JPS63257901A - Magnetic recorder - Google Patents
Magnetic recorderInfo
- Publication number
- JPS63257901A JPS63257901A JP9225987A JP9225987A JPS63257901A JP S63257901 A JPS63257901 A JP S63257901A JP 9225987 A JP9225987 A JP 9225987A JP 9225987 A JP9225987 A JP 9225987A JP S63257901 A JPS63257901 A JP S63257901A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- temp
- medium
- recording
- 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.)
- Granted
Links
- 230000005291 magnetic effect Effects 0.000 title claims abstract description 35
- 229910052726 zirconium Inorganic materials 0.000 claims abstract description 9
- 229910045601 alloy Inorganic materials 0.000 claims abstract description 7
- 239000000956 alloy Substances 0.000 claims abstract description 7
- 229910052804 chromium Inorganic materials 0.000 claims abstract description 6
- 229910052758 niobium Inorganic materials 0.000 claims abstract description 5
- 229910052735 hafnium Inorganic materials 0.000 claims abstract description 3
- 229910052715 tantalum Inorganic materials 0.000 claims abstract 2
- 230000004907 flux Effects 0.000 abstract description 5
- 230000006866 deterioration Effects 0.000 abstract description 4
- 229910000702 sendust Inorganic materials 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 5
- 239000000654 additive Substances 0.000 description 4
- 230000000996 additive effect Effects 0.000 description 3
- 229910000684 Cobalt-chrome Inorganic materials 0.000 description 2
- 239000010952 cobalt-chrome Substances 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 229910001257 Nb alloy Inorganic materials 0.000 description 1
- -1 composed of Co Inorganic materials 0.000 description 1
- 238000012217 deletion Methods 0.000 description 1
- 230000037430 deletion Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 238000001755 magnetron sputter deposition Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
Landscapes
- Magnetic Record Carriers (AREA)
- Recording Or Reproducing By Magnetic Means (AREA)
Abstract
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MR81−8rリングヘ
ッドによる垂直異方性膜への記録J)。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 onto a vertically anisotropic film using a MR81-8r ring head J). 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、磁気ヘッドの特性に磁気記
録媒体の特性をあわせることによりこのような欠点をな
くし、使用温度T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 by matching the characteristics of the magnetic head with the characteristics of the magnetic recording medium, and to provide magnetic recording in which the override erase rate does not deteriorate even if the operating temperature T changes. The goal is to provide equipment.
(問題点を解決するための手段)
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Co、 Zr及びNbを主成分とする合金からな
る磁気ヘッドと、CoとCrを主成分とし、1゜9〜3
.0at%のZr、2.1〜3.5at%Hf、2.1
〜3.5at%のTaのいづれか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 includes a magnetic head in which the vicinity of the gap or the entire core is made of an alloy mainly composed of Co, Zr, and Nb, and a magnetic head mainly composed of Co and Cr. 1°9~3
.. 0 at% Zr, 2.1-3.5 at% Hf, 2.1
The recording medium is characterized in that it has a structure in which Ta is added in an amount of 3.5 at% to 3.5 at%.
(作用)
このような添加物を入れることにより、CoCr膜では
−0,34%/degであった抗磁力の温度数が第1図
のように変化する。図中の破線はCoZrNbの飽和磁
束密度の温度係数−0,032%/degを示したもの
である。(Function) By adding such an additive, the temperature number of the coercive force, which was -0.34%/deg in the CoCr film, changes as shown in FIG. The broken line in the figure indicates the temperature coefficient of the saturation magnetic flux density of CoZrNb -0,032%/deg.
