the base station apparatus 91, and a turntable 96 on which the transmission antenna 92 is mounted (in this example, the base station apparatus 91 is also mounted on the turntable 96). ), A receiving antenna 93 installed at a position separated by a predetermined distance from the transmitting antenna 92, and a power measuring device 95 for measuring the power of radio waves received by the receiving antenna 93.

受信アンテナ93は、送信アンテナ92から受信アンテナ93に向けて放射された電波を受信する。電力測定器95は、受信アンテナ93で受信した電波の電力を測定する。受信アンテナ93の利得および送信アンテナ92と受信アンテナ93との間の距離から伝搬損が求められる。したがって、電力測定器95で受信電力を測定することによって、受信アンテナ93の利得と伝搬損から送信アンテナ92から放射された電波の電力を推定できる。全放射電力を測定する場合には、送信アンテナ92を中心とする球面上で受信アンテナ93を移動させ、電力測定器95で測定された受信電力から各方向での放射電力を推定し、各方向の放射電力の和を求める。または、受信アンテナ93を固定し、回転台96を水平方向と垂直方向の組み合わせで2軸回転させ、電力測定器95で測定された受信電力から各方向での放射電力を推定し、各方向の放射電力の和を求めてもよい。   The receiving antenna 93 receives a radio wave radiated from the transmitting antenna 92 toward the receiving antenna 93. The power measuring device 95 measures the power of the radio wave received by the receiving antenna 93. The propagation loss is determined from the gain of the receiving antenna 93 and the distance between the transmitting antenna 92 and the receiving antenna 93. Therefore, the power of the radio wave radiated from the transmitting antenna 92 can be estimated from the gain and the propagation loss of the receiving antenna 93 by measuring the received power with the power measuring device 95. When measuring the total radiated power, the receiving antenna 93 is moved on a spherical surface around the transmitting antenna 92, and the radiated power in each direction is estimated from the received power measured by the power measuring device 95, and the radiated power in each direction is estimated. The sum of the radiated power of Alternatively, the receiving antenna 93 is fixed, the turntable 96 is biaxially rotated in a combination of the horizontal direction and the vertical direction, the radiated power in each direction is estimated from the received power measured by the power meter 95, and the radiated power in each direction is estimated. The sum of the radiated powers may be obtained.

一般的に、回転台96の動作として連続回転とステップ回転がある。連続回転は、回転を停止させずに一定の速度で連続的に回転する回転方法である。ステップ回転は、角度標本ごとで回転を一時的に止める回転方法である。連続回転は或る角度から次の角度に移動するまでの時間が一定であるため、或る角度における受信電力測定は回転台96が次の角度に到達するまでに終える必要がある。   Generally, the operation of the turntable 96 includes continuous rotation and step rotation. Continuous rotation is a method of rotating continuously at a constant speed without stopping the rotation. Step rotation is a rotation method in which rotation is temporarily stopped for each angle sample. Since continuous rotation has a constant time required to move from a certain angle to the next angle, the reception power measurement at a certain angle needs to be completed before the turntable 96 reaches the next angle.

また、移動体通信のように情報伝送を行う場合、基地局装置から送信される信号は帯域幅を有する変調信号(以下、帯域信号と呼称する)である。帯域信号電力は帯域内の積分電力である。しかし、一般的に、測定精度を一定とした場合、広帯域信号であればあるほど測定に時間を要する。   When information is transmitted as in mobile communication, a signal transmitted from a base station device is a modulated signal having a bandwidth (hereinafter, referred to as a band signal). The band signal power is the integrated power in the band. However, in general, when the measurement accuracy is fixed, the wider the broadband signal, the longer the time required for the measurement.

東陽テクニカ、“OTA測定システム(電波暗室)”、[online]、東陽テクニカ、[平成30年8月2日検索]、インターネット〈URL:http://www.toyo.co.jp/emc/products/detail/id=1754〉Toyo Technica, "OTA Measurement System (Anechoic Chamber)", [online], Toyo Technica, [Search August 2, 2018], Internet <URL: http://www.toyo.co.jp/emc/products / detail / id = 1754>

従来のOTA電力測定システム900によると、全放射電力を測定する場合、送信アンテナ92を中心とする球面上の複数の測定点のそれぞれで放射電力を測定する必要がある。回転台96が連続回転する場合、広帯域信号の積分電力の測定に長い時間を要するので、連続回転速度を低下させる必要がある。また、測定精度を確保するため、球面上の多数の測定点で測定する必要があるが、ステップ回転での測定は球面上をスキャンするのに必要な時間が長くなるため現実的ではない。   According to the conventional OTA power measurement system 900, when measuring the total radiated power, it is necessary to measure the radiated power at each of a plurality of measurement points on a spherical surface around the transmission antenna 92. When the turntable 96 rotates continuously, it takes a long time to measure the integrated power of the broadband signal, so that it is necessary to reduce the continuous rotation speed. Further, in order to ensure the measurement accuracy, it is necessary to perform measurement at a large number of measurement points on the spherical surface. However, the measurement by the step rotation is not realistic because the time required for scanning on the spherical surface becomes long.

そこで本発明は、短時間で効率的に且つ高精度に全放射電力を推定できる放射電力推定技術を提供することを目的とする。   Therefore, an object of the present invention is to provide a radiation power estimation technique that can efficiently and accurately estimate the total radiation power in a short time.

