JPS5958616A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS5958616A
JPS5958616A JP16940782A JP16940782A JPS5958616A JP S5958616 A JPS5958616 A JP S5958616A JP 16940782 A JP16940782 A JP 16940782A JP 16940782 A JP16940782 A JP 16940782A JP S5958616 A JPS5958616 A JP S5958616A
Authority
JP
Japan
Prior art keywords
output
recording medium
frequency
head
heads
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
JP16940782A
Other languages
Japanese (ja)
Inventor
Makoto Shimokooriyama
下郡山 信
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP16940782A priority Critical patent/JPS5958616A/en
Publication of JPS5958616A publication Critical patent/JPS5958616A/en
Pending 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

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

Abstract

PURPOSE:To lower and raise output levels of low frequency and high frequency regions respectively to improve the SN ratio, by arranging plural reading heads in the running direction of a magnetic recording medium and adding or subtracting their output signals and outputting results. CONSTITUTION:Reading heads 2a and 2b having an approximtely equal reproducing frequency characteristic are arranged a length (a) apart from each other in the running direction of an arrow A of a recording medium 3, and output signals are added or subtracted in an operating circuit 4. The length (a) is selected properly for the running speed of the recording medium to lower and raise output level of low and high frequency regions of the synthesized output, respectively, thus improving the SN ratio.

Description

【発明の詳細な説明】 技術分野 本発明は複数個の読出しヘッドを近接して設け、それぞ
れの読出しヘッドから出力された信号を加算又は減算す
る構成とした磁気ヘッドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to a magnetic head having a structure in which a plurality of read heads are provided close to each other and signals outputted from the respective read heads are added or subtracted.

従来技術 従来、磁気抵抗効果素子(以下M R素子と呼5)は、
磁界を検出するために用いられているか、最近では磁気
記録角化装置の読出しヘッドとしても用いられている。
Conventional technology Conventionally, a magnetoresistive element (hereinafter referred to as an MR element5) is
It has been used to detect magnetic fields or, more recently, as a read head in magnetic recording anglers.

しかし、MR素子の再生周波数特性は、例えば第1図の
グラフで示すように周波数が高くなるに従って出力され
る信号のレベルが減衰するいわゆる低域通過特性になっ
ている。
However, the reproduction frequency characteristic of the MR element is, for example, a so-called low-pass characteristic in which the level of the output signal attenuates as the frequency increases, as shown in the graph of FIG.

このような周波数特性を示す記録再生系において高密度
な記録再生を行う場合には、その特性に適応したイコラ
イザを構成して再生周波数特性の補正をしなければなら
ない。
When performing high-density recording and reproduction in a recording and reproduction system exhibiting such frequency characteristics, it is necessary to configure an equalizer adapted to the characteristics to correct the reproduction frequency characteristics.

しかし、イコライザを構成するとシステムの規模が大き
くなってしまう欠点がある。
However, configuring an equalizer has the disadvantage that the scale of the system increases.

目      的 本発明は前述したイコライザ等によって再生周波数特性
の補正をする事なく低周波数域における出力レベルを抑
制し、かつ高周波数域では出力レベルを上げる事により
SN比を向上させた磁気ヘッドを提供する事を目的とし
ている。
Purpose The present invention provides a magnetic head that suppresses the output level in the low frequency range without correcting the reproduction frequency characteristics using the above-mentioned equalizer or the like, and improves the S/N ratio by increasing the output level in the high frequency range. is intended to do.

そのために、本発明においては複数の読出しヘッドを記
録媒体の走行する方向に沿って配置し、該複数の読出し
ヘッドから出力した信号を加算し、又は減算して出力す
るように構成した。
To this end, in the present invention, a plurality of read heads are arranged along the traveling direction of the recording medium, and the signals output from the plurality of read heads are added or subtracted and output.

実施例 以下、図に示した実施例に基づいて本発明の詳細な説明
する。
EXAMPLES Hereinafter, the present invention will be explained in detail based on the examples shown in the drawings.

