JP3462769B2 - Broadband waveguide optical electric field sensor - Google Patents

Broadband waveguide optical electric field sensor

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Publication number
JP3462769B2
JP3462769B2 JP30637398A JP30637398A JP3462769B2 JP 3462769 B2 JP3462769 B2 JP 3462769B2 JP 30637398 A JP30637398 A JP 30637398A JP 30637398 A JP30637398 A JP 30637398A JP 3462769 B2 JP3462769 B2 JP 3462769B2
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JP
Japan
Prior art keywords
electric field
field sensor
optical electric
optical
substrate
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.)
Expired - Fee Related
Application number
JP30637398A
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Japanese (ja)
Other versions
JP2000121682A (en
Inventor
直美 日高
秀晃 菅間
亮 臼井
誠 安田
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.)
Kanagawa Prefecture
Original Assignee
Kanagawa Prefecture
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Priority to JP30637398A priority Critical patent/JP3462769B2/en
Publication of JP2000121682A publication Critical patent/JP2000121682A/en
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Publication of JP3462769B2 publication Critical patent/JP3462769B2/en
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Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、電磁波障害対策
(EMC対策)のための電磁界測定や、情報通信産業に
おける光変調器等として使用するのに好適な広帯域導波
路型光電界センサに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a broadband waveguide type optical electric field sensor suitable for use in electromagnetic field measurement for countermeasures against electromagnetic interference (EMC countermeasures) and as an optical modulator in the information communication industry.

【0002】[0002]

【従来の技術】電子機器は、それ自身から発生する電磁
波によって、他の電子機器に誤作動等の悪影響を及ぼす
ことがある。そのため、各種の規格によって、当該電子
機器が外部に放射する電磁波の許容値並びに当該電子機
器にとって誤作動の原因となる外部からの電磁界放射に
対して、当該電子機器がどの程度まで耐えられるか(イ
ミュニティ試験)についての基準が定められている。
2. Description of the Related Art An electronic device may adversely affect other electronic devices such as malfunction due to electromagnetic waves generated from the electronic device. Therefore, the various standards allow the electronic device to withstand the allowable value of electromagnetic waves radiated by the electronic device to the outside and the electromagnetic field radiation from the outside that causes malfunction of the electronic device. Standards for (immunity test) are defined.

【0003】電子機器がこれらの規格に適合しているか
否かを検査する場合、図6に示すような電波暗室でその
試験が行われる。特に、イミュニティ試験においては電
子機器に照射する電磁界を測定するために光電界センサ
が用いられる。
When inspecting whether or not an electronic device complies with these standards, the test is performed in an anechoic chamber as shown in FIG. Particularly, in the immunity test, an optical electric field sensor is used to measure an electromagnetic field applied to an electronic device.

【0004】上記の光電界センサは、電磁波の強度とそ
の周波数を測定するものであり、図4は、バルク型ポッ
ケルス素子16を用いたものである。この光電界センサ
は、外部との接続に、誘電体である光ファイバ17が用
いられており、電界検出のために最小限必要なアンテナ
20及び電極21以外には金属部分を持っていない。そ
のため、光電界センサは、金属製の同軸線路で外部と接
続されている通常のアンテナに比べ、アンテナ周囲の電
磁界を乱すことが極端に少なく、正確な電磁界の測定が
要求される場合に使用される。なお、図4において18
は偏光子、19は1/4λ板である。
The above optical electric field sensor measures the intensity and frequency of electromagnetic waves, and FIG. 4 uses a bulk type Pockels element 16. This optical electric field sensor uses an optical fiber 17 which is a dielectric for connection to the outside, and has no metal portion other than the antenna 20 and the electrode 21 which are the minimum necessary for electric field detection. Therefore, the optical electric field sensor is extremely less likely to disturb the electromagnetic field around the antenna than an ordinary antenna connected to the outside by a metal coaxial line, and when an accurate electromagnetic field measurement is required. used. In addition, in FIG.
Is a polarizer, and 19 is a quarter-lambda plate.

【0005】ところで、この光電界センサの感度を高め
るためには、電磁波によって光を変調する変調器部分の
構造を最適に設計する必要がある。一般的に、変調器部
分の電極幅を狭くし、電極長を長くすることによってそ
の感度を高めることができる。
In order to increase the sensitivity of this optical electric field sensor, it is necessary to optimally design the structure of the modulator portion that modulates light with electromagnetic waves. In general, the sensitivity can be increased by narrowing the electrode width of the modulator portion and increasing the electrode length.

