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JPS6239227B2 - - Google Patents
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JPS6239227B2 - - Google Patents

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Publication number
JPS6239227B2
JPS6239227B2 JP57065505A JP6550582A JPS6239227B2 JP S6239227 B2 JPS6239227 B2 JP S6239227B2 JP 57065505 A JP57065505 A JP 57065505A JP 6550582 A JP6550582 A JP 6550582A JP S6239227 B2 JPS6239227 B2 JP S6239227B2
Authority
JP
Japan
Prior art keywords
amorphous alloy
magnetostriction
atomic
alloy
iron
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
JP57065505A
Other languages
Japanese (ja)
Other versions
JPS58185753A (en
Inventor
Koichiro Inomata
Hiroshi Tateishi
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 JP6550582A priority Critical patent/JPS58185753A/en
Publication of JPS58185753A publication Critical patent/JPS58185753A/en
Publication of JPS6239227B2 publication Critical patent/JPS6239227B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の技術分野〕 本発明は、新規な磁気ヘツド用鉄基非晶質合金
に関し、更に詳しくは、高磁束密度、低磁歪及び
高耐摩耗性を有する磁気ヘツド用鉄基非晶質合金
に関する。 〔発明の技術的背景とその問題点〕 従来、磁気ヘツドに用いられる高透磁率材料と
しては、結晶構造を有するFe―Ni合金(パーマ
ロイ)、Fe―Si―Al合金(センダスト)等があつ
た。 しかし、Fe―Ni合金は、透磁率は高いが、耐
摩耗性に劣り、Fe―Si―Al合金は、耐摩耗性は
優れるが、脆弱であるため、塑性加工が非常に困
難であるという欠点を有していた。 ところが、最近になり、結晶構造を持たない非
晶質合金において、優れた磁気的及び機械的特性
が見出された。特に、CoとFeの原子比が94:6
付近のコバルト基非晶質合金は、磁歪が零付近に
なり、透磁率が高いため、磁気ヘツド用材料とし
て注目されている。 しかし、上記コバルト基非晶質合金は、一般
に、飽和磁束密度が9KG以下と低いものであつ
た。9KG以上のコバルト基非晶質合金を製造する
ことは可能であるが、この場合には、キユリー点
(Tc)が結晶化温度(Tx)よりも高くなり、そ
の結果、高透磁率とするためには、回転磁場中で
の熱処理等、特殊な処理を要するという煩雑さが
あつた。また、コバルト基であるために高価とな
り、更には耐摩耗性に劣るという欠点もあつた。 一方、鉄基非晶質合金としては、Ruのみを添
加してなる合金(特開昭54−43118号明細書)等
が知られているが、この合金では、磁歪について
は考慮されていない。一般に、鉄基非晶質合金は
安価で、かつ、高磁束密度であるという利点を有
する反面、磁歪が大きく(低透磁率)、また、磁
気ヘツド製造工程中の樹脂モールドによる磁気特
性劣下が著しい等の問題があるため、磁気ヘツド
材料としてはほとんど注目されていない。 そのため、安価で、かつ磁気ヘツド用として優
れた諸特性を有する非晶質合金の開発が当業界に
おいて要望されていた。 〔発明の目的〕 本発明の目的は、安価な鉄基非晶質合金からな
り、しかも、高磁束密度を有し、かつ、特殊な熱
処理を必要とせずに高透磁率を有し、更には、耐
摩耗性にも優れた磁気ヘツド用材料を提供するこ
とにある。 〔発明の概要〕 本発明者らは、鉄基非晶質合金において、Ru
に加えてTi、Hf、V、Nb、Ta、Cr、Mo又はW
を添加することにより、該合金は、著しく磁歪が
低下し、その結果、高透磁率になると共に耐摩耗
性も優れたものとなることを見出し、本発明を完
成するに至つた。 本発明は、次式: (Fe1-a-bRuaMb100-cc [式中、MはTi、Hf、V、Nb、Ta、Cr、Mo、W
の群から選ばれる少くとも1種の元素を表わし;
XはBを表わし;a、b、cはそれぞれ0.01≦a
≦0.2、0.02≦b≦0.1、10≦c≦18の関係を満足
する数を表わす。]で示される磁気ヘツド用鉄基
非晶質合金及び次式: (Fe1-a-bRuaMb100-cc [式中、MはTi、Hf、V、Nb、Ta、Cr、Mo、W
の群から選ばれる少くとも1種の元素を表わし;
XはBとSi[Bは10原子%以上であり、Siは7原
子%以下(但し、0原子%は含まない)である]
を表わし;a、b、cはそれぞれ0.01≦a≦
0.2、0.02≦b≦0.1、10≦c≦18の関係を満足す
る数を表わす。]で示される磁気ヘツド用鉄基非
晶質合金に関する。 本発明の非晶質合金において、Ruは、鉄基非
晶質合金の耐摩耗性を向上させ、かつ、磁歪を低
下させるのに有効な元素で、その包含される量:
aは原子%で表示して、0.01≦a≦0.2の範囲に
設定される。aが0.01未満の場合には、耐摩耗性
の向上が顕著でなく、0.2を超えると飽和磁束密
度の低下が著しい。 また、M(Ti、Hf、V、Nb、Ta、Cr、Mo、
W)は、鉄基非晶質合金の磁歪を低下させるのに
必須な成分で、その包含される量:bは原子%で
表示して、0.02≦b≦0.1の範囲に設定される。
bが0.02未満の場合には、磁歪の低下が顕著でな
く、0.1を超えると飽和磁束密度の低下が著しい
ため、好ましくない。元素Mとしては、特に
Nb,Taが有効である。 X(BBとSi)は鉄基合金の非晶質化に有効な
元素で、その包含される量:cは原子%で表示し
て、10≦c≦18の範囲に設定される。cが10未満
の場合には、合金の非晶質化が困難となり、18を
超えると磁歪の低下が顕著でなくなる。なお、X
がBとSiである非晶質合金においては、BとSiの
割合は、Bが10原子%以上であり、Siが7原子%
以下(但し、0原子%は含まない)である。 ここでSiは、非晶質合金の製造を容易にするの
に有効な原素であるが、磁歪を増大させるという
欠点があるため、その包含される量は7原子%以
下(但し、0原子%は含まない)である。非晶質
合金製造の容易化及び磁歪の低減のためのは、
0.01原子%以上0.1原子%未満であることが好ま
しい。 本発明の非晶質合金は、前記した各成分を所定
の割合で混合した後、溶融し、これを例えば、液
体(溶湯)急冷法等によつて非晶質合金化し、必
要に応じて熱処理を施すことにより、容易に製造
される。 〔発明の実施例〕 実施例 1 (Fe0.95-bRu0.05Nbb85Si3B12で示される組成の
非晶質合金を、単ロール法により製造した。即
ち、上記組成に混合した合金を溶融し、ついで、
該溶融合金を、高速回転する単ロール表面上に、
