JPH05119288A - Magneto-optical film of magneto-optical field sensor - Google Patents

Magneto-optical film of magneto-optical field sensor

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Publication number
JPH05119288A
JPH05119288A JP3279586A JP27958691A JPH05119288A JP H05119288 A JPH05119288 A JP H05119288A JP 3279586 A JP3279586 A JP 3279586A JP 27958691 A JP27958691 A JP 27958691A JP H05119288 A JPH05119288 A JP H05119288A
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JP
Japan
Prior art keywords
magneto
optical
film
sensitivity
magnetic field
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
JP3279586A
Other languages
Japanese (ja)
Other versions
JP2783012B2 (en
Inventor
Nobuo Nakamura
宣夫 中村
Yosuke Asahara
陽介 浅原
Shuji Osumi
修司 大住
Satoaki Asakura
聡章 朝倉
Haruo Ishikawa
治男 石川
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.)
Sumitomo Metal Mining Co Ltd
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Sumitomo Metal Mining Co Ltd
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Priority to JP27958691A priority Critical patent/JP2783012B2/en
Publication of JPH05119288A publication Critical patent/JPH05119288A/en
Application granted granted Critical
Publication of JP2783012B2 publication Critical patent/JP2783012B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To provide the magneto-optical film which has a high sensitivity and is formed to eliminate the influence of temp. on this sensitivity as the magneto-optical film of the magneto-optical sensor for which a magneto-optical effect is utilized. CONSTITUTION:The magneto-optical film to be used for the magnetic field sensor for which the magneto-optical effect is utilized is a magnetic garnet film which consists of a compsn. expressed by YbXTbYBi3-x-yFe3O12 where (x) and (y) are so determined as to satisfy the following conditions: 1.82-1.27x<=y<=2.02-1.27x.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、磁気光学素子のファラ
デー効果を利用して磁界強度を測定する光磁界センサに
使用される磁気光学膜に関し、特に電力を供給する配電
線の周囲に発生する磁界強度を測定しその電流の大きさ
を検知するようにした光磁界センサ用の磁気光学膜に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical film used in an optical magnetic field sensor for measuring the magnetic field strength by utilizing the Faraday effect of a magneto-optical element, and particularly to a magneto-optical film formed around a distribution line supplying electric power. The present invention relates to a magneto-optical film for an optical magnetic field sensor that measures magnetic field strength and detects the magnitude of the current.

【0002】[0002]

【従来の技術】近年、発電所から末端の電力消費者まで
の電力輸送路において、変電所,送電線及び配電線等に
流れる電流の大きさを測定してその異常を発見する電流
センサとして、電流が流れる導線の周囲に発生する磁界
を磁気光学効果を利用して測定し、電流値を求めるよう
にした光磁界センサを用いる計画が進んでいる。そして
特に変電所や高圧送電線など大電流を扱い、また事故時
の被害が広い範囲に及ぶ場合等、既に一部で実用化が開
始されている。
2. Description of the Related Art In recent years, as a current sensor for detecting the abnormality by measuring the magnitude of the current flowing through a substation, a transmission line, a distribution line, etc. in an electric power transmission path from a power plant to a terminal electric power consumer, A plan is underway to use an optical magnetic field sensor that measures the magnetic field generated around the conducting wire through which the current flows by utilizing the magneto-optical effect and obtains the current value. In particular, when large currents such as substations and high-voltage transmission lines are handled, and damage from an accident spreads over a wide range, practical application has already started in some areas.