【0006】図5はバルク型ポッケルス素子の電極長を
30mm、電極間隔を2mmとし、これに長さ243m
m又は126mmのアンテナを取り付けた場合の光電界
センサの特性を示すものであるが、このポッケルス素子
を用いた光電界センサの感度を向上させるためには、ポ
ッケルス素子の電極長を長くするか、或いは、電極間隔
を狭くすることが必要である。しかしながら、電極長を
長くすることにより、センサ周辺の空間電磁界とポッケ
ルス素子中を進行する光との相互の位相の不整合が起こ
る。図4に示すように、電極長30mmの場合、この不
整合が原因で約2GHz以上では感度がなくなる。ま
た、図4のような構造では、光のビーム径を十分に絞る
ことができないことから、電極間隔をこれ以上狭くする
ことができない。そこで、光ファイバーのように10μ
m程度の狭い幅に光を閉じこめて、これを導波させるこ
とのできる光導波路を利用した、導波路型光電界センサ
を用いることにより、この電極幅を限界まで狭めること
ができる。ところが、従来の導波路型電界センサでは、
アンテナが1対のダイポールアンテナであり、かつ、長
さが数センチであるため、高い周波数のマイクロ波の検
出には適さなかった。そこで、これまでより高い周波数
において使用可能な光電界センサの開発が望まれてい
た。
FIG. 5 shows that the bulk Pockels element has an electrode length of 30 mm and an electrode interval of 2 mm, and a length of 243 m.
The characteristics of the optical electric field sensor when an m or 126 mm antenna is attached are shown. In order to improve the sensitivity of the optical electric field sensor using this Pockels element, the electrode length of the Pockels element is increased, or Alternatively, it is necessary to narrow the electrode interval. However, by increasing the electrode length, the mutual phase mismatch between the spatial electromagnetic field around the sensor and the light traveling in the Pockels element occurs. As shown in FIG. 4, when the electrode length is 30 mm, the sensitivity is lost at about 2 GHz or higher due to this mismatch. Further, in the structure as shown in FIG. 4, the beam diameter of light cannot be sufficiently narrowed, so that the electrode interval cannot be further narrowed. So, like optical fiber, 10μ
The electrode width can be narrowed to the limit by using a waveguide type optical electric field sensor that utilizes an optical waveguide capable of confining light in a narrow width of about m and guiding the light. However, in the conventional waveguide type electric field sensor,
Since the antenna is a pair of dipole antennas and its length is several centimeters, it was not suitable for detecting high frequency microwaves. Therefore, it has been desired to develop an optical electric field sensor that can be used at higher frequencies.

【0007】[0007]

【発明が解決しようとする課題】本発明は、上記の課題
の解決を図ったもので、光電界センサの使用可能な周波
数を低周波側に制限することなく、高周波の電磁波を
も、より高感度で測定可能とすることを目的とするもの
であり、また、低周波域からより高周波域に至るまで光
電界センサの感度を均一にすることを目的とするもので
ある。
DISCLOSURE OF THE INVENTION The present invention is intended to solve the above-mentioned problems, and it is possible to obtain a high frequency electromagnetic wave without limiting the usable frequency of the optical electric field sensor to the low frequency side. The purpose is to enable measurement with sensitivity, and the purpose is to make the sensitivity of the optical electric field sensor uniform from a low frequency region to a higher frequency region.

【0008】[0008]

【課題を解決するための手段】すなわち、本発明の広帯
域導波路型光電界センサは、請求項1に記載の通り、基
板の中央に光導波路を設けるとともに、前記光導波路を
中心にそれぞれ長さの異なるダイポールアンテナをアレ
イ状、かつ、前記各ダイポールアンテナの長さ及び隣接
する前記ダイポールアンテナ間の間隔をそれぞれ対数周
期的に配置したことを特徴とする。また、請求項2記載
の広帯域導波路型光電界センサは、請求項1記載の広帯
域導波路型光電界センサにおいて、基板周囲を進む電磁
波の速度と光導波路中を進む光の速度とを一致させるべ
く、基板の周囲に特定の誘電率を有する粉体又は液体か
らなる物質を充填配置したことを特徴とする。
That is, a broadband waveguide type optical electric field sensor according to the present invention has an optical waveguide provided in the center of a substrate and a length centered on the optical waveguide as described in claim 1. Array of different dipole antennas, and the length and adjacency of each dipole antenna
The intervals between the dipole antennas are arranged logarithmically. The broadband waveguide type optical electric field sensor according to claim 2 is the broadband waveguide type optical electric field sensor according to claim 1, wherein the speed of the electromagnetic wave traveling around the substrate and the speed of the light traveling through the optical waveguide are matched. Therefore, it is characterized in that a substance made of powder or liquid having a specific dielectric constant is filled and arranged around the substrate.