石英管ノズルからアルゴンガス圧(1.0〜2.0Kg/
cm2)で噴出させ、得られた薄帯を急冷して幅10
mm、板厚約20μmの長尺テープ状の薄帯とした。
次に、該薄帯を長さ20mmに切取り、これを試料と
した。 以上の試料につき、ストレインゲージ法により
飽和磁歪を測定した。結果を、組成比bとの関係
曲線として第1図に示した。 図より、Nbの組成比が増大するとともに磁歪
が著しく低下し、特にbが0.02以上の場合、磁歪
定数が10×10-6以下となることが判明した。 更に、Nbに代えて、Ti、Hf、V、Ta、Cr、
Mo、Wを添加した前記組成の非晶質合金につい
て、同様の測定を行なつた結果、Nbの場合と類
似の挙動を示した。 実施例 2 (Fe0.90Ru0.05Nb0.05)zSi88-zB12で示される組
成の非晶質合金を、実施例1と同様に単ロール法
により製造し、飽和磁歪を測定した。結果を組成
比zとの関係曲線Aとして第2図に示した。 図より、zの増大とともに磁歪が著しく低下
し、zが、82以上の場合には磁歪定数が10×10-6
以下になることが判明した。 また、Ru、Nbを含有しないFezSi90-zB10で示
される組成の非晶質合金についても、同様の測定
を行いその結果を、組成比zとの関係曲線Bとし
て第2図に合わせて示した。 これらの結果より、磁歪低下に対するRu、Nb
の添加効果は顕著であることが判明した。 実施例 3 表に示した非晶質合金を、実施例1と同様に単
ロール法を用いて幅10mm、板厚約20μmの長尺テ
ープ状の薄帯とした。この薄帯を長さ1mに切取
り、これをトロイダル状に巻回した後、キユリー
点以上結晶化温度以下の温度域で熱処理を施し、
試料とした。尚、回転磁場処理は施さなかつた。 この試料について、マツクスウエルブリツジを
用いて1〜100KHzにおける実効透磁率を測定
し、また試料振動型磁力計を用いて飽和磁束密度
を測定するとともに実施例1と同様に飽和磁歪も
測定した。1KHzにおける実効透磁率(〓′1K)、
飽和磁歪及び飽和磁束密度の値を表に示した。 比較例として、Ru並びにM元素を含まない非
晶質合金、M元素を含まない非晶質合金について
も表に合わせて示した。
[Technical Field of the Invention] The present invention relates to a novel iron-based amorphous alloy for magnetic heads, and more particularly to an iron-based amorphous alloy for magnetic heads having high magnetic flux density, low magnetostriction, and high wear resistance. . [Technical background of the invention and its problems] Conventionally, high magnetic permeability materials used in magnetic heads include Fe--Ni alloy (permalloy) and Fe--Si--Al alloy (sendust), which have a crystal structure. . However, the Fe-Ni alloy has high magnetic permeability but poor wear resistance, and the Fe-Si-Al alloy has excellent wear resistance but is brittle, making plastic working very difficult. It had However, recently, excellent magnetic and mechanical properties have been discovered in amorphous alloys that do not have a crystalline structure. In particular, the atomic ratio of Co and Fe is 94:6.
Nearby cobalt-based amorphous alloys have magnetostriction near zero and high magnetic permeability, so they are attracting attention as materials for magnetic heads. However, the cobalt-based amorphous alloys generally have a low saturation magnetic flux density of 9 KG or less. Although it is possible to produce cobalt-based amorphous alloys of 9KG or more, in this case the Kyrie point (Tc) will be higher than the crystallization temperature (Tx), resulting in high magnetic permeability. This method is complicated in that it requires special treatments such as heat treatment in a rotating magnetic field. Furthermore, since it is based on cobalt, it is expensive and has the disadvantage of poor wear resistance. On the other hand, as an iron-based amorphous alloy, an alloy in which only Ru is added (Japanese Unexamined Patent Publication No. 43118/1983) is known, but magnetostriction is not taken into account in this alloy. In general, iron-based amorphous alloys have the advantages of being inexpensive and having high magnetic flux density, but on the other hand, they have large magnetostriction (low magnetic permeability) and are susceptible to deterioration of magnetic properties due to resin molding during the magnetic head manufacturing process. Due to serious problems, it has received little attention as a magnetic head material. Therefore, there has been a demand in the art for the development of an amorphous alloy that is inexpensive and has excellent properties for use in magnetic heads. [Objective of the Invention] The object of the present invention is to make an inexpensive iron-based amorphous alloy, which has high magnetic flux density, high magnetic permeability without the need for special heat treatment, and The object of the present invention is to provide a material for a magnetic head that also has excellent wear resistance. [Summary of the Invention] The present inventors have discovered that in an iron-based amorphous alloy, Ru
