JPH0258683B2 - - Google Patents

Info

Publication number
JPH0258683B2
JPH0258683B2 JP14054882A JP14054882A JPH0258683B2 JP H0258683 B2 JPH0258683 B2 JP H0258683B2 JP 14054882 A JP14054882 A JP 14054882A JP 14054882 A JP14054882 A JP 14054882A JP H0258683 B2 JPH0258683 B2 JP H0258683B2
Authority
JP
Japan
Prior art keywords
recording
magnetic pole
reproducing
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.)
Expired
Application number
JP14054882A
Other languages
Japanese (ja)
Other versions
JPS5930202A (en
Inventor
Masahiro Honjo
Masaaki Kobayashi
Akio Hashima
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP57140548A priority Critical patent/JPS5930202A/en
Publication of JPS5930202A publication Critical patent/JPS5930202A/en
Publication of JPH0258683B2 publication Critical patent/JPH0258683B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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
    • G11B5/02Recording, reproducing, or erasing methods; Read, write or erase circuits therefor

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は磁気記録媒体に磁気層に対し、その厚
み方向に磁化することにより情報の記録を行う短
波長磁気記録に適した磁気記録再生装置に関する
ものである。
[Detailed Description of the Invention] Industrial Application Field The present invention relates to a magnetic recording and reproducing device suitable for short wavelength magnetic recording, which records information by magnetizing a magnetic layer in the thickness direction of a magnetic recording medium. It is.

従来例の構成とその問題点 従来、ビデオテーブレコーダなどの磁気記録再
生装置においては、磁気記録媒体として磁気テー
プを用い、磁気ヘツドあるいは磁気テープを上記
磁気ヘツドの幅方向に対し、ほぼ直角あるいは数
度のアジマス角をもつて走行させることにより、
記録または再生を行なつている。このような媒体
の運動方向に磁化する磁化方式は、長手方向磁化
と称され、ビデオテーブレコーダなどにおいて
は、記録波長1μm程度のところから記録減磁が増
加し、これ以上の短波長記録の実用化は困難であ
つた。
Conventional configurations and their problems Conventionally, in magnetic recording and reproducing devices such as video table recorders, magnetic tape is used as a magnetic recording medium, and the magnetic head or magnetic tape is placed at approximately right angles or several times with respect to the width direction of the magnetic head. By running with an azimuth angle of
Recording or playback is in progress. This type of magnetization in which the medium is magnetized in the direction of motion is called longitudinal magnetization, and in video table recorders, etc., recording demagnetization increases from a recording wavelength of about 1 μm, making recording at shorter wavelengths impractical. It was difficult to adapt.

一方、これ以上の短波長記録を目的とした垂直
磁化方式が検討され、実用化への提案が数多くさ
れている。例えば、その1つに、信号電流を流す
ための巻線が施された補助磁極と、その補助磁極
の端面積より小なる端面積をもち対向して設置さ
れる主磁極を備えた垂直磁気記録再生装置があ
る。これは主磁極の厚さLで記録再生を行う場
合、厚さL以下の短波長記録が可能な反面、再生
時には長手記録再生におけるギヤツプロスに相当
する損失が発生し、厚さL以下の波長は十分再生
されないという欠点があつた。
On the other hand, perpendicular magnetization systems aimed at recording at even shorter wavelengths have been studied, and many proposals for practical use have been made. For example, one example is perpendicular magnetic recording, which includes an auxiliary magnetic pole equipped with a winding for passing a signal current, and a main magnetic pole facing each other and having an end area smaller than the end area of the auxiliary magnetic pole. There is a playback device. This is because when recording and reproducing with the thickness L of the main pole, it is possible to record short wavelengths less than the thickness L, but at the time of reproduction, a loss equivalent to the gear loss in longitudinal recording and reproduction occurs, and the wavelength less than the thickness L The problem was that it was not played back enough.

発明の目的 本発明は上述した従来の欠点を除去し、大幅な
短波長記録を可能にする磁気記録再生装置を提供
することを目的とするものである。
OBJECTS OF THE INVENTION It is an object of the present invention to provide a magnetic recording/reproducing device which eliminates the above-mentioned conventional drawbacks and enables recording at significantly shorter wavelengths.