【0009】[0009]

【実施例】以下に本発明の実施例について図面に基づき
説明する。図1は本発明センサの実施例を示す斜視図、
図2は本発明の他実施例を示す斜視図、図3は図1に示
す本発明センサの感度特性図、図4はバルク型ポッケル
ス素子を用いた光電界センサの斜視図、図5はその感度
特性図、図6は光電界センサと電波暗室の測定系を示す
説明図である。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a perspective view showing an embodiment of the sensor of the present invention,
2 is a perspective view showing another embodiment of the present invention, FIG. 3 is a sensitivity characteristic diagram of the sensor of the present invention shown in FIG. 1, FIG. 4 is a perspective view of an optical electric field sensor using a bulk type Pockels element, and FIG. FIG. 6 is a sensitivity characteristic diagram, and FIG. 6 is an explanatory diagram showing a measurement system of an optical electric field sensor and an anechoic chamber.

【0010】図1及び図2において、1は電気光学効果
を有するニオブ酸リチウム等の材料からなる基板で、そ
の中央に光導波路2が設置されている。3はこの光導波
路2を中心にアレイ状に配置されたダイポールアンテ
ナ、4は前記の各ダイポールアンテナ3と接続する電極
で、隣接するアンテナとは電気的に分離されている。な
お、これらのアンテナ3及び電極4は真空蒸着等の方法
により基板1に直接プリントされている。5は前記基板
1の周囲に充填配置された特定の誘電率を有する粉体又
は液体からなる誘電物質、6は前記誘電物質5を収容し
た円筒形の容器である。
In FIGS. 1 and 2, reference numeral 1 is a substrate made of a material such as lithium niobate having an electro-optical effect, and an optical waveguide 2 is installed in the center thereof. Reference numeral 3 denotes a dipole antenna arranged in an array with the optical waveguide 2 as a center, and reference numeral 4 denotes an electrode connected to each of the above dipole antennas 3, which is electrically separated from an adjacent antenna. The antenna 3 and the electrode 4 are directly printed on the substrate 1 by a method such as vacuum deposition. Reference numeral 5 denotes a dielectric substance filled around the substrate 1 and made of a powder or liquid having a specific dielectric constant, and 6 denotes a cylindrical container containing the dielectric substance 5.

【0011】本発明は、前記のようにダイポールアンテ
ナ3をアレイ状に配置することにより、アンテナに指向
性が得られる。すなわち、光導波路2の延長方向のアン
テナ利得が最も大きくなる。さらに、検出しようとする
電磁波の方向と光の進行方向を一致させることにより、
光と電磁波の位相整合が得られ易くなり、電磁波の方向
が光の進行方向と反対である場合に比較して、より高い
周波数の電界を検出することが可能となる。
According to the present invention, the dipole antennas 3 are arranged in an array as described above, so that the antenna has directivity. That is, the antenna gain in the extension direction of the optical waveguide 2 becomes the largest. Furthermore, by matching the direction of the electromagnetic wave to be detected with the traveling direction of light,
Phase matching between light and electromagnetic waves is easily obtained, and an electric field of a higher frequency can be detected as compared with the case where the direction of electromagnetic waves is opposite to the traveling direction of light.

