JPS607634A - Photothermomagnetic recording medium - Google Patents

Photothermomagnetic recording medium

Info

Publication number
JPS607634A
JPS607634A JP11496383A JP11496383A JPS607634A JP S607634 A JPS607634 A JP S607634A JP 11496383 A JP11496383 A JP 11496383A JP 11496383 A JP11496383 A JP 11496383A JP S607634 A JPS607634 A JP S607634A
Authority
JP
Japan
Prior art keywords
magnetic
film
recording medium
recording
sides
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
Application number
JP11496383A
Other languages
Japanese (ja)
Inventor
Hiroyoshi Kishi
博義 岸
Masaaki Matsushima
正明 松島
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP11496383A priority Critical patent/JPS607634A/en
Publication of JPS607634A publication Critical patent/JPS607634A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • G11B11/10Recording 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
    • G11B11/105Recording 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
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording 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
    • G11B11/10Recording 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
    • G11B11/105Recording 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
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10586Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 本発明は光磁気メモリー、磁気記録・表示素子などに用
いられ、磁8気カー効果、7アラデー効果などの磁気光
学効果を用いて読み出すことのできる光熱磁気記録媒体
に関するもので、特に両面からの記録再生が可能な磁性
薄膜記録幼体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magneto-optical recording medium that is used in magneto-optical memories, magnetic recording/display elements, etc. and can be read using magneto-optic effects such as the magneto-8 Kerr effect and the Alladay effect. In particular, the present invention relates to a magnetic thin film recording medium capable of recording and reproducing information from both sides.

従来、光熱磁気記録媒体としては、MnBi、MnCu
B1等の多結晶薄膜−1GdIG等の、・単結晶薄膜、
GdCo 、 GdFe 、TbFe、GdTbFe 
、TbFeC!o 、 CdTbFeCo等の非晶質薄
膜等が知ら′れている。
Conventionally, as photothermal magnetic recording media, MnBi, MnCu
Polycrystalline thin film such as B1 - Single crystalline thin film such as 1GdIG,
GdCo, GdFe, TbFe, GdTbFe
, TbFeC! Amorphous thin films such as CdTbFeCo and CdTbFeCo are known.

これら光熱磁気記録媒体の記録法は、まず記録媒体を、
磁性膜を飽和させるのに充分な磁場の中において、一方
向に磁化させておき、記録したい部分を、レーザ光等に
より照射加熱してその部分の磁化を消失もしくは減少さ
せ、冷却時に外部印加磁場、もしくは、周囲媒体からの
もれ磁界によりその部分の磁化の向きを反転させること
により行なわれる。
In the recording method of these photothermal magnetic recording media, first, the recording medium is
The area to be recorded is magnetized in one direction in a magnetic field sufficient to saturate the magnetic film, and the area to be recorded is irradiated and heated with a laser beam, etc. to eliminate or reduce the magnetization of that area, and when cooled, an externally applied magnetic field is applied. Alternatively, this can be done by reversing the direction of magnetization in that part using a leakage magnetic field from the surrounding medium.

再生1法は、レーザ光等の記録に使用した照射パワーよ
り小さいパワーで偏光r−を通して記録部(垂直磁性膜
)に照射する。この時の反射光(あるいは透過光)の偏
光面が磁化の向きに応して、右または左に回転するから
、これを検光子を通ず事により、磁、化の向きのちがい
による丸頃の差異が生じ、この光量を光検出器で電気信
号に変換することにより行なわれる。
In the reproduction method 1, the recording section (perpendicular magnetic film) is irradiated with polarized light r- at a power smaller than the irradiation power used for recording, such as a laser beam. At this time, the polarization plane of the reflected light (or transmitted light) rotates to the right or left depending on the direction of magnetization, so by passing it through an analyzer, it is possible to rotate the polarization plane depending on the direction of magnetization. This is done by converting this amount of light into an electrical signal using a photodetector.

