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JPS645283B2 - - Google Patents
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JPS645283B2 - - Google Patents

Info

Publication number
JPS645283B2
JPS645283B2 JP6764280A JP6764280A JPS645283B2 JP S645283 B2 JPS645283 B2 JP S645283B2 JP 6764280 A JP6764280 A JP 6764280A JP 6764280 A JP6764280 A JP 6764280A JP S645283 B2 JPS645283 B2 JP S645283B2
Authority
JP
Japan
Prior art keywords
magneto
faraday rotation
temperature
mixed crystal
optical element
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
Application number
JP6764280A
Other languages
Japanese (ja)
Other versions
JPS56162715A (en
Inventor
Osamu Kamata
Tetsuo Yanai
Yoshinobu Tsujimoto
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP6764280A priority Critical patent/JPS56162715A/en
Publication of JPS56162715A publication Critical patent/JPS56162715A/en
Publication of JPS645283B2 publication Critical patent/JPS645283B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/0009Materials therefor
    • G02F1/0036Magneto-optical materials

Landscapes

  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Compounds Of Iron (AREA)
  • Measuring Magnetic Variables (AREA)

Description

【発明の詳細な説明】 本発明は、広い温度範囲にわたつてフアラデイ
回転能をほぼ一定にした磁気光学素子に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magneto-optical element with substantially constant Faraday rotation ability over a wide temperature range.

フアラデイ回転能を利用した磁気光学素子は、
光通信用光アイソレータ用として広く用いられて
いる。なお、フアラデイ回転能とは、飽和磁化状
態でのフアラデイ回転角である。
Magneto-optical elements that utilize Faraday rotation ability are
Widely used as optical isolators for optical communications. Note that the Faraday rotation ability is the Faraday rotation angle in a saturated magnetization state.

一般に光アイソレータは、第1図に示すよう
に、偏光プリズム1,2と磁気光学素子3と永久
磁石4とにより構成されており、磁気光学素子3
としては、希土類鉄ガーネツトの一種である
Y3Fe5O12が多く使用されている。永久磁石4に
より磁気光学素子3を飽和磁化の状態に保ち、磁
気光学素子3のフアラデイ効果に基づく偏向面の
回転角を例えば45゜に規定し、偏光プリズム1,
2を45゜だけ偏向方向が異なるように配置する。
これにより、順方向に進む光5は、偏光プリズム
1で単一偏向に選択され、磁気光学素子3を通過
することにより偏向面を45゜だけ回転したのち、
偏光プリズム2を通過することができる。しか
し、逆方向に進む光6は、偏光プリズム2で単一
偏光に選択され、磁気光学素子3を通過すること
により偏向面を上記順方向の場合と同一に45゜だ
け回転させられるため磁気光学素子3通過後の偏
光方向と、偏光プリズム1の偏光方向が直交す
る。そのため、逆方向に進む光6は、偏光プリズ
ム1を通過することができないので通過特性に方
向性を持たせることができるのである。
Generally, an optical isolator is composed of polarizing prisms 1 and 2, a magneto-optical element 3, and a permanent magnet 4, as shown in FIG.
It is a kind of rare earth iron garnet.
Y 3 Fe 5 O 12 is often used. The magneto-optical element 3 is kept in a state of saturation magnetization by the permanent magnet 4, the rotation angle of the deflection surface based on the Faraday effect of the magneto-optical element 3 is defined to, for example, 45 degrees, and the polarizing prism 1,
2 are arranged so that their deflection directions differ by 45 degrees.
As a result, the light 5 traveling in the forward direction is selected to have a single polarization by the polarizing prism 1, and after rotating the polarization plane by 45 degrees by passing through the magneto-optical element 3,
It can pass through the polarizing prism 2. However, the light 6 traveling in the opposite direction is selected as a single polarized light by the polarizing prism 2, and by passing through the magneto-optic element 3, the polarization plane is rotated by 45 degrees, the same as in the case of the forward direction. The polarization direction after passing through the element 3 and the polarization direction of the polarizing prism 1 are orthogonal. Therefore, the light 6 traveling in the opposite direction cannot pass through the polarizing prism 1, so that the passing characteristic can be given directionality.