【0012】ところで、光電界センサを空気中に置いた
場合、基板1の周囲を進む電磁波の速度と導波路中を進
む光の速度が一致しないために、更に高い周波数では電
磁波と光の位相がずれ、図3に示す光電界センサの感度
特性図における細線から明らかなように約12GHzで
は感度がなくなってしまう。そこで、本発明において
は、基板1の周囲に特定の誘電率を有する粉体又は液体
からなる誘電物質5を充填配置するようにした。図1に
示す構造の光電界センサを作製し、この光電界センサを
空気中に置いた場合と、誘電物質5として塩化カリウム
を用い、光電界センサをその中に置いた場合の周波数特
性を測定した結果を前記の図3に示してある。この感度
特性図(図3)における太線に示すように、電磁波と光
の位相が整合され、その結果、基板1の周囲が空気であ
る場合に比較して高周波数の電磁波を感度よく検出する
ことが可能となる。
By the way, when the optical electric field sensor is placed in the air, since the speed of the electromagnetic wave traveling around the substrate 1 and the speed of the light traveling in the waveguide do not match, the phases of the electromagnetic wave and the light are higher at higher frequencies. However, as is clear from the thin line in the sensitivity characteristic diagram of the optical electric field sensor shown in FIG. 3, the sensitivity is lost at about 12 GHz. Therefore, in the present invention, the dielectric substance 5 made of powder or liquid having a specific dielectric constant is filled and arranged around the substrate 1. The frequency characteristics of the optical electric field sensor having the structure shown in FIG. 1 was measured, and the optical electric field sensor was placed in the air, and potassium chloride was used as the dielectric substance 5, and the optical electric field sensor was placed therein. The results are shown in FIG. 3 above. As shown by the thick line in this sensitivity characteristic diagram (FIG. 3), the phases of the electromagnetic wave and the light are matched, and as a result, it is possible to detect the electromagnetic wave of high frequency with high sensitivity as compared with the case where the surrounding of the substrate 1 is air. Is possible.

【0013】上記の特定の誘電率を有する粉体又は液体
からなる誘電物質5としては塩化カリウム(KCl)が
適当である。すなわち、塩化カリウムの誘電率は約4.
8であり、これは電磁波が感じる屈折率として約2.1
9に相当する。一方、基板1の材料であるニオブ酸リチ
ウム中の光の屈折率は約2.23であり、このことから
基板1の周囲の電磁波の速度が導波路2中を進む光の速
度とほぼ一致することがわかる。なお、このとき電磁波
の方向と光の進行方向を一致させている。前記のよう
に、図3において、細線は光電界センサを空気中に置い
た場合、太線は光電界センサを塩化カリウム中に置いた
場合の感度を示すものであるが、光電界センサを空気中
においた場合は約12GHzで感度がなくなっている。
これは、この周波数において、電磁波と光の位相が半波
長分ずれるために生ずる現象である。これに対し、光電
界センサを塩化カリウム中に置いた場合には、前記周波
数における急激な感度の低下はみられない。このことか
ら、光電界センサの周囲に塩化カリウム等の誘電物質5
を充填配置することにより、電磁波と光の位相整合が得
られていることがわかる。また誘電物質5を充填配置し
た場合は感度が幾分高くなっているのが認められるが、
これは前記誘電物質5の誘電率が空気より大きいために
電磁波が集中することによるものである。
Potassium chloride (KCl) is suitable as the dielectric substance 5 made of powder or liquid having the above-mentioned specific dielectric constant. That is, the dielectric constant of potassium chloride is about 4.
8, which is about 2.1 as the refractive index felt by electromagnetic waves.
Equivalent to 9. On the other hand, the refractive index of light in lithium niobate, which is the material of the substrate 1, is about 2.23, which means that the velocity of the electromagnetic wave around the substrate 1 substantially matches the velocity of the light traveling in the waveguide 2. I understand. At this time, the electromagnetic wave direction and the light traveling direction are made to coincide with each other. As described above, in FIG. 3, the thin line indicates the sensitivity when the optical electric field sensor is placed in air, and the thick line indicates the sensitivity when the optical electric field sensor is placed in potassium chloride. In the case of exposure, the sensitivity is lost at about 12 GHz.
This is a phenomenon that occurs because the phases of the electromagnetic wave and the light are shifted by a half wavelength at this frequency. On the other hand, when the optical electric field sensor is placed in potassium chloride, a sharp decrease in sensitivity at the frequency is not observed. From this fact, a dielectric substance 5 such as potassium chloride is provided around the optical electric field sensor.
It can be seen that the phase matching between the electromagnetic wave and the light is obtained by filling and arranging. Also, it can be seen that the sensitivity is somewhat higher when the dielectric material 5 is filled and arranged.
This is because the dielectric constant of the dielectric material 5 is larger than that of air, so that electromagnetic waves are concentrated.