本発明の放射電力推定方法は、基地局装置と、基地局装置に接続されている送信アンテナと、送信アンテナを回転させる回転台と、送信アンテナから到来する電波を受信する受信アンテナと、受信した電波の電力を測定する電力測定器とを含む測定システムにおいて送信アンテナの全放射電力を推定する放射電力推定方法であって、電力測定器が、回転台が連続回転する間に、予め定められた角度標本のそれぞれにおいて、送信アンテナが送信し且つ受信アンテナが受信した信号の帯域内の一部での電力を測定する第1ステップと、電力測定器が、電力の最大値に対する各角度標本で得られた電力の比が予め定めた閾値以上である角度標本を特定する第2ステップと、電力測定器が、特定された角度標本で、信号の帯域の全体での電力を測定する第3ステップと、第3ステップで得られた電力から全放射電力を推定する第4ステップを有する。   The method of estimating radiated power according to the present invention includes a base station apparatus, a transmitting antenna connected to the base station apparatus, a turntable for rotating the transmitting antenna, a receiving antenna for receiving a radio wave coming from the transmitting antenna, A radiation power estimation method for estimating the total radiation power of a transmitting antenna in a measurement system including a power measurement device for measuring electric power of a radio wave, wherein the power measurement device is a predetermined method while the turntable continuously rotates. A first step of measuring the power in a portion of the band of the signal transmitted by the transmitting antenna and received by the receiving antenna at each of the angular samples; A second step of identifying an angular sample whose ratio of the determined power is equal to or greater than a predetermined threshold; and a power measuring device measuring the power of the entire signal band with the determined angle sample. That has a third step, a fourth step of estimating the total radiated power from the power obtained in the third step.

本発明によると、短時間で効率的に且つ高精度に全放射電力を推定できる。   According to the present invention, it is possible to efficiently and accurately estimate the total radiation power in a short time.

測定システムの構成例を示す図。FIG. 2 is a diagram illustrating a configuration example of a measurement system. 極角θと方位角φの定義を説明する図。The figure explaining the definition of polar angle (theta) and azimuth (phi). 基地局装置から放射されるEIRPの角度分布の一例を示す図。The figure which shows an example of the angular distribution of EIRP radiated from a base station apparatus. 実施形態における処理フロー図。FIG. 4 is a processing flowchart in the embodiment.

図面を参照して本発明の実施形態を説明する。   An embodiment of the present invention will be described with reference to the drawings.

<実施形態1>
以下、実施形態1の全放射電力推定方法について説明する。実施形態1の放射電力推定方法は、図1に示す従来のOTA電力測定システム900において、後述する手順で全方向における全放射電力(Total Radiated Power: TRP)を推定する方法である。
<First embodiment>
Hereinafter, the total radiation power estimation method of the first embodiment will be described. The radiated power estimation method of the first embodiment is a method of estimating total radiated power (Total Radiated Power: TRP) in all directions in the conventional OTA power measurement system 900 shown in FIG.

一般的に、TRPは、式(1)で定義される。

Figure 2020024165
Generally, TRP is defined by equation (1).
Figure 2020024165

EIRP(θ,φ)は、等価等方輻射電力(Effective Isotropic Radiated Power)であり、送信電力Ptについて、アンテナの指向性が等方性であるとき、送信源から距離rにおける放射電力密度がPt/4πr2となることに基づき定義されたものである。EIRP(θ,φ)は、θ,φ方向の電界成分を測定することで得られるEIRPθ(θ,φ)およびEIRPφ(θ,φ)を用いて式(2)で表される。

Figure 2020024165
EIRP (θ, φ) is an equivalent isotropic radiated power (Effective Isotropic Radiated Power), and for the transmission power Pt, when the directivity of the antenna is isotropic, the radiation power density at a distance r from the transmission source is Pt / 4πr 2 is defined. EIRP (θ, φ) is expressed by equation (2) using EIRP θ (θ, φ) and EIRP φ (θ, φ) obtained by measuring electric field components in the θ, φ directions.
Figure 2020024165

全放射電力の評価には、全ての方向に関する、すなわち図2に示す球面座標系の極角θおよび方位角φに関するEIRPの和を求める。実際の測定では離散的な測定点(角度標本)でEIRPを求めるから、全放射電力TRPは、θおよびφの方向の分割数をそれぞれNθおよびNφとすると、式(3)で表される。ここで、θi=(i-1)Δθ,φj=(j-1)Δφ,Δθ=π/Nθ,Δφ=2π/Nφである。このため、角度標本の総数NはN=NθNφである。

Figure 2020024165
In the evaluation of the total radiated power, the sum of EIRP in all directions, that is, the polar angle θ and the azimuth angle φ in the spherical coordinate system shown in FIG. 2 is obtained. Since the actual measurement seeking EIRP at discrete measuring points (angles sample), total radiated power TRP is, theta and phi direction of the division number of each When N theta and N phi, is expressed by equation (3) You. Here, θ i = (i−1) Δθ, φ j = (j−1) Δφ, Δθ = π / N θ , and Δφ = 2π / N φ . For this reason, the total number N of angle samples is N = N θ N φ .
Figure 2020024165

また、θおよびφの回転角度を得るために回転台96は2軸の回転機構を備える。このような回転機構は周知であるから説明を省略する。各軸について連続回転とステップ回転が可能である。上述のとおり、連続回転は、回転を停止させずに一定の速度で連続的に回転する回転方法であり、ステップ回転は、角度標本ごとで回転を一時的に止める回転方法である。つまり、1回転に費やす時間は連続回転よりもステップ回転の方が長い。   In addition, the turntable 96 includes a two-axis rotation mechanism to obtain the rotation angles θ and φ. Such a rotating mechanism is well-known, and thus description thereof is omitted. Continuous rotation and step rotation are possible for each axis. As described above, continuous rotation is a rotation method in which rotation is continuously stopped at a constant speed without stopping rotation, and step rotation is a rotation method in which rotation is temporarily stopped for each angle sample. That is, the time required for one rotation is longer in the step rotation than in the continuous rotation.

