JPS5817505A - Photothermomagnetic track moving method - Google Patents

Photothermomagnetic track moving method

Info

Publication number
JPS5817505A
JPS5817505A JP11484581A JP11484581A JPS5817505A JP S5817505 A JPS5817505 A JP S5817505A JP 11484581 A JP11484581 A JP 11484581A JP 11484581 A JP11484581 A JP 11484581A JP S5817505 A JPS5817505 A JP S5817505A
Authority
JP
Japan
Prior art keywords
light
track
bit
magnetic field
bit information
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
JP11484581A
Other languages
Japanese (ja)
Other versions
JPH0440761B2 (en
Inventor
Masahiko Kaneko
正彦 金子
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP11484581A priority Critical patent/JPS5817505A/en
Publication of JPS5817505A publication Critical patent/JPS5817505A/en
Publication of JPH0440761B2 publication Critical patent/JPH0440761B2/ja
Granted 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

Abstract

PURPOSE:To perform diverse operation such as information rewriting by moving a track, having an array of pieces of bit information recorded photothermomagnetically, over light irradiation, and erasing and selectively reading the pieces of bit information. CONSTITUTION:A nonreflective coating layer 1c, a reflective film 1d, and a protective 1e are adhered to the thin film obtained by growing a magnetic thin film 1a of garnet on a crystal substrate 1b. This constituted thermomagnetic record reader 1 is fixed to a bias magnetic field generator 2 and applied with a bias magnetic field. Laser light from a light generator 5 is introduced into an optical modulator 6 to form bits on the device 1 through the constitution shown in the figure. Then, the repetitive frequency is set to 100Hz and while the bias magnetic field is unchanged, light irradiation is carried out in the opposite direction to writing. As a result, the bits move to the opposite side to form a new track. For the reading of the bit information, reflected light is introduced into a detector 15 and observed.

Description

【発明の詳細な説明】 不発明は、光熱磁気トラック移動方法に関するものでT
o9、更ζこWg4こ扛、光熱磁気起鰍されたビット情
横が並んでいるトラックを光照射によって4動名せて、
%にビット情報の消去%am的輯み出し、情報の書き換
えなどの多様な操作を可能にする他めて有用な技術に関
するものである。
DETAILED DESCRIPTION OF THE INVENTION The invention relates to a photothermal magnetic track moving method.
o9、More
The present invention relates to a technology that is useful in addition to enabling various operations such as erasing bit information, rewriting information, etc.

従来の光熱磁気記憶轄すべて大きな抗磁力を利用してビ
ット情報の保持・安定化を得ているので、一旦書き込ま
れたビット情報を移動させること紘抗磁力が大きい九め
に不可能であった・とζろか、本発明考によって、十分
に小さな抗磁力を有する磁性材料を用いて作成し九−性
11JIIにビット情報が安定して保持場れることが見
出された顔果、従来までの技術で扛不可能であり九ビッ
ト情報のトラツタを選択的に移動する方法か完成された
Conventional photothermal magnetic storage systems all use large coercive force to retain and stabilize bit information, so it is impossible to move bit information once it has been written due to the large coercive force.・In addition, the present invention has found that the bit information can be stably retained in the 9-character 11JII by using a magnetic material with a sufficiently small coercive force, which is different from the conventional method. A method has been perfected for selectively moving 9-bit information that cannot be captured by technology.

したがって、本発明に、光熱−気記憶されたビット情報
が並んでいるトラックを光照射によって選択的に移動さ
せる方法を提供するものである・本発明に使用で龜る磁
性材料社、その−蝋抗龜力がビット情報の記録のと亀に
印加されるバイアス磁界よりも充分に小さく、そのW&
性博威の膜―に垂直な方向に強い一軸磁気異方性を有し
かつそのm面に磁化容易軸を有す小軟磁性の材料であり
て、いわゆる軟磁性膜面mtm容易磁化膜を形成しりる
ものである◎壕九七の軟iIl性のartにしても、こ
の歌碑性膜1ifi直容易磁化膜を磁気記録媒体として
過用した場合に、そζに賽き込まれるビットの径が実質
的には印加するバイアス磁界のみで決定される4!!&
であるのが好ましい0その丸め、使用する磁性材料の抗
磁力は約30e以下であるのが好ましく、約30e以下
であるのがさらに好ましい。
Therefore, the present invention provides a method for selectively moving tracks in which bit information stored photothermally and thermally is arranged by irradiation with light. The anti-adhesive force is sufficiently smaller than the bias magnetic field applied to the bit information recording mechanism, and its W&
It is a small soft magnetic material that has strong uniaxial magnetic anisotropy in the direction perpendicular to the magnetic film and has an axis of easy magnetization in the m-plane, and is a so-called soft magnetic film surface mtm easily magnetized film. ◎ Even in the case of the soft-type art of the trench ninety-seven, if this easily magnetized film is overused as a magnetic recording medium, the diameter of the bit that will be inserted into it will be is essentially determined only by the applied bias magnetic field 4! ! &
The coercive force of the magnetic material used is preferably about 30e or less, more preferably about 30e or less.