【0003】かかる電流計測用の光磁界センサは、一般
に野外で使用されるため、環境特に温度の変化に対して
安定した感度を備えていることが重要であり、例えば−
20〜+80°Cの温度範囲でその感度の変動率(SR
=ΔS/S(%))が±1%以内であることが要求され
ている。なお、ここに感度とは、磁界の変化に対するセ
ンサ出力の変化率をいう。そして上記のように大電流を
扱う変電所や高圧送電線などで使用される光磁界センサ
では、感度は小さいが(1×10-4/ Oe (エルステッ
ド)以下)、大きな磁界に対して磁気飽和が生じない鉛
ガラス,ZnSe,BGO,BSO等の常磁性材料又は
反磁性材料が磁気光学材料として用いられている。そし
てこれらの材料は、温度に対する感度の変動も小さく、
良好な結果が得られている。
Since the optical magnetic field sensor for current measurement is generally used outdoors, it is important that it has a stable sensitivity to changes in the environment, especially in temperature.
Fluctuation rate of the sensitivity in the temperature range of 20~ + 80 ° C (S R
= ΔS / S (%)) is required to be within ± 1%. The sensitivity here means the rate of change of the sensor output with respect to the change of the magnetic field. As described above, the optical magnetic field sensor used in a substation that handles a large current or a high-voltage power transmission line has a low sensitivity (1 × 10 −4 / Oe (Oersted) or less), but a magnetic saturation in a large magnetic field. A paramagnetic material or a diamagnetic material such as lead glass, ZnSe, BGO, BSO, etc., which does not cause the phenomenon is used as the magneto-optical material. And these materials have a small sensitivity variation with temperature,
Good results have been obtained.

【0004】一方、最近では電力消費者に近い小電流を
扱う配電線においてもこの種の光磁界センサを用いる計
画も進んできている。かかる配電線の場合、発生する磁
界が小さいため1×10-4/ Oe 以上の高い感度が要求
される。このため、上記鉛ガラス,ZnSe,BGO,
BSO等の磁気光学材料では、十分な感度を得ることが
できず、正確な測定を行うことが困難になる。そこで、
このような配電線に対するものとして、磁気感度が高い
磁性ガーネット膜さらにはBi置換型の磁性ガーネット
膜を使用する光磁界センサの開発・研究が行われてい
る。なお、配電線用の光磁界センサは一部を除き、コス
トが安価であることが要求され、また通常では0.85
μm程度の波長の光が用いられる。
On the other hand, recently, a plan to use this kind of optical magnetic field sensor is also progressing in a distribution line handling a small current close to that of a power consumer. In the case of such a distribution line, since the magnetic field generated is small, a high sensitivity of 1 × 10 −4 / Oe or more is required. Therefore, the lead glass, ZnSe, BGO,
With magneto-optical materials such as BSO, sufficient sensitivity cannot be obtained, and accurate measurement becomes difficult. Therefore,
As such a distribution line, an optical magnetic field sensor using a magnetic garnet film having high magnetic sensitivity and further a Bi substitution type magnetic garnet film has been developed and studied. The optical magnetic field sensor for the distribution line is required to be inexpensive, except for a part, and normally 0.85.
Light having a wavelength of about μm is used.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、上記磁
性ガーネット膜は強磁性体であるため、特に上記ZnS
e,BGO,BSO等の常磁性材料又は反磁性材料と比
較して、飽和磁界Hsやファラデー回転係数θfなどの
磁気特性や磁気光学特性が温度によって著しく変化し、
このため感度自体も温度の変化により大きく変動せしめ
られるという問題がある。このように従来の磁性材料そ
のままでは、この種の光磁界センサ用の磁性ガーネット
膜を実現することができなかった。
However, since the above-mentioned magnetic garnet film is a ferromagnetic substance, the above-mentioned ZnS is especially used.
Compared with paramagnetic materials or diamagnetic materials such as e, BGO, and BSO, magnetic characteristics such as the saturation magnetic field Hs and Faraday rotation coefficient θf and magneto-optical characteristics significantly change depending on temperature,
For this reason, there is a problem in that the sensitivity itself can be largely changed due to a change in temperature. As described above, it was not possible to realize a magnetic garnet film for this type of optical magnetic field sensor using the conventional magnetic material as it is.

【0006】本発明は、この種の光磁界センサにおいて
高い感度を備え、且つこの感度に対する温度の影響をな
くするようにした磁気光学膜を提供することを目的とす
る。
It is an object of the present invention to provide a magneto-optical film having a high sensitivity in this type of optical magnetic field sensor and eliminating the influence of temperature on this sensitivity.

