JPH01173402A - Exciting element for magneto-optical recording - Google Patents
Exciting element for magneto-optical recordingInfo
- Publication number
- JPH01173402A JPH01173402A JP33343087A JP33343087A JPH01173402A JP H01173402 A JPH01173402 A JP H01173402A JP 33343087 A JP33343087 A JP 33343087A JP 33343087 A JP33343087 A JP 33343087A JP H01173402 A JPH01173402 A JP H01173402A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- parallel
- core
- recording medium
- magneto
- 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.)
- Pending
Links
Landscapes
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
この発明は、光磁気記録用励磁素子に関するものである
。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an excitation element for magneto-optical recording.
(従来の技術0
従来、この種の光磁気記録用励磁素子として、特開昭6
2−172504号公報に示されるように、左右対称の
E型のコアよりなる励磁素子が提案されている。(Conventional technology 0) Conventionally, as this type of excitation element for magneto-optical recording,
As shown in Japanese Patent No. 2-172504, an excitation element having a laterally symmetrical E-shaped core has been proposed.
第2図に励磁素子を光磁気記録ディスク装置に設けた時
の媒体および光学系との配置を示す0図において、(1
)は励磁素子で(2)の主コア、(3a)、(3b)の
補助コア、(4)のコイルより構成される。(6)はデ
ィスク媒体で−あり、(7)の磁化層と(8)の基板よ
り構成される。In Figure 2, which shows the arrangement of the medium and optical system when an excitation element is provided in a magneto-optical recording disk device, (1
) is an excitation element consisting of a main core (2), auxiliary cores (3a) and (3b), and a coil (4). (6) is a disk medium, which is composed of a magnetic layer (7) and a substrate (8).
(9)は光収束用の対物レンズ、(10)はレーザー光
源である。(5a)、(5b)は主コアより発生する磁
界のベクトルである。(9) is an objective lens for converging light, and (10) is a laser light source. (5a) and (5b) are vectors of the magnetic field generated from the main core.
次に動作について説明する。光磁気記録は一最に、レー
ザー光をレーザー光源(10)より発生させ光収束用の
対物レンズ(9)を通して、ディスク媒体の磁化層(7
)上で、1〜2μm径の微小スポットに絞り、媒体温度
を上昇させると同時にバイアス磁界を印加し、バイアス
磁界方向に磁化された磁区を残すことで、信号を記録す
る。Next, the operation will be explained. In magneto-optical recording, first, a laser beam is generated from a laser light source (10), passes through an objective lens (9) for converging the light, and is applied to a magnetic layer (7) of a disk medium.
), a minute spot with a diameter of 1 to 2 μm is focused, a bias magnetic field is applied at the same time as the medium temperature is raised, and a signal is recorded by leaving a magnetic domain magnetized in the direction of the bias magnetic field.
励磁素子(1)のコイル(4)に電流を流すことで、主
コア(2)より、(5a)、(5b)のバイアス磁界を
発生させる。なお、コアの効率を上げるために、補助コ
ア(3a)、(3b)を1コアの左右に設け、空気中の
磁路長を短くしている。By passing current through the coil (4) of the excitation element (1), bias magnetic fields (5a) and (5b) are generated from the main core (2). In addition, in order to increase the efficiency of the core, auxiliary cores (3a) and (3b) are provided on the left and right sides of one core to shorten the length of the magnetic path in the air.
(発明が解決しようとする問題点)
従来のE型のコアよりなる励磁素子は主コアの左右に補
助コアがあるためコアが大型化するだけでなく、構造が
複雑になりその加工も容易でなくなるなどの問題点があ
った。(Problems to be Solved by the Invention) The conventional excitation element with an E-shaped core has auxiliary cores on the left and right sides of the main core, which not only increases the size of the core, but also makes the structure complex and difficult to process. There were some problems, such as it disappearing.
