JPS619840A - Optical storage method - Google Patents

Optical storage method

Info

Publication number
JPS619840A
JPS619840A JP13074184A JP13074184A JPS619840A JP S619840 A JPS619840 A JP S619840A JP 13074184 A JP13074184 A JP 13074184A JP 13074184 A JP13074184 A JP 13074184A JP S619840 A JPS619840 A JP S619840A
Authority
JP
Japan
Prior art keywords
recording medium
laser beams
recording
radio wave
storage method
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
JP13074184A
Other languages
Japanese (ja)
Inventor
Koichi Sano
貢一 佐野
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.)
Tokyo Sanyo Electric Co Ltd
Toshiba TEC Corp
Original Assignee
Tokyo Sanyo Electric Co Ltd
Tokyo Electric Co Ltd
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 Tokyo Sanyo Electric Co Ltd, Tokyo Electric Co Ltd filed Critical Tokyo Sanyo Electric Co Ltd
Priority to JP13074184A priority Critical patent/JPS619840A/en
Publication of JPS619840A publication Critical patent/JPS619840A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B7/00Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
    • G11B7/12Heads, e.g. forming of the optical beam spot or modulation of the optical beam
    • G11B7/14Heads, e.g. forming of the optical beam spot or modulation of the optical beam specially adapted to record on, or to reproduce from, more than one track simultaneously

Landscapes

  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Recording Or Reproduction (AREA)

Abstract

PURPOSE:To obtain the storage method where a plurality of information are recorded or reproduced simultaneously and a recording medium is not damaged, by converting plural radio signals to laser beams and storing them independently of one another by the optical storage method. CONSTITUTION:In a recording part 4, semiconductor lasers 5 are arranged in a sector, and laser beams from these semiconductor lasers 5 are shaped to parallel beams by a shaping lens 6 after bein condensed at a point A. Intervals of laser beams are narrowed to close gaps between tracks. Parallel beams are reflected on a totally reflecting mirror 7 and are turned at 90 deg. and are condensed linearly on a recording medium 9 by a cylindrical lens 8. This condensing direction crosses the advance direction of the recording medium 9, and pits are formed on individual tracks of the recording medium, and plural radio signals received by a radio receiving part 1 are recorded on individual tracks of the recording medium 9 independently of one another.

Description

【発明の詳細な説明】 発明の技術分野 本発明は、光学記憶方法に関する。[Detailed description of the invention] Technical field of invention The present invention relates to an optical storage method.

発明の技術的背景及び問題点 テレビやラジオ等の電波信号を記録する方法としては、
ビデオテープやカセットテープなどを用いた磁気的手段
によるものが一般的である。ところが、磁気的手段を用
いた場合、構造上から複数トラックの記録に不利であり
、複数チャンネルの同時記録や同時記録・再生が困難で
あるという欠点を有する。
Technical Background and Problems of the Invention Methods for recording radio signals from television, radio, etc.
Generally, magnetic means such as video tapes and cassette tapes are used. However, when magnetic means are used, it is disadvantageous in that it is structurally disadvantageous for recording on multiple tracks, and it is difficult to simultaneously record on multiple channels or simultaneously record/reproduce.

又、磁気的な記録・再生にあっては、磁気ヘッド上を記
録媒体が摺動するので両者間に摺動摩擦が生し、記録媒
体に損傷を与えるばかりでなく、長期的にみれば磁気ヘ
ッドにも磨耗をもたらすという欠点を有する。
Furthermore, in magnetic recording and reproduction, since the recording medium slides on the magnetic head, sliding friction occurs between the two, which not only damages the recording medium but also damages the magnetic head in the long run. It also has the disadvantage of causing wear.

発明の目的 本発明は、このような点に鑑みなされたもので、複数チ
ャネルの同時記録・再生を行なうことができ、あわせて
記録媒体に損傷を与えない記憶方法を得ることを目的と
する。
OBJECTS OF THE INVENTION The present invention has been made in view of the above-mentioned problems, and an object of the present invention is to provide a storage method that allows simultaneous recording and reproduction of a plurality of channels and that does not damage the recording medium.

