JPH0266701A - Exciting element for magneto-optical recording - Google Patents
Exciting element for magneto-optical recordingInfo
- Publication number
- JPH0266701A JPH0266701A JP21872088A JP21872088A JPH0266701A JP H0266701 A JPH0266701 A JP H0266701A JP 21872088 A JP21872088 A JP 21872088A JP 21872088 A JP21872088 A JP 21872088A JP H0266701 A JPH0266701 A JP H0266701A
- Authority
- JP
- Japan
- Prior art keywords
- core
- magnetic field
- magneto
- optical recording
- coil
- 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
- 230000005284 excitation Effects 0.000 claims description 14
- 230000005381 magnetic domain Effects 0.000 abstract description 3
- 230000017525 heat dissipation Effects 0.000 description 7
- 230000000694 effects Effects 0.000 description 3
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000004898 kneading Methods 0.000 description 1
- 230000005415 magnetization Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 239000013598 vector Substances 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B33/00—Constructional parts, details or accessories not provided for in the other groups of this subclass
- G11B33/14—Reducing influence of physical parameters, e.g. temperature change, moisture, dust
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B11/00—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
- G11B11/10—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
- G11B11/105—Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
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し、特にその熱
放散性の改善に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to an excitation element for magneto-optical recording, and particularly to improvement of its heat dissipation properties.
従来、この糧の光磁気記録用励磁素子として、例えば特
開昭62−172504号公報に示されるように、透磁
率の高い部材をコアとした電磁石を用いることが提案さ
れている。第3図にこのような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。図において、tlli励磁素子であり、主コア(2
)、補助コア(3a) 、(3b)およびコイル(4)
より構成される。(6)はディスク媒体であり、磁化層
(7)と基板(8)より構成される。(9)は光集束用
の対物レンズ、(101Uレーザー光源である。(5g
)、(5b) Uそれぞれ主コア(2)の記録媒体面と
平行および交差する面より発生する磁界のベクトルであ
る。Conventionally, as an excitation element for magneto-optical recording, it has been proposed to use an electromagnet having a core made of a material with high magnetic permeability, as disclosed in, for example, Japanese Patent Laid-Open No. 172504/1983. FIG. 3 shows the arrangement of a medium and an optical system when such an excitation element is provided in a magneto-optical recording disk device. In the figure, it is the tlli excitation element, and the main core (2
), auxiliary cores (3a), (3b) and coils (4)
It consists of (6) is a disk medium, which is composed of a magnetic layer (7) and a substrate (8). (9) is an objective lens for light focusing, (101U laser light source. (5g
), (5b) U are vectors of magnetic fields generated from planes parallel to and intersecting the recording medium plane of the main core (2), respectively.
次に動作について説明する。光磁気記録a一般に、レー
ザー光をレーザー光源(101より発生させ光集束用の
対物レンズ(9)ヲ通して、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. Magneto-optical recording a Generally, a laser beam is generated from a laser light source (101) and passed through an objective lens (9) for focusing the light to record the magnetic layer (7) of the 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11)のコイル(4)に電流を流すことで、主
コア(2)より磁界(5a) 、(5b)を発生させる
。なお、コアの効率を上げるために、補助コア(3m)
、(3b)を主コアの左右に設け、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 11), magnetic fields (5a) and (5b) are generated from the main core (2). In addition, in order to increase the efficiency of the core, an auxiliary core (3m)
, (3b) are provided on the left and right sides of the main core to shorten the magnetic path length in the air.
以上のように構成され念従来の光磁気記録用励磁素子で
に、主コア(2)および補助コア(3a)−(3b)が
熱伝導率の低いフェライトで形成されるのが一般的であ
り、電流印加時に発生する熱が素子より放散しにくいた
め、素子の温度を上昇させ、発生磁界強度が不安定にな
ることがあるという問題点があった。In the conventional excitation element for magneto-optical recording constructed as described above, the main core (2) and the auxiliary cores (3a)-(3b) are generally formed of ferrite having low thermal conductivity. However, since the heat generated when a current is applied is more difficult to dissipate than the element, there is a problem in that the temperature of the element increases and the strength of the generated magnetic field may become unstable.
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、小型で大電流印加時にも温度上昇が少ない光
磁気記録用励磁素子を提供することを目的とする。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide an excitation element for magneto-optical recording that is small and has a small temperature rise even when a large current is applied.
この発明に係る光磁気記録用励磁素子は、バイアス磁界
発生用コア、上記コアを励磁するコイルおよび上記コア
の少なくとも一面に密着配置された放熱部材分備えたも
のである。The excitation element for magneto-optical recording according to the present invention includes a core for generating a bias magnetic field, a coil for exciting the core, and a heat dissipation member disposed in close contact with at least one surface of the core.
〔作用〕
この発明における放熱部材は、磁界発生時にコイルにお
いて発生した熱を周囲に放散するので、バイアス磁界発
生用コア等の温度上昇が低減される。[Function] The heat dissipation member of the present invention dissipates the heat generated in the coil when a magnetic field is generated to the surroundings, thereby reducing the temperature rise of the bias magnetic field generation core and the like.
以下、この発明の一実施例を図をもとに説明する。第1
図において、(Illi放熱部材であり、例えばアルミ
ニウムや銅などの金属で形成され、主コア(2)詔よび
補助コア(3a)=(3b)の3面に密着配置されてい
る。An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, (Illi) is a heat dissipating member, made of metal such as aluminum or copper, and is arranged in close contact with three sides of the main core (2) and the auxiliary cores (3a) and (3b).
