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JPS59194406A - High permeability magnetic material - Google Patents

High permeability magnetic material

Info

Publication number
JPS59194406A
JPS59194406A JP58068709A JP6870983A JPS59194406A JP S59194406 A JPS59194406 A JP S59194406A JP 58068709 A JP58068709 A JP 58068709A JP 6870983 A JP6870983 A JP 6870983A JP S59194406 A JPS59194406 A JP S59194406A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic material
fe2o3
mno
high permeability
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
JP58068709A
Other languages
Japanese (ja)
Inventor
Kazuhiko Okita
和彦 沖田
Junichi Horikawa
順一 堀川
Toshiharu Hoshi
星 敏春
Haruo Saji
佐治 晴夫
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP58068709A priority Critical patent/JPS59194406A/en
Publication of JPS59194406A publication Critical patent/JPS59194406A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/34Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials non-metallic substances, e.g. ferrites
    • H01F1/342Oxides
    • H01F1/344Ferrites, e.g. having a cubic spinel structure (X2+O)(Y23+O3), e.g. magnetite Fe3O4

Landscapes

  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Magnetic Ceramics (AREA)
  • Soft Magnetic Materials (AREA)

Abstract

PURPOSE:To obtain magnetic material which has little temperature dependence and high permeability at the practical temperature range by doping the magnetic material containing Fe2O3, MnO and ZnO with CoO. CONSTITUTION:When the content of Fe2O3 is 53-54mol%, the composition of MnO and ZnO is selected in such a manner that the point at which K1 (the primary crystal magnetic unisotropy constant) +K2 (the secondary crystal magnetic unisotropy constant)/9=0 is to be, for instance -30 deg.C-30 deg.C. These raw materials are doped with 0.5-2.0mol of CoO and mixed so that the absolute values of K1 and K2 at the room temperature may be reduced and the point at which K1+K2/9=0 may be below zero. With this constitution, the magnetic material which has very little temperature dependence and the high permeability at the practical temperature range can be obtained and, if this material is introduced to make a magnetic head, that head can have very little variation of the permeability and the stable high output during the operation.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、映像信号の記録、再生用ヘッド等に用いられ
る高透磁率磁性制別に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a high magnetic permeability magnetic disc used in a head for recording and reproducing video signals.

従来例の構成とその問題点 従来、映像信号用の記録、再生用ヘッドの素材としては
、主としてMn −Zn系単結晶フェライトが用いられ
ている。それは磁気ヘッドとして一般的に要求される特
性、即ち透磁率μが太さいこと。
Conventional Structure and Problems Conventionally, Mn--Zn single-crystal ferrite has been mainly used as a material for recording and reproducing heads for video signals. This is a characteristic generally required for magnetic heads, that is, a large magnetic permeability μ.

飽和磁束密度Bs が犬さいこと、抗磁力Hcが小さい
こと、キュリ一温度Tc が高いこと、それに加えて精
密加工に耐え、耐摩耗性に優れていること、およびヘッ
ド化した時の摺動ノイズ領域が使用帯域外にあることな
どにおいてMn −Zn系単結晶フェライト(ri満足
すべき特性をイtiiiえていることによるものである
つところで、Mn −Zn系単結晶フェライトの透磁率
μは、それらの成分である酸化第二鉄Fe2O3,酸化
亜鉛ZnO、酸化マンガンMnOの各々の余有量及び温
度に犬きく左右される。結晶磁気異方性定数全に1飽和
磁化をIs  とするとμ” 工s / IKIの関係
から透磁率71は結晶磁気異方性定数にと逆比例の関係
にありKが温度依存性を持っているため、μも大きな温
度依存性を持っている。K−=Qになる組成の近傍でμ
が最大を示すが、KyOの点はその素材の組成により室
温付近になったり、低温付近になったりする。
The saturation magnetic flux density Bs is small, the coercive force Hc is small, the Curie temperature Tc is high, and in addition, it has to withstand precision machining, has excellent wear resistance, and has low sliding noise when made into a head. This is due to the fact that the Mn-Zn single-crystal ferrite (RI) satisfies the characteristics of the Mn-Zn single-crystal ferrite in that the area is outside the usage band. It is strongly influenced by the remaining amount and temperature of each of the components of ferric oxide Fe2O3, zinc oxide ZnO, and manganese oxide MnO.If Is is 1 saturation magnetization for the crystal magnetic anisotropy constant, then μ'' From the relationship of s/IKI, the magnetic permeability 71 is inversely proportional to the magnetocrystalline anisotropy constant, and since K has a temperature dependence, μ also has a large temperature dependence.K-=Q In the vicinity of the composition where μ
shows the maximum, but the KyO point may be near room temperature or near low temperature depending on the composition of the material.

