JPS6025002A - Magnetic recording and reproducing device - Google Patents

Magnetic recording and reproducing device

Info

Publication number
JPS6025002A
JPS6025002A JP13249583A JP13249583A JPS6025002A JP S6025002 A JPS6025002 A JP S6025002A JP 13249583 A JP13249583 A JP 13249583A JP 13249583 A JP13249583 A JP 13249583A JP S6025002 A JPS6025002 A JP S6025002A
Authority
JP
Japan
Prior art keywords
electron beam
recording
magnetic field
magnetic
signal
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
JP13249583A
Other languages
Japanese (ja)
Inventor
Shiro Okamura
岡村 史良
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP13249583A priority Critical patent/JPS6025002A/en
Publication of JPS6025002A publication Critical patent/JPS6025002A/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
    • G11B13/00Recording simultaneously or selectively by methods covered by different main groups among G11B3/00, G11B5/00, G11B7/00 and G11B9/00; Record carriers therefor not otherwise provided for; Reproducing therefrom not otherwise provided for
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B9/00Recording or reproducing using a method not covered by one of the main groups G11B3/00 - G11B7/00; Record carriers therefor
    • G11B9/10Recording or reproducing using a method not covered by one of the main groups G11B3/00 - G11B7/00; Record carriers therefor using electron beam; Record carriers therefor
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B2005/0002Special dispositions or recording techniques
    • G11B2005/0005Arrangements, methods or circuits
    • G11B2005/0021Thermally assisted recording using an auxiliary energy source for heating the recording layer locally to assist the magnetization reversal

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To attain high density recording by heating a magnetic body at an extremely small part with an electron beam almost up to a Curie point, and applying a signal magnetic field. CONSTITUTION:A vacuum vessel 1 is evacuated through an air release pipe 7. A disk having a magnetic surface is rotated by a motor 9 through a driving part 5. The electron beam 4 from an electron gun 3 strikes the disk 2 through a signal coil 6 to make a rotary scan. The magnetic surface 2 is heated almost up to the Curie point with the electron beam and when a magnetic field is applied by the coil 6 at the same time, the surface is magnetized intensely with a signal after cooling. The recorded disk 2 is scanned with the electron beam 4' of an electron gun 3' in the vacuum vessel in reproduction, and the reflected beam 4'' is deflected by a recording magnetic field if the beam slants to the recording magnetic field. The electron beam 3 of the gun 3 is so much weaker than that of the gun 3 as to inhibit erasure. The deflected electron beam 4'' enters an electrode 14 to generate a differential output, which is nearly proportional to the recording magnetic field. This differential output is amplified by an operational amplifier 15 into a signal output.

Description

【発明の詳細な説明】 この発明は特に高密度磁気記録再生装置に関する。[Detailed description of the invention] The present invention particularly relates to a high-density magnetic recording/reproducing device.

高密度磁気記録再生装置として、従来垂直磁化法や光磁
気記録法が検討されているが、なお磁性媒体を十分高密
度に記録再生できない欠点がある。
Conventionally, perpendicular magnetization methods and magneto-optical recording methods have been studied as high-density magnetic recording and reproducing apparatuses, but they still have the drawback of not being able to record and reproduce magnetic media at a sufficiently high density.

本発明は電子ビームを用いて極めて精細高密度の記録を
行なうことを特徴とする。
The present invention is characterized in that it performs extremely fine and high-density recording using an electron beam.

従来、磁気記録の高密度化をはばんできたものの一つは
磁気ヘッドの困難である。すなわち磁気はその特性上フ
リンジ効果が大きく、実効ヘッド間隙が1μm程度以下
にし難いことである。光磁気記録はレーザビームを収束
して磁性体を局部的に加熱して記録を行なうが、レーザ
、光学系に内題がある。更に何れの方式も再生方法に困
難が大きい。
One of the things that has hindered the development of higher density magnetic recording in the past is the difficulty of developing magnetic heads. That is, magnetism has a large fringe effect due to its characteristics, and it is difficult to reduce the effective head gap to about 1 μm or less. Magneto-optical recording performs recording by focusing a laser beam and locally heating a magnetic material, but there are internal problems with the laser and optical system. Furthermore, both methods have great difficulty in reproducing.

本発明は電子ビームによって極めて小部分の磁性体をキ
ューり点近くに加熱し同時に加えた信号磁界によって高
密度記録を行なう。
The present invention uses an electron beam to heat a very small portion of a magnetic material near the cue point, and simultaneously applies a signal magnetic field to perform high-density recording.

第1図は本発明実施例を示す。1は真空容器で、排気管
7から排気を行なう。2は磁性表面を持つディスクで、
モータ9から駆動部5を介して回転する。3は電子銃で
その電子ビーム4は信号コイル6を経てディスク2に当
り回転走査する。
FIG. 1 shows an embodiment of the invention. Reference numeral 1 denotes a vacuum container, which is evacuated through an exhaust pipe 7. 2 is a disk with a magnetic surface,
It rotates from a motor 9 via a drive unit 5. Reference numeral 3 denotes an electron gun whose electron beam 4 passes through a signal coil 6 and hits the disk 2 for rotational scanning.

