JPS5946042B2 - Magnetic information reproducing device - Google Patents

Magnetic information reproducing device

Info

Publication number
JPS5946042B2
JPS5946042B2 JP51004833A JP483376A JPS5946042B2 JP S5946042 B2 JPS5946042 B2 JP S5946042B2 JP 51004833 A JP51004833 A JP 51004833A JP 483376 A JP483376 A JP 483376A JP S5946042 B2 JPS5946042 B2 JP S5946042B2
Authority
JP
Japan
Prior art keywords
magnetoresistive element
pulse
current
magnetic
magnetic 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.)
Expired
Application number
JP51004833A
Other languages
Japanese (ja)
Other versions
JPS5288315A (en
Inventor
立雄 藤原
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP51004833A priority Critical patent/JPS5946042B2/en
Publication of JPS5288315A publication Critical patent/JPS5288315A/en
Publication of JPS5946042B2 publication Critical patent/JPS5946042B2/en
Expired 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
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/33Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only
    • G11B5/39Structure or manufacture of flux-sensitive heads, i.e. for reproduction only; Combination of such heads with means for recording or erasing only using magneto-resistive devices or effects
    • 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

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Description

【発明の詳細な説明】 本発明は、磁気抵抗素子からなる再生ヘッドを用いた磁
気情報の再生装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic information reproducing apparatus using a reproducing head made of a magnetoresistive element.

第1図に従来の磁気抵抗素子を用いた磁気情報の再生装
置の一例を示す。
FIG. 1 shows an example of a magnetic information reproducing apparatus using a conventional magnetoresistive element.

磁気テープ1に記録されている磁気情報を磁気抵抗素子
2を介して取り出す場合、磁気抵抗素子2が磁気テープ
1から受ける磁界をH)磁界による磁気抵抗素子2の電
気抵抗分を」R、定電流回路3により磁気抵抗素子2に
流す電流をIとすると、適当なバイアス磁界のもとで磁
気抵抗素子2の両端に生じる電圧EはEocJR−I−
Hなる関係を持つ。これより磁気抵抗素子2の両端電圧
Eを大きくし、これを出力信号として再生アンプ4に取
り出す場合、10ΔR、Hのいずれかを大きくしなけれ
ばならないが、Hは磁気テープ1に記録されている磁気
情報により決定され、ΔRは磁気抵抗素子2の特性によ
り決定される。従つて大きな出力信号を得るためには磁
気抵抗素子2に流す電流Iを大きくする以外にないが、
Iを大きくすると磁気抵抗素子2の消費電力が大きくな
り、ついには磁気抵抗素子2を破壊するにいたる。特に
磁気抵抗素子は薄膜構造によるため磁気抵抗素子に流し
得る電流の制限はきびしく、大きな出力信号を取り出す
ための支障となつている。本発明はこのような事情に鑑
み、磁気抵抗素子を用いた磁気情報の再生装置において
出力信号を大幅に増大することのできる磁気情報の再生
装置を提供することを目的とする。
When magnetic information recorded on the magnetic tape 1 is retrieved via the magnetoresistive element 2, the magnetic field that the magnetoresistive element 2 receives from the magnetic tape 1 is defined as: H) The electric resistance of the magnetoresistive element 2 due to the magnetic field is defined as "R". If the current flowing through the magnetoresistive element 2 by the current circuit 3 is I, the voltage E generated across the magnetoresistive element 2 under an appropriate bias magnetic field is EocJR-I-
They have an H relationship. If you want to increase the voltage E across the magnetoresistive element 2 and take it out as an output signal to the reproduction amplifier 4, either 10ΔR or H must be increased, but H is recorded on the magnetic tape 1. It is determined by magnetic information, and ΔR is determined by the characteristics of the magnetoresistive element 2. Therefore, the only way to obtain a large output signal is to increase the current I flowing through the magnetoresistive element 2.
When I is increased, the power consumption of the magnetoresistive element 2 increases, which eventually leads to the destruction of the magnetoresistive element 2. In particular, since the magnetoresistive element has a thin film structure, the current that can be passed through the magnetoresistive element is severely limited, which is an obstacle to extracting a large output signal. In view of these circumstances, it is an object of the present invention to provide a magnetic information reproducing device that uses a magnetoresistive element and can significantly increase the output signal.

以下、本発明を第2図に示す一実施例により説明する。The present invention will be explained below with reference to an embodiment shown in FIG.

