JP2985298B2 - Recording method on perpendicular magnetic recording medium - Google Patents

Recording method on perpendicular magnetic recording medium

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Publication number
JP2985298B2
JP2985298B2 JP2413509A JP41350990A JP2985298B2 JP 2985298 B2 JP2985298 B2 JP 2985298B2 JP 2413509 A JP2413509 A JP 2413509A JP 41350990 A JP41350990 A JP 41350990A JP 2985298 B2 JP2985298 B2 JP 2985298B2
Authority
JP
Japan
Prior art keywords
recording
signal
recording medium
perpendicular magnetic
magnetic recording
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.)
Expired - Fee Related
Application number
JP2413509A
Other languages
Japanese (ja)
Other versions
JPH04221406A (en
Inventor
浩 内山
直樹 本多
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 JP2413509A priority Critical patent/JP2985298B2/en
Publication of JPH04221406A publication Critical patent/JPH04221406A/en
Application granted granted Critical
Publication of JP2985298B2 publication Critical patent/JP2985298B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Digital Magnetic Recording (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)
  • Magnetic Heads (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、例えば垂直磁気記録媒
体(フロッピーディスクやビデオテープ等)にディジタ
ルデータを磁気記録する磁気記録装置等に適用して好適
な垂直磁気記録媒体への記録方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a recording method for a perpendicular magnetic recording medium suitable for application to a magnetic recording apparatus for magnetically recording digital data on a perpendicular magnetic recording medium (floppy disk, video tape, etc.). .

【0002】[0002]

【従来の技術】従来、予め垂直に磁化され易いようにな
された垂直磁気記録媒体(フロッピーディスクやビデオ
テープ等)が提案されている。このような垂直磁気記録
媒体に信号を記録したり、この垂直磁気記録媒体に記録
された信号を再生したりするには、周知の磁気記録媒体
の磁性体を水平方向に磁化することにより信号を記録
し、この磁気記録媒体に記録された信号を再生する磁気
記録再生装置と同様に、磁気ヘッドに記録電流を流した
り、磁気ヘッドよりの信号を再生したりすることによっ
て行っている。また、このような垂直磁気記録媒体には
Co−Cr(コバルト−クロム)等が使用されている。
記録の方式としては、矩形波を記録信号とするいわゆ
る矩形波記録とサイン波を記録信号とするサイン波記録
の2つの方式がある。図3Eに示すように、上述の2つ
の方式の何れの方式にても、即ち、矩形波を記録信号と
しても、サイン波を記録信号としても、一旦信号を記録
した垂直磁気記録媒体より磁気ヘッドによって再生した
波形はこのようにダイパルス波形となる。
2. Description of the Related Art A perpendicular magnetic recording medium (floppy disk, video tape, or the like) which has been easily magnetized perpendicularly in advance has been proposed. In order to record a signal on such a perpendicular magnetic recording medium or to reproduce a signal recorded on the perpendicular magnetic recording medium, the signal is obtained by magnetizing a magnetic material of a known magnetic recording medium in the horizontal direction. As in the magnetic recording / reproducing apparatus for recording and reproducing the signal recorded on the magnetic recording medium, the recording is performed by supplying a recording current to the magnetic head or reproducing the signal from the magnetic head. For such a perpendicular magnetic recording medium, Co-Cr (cobalt-chromium) or the like is used.
As a recording method, there are two methods of so-called rectangular wave recording using a rectangular wave as a recording signal and sine wave recording using a sine wave as a recording signal. As shown in FIG. 3E, in either of the above-mentioned two systems, that is, whether a rectangular wave is used as a recording signal or a sine wave is used as a recording signal, a magnetic head is read from a perpendicular magnetic recording medium on which a signal is once recorded. Thus, the waveform reproduced in this manner becomes a dipulse waveform.