かかる磁性*ga、軟磁性ガリクムガーネツド(GGG
)などのような布上類ガリウムガーネットなどの結晶基
板上にY8mCak’eGe系ガーネツFなどの結晶を
液相エビタキVヤル法(LPn)によって成長させて形
成するのが好ましい。
Such magnetic *ga, soft magnetic gallium garnet (GGG
It is preferable to grow a crystal such as Y8mCak'eGe-based garnet F on a crystal substrate such as cloth-like gallium garnet such as ) by liquid phase epitaxy method (LPn).

前述し九ようにして得られた軟磁性膜面垂直容易磁化−
には、所定強直のバイアス磁界を印加することによって
、その腺の金山に皿って、その膜面に対して垂直方向に
かつゆ加しているバイアス蝉拌の磁化方向と同じ方向に
磁化を有する単−区が形成される0この*ia区番こ光
パルスを照射すると、印加しているバイアス磁界とは逆
方向であって膜面に対しては画直な磁化を有する円筒磁
区としてビットが形成される。このビットを形成する際
に印加されるバイアス磁界は、2ノアウド硫界H2と;
ラプス磁界HOとの間である。この範囲は、使用する磁
性材料によって多少異なるのは轟然でめるが、例えは前
述したYamCaFeGe系ガーネットの1槽である(
YslrICa)i(FeGe)s01*LPj! 1
14ζお−て昧、5106と750eとの閏である。
Easy magnetization perpendicular to the surface of the soft magnetic film obtained as described above.
By applying a predetermined tonic bias magnetic field, the gold mine of the gland is magnetized in the same direction as the magnetization direction of the bias stirrer applied perpendicularly to the membrane surface. When this *ia zone number is irradiated with a light pulse, a bit is formed as a cylindrical magnetic domain with magnetization in the opposite direction to the applied bias magnetic field and perpendicular to the film surface. is formed. The bias magnetic field applied when forming this bit is 2 Noaud sulfur fields H2;
and the lapse magnetic field HO. This range obviously varies somewhat depending on the magnetic material used, but an example is the case of the YamCaFeGe garnet mentioned above (
YslrICa)i(FeGe)s01*LPj! 1
14ζ is a leap between 5106 and 750e.

前述し良ようにして形成されたビットが並んでいるトラ
ックから所望のビットを移動させる醗こ拡、ランアクト
磁界とコツフ゛ス磁界とのm回内のバイアス磁界を印加
しながら、実質的な連続光をそのトラックから所定距離
ずらして照射し、その連続光に伴っているビットか、そ
の光入射によって形成される温度勾配によって近をって
きた移動すべきビットを反億力によってトラックの外@
に社ね飛はすことによって行なわれる。
A desired bit is moved from the track where the bits formed in the manner described above are lined up, and a substantially continuous light is emitted while applying a bias magnetic field of m times the difference between the run act magnetic field and the coppice magnetic field. It is irradiated at a predetermined distance from the track, and the bits accompanying the continuous light or the bits to be moved that are approaching due to the temperature gradient formed by the incident light are removed from the track by counterforce.
This is done by jumping to the shrine.

本発明において使用される実質的な連続光と紘、通常の
連続光の他に、光が入射しても記録が残らない機成の断
続光をも包含するものと通解されゐべ龜であって、ビー
ムのノ(ルス繰り返しが磁性薄膜とビームとの相対速度
に比べて士分速けれは任意でよい。この実質的な連続光
は1 (IIのビットを常に伴っていることを要し、そ
の強度は、その光入射によって形成される温度勾配によ
りて弓1き寄せられる移動すべ龜ピッ[を引き込まずに
反撥力によって所定距離社ね飛ばすこと力Sで龜る程度
であるのか好ましい。なお、その実質的な連続光の強度
が大きくても、移動させるトラックカーらの光入射の距
離を一節することによって、ビット同士の反撥力を虫じ
るように一節司耗である。
It should be understood that the term "substantially continuous light" used in the present invention includes, in addition to normal continuous light, mechanically intermittent light that does not leave a record even when the light is incident. Therefore, the pulse repetition rate of the beam may be arbitrarily fast compared to the relative speed between the magnetic thin film and the beam. This substantially continuous light must always accompany the bit 1 (II). It is preferable that the intensity is such that the bow 1 is attracted by the temperature gradient formed by the incident light, and the force S allows the bow to be thrown a predetermined distance by the repulsive force without being drawn in. However, even if the intensity of the continuous light is high, the distance from which the light enters the moving truck cars is reduced, which reduces the repulsive force between the bits.