各角度標本において電力測定を行う時、電力測定には所定の時間が必要となるが、この時間は測定信号種別や測定精度によって異なり、広帯域信号になるほど、また高い精度であるほど長い測定時間を要する。具体的には、電力測定器95で帯域信号を測定する場合、精度を確保するため分解能帯域幅(RBW;resolution bandwidth)の設定を適切に行うことが重要である。任意のRBWを設定でき、RBWを小さくするほど周波数分解能が向上し、スペクトラムの細部をより忠実に測定できる。また、RBWを小さくするとノイズのパワーも減るのでノイズレベルが下がりダイナミックレンジが向上する。すなわち、小さい電力まで精度良く測定できる。しかし、RBWを小さくすると応答が遅くなるため、緩やかに周波数掃引しなければならず、このため測定に時間がかかる。つまり、測定信号が広帯域信号の場合、精度を上げるためにRBWを小さくすると、長い測定時間が必要である。   When power measurement is performed on each angle sample, a predetermined time is required for power measurement.This time differs depending on the type of measurement signal and measurement accuracy, and the longer the measurement time becomes, the wider the signal becomes and the higher the accuracy becomes. It costs. Specifically, when measuring the band signal with the power measuring device 95, it is important to appropriately set a resolution bandwidth (RBW) in order to ensure accuracy. Arbitrary RBW can be set, and the smaller the RBW, the higher the frequency resolution is and the more detail in the spectrum can be measured more faithfully. Also, when the RBW is reduced, the noise power is also reduced, so that the noise level is reduced and the dynamic range is improved. That is, even small power can be measured with high accuracy. However, if the RBW is reduced, the response becomes slow, so that the frequency must be gently swept, and it takes a long time for the measurement. That is, when the measurement signal is a wideband signal, a long measurement time is required if the RBW is reduced to improve the accuracy.

さらに、測定時間は回転台96の動作の影響も受ける。測定時間の短縮のため一回転に必要な時間が短い連続回転とした場合、或る角度標本での電力測定は、回転台96が次の角度に到達する前に完了しなければならない。完了できない場合、当該角度標本における測定電力は正確でないため、全放射電力推定に大きな誤差が生じる。他方、連続回転の回転速度を下げる、または、ステップ回転を採用する場合、両方とも測定に要する時間が長くなる。ステップ回転を採用した場合、或る角度標本で電力測定を完了してから回転台96を次の角度標本に回転させることによって、どの角度標本においても受信電力を正確に測定できる。しかし、一般的に、ステップ回転の場合、角度標本の数が増えるほどTRP測定精度は向上するが、測定時間は角度標本の数に比例して増加する。   Further, the measurement time is affected by the operation of the turntable 96. In the case of a continuous rotation in which the time required for one rotation is short in order to reduce the measurement time, the power measurement at a certain angle sample must be completed before the turntable 96 reaches the next angle. If it cannot be completed, the measured power at the angle sample is not accurate, and a large error occurs in the total radiation power estimation. On the other hand, when the rotation speed of the continuous rotation is reduced or when the step rotation is adopted, the time required for the measurement becomes longer in both cases. When the step rotation is adopted, the received power can be accurately measured at any angle sample by rotating the turntable 96 to the next angle sample after completing the power measurement at a certain angle sample. However, in general, in the case of the step rotation, as the number of angle samples increases, the TRP measurement accuracy improves, but the measurement time increases in proportion to the number of angle samples.

ここで、図3に実際の基地局装置から放射されるEIRPの角度分布の一例を示す。一般的に、基地局装置91の送信アンテナ92のメインローブは、エリアの方向に放射電力が最大となるように設計されるので、EIRPの角度分布は特定方向で最大となる。その他の方向ではサイドローブによる電力放射があるが、サイドローブの放射電力はメインローブの放射電力より小さい。   Here, FIG. 3 shows an example of an angular distribution of EIRP radiated from an actual base station apparatus. In general, the main lobe of the transmitting antenna 92 of the base station device 91 is designed so that the radiated power becomes maximum in the direction of the area, so that the angular distribution of EIRP becomes maximum in a specific direction. In the other direction, there is power radiation by the side lobe, but the radiation power of the side lobe is smaller than the radiation power of the main lobe.

表1は、異なる放射パターンにおける、各角度標本におけるEIRPと最大EIRPとの比が閾値以上となる角度標本の数の角度標本の総数に対する割合(測定標本率)とその際の測定誤差を示している。誤差の基準は全ての角度標本から求めたTPRである。表1から、閾値が大きくなるほど(つまり閾値を最大EIRPに近づけるほど)測定標本率が小さくなるとともに測定誤差が大きくなり、閾値が小さくなるほど(つまり閾値を最大EIRPから遠ざけるほど)測定標本率が大きくなるとともに測定誤差が小さくなることがわかる。閾値が例えば−10dBの時、測定標本率は基地局装置Aでは7%であり基地局装置Bでは3%であるが、測定誤差がそれぞれ−0.8dB,−1.2dBである(つまり、閾値が−10dBの時、測定標本率は十分に小さいが測定誤差が大きい)のに対して、閾値が例えば−40dBの時、測定誤差は基地局装置A,Bでは0dBであるが、測定標本率が基地局装置Aでは91%であり、基地局装置Bでは81%である(つまり、閾値が−40dBの時、測定誤差は十分に小さいが測定標本率が大きい)。したがって、短時間で効率的に且つ高精度に全放射電力を推定するためには、できるだけ小さい測定標本率でできるだけ小さい測定誤差を達成できる閾値を設定するのが良い。閾値は、測定システム900の構成や測定条件(例えば要求される精度)などによって変更できるが、好ましくは、測定標本率が50%以下であり且つ測定誤差が−0.3dB以上であることを満足する値として設定されるのが好ましい。表1からは、閾値は、−15dB以下かつ−30dB以上の所定の値であるのが好ましい。閾値が−20dB程度であれば誤差は非常に小さく、且つ、測定標本率が20%(全体の1/5程度)になっている。このように、閾値は、いくつかのシミュレーションモデルにおける測定標本率と測定誤差とのトレードオフに基づいて事前に決定される。なお、シミュレーションモデルは、実際の測定システムを前提に作られたものでなくてもよい。