【0003】[0003]

【発明が解決しようとする課題】ところで、上述の2つ
の方式、即ち、矩形波を記録信号とする場合及びサイン
波を記録信号とする場合の内、サイン波を記録信号とし
た場合は、その再生波形は図3Fに示す如き、図3Eに
示したダイパルス波形が乱れた異常波形となることがあ
る。このような異常波形が発生した場合は、この図3F
に示すように、図3Eに示したダイパルス波形において
はピークが1つしかない所にピークが2つ以上現れ、こ
れによってピークを検出する再生系の回路が誤った動作
をしてしまう。従って、C/N(Color/Nois
e)やS/N(Sound/Noise)の他に、エラ
ーレートを劣化させる不都合がある。
By the way, of the two methods described above, namely, a case where a rectangular wave is used as a recording signal and a case where a sine wave is used as a recording signal, when a sine wave is used as a recording signal, As shown in FIG. 3F, the reproduction waveform may be an abnormal waveform in which the dipulse waveform shown in FIG. 3E is disturbed. When such an abnormal waveform is generated, FIG.
As shown in FIG. 3E, in the dipulse waveform shown in FIG. 3E, two or more peaks appear where there is only one peak, which causes the reproduction system circuit for detecting the peak to operate erroneously. Therefore, C / N (Color / Nois
In addition to e) and S / N (Sound / Noise), there is a disadvantage of deteriorating the error rate.

【0004】本発明はかかる点に鑑みてなされたもの
で、垂直磁気記録媒体より記録した信号を再生したとき
にその信号のC/N、S/N及びエラーレートが劣化す
ることのない垂直磁気記録媒体への記録方法を提案しよ
うとするものである。
[0004] The present invention has been made in view of the above point, and when a signal recorded from a perpendicular magnetic recording medium is reproduced, the C / N, S / N and error rate of the signal are not degraded. It is intended to propose a recording method on a recording medium.

【0005】[0005]

【課題を解決するための手段】本発明垂直磁気記録媒体
への記録方法は例えば図1に示す如く、垂直磁気記録媒
体1へサイン波で記録を行う際に、磁気ヘッド2に流す
電流I[AT0-p]及び記録波長λ[μm]の関係がI/
λ>0.1[AT0-p /μm]となるようにしたものであ
る。
According to the method of recording on a perpendicular magnetic recording medium of the present invention, for example, as shown in FIG. 1, a current I [ AT0-p] and the recording wavelength λ [μm] are I /
λ> 0.1 [AT0-p / μm].

【0006】[0006]

【作用】上述せる本発明によれば、垂直磁気記録媒体1
へサイン波で記録を行う際に、磁気ヘッド2に流す電流
I[AT0-p]及び記録波長λ[μm]の関係がI/λ>
0.1[AT0-p /μm]となるようにしたので垂直磁気記
録媒体1より記録した信号を再生したときにその信号の
C/N、S/N及びエラーレートが劣化しないようにす
ることができる。
According to the present invention described above, the perpendicular magnetic recording medium 1 is provided.
When performing recording with a sine wave, the relationship between the current I [AT0-p] flowing through the magnetic head 2 and the recording wavelength λ [μm] is I / λ>
Since it is set to 0.1 [AT0-p / μm], it is possible to prevent the C / N, S / N and error rate of the signal from deteriorating when the signal recorded from the perpendicular magnetic recording medium 1 is reproduced. .

【0007】[0007]

【実施例】以下に、図1を参照して本発明垂直磁気記録
媒体への記録方法の例について詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, an example of a recording method for a perpendicular magnetic recording medium according to the present invention will be described in detail with reference to FIG.

【0008】この図1においては、例えば図2に示すよ
うな記録装置により、信号処理回路4よりの信号(サイ
ン波)を記録増幅器3及び磁気ヘッド2を介して磁気記
録媒体1に任意の記録電流I[AT0-p]及び任意の記
録波長λ[μm]で記録し、この記録した信号を再生
し、その結果異常波形が見られた任意の記録電流I及び
記録波長λの点について「×」を示し、異常波形が見ら
れなかった任意の記録電流I及び記録波長λの点につい
て「○」を示している。そしてこれら「×」の点及び
「○」の点の境界をI=0.106 λを満たす実線aで示し
ている。この図1から明らかなように、記録電流Iが小
さくなるにしたがって、また記録波長が長くなるにした
がって異常波形が発生しやすいことが判明した。即ち、
I>0.1 λを満たすことにより異常波形が発生しないこ
とが判明した。
In FIG. 1, for example, a signal (sine wave) from a signal processing circuit 4 is arbitrarily recorded on a magnetic recording medium 1 via a recording amplifier 3 and a magnetic head 2 by a recording apparatus as shown in FIG. Recording was performed at the current I [AT0-p] and an arbitrary recording wavelength λ [μm], and the recorded signal was reproduced. As a result, a point of the arbitrary recording current I and the recording wavelength λ where an abnormal waveform was observed was evaluated as “× ”, And“ ○ ”indicates an arbitrary recording current I and a recording wavelength λ where no abnormal waveform was observed. The boundary between these "x" points and "o" points is indicated by a solid line a satisfying I = 0.106 λ. As is clear from FIG. 1, it has been found that an abnormal waveform is more likely to occur as the recording current I decreases and as the recording wavelength increases. That is,
It was found that no abnormal waveform was generated by satisfying I> 0.1λ.