本発明において、トラック移動の−の)(イアス磁界は
、ビット情報の記録の−のバイアス−界の印加方向を変
えることなく印加されlI!けるので、その実質的な連
続光の入射に伴ってくるビットは、記録されているビッ
トの硫化方向と同じ員イヒ方向を有して−る。したがっ
て1両ビットは同−凪(t。
In the present invention, the bias magnetic field for track movement is applied without changing the direction of application of the bias field for recording bit information, so that it is applied along with the substantially continuous incidence of the light. The coming bit has the same direction of sulfidation as the recorded bit.Therefore, one bit has the same direction of sulfidation (t).

方向を有するところから、−足動#I!まで近寄ったと
きに、そのELii力が引龜寄せたビットを吸収する力
よりも大−けれは移動場せるビットを昧ね飛ばしてしま
うことができる。この力撥力紘ビット極が大島い楊大1
(な9、そのビット径はバイアス磁界が小さい機大龜く
なる。し九がって、ビット情報を移動させるための光入
射は、2ンアクト磁界と=ラプス磁界の範囲内であって
、できるだけ小さいバイアス磁界を印加して行なうこと
が好ましい。例えばs (Yl、転8ma、1cao、
m)(I?e4.cmGeo、es)01gガーネット
の場合にはs 480eと560Cとの@髄内のバイア
ス磁界を印加することによってWJm″′ehるO 他方、トラック移動をさせる丸めに照射される実質的な
連続光によって生ずる温度勾配によpピットが引奄寄せ
られる力昧次式で表わすことかできる0 8)Lc十門慕 質重 、 =cM□−01)− μV;易動度 CM%Cq:物理電歇で決まる正のmavd:ビットの
移動速度 m:il化 g、:1iliエネルギー ΔM易:ビット径両端における磁化画の勾配Δ#w:ビ
ット径両端における磁壁エネルギーの勾配 ζこにおいて、一般に、#、の温度係数は負であって、
その絶対値株地の温度係数より大きいので、ピッ叶の移
動方向は、上式における右辺の第2項によって支配され
、#1の小さい方、すなわち温度の鳥い方向である。ま
た、上式から分かるように、ビットを光、ビームに退隠
させるには抗−力(&)が十分に小さいことが必要であ
る。
From having direction - foot movement #I! When you get close to the target, its ELii force is greater than the ability to absorb the attracted bit, and it can send the bit flying away. This power repellent power bit pole is Oshima, Yang Dai 1
(9) The bit diameter is large enough for the bias magnetic field to be small. Therefore, the light incident for moving the bit information must be within the range of the 2-act magnetic field and the lapse magnetic field, and as much as possible. It is preferable to apply a small bias magnetic field.For example, s (Yl, rotation 8ma, 1cao,
m) (I?e4.cmGeo,es)01g In case of garnet, WJm'''eh is applied by applying an intramedullary bias magnetic field of s 480e and 560C. The force that the p-pit is attracted to by the temperature gradient caused by the substantially continuous light can be expressed by the following equation. CM%Cq: Positive mavd determined by physical switch: Bit moving speed m: Ilization g,: 1ili energy ΔM: Gradient of magnetization picture at both ends of the bit diameter Δ#w: Gradient of domain wall energy at both ends of the bit diameter ζ Here, the temperature coefficient of # is generally negative, and
Since its absolute value is larger than the temperature coefficient of the stock, the direction of movement of the pickle is controlled by the second term on the right side of the above equation, and is the smaller one of #1, that is, the direction of the temperature. Furthermore, as can be seen from the above equation, the drag force (&) needs to be sufficiently small to make the bit disappear into the light or beam.

したがって、前述した如く、ビット同士の反撥力が、光
入射に浄なり熱磁気効果による温度勾配によってビット
を引龜寄せる力よ〕も大暑くなるように調節することに
よって所望の態様でビット情報のトラック移動を可能に
している。
Therefore, as mentioned above, by adjusting the repulsive force between the bits to become much hotter than the force that attracts the bits due to the temperature gradient caused by the thermomagnetic effect due to the incidence of light, bit information can be obtained in a desired manner. Allows for truck movement.