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GB
Sと媒体の抗磁力の温度係数αHCが近い値にしである
と、記録深さyの温度変化dy/dTが
y
□兄αBS−αHe
T
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。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. In this way, the temperature coefficient GB of the saturation magnetic flux density of the head is
If S and the temperature coefficient αHC of the coercive force of the medium are close to each other, the temperature change dy/dT in the recording depth y becomes y □ αBS - αHe T, so there is little change in the recording depth due to temperature. A magnetic recording device is created. 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.
ra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
CozrNb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°dセ書き込み50°
Cで重ね書きしたときのオーバーライド消去(0/WI
O−50)、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(0/W5010)をまと
めたものである。測定方法を述べると、先づ50kFR
PI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0/W2s、O/WIQ 5Q、 O/W5
Q IQのいづれもが一26dB以下である必要がある
。A pellet of RA 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 CozrNb head with a gap length of 0°3 pm, and 10° d cell writing 50°
Override deletion when overwriting with C (0/WI
O-50), override erasure (0/W5010) when writing at 50°C and overwriting at 10°C. To explain the measurement method, first, 50kFR.
A PI signal was written and stored, 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. To serve as a device, 0/W2s, O/WIQ 5Q, O/W5
Both Q and IQ must be less than 126 dB.
実施例では媒体の抗磁力の温度係数がセンダストの飽和
磁化のそれ(−0,032%/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/W10−50、O/W50−10がO/W2
5に比べて大きく劣化することはないが、参考例のCo
Crや添加原素の少いものではO/W50−10が劣化
して一26dBを上回ってしまう。In the example, the temperature coefficient of the coercive force of the medium is within the range of ±0.04%/deg (the range indicated by the dotted line in Figure 1) with respect to that of Sendust's saturation magnetization (-0.032%/deg). O/W10-50, O/W50-10 is O/W2
Although it does not deteriorate significantly compared to Co. 5, the reference example Co
If the amount of Cr or additive elements is small, the O/W50-10 deteriorates and exceeds -26 dB.
なお、磁気へラドコアの一部、もしくは全体にCoZr
Nb合金を用いているが、この合金にその他の添加元素
を加えて組成比が変わっても飽和磁化の温度係数が本実
施例に近い範囲(±0.04%/deg)であ(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。In addition, CoZr is applied to a part or the whole of the magnetic herad core.
Although a Nb alloy is used, even if other additive elements are added to this alloy and the composition ratio is changed, the temperature coefficient of saturation magnetization remains within a range close to that of this example (±0.04%/deg) (in accordance with the invention). Effects) 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 small extent.
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箔 1 図
添加量 rat%]
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 foil Figure 1 Addition amount rat%] Figure 2 Figure 3 Figure 4
Claims (3)
びNbを主成分とする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1.9〜3.0at%であることを特徴とする磁気記
録装置。(1) A magnetic head in which the vicinity of the gap or the entire core is made of an alloy whose main components are Co, Zr, and Nb;
1. A magnetic recording device configured with a magnetic storage medium containing Cr and Zr as main components, characterized in that the content of Zr in the magnetic recording medium is 1.9 to 3.0 at%.
びNbを主成分とする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2.1〜3.5at%であることを特徴とする磁気記
録装置。(2) A magnetic head in which the vicinity of the gap or the entire core is made of an alloy whose main components are Co, Zr, and Nb;
1. A magnetic recording device configured with a magnetic recording medium containing Cr and Hf as main components, characterized in that the content of Hf in the magnetic recording medium is 2.1 to 3.5 at%.
びNbを主成分とする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2.1〜3.5at%であることを特徴とする磁気記
録装置。(3) A magnetic head in which the vicinity of the gap or the entire core is made of an alloy whose main components are Co, Zr, and Nb;
1. A magnetic recording device configured with a magnetic recording medium containing Cr and Ta as main components, characterized in that the content of Ta in the magnetic recording medium is 2.1 to 3.5 at%.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9225987A JPH0619804B2 (en) | 1987-04-14 | 1987-04-14 | Magnetic recording device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9225987A JPH0619804B2 (en) | 1987-04-14 | 1987-04-14 | Magnetic recording device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63257901A true JPS63257901A (en) | 1988-10-25 |
JPH0619804B2 JPH0619804B2 (en) | 1994-03-16 |
Family
ID=14049412
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9225987A Expired - Lifetime JPH0619804B2 (en) | 1987-04-14 | 1987-04-14 | Magnetic recording device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0619804B2 (en) |
-
1987
- 1987-04-14 JP JP9225987A patent/JPH0619804B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH0619804B2 (en) | 1994-03-16 |
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