次に動作について説明する。記録及び消去の原理は従来
例と同じく、レーザー光源[10)より発生するレーザ
ー光を対物レンズ(9)ヲ用いてディスク媒体(6)の
磁化層(7)上で1〜27m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、
磁化層(7)に反転磁区を形成することで、記録を行な
う。Next, the operation will be explained. The principle of recording and erasing is the same as in the conventional example, using a laser beam generated from a laser light source [10] to create a minute spot with a diameter of 1 to 27 m on the magnetic layer (7) of the disk medium (6) using the objective lens (9). Narrow it down to
Applying a bias magnetic field at the same time as increasing the medium temperature,
Recording is performed by forming reversed magnetic domains in the magnetization layer (7).
磁界発生時にコイル(4)において発生した熱に主コア
(2)及び補助コア(3)に伝わり、さらに熱伝導率の
高い放熱部材(11)に伝わり周囲に放散される之め、
主コア(2)及びコイル(4)の温度上昇が低減される
。The heat generated in the coil (4) when a magnetic field is generated is transmitted to the main core (2) and the auxiliary core (3), further transmitted to the heat dissipation member (11) with high thermal conductivity, and dissipated to the surroundings.
Temperature increases in the main core (2) and coil (4) are reduced.
なお、上記実施例では主コア(2)および補助コア(3
a ) 、 (3b)の3面に放熱部材(II)が密着
配置されている場合について示したが、こねに限るもの
でばなく、例えば第2図に示すように一面のみに密着配
置されていてもよく、上記実施例と同様の効果が得られ
る。In the above embodiment, the main core (2) and the auxiliary core (3)
Although the case in which the heat dissipation member (II) is closely placed on the three sides of a) and (3b) is shown, this is not limited to kneading. The same effect as in the above embodiment can be obtained.
また、上記実施例でにコイル(4)が主コア(2)に巻
かれている場合について示したが、補助コア(3m)。In addition, although the above embodiment shows the case where the coil (4) is wound around the main core (2), the auxiliary core (3 m) is used.
(3b)に巻かれていてもよい。さらに、補助コア(3
a)、(3b)が無い場合にもこの発明に適用できる。(3b) may be wound. In addition, the auxiliary core (3
This invention can also be applied to cases where a) and (3b) are not present.
以上のように、この発明によれば、バイアス磁界発生用
コア、上記コアを励磁するコイル、および上記コアの少
なくとも一面に密着配置された放熱部材分備えたので、
大電流印加時にも温度上昇が少なく、発生磁界強度の安
定した光磁気記録用励磁素子が得られる効果がある。As described above, according to the present invention, the core for generating a bias magnetic field, the coil for exciting the core, and the heat dissipation member disposed in close contact with at least one surface of the core are provided.
This has the effect of providing an excitation element for magneto-optical recording in which the temperature rise is small even when a large current is applied, and the strength of the generated magnetic field is stable.
第1図はこの発明の一実施例による光磁気記録用励磁素
子を示す斜視図、第2図はこの発明の他の実施例による
光磁気記録用励磁素子を示す斜視図、第3図に従来の光
磁気記録用励磁素子を示す斜視図である。
図において、fi+は励磁素子、(2)ぼ主コア、(3
a)。
(3b)H補助コア、[41iコイル、(61fiディ
スク媒体、(9)は対物レンズ、(lO)はレーザー光
源、(ll)に放熱部材である。
なお、図中、同一符号に同一またに相当部分を示す。FIG. 1 is a perspective view showing an excitation element for magneto-optical recording according to one embodiment of the present invention, FIG. 2 is a perspective view showing an excitation element for magneto-optical recording according to another embodiment of the invention, and FIG. 3 is a perspective view showing a conventional excitation element for magneto-optical recording. FIG. 2 is a perspective view showing an excitation element for magneto-optical recording. In the figure, fi+ is an exciting element, (2) main core, (3
a). (3b) H auxiliary core, [41i coil, (61fi disk medium), (9) is an objective lens, (lO) is a laser light source, and (ll) is a heat dissipation member. A considerable portion is shown.
Claims (1)
および上記コアの少なくとも一面に密着配置された放熱
部材を備えた光磁気記録用励磁素子。A core for generating a bias magnetic field, a coil that excites the core,
and an excitation element for magneto-optical recording, comprising a heat dissipating member closely disposed on at least one surface of the core.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21872088A JPH0266701A (en) | 1988-08-31 | 1988-08-31 | Exciting element for magneto-optical recording |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21872088A JPH0266701A (en) | 1988-08-31 | 1988-08-31 | Exciting element for magneto-optical recording |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0266701A true JPH0266701A (en) | 1990-03-06 |
Family
ID=16724383
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21872088A Pending JPH0266701A (en) | 1988-08-31 | 1988-08-31 | Exciting element for magneto-optical recording |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0266701A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113046743A (en) * | 2021-02-05 | 2021-06-29 | 江苏大学 | Device and method for magnetic field assisted ultrahigh-speed laser cladding of pipe coatings |
-
1988
- 1988-08-31 JP JP21872088A patent/JPH0266701A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113046743A (en) * | 2021-02-05 | 2021-06-29 | 江苏大学 | Device and method for magnetic field assisted ultrahigh-speed laser cladding of pipe coatings |
CN113046743B (en) * | 2021-02-05 | 2022-05-20 | 江苏大学 | Device and method for magnetic field assisted ultrahigh-speed laser cladding of pipe coatings |
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