【0007】[0007]

【課題を解決するための手段】本発明の磁気光学膜は、
YbX TbY Bi3-X-Y Fe3 O12 の組成で成り、x及びyが次
の(1)式を満足するようにしたものである。 1.82−1.27x≦y≦2.02−1.27x (1)
The magneto-optical film of the present invention comprises:
Made in the composition of Yb X Tb Y Bi 3-XY Fe 3 O 12, x and y is obtained so as to satisfy the following equation (1). 1.82-1.27x ≦ y ≦ 2.02-1.27x (1)

【0008】また、本発明の磁気光学膜は、上記xは
0.8〜1.1の範囲にあり、且つ膜厚が10〜30μ
mであることを特徴とする。
In the magneto-optical film of the present invention, x is in the range of 0.8 to 1.1 and the film thickness is 10 to 30 μm.
It is characterized by being m.

【0009】[0009]

【作用】先ずここで、磁性ガーネット膜を使用した光磁
界センサの感度Sは、該磁性ガーネット膜の膜厚をLと
すると、次の(2)式によって表される。 S=sin(2θf・L)/Hs (2) 上記(2)式中、飽和磁界Hs及びファラデー回転係数
θfは温度によって変化し、従って(2)式において温
度変化に対する sin(2θf・L)とHsの変化の仕方
を同一にすることにより、それらの比である上記(2)
式によって表される感度は温度が変化しても一定になる
ようにすることができる。また、磁性ガーネット膜の組
成が決まれば、ファラデー回転係数θf及び飽和磁界H
sの各温度変化率も決定されるため、感度Sの温度に対
する変動率SR は磁性ガーネット膜の組成に依存するこ
とになる。そしてまた、かかる変動率SR は、感度Sが
θf・Lのsin関数を問題とするため、膜厚Lにも依
存する。即ち、同一組成の磁性ガーネット膜でも、変動
率SR は膜厚Lによって変化する。
First, the sensitivity S of the optical magnetic field sensor using the magnetic garnet film is expressed by the following equation (2), where L is the thickness of the magnetic garnet film. S = sin (2θf · L) / Hs (2) In the above formula (2), the saturation magnetic field Hs and the Faraday rotation coefficient θf change depending on the temperature. Therefore, in the formula (2), sin (2θf · L) with respect to temperature change is expressed as By making the change of Hs the same, the ratio (2)
The sensitivity represented by the formula can be made constant even when the temperature changes. Further, if the composition of the magnetic garnet film is determined, the Faraday rotation coefficient θf and the saturation magnetic field H
Since each temperature change rate of s is also determined, the variation rate S R of the sensitivity S with respect to temperature depends on the composition of the magnetic garnet film. Further, the fluctuation rate S R also depends on the film thickness L because the sensitivity S has a problem of the sin function of θf · L. That is, even in the case of the magnetic garnet film having the same composition, the variation rate S R changes depending on the film thickness L.

【0010】本発明によれば、上記の点を考慮して磁性
ガーネット膜の組成設計を行い、さらに変動率SR を小
さくする膜厚Lを求めることにより、この種の光磁界セ
ンサに好適な磁気光学膜を得ることができる。そして特
に、希土類元素を変えたときのBi置換鉄ガーネットの
飽和磁化及びファラデー回転係数θf並びにそれらの温
度に対する変化の試験結果から、(Yb Tb Bi)3 Fe3 O12
系の材料が好適であることが判明した。
According to the present invention, the composition of the magnetic garnet film is designed in consideration of the above points, and the film thickness L for reducing the variation rate S R is determined, which is suitable for this type of optical magnetic field sensor. A magneto-optical film can be obtained. And, in particular, from the saturation magnetization and the Faraday rotation coefficient θf of the Bi-substituted iron garnet when changing the rare earth element and the test results of the change with respect to the temperature, (Yb Tb Bi) 3 Fe 3 O 12
The materials of the system have proved to be suitable.