【0009】さて、この異常波形が発生しない条件がI
>0.1λとなることにつき説明する。垂直磁気記録の場
合は、図3A(縦軸を記録電流Iとし、横軸を時間tと
する)に示すような記録電流信号(サイン波)がある程
度以上大きくなって(図3AにおいてI0≦|I|)は
じめて磁界が媒体内の磁化を反転するため、サイン波記
録の場合には磁化反転をなさない領域bが発生する。こ
のため、磁化反転時の磁化分布が図3B(縦軸を磁化M
とし、横軸を時間tとする)に示すようになる。このよ
うに磁化反転の磁化分布に磁化Mが略0のところが或一
定以上の幅(時間)となると、磁化反転の再生信号の波
形は図3Cに示すようになり、更にこれが合成されて図
3Dに示すような異常波形となる。従って、磁化反転を
なさない領域bが広いか狭いかによって異常波形の有無
がわかる。
The condition under which this abnormal waveform does not occur is I
It will be described that> 0.1λ. In the case of perpendicular magnetic recording, the recording current signal (sine wave) as shown in FIG. 3A (the ordinate represents the recording current I and the abscissa represents the time t) increases to a certain degree or more (in FIG. 3A, I0 ≦ | I |) Since the magnetic field reverses the magnetization in the medium for the first time, in the case of sine wave recording, a region b where the magnetization is not reversed occurs. For this reason, the magnetization distribution at the time of the magnetization reversal is shown in FIG.
And the horizontal axis is time t). When the width (time) of the magnetization inversion where the magnetization M is substantially zero becomes a certain value or more as shown in FIG. 3C, the waveform of the reproduction signal of the magnetization inversion becomes as shown in FIG. An abnormal waveform as shown in FIG. Therefore, the presence or absence of an abnormal waveform can be determined depending on whether the region b where the magnetization reversal is not performed is wide or narrow.

【0010】ここで磁化反転されない領域bが或幅x0
下のときには異常波形が発生しないとする。そして、数
1を仮定する。
[0010] and abnormal waveform does not occur here when regions not magnetized inversion b are certain width x 0 or less. Then, Equation 1 is assumed.

【数1】 また、図3Aの記録電流の関数を数2とおく。(Equation 1) The function of the recording current in FIG.

【数2】 このとき、t=0においての傾きは数2より、数3が導
きだされる。
(Equation 2) At this time, Equation 3 is derived from Equation 2 for the slope at t = 0.

【数3】 更に、図3Aの記録電流信号が磁化反転をなさない領域
bの幅t0間の記録電流信号を直線近似した場合は数4と
なる。
(Equation 3) Further, a region where the recording current signal of FIG.
Equation 4 is obtained when the recording current signal for the width t0 of b is linearly approximated.

【数4】 そして、この数3を数1に代入すると、数5が導き出さ
れる。
(Equation 4) By substituting Equation 3 into Equation 1, Equation 5 is derived.

【数5】 ここで、v/f=λ(記録波長)であるので、x0は数
6で示す如くなり、ゆえに数7が成り立つ。
(Equation 5) Here, since v / f = λ (recording wavelength), x 0 is as shown in Expression 6, and therefore Expression 7 is satisfied.

【数6】 (Equation 6)

【数7】 即ち、I/λが或値より大きい場合には異常波形が発生
しない。
(Equation 7) That is, when I / λ is larger than a certain value, no abnormal waveform is generated.