なお、6.2の電位は電子ビームを収束するよう適当な
値とする。2の磁性面が電子ビームによってキューり点
近傍に加熱され、同時にコイル2によって磁界が加わる
と、冷却後は強力に信号による磁化が行なわれることは
光磁気記録方式の場合と同様である、6の構成は磁気ヘ
ッド状として電子ビームを間隙から通すようにし、ある
いは磁性体の裏面から磁界を加えるようにしてもよい。
Note that the potential of 6.2 is set to an appropriate value so as to converge the electron beam. When the magnetic surface of 2 is heated near the cue point by the electron beam and at the same time a magnetic field is applied by the coil 2, strong signal magnetization occurs after cooling, as in the case of magneto-optical recording.6 The configuration may be in the form of a magnetic head so that the electron beam passes through the gap, or the magnetic field may be applied from the back surface of the magnetic material.

更に発明者先願特願昭57− 号明 細書に記載の如く、予わディスク2に一定信号を記録し
ておいて、電子ビームで加熱して位相部を一部または全
部消去するようにしてもよい。この場合は信号コイルは
不要である、電子銃、信号コイル、モータ駆動部等は図
示の如く真空容器紙8から気密リードで通電する。
Furthermore, as described in the specification of the inventor's earlier patent application No. 1983, a certain signal is recorded on the disk 2 in advance, and the phase portion is partially or completely erased by heating with an electron beam. Good too. In this case, the signal coil is not required; the electron gun, signal coil, motor drive unit, etc. are energized through airtight leads from the vacuum container paper 8 as shown.

第2図は再生装置を示す。記録された磁気ディスク2は
光磁気の場合と同様に光源10.偏向板11.12、光
電変換器13により、磁気記録によって起るファラデー
効果による偏波面の回転その他の方法で再生できるが、
この方法は周知の如く表面処理しないとS/Nが悪い。
FIG. 2 shows a playback device. The recorded magnetic disk 2 is exposed to a light source 10 as in the magneto-optical case. The polarization plates 11 and 12 and the photoelectric converter 13 can be used to rotate the plane of polarization due to the Faraday effect caused by magnetic recording, or to reproduce it by other methods.
As is well known, this method has a poor S/N ratio unless the surface is treated.

また、従来の磁気ヘッドでも再生できるが、有効間隙が
分数μmのものの製作は容易でない。
Although conventional magnetic heads can also be used for reproduction, it is not easy to manufacture one with an effective gap of a fraction of micrometers.

第3図は本発明による磁気記録再生装置を示す。記録さ
れたディスク2は真空容器中で電子銃3′の電子ビーム
4′で走査されるが、記録磁界に対してビームが斜交し
ていると、記録磁界によって反射ビーム4″は偏向する
。3′の電子ビームは第1図の3のビームよりはずフと
弱くして消去が起らないようにする。もちろん第1図の
装置のままで電圧を変えで用いてもよい。偏向された電
子ビーム4”は2電極14に入り差動出力を与えこの差
動出力が記録磁界にほぼ比例する。この差動出力はオペ
アンプ15で増幅され信号出力となる。
FIG. 3 shows a magnetic recording and reproducing apparatus according to the present invention. The recorded disk 2 is scanned in a vacuum container by an electron beam 4' of an electron gun 3', but if the beam is oblique to the recording magnetic field, the reflected beam 4'' is deflected by the recording magnetic field. The electron beam 3' should be made much weaker than the beam 3 in Fig. 1 to prevent erasure from occurring.Of course, the device shown in Fig. 1 may be used by changing the voltage. The electron beam 4'' enters the two electrodes 14 and gives a differential output, which is approximately proportional to the recording magnetic field. This differential output is amplified by the operational amplifier 15 and becomes a signal output.

第3図に示す再生装置は、第1図の方法で記録されたデ
ィスクの再生に適するが、もちろん他の高密度記録や垂
直磁化記録の再生に有効である。
The reproducing apparatus shown in FIG. 3 is suitable for reproducing a disk recorded by the method shown in FIG. 1, but is of course also effective for reproducing other high-density recording or perpendicular magnetization recording.

従来この種の高密度記録の再生は好適な方法がなくS/
Nが不良であった。
Conventionally, there was no suitable method for reproducing this type of high-density recording, and S/
N was defective.

第4図は磁性媒体を真空容器外における本発明実施例で
ある。磁気テープ23はその膜面を上にして、真空容器
8の小孔18に接しリール21から22へ巻取られる。
FIG. 4 shows an embodiment of the present invention in which the magnetic medium is placed outside the vacuum container. The magnetic tape 23 is wound onto the reels 21 to 22 in contact with the small hole 18 of the vacuum container 8 with its film side facing up.