本発°明に係る方法によって、所望のビット情報を選択
的にそのトラックから移動させることがで書、必要な所
定のビット情報だけを読み出した9、まえ慎のビット情
報と組合せて利用することなどがIJ能である◎また、
実質的な連続光の入射位置によって、所望のビット情報
をそのトラックの右側でも左側でも選択的に移動させる
ことができ、この移動操作は、操作途中においても可能
であ)実用上極めて便利である。例えd%まず連続光を
トラックの左側の所定位置に入射し続けてビット情報を
トラックの右方に移動させ、次いでその連続光をそのト
ラックの右側の所定位置に移動さ破入射を続けると今度
はビット情報をそのトラックの左方に移動させることが
できる。を九、移動1せる必要のないビット情報が同一
12ツタ中にあれば、連続光を一旦遠くに醸してその温
度勾配の影響が及ばない位置に移動させることによって
ビット情報を選択的に移動させることもで龜る。爽に、
本発明の方法によれは、同様にして、移1IIl畜せ九
ビット情報の外側にかかる連続光を入射することによっ
てそのビット情報をトラックの元の位置に戻すこと−で
亀る〇 なお、入射する夷買′的な連続光の入射位置中入射光量
などを一定にすれは、ビットの移−量e一定にすること
ができる。この場合、ト2ツキンダサーボと称せられる
方法を用いれは任意のビットを任意の方向に正確に移動
させることができる〇このように一定の移動量をもって
移動させられ九ビット情報のトラックは新友なトラック
を形成し、これだけで必要な情報の読み出し一司能であ
る。
By the method according to the present invention, desired bit information can be selectively moved from the track, and only the necessary predetermined bit information can be read out and used in combination with the previous bit information. etc. are IJ Noh◎Also,
Depending on the incident position of the substantially continuous light, the desired bit information can be selectively moved to the right or left side of the track, and this movement operation is possible even during the operation), which is extremely convenient in practice. . For example, if d% first continues to inject the continuous light into a predetermined position on the left side of the track to move the bit information to the right side of the track, and then moves the continuous light to a predetermined position on the right side of the track and continues the injection, then can move bit information to the left of the track. 9. If there is bit information in the same vine that does not need to be moved, the bit information can be selectively moved by emitting continuous light at a distance and moving it to a position where it is not affected by the temperature gradient. It also slows down. Refreshingly,
In the method of the present invention, similarly, the bit information can be returned to its original position on the track by injecting continuous light on the outside of the transferred 9-bit information. If the amount of incident light at the incident position of the continuous light is kept constant, the amount of bit movement e can be kept constant. In this case, any bit can be accurately moved in any direction by using a method called two-way servo. In this way, the 9-bit information track that is moved with a constant amount of movement becomes a new friend's track. This is all you need to read out the information you need.

したがって、このように移動させた新しいトラックも、
元のトラックも絖み出しに使用することがで亀、いずれ
のトラックに沿って、488nmの波長であれdビット
に影響を与えない横置の弱い光を九は吸収の弱い兼波長
の光を入射させて読み出しをすることができる。この場
合、移動させて形成させた新らしいトラックで扛、移動
させなかったビット情報が消去されたことになるし、ま
た元のトラックでa%移動させ九ビット情報が消去畜れ
たことになる。ま九前述したような操作を選択的に組合
せて実施することにより、情報を選別して情味の書自換
えがilJ能であるoILに1移動させ九ビット情報の
跡に新たなビット情報を起鍮させることもで龜るので、
1つのトラックに多様な情報を紀録畜せることもで電離
めで有用である0以上述べたよう番こ、本発明に係る光
熱磁気トラック移動方法によって、ビット情報の消去、
遺択的読み出し、情報の書き換えなどの多種多様の操作
が可能である。
Therefore, the new truck moved in this way also
The original track can also be used to create a headset. Along either track, horizontally placed weak light that does not affect the d bit, even at a wavelength of 488 nm, can be used to absorb light with a weak absorption wavelength. It can be read out by making it incident. In this case, the bit information that was not moved was erased by the new track that was moved and formed, and the 9-bit information that was moved by a% was erased from the original track. . By selectively combining and performing the above-mentioned operations, it is possible to select information and move it by 1 to the OIL, which has the ability to rewrite the information, and write new bit information in the place of the 9-bit information. It also slows down the process, so
It is also possible to record a variety of information on one track, which is useful for preventing ionization.
A wide variety of operations such as selective reading and rewriting of information are possible.

