JPS63253501A - Magnetic recorder - Google Patents

Magnetic recorder

Info

Publication number
JPS63253501A
JPS63253501A JP8827587A JP8827587A JPS63253501A JP S63253501 A JPS63253501 A JP S63253501A JP 8827587 A JP8827587 A JP 8827587A JP 8827587 A JP8827587 A JP 8827587A JP S63253501 A JPS63253501 A JP S63253501A
Authority
JP
Japan
Prior art keywords
temp
magnetic recording
magnetic
coefft
recording medium
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.)
Granted
Application number
JP8827587A
Other languages
Japanese (ja)
Other versions
JPH0619803B2 (en
Inventor
Takayuki Takeda
武田 隆幸
Masamichi Tagami
勝通 田上
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP62088275A priority Critical patent/JPH0619803B2/en
Publication of JPS63253501A publication Critical patent/JPS63253501A/en
Publication of JPH0619803B2 publication Critical patent/JPH0619803B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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 Record Carriers (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To hold the deterioration in an overwrite erasing rate at an extremely small value by a change in ambient temp. by providing a magnetic recording medium which consists essentially of Co and Cr and is added respectively specific ratios of Zr or Hf or Ta. CONSTITUTION:The magnetic recording medium which consists essentially of Co and Cr and is added respectively with 1.2-2.0at.% or 1.3-2.3at.% or 1.5-2.5at.% Zr or Hf or Ta is provided. The temp. coefft. of the coercive force approximate to the temp. coefft. of the saturation magnetic flux density of 'SENDUST(R)' is thereby provided to the magnetic recording medium. The temp. change dy/dT of a recording depth y attains dy/dTproportional aBS-aHC if the temp. coefft. aBS of the saturation magnetic flux density of a head and the temp. coefft. aHC of the coercive force of the medium are set at the approximate values in such a manner and, therefore, the magnetic recorder which is less changed in recording depth by temp. is formed. The deterioration of the over write erasing rate is thus extremely minimized.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、フレキシブルディスクやハードディスクなど
、消去を行わず、重ね書き(オーバーライド)によりデ
ータの書き換えを行う磁気記録装置に関するものである
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a magnetic recording device, such as a flexible disk or a hard disk, that rewrites data by overwriting without erasing.

(従来の技術) 第4図は従来のオーバーライドの概念図である。(Conventional technology) FIG. 4 is a conceptual diagram of a conventional override.

媒体1に記録されている信号6の上に広めのギャップ長
のヘッド2により新しい信号4を重ね書き(オーバーラ
イド)することによって、同時に前の信号を消去するも
のである。温度等の変化により記録領域3の大きさが多
少変わっても、媒体の底まで達しているので、十分な消
去率が得られる。
By overwriting a new signal 4 on top of the signal 6 recorded on the medium 1 using the head 2 with a wider gap length, the previous signal is simultaneously erased. Even if the size of the recording area 3 changes somewhat due to changes in temperature, etc., a sufficient erasing rate can be obtained because it reaches the bottom of the medium.

(発明が解決しようとする問題点) 以上述べたオーバーライドは、記録密度が低い、すなわ
ち、ヘッドのギャップ長が広く媒体の底まで十分に飽和
記録できるような装置では問題なく機能した。
(Problems to be Solved by the Invention) The above-mentioned override functioned without problems in an apparatus with a low recording density, that is, with a wide head gap length and capable of performing saturation recording sufficiently to the bottom of the medium.

一方、単層垂直媒体とリングヘッドによる垂直磁気記録
では、急峻な書き込み磁場が得られる狭ギャップのヘッ
ドと比較的厚めの媒体の組み合わせで、良好な記録再生
特性が得られている(信学技報MR81−8fリングヘ
ッドによる垂直異方性膜への記録」)。このような組み
合わせでは、媒体を底まで十分に飽和記録することは困
難で、表層記録に近いものとなる。
On the other hand, in perpendicular magnetic recording using a single-layer perpendicular medium and a ring head, good recording and reproducing characteristics are obtained by combining a narrow gap head that can obtain a steep writing magnetic field and a relatively thick medium (IEICE (Recording on a vertically anisotropic film using a MR81-8f ring head). With such a combination, it is difficult to perform saturation recording to the bottom of the medium, resulting in near-surface recording.