In addition to Ti, Hf, V, Nb, Ta, Cr, Mo or W
It has been discovered that by adding , the magnetostriction of the alloy is significantly reduced, resulting in high magnetic permeability and excellent wear resistance, and the present invention has been completed. The present invention is based on the following formula: (Fe 1-ab Ru a M b ) 100-c X c [wherein M is Ti, Hf, V, Nb, Ta, Cr, Mo, W
represents at least one element selected from the group;
X represents B; a, b, and c are each 0.01≦a
Represents a number that satisfies the following relationships: ≦0.2, 0.02≦b≦0.1, and 10≦c≦18. ] and the following formula: (Fe 1-ab Ru a M b ) 100-c X c [wherein M is Ti, Hf, V, Nb, Ta, Cr, Mo, W.
represents at least one element selected from the group;
X is B and Si [B is 10 atomic % or more, Si is 7 atomic % or less (however, 0 atomic % is not included)]
represents; a, b, c are each 0.01≦a≦
It represents a number that satisfies the following relationships: 0.2, 0.02≦b≦0.1, and 10≦c≦18. ] This invention relates to an iron-based amorphous alloy for magnetic heads. In the amorphous alloy of the present invention, Ru is an element effective in improving the wear resistance of the iron-based amorphous alloy and reducing magnetostriction, and the amount included:
a is expressed in atomic % and is set in the range of 0.01≦a≦0.2. When a is less than 0.01, the improvement in wear resistance is not significant, and when it exceeds 0.2, the saturation magnetic flux density is significantly reduced. Also, M(Ti, Hf, V, Nb, Ta, Cr, Mo,
W) is an essential component for lowering the magnetostriction of the iron-based amorphous alloy, and its included amount: b is expressed in atomic % and is set in the range of 0.02≦b≦0.1.
If b is less than 0.02, the decrease in magnetostriction is not significant, and if b exceeds 0.1, the saturation magnetic flux density is significantly decreased, which is not preferable. As element M, especially
Nb and Ta are effective. X (BB and Si) is an element effective in making the iron-based alloy amorphous, and its contained amount: c is expressed in atomic % and is set in the range of 10≦c≦18. If c is less than 10, it will be difficult to make the alloy amorphous, and if c is more than 18, the magnetostriction will not decrease significantly. In addition, X
In an amorphous alloy in which B and Si are B and Si, the ratio of B and Si is 10 at% or more for B and 7 at% for Si.
The following (however, 0 atomic % is not included): Here, Si is an effective element for facilitating the production of amorphous alloys, but it has the drawback of increasing magnetostriction, so the amount included is less than 7 atomic percent (however, 0 atomic percent). % is not included). To facilitate the production of amorphous alloys and reduce magnetostriction,