【0011】[0011]

【実施例】以下、図1及び図2に基づき本発明による光
磁界センサの磁気光学膜の一実施例を説明する。本発明
の磁気光学膜は、YbX TbY Bi3-X-Y Fe3 O12 の組成で成
るが、この磁性ガーネット膜は液相エピタキシャル法に
より上記 Yb X TbY Bi3-X-Y Fe3 O12 におけるx及びy
を変えて組成が異なる種類のものが製作された。即ち、
先ず白金ルツボ中にPbO,Bi2 3 ,B2 3 をフ
ラックスとしてYb2 3 ,Tb2 3 ,Fe2 3
溶かし込んだ融液を作成した。そして該融液を温度77
0〜790°Cに加熱しながら、その融液表面にガドリ
ニウム・ガリウムガーネット単結晶基板(以下、GGG
基板という)を付着させて100rpmで回転させるこ
とにより、上記GGG基板の片面に厚さ70μmのYbX
Tb Y Bi3-X-Y Fe3 O12 磁性ガーネット膜を成長させた。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The light according to the present invention will be described below with reference to FIGS. 1 and 2.
An example of the magneto-optical film of the magnetic field sensor will be described. The present invention
The magneto-optical film of YbXTbYBi3-XYFe3O12The composition of
However, this magnetic garnet film is suitable for liquid phase epitaxial method.
More above YbXTbYBi3-XYFe3O12X and y in
Different types were produced with different compositions. That is,
First, PbO, Bi in the platinum crucible203, B203The
Yb as a Lux203, Tb203, Fe203To
A melt was prepared by melting. The melt is heated to a temperature of 77
While heating to 0 to 790 ° C, gadly on the surface of the melt
Ni-Gallium garnet single crystal substrate (hereinafter GGG
Substrate) and spin at 100 rpm
As a result, Yb with a thickness of 70 μm is formed on one surface of the GGG substrate.X
Tb YBi3-XYFe3O12A magnetic garnet film was grown.

【0012】上記の場合、融液中のYb2 3 とTb2
3 の含有割合を変えることにより、上記x及び上記y
が相違する異なる組成の試料が製作される。なお、液相
エピタキシャル法では、磁性ガーネット膜の格子定数と
上記GGG基板の格子定数(12.496A)とがほぼ
一致している必要があるため、これらx,yには前記
(1)式を満足する条件が加わる。従ってx,yのうち
xが決まればyも一義的に決定される。また、作成した
磁性ガーネット膜の膜厚Lを70μmとしたが、これは
該膜厚Lが70μm以上では波長0.85μmの光の場
合にその損失が大きくなり、事実上、磁性ガーネット膜
を光磁界センサに使用し得ないためである。
In the above case, Yb 2 O 3 and Tb 2 in the melt are
By changing the content ratio of 0 3 , the above x and the above y can be obtained.
Samples with different compositions are produced. In the liquid phase epitaxial method, the lattice constant of the magnetic garnet film and the lattice constant of the GGG substrate (12.496A) need to be substantially equal to each other. Satisfaction conditions are added. Therefore, if x of x and y is determined, y is also uniquely determined. Further, the film thickness L of the magnetic garnet film prepared was set to 70 μm. However, when the film thickness L is 70 μm or more, the loss becomes large in the case of light having a wavelength of 0.85 μm. This is because it cannot be used as a magnetic field sensor.

【0013】次に上記x及び上記yが相違する各磁性ガ
ーネット膜毎に30個ずつ試料として取り出し、各々研
磨によってL=5〜65μmとなるように形成した。つ
まり、各上記xの組成に対して5〜65μmの範囲で3
0種類の膜厚の試料を製作した。さらに各試料のGGG
基板面及び磁性ガーネット膜面に波長0.85μm用の
SiO2 単層で成る無反射コートを施した。
Next, 30 samples of each magnetic garnet film having different x and y were taken out as samples, and formed by polishing so that L = 5 to 65 μm. That is, in the range of 5 to 65 μm for each of the above x compositions, 3
Samples with 0 kinds of film thickness were manufactured. Furthermore, GGG of each sample
The substrate surface and the magnetic garnet film surface were coated with a non-reflective coating consisting of a SiO 2 single layer for a wavelength of 0.85 μm.