発明の構成 上記目的を達成するために、本発明は磁気記録
媒体の磁気層に対し、その厚み方向に磁化するこ
とにより情報の記録を行うように構成し、かつ、
磁極の厚さLを有する記録再生磁極または記録磁
極と磁極の厚さLを有する再生磁極を具備し、前
記記録再生磁極または記録磁極が記録媒体上を相
対的に多くとも距離L移動する区間だけ信号を記
録し、次に前記記録再生磁極または記録磁極が記
録媒体上を相対的に少なくとも距離L移動する区
間は記録を停止するように構成したものである。
Structure of the Invention In order to achieve the above object, the present invention is configured to record information by magnetizing a magnetic layer of a magnetic recording medium in the direction of its thickness, and
comprising a recording/reproducing magnetic pole having a magnetic pole thickness L or a recording magnetic pole and a reproducing magnetic pole having a magnetic pole thickness L, and only in an area where the recording/reproducing magnetic pole or the recording magnetic pole relatively moves at most a distance L on the recording medium. The apparatus is configured to record a signal and then stop recording during a section in which the recording/reproducing magnetic pole or the recording magnetic pole moves relatively at least a distance L on the recording medium.

さらに、本発明は磁極の厚さLを有する再生磁
極を具備し、多くとも距離Lの区間だけ記録さ
れ、次の少なくとも距離Lの区間は記録されてい
ない前記磁気記録媒体を、前記再生磁極により再
生して再生信号を得るように構成したものであ
る。
Furthermore, the present invention includes a reproducing magnetic pole having a magnetic pole thickness L, and the reproducing magnetic pole records the magnetic recording medium in which a section of at most a distance L is recorded, and a subsequent section of at least a distance L is not recorded. It is configured to reproduce and obtain a reproduced signal.

実施例の説明 以下本発明の一実施例を図面に基づいて説明す
る。第1図は垂直磁気記録媒体の主磁極1、記録
波形2、磁気テープ3、テープ走行方向イ、主磁
極の厚さL、補助磁極4、巻線5を示したもの
で、記録ヘツドとしての主磁極1は磁気テープ3
の磁気層を厚さ方向に磁化する。ここで、記録波
形2は磁気テープ3が主磁極1の終端部gを通過
する時に加わる記録信号により決定されると考え
てよく、記録信号の波長λは主磁極の厚さLと何
ら関係しない。すなわち、主磁極の厚さLよりも
短い波長をもつ信号の記録が可能であることがわ
かる。これは従来の長手方向磁化方式では記録減
磁により実現が困難であつた。
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below based on the drawings. Figure 1 shows the main magnetic pole 1, the recording waveform 2, the magnetic tape 3, the tape running direction, the thickness L of the main pole, the auxiliary magnetic pole 4, and the winding 5 of a perpendicular magnetic recording medium. Main pole 1 is magnetic tape 3
magnetize the magnetic layer in the thickness direction. Here, it can be considered that the recording waveform 2 is determined by the recording signal applied when the magnetic tape 3 passes the terminal end g of the main magnetic pole 1, and the wavelength λ of the recording signal has no relation to the thickness L of the main magnetic pole. . That is, it can be seen that it is possible to record a signal having a wavelength shorter than the thickness L of the main pole. This was difficult to achieve with the conventional longitudinal magnetization method due to recording demagnetization.

次に、このように記録された信号の再生例を第
2図に示す。ここで、再生ヘツドとして前述した
主磁極を用いてももちろんかまわないが、以下再
生ヘツドと称することにする。この場合再生ヘツ
ド幅Lは前述した主磁極厚さLに対応することに
なる。第2図aは再生ヘツド幅Lの中に半波長入
る信号が示されており、この時再生出力は最大と
なる。これは再生出力はヘツド内を通る磁束の変
化と考えると、再生信号の波長λがヘツド幅Lと
λ=2Lの関係の時磁束の変化量が最大になるこ
とから明らかである。
Next, an example of reproduction of a signal recorded in this manner is shown in FIG. Although it is of course possible to use the main pole described above as the reproducing head, it will be referred to as the reproducing head hereinafter. In this case, the read head width L corresponds to the main pole thickness L mentioned above. FIG. 2a shows a signal that falls within half a wavelength within the width L of the reproducing head, and at this time the reproducing output is at its maximum. This is clear from the fact that when the reproduced output is considered to be a change in magnetic flux passing through the head, the amount of change in magnetic flux becomes maximum when the wavelength λ of the reproduced signal has a relationship of λ=2L with the head width L.