以下1本発明を実施例によって説明する。The present invention will be explained below by way of examples.

実施例1 試料として、厚みu5■のGdB(ja5012基礪上
に液相エピタキシャル法(LPE )によって成長させ
fir、 (Yl、?I 8m(1,I C!io、t
s ) (Fe4.02 Ge O,9B ) 01z
  ガーネットの厚み4.6ewr  の薄膜を用い九
。この薄膜の飽和磁化4gM5== 1420%a壁抗
11 力Hc= CL50e %:1ップス磁界地= 
62.70eで6つ九〇このII膜を用いて、第1図に
示すような熱鼻気光記轍耽み出し装置(1)を形成し九
〇この装置は、前述した( Y8mCa )1(FeG
e )6012ガーネツトなどの確性薄膜(1畠)を希
土類ガリクムガーネットの一晶基4K(1b)に液相エ
ピタキシャル法でlIc長させて得丸薄膜に、無反射=
−テインダ層(1C)をその結晶基板の碑**gを設は
九反対側にそして例えに厚み0.3B1g11のアル建
エクム蒸着膜からなる反射j[(14)およびその外側
に例えば厚みα5声諺の二酸化ケイ素からなる保−膜(
1・)を被着させ九構成になっている@このような構成
からなる熱磁気光記録み出しMt(1)を%lI2−に
示すように、永久磁石などのバイアス砿界尭生装置m(
2)に、九とえは着脱自在に被着させて固定させ常時バ
イアス磁界が印加されるように配置する。この熱磁気光
記録読み出し装置は、モータ(3)などによって移動で
きるように構成することがて龜る。また、その装置の周
辺、に嬬袖助バイアス用コイル(4)を配置して、必要
に応じて、バイアス−昇を増加させることも5で暑る〇
このような構成を有する1it(1)番こ対して、光発
生装置く5)から発生−8<九例えは波幾484$nm
 のアルゴンレーずを光変llI器(6)に導入してパ
ルス光として4E9出し、そのパルス光を偏光子(7)
およびバー7ミツー(8)を介してレンズ(9)によっ
て入射させてビットをS成させた。この場合における入
射光jliPは15mW、パルス−嬬50μ易、繰り返
し周波数線IMgおよびバイアス蝉界紘510eであり
た。
Example 1 As a sample, fir, (Yl,?I 8m(1,IC!io,t
s ) (Fe4.02 Ge O,9B ) 01z
A thin film of garnet with a thickness of 4.6 ewr was used. Saturation magnetization of this thin film 4gM5== 1420%a Wall resistance 11 Force Hc= CL50e %:1 ps Magnetic field=
62.70e 90 Using this II membrane, form a thermonasal air recording device (1) as shown in Fig. 1. (FeG
e) A solid thin film (1 field) of 6012 garnet etc. is grown to lIc length by liquid phase epitaxial method on a single crystal group 4K (1b) of rare earth gallium garnet to obtain a round thin film, non-reflective =
- A reflector layer (1C) is placed on the opposite side of the crystal substrate, and a reflection j[(14) made of an Al-based Ecum vapor-deposited film with a thickness of 0.3B1g11 and a thickness α5 on the outside thereof. The proverbial protective film made of silicon dioxide (
As shown in %lI2-, the thermomagneto-optical recording projection Mt (1) consisting of a magneto-optical recording device with a magneto-optical structure as shown in FIG. (
In 2), the nine toes are removably attached and fixed, and arranged so that a bias magnetic field is constantly applied. This thermomagneto-optical recording/reading device can be configured to be movable by a motor (3) or the like. In addition, it is also possible to place a bias coil (4) around the device and increase the bias voltage if necessary.〇1it (1) with such a configuration In contrast, the light generation device 5) generates −8<9, for example, the wave height is 484 $nm.
The argon laser is introduced into the light converter (6) to emit 4E9 pulsed light, and the pulsed light is sent to the polarizer (7).
Then, the bit was made incident through the lens (9) through the bar 7 (8). The incident light jliP in this case was 15 mW, pulse power 50μ, repetition frequency line IMg, and bias voltage 510e.