大気圧によって小孔18にテープは密着するが、なお真
空グリース類で漏洩を防いだ方がよい。電子ビームは1
8を通して同様に記録を行なうが、偏向手段20によっ
てビーム4を偏向させれば、テープは高密度斜記録を行
ない得て長い時間、大容量の記録ができる。偏向が容易
なことは電子ビームの特徴で任意の高速偏向が可能であ
る。信号磁界はテープ裏面から与えてよい。小孔18は
幅を数10μmとし漏洩を少なくする。
Although the tape adheres tightly to the small hole 18 due to atmospheric pressure, it is better to prevent leakage with vacuum grease. The electron beam is 1
Recording is performed in the same manner through the tape 8, but by deflecting the beam 4 by the deflection means 20, the tape can perform high-density oblique recording, allowing long-time, large-capacity recording. A characteristic of electron beams is that they can be easily deflected, and any high-speed deflection is possible. The signal magnetic field may be applied from the back side of the tape. The small hole 18 has a width of several tens of μm to reduce leakage.

第5図は第4図に示す装置で記録された磁気チー123
の記録バタン25を示し、図示の如く並列した斜め記録
が行なわれる。
FIG. 5 shows a magnetic chip 123 recorded by the device shown in FIG.
A recording button 25 is shown, and parallel diagonal recording is performed as shown.

第4図に示す装置において、小孔18の部に薄膜を設は
真密度を完全にしてもよい。
In the apparatus shown in FIG. 4, a thin film may be provided in the small holes 18 to completely maintain the true density.

第6図はこの模様を示す。30は金属、半導体マイカそ
の他の薄膜で、なるべく熱を拡散しないで伝えるものが
よい。30は幅が100μm程度以下で十分電子ビーム
が通ればよい。なお、磁気テープを介して大気圧が加わ
るので、30は10μm内外と薄くできる。
Figure 6 shows this pattern. The reference numeral 30 is preferably a thin film of metal, semiconductor mica, or the like, which transmits heat without diffusing it as much as possible. 30 may have a width of about 100 μm or less, which is enough for the electron beam to pass through. In addition, since atmospheric pressure is applied via the magnetic tape, the thickness of 30 can be made as thin as about 10 μm.

第4図に示す装置はもちろんディスク、ドラム等の形式
の記録媒体でもよい。第4図の装置はビームエネルギー
を減して再生にも使えるが、例えば第2図あるいは他の
磁気ヘッドによる再生を行なっでもよい。
The device shown in FIG. 4 may of course be a recording medium in the form of a disk, drum, or the like. Although the apparatus of FIG. 4 can be used for reproduction by reducing the beam energy, it may also be used for reproduction using, for example, the magnetic head of FIG. 2 or another magnetic head.

本発明における真空容器への磁気記録媒体の出入は自動
的に行ないセットするようにでき、最近の真空技術は短
時間に動作するようにできる。
In the present invention, the magnetic recording medium can be automatically moved and set in and out of the vacuum container, and recent vacuum technology can be operated in a short time.

本発明は上起特定例に限らず種々の変形ができる。The present invention is not limited to the above-mentioned specific example and can be modified in various ways.

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

第1図は本発明による記録再生装置を示す。第2図は本
発明による記録の再生装置を示す。第3図は本発明によ
る再生装置を示す。第4図は本発明による記録再生装置
を示す。第5図は第4図の装置による記録パタンを示す
。第6図は第4図の部分変形を示す。
FIG. 1 shows a recording/reproducing apparatus according to the present invention. FIG. 2 shows a recording and reproducing apparatus according to the present invention. FIG. 3 shows a reproduction device according to the invention. FIG. 4 shows a recording/reproducing apparatus according to the present invention. FIG. 5 shows a pattern recorded by the apparatus of FIG. FIG. 6 shows a partial modification of FIG. 4.

Claims (1)

【特許請求の範囲】[Claims] 磁性記録媒体と、電子ビーム生成手段と、該電子ビーム
によって該記録媒体を走査する手段とを備えた磁気記録
再生装置。
A magnetic recording and reproducing apparatus comprising a magnetic recording medium, an electron beam generating means, and a means for scanning the recording medium with the electron beam.
JP13249583A 1983-07-20 1983-07-20 Magnetic recording and reproducing device Pending JPS6025002A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13249583A JPS6025002A (en) 1983-07-20 1983-07-20 Magnetic recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13249583A JPS6025002A (en) 1983-07-20 1983-07-20 Magnetic recording and reproducing device

Publications (1)

Publication Number Publication Date
JPS6025002A true JPS6025002A (en) 1985-02-07

Family

ID=15082706

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13249583A Pending JPS6025002A (en) 1983-07-20 1983-07-20 Magnetic recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS6025002A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008052440A (en) * 2006-08-23 2008-03-06 Toyota Motor Corp Data holding device
JP2008305164A (en) * 2007-06-07 2008-12-18 Sony Corp Electronic apparatus, communication control device and communication control method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008052440A (en) * 2006-08-23 2008-03-06 Toyota Motor Corp Data holding device
JP2008305164A (en) * 2007-06-07 2008-12-18 Sony Corp Electronic apparatus, communication control device and communication control method

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