次に、第2図bにヘツド幅Lに1波長が入る信
号を示す。この時再生ヘツドが移動しても、再生
ヘツドコア内に磁束の変化は発生せず再生出力は
0となる。つまり再生信号の波長λ=L/n(nは 自然数)を満たす時、再生出力は0となり、これ
は従来の長手方向記録におけるギヤツプロスに相
当すると考えられる。なお第2図以後の図例にお
いて補助磁極は省略している。
Next, FIG. 2b shows a signal in which one wavelength is included in the head width L. Even if the reproducing head moves at this time, no change in magnetic flux occurs within the reproducing head core, and the reproducing output becomes zero. That is, when the wavelength of the reproduced signal λ=L/n (n is a natural number), the reproduced output becomes 0, which is considered to correspond to the gear loss in conventional longitudinal recording. Note that the auxiliary magnetic pole is omitted in the illustrations from FIG. 2 onwards.

次に第2図bにおいて、1波長のみ記録されて
いた場合の再生出力を考えてみる。第3図のt1
記録信号の先端S1が再生ヘツドの先端h1と一致し
再生されはじめる瞬間を示した図、t2はヘツド幅
Lの中に1波長入つている状態の図、t3は再生が
終つた瞬間の図を示している。上記t1の状態から
t2の状態を経てt3の状態までの再生ヘツドコア内
を通る磁束φと磁束φの微分dφ/dtを第4図に示 す。ここでdφ/dtは再生出力を示している。
Next, in FIG. 2b, consider the reproduction output when only one wavelength is recorded. In Fig. 3, t 1 is a diagram showing the moment when the leading edge S 1 of the recording signal coincides with the leading edge h 1 of the reproducing head and reproduction begins, and t 2 is a diagram showing a state in which one wavelength is included in the head width L. t 3 shows the diagram at the moment the playback ends. From the state of t 1 above
FIG. 4 shows the magnetic flux φ passing through the read head core from the state t 2 to the state t 3 and the differential dφ/dt of the magnetic flux φ. Here, dφ/dt indicates the reproduction output.

ここで、再生途中において、第3図に示すヘツ
ド先端部分h1とヘツド後端部分h2の間を通過して
いる信号はヘツドのコアを通る磁束φの変化には
何ら寄与しない(dφ/dt=0)ため、再生出力には 現われてこない。つまり第4図の再生出力dφ/dtに おいて、t1〜t2区間はヘツド先端h1での再生波形
と考えられ、t2〜t3区間はヘツド後端h2での再生
波形と考えられる。
During reproduction, the signal passing between the head tip h1 and the head rear end h2 shown in FIG. 3 does not contribute to the change in the magnetic flux φ passing through the head core (dφ/ dt=0), it does not appear in the playback output. In other words, in the reproduced output dφ/dt in Fig. 4, the interval t 1 to t 2 is considered to be the reproduced waveform at the head tip h 1 , and the interval t 2 to t 3 is considered to be the reproduced waveform at the rear end h 2 of the head. .

このように、波長λ=L/n(L:ヘツド幅、
n:自然数)である信号の再生において、第2図
bに示したように連続波では再生出力は得られな
いが、第3図の如くバースト状に記録することに
よつて再生が可能となる。
In this way, the wavelength λ=L/n (L: head width,
When reproducing a signal where n is a natural number, it is not possible to obtain a reproduction output with continuous waves as shown in Figure 2b, but reproduction is possible by recording in burst form as shown in Figure 3. .

再生出力として、第4図のt1〜t2間に得られる
波形を用いてもよく、t2〜t3間に得られる波形を
用いてもよく、また両方の波形を合成して得るこ
ともできる。この合成方法の一例を簡単に述べ
る。
As the reproduction output, the waveform obtained between t 1 and t 2 in FIG. 4 may be used, the waveform obtained between t 2 and t 3 may be used, or both waveforms may be synthesized. You can also do it. An example of this synthesis method will be briefly described.