Figure 2020024165
Table 1 shows the ratio (measurement sample rate) of the number of angle samples in which the ratio of EIRP to the maximum EIRP in each angle sample is equal to or larger than the threshold to the total number of angle samples (measurement sample rate) and the measurement error at that time. I have. The error criterion is the TPR obtained from all angle samples. From Table 1, it can be seen that the larger the threshold (ie, the closer the threshold is to the maximum EIRP), the smaller the measurement sample rate and the greater the measurement error, and the smaller the threshold (ie, the further the threshold is away from the maximum EIRP), the greater the measurement sample rate. It can be seen that the measurement error becomes smaller as the distance increases. When the threshold value is, for example, −10 dB, the measurement sample rate is 7% in the base station device A and 3% in the base station device B, but the measurement errors are −0.8 dB and −1.2 dB, respectively (that is, When the threshold value is -10 dB, the measurement sample rate is sufficiently small but the measurement error is large. On the other hand, when the threshold value is -40 dB, the measurement error is 0 dB in the base station apparatuses A and B. The rate is 91% in the base station apparatus A and 81% in the base station apparatus B (that is, when the threshold value is −40 dB, the measurement error is sufficiently small but the measurement sample rate is large). Therefore, in order to estimate the total radiated power efficiently and with high accuracy in a short time, it is preferable to set a threshold value that can achieve the smallest possible measurement error with the smallest possible sample rate. The threshold value can be changed depending on the configuration of the measurement system 900, measurement conditions (for example, required accuracy), etc., but preferably, the measurement sample rate is 50% or less and the measurement error is -0.3 dB or more. It is preferably set as a value to be set. From Table 1, it is preferable that the threshold value is a predetermined value of -15 dB or less and -30 dB or more. If the threshold value is about -20 dB, the error is very small, and the measurement sample rate is 20% (about 1/5 of the whole). As described above, the threshold is determined in advance based on a trade-off between the measurement sample rate and the measurement error in some simulation models. Note that the simulation model does not have to be created based on an actual measurement system.
Figure 2020024165

このような特徴に鑑みて、実施形態1では、まず、電力測定器95が、回転台96が一定速度で連続回転する間に、予め定められた角度標本のそれぞれにおいて、送信アンテナ92が送信し且つ受信アンテナ93が受信した信号の帯域内の一部での受信電力EIRP(θ,φ)を測定する(ステップS1)。この時の角度分解能は測定精度に影響するので、比較的小さい分解能であることが好ましい。基地局装置91からの送信信号が帯域信号である場合、連続回転では上述したように全帯域の信号電力を測定することができない場合があるため、信号帯域内の一部の帯域のみの電力を測定する。電力を測定できなかった場合には、例えば測定帯域幅を半分に更新し、電力測定器95が再度、連続回転で各角度標本の受信電力を測定する。このプロセスを一回転分の電力測定結果を得るまで実行する。   In view of such a feature, in the first embodiment, first, the power measuring device 95 transmits the transmission antenna 92 at each of the predetermined angle samples while the turntable 96 continuously rotates at a constant speed. In addition, the reception power EIRP (θ, φ) in a part of the band of the signal received by the reception antenna 93 is measured (step S1). Since the angular resolution at this time affects measurement accuracy, it is preferable that the resolution be relatively small. When the transmission signal from the base station apparatus 91 is a band signal, the signal power of the entire band cannot be measured in the continuous rotation as described above, so that the power of only a part of the signal band is reduced. Measure. If the power cannot be measured, for example, the measurement bandwidth is updated to half, and the power measuring device 95 again measures the received power of each angular sample by continuous rotation. This process is performed until the power measurement result for one rotation is obtained.

次に、電力測定器95は、連続回転で得られたEIRP(θ,φ)の最大値を求め、EIRP(θ,φ)の最大値に対する各角度標本のEIRP(θ,φ)の比を計算し、比が予め設定した閾値以上である角度標本を特定する(ステップS2)。ここでは、特定された角度標本の座標を(θij),(i,j)∈{(ap,bq)|ap∈{a1,a2,…,an},bq∈{b1,b2,…,bm}},ak∈{1,2,…,Nθ},bh∈{1,2,…,Nφ},k∈{1,2,…,n},h∈{1,2,…,m}と書くことにする。ただし、(i,j)は集合(ap,bq)の全ての元を亘るとは限らない。 Next, the power measuring device 95 obtains the maximum value of EIRP (θ, φ) obtained by continuous rotation, and calculates the ratio of the EIRP (θ, φ) of each angle sample to the maximum value of EIRP (θ, φ). Calculate and specify an angle sample whose ratio is equal to or greater than a preset threshold (step S2). Here, the coordinates of the specified angle sample are represented by (θ i , φ j ), (i, j) ∈ {(a p , b q ) | a p ∈ {a 1 , a 2 , ..., a n }, b q ∈ {b 1 , b 2 , ..., b m }}, ak ∈ {1,2, ..., N θ }, b h ∈ {1,2, ..., N φ }, k∈ {1, 2,…, n}, h∈ {1,2,…, m}. However, (i, j) does not necessarily cover all elements of the set (a p , b q ).