第11図に光熱磁気記録媒体の記録再生装置の構成を示
す。記録媒体1は、モーター2で回転駆動され半動体レ
ーザー3から発したソCは、コリメーターレンズ4で平
行光束となる。5はビームスプリッタで入射光と反射光
を分離するものである。
FIG. 11 shows the configuration of a recording/reproducing apparatus for a photothermal magnetic recording medium. The recording medium 1 is rotationally driven by a motor 2, and the beam C emitted from the semi-moving body laser 3 is turned into a parallel light beam by the collimator lens 4. A beam splitter 5 separates incident light and reflected light.

6は才波長板であり入射光束は集光レンズ7により微小
スポットとなって記録媒体に当り記録される。一方記録
媒体からの反射光はビームスプリッタ−より、取り出さ
れフォーカス制御器18により記録媒体面上の入射光束
の焦点を合わせるフォーカスサーボに利用される。16
は磁石であり、その磁場は、記録媒体の保磁力よりは小
さく、記録媒体の磁性膜の磁化方向と反対になる様に記
録媒体に印加されており、磁場の大きさにより記録媒体
の見かけの感度が向上する。再生は、半導体レーザー6
′から発した光が、コリメーターレンズ4′で平行光束
となり、6′は偏光子で光束を直接偏光とし、記録媒体
1に入射させる。5′はビームスプリッタ−で、入射光
と記録媒体からの反射光を分離するものである。入射光
束は、集光レンズ7′によす微小スポットとなって記録
媒体1に当り、記録媒体の磁化方向に対応して、その偏
光面をカー効果によってθk(カー回転角)あるいは、
−θに回転して反射される。この反射光は、ビームスプ
リッタ−5′によって取り出され、ノ1−7ミラー8に
よって2方向に分割される。分割された光束は、それぞ
れ検光子9.10、集光レンズ11.12を通り、光検
出器16.14、に導びかれ、電気信号として取り出さ
れる。このような2つの電気信号は差動増幅器15で差
分を取り、情報再生信号として取り出される。17は消
却用の磁石であり、その磁場の大きさは、媒体の保磁力
よりは小さく、その磁場の向きは、媒体を一様に磁化し
た向きと同じ方向である。消去は、消去用磁石1.7を
基板に近づけ、記録された領域(磁化反転部分)にレー
ザ光を照射し、冷却時に消去用磁石による磁場により、
もとの方向に磁化がそろうことにより実現される。
Reference numeral 6 denotes a wavelength plate, and the incident light beam is turned into a minute spot by a condensing lens 7 and is recorded on a recording medium. On the other hand, the reflected light from the recording medium is taken out by a beam splitter and used by a focus controller 18 for focus servo to focus the incident light beam on the surface of the recording medium. 16
is a magnet, and its magnetic field is applied to the recording medium in such a way that it is smaller than the coercive force of the recording medium and is opposite to the magnetization direction of the magnetic film of the recording medium.The size of the magnetic field changes the apparent appearance of the recording medium. Sensitivity is improved. Reproduction is performed using semiconductor laser 6
The light emitted from ' is converted into a parallel light beam by a collimator lens 4 ′, and the light beam is directly polarized by a polarizer 6 ′, and is made incident on the recording medium 1 . 5' is a beam splitter that separates incident light and reflected light from the recording medium. The incident light flux hits the recording medium 1 as a minute spot on the condensing lens 7', and the plane of polarization is changed by the Kerr effect to θk (Kerr rotation angle) or
It is rotated to -θ and reflected. This reflected light is taken out by a beam splitter 5' and split into two directions by a No. 1-7 mirror 8. The divided light beams pass through an analyzer 9.10 and a condenser lens 11.12, respectively, and are guided to a photodetector 16.14, where they are extracted as electrical signals. The difference between these two electrical signals is taken by a differential amplifier 15, and the difference is taken out as an information reproduction signal. Reference numeral 17 denotes an extinction magnet, and the magnitude of its magnetic field is smaller than the coercive force of the medium, and the direction of the magnetic field is the same as the direction in which the medium is uniformly magnetized. Erasing is carried out by bringing the erasing magnet 1.7 close to the substrate, irradiating the recorded area (magnetization reversal area) with a laser beam, and using the magnetic field of the erasing magnet during cooling.
This is achieved by aligning the magnetization in the original direction.