第5図aは再生波形、bはヘツド先端で再生さ
れた信号波形、cはbを再生ヘツドがテープ上を
相対的に距離L移動する時間Tlだけ遅延させた
波形、dはcの位相を反転させた波形、そしてe
は再生成形とdの波形を重ねあわせたことにより
得られる波形を示しており、明らかにS/N比が
6dB向上する。
In Figure 5, a is the reproduced waveform, b is the signal waveform reproduced at the tip of the head, c is the waveform obtained by delaying b by the time Tl during which the reproducing head moves a distance L relative to the tape, and d is the phase of c. Inverted waveform, and e
shows the waveform obtained by superimposing the remolded waveform and the waveform of d, and it is clear that the S/N ratio is
Improved by 6dB.

この合成方法を実現するための回路ブロツク図
で第6図に示す。回路はアンプ8、アナログスイ
ツチSW1,SW2、遅延回路5、位相反転回路
6、ミツクス回路7から構成されている。第4図
で示したt1〜t2間はスイツチSW2がONし、t2
t3間はスイツチSW1がONする。スイツチSW2
を通つた信号すなわちヘツド先端部で検出された
信号は前記遅延回路9で前記時間Tl遅延させら
れ、位相反転回路6で位相反転した後、ミツクス
回路7へ送られる。このミツクス回路7では、上
記信号とスイツチSW1を通つた信号は同波形に
なつており、加算することにより、S/Nを6dB
向上することができる。
FIG. 6 shows a circuit block diagram for realizing this synthesis method. The circuit is composed of an amplifier 8, analog switches SW1 and SW2, a delay circuit 5, a phase inversion circuit 6, and a mixer circuit 7. Switch SW2 is ON between t 1 and t 2 shown in Fig. 4, and from t 2 to t 2
Switch SW1 is ON during t3 . Switch SW2
The signal passed through, that is, the signal detected at the tip of the head, is delayed by the time Tl in the delay circuit 9, phase inverted in the phase inversion circuit 6, and then sent to the mixer circuit 7. In this mix circuit 7, the above signal and the signal passing through switch SW1 have the same waveform, and by adding them together, the S/N is reduced by 6 dB.
can be improved.

ここで、上記記録再生方式では、従来長手方向
における記録減磁、再生時におけるギヤツプロス
が発生しないため、短波長記録再生が可能とな
る。
Here, in the above-mentioned recording and reproducing method, short wavelength recording and reproducing is possible because conventional recording demagnetization in the longitudinal direction and gear loss during reproduction do not occur.

そこで、次に短波長記録再生の一例を示す。第
7図は、ヘツド幅L=5μとして、波長1μの記録
再生の例を示したものである。aは記録時の状
態、bは再生状態、cは再生波形、dは前記ミツ
クス回路を用いてS/Nを向上させた場合の出力
波形を示している。すなわち、バースト状に記録
することによりヘツド幅に関係なく、短波長記録
再生が可能であることがわかる。
Next, an example of short wavelength recording and reproduction will be shown. FIG. 7 shows an example of recording and reproducing at a wavelength of 1 μm with the head width L=5 μm. a shows the recording state, b shows the playback state, c shows the playback waveform, and d shows the output waveform when the S/N is improved using the mix circuit. That is, it can be seen that short wavelength recording and reproduction is possible by recording in burst form, regardless of the head width.

ここで、記録する区間は、再生ヘツド幅Lによ
つて決定され、記録ヘツド幅には何ら関係しない
ため、記録ヘツド幅がLである必要はない。また
ヘツド幅Lを有する記録再生ヘツドを使用するよ
うにしてもよい。
Here, the recording section is determined by the reproduction head width L and has no relation to the recording head width, so the recording head width does not need to be L. Alternatively, a recording/reproducing head having a head width L may be used.

このように、従来の垂直磁気記録方式におい
て、再生ヘツド幅Lとするとλ=L/n(nは自
然数)なる波長をもつ信号は再生できなかつた
が、以上述べてきたように、記録ヘツドが記録媒
体上を多くとも距離Lを移動する間だけ記録し、
次の少なくとも距離L移動する間記録を停止す
る、いわゆるバースト状に記録することにより、
短波長領域までフラツトな周波数特性が再生で
き、良好な短波長記録再生が可能となる。
In this way, in the conventional perpendicular magnetic recording system, it was not possible to reproduce a signal with a wavelength of λ = L/n (n is a natural number), where the width of the reproducing head is L. Record only while moving a distance L at most on the recording medium,
By recording in a so-called burst, in which recording is stopped while moving at least a distance L,
A flat frequency characteristic can be reproduced up to the short wavelength region, and good short wavelength recording and reproduction is possible.