第2図(a) 、 (b)は本発明の磁気ヘッドの異な
る実施例をそれぞれ示した構成図である。図において、
1は基台、2a、2bは基台1の両側(図(a))又は
片側(図(b))にそれぞれ取付けられたMR素子を用
いた読出しヘッド、6は磁気テープや磁気シートなどの
磁気記録媒体、4は読出しヘッド2a、2bから出力さ
れた信号を加算し、又は減算するための演算器である。
FIGS. 2(a) and 2(b) are configuration diagrams showing different embodiments of the magnetic head of the present invention. In the figure,
1 is a base, 2a and 2b are read heads using MR elements attached to both sides (Figure (a)) or one side (Figure (b)) of the base 1, and 6 is a magnetic tape, magnetic sheet, etc. The magnetic recording medium 4 is an arithmetic unit for adding or subtracting signals output from the read heads 2a and 2b.

第2図(a) 、 (b)において、記録媒体3が矢印
Aの方向へV″/s e c  の速度で走行している
とする。
In FIGS. 2(a) and 2(b), it is assumed that the recording medium 3 is traveling in the direction of arrow A at a speed of V''/sec.

いま、再生周波数特性等が互いにはぼ等しい読出しヘラ
)”2a、2bを基台1の両側又は片側で距離amだけ
離して設けると、読出しヘッド2bから出力する信号は
読出しヘッド2aから出力する信号より一秒遅延されて
出力する。
Now, if the readout head 2a and 2b, which have substantially the same reproduction frequency characteristics, are provided on both sides or one side of the base 1, separated by a distance am, the signal output from the readout head 2b will be the same as the signal outputted from the readout head 2a. The output is delayed by one second.

このため、読出しヘッド2a及び2bから出力する信号
を互いに加算又は減算すると、記録媒体乙に記録されて
いる情報の周波数に応じて第3図のグラフに示したよう
な周波数特性を持たせる事が出来る。
Therefore, when the signals output from the read heads 2a and 2b are added or subtracted from each other, the frequency characteristics shown in the graph of FIG. 3 can be obtained depending on the frequency of the information recorded on the recording medium B. I can do it.

例えば、周波数が極めて低い部分(グラフの左端)では
誌出しヘッド2a及び2bから出力する信号はほぼ等し
いレベルであるから加算すれば最大値となる特性5(破
lIM)を呈し、減算すれば最小値となる特性6(実線
)を呈する事が分かる。
For example, in the part where the frequency is extremely low (the left end of the graph), the signals output from the magazine feed heads 2a and 2b are at almost the same level, so if they are added, the maximum value is characteristic 5 (broken IIM), and if they are subtracted, the signal is the minimum value. It can be seen that the value exhibits characteristic 6 (solid line).

ここで、遅延した信号を減算することで得られる周波数
特性G (f)は G(f)=ls団(πf−ユ)1  ・・・(1)であ
り、同様にして加算では G(fl = 1cos(πf−,)l   ・・・(
1丁によって表わすことができる。
Here, the frequency characteristic G (f) obtained by subtracting the delayed signal is G (f) = ls group (πf - u) 1 ... (1), and similarly, by addition, G (fl = 1cos(πf-,)l...(
It can be represented by one piece.

一方、耽出しヘッドの周波数特性をH(f)とすると、
記録再生系によって得られる周波数特性T (f)は T(f) = Cr ffl −H(f)      
・・・(2)となる。
On the other hand, if the frequency characteristic of the indulgence head is H(f),
The frequency characteristic T(f) obtained by the recording/reproducing system is T(f) = Cr ffl −H(f)
...(2) becomes.

つまり、T (flは第1図に示した周波数特性を有し
、G (f)は第3図の特性5又は乙に示した周波数特
性を有するものである。
That is, T (fl has the frequency characteristic shown in FIG. 1, and G (f) has the frequency characteristic shown in characteristic 5 or B of FIG. 3.

いま、第3図に示した特性6(実線)においてv/2a
=10h旧l となるように設定するためには、記録媒
体30走行速度をv” 7.5 m/seeとすると第
2図fa) 、 (b)に示したヘッド間距離はa−0
,675Iijnとなる。
Now, in characteristic 6 (solid line) shown in Fig. 3, v/2a
In order to set the recording medium 30 running speed to v'' 7.5 m/see, the distance between the heads shown in Figure 2 fa) and (b) is a-0.
, 675Iijn.