このような記録媒体において、その1枚当りのでいるた
め、両面の磁性膜が同じ種類の膜ならば、磁化した場合
、第2図に示す様に両面とも同一方向に磁化されること
になる。そのため、記録時に、外部磁場を印加する時は
、片面毎に印加する磁場の向きを逆にしなければならな
い。また消去時も片面毎に印加する磁場の向きを逆にし
なければならない。また、再生時には、記録ドツトの出
力が、片面毎に正負逆になるため1、実際には、どちら
の而であるかを検出した上で、電気信号を処理する様玉
夫しなければなうない。
In such a recording medium, if the magnetic films on both sides are of the same type, both sides will be magnetized in the same direction as shown in FIG. Therefore, when applying an external magnetic field during recording, the direction of the applied magnetic field must be reversed for each side. Also, during erasing, the direction of the magnetic field applied to each side must be reversed. Also, during playback, the output of the recording dots is reversed for each side (1), so in reality, it is necessary to detect which side the output is and then process the electrical signal. .

本発明の目的は、両面からの記録再生が可能な光熱磁気
記録媒体であって、片面毎の記録時および消去時の外部
印加磁場の向きの反転や、再生時の電気信号処理の反転
のわずられしさのない垂直磁性膜を有する新規な光熱磁
気記録媒体を提供することである。
An object of the present invention is to provide a photothermal magnetic recording medium capable of recording and reproducing from both sides, which is capable of reversing the direction of an externally applied magnetic field during recording and erasing on each side, and reversing electrical signal processing during reproduction. An object of the present invention is to provide a novel photothermal magnetic recording medium having a perpendicular magnetic film that does not shift.

本発明は基板の両面に、面に垂直な磁化容易軸を有する
磁性膜が形成されてお刊、且その両磁性膜の組成が、丁
度室温におけ°る磁気補償組成の両側の組成の関係にあ
ることを、特徴とする光熱磁気記録媒体である。
In the present invention, magnetic films having easy magnetization axes perpendicular to the surfaces are formed on both sides of the substrate, and the compositions of both magnetic films are exactly related to the composition on both sides of the magnetic compensation composition at room temperature. This is a photothermal magnetic recording medium characterized by the following.

本発明において、両磁性膜の組成が1丁度室温における
磁気補償組成の両側の′組成の関係であると は、たと
えば、Ga、 Tb、 Dy等あるいはそれらの合金で
ある希土類と、Fe 、 Co等あるいはそれらの合金
である遷移金属との非晶質磁性膜を用いた場合は、面部
記録媒体のある一面は、希土類−・遷移金属垂直磁性膜
の補償組成に対して磁気的に希土類リンチな組成であり
、他の面は逆に磁気的に遷移金属リッチな組成であれば
よい。
In the present invention, the relationship between the compositions of both magnetic films on both sides of the magnetic compensation composition at room temperature means, for example, rare earth elements such as Ga, Tb, Dy, or alloys thereof, and rare earth elements such as Fe, Co, etc. Alternatively, in the case of using an amorphous magnetic film with a transition metal that is an alloy of these, one surface of the planar recording medium has a composition that magnetically has a rare earth lynchium with respect to the compensation composition of the rare earth-transition metal perpendicular magnetic film. On the other hand, the other surfaces only need to have a composition that is magnetically rich in transition metals.

本発明における両磁性膜の組成は、上記の如く丁度室温
における磁気補償組成の両側の組成の関係であればよい
が、実用的にはその保磁力の大きさは10KOe以下で
あるものが望ましく、一方その磁化の大きさは、膜面に
垂直な磁化容易軸を有する磁性膜が形成される程度の大
きさであることが必要である。
The compositions of both magnetic films in the present invention may be just the relationship between the compositions on both sides of the magnetic compensation composition at room temperature as described above, but in practical terms, it is desirable that the coercive force is 10 KOe or less. On the other hand, the magnitude of the magnetization must be such that a magnetic film having an axis of easy magnetization perpendicular to the film surface is formed.