このときに問題となるのはオーバーライド消去率の確保
である。媒体の磁気特性を選べば、表層記録であっても
一28dB程度のオーバーライド消去率が確保できる(
第2図)が、媒体の抗磁力やヘッドの飽和磁束密度が温
度により変化すると、第3図のように記録深さが変化し
、消し残りの信号5のためにオーバーライド消去率が劣
化する。(第10回日本応用磁気学会学術講演概要集5
aA−9)本発明の目的は、このような欠点をなくし、
使用温度が変化してもオーバーライド消去率が劣化する
ことのない磁気記録装置を提供することにある。
The problem at this time is ensuring the override erasure rate. By selecting the magnetic properties of the medium, it is possible to secure an override erasure rate of about -28 dB even for surface recording (
2), but when the coercive force of the medium and the saturation magnetic flux density of the head change with temperature, the recording depth changes as shown in FIG. 3, and the override erasing rate deteriorates due to the unerased signal 5. (The 10th Japanese Society of Applied Magnetics Academic Lecture Abstracts 5
aA-9) The purpose of the present invention is to eliminate such drawbacks,
It is an object of the present invention to provide a magnetic recording device whose override erasure rate does not deteriorate even if the operating temperature changes.

(問題点を解決するだめの手段) 本発明の磁気記録装置は、ギャップの近傍もしくはコア
全体がセンダスト系合金からなる磁気ヘッドと、Coと
Crを主成分とし、1.2〜2.0at%のZr、1.
3〜2.3at%Hf、1.5〜2.5at%のTaの
いづれがが添加されている記録媒体の構成であることを
特徴としている。
(Means for Solving the Problems) The magnetic recording device of the present invention has a magnetic head in which the vicinity of the gap or the entire core is made of a Sendust alloy, and the main components are Co and Cr, and 1.2 to 2.0 at% Zr, 1.
The recording medium is characterized in that either 3 to 2.3 at% Hf or 1.5 to 2.5 at% Ta is added.

(作用) このような添加物を入れることにより、CoCr膜では
一〇、34%/degであった抗磁力の温度係数が第1
図のように変化する。図中の破線はセンダストの飽和磁
束密度の温度係数−0,11%/degを示したもので
ある。前述のような添加量とすることで、センダストの
飽和磁束密度の温度係数と近い抗磁力の温度係数を持つ
媒体になる。このようにヘッドの飽和磁束密度の温度係
数QBsと媒体の抗磁力の温度係数αHeが近い値にし
であると、記録深さyの温度変化dy/dTが となることから、温度による記録深さの変化が少ない磁
気記録装置ができる。したがって、温度変化による第3
図のようなオーバーライド消去率の劣化をきわめて小さ
くできる。
(Function) By adding such additives, the temperature coefficient of coercive force, which was 10.34%/deg in the CoCr film, became the first.
It changes as shown in the figure. The broken line in the figure indicates the temperature coefficient of the saturation magnetic flux density of Sendust -0.11%/deg. By adding the amount as described above, the medium has a temperature coefficient of coercive force close to the temperature coefficient of the saturation magnetic flux density of Sendust. If the temperature coefficient QBs of the saturation magnetic flux density of the head and the temperature coefficient αHe of the coercive force of the medium are set to values close to each other in this way, the temperature change dy/dT of the recording depth y becomes It is possible to create a magnetic recording device with little change in . Therefore, the third
The deterioration of the override erasure rate as shown in the figure can be extremely minimized.

(実施例) 以下、本発明の実施例および参考例を示す。媒体は20
at%CrのCoCr合金ターゲットの上にZr、 H
f。
(Example) Examples and reference examples of the present invention are shown below. The medium is 20
Zr, H on top of CoCr alloy target with at%Cr
f.