つまり、ヘッド間距離aと記録媒体の走行速度Vとを前
述した値に定めた場合には、0〜10〜420周波数範
囲内において低域周波数で出力レベルを減衰させるよう
に作用する。従って、読出しヘッド2a 、 2bの出
力信号を減算する事によって得られる特性6(第6図)
の再生系に対して、第1図に示したように低域周波数で
出力レベルの高い信号・を通せば、第4図に示したより
な特性が得られて周波数特性を平滑化する事が可能にな
る。
That is, when the distance a between the heads and the running speed V of the recording medium are set to the above-mentioned values, the output level is attenuated at low frequencies within the frequency range of 0 to 10 to 420. Therefore, characteristic 6 (Fig. 6) obtained by subtracting the output signals of the read heads 2a and 2b
If you pass a signal with a low frequency and high output level to the reproduction system as shown in Figure 1, you can obtain the characteristics shown in Figure 4 and smooth the frequency characteristics. become.

そして、D50と呼ばれる周波数特性の最大値から、最
大値の半値(Σの値)罠なるまでの周波数帯域が広くな
り、かつ高域周波数においてSN比が改善される。具体
的には第6図において時局波数においてはSN比が3d
B改善される。
Then, the frequency band from the maximum value of the frequency characteristic called D50 to the half value of the maximum value (the value of Σ) becomes wider, and the S/N ratio is improved at high frequencies. Specifically, in Figure 6, the S/N ratio is 3d at the local wave number.
B.Improved.

尚、第2図t8) 、 (b)に示した耽出しヘッド2
a。
In addition, the indulgence head 2 shown in Fig. 2 t8) and (b)
a.

2bは薄膜技術を用いて製造するが、前述したようなヘ
ッド間距離a = 0.575μmで(工、第2図(b
lに示したように基台1の片側でNI I?素子を積層
させる構成が実用的である。
2b is manufactured using thin film technology, and the head-to-head distance a = 0.575 μm as described above (Fig. 2(b)).
NI I? on one side of the base 1 as shown in 1. A configuration in which elements are stacked is practical.

このような薄膜積層ヘッドにおいて、各読出しヘッド部
を構成するNjR素子部分を直列又は並列に接続して演
算器40機能を持たせる事ができろ。第5図(a) 、
 (b)はM几素子部分をそれぞれ直列又は並列に接続
した等何回路を表わしている。
In such a thin film laminated head, it would be possible to provide the function of the arithmetic unit 40 by connecting the NjR element portions constituting each read head section in series or in parallel. Figure 5(a),
(b) represents a circuit in which M element parts are connected in series or in parallel.

紀5図(a)において、抵抗損、R12はM R素子で
あり、電圧源Eから直列に接続された抵抗R1,R2に
バイアス電61t、を供給する。
In Fig. 5(a), resistance loss R12 is an MR element, and a bias current 61t is supplied from voltage source E to resistors R1 and R2 connected in series.

いま、抵抗R1,R2を第2図に示した読出しヘッド2
a 、2bに対応させて記録媒体ろから情報な読出した
とすると、抵抗i(,1,R2の抵抗値は磁束の変化に
対応してそれぞれR1+ΔR+ 、 R2+△R2の値
に変化する。ここで、R,1==R2= R、R>ΔR
1゜△R2とすると、出力端子7a、7b間の電圧の変
化分△Vは △■=に1(△R2−△R1)    ・・・(6)で
表わす事ができる。(但し、klは定数)。
Now, resistors R1 and R2 are connected to the read head 2 shown in FIG.
When information is read from the recording medium in correspondence to a and 2b, the resistance values of the resistors i(,1 and R2 change to the values of R1+ΔR+ and R2+ΔR2, respectively, in response to changes in magnetic flux.Here, R,1==R2=R,R>ΔR
Assuming 1° ΔR2, the variation ΔV in the voltage between the output terminals 7a and 7b can be expressed as Δ■=1(ΔR2−ΔR1) (6). (However, kl is a constant).

即ち、第2図に示した耽出しヘッド2a、2bの出力部
分を第5図に示した構成にすれば2つのヘッドの差の出
力を取出す事が出来るので第6図に示した特性6を呈し
、従って第4図に示した出力特性が容易に得られる。
That is, if the output parts of the indulgence heads 2a and 2b shown in FIG. 2 are configured as shown in FIG. 5, it is possible to extract the output difference between the two heads, so that characteristic 6 shown in FIG. 6 can be obtained. Therefore, the output characteristics shown in FIG. 4 can be easily obtained.