しかしながら、従来は、透磁率金入きくする1]的でに
=Qの点が室温付近で実現されるように素材の組51選
んでいた。一般に一次の結晶磁気異方性定数e K+ 
*二次の結晶磁気異方性定数ヲに2とすると、結晶磁気
異方性定数はにミに1+δに2と定義される。ここで、
δは結晶の構造と方位に関する定数で立方晶構造の場合
、理論的に透磁率に対して回転4iB化機構が支配的な
場合にδ−1/9と[〜、K、+に2/9=Oで透磁率
が最大上なることがわかっている。又に+ + K2 
/9 > oで容易磁化方向が< 100 >、K1+
に2/9(Oて容易磁化方向が〈111〉となろう従っ
て、K、−1−に2/9二〇の点を室温付近に実現させ
た場合、磁気ヘッドの透磁率は、テープの摺動による温
度変化により、容易磁化方向かく100>全面いたり、
<111>全面いたり(−て極めて不安定な値となり、
その結果使用直後とある程度時間がたってからでは出力
にかなりの差がでてし1つ。
However, in the past, the set of materials 51 was selected so that the point =Q, where the magnetic permeability was determined, was achieved near room temperature. In general, the first-order magnetocrystalline anisotropy constant e K+
*If the second-order magnetocrystalline anisotropy constant is 2, then the magnetocrystalline anisotropy constant is defined as 1 + δ = 2. here,
δ is a constant related to the structure and orientation of the crystal. In the case of a cubic crystal structure, theoretically when the rotational 4iB mechanism is dominant for magnetic permeability, δ-1/9 and [~, K, +2/9 It is known that the magnetic permeability is maximized when =O. Also + + K2
/9 > o, easy magnetization direction < 100 >, K1+
The easy magnetization direction will be <111> at 2/9 (O). Therefore, if the point 2/920 at K, -1- is realized near room temperature, the magnetic permeability of the magnetic head will be the same as that of the tape. Due to temperature changes due to sliding, the direction of magnetization is easily changed from 100 to the entire surface,
<111>The entire surface is present (-, resulting in an extremely unstable value,
As a result, there is a considerable difference in output between immediately after use and after a certain amount of time.

発明の目的 本発明は、以」−のような従来の問題点を解決j〜磁気
ヘッドの実用温度範囲内で極めて温度依存性の少く、且
つ太さな値の透磁率をもった磁気ヘッド用素材としての
高透磁率磁性材料を提供することを目的とするものであ
る。
Purpose of the Invention The present invention solves the following conventional problems. The purpose is to provide a high permeability magnetic material as a raw material.

発明の構成 この目的全達成するために本発明は、K1−1−に2/
9−〇となる点が、例えば−30’C〜30゛0になる
よつに、MnO、ZnO、Fe2C)5 rTr組成ヲ
I穴び、才だこれらの索胴に添加物金沢ぜることにより
、室温におけるに、、x2の値合手さく(−1又に1−
)K2/9−0となる点を0℃以下にし、実用温度範囲
におけるイ臓気ヘッドの透磁率の温度依イf律l:全極
めて小さくした高透磁率磁性A/1月ω提供するもので
ある。
Structure of the Invention In order to achieve all of these objects, the present invention provides K1-1-2/
When the point 9-0 becomes, for example, -30'C to 30'0, the MnO, ZnO, Fe2C)5 rTr composition is drilled and the additive is added to the cable trunk. Therefore, at room temperature, the value of x2 (-1 or 1-
) The temperature dependence of the magnetic permeability of the magnetic head in the practical temperature range by setting the point at which K2/9-0 is below 0°C, and the temperature dependence of the magnetic permeability of the magnetic head in the practical temperature range. It is.