Taのペレットをおき、RFマグネトロンスパッタにて
作成した。第1表は実施例および参考例の添加物とその
量、および抗磁力の温度係数、ギャップ長0.3pmの
センダストヘッドで測定した25°Cでのオーバーライ
ド消去率(0/W25)、10°Cで書き込ミ50°C
で重ね書きしたときのオーバーライド消去率(0/WI
Q−5Q)、50°Cで書き込み10°Cで重ね書きし
たときのオーバーライド消去率(0/W50−1o)を
まとめたものである。測定方法を述べると、先づ50k
FRPIの信号を書き込んでおき、22kFRPIの信
号を重ね書きし、重ね書きによる50kFRPIの信号
の減衰量をオーバーライド消去率とした。装置として供
するためにはO/W25、O/W10−50. O/W
50−1oのいづれもが一26dB以下である必要があ
る。
A Ta pellet was placed and produced by RF magnetron sputtering. Table 1 shows the additives and their amounts in Examples and Reference Examples, the temperature coefficient of coercive force, the override erasure rate (0/W25) at 25°C measured with a Sendust head with a gap length of 0.3 pm, and 10° Write at 50°C
Override erasure rate (0/WI
Q-5Q), the override erasure rate (0/W50-1o) when writing at 50°C and overwriting at 10°C is summarized. To explain the measurement method, first 50k
A FRPI signal was written, a 22 kFRPI signal was overwritten, and the amount of attenuation of the 50 kFRPI signal due to overwriting was taken as the override erasure rate. In order to serve as a device, O/W25, O/W10-50. O/W
50-1o must be less than 126 dB.

実施例では温度係数がセンダストの飽和磁化のそれ(−
0,11%/deg)に対して±0゜04%/degの
範囲(第1図の点線の範囲)に入っており、O/W10
−5Q。
In the example, the temperature coefficient is that of Sendust's saturation magnetization (-
O/W10 is within the range of ±0°04%/deg (range indicated by the dotted line in Figure 1).
-5Q.

01/w5o 10がO/W25に比べて大きく劣化す
ることはないが、参考例のCoCrや添加原素の少いも
のでは0/W50− IQが劣化して一26dBを上回
ってしまう。ま(発明の効果) 以上のように本発明の磁気記録装置では表層記録的であ
っても、周囲温度の変化によるオーバーライド消去率の
劣化をきわめて少く抑えることができる。
01/w5o10 does not deteriorate significantly compared to O/W25, but in the reference example of CoCr and those with a small amount of added elements, 0/W50-IQ deteriorates to exceed -26 dB. (Effects of the Invention) As described above, in the magnetic recording device of the present invention, even in surface recording, deterioration in the override erasure rate due to changes in ambient temperature can be suppressed to an extremely low level.

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

第1図は添加原素量によるCoCrZr、 CoCrH
f。 CoCrTaの抗磁力の温度係数の変化を示した図であ
る。 第2図は本発明の実施したときのオーバーライドの概念
図である。 第3図は温度特性を無視して作製した装置のオーバーラ
イドの概念図である。 第4図は従来装置のオーバーライドの概念図である。 図において、 1・・・媒体の記録層、2・・・ヘッド3・・・記録領
域、4・・・新しい信号5・・・消し残りの信号、6・
・・既に記録されている信号第1図 添加量 [at%l 第2図 第3図 第4図
Figure 1 shows CoCrZr and CoCrH depending on the amount of added elements.
f. FIG. 3 is a diagram showing changes in the temperature coefficient of coercive force of CoCrTa. FIG. 2 is a conceptual diagram of override when the present invention is implemented. FIG. 3 is a conceptual diagram of an override of a device manufactured ignoring temperature characteristics. FIG. 4 is a conceptual diagram of overriding in a conventional device. In the figure, 1...recording layer of medium, 2...head 3...recording area, 4...new signal 5...signal remaining after erasing, 6...
...Already recorded signal Fig. 1 addition amount [at%l Fig. 2 Fig. 3 Fig. 4

Claims (1)