【0011】上述より明らかなように、磁気ヘッド2に
流す電流I[AT0-p]及び記録波長λ[μm]の関係が
I/λ>0.1[AT0-p/μm]となるようにしたので、
垂直磁気記録媒体1より記録した信号を再生したときに
その信号のC/N、S/N及びエラーレートが劣化しな
いようにすることができる。
As is apparent from the above description, the relationship between the current I [AT0-p] flowing through the magnetic head 2 and the recording wavelength λ [μm] is such that I / λ> 0.1 [AT0-p / μm]. ,
When a signal recorded from the perpendicular magnetic recording medium 1 is reproduced, the C / N, S / N and error rate of the signal can be prevented from deteriorating.

【0012】[0012]

【0013】尚、本発明は上述の実施例に限ることなく
本発明の要旨を逸脱することなくその他種々の構成が取
り得ることは勿論である。
It should be noted that the present invention is not limited to the above-described embodiment, but can adopt various other configurations without departing from the gist of the present invention.

【0014】[0014]

【発明の効果】上述せる本発明よれば、垂直磁気記録媒
体へサイン波で記録を行う際に、磁気ヘッドに流す電流
I[AT0-p]及び記録波長λ[μm]の関係がI/λ>
0.1[AT0-p /μm]となるようにしたので、垂直磁気
記録媒体より記録した信号を再生したときにその信号の
C/N、S/N及びエラーレートが劣化しないようにす
ることができる利益がある。また、これにより、波形の
複雑な矩形波の記録電流信号を用いなくとも、サイン波
の記録電流信号を用いてディジタル記録再生が可能とな
る利益がある。
According to the present invention described above, when recording is performed on a perpendicular magnetic recording medium with a sine wave, the relationship between the current I [AT0-p] flowing through the magnetic head and the recording wavelength λ [μm] is I / λ. >
Since it is set to 0.1 [AT0-p / μm], it is possible to prevent the C / N, S / N and error rate of the signal from deteriorating when the signal recorded from the perpendicular magnetic recording medium is reproduced. There is a benefit. In addition, there is an advantage that digital recording and reproduction can be performed using a sine wave recording current signal without using a rectangular waveform recording current signal having a complicated waveform.

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

【図1】本発明垂直磁気記録媒体への記録方法の説明に
共する記録電流、波長による異常波形の有無を示すグラ
フである。
FIG. 1 is a graph showing the presence / absence of an abnormal waveform depending on a recording current and a wavelength for explaining a recording method on a perpendicular magnetic recording medium of the present invention.

【図2】本発明垂直磁気記録媒体への記録方法の説明に
共する記録装置の構成例を示す図である。
FIG. 2 is a diagram showing a configuration example of a recording apparatus for explaining a recording method on a perpendicular magnetic recording medium according to the present invention.

【図3】波形図である。FIG. 3 is a waveform diagram.

【符号の説明】[Explanation of symbols]

1 磁気記録媒体 2 磁気ヘッド 3 記録増幅器 4 記録信号処理回路 1 Magnetic recording medium 2 Magnetic head 3 Recording amplifier 4 Recording signal processing circuit

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 垂直磁気記録媒体へサイン波で記録を行
う際に、磁気ヘッドに流す電流I[AT0-p]及び記録
波長λ[μm]の関係がI/λ>0.1[AT0-p /μm]
となるようにしたことを特徴とする垂直磁気記録媒体へ
の記録方法。
When performing recording with a sine wave on a perpendicular magnetic recording medium, the relationship between a current I [AT0-p] flowing through a magnetic head and a recording wavelength λ [μm] is I / λ> 0.1 [AT0-p / μm]
A recording method for a perpendicular magnetic recording medium, characterized in that:
JP2413509A 1990-12-21 1990-12-21 Recording method on perpendicular magnetic recording medium Expired - Fee Related JP2985298B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2413509A JP2985298B2 (en) 1990-12-21 1990-12-21 Recording method on perpendicular magnetic recording medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2413509A JP2985298B2 (en) 1990-12-21 1990-12-21 Recording method on perpendicular magnetic recording medium

Publications (2)

Publication Number Publication Date
JPH04221406A JPH04221406A (en) 1992-08-11
JP2985298B2 true JP2985298B2 (en) 1999-11-29

Family

ID=18522138

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2413509A Expired - Fee Related JP2985298B2 (en) 1990-12-21 1990-12-21 Recording method on perpendicular magnetic recording medium

Country Status (1)

Country Link
JP (1) JP2985298B2 (en)

Also Published As

Publication number Publication date
JPH04221406A (en) 1992-08-11

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