It is preferably 0.01 atomic % or more and less than 0.1 atomic %. The amorphous alloy of the present invention is produced by mixing the above-mentioned components in a predetermined ratio, melting the mixture, turning the mixture into an amorphous alloy by, for example, a liquid (molten metal) quenching method, and heat-treating as necessary. It can be easily manufactured by applying [Examples of the Invention] Example 1 (Fe 0 . 95-b Ru 0 . 05 Nb b ) An amorphous alloy having the composition shown by 85 Si 3 B 12 was manufactured by a single roll method. That is, the alloy mixed with the above composition is melted, and then,
The molten alloy is placed on the surface of a single roll rotating at high speed,
Argon gas pressure (1.0~2.0Kg/
cm 2 ), and the resulting ribbon was quenched to a width of 10
It was made into a long tape-like thin strip with a thickness of about 20 μm and a plate thickness of about 20 μm.
Next, the ribbon was cut to a length of 20 mm and used as a sample. The saturation magnetostriction of the above samples was measured by the strain gauge method. The results are shown in FIG. 1 as a relationship curve with composition ratio b. From the figure, it was found that as the composition ratio of Nb increases, the magnetostriction decreases significantly, and especially when b is 0.02 or more, the magnetostriction constant becomes 10×10 −6 or less. Furthermore, in place of Nb, Ti, Hf, V, Ta, Cr,
Similar measurements were performed on an amorphous alloy with the above composition to which Mo and W were added, and the result showed behavior similar to that of Nb. Example 2 An amorphous alloy having the composition shown by (Fe 0 . 90 Ru 0 . 05 Nb 0 . It was measured. The results are shown in FIG. 2 as a relationship curve A with the composition ratio z. From the figure, the magnetostriction decreases significantly as z increases, and when z is 82 or more, the magnetostriction constant becomes 10×10 -6
It turned out to be the following. In addition, similar measurements were made for an amorphous alloy with the composition shown by FezSi 90-z B 10 that does not contain Ru or Nb, and the results are plotted as relationship curve B with the composition ratio z according to Figure 2. Indicated. From these results, it is clear that Ru, Nb and
The effect of the addition of was found to be significant. Example 3 The amorphous alloy shown in the table was made into a long tape-like thin strip having a width of 10 mm and a plate thickness of about 20 μm using the single roll method in the same manner as in Example 1. This thin strip was cut to a length of 1 m, wound into a toroidal shape, and then heat treated in a temperature range above the Curie point and below the crystallization temperature.
It was used as a sample. Note that no rotating magnetic field treatment was performed. Regarding this sample, the effective magnetic permeability at 1 to 100 KHz was measured using a Maxwell bridge, the saturation magnetic flux density was measured using a sample vibrating magnetometer, and the saturation magnetostriction was also measured in the same manner as in Example 1. Effective magnetic permeability at 1KHz (〓′1K),
The values of saturation magnetostriction and saturation magnetic flux density are shown in the table. As comparative examples, amorphous alloys that do not contain Ru or M elements, and amorphous alloys that do not contain M elements are also shown in the table.