実施例の説明 以下に本発明の実施例を図面を用いて説明する。Description of examples Embodiments of the present invention will be described below with reference to the drawings.

第1図(d MnOが29mo1%、 ZnOが17 
mo1%。
Figure 1 (d MnO: 29 mo1%, ZnO: 17 mo
mo1%.

Fe2O3がs 4 mo1%の組成におけるに1.に
2の温度依存性の測定結果であり、図中1 (d K+
 、 2 fdK2の測定結果であり、aばに、+に2
/9 =oとなる点である。組成ケ変えることによりa
の点を左右に移動させることができるが、この組成にお
いては約−16℃に位置(〜でいる。この組成に添加物
とじてCoo ? 1mo1%程度添加すると、すなわ
ちMnOが28.6 mo1%、 ZnOが16.5 
mo1%、 Co。
1 in a composition with Fe2O3 of s 4 mo1%. In the figure, 1 (d K+
, 2 is the measurement result of fdK2, and abani, +2
/9 = o. By changing the composition a
The point can be moved to the left or right, but in this composition it is located at about -16°C.If about 1% of Coo as an additive is added to this composition, that is, MnO is 28.6% by mo1. , ZnO is 16.5
mo1%, Co.

が1 mo1% 、Fe2O3が64mo1%の組成で
、K、、 K2の温度依存性を測定すると第2図のよう
になる。
When the temperature dependence of K, K2 is measured with a composition of 1 mo1% of Fe2O3 and 64 mo1% of Fe2O3, the results are shown in Figure 2.

この組l戎におけるに、+に2/9−○となる点に約−
30℃に位置(〜ている。つ丑りCoOを少量添加する
ことにより、K、+に2/9=Oと々る点孕移動させる
ことができる。壕だ一方において実用温度範囲、i&l
l LばO’C〜100’Cにおけるに、、に2/7)
絶対値を小さくすることがでさるのでその結果、透磁率
(5kUl+ ) 9CoO添加前/7)620から1
740と太さぐすることができる。寸だ、Cooの添加
量を0.5 mo1%〜2.0mol係変化させても同
様に実用温度範囲において透磁率を大さくすることがで
さた。しか(−120!+101係以上になると透磁率
は減少の傾向を示[〜だ。従ってCooの添加量として
0.6mo1%〜2.□ mo1%が適当と思われる0
第二の実施例としてに1+に2/9;Oとなる点が一3
0′C〜3Q′Cにある、Fe2O3が53〜ssmo
1%、ZnOが14〜24 mo1% 、’MnOが2
1〜33m01%の組成にGoo f少量添加(Fe2
O3が63〜55mo1%、Cooが0.5〜2.0 
mo1% 、残りがMnOとznO)することによって
も、第一の実施例同様にK 、 −)−K 2/9=0
となる点をO′C以下にするOとかでさ、徒だ室温にお
けるに、、に2の絶対値を小さくでさることを確認する
ことがでさた。しか(、Fe2O3が53mol係以下
になるとCooの添加量が2.Omol係以上でないと
に1+に2/9 =O,l!:なる点が0℃以下になら
ず、従って、Cooの添加量が多すきるため透磁率の低
下の傾向が現れた。またFe2O3か55 mol係り
、上になると室温におけるに1.に2の絶対値が太さい
ため、000を0.6〜2゜Omo1%添加しても多少
の透磁率の向」二は見られるものの使用に耐えつるよつ
な太ささ寸でには至らなかった。従ってF+、703が
63〜55m01%、C00が0.6−2.○mo1%
 、残ジがMnOとZnO(n組成が高透磁率JAf1
:材料として最も適していると思わ汎る。
In this set l, the point where + is 2/9-○ is about -
By adding a small amount of Tsukushi CoO, it is possible to move K, + to 2/9=O.
2/7)
As a result, the magnetic permeability (5kUl+) 9Before adding CoO/7) can be reduced from 620 to 1 because the absolute value can be reduced.
It can be made as thick as 740. Even if the amount of Coo added was changed by 0.5 mol% to 2.0 mol, it was possible to similarly increase the magnetic permeability in the practical temperature range. However, when it becomes -120!+101 coefficient or higher, the magnetic permeability shows a tendency to decrease [~.Therefore, the appropriate amount of Coo to be added is 0.6 mo1% to 2.□ mo1%0
As a second example, the point where 1+ becomes 2/9; O is 13.
Fe2O3 in 0'C~3Q'C is 53~ssmo
1%, ZnO 14-24 mo1%, 'MnO 2
A small amount of Goof is added to the composition of 1-33m01% (Fe2
O3 is 63-55 mo1%, Coo is 0.5-2.0
mo1%, the rest being MnO and znO), K, -)-K2/9=0 as in the first embodiment.
By making the point below O'C, we were able to confirm that the absolute value of 2 at room temperature can be made small. However, if Fe2O3 is below 53 mol, the amount of Coo added must be 2. There was a tendency for the magnetic permeability to decrease due to the large amount of Fe2O3.Also, as Fe2O3 is 55 mol, the absolute value of 1 and 2 at room temperature is large, so 000 is 0.6~2゜Omo1%. Although some degree of magnetic permeability was observed even when added, it did not reach a size that was strong enough to withstand use.Therefore, F+, 703 was 63-55m01%, and C00 was 0.6-2. .○mo1%
, the residue is MnO and ZnO (n composition is high permeability JAf1
: I think it is the most suitable material.