本発明の光熱磁気記録媒体は、このように基板の両面の
磁性膜の組成が、丁度室温における磁気補償組成の両側
の組成の関係になっているので、これをN極、S極が対
向した磁極の間隙にはさみ、強い磁場を加えると、第4
図に示すように、両面の磁化の向きが互に逆向きの関係
になる。従って、この記録媒体を用いて第1図に示した
様な装置で記録再生を行なうと、記録媒体の両面のどち
らを使用する場合も、記録は磁石16の磁場の向きを変
えることなく、再生も記録部がどちらの面であるかを検
出した上で記録ドツトの出力が逆にならないように電気
信号処理を施こすことなく、また消去時も消去用磁石1
7の磁場の向きを変えることな〈実施できるので使用時
のわずられしさが全く解消される。
In the photothermal magnetic recording medium of the present invention, the compositions of the magnetic films on both sides of the substrate are in the same relationship as the compositions on both sides of the magnetic compensation composition at room temperature. When placed between the magnetic poles and applying a strong magnetic field, a fourth
As shown in the figure, the directions of magnetization on both sides are opposite to each other. Therefore, if this recording medium is used for recording and reproduction in an apparatus such as that shown in FIG. After detecting which side the recording section is on, no electrical signal processing is performed to prevent the output of the recording dots from being reversed, and the erasing magnet 1 is also used during erasing.
Since it can be carried out without changing the direction of the magnetic field in step 7, the troublesomeness during use is completely eliminated.

以下、実施例に基いて本発明を更に説明する。The present invention will be further explained below based on Examples.

実施例1 高周波スパッタ装置において、100wnψ、厚み1゜
2wnの白板ガラスを基板とし、第1のターゲットとし
て4インチψのT t)2 o F es o合金と第
2のターゲットとして4インチψのTb25Fe75合
金を使用して成膜を行なった。チャンバー内を1.5X
10P&以下になるまで真空排気した後、Arガスを4
×10“2P2Lまで導入し、真空排気系のメインバル
ブを操作することにより、Ar圧を3Paにした。高周
波電源よりまず第1のターゲットにスパッタ電力250
Wと一定として、Tb2゜Fe8゜膜を10001成膜
した。次にガラス基板の裏面に同様の操作で第2の少−
ケラトラ使用しテ’rb、、 5pe7 s膜を100
OA成膜した9、第6:図(a)にTb2゜Fe@o膜
の、第6図(b) ニTb25 F e75膜の極力−
効果による磁気ヒステリシスを示−$2. TbFe膜
の補償組成は、Tbが22at□rr+%のところであ
るから、Tb2oFe8o膜は、磁気的にFe ric
hな組成膜、Tt)2 s Fa7s膜は、磁気的にT
b richな膜テアリ、両面の膜とも保磁力IKOe
の垂直磁性膜であった。尚、第6図(a)および(b)
において、横軸は保磁力の大きさを、たて軸は磁性膜の
極力−効果による光検出器の出力の大きさを表わしてお
り、図中にそれぞれI KOeの大きさを示しである。
Example 1 In a high frequency sputtering device, a white plate glass of 100 wn ψ and a thickness of 1°2 wn was used as a substrate, a Tt)2 o F es o alloy of 4 inch ψ was used as the first target, and Tb25Fe75 of 4 inch ψ was used as the second target. The film was formed using an alloy. 1.5X inside the chamber
After evacuation to 10P& or less, Ar gas was evacuated to 4
By introducing up to ×10" 2P2L and operating the main valve of the vacuum exhaust system, the Ar pressure was set to 3 Pa. First, the first target was sputtered with a power of 250
Assuming that W was constant, 10,001 Tb2°Fe8° films were formed. Next, apply a second layer to the back side of the glass substrate in the same manner.
Using Keratra Te'rb,, 5pe7s membrane 100
OA film-formed 9, No. 6: Figure (a) shows the Tb2°Fe@o film, and Figure 6 (b) shows the Tb25Fe75 film as much as possible.
Showing magnetic hysteresis due to effect - $2. Since the compensation composition of the TbFe film is that Tb is 22at□rr+%, the Tb2oFe8o film is magnetically Fe ric
h composition film, Tt)2s Fa7s film is magnetically T
b rich film tear, coercive force IKOe for both films
It was a perpendicular magnetic film. Furthermore, Fig. 6 (a) and (b)
In the figure, the horizontal axis represents the magnitude of coercive force, and the vertical axis represents the magnitude of the output of the photodetector due to the maximum effect of the magnetic film, and the magnitude of IKOe is shown in each figure.