しかしながら、磁気光学素子3のフアラデイ回
転能に例えば第2図(1.15μmの波長λの光の場
合)に示すように温度依存性があるため、光アイ
ソレータの順方向および逆方向の損失が温度によ
り変化する。そのため、光アイソレータの使用温
度を一定に保持しなければ、十分な方向性を得る
ことができないという欠点があつた。
However, since the Faraday rotation ability of the magneto-optical element 3 has a temperature dependence, as shown in FIG. Change. Therefore, there was a drawback that sufficient directionality could not be obtained unless the operating temperature of the optical isolator was kept constant.

本発明は、フアラデイ回転能が、正の温度係数
であるY3Fe5O12と負の温度係数の希土類鉄ガー
ネツトGd3Fe5O12とを特定比で混晶化することに
より、広い温度範囲にわたつてフアラデイ回転能
をほぼ一定にした磁気光学素子を提供することを
目的とする。
The present invention has a Faraday rotation ability that can be adjusted over a wide range of temperatures by mixing Y 3 Fe 5 O 12 , which has a positive temperature coefficient, and rare earth iron garnet Gd 3 Fe 5 O 12 , which has a negative temperature coefficient, in a specific ratio. It is an object of the present invention to provide a magneto-optical element whose Faraday rotation ability is substantially constant over a range.

以下本発明を図面を用いて説明する。 The present invention will be explained below using the drawings.

磁気光学物質Y3Fe5O12は第2図に示すように
−75゜以上の温度に対し、温度上昇とともにフア
ラデイ回転能は減少する。温度上昇とともにフア
ラデイ回転能が減少するのが希土類鉄ガーネツト
の一般的傾向であるが、中には第3図に示す
Gd3Fe5O12のように反対の温度係数を持つものも
ある。
As shown in FIG. 2, the Faraday rotation ability of the magneto-optical material Y 3 Fe 5 O 12 decreases as the temperature rises above -75°. The general tendency of rare earth iron garnets is that the Faraday rotation ability decreases as the temperature increases, but some
Some have opposite temperature coefficients, such as Gd 3 Fe 5 O 12 .

したがつて、Y3Fe5O12とGd3Fe5O12との混晶
(Y1-XGdX3Fe5O12において、Xの値を調整する
ことによりフアラデイ回転能の温度係数を零に近
づけることが可能である。なお、(Y1-XGdX
3Fe5O12を得るには、Y3Fe5O12とGd3Fe5O12とを
周知の方法にて混晶化すればよい。
Therefore, in the mixed crystal of Y 3 Fe 5 O 12 and Gd 3 Fe 5 O 12 ( Y 1-X Gd It is possible to bring it close to zero. Furthermore, (Y 1-X Gd X )
3 Fe 5 O 12 can be obtained by mixing Y 3 Fe 5 O 12 and Gd 3 Fe 5 O 12 by a well-known method.

第4図は、上記例においてXの値を0〜0.7ま
で調整し温度を−50℃〜+100℃の範囲で変化さ
せた場合のフアラデイ回転能の変化範囲を示した
ものである。これより明らかなように混晶比X=
0.3付近でフアラデイ回転能の温度係数は極小値
となり、第4図に示すように0.1≦X≦0.45なる
液晶では−50℃〜+100℃の広い範囲にわたりフ
アラデイ回転能の温度係数をほぼ2.7%以下とな
すことができ、実用上フアラデイ回転能の温度に
よる変化を無視しうる程度となしえた。
FIG. 4 shows the range of change in Faraday rotational performance when the value of X is adjusted from 0 to 0.7 and the temperature is varied from -50°C to +100°C in the above example. As is clear from this, the mixed crystal ratio X=
The temperature coefficient of Faraday rotation ability reaches a minimum value around 0.3, and as shown in Figure 4, for liquid crystals with 0.1≦X≦0.45, the temperature coefficient of Faraday rotation ability is approximately 2.7% or less over a wide range of -50℃ to +100℃. In practical terms, the change in Faraday rotational ability due to temperature can be ignored.

さらに、Y3Fe5O12の飽和磁化が1200Oeである
のに対し、(Y0.7Gd0.33Fe5O12の飽和磁化は、
900Oeであるため、第1図に示すような光アイソ
レータに用いた場合永久磁石が小さくできるとい
う利点がある。
Furthermore, while the saturation magnetization of Y 3 Fe 5 O 12 is 1200 Oe, the saturation magnetization of (Y 0.7 Gd 0.3 ) 3 Fe 5 O 12 is
Since it is 900 Oe, it has the advantage that the permanent magnet can be made smaller when used in an optical isolator as shown in FIG.