発明の詳細 な説明1〜たよりに本発明は、少量の添加物を加え、、
 Kj+に2/9 =Oとなる点をO°0以下にし、な
お且つに、、に2の絶対値合手さくすることによ(9、
実用温度範囲で、極めて温度依存性が少く、且つ高い透
jjB率を治した高透磁率磁性材料を得るものであジ、
本発明の材料を用いて、磁気ヘッドを作製(〜だ場合、
使用中における透磁率の変化の少い、安定(〜た品出力
を得る磁気ヘッドの作製が可能であるため、長時間録画
再生用VTRや苛酷な条件下で使用されろKNG用VT
R用ヘッドどして使用さn、その工業的価値は多大であ
る。
Detailed description of the invention
By setting the point where 2/9 = O to Kj+ to be less than O°0, and by increasing the absolute value of 2 to (9,
To obtain a high permeability magnetic material with extremely low temperature dependence and high permeability in a practical temperature range.
A magnetic head is manufactured using the material of the present invention (in the case of...
It is possible to create a magnetic head that produces a stable output with little change in magnetic permeability during use, so it can be used for long-time recording and playback VTRs and KNG VTs that can be used under harsh conditions.
It is used as an R head and has great industrial value.

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

第1図は添加物?含1ない場合のに、 +  K2の温
度依存性の測定結果牙示す図、第2図はCoo f少量
添加1〜たとさのに、、に2の温度依存性の測定結果を
示す図である。 代理人の氏名 カリ111士 中 尾 敏 男 ほか1
名手続補正書 昭和58年1り月//口 昭和58年特許願第68709号 2発明の名称 高透磁率磁性材料 3補正をする者 211イ・1との関係      特   許   出
願人住 所  大阪府門真市大字門真1006番地名 
称 (582)松下電器産業株式会社代表′1ゴ   
    山   下   俊   彦4代理人 〒57
1 住 所  大阪府門真市太字門真1006番地松下電器
産業株式会社内 明細書の開明の計測な欣り一−5al’l、14  。 6、補正の内容 (1)明細書第4ページ第19行目の「−16℃」を「
−18℃」に補正し丑す〇 (2)同第5ページ第11行目の1できる。」を「でき
プこ。」に補正します。
Is Figure 1 an additive? Figure 2 shows the measurement results of the temperature dependence of +K2 in the case of no addition of Coof. . Name of agent: Cali 111 Toshio Nakao and 1 other person
Name Procedural Amendment Document January 1980 // Mouth Patent Application No. 68709 of 1982 2 Name of the Invention High Permeability Magnetic Material 3 Person Making the Amendment 211 A.1 Relationship Patent Applicant Address Osaka Prefecture Kadoma City Oaza Kadoma 1006 address name
(582) Matsushita Electric Industrial Co., Ltd. Representative '1go
Toshihiko Yamashita 4th agent 〒57
1 Address: Matsushita Electric Industrial Co., Ltd., 1006 Kadoma, Kadoma City, Osaka Prefecture, 14. 6. Contents of amendment (1) “-16°C” on page 4, line 19 of the specification was changed to “
-18℃" (2) 1, page 5, line 11. " is corrected to "dekipuko."