【0014】次に、上記のように製作された磁気光学膜
の温度変化に対する感度の試験結果について説明する。
上記磁性ガーネット膜の各試料に対して温度−20〜+
80°Cの温度範囲でその感度を測定するが、ここで図
1は、かかる試験を行うための測定系の構成例を示して
いる。図において、レーザダイオード1から出射した波
長0.85μmの光はレンズ2及び偏光子3を通過して
直線偏光になり、磁性ガーネット膜4に入射する。そし
てこの磁性ガーネット膜4を通過するときに被測定磁界
(以下、単に磁界という)の強さに応じた旋光作用を受
けた光は、さらにレンズ5及び偏光子6を通過して上記
磁界の強さに対応する強度になる。この後、偏光子6か
らシリコンフォトダイオード7へ入射した光の強度が検
出されるようになっている。上記の場合、±300 Oe
の磁界が光路と平行に加えられると共に、磁性ガーネッ
ト膜4の温度は図示しないペルチェ素子によって変化せ
しめられる。
Next, the test results of the sensitivity of the magneto-optical film manufactured as described above to temperature changes will be described.
For each sample of the magnetic garnet film, the temperature is -20 to +
Its sensitivity is measured in the temperature range of 80 ° C., and FIG. 1 shows an example of the configuration of a measurement system for performing such a test. In the figure, light having a wavelength of 0.85 μm emitted from the laser diode 1 passes through the lens 2 and the polarizer 3 to become linearly polarized light, and enters the magnetic garnet film 4. Then, the light that has been subjected to the optical rotatory action according to the strength of the magnetic field to be measured (hereinafter, simply referred to as magnetic field) when passing through the magnetic garnet film 4 further passes through the lens 5 and the polarizer 6 and the strength of the magnetic field. It becomes the strength corresponding to. After that, the intensity of the light incident on the silicon photodiode 7 from the polarizer 6 is detected. In the above case, ± 300 Oe
Is applied in parallel to the optical path, and the temperature of the magnetic garnet film 4 is changed by a Peltier device (not shown).

【0015】そして、各磁性ガーネット膜試料の−20
〜+80°Cの温度範囲における感度Sを調べ、その変
動率SR が±1%以内となる Yb X TbY Bi3-X-Y Fe3 O
12 におけるx及び膜厚Lを求めたところ、図2に示さ
れる結果が得られた。即ち、図2のグラフにおいて、直
線a,b及びcによって囲まれた領域の場合、温度−2
0〜+80°Cの範囲で感度Sの変動率SR が±1%以
内である。なお、同グラフ中、直線dよりも下側の領域
では感度S自体が既に1×10-4/ Oe 以下である。つ
まり、上記直線a,b,c及びdによって囲まれた領域
(斜線部分)では、−20〜+80°Cの温度範囲にお
ける感度Sの変動率SR が±1%以内となり、且つ感度
S自体が1×10-4〜4×10-4/ Oe となる。
-20 of each magnetic garnet film sample
The sensitivity S in the temperature range of + 80 ° C is investigated, and the variation S R is within ± 1% Yb X Tb Y Bi 3-XY Fe 3 O
When x and the film thickness L in 12 were obtained, the results shown in FIG. 2 were obtained. That is, in the case of the region surrounded by the straight lines a, b and c in the graph of FIG.
The variation rate S R of the sensitivity S is within ± 1% in the range of 0 to + 80 ° C. In the graph, in the region below the straight line d, the sensitivity S itself is already 1 × 10 −4 / Oe or less. That is, in the region surrounded by the straight lines a, b, c and d (hatched part), the variation rate S R of the sensitivity S in the temperature range of −20 to + 80 ° C. is within ± 1%, and the sensitivity S itself. Is 1 × 10 −4 to 4 × 10 −4 / Oe.

【0016】従って、YbX TbY Bi3-X-Y Fe3 O12 磁性ガ
ーネット膜において、かかる領域に対応するxの範囲が
0.8〜1.1であり且つ該磁性ガーネット膜の膜厚L
が10〜30μmであるときには、温度−20〜+80
°Cの範囲で感度Sの変動率SR が±1%以内なり、感
度S自体が1×10-4〜4×10-4/ Oe となるから、
このような磁性ガーネット膜を使用する光磁界センサは
温度がかなり変化しても微小な磁界を高い精度で安定し
て測定することがきる。
Therefore, in the Yb X Tb Y Bi 3-XY Fe 3 O 12 magnetic garnet film, the range of x corresponding to such a region is 0.8 to 1.1 and the film thickness L of the magnetic garnet film is L.
Is 10 to 30 μm, the temperature is −20 to +80.
In the range of ° C, the variation rate S R of the sensitivity S is within ± 1%, and the sensitivity S itself becomes 1 × 10 -4 to 4 × 10 -4 / Oe.
An optical magnetic field sensor using such a magnetic garnet film can stably measure a minute magnetic field with high accuracy even if the temperature changes considerably.