実際の記録、再生用には、この気録媒体の両面の磁性膜
の上に、保護膜と反射防止j模として、SiOを70O
A成膜して、次にN 4rdj 3極が対向した磁石対
の間隙にはさみ、5KOeの磁場を加えて磁化をした。
For actual recording and reproduction, 70O of SiO is applied as a protective film and anti-reflection layer on the magnetic films on both sides of this air recording medium.
A film was formed, and then N 4rdj three poles were placed in the gap between a pair of opposing magnets and magnetized by applying a magnetic field of 5 KOe.

この時の磁化の向きを第4図に示す。The direction of magnetization at this time is shown in FIG.

録は磁石16の磁場の方向を変えることなしに、また再
生もどちらの面であるかを検出した上で、記録ドツトの
出力が片面毎に逆にならないような特別な電気信号処理
を施こす事なく行なえ、消去も消去用磁石17の磁場の
方向を変えることなしに行なえた。
Recording is performed without changing the direction of the magnetic field of the magnet 16, and after detecting which side is used for reproduction, special electrical signal processing is performed to prevent the output of recording dots from being reversed on each side. The data could be erased without any problems, and erasing was also possible without changing the direction of the magnetic field of the erasing magnet 17.

実施例2 高周波スパッタ装置において、1[]Qmψ厚み1.2
叫の白板ガラスを基板とし、第1のターゲットととして
、4インチψのFe」二に51廁角のGds o T婉
0 合金片を均一に12枚並べたものと、第2のターゲ
ットとして、4イン。チψのFe上に、5關角のGds
 oT v’s 。
Example 2 In a high frequency sputtering device, 1[]Qmψ thickness 1.2
A white glass plate was used as a substrate, a first target was a 4 inch ψ Fe''251 angle Gds o T 婉0 12 uniformly arranged pieces, and a second target was 4 in. Gds of 5 angles on Fe of ψ
oT v's.