Claims (2)

【特許請求の範囲】[Claims] (1)酸化第二鉄Fe2O3,酸化マンガンMnO、酸
化亜鉛ZnOf少なくとも含み、さらに酸化コバルトC
00全0.5〜2.0mo1%添加したこと全特徴とす
る高透磁率磁性材料。
(1) Contains at least ferric oxide Fe2O3, manganese oxide MnO, zinc oxide ZnOf, and further contains cobalt oxide C
A high permeability magnetic material characterized by the addition of 0.5 to 2.0 mo1%.
(2)酸化第二鉄Fe2O3の含有率が53〜5smo
1%であること全特徴とする特許請求の範囲第1項記載
の高透磁率磁性制別。
(2) The content of ferric oxide Fe2O3 is 53-5smo
1%. A high magnetic permeability magnetic separator according to claim 1, which is characterized in that it is 1%.
JP58068709A 1983-04-18 1983-04-18 High permeability magnetic material Pending JPS59194406A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58068709A JPS59194406A (en) 1983-04-18 1983-04-18 High permeability magnetic material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58068709A JPS59194406A (en) 1983-04-18 1983-04-18 High permeability magnetic material

Publications (1)

Publication Number Publication Date
JPS59194406A true JPS59194406A (en) 1984-11-05

Family

ID=13381574

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58068709A Pending JPS59194406A (en) 1983-04-18 1983-04-18 High permeability magnetic material

Country Status (1)

Country Link
JP (1) JPS59194406A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6265969A (en) * 1985-09-17 1987-03-25 日立フェライト株式会社 Mn-zn-co type ferrite

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS524753A (en) * 1975-06-30 1977-01-14 Fujitsu Ltd Mic circulator
JPS5410995A (en) * 1977-06-27 1979-01-26 Citizen Watch Co Ltd Manufacture of pattern transparent conductive membrane
JPS5512099A (en) * 1978-07-07 1980-01-28 Volvo Ab Packing container and method and device for making said container
JPS5633681A (en) * 1979-08-28 1981-04-04 Fujitsu Ltd Vacuum deposition mask
JPS5658209A (en) * 1979-10-17 1981-05-21 Iwaki Denshi Kk Ferrite memory core for direct driving of ttl-ic
JPS5665980A (en) * 1979-11-05 1981-06-04 Hitachi Ltd Vacuum deposition device
JPS5770273A (en) * 1980-10-16 1982-04-30 Matsushita Electric Ind Co Ltd Method for fixing mask for vapor deposition

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS524753A (en) * 1975-06-30 1977-01-14 Fujitsu Ltd Mic circulator
JPS5410995A (en) * 1977-06-27 1979-01-26 Citizen Watch Co Ltd Manufacture of pattern transparent conductive membrane
JPS5512099A (en) * 1978-07-07 1980-01-28 Volvo Ab Packing container and method and device for making said container
JPS5633681A (en) * 1979-08-28 1981-04-04 Fujitsu Ltd Vacuum deposition mask
JPS5658209A (en) * 1979-10-17 1981-05-21 Iwaki Denshi Kk Ferrite memory core for direct driving of ttl-ic
JPS5665980A (en) * 1979-11-05 1981-06-04 Hitachi Ltd Vacuum deposition device
JPS5770273A (en) * 1980-10-16 1982-04-30 Matsushita Electric Ind Co Ltd Method for fixing mask for vapor deposition

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6265969A (en) * 1985-09-17 1987-03-25 日立フェライト株式会社 Mn-zn-co type ferrite
JPH0433755B2 (en) * 1985-09-17 1992-06-03 Hitachi Ferrite Ltd

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