そして、電力測定器95は、回転台96のステップ回転において、ステップS2の処理で特定した角度標本のそれぞれにおいて信号帯域の全体での電力を測定する(ステップS3)。この処理で得られた各角度標本での電力をEIRP(θij),(i,j)∈{(ap,bq)|ap∈{a1,a2,…,an},bq∈{b1,b2,…,bm}},ak∈{1,2,…,Nθ},bh∈{1,2,…,Nφ},k∈{1,2,…,n},h∈{1,2,…,m}とする。 Then, in the step rotation of the turntable 96, the power measuring device 95 measures the power of the entire signal band in each of the angle samples specified in the process of step S2 (step S3). The power at each angle sample obtained by this processing is calculated as EIRP (θ i , φ j ), (i, j) ∈ {(a p , b q ) | a p ∈ {a 1 , a 2 , ..., a n }, b q ∈ {b 1 , b 2 , ..., b m }}, a k ∈ {1, 2, ..., N θ }, b h ∈ {1, 2, ..., N φ }, k∈ {1, 2, ..., n}, h} {1, 2, ..., m}.

最後に、電力測定器95は、ステップS3の処理で求めた各角度標本での全帯域電力測定結果EIRP(θij),(i,j)∈{(ap,bq)|ap∈{a1,a2,…,an},bq∈{b1,b2,…,bm}},ak∈{1,2,…,Nθ},bh∈{1,2,…,Nφ},k∈{1,2,…,n},h∈{1,2,…,m}と式(4)を用いてTRPを求める(ステップS4)。ただし、Δθ=π/Nθ,Δφ=2π/Nφである。

Figure 2020024165
Finally, the power measuring device 95 obtains the EIRP (θ i , φ j ), (i, j) ∈ {(a p , b q ) | a p ∈ {a 1 , a 2 , ..., a n }, b q ∈ {b 1 , b 2 , ..., b m }}, ak ∈ {1,2, ..., N θ }, b h ∈ A TRP is obtained using {1, 2,..., N φ }, k∈ {1, 2,..., N}, h∈ {1, 2,..., M} and equation (4) (step S4). Here, Δθ = π / N θ and Δφ = 2π / N φ .
Figure 2020024165

放射電力は帯域によらず送信アンテナ92と受信アンテナ93との離隔距離に応じた一定の減衰を受けるので、帯域信号の角度依存性と、帯域信号内の一部の帯域信号の角度依存性は等しい。つまり、送信アンテナ92による放射電力の角度分布は帯域内の一部の帯域の放射電力の角度分布と等しく、両者において最大EIRPに対する各角度標本のEIRPの比も等しい。また、一定強度以上のEIRPを測定すれば精度の高いTRPを推定できるため、精度を保ちつつ角度標本数の削減による測定時間の短縮が可能となる。   Since the radiated power receives a constant attenuation according to the separation distance between the transmitting antenna 92 and the receiving antenna 93 regardless of the band, the angle dependence of the band signal and the angle dependence of some band signals in the band signal are: equal. That is, the angular distribution of the radiated power by the transmitting antenna 92 is equal to the angular distribution of the radiated power in some of the bands, and the ratio of the EIRP of each angular sample to the maximum EIRP is also equal in both cases. In addition, if EIRP having a certain intensity or higher is measured, highly accurate TRP can be estimated. Therefore, measurement time can be reduced by reducing the number of angle samples while maintaining accuracy.

実施形態1の推定法によると、連続回転で帯域内の一部の放射電力分布を短時間で測定し、TRPへの寄与が大きい角度標本を選択し、当該角度標本での全帯域の放射電力をステップ回転で正確に取得することによって短時間で精度の高いTRP推定が可能である。   According to the estimation method of the first embodiment, the radiant power distribution in a part of the band is measured in a short time by continuous rotation, an angular sample having a large contribution to TRP is selected, and the radiant power of the entire band in the angular sample is selected. TRP estimation can be performed in a short time and with high accuracy by accurately acquiring by the step rotation.

<実施形態2>
実施形態2では、ステップS1の処理にて、基地局装置91からの送信信号が帯域信号である場合、電力測定器95が帯域中心周波数での電力を測定する。この場合、電力測定器95は帯域内電力を積分する必要が無い。また、ピーク電力をサーチし、その電力を測定するから、測定精度が向上するとともに、高ダイナミックレンジの推定を構築できる。特に受信電力が小さい場合に有効である。
<Embodiment 2>
In the second embodiment, when the transmission signal from the base station device 91 is a band signal in the process of step S1, the power measuring device 95 measures the power at the band center frequency. In this case, the power measuring device 95 does not need to integrate the in-band power. Further, since the peak power is searched and the power is measured, the measurement accuracy is improved, and a high dynamic range can be estimated. This is particularly effective when the reception power is small.

なお、各実施形態において閾値を−20dBに設定することによって、角度標本数を1/5以下にでき、且つ、測定時間を1/5以下にできる。   In each embodiment, by setting the threshold value to -20 dB, the number of angle samples can be reduced to 1/5 or less, and the measurement time can be reduced to 1/5 or less.

<補遺>
明細書と特許請求の範囲において、処理手順、シーケンス、フローチャートなどは、矛盾の無い限り、順序を入れ替えてもよい。
<Addendum>
In the specification and the claims, the order of processing procedures, sequences, flowcharts, and the like may be changed as long as there is no inconsistency.