また再生出力としては、再生ヘツド先端部分に
よる再生信号、つまり信号が再生され始めてから
再生ヘツドが記録媒体上を相対的に多くとも距離
L移動する間に得られた情報を用いてもよく、ま
た再生ヘツド後端部分による再生信号、つまり信
号が再生され始めてから再生ヘツドが記録媒体上
を相対的に少なくとも距離L移動した後より得ら
れる情報を用いてもよく、また本実施例で述べた
如く上記両方の情報を合成することによつても得
ることができる。
Further, as the reproduction output, a reproduction signal from the leading end of the reproduction head, that is, information obtained while the reproduction head moves relatively at most a distance L over the recording medium after the signal starts to be reproduced may be used. The reproduction signal from the rear end portion of the reproduction head, that is, the information obtained after the reproduction head has moved at least a distance L relative to the recording medium after the signal starts to be reproduced may be used, and as described in this embodiment. It can also be obtained by combining both of the above information.

また上記説明では、アナログ信号の記録再生の
例を示したが、本発明は原理的にデイジタル記録
再生に適しており、その場合デイジタル信号2ビ
ツト長が本説明で述べた1波長に相当すると考え
てよい。
Furthermore, in the above explanation, an example of recording and reproducing an analog signal was shown, but in principle, the present invention is suitable for digital recording and reproducing, and in that case, it is considered that the 2-bit length of the digital signal corresponds to one wavelength as described in this explanation. It's fine.

発明の効果 以上の説明で明らかなように、本発明によれ
ば、これらは垂直磁気記録であるので、記録の際
に記録減磁が発生せず、また再生においても短波
長再生が可能となるため、記録再生密度は飛躍的
に向上する。
Effects of the Invention As is clear from the above explanation, according to the present invention, since these are perpendicular magnetic recording, recording demagnetization does not occur during recording, and short wavelength reproduction is possible during reproduction. Therefore, the recording and reproducing density is dramatically improved.

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

第1図は垂直記録方式を示した図、第2は垂直
記録方式での再生を示した図、第3図は本発明で
の再生を示した図、第4図は本発明の再生におけ
るヘツドコア内の磁束と再生出力を示した図、第
5図は本発明の再生方法を説明するための図、第
6図は再生方法の一例を示すブロツク図、第7図
は高密度記録再生を示した図である。 1……主磁極、2……記録波形、3……磁気テ
ープ、4……補助磁極、5……巻線、6……反転
回路、7……ミツクス回路、9……遅延回路。
Figure 1 is a diagram showing the perpendicular recording system, Figure 2 is a diagram showing reproduction in the perpendicular recording system, Figure 3 is a diagram showing reproduction in the present invention, and Figure 4 is a diagram showing the head core in reproduction in the present invention. Figure 5 is a diagram for explaining the reproduction method of the present invention, Figure 6 is a block diagram showing an example of the reproduction method, and Figure 7 shows high-density recording and reproduction. This is a diagram. 1... Main magnetic pole, 2... Recording waveform, 3... Magnetic tape, 4... Auxiliary magnetic pole, 5... Winding wire, 6... Inverting circuit, 7... Mixing circuit, 9... Delay circuit.

Claims (1)