一方、図3に示すようなINTERNATI○NAL
SYNPO3IUM ON 0PTICAL
MEMORY 1987 P2N2で提案された励
磁素子は補助コアが1個であるため、補助コアから離れ
た点の主コア上の磁界(5b)はど小さくなり、磁界分
布の均一性などに問題点があった。On the other hand, INTERNATI○NAL as shown in Figure 3
SYNPO3IUM ON 0PTICAL
MEMORY 1987 Since the excitation element proposed in P2N2 has one auxiliary core, the magnetic field (5b) on the main core at a point away from the auxiliary core becomes very small, causing problems such as the uniformity of the magnetic field distribution. Ta.
この発明は上記のような問題点を解消するためになされ
たもので、小型で加工性も良く磁界分布が均一でコア効
率の良い励磁素子を得ることを目的としている。This invention was made to solve the above-mentioned problems, and aims to provide an excitation element that is small, has good workability, has a uniform magnetic field distribution, and has a high core efficiency.
(問題点を解決するための手段)
この発明に係わるわる光磁気記録用励磁素子は主コアと
、その側部に配置される補助コアより措成し、記録媒体
面に対向する主コアが、記録媒体面と平行になる面と非
平行になる面を有するようしたものである。(Means for Solving the Problems) A magneto-optical recording excitation element according to the present invention is composed of a main core and an auxiliary core disposed on the side thereof, and the main core facing the recording medium surface is It has a surface that is parallel to the surface of the recording medium and a surface that is not parallel to the surface of the recording medium.
(作用)
この発明における光磁気記録用励磁素子は、記録媒体面
に対向する主コアが、記録媒体面と平行になる面と非平
行になる面を有することで、分布が均一のバイアス磁界
を効率良く発生できる。(Function) The excitation element for magneto-optical recording according to the present invention has a main core facing the recording medium surface, which has a surface parallel to the recording medium surface and a surface nonparallel to the recording medium surface, so that a bias magnetic field with a uniform distribution can be generated. It can be generated efficiently.
(実施例)
以下、この発明の一実施例を図について説明する。第1
図において、(1)は励磁素子で(2)の主コア、(3
)の補助コア、(4)のコイルより構成される。(20
1)は、記録媒体面と平行になる面、(202)は補助
コアの反対側に設けられた非平行になる面である。(6
)はディスク媒体であり、(7)の磁化層と(8)の基
板より構成される。(9)は光収束用の対物レンズ、(
10)はレーザー光源である。(5a)、(5b)、(
5b’ )は主コアの記録媒体面と平行になる面より、
(5c)は非平行になる面より発生する磁界のベクトル
である。(Example) Hereinafter, an example of the present invention will be described with reference to the drawings. 1st
In the figure, (1) is an excitation element, (2) is the main core, (3 is
It consists of an auxiliary core () and a coil (4). (20
1) is a surface that is parallel to the recording medium surface, and (202) is a non-parallel surface provided on the opposite side of the auxiliary core. (6
) is a disk medium, which is composed of a magnetic layer (7) and a substrate (8). (9) is the objective lens for light convergence, (
10) is a laser light source. (5a), (5b), (
5b') from the plane parallel to the recording medium surface of the main core,
(5c) is the vector of the magnetic field generated by the non-parallel surfaces.
次に動作について説明する。記録および消去の原理は従
来例と同じ<(10)のレーザー光源より発生するレー
ザー光を対物レンズ(9)を用いてディスク媒体(6)
の磁化層(7)上で1〜2μm径の微小スポットに絞り
、媒体温度を上昇させると同時にバイアス磁界を印加し
、バイアス磁界方向に磁化された磁区を残すことで、信
号を記録する。磁化層に反転磁区を形成することで、記
録を行う。Next, the operation will be explained. The principles of recording and erasing are the same as in the conventional example. Laser light generated from a laser light source (10) is transferred to a disk medium (6) using an objective lens (9).
A signal is recorded by narrowing the spot to a minute spot with a diameter of 1 to 2 μm on the magnetization layer (7), increasing the medium temperature and simultaneously applying a bias magnetic field to leave a magnetic domain magnetized in the direction of the bias magnetic field. Recording is performed by forming reversed magnetic domains in the magnetization layer.