発明の概要 本発明は、複数の電波信号を同時に電波受信部で受信し
、それらの電波信号を分離して複数のレーザビームに変
換し、テープ状の記録媒体にその進行方向と交錯する方
向に複数のレーザビームを並列的に集光させ、レーザビ
ームに変換された複数の電波信号を記録媒体に同時に記
録・再生するようにしたので、複数チャンネルの同時記
録・再生ができ、しかも記録媒体はレーザビームに照射
されつつ移動するだけなので、記録媒体等の損傷をなく
すことができるように構成したものである。
Summary of the Invention The present invention simultaneously receives multiple radio wave signals in a radio wave receiving unit, separates the radio wave signals, converts them into a plurality of laser beams, and transmits the laser beams onto a tape-shaped recording medium in a direction intersecting with the traveling direction of the laser beams. By concentrating multiple laser beams in parallel and simultaneously recording and reproducing multiple radio wave signals converted into laser beams onto a recording medium, simultaneous recording and reproducing of multiple channels is possible, and the recording medium is Since the device only moves while being irradiated with a laser beam, it is configured to prevent damage to the recording medium and the like.

発明の実施例 本発明の一実施例を第1図ないし第3図に基づいて説明
する。第1図は本発明のブロック図である。まず、複数
チャンネルの電波信号を受信する電波受信部1が設けら
れ、この電波受信部lで受信された複数の信号を同調し
て1チヤンネルごとに分離するバンドパスフィルタ2が
設けられ、とのバンドパスフィルタ2から送られてくる
搬送波を含む信号を復調する復調回路3が設けられてい
る。更に、復調回路3からの信号をレーザビームに変換
して記録する記録部4が設けられており、その原理は第
2図及び第3図に示す。すなわち、前記復調回路3から
の信号を駆動信号に変換する図示しない駆動回路が設れ
られ、その駆動信号に応じてレーザビームを照射する複
数個の半導体レーザ5が設けられている。そして、複数
個の半導体レーザ5から照射された複数本のレーザビー
ムを平行光線にする整形レンズ6と、反射して進行方向
を90°変える全反射ミラー7と、平行光線を線状に集
光するシリンドリカルレンズ8とが設けられ、集光線上
には透過形でテープ状の記録媒体9が配設されている。
Embodiment of the Invention An embodiment of the present invention will be described with reference to FIGS. 1 to 3. FIG. 1 is a block diagram of the present invention. First, a radio wave receiving section 1 that receives radio wave signals of a plurality of channels is provided, and a band pass filter 2 is provided that tunes the plurality of signals received by the radio wave receiving section 1 and separates them channel by channel. A demodulation circuit 3 that demodulates a signal containing a carrier wave sent from the bandpass filter 2 is provided. Furthermore, there is provided a recording section 4 that converts the signal from the demodulation circuit 3 into a laser beam and records it, the principle of which is shown in FIGS. 2 and 3. That is, a drive circuit (not shown) that converts the signal from the demodulation circuit 3 into a drive signal is provided, and a plurality of semiconductor lasers 5 that emit laser beams in accordance with the drive signal are provided. Then, a shaping lens 6 converts the plurality of laser beams irradiated from the plurality of semiconductor lasers 5 into parallel light beams, and a total reflection mirror 7 which reflects and changes the traveling direction by 90 degrees, condenses the parallel light beams into a linear shape. A cylindrical lens 8 is provided, and a transmissive tape-shaped recording medium 9 is provided on the condensing line.

又、この記録媒体9を透過して再び広がりながら進むレ
ーザビームを線状に集光する再生用シリンドリカルレン
ズ1oが設けられ、こちらの集光線上にはディテクタ1
1が配設されている。
Further, a reproducing cylindrical lens 1o is provided to linearly condense the laser beam that passes through the recording medium 9 and spreads again, and a detector 1 is placed on this converging line.
1 is arranged.