磁気テープ5に磁気抵抗素子6を対向設置させる。磁気
テープ5の表面には情報としての磁界Hが発生していて
磁気テープ5の矢印A方向への移動により磁界Hは変化
する。この磁界Hの変化を時間Tを横軸として表わすと
第3図aのようになる。定電流パルス回路7を磁気抵抗
素子6に接続し、磁気抵抗素子6にパルス高が一定であ
るよう・なパルス電流を間欠的に流す。このパルス電流
の波形を第3図bに示す。ここでパルス休止i 期間は
パルス電流が零になるパルス(RZパルス:リターント
ウゼロパルス)とすると、磁気抵抗素子6の両端電圧E
sはEs=ΔR−H−Ipとなる。但しIpはパルス電
流のピーク値、Esはパルス電圧のピーク値であつて、
このEsが出力信・ 号となる。出力信号Esは第3図
cに示すように高さの異るパルス列となる。このパルス
列を再生アンプ等の検出器8で検出したのちサンプル・
ホールド回路9でサンプル・ホールドすることにより第
3図dに示すような波形信号が得られる。この信号をフ
イルタ回路10を通過させることにより第3図eに示す
ような出力を得ることができる。なおサンプル・ホール
ド回路9におけるサンプリングは磁気抵抗素子6に流す
電流1がピークになつた時に定電流パルス回路7と同期
して行う必要がある。また磁気抵抗素子6に流すパルス
電流1の周期tは短(・ほど正確な再生ができるが平均
電流値の点で自ら制限がある。なおパルス電流1の周期
tより導びかれるパルス周波数はサンプリング定理より
少なくとも再生しようとする信号の2倍以上は必要であ
る。このような装置における磁気抵抗素子での消費電力
は12・ΔRとなり平均電流1の2乗に比例する。
A magnetoresistive element 6 is placed opposite to the magnetic tape 5. A magnetic field H as information is generated on the surface of the magnetic tape 5, and the magnetic field H changes as the magnetic tape 5 moves in the direction of arrow A. When the change in the magnetic field H is expressed with time T as the horizontal axis, it becomes as shown in FIG. 3a. A constant current pulse circuit 7 is connected to the magnetoresistive element 6, and a pulse current having a constant pulse height is intermittently passed through the magnetoresistive element 6. The waveform of this pulse current is shown in FIG. 3b. Here, assuming that the pulse rest i period is a pulse in which the pulse current becomes zero (RZ pulse: return-to-zero pulse), the voltage E across the magnetoresistive element 6
s becomes Es=ΔR−H−Ip. However, Ip is the peak value of the pulse current, Es is the peak value of the pulse voltage,
This Es becomes the output signal. The output signal Es becomes a pulse train having different heights as shown in FIG. 3c. After detecting this pulse train with a detector 8 such as a reproducing amplifier, the sample
By sampling and holding in the hold circuit 9, a waveform signal as shown in FIG. 3d is obtained. By passing this signal through the filter circuit 10, an output as shown in FIG. 3e can be obtained. Note that sampling in the sample/hold circuit 9 must be performed in synchronization with the constant current pulse circuit 7 when the current 1 flowing through the magnetoresistive element 6 reaches its peak. In addition, the shorter the period t of the pulse current 1 flowing through the magnetoresistive element 6, the more accurate reproduction is possible, but there is a limit in terms of the average current value.The pulse frequency derived from the period t of the pulse current 1 is sampled. According to the theorem, at least twice the signal to be reproduced is required.The power consumption of the magnetoresistive element in such a device is 12·ΔR, which is proportional to the square of the average current 1.

このため、本発明のようにパルス電流を磁気抵抗素子6
に流す場合、平均電流1は小さくなり消費電力も非常に
小さくなる。従つて従来の装置と同じ平均電流を使用す
るものとすればパルス電流のピーク値を十分大きくする
ことができる。このため出力電圧は非常に大きく従来の
装置に比して10倍以上にもなる。又、従来と同一出力
電圧を得る場合には磁気抵抗素子6における消費電力を
小さ−ぐでき、磁気抵抗素子6の温度上昇を低く抑える
ことができる二一なお、上述した実施例においては磁気
記録媒体として磁気テープ5を用いた例を示したが、こ
れに限らず他の磁気記録媒体たとえば磁気カードあ〉る
いは磁気ドラム等であつても良い。
Therefore, as in the present invention, the pulse current is passed through the magnetoresistive element 6.
When the current is passed through the current, the average current 1 becomes small and the power consumption becomes very small. Therefore, if the same average current as in the conventional device is used, the peak value of the pulse current can be made sufficiently large. Therefore, the output voltage is extremely large, more than 10 times that of conventional devices. Furthermore, when obtaining the same output voltage as the conventional one, the power consumption in the magnetoresistive element 6 can be reduced, and the temperature rise of the magnetoresistive element 6 can be kept low. Although an example has been shown in which the magnetic tape 5 is used as the medium, the present invention is not limited to this, and other magnetic recording media such as a magnetic card or a magnetic drum may be used.