【表】【table】

【表】 これらの結果より、本発明の非晶質合金は、磁
歪が小さいため、実効透磁率が大きいことが判明
した。 実施例 4 実施例3で得られた薄帯から、オーデイオ用磁
気ヘツド形状を打抜き、磁気ヘツドを試作して、
それらの耐摩耗性を評価した。評価は、γ―
Fe2O3塗布の市販オーデイオ用カセツトテープを
速度4.7cm/secで100時間走行させた前後におけ
る、磁気ヘツドのテープ摺動面の摩耗量を表面粗
さ計を用いて測定することにより行なつた。摩耗
量を表に合わせて示した。 これらの結果より、本発明の非晶質合金は著し
く耐摩耗性が向上していることが判明した。 〔発明の効果〕 本発明の非晶質合金は、鉄を主体にしているた
め安価であり、また、磁歪が小さいため実効透磁
率が大きい。しかも、特殊な熱処理を必要としな
い。更には、飽和磁束密度が大きく、耐摩耗性に
優れている等の特徴を有するものである。従つ
て、磁気ヘツド用材料として優れた適性を有し、
その工業的価値は極めて大きい。
[Table] From these results, it was found that the amorphous alloy of the present invention has a low magnetostriction and therefore a high effective magnetic permeability. Example 4 The shape of an audio magnetic head was punched out from the ribbon obtained in Example 3, and a magnetic head was prototyped.
Their wear resistance was evaluated. The evaluation is γ-
This was done by measuring the amount of wear on the tape sliding surface of the magnetic head using a surface roughness meter before and after running a commercially available audio cassette tape coated with Fe 2 O 3 at a speed of 4.7 cm/sec for 100 hours. Ta. The amount of wear is also shown in the table. These results revealed that the amorphous alloy of the present invention has significantly improved wear resistance. [Effects of the Invention] The amorphous alloy of the present invention is inexpensive because it is mainly made of iron, and has a high effective magnetic permeability because of its low magnetostriction. Furthermore, no special heat treatment is required. Furthermore, it has characteristics such as a high saturation magnetic flux density and excellent wear resistance. Therefore, it has excellent suitability as a material for magnetic heads.
Its industrial value is extremely large.