明細書と特許請求の範囲において、入力あるいは出力された情報等は、特定の場所(例えば、メモリ)に保存されてもよいし、管理テーブルで管理されてもよい。入力あるいは出力される情報等は、上書き、更新、または追記され得る。出力された情報等は削除されてもよい。入力された情報等は必要に応じて他の装置へ送信されてもよい。   In the description and the claims, the input or output information or the like may be stored in a specific place (for example, a memory) or may be managed in a management table. Information to be input or output can be overwritten, updated, or added. The output information or the like may be deleted. The input information or the like may be transmitted to another device as needed.

明細書と特許請求の範囲において、判定は、1ビットで表される値(0か1か)によって行われてもよいし、真偽値(Boolean:trueまたはfalse)によって行われてもよいし、数値の比較(例えば、所定の値との比較)によって行われてもよい。   In the description and the claims, the determination may be made by a value represented by 1 bit (0 or 1) or by a Boolean value (Boolean: true or false). , May be performed by comparing numerical values (for example, comparison with a predetermined value).

上述の実施形態において、所定の情報の通知(例えば、「Xであること」の通知)は、明示的に行うことに限られず、暗黙的(例えば、当該所定の情報の通知を行わない)に行われてもよい。   In the above-described embodiment, the notification of the predetermined information (for example, the notification of “X”) is not limited to being performed explicitly, and is implicit (for example, the notification of the predetermined information is not performed). May be performed.

明細書と特許請求の範囲において、「システム」という用語と「ネットワーク」という用語は、互換的に使用され得る。   In the description and the claims, the terms "system" and "network" may be used interchangeably.

明細書と特許請求の範囲では、「接続された」という用語とこのあらゆる語形変形は、2又はそれ以上の要素間の直接的又は間接的な接続を意味し、互いに「接続」された2つの要素の間に1又はそれ以上の中間要素が存在することを含むことができる。要素と要素との接続は、物理的接続であっても、論理的接続であっても、或いはこれらの組み合わせであってもよい。明細書と特許請求の範囲で使用する場合、2つの要素は、1又はそれ以上の電線、ケーブルおよび/またはプリント電気接続を使用することによって、並びにいくつかの非限定的かつ非包括的な例として、無線周波数領域、マイクロ波領域及び光(可視及び不可視の両方)領域の波長を有する電磁エネルギーなどの電磁エネルギーを使用することによって、互いに「接続」されると考えることができる。   In the description and in the claims, the term "connected" and any variants thereof mean a direct or indirect connection between two or more elements, It may include the presence of one or more intermediate elements between the elements. The connection between elements may be a physical connection, a logical connection, or a combination thereof. As used in the specification and the claims, two elements may involve the use of one or more electrical wires, cables and / or printed electrical connections, as well as some non-limiting and non-exhaustive examples. As such, they can be considered "connected" to each other by using electromagnetic energy, such as electromagnetic energy having wavelengths in the radio frequency, microwave, and light (both visible and invisible) regions.

明細書と特許請求の範囲では、序数詞(例えば、接頭辞「第」に漢数詞または算用数字を組み合わせた「第○」)は、特段の断りが無い限り、助数詞の定義にもかかわらず、序数詞で修飾されるまたは助数詞と結合する要素を当該要素の順序または当該要素の量で限定することを意図しない。助数詞の使用は、特段の断りが無い限り、単に、2つ以上の要素を互いに区別する便利な表現方法として使用される。したがって、例えば語句「第1のX」と語句「第2のX」は、2つのXを区別するための表現であり、Xの総数が2であることを意味するものでは必ずしもなく、あるいは、第1のXが第2のXに先行しなければならないことを意味するものでは必ずしもない。   In the description and the claims, ordinal numbers (for example, the prefix "No." combined with a Chinese number or an arithmetic digit "No. ○"), unless otherwise noted, It is not intended that the elements modified by ordinal or combined with the classifier be limited by the order of the elements or the amount of the elements. The use of classifiers is used merely as a convenient way of distinguishing two or more elements from each other, unless otherwise specified. Therefore, for example, the phrase “first X” and the phrase “second X” are expressions for distinguishing two Xs, and do not necessarily mean that the total number of Xs is 2, or It does not necessarily mean that the first X must precede the second X.

明細書と特許請求の範囲では、用語「含む」とその語形変化は非排他的表現として使用されている。例えば、「XはAとBを含む」という文は、XがAとB以外の構成要素(例えばC)を含むことを否定しない。また、明細書と特許請求の範囲において或る文が用語「含む」またはその語形変化が否定辞と結合した語句を含む場合、当該文は用語「含む」またはその語形変化の目的語について言及するだけである。したがって、例えば「XはAとBを含まない」という文は、XがAとB以外の構成要素を含む可能性を認めている。さらに、明細書あるいは特許請求の範囲において使用されている用語「または」は排他的論理和ではないことが意図される。   In the description and claims, the term "comprise" and its conjugations are used as non-exclusive expressions. For example, the sentence "X includes A and B" does not deny that X includes a component other than A and B (for example, C). In addition, in the specification and claims, when a sentence includes the term “include” or its inflection includes a word combined with a negative word, the sentence refers to the term “include” or the object of the inflection. Only. Thus, for example, the sentence "X does not include A and B" acknowledges that X may include components other than A and B. Further, the term "or" as used in the description or the claims is not intended to be an exclusive or.