【特許請求の範囲】 (1)ギャップの近傍もしくは全体がセンダスト系合金
からなる磁気ヘッドとCo、Cr及びZrを主成分とす
る磁気記憶媒体の構成による磁気記録装置において、磁
気記録媒体中のZrの含有量が 1.2〜2.0at%であることを特徴とする磁気記録
装置。 (2)ギャップの近傍もしくは全体がセンダスト系合金
からなる磁気ヘッドとCo、Cr及びHfを主成分とす
る磁気記録媒体の構成による磁気記録装置において、磁
気記録媒体中のHfの含有量が 1.3〜2.3at%であることを特徴とする磁気記録
装置。 (3)ギャップの近傍もしくは全体がセンダスト系合金
からなる磁気ヘッドとCo、Cr及びTaを主成分とす
る磁気記録媒体の構成による磁気記録装置において、磁
気記録媒体中のTaの含有量が 1.5〜2.5at%であることを特徴とする磁気記録
装置。
[Scope of Claims] (1) In a magnetic recording device configured with a magnetic head in which the vicinity of the gap or the entire gap is made of a Sendust-based alloy and a magnetic storage medium whose main components are Co, Cr, and Zr, Zr in the magnetic recording medium A magnetic recording device characterized in that the content of is 1.2 to 2.0 at%. (2) In a magnetic recording device configured with a magnetic head in which the vicinity of the gap or the entire gap is made of a Sendust-based alloy and a magnetic recording medium whose main components are Co, Cr, and Hf, the content of Hf in the magnetic recording medium is 1. A magnetic recording device characterized in that the concentration is 3 to 2.3 at%. (3) In a magnetic recording device configured with a magnetic head in which the vicinity of the gap or the entire gap is made of a Sendust-based alloy and a magnetic recording medium whose main components are Co, Cr, and Ta, the Ta content in the magnetic recording medium is 1. A magnetic recording device characterized in that the concentration is 5 to 2.5 at%.
JP62088275A 1987-04-09 1987-04-09 Magnetic recording device Expired - Lifetime JPH0619803B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62088275A JPH0619803B2 (en) 1987-04-09 1987-04-09 Magnetic recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62088275A JPH0619803B2 (en) 1987-04-09 1987-04-09 Magnetic recording device

Publications (2)

Publication Number Publication Date
JPS63253501A true JPS63253501A (en) 1988-10-20
JPH0619803B2 JPH0619803B2 (en) 1994-03-16

Family

ID=13938352

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62088275A Expired - Lifetime JPH0619803B2 (en) 1987-04-09 1987-04-09 Magnetic recording device

Country Status (1)

Country Link
JP (1) JPH0619803B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61182915A (en) * 1985-02-12 1986-08-15 Mitsubishi Petrochem Co Ltd Injection molding method of box-shaped two-layer molded member
JPS61213145A (en) * 1985-03-19 1986-09-22 椎名 二三幸 Composite plastic molded shape

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61182915A (en) * 1985-02-12 1986-08-15 Mitsubishi Petrochem Co Ltd Injection molding method of box-shaped two-layer molded member
JPS61213145A (en) * 1985-03-19 1986-09-22 椎名 二三幸 Composite plastic molded shape

Also Published As

Publication number Publication date
JPH0619803B2 (en) 1994-03-16

Similar Documents

Publication Publication Date Title
JPH0415521B2 (en)
JPS5968854A (en) Photomagnetic recording medium
JPS6139911A (en) Magnetic recording and reproducing device
JPS63253501A (en) Magnetic recorder
JPH0237501A (en) Magnetic recording system and magnetic recording device
Bertram et al. The print-through phenomenon
JPS63257901A (en) Magnetic recorder
JP2001319302A (en) Information recorder
JPH0785401A (en) Magnetic recording method
JP2964596B2 (en) Manufacturing method of magnetic recording medium
JPH09298114A (en) Vertical magnetic recording medium and magnetic recording device using it
JP2001283419A (en) Perpendicular magnetic recording medium and magnetic storage device
JPH06162419A (en) Magnetic recording method
JPH06162420A (en) Magnetic recording method
JP3386270B2 (en) Magnetic head and magnetic recording device
Li et al. Dependence of frequency on reverse overwrite processes in perpendicular recording
JP2511997B2 (en) Magnetic recording media
JP2508639B2 (en) Perpendicular magnetic recording media
JPS6331001A (en) Magnetic recording device
JPS63229609A (en) Both sides type magnetic head
JPH01155502A (en) Magnetic recording and reproducing device
JPH0664681B2 (en) Magnetic recording / reproducing method
JPH07272242A (en) Magnetic recording medium
JPH0319101A (en) Magnetic disk device
JPS61187102A (en) Magnetic recording and reproducing device