上述した囁件下でパルス光を照射しながら、装置(1)
を一定速度で一方向に移動させて関隔約27−で一直線
にビットが並んだトラックが形gされ九・次に、光の強
度および輪を変えずに繰9返し周ff1a100Hzに
しかつバイアス磁界も変えずに書龜込みの際の装置移動
方向とは逆方向にトラックからビット径のはは半分楊離
して光を照射した。その結果、ビットは、10(Jjd
gのパルス光を照射し良民対側にははビットI!!、m
度離れ九位置に移動して新しいトラックを形成している
ことが判明し九G本発明における実質的な連続光の照射
位を紘、モータ(3)に取付けた回転検出機構a麺によ
って決められ、そのトラッキングの移動は、それに連動
するように設けられてiる駆動ギヤa−によって移動シ
ャーシasによってモータの位置を1mさせることによ
って行なうことかで龜る。
While irradiating pulsed light under the above-mentioned conditions, the device (1)
is moved in one direction at a constant speed to form a track with bits lined up in a straight line with a separation of about 27-.Next, the frequency is set to 100 Hz and the bias magnetic field is repeated 9 times without changing the intensity of the light and the ring. Light was irradiated at a distance of half the diameter of the bit from the track in the opposite direction to the direction in which the device was moved when loading the book without changing the information. As a result, the bits are 10 (Jjd
The pulsed light of g is irradiated and the opposite side is bit I! ! , m
It was found that the irradiation position of the continuous light in the present invention is determined by the rotation detection mechanism a-men attached to the motor (3). The tracking movement is facilitated by moving the motor by 1 m using the movable chassis as by means of a driving gear a provided in conjunction with the moving chassis as.

この熱磁気光記録読み出し装置(1)に記−されたビッ
ト情報の観み出し線、この装置の反射膜(鐘)での偏光
畜れ良民・・射光を検出子−に導入し、その光を光電子
増倍管μのに送p、その出力をオシ−スクープaηなど
でmarろようにしてもよい。なか、透過光によって記
憶軌み出しを行う場合に社、その貌み出し装置(1)か
ら反射膜(1d)を除き、バイアス砿界発生装置(2)
をそのiI!置の下部ではなく周辺部にtm亀特にファ
ラデー効果で直線偏光されえ透過光によって貌み出しを
すればよい〇 実施例2 実施例1と同じ試料および条件によってwi2碌し九ビ
ットのトラックを実施?111と同様にしてそのトラッ
クを移動させた。この場合の入射光量およびバイアス鼻
界嬬変えずに、試料移動速度マを2?声謹/秒にかり絞
υ込み対吻Vノズx20を使用してトラック移動状虐を
−ベ九。その結果を第511に示す。図中において、−
1五の右万偵域ては、近付いてきたビットは光に吸収さ
れて消滅してしまい、**aの下方IKjllcではビ
ットは光ビームに追随していかず堆lI残されてしまい
移動で亀ない0し九がって、ビット情報のトラックを移
動できる領域は、−一五の左III領域と、 1lli
iBの上側領域である。
The head line of the bit information written on this thermomagnetic optical recording/reading device (1), the polarized light from the reflective film (bell) of this device is introduced into the detector, and the light is It is also possible to send p to a photomultiplier tube .mu., and its output to be outputted by an osci scoop a.eta. Among them, when performing memory alignment using transmitted light, the reflective film (1d) is removed from the exposure device (1), and the bias field generating device (2) is used.
That iI! The tm light is linearly polarized, especially due to the Faraday effect, at the periphery of the device rather than at the bottom, and it is only necessary to make it visible by transmitted light.Example 2 Using the same sample and conditions as Example 1, a 9-bit track was performed using WI2. ? The truck was moved in the same way as 111. In this case, the sample moving speed is set to 2? without changing the amount of incident light and the bias value. The track movement situation was improved by using 20 x V-noses for aperture per second. The results are shown in No. 511. In the figure, -
In the right corner of 15, the approaching bit is absorbed by the light and disappears, and in the lower IKjllc of **a, the bit does not follow the light beam and is left behind, causing a tortoise movement. Therefore, the areas where the track of bit information can be moved are the left III area of -15 and 1lli
This is the upper area of iB.