【0014】また、図2に示す他実施例では、広帯域の
周波数範囲に亘って均一な感度が得られるようにしたも
のである。すなわち、図1に示すようなダイポールアン
テナ3の長さを一定にして、アレイ状に配置した場合、
特定の周波数で感度が高くなり、従って通信用のアンテ
ナには適しているが、広い周波数範囲で均一な感度を得
る必要がある電磁界計測用のアンテナとしては適してい
ない。そこで、本実施例においては図2に示すように、
ダイポールアンテナ3のアレイを対数周期的に配置し
た。このようにダイポールアンテナ3を配置すると、各
アンテナはそれぞれ長さが異なるので、それぞれ特定の
周波数に対して固有の感度を有するため、結果として、
広い周波数範囲で均一な感度を得ることができる。
Further, in another embodiment shown in FIG. 2, uniform sensitivity is obtained over a wide frequency range. That is, when the lengths of the dipole antennas 3 as shown in FIG. 1 are fixed and arranged in an array,
The sensitivity is high at a specific frequency, and therefore it is suitable as an antenna for communication, but is not suitable as an antenna for electromagnetic field measurement that requires uniform sensitivity in a wide frequency range. Therefore, in the present embodiment, as shown in FIG.
The array of dipole antennas 3 was arranged logarithmically. When the dipole antenna 3 is arranged in this way, the antennas have different lengths, and thus each antenna has its own sensitivity to a specific frequency. As a result,
Uniform sensitivity can be obtained in a wide frequency range.

【0015】例えば、上記のような構成を有する光電界
センサを図6に示す電波暗室7内に設置し、測定室(シ
ールドルーム)8内に設けたLD励起レーザ等のレーザ
光源9で発生したレーザ光を偏波コントローラ10を介
して基板1の中央に設置した光導波路2に導入するとと
もに、前記測定室8内に設けた信号発生器13により発
生し、可変増幅器(パワーアンプ)14を介してLPD
A15から発射される高周波信号を光電界センサに照射
して、高周波信号を光信号に変調し、その光信号を光シ
グナルアナライザ11に導入して電磁波の測定を行うこ
とで、低周波範囲から高周波範囲まで広い周波数範囲で
均一な感度での測定を行うことができる。なお、12は
演算装置で、光シグナルアナライザ11の作動と信号発
生器13の作動を制御するためのものである。
For example, the optical electric field sensor having the above-mentioned configuration is installed in the anechoic chamber 7 shown in FIG. 6, and is generated by the laser light source 9 such as an LD pump laser provided in the measurement room (shield room) 8. The laser light is introduced into the optical waveguide 2 installed in the center of the substrate 1 via the polarization controller 10, and is generated by the signal generator 13 provided in the measurement chamber 8 through the variable amplifier (power amplifier) 14. LPD
By irradiating the optical electric field sensor with the high-frequency signal emitted from A15, modulating the high-frequency signal into an optical signal, introducing the optical signal into the optical signal analyzer 11, and measuring the electromagnetic wave, the high-frequency signal from the low frequency range is increased. It is possible to perform measurement with uniform sensitivity in a wide frequency range. Reference numeral 12 is an arithmetic unit for controlling the operation of the optical signal analyzer 11 and the operation of the signal generator 13.

【0016】[0016]

【発明の効果】以上、説明したように、本発明の広帯域
導波路型光電界センサによれば、光電界センサによる電
磁波の測定に際し、低周波からより高周波に至るまで高
感度の測定を行うことができる。また、高周波側におけ
る周波数特性の均一化を図ることが可能である等々、そ
の効果は極めて大きい。
As described above, according to the broadband waveguide type optical electric field sensor of the present invention, when the electromagnetic field is measured by the optical electric field sensor, it is possible to measure with high sensitivity from low frequency to higher frequency. You can Further, it is possible to make the frequency characteristics uniform on the high frequency side, and the like, which is extremely effective.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例を示す斜視図。FIG. 1 is a perspective view showing an embodiment of the present invention.

【図2】本発明の他実施例を示す斜視図。FIG. 2 is a perspective view showing another embodiment of the present invention.