以上、本発明の実施形態について説明したが、本発明はこれらの実施形態に限定されるものではない。本発明の要旨を逸脱しない範囲において種々の変更と変形が許される。選択され且つ説明された実施形態は、本発明の原理およびその実際的応用を解説するためのものである。本発明は様々な変更あるいは変形を伴って様々な実施形態として使用され、様々な変更あるいは変形は期待される用途に応じて決定される。そのような変更および変形のすべては、添付の特許請求の範囲によって規定される本発明の範囲に含まれることが意図されており、公平、適法および公正に与えられる広さに従って解釈される場合、同じ保護が与えられることが意図されている。   The embodiments of the present invention have been described above, but the present invention is not limited to these embodiments. Various changes and modifications are allowed without departing from the spirit of the present invention. The embodiments selected and described are illustrative of the principles of the invention and its practical application. The invention may be used in various embodiments with various modifications or variations, which will be determined according to the expected application. All such changes and modifications are intended to be included within the scope of the invention as defined by the appended claims, and should be construed in accordance with the breadth given fairly, lawfully and fairly. It is intended that the same protection be provided.

Claims (4)

基地局装置と、当該基地局装置に接続されている送信アンテナと、当該送信アンテナを回転させる回転台と、当該送信アンテナから到来する電波を受信する受信アンテナと、受信した当該電波の電力を測定する電力測定器とを含む測定システムにおいて当該送信アンテナの全放射電力を推定する放射電力推定方法であって、
前記電力測定器が、前記回転台が連続回転する間に、予め定められた角度標本のそれぞれにおいて、前記送信アンテナが送信し且つ前記受信アンテナが受信した信号の帯域内の一部での電力を測定する第1ステップと、
前記電力測定器が、前記電力の最大値に対する各前記角度標本で得られた前記電力の比が予め定めた閾値以上である前記角度標本を特定する第2ステップと、
前記電力測定器が、特定された前記角度標本で、前記信号の帯域の全体での電力を測定する第3ステップと
前記第3ステップで得られた前記電力から全放射電力を推定する第4ステップと
を有する放射電力推定方法。
A base station device, a transmitting antenna connected to the base station device, a turntable for rotating the transmitting antenna, a receiving antenna for receiving a radio wave coming from the transmitting antenna, and measuring the power of the received radio wave A radiation power estimation method for estimating the total radiation power of the transmission antenna in a measurement system including a power measuring device that performs
The power meter measures the power in a part of the band of the signal transmitted by the transmitting antenna and received by the receiving antenna in each of the predetermined angle samples while the turntable continuously rotates. A first step of measuring;
A second step in which the power measuring device specifies the angle sample in which the ratio of the power obtained in each of the angle samples to the maximum value of the power is equal to or greater than a predetermined threshold value;
A third step of measuring the power in the entire band of the signal with the specified angular sample, and a fourth step of estimating a total radiated power from the power obtained in the third step; A radiation power estimation method comprising:
請求項1に記載の放射電力推定方法において、
前記第1ステップにおいて、前記一部は中心周波数である
ことを特徴とする放射電力推定方法。
The radiation power estimation method according to claim 1,
In the first step, the part is a center frequency.
請求項1または請求項2に記載の放射電力推定方法において、
前記閾値は、事前のシミュレーションモデルにおいて、各角度標本における等価等方輻射電力と最大等価等方輻射電力との比が閾値以上となる角度標本の数の角度標本の総数に対する割合である測定標本率と、全ての角度標本から求めた全放射電力に対する測定誤差と、のトレードオフに基づいて予め決定されている
ことを特徴とする放射電力推定方法。
In the radiation power estimation method according to claim 1 or 2,
The threshold is a ratio of the number of angle samples at which the ratio between the equivalent isotropic radiation power and the maximum equivalent isotropic radiation power at each angle sample is equal to or greater than the threshold value to the total number of angle samples in the prior simulation model. A radiation error estimating method, which is determined in advance based on a trade-off between a measurement error with respect to total radiation power obtained from all angle samples and a measurement error.
請求項1または請求項2に記載の放射電力推定方法において、
前記閾値は、−15dB以下かつ−30dB以上の所定の値である
ことを特徴とする放射電力推定方法。
In the radiation power estimation method according to claim 1 or 2,
The radiation power estimation method, wherein the threshold value is a predetermined value of -15 dB or less and -30 dB or more.
JP2018149490A 2018-08-08 2018-08-08 Radiation power estimation method Active JP7016303B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2018149490A JP7016303B2 (en) 2018-08-08 2018-08-08 Radiation power estimation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2018149490A JP7016303B2 (en) 2018-08-08 2018-08-08 Radiation power estimation method

Publications (2)

Publication Number Publication Date
JP2020024165A true JP2020024165A (en) 2020-02-13
JP7016303B2 JP7016303B2 (en) 2022-02-04

Family

ID=69618545

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2018149490A Active JP7016303B2 (en) 2018-08-08 2018-08-08 Radiation power estimation method

Country Status (1)

Country Link
JP (1) JP7016303B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112881791A (en) * 2021-01-19 2021-06-01 中国电子科技集团公司第二十九研究所 Method for calculating transmitting power of unknown ground radiation source through pitch angle and azimuth angle
CN116106644A (en) * 2023-04-10 2023-05-12 中国人民解放军63921部队 Antenna far-field radiation power fitting method, system and medium considering angle error
WO2023103798A1 (en) * 2021-12-10 2023-06-15 中兴通讯股份有限公司 Power measurement method and apparatus, and storage medium and program product
CN116366175A (en) * 2023-05-26 2023-06-30 北京星河亮点技术股份有限公司 Power measurement method, device, system, electronic equipment and storage medium