合金片を均一に15枚並べたものを使用して成膜を行な
った。実施例1と同様のプロセスでガラス基板の片面に
(Gd5o Tb5o)z+’ Fe79膜を100O
A成膜し、他の面に (Gd5o Tb5o)zs F
eys +dを100OA成膜した。(Gd5o T畑
o)zx Fe7g膜および(G’ao Tb1o )
25 Fe75膜の倹カー効果による磁気ヒステリシス
はそれぞれ第ろ図(a)および第6図(b)の場合と同
様であった(、 GdTbFe膜の補償組成は、(Gd
5o ’ Tb5o)が26atom%のところである
から、(Gd5o Tb50)21 Feys膜は、磁
気的にFor]−Chな組成膜(G45o Ttbo)
25Fey5膜は、磁気的に希土類(GdTb) ri
chな膜であり、両面の膜とも保磁力IKOθの垂直磁
性膜であった。次に保護膜と反射防止膜を兼ねたSiO
を成膜するのであるが、((Jr+o Tt)so)z
t Fe7g膜には反射率が27%になるようにコント
ロールして成膜し、(Gd5oTbs o )25Fe
7−5膜には反射率が22%になる様にコントロールし
て成膜した。これは(Gd5゜Fl)5 o) 2’t
 F e79膜が(G由OT堵0)25Fe75膜に比
較してキューリ一温度が低く、感度的に良いため、反射
時11―膜により両面の感度をそろえたためである。な
お、反射率°の違いによる再生S/Nへの影響はほとん
どなかった。
Film formation was performed using 15 uniformly arranged alloy pieces. A (Gd5o Tb5o)z+' Fe79 film was deposited at 100O on one side of a glass substrate using the same process as in Example 1.
A film was formed and (Gd5o Tb5o)zs F was formed on the other surface.
A 100OA film of eys +d was formed. (Gd5o T field o)zx Fe7g film and (G'ao Tb1o)
The magnetic hysteresis due to the Kerr effect of the 25Fe75 film was similar to that in Figures 6(a) and 6(b), respectively (the compensation composition of the GdTbFe film was (Gd
5o' Tb5o) is around 26 atom%, so the (Gd5o Tb50)21 Feys film is a magnetically For]-Ch composition film (G45o Ttbo)
The 25Fey5 film is magnetically rare earth (GdTb) ri
Both films on both sides were perpendicular magnetic films with coercive force IKOθ. Next, SiO which serves as both a protective film and an anti-reflection film.
((Jr+o Tt)so)z
The tFe7g film was formed by controlling the reflectance to 27%, and (Gd5oTbs o )25Fe
The film 7-5 was formed with a controlled reflectance of 22%. This is (Gd5゜Fl)5 o) 2't
This is because the Fe79 film has a lower Curie temperature and better sensitivity than the (G-derived OT and 0)25Fe75 film, so the sensitivity on both sides was made equal during reflection by the 11-film. Note that there was almost no influence on the reproduced S/N due to the difference in reflectance.

この両面記録媒体を一様に磁°化した後、前述した装置
により記録、再生したところ、記録媒体の1ilq面と
も、記録は磁石16の磁場の方向を変えることなしに、
また再生も、どちらの而であるかを検出した上で記録パ
ターンの出力が片面毎に逆にならないような一特別な電
気信号処理を施こす事なく行なえ、消去も、消去用磁石
の磁場の方向を変えることなしに行なえた。本発明の他
の実施態様茅しては、基板の片面だけに垂直磁性膜を成
膜し、これを2枚、基板側あるいは1.膜面側で貼り合
わせた両面記録媒体でも、その2枚の垂直磁性膜の組成
が室温における補償組成の両側の組成であれば、同様な
効果が表われる。
After uniformly magnetizing this double-sided recording medium, recording and reproduction were performed using the above-mentioned apparatus. As a result, recording was performed on both sides of the recording medium without changing the direction of the magnetic field of the magnet 16.
In addition, playback can be performed without special electrical signal processing that detects which side the recording pattern is on and prevents the output of the recorded pattern from being reversed for each side, and erasing can also be performed using the magnetic field of the erasing magnet. This was done without changing direction. In another embodiment of the present invention, a perpendicular magnetic film is formed on only one side of the substrate, and two perpendicular magnetic films are formed on the substrate side or one side. Even in a double-sided recording medium that is bonded together on the film side, a similar effect will appear if the compositions of the two perpendicular magnetic films are on both sides of the compensation composition at room temperature.

このように本発明によれば、両面記録媒体の各面に垂直
な磁化容易軸を存する垂直磁性膜が形成され、その両垂
直磁性膜の組成が室温における補償組成の両側の組成で
あるかキ光熱磁気記録媒体を用いることにより片面毎の
記録時や消去時の外部印加磁場の向きの反転や再生時の
電気信号処理の反転のわずられしさなしで、記録再生可
能な両面記録媒体を提供できる。
As described above, according to the present invention, perpendicular magnetic films having perpendicular easy magnetization axes are formed on each side of a double-sided recording medium, and it is possible to determine whether the compositions of both perpendicular magnetic films are on both sides of the compensation composition at room temperature. By using a photothermal magnetic recording medium, we provide a double-sided recording medium that allows recording and reproduction without the hassle of reversing the direction of an externally applied magnetic field during recording or erasing on each side, or reversing electrical signal processing during reproduction. can.