実施例6 実施例1と同じ試料および条件によって配置したビット
のトラックを実施例1と同様にしてそのトラックの移動
をさせえ。なお、トラック移動に使用した光の入射光量
をi 1.3 mW%/(ルスーを50A11.バイア
ス磁界を5606にして、1llI!1liIIの11
111Bに対応してビットが光ビームについていく臨界
光パルス74uIL#ν(出)を試料移動速度マ(μ重
、X沙)の関数として求めた。その結果を第4賊に示す
。第4図から、li&界光ノ(ルス周波数νと試料移動
速1.ILマとは比例することが判明したOこの結果か
ら、マ/ν、すなわち九)(ルス閣のビットの移動量が
ある値(184図において拡9.5μ重)を越すとビッ
トが光ビーム曇こりいていけないことが示された。なお
、第4−において、il−の上側領域がトラック移動可
能領域でめる。
Embodiment 6 A bit track arranged using the same sample and conditions as in Embodiment 1 was moved in the same manner as in Embodiment 1. Incidentally, the incident light amount of the light used for track movement is i 1.3 mW%/(Rousse is 50A11. Bias magnetic field is set to 5606, 1llI!1liII11
The critical light pulse 74uIL#ν (output) at which the bit follows the light beam corresponding to 111B was determined as a function of the sample moving speed Ma (μ weight, Xsha). Show the results to the fourth thief. From Figure 4, it was found that li & field light (Rus frequency ν and sample moving speed 1. It has been shown that the bit cannot be clouded by the light beam if it exceeds a certain value (9.5μ weight in FIG. 184).In addition, in the 4th-, the upper region of il- is within the track movable region.

実施例4 実施例6で使用したのと同様の試料および条件を用いて
トラック移動を行った。なお、トラック移動に使用した
光拡パルス−が5Ll#sであって、バイアスlll#
を560Cにして試料を29#Il汚で移動させて臨界
光パルス周波数νを変えて入射光量PO)@数として光
パルス間試料移動量マ/ν(μm)を求めた。その結果
を185図に示す。第5図において、繭−の上側領域が
トラック移動可能領域である。
Example 4 Tracking was performed using the same sample and conditions as used in Example 6. Note that the light expansion pulse used for track movement is 5Ll#s, and the bias lll#
The temperature was set to 560C, the sample was moved with a 29#Il stain, and the critical light pulse frequency ν was changed to determine the amount of sample movement between light pulses Ma/ν (μm) as the incident light amount PO)@number. The results are shown in Figure 185. In FIG. 5, the upper area of the cocoon is the area where the track can be moved.

なおsub図ないし第5図においてトラック移動可能領
域では、実施例1においても示されたように、トラック
移動が行われるために次のような必要な条件が同時に一
九されている。すなわち8、トラック移動のため−こ入
射される光ビームに伴っているビットと、近付いてくる
他のビットとの間に生ずる反豊力が、光ビームの入射に
よって形成されるm度勾配によって他のビットを引きつ
ける力よpも強く、かつ、光ビームは他のビットが存在
しないところでも常にisのビットを伴っていて1 ト
ラック移動に使用される繰p返し光ビームの位置とその
ビット間隔が光の切れている閾に−れていても次のパル
スで杏び他のビットを引事寄せることがで亀るものであ
る〇 ま九、ll3−ないし第5図において、☆両扉および直
線で示される境界線ぎ1→の領域でも原理的にはトラッ
ク移動ができるけれども、トラツタ移動の丸めに入射さ
れる光ビームに他のビットが近づいてきて光ビーム内の
ビットに反量゛されて嬬じかれるときに、反作用によっ
て光ビームに斧っているビットも光ビームから扛じかれ
て飛び出してしまうから、トラック移動させるーには境
界illぎ9ぎ9の領域の党ビーム紘使用しない方が実
用的には好ましく、入射光量などの条件に余裕をも九せ
るなとの装置を講するのがilましい。爽にかかる境界
線ぎりぎりの領域の条件下では、試料の物性などが不均
一であつ九ときに拡−動作を行なうことも考えられるの
で、かかる条件は避けるのが好ましい。
In the sub-figures to FIG. 5, in the track movable area, as shown in the first embodiment, the following necessary conditions are met at the same time for track movement to be performed. 8. Due to track movement, the reaction force generated between the bit accompanying the incident light beam and other approaching bits is reduced by the m-degree gradient formed by the incident light beam. The force p that attracts the bit is also strong, and the light beam always accompanies the bit is even in the absence of other bits. Even if the light is at the threshold where the light is broken, it is possible to catch the next pulse and attract other bits. In principle, track movement is possible even in the boundary line 1→ region shown by When it is hit, the bit that is attached to the light beam will also be snatched away from the light beam by the reaction and fly out, so it is better not to use the party beam in the area between 9 and 9 when moving the track. It is preferable from a practical standpoint, and it is undesirable to provide a device that allows for less leeway in conditions such as the amount of incident light. Under such conditions on the edge of the boundary line, it is possible that the physical properties of the sample are non-uniform and the expansion operation may be performed at some point, so it is preferable to avoid such conditions.