以上説明したように、本発明は、従来、本質的
に避けることのできなかつた、飽和磁化中でのフ
アラデイ回転能の温度による変化を事実上なくす
ることができるものであるから、広範囲に温度が
変化する環境下においても恒温装置等を要するこ
となく安定な動作を確保しうる光アイソレータ,
光スイツチ等を容易に提供することができ、その
実用性は大きい。
As explained above, the present invention can virtually eliminate the temperature-related change in Faraday rotation ability during saturation magnetization, which was essentially unavoidable in the past. An optical isolator that can ensure stable operation without the need for a constant temperature device, even under changing environments.
Light switches and the like can be easily provided, and its practicality is great.

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

第1図は磁気光学素子を用いた光アイソレータ
の構成を示す図、第2図はY3Fe5O12のフアラデ
イ回転能の温度依存性を示す図、第3図は
Gd3Fe5O12のフアラデイ回転能の温度依存性を示
す図、第4図は(Y1-XGdX3Fe5O12の温度範囲−
50℃〜+100℃での混晶化によるフアラデイ回転
能の変化率を示す図、第5図は本発明の一実施例
である(Y0.7Gd0.33Fe5O12のフアラデイ回転能の
温度依存性を示す図である。 1,2……偏光プリズム、3……磁気光学素
子、4……永久磁石、5……順方向に進む光、6
……逆方向に進む光。
Figure 1 shows the configuration of an optical isolator using a magneto-optical element, Figure 2 shows the temperature dependence of the Faraday rotation ability of Y 3 Fe 5 O 12 , and Figure 3 shows the structure of an optical isolator using a magneto-optical element.
A diagram showing the temperature dependence of Faraday rotation ability of Gd 3 Fe 5 O 12 , Figure 4 shows the temperature range of (Y 1-X Gd X ) 3 Fe 5 O 12 -
Figure 5 shows the rate of change in Faraday rotational power due to mixed crystallization at 50°C to + 100 ° C , which is an example of the present invention. It is a diagram showing dependence. 1, 2...Polarizing prism, 3...Magneto-optical element, 4...Permanent magnet, 5...Light traveling in the forward direction, 6
...Light traveling in the opposite direction.

Claims (1)

【特許請求の範囲】[Claims] 1 第1、第2の偏光プリズム間の光路中に、一
般式(Y1-xGdx3Fe5O12で示され前記xが0.1≦x
≦0.45である希土類ガーネツト混晶を配置し、前
記混晶の周囲に磁石を設置し、前記磁石により前
記混晶を磁気的に飽和させ、前記光路を進む光を
前記混晶でフアラデー回転させることを特徴とす
る磁気光学素子。
1 In the optical path between the first and second polarizing prisms, the general formula (Y 1-x Gd x ) 3 Fe 5 O 12 is expressed, and x is 0.1≦x
≦0.45 rare earth garnet mixed crystal is arranged, a magnet is installed around the mixed crystal, the mixed crystal is magnetically saturated by the magnet, and the light traveling along the optical path is subjected to Faraday rotation by the mixed crystal. A magneto-optical element featuring:
JP6764280A 1980-05-20 1980-05-20 Magnetic and optical element Granted JPS56162715A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6764280A JPS56162715A (en) 1980-05-20 1980-05-20 Magnetic and optical element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6764280A JPS56162715A (en) 1980-05-20 1980-05-20 Magnetic and optical element

Publications (2)

Publication Number Publication Date
JPS56162715A JPS56162715A (en) 1981-12-14
JPS645283B2 true JPS645283B2 (en) 1989-01-30

Family

ID=13350854

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6764280A Granted JPS56162715A (en) 1980-05-20 1980-05-20 Magnetic and optical element

Country Status (1)

Country Link
JP (1) JPS56162715A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2504192B2 (en) * 1989-06-15 1996-06-05 株式会社村田製作所 Microwave / millimeter wave magnetic composition
JP2504273B2 (en) * 1990-04-04 1996-06-05 株式会社村田製作所 Microwave / millimeter wave magnetic composition

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3784281A (en) * 1973-03-06 1974-01-08 Bbc Brown Boveri & Cie Ferrimagnetic garnet corrected for temperature dependence of the faraday effect and method for making the same
JPS512320A (en) * 1974-05-17 1976-01-09 Matsushita Electric Industrial Co Ltd Johoden sosochi

Also Published As

Publication number Publication date
JPS56162715A (en) 1981-12-14

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