このような構成において、電波受信部1で受信された複
数の電波信号は、搬送波を含んだままバントパスフィル
タ2で同調さ汎てlチャンネルごとに分離され、復調回
路3で復調されて記録部4へ送られる。記録部4ではそ
れらの信号を半導体レーザ5を駆動する駆動信号に変換
し、この駆動信号により半導体レーザ5からレーザビー
ムを照射させている。そして、第3図に記録部4の平面
図を示すが、半導体レーザ5は扇状に配置、されており
、これらの半導体レーザ5からのレーザビームは図中A
点で集光された後に整形レンズ6で平行光線とされる。
In such a configuration, a plurality of radio wave signals received by the radio wave receiving unit 1 are tuned by the band pass filter 2 while containing carrier waves, separated into l channel units, demodulated by the demodulation circuit 3, and sent to the recording unit. Sent to 4. The recording unit 4 converts these signals into a drive signal for driving the semiconductor laser 5, and this drive signal causes the semiconductor laser 5 to emit a laser beam. FIG. 3 shows a plan view of the recording section 4. The semiconductor lasers 5 are arranged in a fan shape, and the laser beams from these semiconductor lasers 5 are directed at A in the figure.
After the light is focused at a point, it is made into parallel light by a shaping lens 6.

これにより、各レーザビーム間の間隔を狭めることがで
き、したがってトラック間隔を詰めることができる。そ
して、平行光線は全反射ミラー7で反射して90°向き
を変え、シリンドリカルレンズ8で記録媒体9上に線状
に集光される。この集光方向は、記録媒体9の進行方向
(第2図中矢印で示す)と交錯する方向であり、これに
より、記録媒体9には各トラックごとにピットが形成さ
れ、電波受信部1で受信された複数の電波信号が記録媒
体9の各トラックごとに独立的に記録されるわけである
This allows the distance between each laser beam to be narrowed, and therefore the track spacing to be reduced. Then, the parallel light beam is reflected by a total reflection mirror 7 to change its direction by 90 degrees, and is focused linearly onto a recording medium 9 by a cylindrical lens 8 . This direction of light convergence intersects the traveling direction of the recording medium 9 (indicated by the arrow in FIG. A plurality of received radio wave signals are independently recorded on each track of the recording medium 9.

一方、再生時には半導体レーザ5より図示しない別口路
によって低出力のレーザビームを照射させ、記録時と同
様の経路で記録媒体9上に集光させる。ここで、低出力
のレーザビームは、記録媒体9を透過して再生用シリン
ドリカルレンズ8を通り、ディテクタ11に集光される
。このとき、記録時に形成された記録媒体9のビットは
、低出力のレーザビームによりディテクタ11に検出さ
れており、これにより再生が行なわれる。
On the other hand, during reproduction, a low-power laser beam is irradiated from the semiconductor laser 5 through a separate path (not shown) and focused onto the recording medium 9 through the same path as during recording. Here, the low-power laser beam passes through the recording medium 9, passes through the reproducing cylindrical lens 8, and is focused on the detector 11. At this time, the bits of the recording medium 9 formed during recording are detected by the detector 11 using a low-power laser beam, and reproduction is thereby performed.

このように本実施例によれば、電波受信部1で受信した
複数の電波信号を記録媒体9上に同時に記録でき、しか
も、記録媒体9に対しての記録・再生ヘットである半導
体レーザ5はおのおの独立しているので、成るチャンネ
ルの記録時に別のトラックの再生をすることもできる。
As described above, according to this embodiment, a plurality of radio wave signals received by the radio wave receiving section 1 can be simultaneously recorded on the recording medium 9, and the semiconductor laser 5, which is the recording/reproducing head for the recording medium 9, Since each track is independent, you can also play back another track while recording a channel.

又、光学的な記憶方法を利用しているので、各トラック
間の間隔を狭めることができ、きわめて多量の情報を同
時に記録・再生することが可能である。そして、記録媒
体9はレーザビームに照射されつつ移動するだけなので
、記録媒体9や記録部4が摺動摩擦による損傷を受ける
ことはない。更に、記録媒体9にはテープ状のものが用
いられているので、大容量の記憶が可能である。
Furthermore, since an optical storage method is used, the spacing between each track can be narrowed, making it possible to record and reproduce an extremely large amount of information at the same time. Since the recording medium 9 only moves while being irradiated with the laser beam, the recording medium 9 and the recording section 4 will not be damaged by sliding friction. Furthermore, since the recording medium 9 is tape-shaped, it is possible to store a large amount of data.