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

111−嬬本発明に使用される熱磁気光記憶観み出し領
置を示す断面−、@2図紘本発明を実施する丸めの@蝋
の1例の概略を示すプルツタ鵬、および第6〜g411
嬬ト2ツク移動の特性を示すグラブでめる◎ なお図面に用いられている符号において、(,1)’ 
?・・・・・・・・・・・磁気光記録読み出し懺置(1
m) ・・・・・・・・・磁性薄膜(1b)・−・・・
・・・結晶基板 (2)・・・・・・・・・・・・バイアス砿界尭生装置
収υ・・・・・・・・・・一回転検出機構I・・・・・
・・・・・・・移動シャーシである◎ 代理人 土産 騰 横材 修 (命令)手続補正書(方式〕 昭和5C年12月 2日 特許庁長官殿 1、事件の表示 昭和56年特許願第114845号
111 - Cross-section showing the thermo-magneto-optical memory display arrangement used in the present invention -, @2 Figure Hiroshi Purutsuta-Hiro showing an outline of an example of a rounded @wax embodying the present invention, and 6th ~ g411
This is a graph showing the characteristics of two-point movement◎ In addition, in the symbols used in the drawings, (,1)'
?・・・・・・・・・Magneto-optical recording readout stand (1
m) ...... Magnetic thin film (1b) ---
・・・Crystal substrate (2) ・・・・・・・・・Bias Kōkai Kyoei device collection υ・・・・・・・One rotation detection mechanism I・・・・・・
・・・・・・・・・It is a mobile chassis ◎ Agent Souvenir Tenyokozai Repair (Order) Procedures Amendment (Method) December 2, 1975 Mr. Commissioner of the Japan Patent Office 1, Case Indication 1988 Patent Application No. No. 114845

Claims (1)

【特許請求の範囲】[Claims] 磁鐘抗磁力が印加するバイアス磁界よ1141充分に小
さな磁性材料からなる磁性薄膜に、印加しているバイア
ス磁界の方向と嬬逆向塾の磁化方間をイアス蝉界の彊さ
をう/アウト磁界とコツブス磁界との関−こして、実質
的な連続光を前記ビット情報のトラックから所定距4−
して照射しその光照射に伴なうビットとの反壷力によっ
て前記トラックから’−,1lIIIJ名ゼることを特
畝とする光熱磁気トラック$ll11方法。
The bias magnetic field applied by the coercive magnetic force of the magnetic bell 1141 The direction of the bias field applied to a magnetic thin film made of a sufficiently small magnetic material and the direction of the magnetization of the magnetic field. In conjunction with the Cottbus magnetic field, substantially continuous light is directed a predetermined distance 4-4 from the bit information track.
11. A photothermal magnetic track $11 method characterized in that the ridges are removed from the track by the repulsive force with the bit that accompanies the light irradiation.
JP11484581A 1981-07-22 1981-07-22 Photothermomagnetic track moving method Granted JPS5817505A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11484581A JPS5817505A (en) 1981-07-22 1981-07-22 Photothermomagnetic track moving method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11484581A JPS5817505A (en) 1981-07-22 1981-07-22 Photothermomagnetic track moving method

Publications (2)

Publication Number Publication Date
JPS5817505A true JPS5817505A (en) 1983-02-01
JPH0440761B2 JPH0440761B2 (en) 1992-07-06

Family

ID=14648140

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11484581A Granted JPS5817505A (en) 1981-07-22 1981-07-22 Photothermomagnetic track moving method

Country Status (1)

Country Link
JP (1) JPS5817505A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1984003991A1 (en) * 1983-03-31 1984-10-11 Sony Corp Thermomagnetic optical recording method
JPS61104443A (en) * 1984-10-26 1986-05-22 Nec Corp Photomagnetic recording/production/erasion device
EP0323232A2 (en) * 1987-12-26 1989-07-05 Sharp Kabushiki Kaisha Recording and reproducing device for magneto-optical card

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1984003991A1 (en) * 1983-03-31 1984-10-11 Sony Corp Thermomagnetic optical recording method
JPS61104443A (en) * 1984-10-26 1986-05-22 Nec Corp Photomagnetic recording/production/erasion device
EP0323232A2 (en) * 1987-12-26 1989-07-05 Sharp Kabushiki Kaisha Recording and reproducing device for magneto-optical card
US5053611A (en) * 1987-12-26 1991-10-01 Sharp Kabushiki Kaisha Device for reducing mechanical vibrations when utilizing a magneto-optical card as a recording medium

Also Published As

Publication number Publication date
JPH0440761B2 (en) 1992-07-06

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