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

第1図は、(Fe0.95bRu0.005Nbb85Si3B12で示さ
れる本発明非晶質合金の組成比bと飽和磁歪との
関係曲線を示した図である。第2図は、
(Fe0.90Ru0.05Nb0.05zSi88zB12で示される本発明
非晶質合金の組成比zと飽和磁歪との関係曲線
A、及び、FezSi90-ZB10で示される非晶質合金の
組成比zと飽和磁歪との関係曲線Bである。
FIG. 1 is a diagram showing a relationship curve between the composition ratio b and saturation magnetostriction of the amorphous alloy of the present invention represented by (Fe 0.95b Ru 0. 005 Nb b85 Si 3 B 12) . Figure 2 is
(Fe 0.90 Ru 0.05 Nb 0.05 ) Relationship curve A between the composition ratio z and saturation magnetostriction of the amorphous alloy of the present invention shown by z Si 88z B 12 and Fe z Si 90− It is a relationship curve B between the composition ratio z of an amorphous alloy represented by Z B 10 and the saturation magnetostriction.

Claims (1)

【特許請求の範囲】 1 次式: (Fe1-a-bRuaMb100-cc [式中、MはTi、Hf、V、Nb、Ta、Cr、Mo、W
の群から選ばれる少くとも1種の元素を表わし;
XはBを表わし;a、b、cはそれぞれ0.01≦a
≦0.2、0.02≦b≦0.1、10≦c≦18の関係を満足
する数を表わす。] で示される磁気ヘツド用鉄基非晶質合金。 2 次式: (Fe1-a-bRuaMb100-cc [式中、MはTi、Hf、V、Nb、Ta、Cr、Mo、W
の群から選ばれる少くとも1種の元素を表わし;
XはBとSi(Bは10原子%以上であり、Siは7原
子%以下(但し、0原子%は含まない)である)
を表わし;a、b、cはそれぞれ0.01≦a≦
0.2、0.02≦b≦0.1、10≦c≦18の関係を満足す
る数を表わす。] で示される磁気ヘツド用鉄基非晶質合金。 3 前記のXで表されるB及びSiのうち、Siが
0.01原子%以上0.1原子%未満である特許請求の
範囲第2項記載の磁気ヘツド用鉄基非晶質合金。
[Claims] Primary formula: (Fe 1-ab Ru a M b ) 100-c X c [wherein M is Ti, Hf, V, Nb, Ta, Cr, Mo, W
represents at least one element selected from the group;
X represents B; a, b, and c are each 0.01≦a
Represents a number that satisfies the following relationships: ≦0.2, 0.02≦b≦0.1, and 10≦c≦18. ] An iron-based amorphous alloy for magnetic heads. Secondary formula: (Fe 1-ab Ru a M b ) 100-c X c [In the formula, M is Ti, Hf, V, Nb, Ta, Cr, Mo, W
represents at least one element selected from the group;
X is B and Si (B is 10 atomic % or more, Si is 7 atomic % or less (however, 0 atomic % is not included))
represents; a, b, c are each 0.01≦a≦
It represents a number that satisfies the following relationships: 0.2, 0.02≦b≦0.1, and 10≦c≦18. ] An iron-based amorphous alloy for magnetic heads. 3 Of B and Si represented by X above, Si is
The iron-based amorphous alloy for a magnetic head according to claim 2, wherein the iron-based amorphous alloy contains 0.01 atomic % or more and less than 0.1 atomic %.
JP6550582A 1982-04-21 1982-04-21 Amorphous iron alloy for magnetic head Granted JPS58185753A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6550582A JPS58185753A (en) 1982-04-21 1982-04-21 Amorphous iron alloy for magnetic head

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Application Number Priority Date Filing Date Title
JP6550582A JPS58185753A (en) 1982-04-21 1982-04-21 Amorphous iron alloy for magnetic head

Publications (2)

Publication Number Publication Date
JPS58185753A JPS58185753A (en) 1983-10-29
JPS6239227B2 true JPS6239227B2 (en) 1987-08-21

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JP6550582A Granted JPS58185753A (en) 1982-04-21 1982-04-21 Amorphous iron alloy for magnetic head

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Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5672153A (en) * 1979-11-14 1981-06-16 Takeshi Masumoto Amorphous iron alloy of high permeability

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JPS58185753A (en) 1983-10-29

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