なお、実施にあたっては、カー効果やファラデー効果な
どの磁気光学効果を用いた光磁気方式や、結晶・アモル
ファス間の相転移による反射率の変化を検出する相転移
方式等の方式による記動部4を使用してもよく、記録媒
体9には反射形のものを用いてもよい。
In addition, in implementation, the recording unit 4 uses a method such as a magneto-optical method that uses magneto-optical effects such as the Kerr effect or Faraday effect, or a phase transition method that detects changes in reflectance due to phase transition between crystal and amorphous. may be used, and the recording medium 9 may be of a reflective type.

発明の効果 本発明は、以上のように、複数の電波信号をレーザビー
ムに変換し、光学記憶方法により独立的に記憶するよう
にしたので、複数の情報を同時に記録・再生することが
でき、したがって、多量の情報を短時間で処理すること
ができ、又、光学的な記憶方法を用いているので、記録
媒体に何ものをも接触させる必要がなく、シたがって、
記録媒体の損傷や機械の磨耗をなくすことができ、更に
Effects of the Invention As described above, the present invention converts a plurality of radio wave signals into laser beams and stores them independently using an optical storage method, so that a plurality of pieces of information can be simultaneously recorded and reproduced. Therefore, a large amount of information can be processed in a short time, and since an optical storage method is used, there is no need for anything to come into contact with the recording medium.
Damage to the recording medium and wear and tear on the machine can be eliminated.

テープ状の記録媒体を用いたことにより大容量の記憶が
できる等の効果を有する。
The use of a tape-shaped recording medium has the advantage of being able to store large amounts of data.

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

第1図は本発明の一実施例を示す全体のブロック図、第
2図は記録部の側面図、第3図はその平面図である。 1・・・電波受信部、9・・・記録媒休出 願 人  
東京電気株式会社 3」 図
FIG. 1 is an overall block diagram showing an embodiment of the present invention, FIG. 2 is a side view of a recording section, and FIG. 3 is a plan view thereof. 1...Radio wave receiving section, 9...Recording medium suspension application person
Tokyo Electric Co., Ltd. 3” Figure

Claims (1)

【特許請求の範囲】[Claims] 複数の電波信号を同時に電波受信部で受信し、それらの
電波信号を分離して複数のレーザビームに変換し、テー
プ状の記録媒体にその進行方向と交錯する方向に複数の
レーザビームを並列的に集光させ、レーザビームに変換
された複数の電波信号を前記記録媒体に同時に記録・再
生するようにしたことを特徴とする光学記憶方法。
Multiple radio wave signals are received simultaneously by the radio wave receiver, those radio wave signals are separated and converted into multiple laser beams, and the multiple laser beams are transmitted in parallel onto a tape-shaped recording medium in a direction that intersects with the traveling direction of the laser beams. 1. An optical storage method characterized in that a plurality of radio wave signals, which are condensed into laser beams and converted into laser beams, are simultaneously recorded and reproduced on the recording medium.
JP13074184A 1984-06-25 1984-06-25 Optical storage method Pending JPS619840A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13074184A JPS619840A (en) 1984-06-25 1984-06-25 Optical storage method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13074184A JPS619840A (en) 1984-06-25 1984-06-25 Optical storage method

Publications (1)

Publication Number Publication Date
JPS619840A true JPS619840A (en) 1986-01-17

Family

ID=15041515

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13074184A Pending JPS619840A (en) 1984-06-25 1984-06-25 Optical storage method

Country Status (1)

Country Link
JP (1) JPS619840A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0376818A2 (en) * 1988-12-29 1990-07-04 Sony Corporation Magneto-optical disk recording apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0376818A2 (en) * 1988-12-29 1990-07-04 Sony Corporation Magneto-optical disk recording apparatus

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