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005333451A (en) * 2004-05-20 2005-12-02 Matsushita Electric Ind Co Ltd Antenna characteristic evaluation system
US20060017630A1 (en) * 2000-03-31 2006-01-26 Per-Simon Kildal Method and an apparatus for measuring the performance of antennas, mobile phones and other wireless terminals
JP2006275967A (en) * 2005-03-30 2006-10-12 Kyocera Corp Antenna characteristics evaluation method and measuring device
WO2009041513A1 (en) * 2007-09-28 2009-04-02 Anritsu Corporation Radiated power measuring method, coupler for radiate power measurement, and radiated power measuring device
JP2010502997A (en) * 2006-09-08 2010-01-28 クゥアルコム・インコーポレイテッド Radiation performance of radio equipment
JP2011019031A (en) * 2009-07-08 2011-01-27 Nec Saitama Ltd Method and system for measuring total radiation sensitivity
JP2012042242A (en) * 2010-08-16 2012-03-01 Fujitsu Ltd Antenna characteristic measurement system and antenna characteristic measurement method
JP2013083455A (en) * 2011-10-06 2013-05-09 Fujitsu Ltd Radio wave measuring apparatus and radio wave measuring method
CN103873161A (en) * 2012-12-17 2014-06-18 上海新蓦尔通信技术有限公司 Uniform testing and identification method for completeness of wireless communication product

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20060017630A1 (en) * 2000-03-31 2006-01-26 Per-Simon Kildal Method and an apparatus for measuring the performance of antennas, mobile phones and other wireless terminals
JP2005333451A (en) * 2004-05-20 2005-12-02 Matsushita Electric Ind Co Ltd Antenna characteristic evaluation system
JP2006275967A (en) * 2005-03-30 2006-10-12 Kyocera Corp Antenna characteristics evaluation method and measuring device
JP2010502997A (en) * 2006-09-08 2010-01-28 クゥアルコム・インコーポレイテッド Radiation performance of radio equipment
WO2009041513A1 (en) * 2007-09-28 2009-04-02 Anritsu Corporation Radiated power measuring method, coupler for radiate power measurement, and radiated power measuring device
JP2011019031A (en) * 2009-07-08 2011-01-27 Nec Saitama Ltd Method and system for measuring total radiation sensitivity
JP2012042242A (en) * 2010-08-16 2012-03-01 Fujitsu Ltd Antenna characteristic measurement system and antenna characteristic measurement method
JP2013083455A (en) * 2011-10-06 2013-05-09 Fujitsu Ltd Radio wave measuring apparatus and radio wave measuring method
CN103873161A (en) * 2012-12-17 2014-06-18 上海新蓦尔通信技术有限公司 Uniform testing and identification method for completeness of wireless communication product

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112881791A (en) * 2021-01-19 2021-06-01 中国电子科技集团公司第二十九研究所 Method for calculating transmitting power of unknown ground radiation source through pitch angle and azimuth angle
CN112881791B (en) * 2021-01-19 2023-05-09 中国电子科技集团公司第二十九研究所 Method for calculating unknown ground radiation source transmitting power through pitch angle and azimuth angle
WO2023103798A1 (en) * 2021-12-10 2023-06-15 中兴通讯股份有限公司 Power measurement method and apparatus, and storage medium and program product
CN116106644A (en) * 2023-04-10 2023-05-12 中国人民解放军63921部队 Antenna far-field radiation power fitting method, system and medium considering angle error
CN116106644B (en) * 2023-04-10 2023-06-27 中国人民解放军63921部队 Antenna far-field radiation power fitting method, system and medium considering angle error
CN116366175A (en) * 2023-05-26 2023-06-30 北京星河亮点技术股份有限公司 Power measurement method, device, system, electronic equipment and storage medium

Also Published As

Publication number Publication date
JP7016303B2 (en) 2022-02-04

Similar Documents

Publication Publication Date Title
JP7016303B2 (en) Radiation power estimation method
US11750303B2 (en) Compact system for characterizing a device under test (DUT) having integrated antenna array
US9699678B2 (en) Plane wave generation within a small volume of space for evaluation of wireless devices
WO2019214570A1 (en) Method, apparatus and system for measuring total radiated power of array antenna
US20190229817A1 (en) Reduced Grid For Measurement Of Total Radiated Power
US20200213016A1 (en) System and method for obtaining far field radiated power with multiple radiated power measurements in middle field range
US11791564B2 (en) Near-field antenna for remote radio control of an antenna array
US10393786B2 (en) Test system and method for over the air (OTA) measurements based on randomly adjusted measurement points
TWI751645B (en) Rapid over-the-air production line test platform
WO2020020251A1 (en) Electromagnetic radiation control method and related device
KR100574226B1 (en) Method for measuring the electromagnetic radiation pattern and gain of a radiator using a TEM waveguide
US11372037B2 (en) Freespace antenna measurement system
CN107037283A (en) Radiosensitivity method of testing and device under the conditions of reverberation chamber
CN109728864B (en) System loss testing method based on antenna measuring system
Li et al. Total isotropic sensitivity measurement in switched beam antenna systems
Goulianos et al. A novel path-loss model for UWB off-body propagation
CN112213566A (en) Method and system for near-field reconstruction in indirect far-field systems
Vick et al. Investigation of Emission Requirements above 1GHz towards 5G
Santos et al. Shielding effectiveness measurements of coaxial cable and connectors using compact open area test site
Chen et al. Single-frequency multipath diagnosis in an anechoic chamber of a hybrid far-field antenna measurement system
Chen et al. An improved method for free-space antenna-factor measurement by using the MUSIC algorithm
TW202318008A (en) Antenna testing method and system thereof
US20240056201A1 (en) Method and system for evaluating radio performance
FUJII et al. 2-6 Site Validation of the Open-Area Test Site and the Semi-Anechoic Chamber
Van Den Biggelaar et al. Method to experimentally verify far-field conditions in a direct far-field measurement setup

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20210128

TRDD Decision of grant or rejection written
A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20211228

A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20220111

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20220125