【特許請求の範囲】 1 磁気記録媒体の磁気層に対し、その厚み方向
に磁化することにより情報の記録を行うように構
成され、かつ、磁極の厚さLを有する記録再生磁
極または記録磁極と磁極の厚さLを有する再生磁
極を具備し、前記記録再生磁極または記録磁極が
記録媒体上を相対的に多くとも距離L移動する区
間だけ信号を記録し、次に前記記録再生磁極また
は記録磁極が記録媒体上を相対的に少なくとも距
離L移動する区間は記録を停止するようにしたこ
とを特徴とする磁気記録再生装置。 2 記録信号の波長もしくは2ビツト長は前記記
録再生磁極または再生磁極の厚さLよりも短いこ
とを特徴とする特許請求の範囲第1項記載の磁気
記録再生装置。 3 磁気記録媒体の磁気層に対し、その厚み方向
に磁化することにより情報の記録を行うように構
成され、かつ、磁極の厚さLを有する再生磁極を
具備し、多くとも距離Lの区間だけ記録され、次
の少なくとも距離Lの区間は記録されていない前
記磁気記録媒体を、前記再生磁極により再生して
再生信号を得るようにしたことを特徴とする磁気
記録再生装置。 4 再生信号は、再生磁極が記録媒体上に記録さ
れた信号を再生し始めてから、前記記録媒体上を
相対的に多くとも距離L移動する区間に得られた
再生磁極出力からのみ得ることを特徴とする特許
請求の範囲第3項記載の磁気記録再生装置。 5 再生信号は、再生磁極が記録媒体上に記録さ
れた信号を再生し始めてから、前記記録媒体上を
相対的に距離L移動した地点よりさらに相対的に
距離L移動した地点までの区間に得られた再生磁
極出力からのみ得ることを特徴とする特許請求の
範囲第3項記載の磁気記録再生装置。 6 再生信号は、再生磁極が記録媒体上に記録さ
れた信号を再生し始めてから、前記記録媒体上を
相対的に多くとも距離L移動する区間に得られた
第1の信号と、その後さらに相対的に距離L移動
する区間に得られた第2の信号を情報とし、前記
第1の信号を所定時間遅延した後、前記第2の信
号と合成することにより得ることを特徴とする特
許請求の範囲第3項記載の磁気記録再生装置。
[Claims] 1. A recording/reproducing magnetic pole or a recording magnetic pole configured to record information by magnetizing the magnetic layer of a magnetic recording medium in its thickness direction, and having a magnetic pole thickness L. A reproducing magnetic pole having a magnetic pole thickness L is provided, the recording/reproducing magnetic pole or the recording magnetic pole records a signal only in a section in which the recording/reproducing magnetic pole or the recording magnetic pole moves relatively at most a distance L on the recording medium, and then the recording/reproducing magnetic pole or the recording magnetic pole 1. A magnetic recording and reproducing apparatus, characterized in that recording is stopped during a section in which the object moves relatively at least a distance L on a recording medium. 2. The magnetic recording/reproducing apparatus according to claim 1, wherein the wavelength or 2-bit length of the recording signal is shorter than the thickness L of the recording/reproducing magnetic pole or the reproducing magnetic pole. 3 The magnetic layer of the magnetic recording medium is configured to record information by magnetizing it in the thickness direction, and is equipped with a reproducing magnetic pole having a magnetic pole thickness L, and only in an area of a distance L at most. A magnetic recording and reproducing apparatus characterized in that a reproduced signal is obtained by reproducing the magnetic recording medium, which has been recorded and in which no data is recorded in the next section of at least a distance L, by means of the reproducing magnetic pole. 4. The reproduction signal is obtained only from the output of the reproduction magnetic pole obtained during a period in which the reproduction magnetic pole moves relatively at most a distance L on the recording medium after the reproduction magnetic pole starts reproducing the signal recorded on the recording medium. A magnetic recording and reproducing apparatus according to claim 3. 5. The reproduced signal is obtained in the interval from when the reproducing magnetic pole starts reproducing the signal recorded on the recording medium to the point where the reproducing magnetic pole has moved a relative distance L further on the recording medium. 4. The magnetic recording/reproducing apparatus according to claim 3, wherein the magnetic recording/reproducing apparatus obtains only the output from the reproduced magnetic pole. 6. The reproduction signal consists of a first signal obtained during a period in which the reproduction magnetic pole starts reproducing the signal recorded on the recording medium and then moves relatively at most a distance L on the recording medium, and then further A second signal obtained in a section where the second signal moves a distance L is used as information, and the first signal is delayed for a predetermined time and then synthesized with the second signal. The magnetic recording and reproducing device according to scope 3.
JP57140548A 1982-08-12 1982-08-12 magnetic recording and reproducing device Granted JPS5930202A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57140548A JPS5930202A (en) 1982-08-12 1982-08-12 magnetic recording and reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57140548A JPS5930202A (en) 1982-08-12 1982-08-12 magnetic recording and reproducing device

Publications (2)

Publication Number Publication Date
JPS5930202A JPS5930202A (en) 1984-02-17
JPH0258683B2 true JPH0258683B2 (en) 1990-12-10

Family

ID=15271231

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57140548A Granted JPS5930202A (en) 1982-08-12 1982-08-12 magnetic recording and reproducing device

Country Status (1)

Country Link
JP (1) JPS5930202A (en)

Also Published As

Publication number Publication date
JPS5930202A (en) 1984-02-17

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