又、磁気抵抗素子に流すパルス電流としては、休止期間
に零に戻らないパルスを用いても本発明の効果はある。
つまり、磁気抵抗素子に微小電流を流しつつ、これにパ
ルス電流を重畳させるようにしてもよい。要するに本発
明はその要旨を逸脱しない範囲で種種変形して実施する
ことができる。以上説明したように本発明は磁気抵抗素
子を用いた磁気情報の再生装置において、磁気抵抗素子
に流す電流にパルス電流を用いるようにしたので、出力
信号を大幅に増大することを可能とした磁気情報の再生
装置を提供できる。
Further, the effect of the present invention can be obtained even if a pulse current that does not return to zero during the rest period is used as the pulse current flowing through the magnetoresistive element.
In other words, while a minute current is flowing through the magnetoresistive element, a pulse current may be superimposed thereon. In short, the present invention can be implemented with various modifications without departing from the gist thereof. As explained above, the present invention uses a pulse current as the current flowing through the magnetoresistive element in a magnetic information reproducing device using a magnetoresistive element, so that the magnetic It is possible to provide an information reproducing device.

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

第1図は従来の磁気情報再生装置の一例を示す図、第2
図は本発明の一実施例の構成を示す図、第3図a−eは
同実施例の動作を示す波形図で、aは磁気情報による磁
界Hの波形図、bは磁気抵抗素子に流れるパルス電流P
の波形図、cは磁気抵抗素子の両端に生じるパルス電圧
Esの波形図、dはサンプル・ホールドされた電圧の波
形図、eはフイルタ一を通つた再生出力電圧の波形図で
ある。 1,5・・・・・・磁気テープ、2,6・・・・・・磁
気抵抗素子、3・・・・・・定電流回路、4・・・・・
・再生アンプ、7・・・・・・定電流パルス回路、8・
・・・・・検出器、9・・・・・・サンプル・ホールド
回路、10・・・・・・フイルタ一回路、11・・・・
・・積分回路。
Fig. 1 shows an example of a conventional magnetic information reproducing device, Fig. 2 shows an example of a conventional magnetic information reproducing device;
The figure is a diagram showing the configuration of an embodiment of the present invention, and Figures 3a to 3e are waveform diagrams showing the operation of the same embodiment, where a is a waveform diagram of the magnetic field H due to magnetic information, and b is a waveform diagram of the magnetic field H flowing through the magnetoresistive element. Pulse current P
c is a waveform diagram of the pulse voltage Es generated across the magnetoresistive element, d is a waveform diagram of the sampled and held voltage, and e is a waveform diagram of the reproduced output voltage passed through the filter 1. 1, 5... Magnetic tape, 2, 6... Magnetoresistive element, 3... Constant current circuit, 4...
・Reproduction amplifier, 7... Constant current pulse circuit, 8.
...Detector, 9...Sample/hold circuit, 10...Filter circuit, 11...
...Integrator circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 磁気記録媒体と、この記録媒体の記録面に対向設置
された磁気抵抗素子からなる再生ヘッドと、このヘッド
に繰返しパルス信号を与える回路と、上記パルス信号印
加時に前記磁気抵抗素子の両端に生じる信号を検出する
手段と、この検出手段によつて検出された信号をサンプ
ル・ホールドして磁気情報を取り出す回路とを備えたこ
とを特徴とする磁気情報の再生装置。
1. A magnetic recording medium, a reproducing head consisting of a magnetoresistive element placed opposite to the recording surface of the recording medium, a circuit that repeatedly applies a pulse signal to this head, and a magnetic recording medium generated at both ends of the magnetoresistive element when the pulse signal is applied. 1. A reproducing device for magnetic information, comprising: means for detecting a signal; and a circuit for sampling and holding the signal detected by the detecting means to extract magnetic information.
JP51004833A 1976-01-19 1976-01-19 Magnetic information reproducing device Expired JPS5946042B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51004833A JPS5946042B2 (en) 1976-01-19 1976-01-19 Magnetic information reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51004833A JPS5946042B2 (en) 1976-01-19 1976-01-19 Magnetic information reproducing device

Publications (2)

Publication Number Publication Date
JPS5288315A JPS5288315A (en) 1977-07-23
JPS5946042B2 true JPS5946042B2 (en) 1984-11-10

Family

ID=11594685

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51004833A Expired JPS5946042B2 (en) 1976-01-19 1976-01-19 Magnetic information reproducing device

Country Status (1)

Country Link
JP (1) JPS5946042B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54113315A (en) * 1978-01-30 1979-09-04 Secr Defence Brit Magnetic reluctance reader
US4625245A (en) * 1983-12-12 1986-11-25 White R Kent Magnetic recording

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
IBM TECHNICAL DISCLOSURE BULLETIN=1972 *
IEEE TRANSACTIONS ON AUDIO=1965 *

Also Published As

Publication number Publication date
JPS5288315A (en) 1977-07-23

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