バイアス磁界は主コア(2)の記録媒体面と平行になる
面(201)より(5a)、(5b)、非平行になる面
(202)より、(5c)が発生する。補助コアから離
れた点の磁界(5b)は(5C)が加算され(5a)と
ほぼ同じ強度の磁界(5b’ )を発生させることがで
きるので(201)上の磁界分布を均一化することがで
きる。Bias magnetic fields (5a) and (5b) are generated from the surface (201) of the main core (2) that is parallel to the recording medium surface, and (5c) is generated from the non-parallel surface (202). Since (5C) is added to the magnetic field (5b) at a point away from the auxiliary core, it is possible to generate a magnetic field (5b') with almost the same strength as (5a), so the magnetic field distribution on (201) can be made uniform. Can be done.
また、補助コアにより空気中の磁路長が短くなっている
コアの効率は高い。In addition, the efficiency of the core is high because the magnetic path length in the air is shortened by the auxiliary core.
なお、上実施例では、コイルが主コアに巻かれている場
合について述べたが、補助コアに巻かれていても、その
効果は変わらない。In the above embodiment, the case where the coil is wound around the main core has been described, but the effect remains the same even if the coil is wound around the auxiliary core.
(発明の効果)
以上のように、この発明によれば、補助コアを有するこ
とで効率良く、主コアが、記録媒体面と並行になる面と
非並行になる面を有することで、分布が均一のバイアス
磁界を発生できる効果がある。(Effects of the Invention) As described above, according to the present invention, the distribution can be improved efficiently by having the auxiliary core, and by having the main core have a surface that is parallel to the surface of the recording medium and a surface that is not parallel to the surface of the recording medium. This has the effect of generating a uniform bias magnetic field.
第1図は、この発明の一実施例による励磁素子を示す側
面図、第2図、第3図は従来の励磁素子を示す側面図で
ある。(1)は励磁素子で(2)は主コア、(3)は補
助コア、(4)はコイルである。
なお、図中、同一符号は同一、または相当部分を示す。FIG. 1 is a side view showing an excitation element according to an embodiment of the present invention, and FIGS. 2 and 3 are side views showing conventional excitation elements. (1) is an excitation element, (2) is a main core, (3) is an auxiliary core, and (4) is a coil. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
る光磁気記録ディスク装置のバイアス磁界発生用コアに
おいて、記録媒体面に対向する主コアが、記録媒体面と
平行になる面と非平行になる面を有することを特徴とす
る光磁気記録用励磁素子。In a bias magnetic field generation core of a magneto-optical recording disk device, which is composed of a main core and an auxiliary core placed on the side thereof, the main core facing the recording medium surface is not parallel to the surface parallel to the recording medium surface. An excitation element for magneto-optical recording, characterized by having parallel surfaces.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP33343087A JPH01173402A (en) | 1987-12-28 | 1987-12-28 | Exciting element for magneto-optical recording |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP33343087A JPH01173402A (en) | 1987-12-28 | 1987-12-28 | Exciting element for magneto-optical recording |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01173402A true JPH01173402A (en) | 1989-07-10 |
Family
ID=18266021
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP33343087A Pending JPH01173402A (en) | 1987-12-28 | 1987-12-28 | Exciting element for magneto-optical recording |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01173402A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2676303A1 (en) * | 1991-05-07 | 1992-11-13 | Commissariat Energie Atomique | INTEGRATED MAGNETO-OPTICAL READING AND WRITING HEAD AND METHOD OF MAKING THE SAME |
-
1987
- 1987-12-28 JP JP33343087A patent/JPH01173402A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2676303A1 (en) * | 1991-05-07 | 1992-11-13 | Commissariat Energie Atomique | INTEGRATED MAGNETO-OPTICAL READING AND WRITING HEAD AND METHOD OF MAKING THE SAME |
US5317800A (en) * | 1991-05-07 | 1994-06-07 | Commissariat A L'energie Atomique | Method of making an integrated magnetooptical read and write head |
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