同様にして、@5図山)に示した減η、のための等価回
路において、R1二R2=TL 、 RL =)(、/
2  とすると出力端子f3a 、 !3b間の電圧の
変化分△Vは△V == &2 (△R1+△n2 )
    @ −(3)’で表わす事ができる。(但し、
k2は定数)。
Similarly, in the equivalent circuit for reduction η shown in @5 Figure 2), R12R2=TL, RL=)(,/
2, the output terminal f3a, ! The change in voltage between 3b △V is △V == &2 (△R1+△n2)
It can be expressed as @-(3)'. (however,
k2 is a constant).

尚、以上の説明においては、2個の読出しヘッドを用い
たものであるが、読出しヘッドの数を2個以上の複数個
とし、それぞれの出力レベルを変えておき、それらの出
力信号を加算し、又は減算する事で望み通りの周波数特
性を得るようにする事も可能である。
In the above explanation, two reading heads are used, but the number of reading heads is two or more, the output level of each is changed, and the output signals are added. Alternatively, it is also possible to obtain the desired frequency characteristics by subtracting.

効   果 前述の如く、再生周波数特性のレベル変化を少なくして
周波数帯域を広くし、高域周波数でSN比を改善できる
。更に、イコライザなどの附加回路を全く必要とせず、
しかもヘッドの取扱いは従来の単体のヘッドと同じであ
るから、装置を簡略化して信頼性の向上を計ることがで
きる。
Effects As mentioned above, it is possible to reduce level changes in the reproduced frequency characteristics, widen the frequency band, and improve the S/N ratio at high frequencies. Furthermore, there is no need for additional circuits such as equalizers,
Furthermore, since the head is handled in the same way as a conventional stand-alone head, the device can be simplified and reliability can be improved.

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

第1図は胱出しヘッド単体の周波数特性を示すグラフ図
、第2図(a) 、 (b)は本発明の磁気ヘッドの異
なる実施例をそれぞれ示した構成図、第3図は演算器に
よって加算又は減算された場合の周波数特性を示したグ
ラフ図、第4図は第1図に示す特性を第3図に示す特性
の系を通す事によって得られるグラフ図、第5図(a)
 、 (b)はそれぞれ減算回路及び加算回路を示した
等価回路の回路図。 1・・・基台 2a、2b・・・読出しヘッド6・・・
記録媒体 4・・・演算回路 周波数f (MHz)
Fig. 1 is a graph showing the frequency characteristics of a single bladder removal head, Fig. 2 (a) and (b) are block diagrams showing different embodiments of the magnetic head of the present invention, and Fig. 3 is a graph showing the frequency characteristics of a single bladder removal head. A graph showing the frequency characteristics when added or subtracted, Figure 4 is a graph obtained by passing the characteristics shown in Figure 1 through the system of characteristics shown in Figure 3, Figure 5 (a)
, (b) is a circuit diagram of an equivalent circuit showing a subtraction circuit and an addition circuit, respectively. 1... Base 2a, 2b... Read head 6...
Recording medium 4... Arithmetic circuit frequency f (MHz)

Claims (1)

【特許請求の範囲】[Claims] 磁気記録媒体の走行方向KGつて複数個の続出しヘッド
を配置し該複数個の読出しヘッドの出力信号を加算又は
減算して出力する構成とした事を特徴とする磁気ヘッド
A magnetic head characterized in that a plurality of successive heads are arranged in a running direction KG of a magnetic recording medium, and output signals of the plurality of reading heads are added or subtracted and output.
JP16940782A 1982-09-28 1982-09-28 Magnetic head Pending JPS5958616A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16940782A JPS5958616A (en) 1982-09-28 1982-09-28 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16940782A JPS5958616A (en) 1982-09-28 1982-09-28 Magnetic head

Publications (1)

Publication Number Publication Date
JPS5958616A true JPS5958616A (en) 1984-04-04

Family

ID=15886022

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16940782A Pending JPS5958616A (en) 1982-09-28 1982-09-28 Magnetic head

Country Status (1)

Country Link
JP (1) JPS5958616A (en)

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