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

第1歯は光熱磁気記録媒体を用いた記録再生装置を説明
するための概念図である。 12図は従来の両面記録用光熱磁気記録媒体を磁化した
ときの磁化方向を示す模式図である。 第4図は本発明ゐ両面記録用光熱磁気記録媒体を磁化し
たときの磁化方向を示す模式図である。 第6図は本発明の実施例の磁性膜の室温における磁気カ
ー効果によるヒ、ステリシス曲線である。 1・・・・・・・・・光熱磁気記録媒体2・・・・・・
・・・モーター 6.6′・・・半導体レーザ 4.4¥・・・コリメータレンズ 5.5′・・・ビームスプリッタ− 6・・・・・・・・・1//4波長板 6′・・・・・・偏光子 7.7′・・・集光レンズ 8・・・・・・・・・ハーフミラ− 9,10・・・検光子 11、12・・・集光レンズ 13.14・・・光検出器 15・・・・・・差動増幅器 16・・・・・・記録用磁石 17・・・・・・消却用磁石 18・・・・・・フォーカス制御器 特許出願人 キャノン株式会社
The first tooth is a conceptual diagram for explaining a recording/reproducing device using a photothermal magnetic recording medium. FIG. 12 is a schematic diagram showing the magnetization direction when a conventional double-sided recording photothermal magnetic recording medium is magnetized. FIG. 4 is a schematic diagram showing the direction of magnetization when the photothermal magnetic recording medium for double-sided recording according to the present invention is magnetized. FIG. 6 is a steresis curve due to the magnetic Kerr effect at room temperature of the magnetic film of the example of the present invention. 1......Photothermal magnetic recording medium 2...
...Motor 6.6'...Semiconductor laser 4.4\...Collimator lens 5.5'...Beam splitter 6...1/4 wavelength plate 6' ...Polarizer 7.7'...Condensing lens 8...Half mirror 9, 10...Analyzer 11, 12...Condensing lens 13.14 ... Photodetector 15 ... Differential amplifier 16 ... Recording magnet 17 ... Erasing magnet 18 ... Focus controller patent applicant Canon Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 基板の両面に、面に垂直な磁化容易軸を有する磁性膜が
形成されており、I4.該両磁性膜の組成が丁度室温に
おける磁気補償組成の両側の組成の関係にあることを特
徴とする光熱、磁気記録媒体。
Magnetic films having easy magnetization axes perpendicular to the surfaces are formed on both sides of the substrate, and I4. A photothermal/magnetic recording medium characterized in that the compositions of both magnetic films are in a relationship of compositions on both sides of a magnetic compensation composition at room temperature.
JP11496383A 1983-06-25 1983-06-25 Photothermomagnetic recording medium Pending JPS607634A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11496383A JPS607634A (en) 1983-06-25 1983-06-25 Photothermomagnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11496383A JPS607634A (en) 1983-06-25 1983-06-25 Photothermomagnetic recording medium

Publications (1)

Publication Number Publication Date
JPS607634A true JPS607634A (en) 1985-01-16

Family

ID=14650965

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11496383A Pending JPS607634A (en) 1983-06-25 1983-06-25 Photothermomagnetic recording medium

Country Status (1)

Country Link
JP (1) JPS607634A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6171436A (en) * 1984-09-14 1986-04-12 Hitachi Ltd magneto-optical recording medium
JPS6355745A (en) * 1986-08-26 1988-03-10 Nippon Telegr & Teleph Corp <Ntt> Double-face type optical recording medium
JPS6415326U (en) * 1987-07-17 1989-01-26

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6171436A (en) * 1984-09-14 1986-04-12 Hitachi Ltd magneto-optical recording medium
JPS6355745A (en) * 1986-08-26 1988-03-10 Nippon Telegr & Teleph Corp <Ntt> Double-face type optical recording medium
JPS6415326U (en) * 1987-07-17 1989-01-26

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