【図3】図1に示す本発明センサの感度特性図。FIG. 3 is a sensitivity characteristic diagram of the sensor of the present invention shown in FIG.

【図4】バルク型ポッケルス素子を用いた光電界センサ
の斜視図。
FIG. 4 is a perspective view of an optical electric field sensor using a bulk type Pockels element.

【図5】その感度特性図。FIG. 5 is a sensitivity characteristic diagram thereof.

【図6】光電界センサと電波暗室の測定系を示す説明
図。
FIG. 6 is an explanatory diagram showing an optical electric field sensor and a measurement system of an anechoic chamber.

【符号の説明】[Explanation of symbols]

1 基板 2 光導波路 3 ダイポールアンテナ 4 電極 5 誘電物質 6 容器 7 電波暗室 8 測定室 9 レーザ光源 10 偏波コントローラ 11 光シグナルアナライザ 12 演算装置 13 信号発生器 14 可変増幅器(パワーアンプ) 15 LPDA 16 光電界センサ 17 光ファイバ 18 偏光子 19 1/4λ板 20 アンテナ 21 電極 1 substrate 2 Optical waveguide 3 dipole antenna 4 electrodes 5 Dielectric material 6 containers 7 Anechoic chamber 8 measuring room 9 Laser light source 10 Polarization controller 11 Optical signal analyzer 12 arithmetic unit 13 Signal generator 14 Variable amplifier (power amplifier) 15 LPDA 16 Optical electric field sensor 17 optical fiber 18 Polarizer 19 1/4 lambda plate 20 antenna 21 electrodes

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平9−51307(JP,A) 特開 平1−204020(JP,A) 特開 平3−170909(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01R 29/08 G02F 1/00 - 1/125 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-9-51307 (JP, A) JP-A-1-204020 (JP, A) JP-A-3-170909 (JP, A) (58) Field (Int.Cl. 7 , DB name) G01R 29/08 G02F 1/00-1/125

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 基板の中央に光導波路を設けるととも
に、前記光導波路を中心にそれぞれ長さの異なるダイポ
ールアンテナをアレイ状、かつ、前記各ダイポールアン
テナの長さ及び隣接する前記ダイポールアンテナ間の間
隔をそれぞれ対数周期的に配置したことを特徴とする広
帯域導波路型光電界センサ。
1. A central provided with an optical waveguide substrate, said optical waveguide, respectively around the different lengths dipole antenna array, and each dipole en
The length of the tenor and the distance between the adjacent dipole antennas
A broadband waveguide type optical electric field sensor characterized in that intervals are arranged logarithmically.
【請求項2】 基板周囲を進む電磁波の速度と光導波路
中を進む光の速度とを一致させるべく、基板の周囲に特
定の誘電率を有する粉体又は液体からなる物質を充填配
置したことを特徴とする請求項1記載の広帯域導波路型
光電界センサ。
2. In order to match the speed of electromagnetic waves traveling around the substrate with the speed of light traveling through the optical waveguide, a substance made of powder or liquid having a specific dielectric constant is placed around the substrate. The broadband waveguide type optical electric field sensor according to claim 1.
JP30637398A 1998-10-13 1998-10-13 Broadband waveguide optical electric field sensor Expired - Fee Related JP3462769B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30637398A JP3462769B2 (en) 1998-10-13 1998-10-13 Broadband waveguide optical electric field sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30637398A JP3462769B2 (en) 1998-10-13 1998-10-13 Broadband waveguide optical electric field sensor

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Publication Number Publication Date
JP2000121682A JP2000121682A (en) 2000-04-28
JP3462769B2 true JP3462769B2 (en) 2003-11-05

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Country Link
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5103579B2 (en) * 2005-05-11 2012-12-19 株式会社ノイズ研究所 Method for improving characteristics of a broadband waveguide type optical electric field sensor
JP4982861B2 (en) * 2007-08-29 2012-07-25 国立大学法人大阪大学 Radio signal receiving and separating device
JP5249553B2 (en) * 2007-11-02 2013-07-31 株式会社エヌ・ティ・ティ・ドコモ Electro-optic probe
JP2009128154A (en) * 2007-11-22 2009-06-11 Noise Laboratory Co Ltd Optical electric field sensor
CN108051654B (en) * 2017-12-04 2019-11-29 北京航空航天大学 A kind of magnet field probe using bevel edge grading structure

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