【0017】[0017]

【発明の効果】上述したように本発明の磁気光学膜は高
い感度を備え、且つこの感度は温度の変化に対して極め
て安定しており、特に配電線等の電流値検出の場合等に
おいて過酷な環境下でしかも微小磁界を高い精度で測定
し得るこの種の光磁界センサを実現することができる等
の利点がある。
As described above, the magneto-optical film of the present invention has a high sensitivity, and this sensitivity is extremely stable with respect to changes in temperature. In particular, it is harsh when detecting a current value of a distribution line or the like. It is possible to realize an optical magnetic field sensor of this kind that can measure a minute magnetic field with high accuracy under various environments.

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

【図1】本発明の磁気光学膜に対する感度試験ための感
度測定系の構成例を示す図である。
FIG. 1 is a diagram showing a configuration example of a sensitivity measurement system for a sensitivity test on a magneto-optical film of the present invention.

【図2】本発明の磁気光学膜に対する感度測定結果によ
る膜組成と膜厚との関係を示すグラフである。
FIG. 2 is a graph showing the relationship between film composition and film thickness based on the results of sensitivity measurement for the magneto-optical film of the present invention.

【符号の説明】[Explanation of symbols]

1 レーザダイオード 2 レンズ 3 偏光子 4 磁性ガーネット膜 5 レンズ 6 偏光子 7 シリコンフォトダイオード 1 Laser diode 2 Lens 3 Polarizer 4 Magnetic garnet film 5 Lens 6 Polarizer 7 Silicon photodiode

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 磁気光学効果を利用した磁界センサに使
用される磁気光学膜において、YbX TbY Bi3-X-Y Fe3 O
12 の組成で成り、上記x及び上記yが下記の条件式を
満足するようにした磁性ガーネット膜であることを特徴
とする磁気光学膜。 1.82−1.27x≦y≦2.02−1.27x
1. A magneto-optical film used in a magnetic field sensor utilizing a magneto-optical effect, comprising: Yb X Tb Y Bi 3-XY Fe 3 O
A magneto-optical film having a composition of 12 , wherein x and y are magnetic garnet films satisfying the following conditional expressions. 1.82-1.27x ≦ y ≦ 2.02-1.27x
【請求項2】 上記xは0.8〜1.1の範囲にあり、
且つ上記磁性ガーネット膜の膜厚が10〜30μmであ
ることを特徴とする請求項1に記載の磁気光学膜。
2. The above x is in the range of 0.8 to 1.1,
The magneto-optical film according to claim 1, wherein the magnetic garnet film has a thickness of 10 to 30 μm.
JP27958691A 1991-10-25 1991-10-25 Magneto-optical film of optical magnetic field sensor Expired - Fee Related JP2783012B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27958691A JP2783012B2 (en) 1991-10-25 1991-10-25 Magneto-optical film of optical magnetic field sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27958691A JP2783012B2 (en) 1991-10-25 1991-10-25 Magneto-optical film of optical magnetic field sensor

Publications (2)

Publication Number Publication Date
JPH05119288A true JPH05119288A (en) 1993-05-18
JP2783012B2 JP2783012B2 (en) 1998-08-06

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Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP2783012B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5691837A (en) * 1995-03-17 1997-11-25 Matsushita Electric Industrial Co., Ltd. Magneto-optical element and optical magnetic field sensor using the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5691837A (en) * 1995-03-17 1997-11-25 Matsushita Electric Industrial Co., Ltd. Magneto-optical element and optical magnetic field sensor using the same
US5835257A (en) * 1995-03-17 1998-11-10 Matsushita Electric Industrial Co., Ltd. Magneto-optical element and optical magnetic field sensor using the same

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