JPH01235005A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH01235005A JPH01235005A JP6099088A JP6099088A JPH01235005A JP H01235005 A JPH01235005 A JP H01235005A JP 6099088 A JP6099088 A JP 6099088A JP 6099088 A JP6099088 A JP 6099088A JP H01235005 A JPH01235005 A JP H01235005A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- shaped core
- film
- length
- 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
Links
- 238000004804 winding Methods 0.000 claims abstract description 13
- 239000000758 substrate Substances 0.000 claims abstract description 6
- 229910052751 metal Inorganic materials 0.000 claims description 24
- 239000002184 metal Substances 0.000 claims description 24
- 239000010408 film Substances 0.000 claims description 21
- 239000000696 magnetic material Substances 0.000 claims description 7
- 239000010409 thin film Substances 0.000 claims description 5
- 239000011521 glass Substances 0.000 abstract description 6
- 229910000808 amorphous metal alloy Inorganic materials 0.000 abstract description 4
- 229910000702 sendust Inorganic materials 0.000 abstract description 3
- AOWKSNWVBZGMTJ-UHFFFAOYSA-N calcium titanate Chemical compound [Ca+2].[O-][Ti]([O-])=O AOWKSNWVBZGMTJ-UHFFFAOYSA-N 0.000 abstract description 2
- 239000000919 ceramic Substances 0.000 abstract description 2
- 239000007769 metal material Substances 0.000 abstract 2
- 230000015556 catabolic process Effects 0.000 abstract 1
- 238000006731 degradation reaction Methods 0.000 abstract 1
- 230000001747 exhibiting effect Effects 0.000 abstract 1
- 230000007423 decrease Effects 0.000 description 3
- 238000004544 sputter deposition Methods 0.000 description 3
- 229910000859 α-Fe Inorganic materials 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- -1 7...Oxide bow A Substances 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 229910052681 coesite Inorganic materials 0.000 description 1
- 229910052906 cristobalite Inorganic materials 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000009545 invasion Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 230000008929 regeneration Effects 0.000 description 1
- 238000011069 regeneration method Methods 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 229910052682 stishovite Inorganic materials 0.000 description 1
- 229910052905 tridymite Inorganic materials 0.000 description 1
Landscapes
- Magnetic Heads (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は特殊再生機能やテープスピード切り替え機能を
有するVTRに好適な高効率の磁気ヘッドに関するもの
である。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a highly efficient magnetic head suitable for a VTR having a special playback function and a tape speed switching function.
従来の技術
映像の記録再生に用いるVTRは最近では特殊再生機能
を有するものが一般的になり、1台のVTRに搭載され
るビデオヘッドの数も従来の2個から4〜8個に増えて
いる。この場合、シリンダー上のひとつのヘッド窓に2
個のヘッドが配置され、例えば、記録再生兼用ヘッドと
特殊再生用ヘッド、あるいは標準テープ速度用ヘッドと
低テープ速度用ヘッド等の組み合わせが用いられている
。このような場合、2個のヘッドのギャップ間距離は主
に水平同期信号の関係からある間隔に決められる。この
間隔は例えばVH8方式の1例では水平同期信号の間隔
の2倍に相当する距離即ち約0.74mmが用いられる
。従ってビデオヘッドとしては第2図に示す様に、一方
のコアの記録媒体走行方向の長さLが他方のコアに比べ
て短い構成のものになり、巻線のスペースを考慮すると
上記長さしは約0.2mm程度になる。ところで従来V
TR等の高周波信号を記録再生する装置においては、高
周波損失の少ないフェライト材料を用いたヘッドが一般
的であった。フェライトヘッドの場合、磁気ギャップ近
傍を除いてコア幅全体がフェライトで構成されているた
め、上記長さしが短(なっても磁路としてコア幅全体が
使えるため、ヘッド効率の低下はそれほど大きくない。Conventional technology Recently, VTRs used for recording and playing back video have become common, with special playback functions, and the number of video heads installed in one VTR has increased from the traditional two to four to eight. There is. In this case, one head window on the cylinder has two
For example, a combination of a recording/reproducing head and a special reproduction head, or a standard tape speed head and a low tape speed head is used. In such a case, the distance between the gaps between the two heads is determined to be a certain interval mainly based on the relationship between the horizontal synchronizing signals. For example, in one example of the VH8 system, this interval is a distance equivalent to twice the interval of horizontal synchronizing signals, that is, about 0.74 mm. Therefore, as shown in Figure 2, the video head has a configuration in which the length L of one core in the recording medium running direction is shorter than the other core, and considering the space for the winding, the length L is shorter than that of the other core. is approximately 0.2 mm. By the way, conventional V
In devices for recording and reproducing high frequency signals such as TRs, heads using ferrite materials with low high frequency loss have generally been used. In the case of a ferrite head, the entire core width is made of ferrite except for the area near the magnetic gap, so even if the length mentioned above is short, the entire core width can be used as a magnetic path, so the drop in head efficiency is not so large. do not have.
発明が解決しようとする課題
最近はVTRにも高画質が要求され短波長特性を向上さ
せるためにビデオテープの抗磁力を高(する方向にある
。このようなVTRに用いるビデオヘッドとしては高周
波特性に優れ、且つ十分な記録能力を有するものが望ま
れ、第3図に示すような高飽和磁束密度の金属磁性膜1
を非磁性体2で挟持した構造のものが用いられている。Problems to be Solved by the Invention Recently, high image quality is required for VTRs, and there is a trend toward increasing the coercive force of video tapes in order to improve short wavelength characteristics. A metal magnetic film 1 with a high saturation magnetic flux density as shown in Fig. 3 is desired.
A structure in which the magnetic material is sandwiched between non-magnetic materials 2 is used.
しがしこのような構造のヘッドの場合、通常の形状では
非常に高効率の特性を示すが、前述したようなI型コア
の長さLが小さ(なると再生効率が急激に低下すること
がわかった。第4図は第3図に示すヘッドにおいて■型
コアの長さしを変えた時のヘッド出力の変化を示したも
のである。実験に用いたヘッドはI型コアの長さの他は
ほぼ同じ仕様のものであり、相対速度は5.8m/s、
周波数は7MHzである。この図かられかるように第3
図に示す構造のヘッドでは、■型コアの長さしが0.2
mm程度になると急激にヘッド出力が低下する。この低
下の度合いはヘッドのトラック幅が小さくなるほど大き
くなる。However, in the case of a head with such a structure, it exhibits extremely high efficiency characteristics in a normal shape, but if the length L of the I-shaped core is small (as mentioned above), the reproduction efficiency may drop sharply. Okay. Figure 4 shows the change in head output when the length of the ■-type core is changed in the head shown in Figure 3. The head used in the experiment has a length of I-type core. The other specifications are almost the same, the relative speed is 5.8 m/s,
The frequency is 7MHz. As you can see from this figure, the third
In the head with the structure shown in the figure, the length of the ■-shaped core is 0.2
When it becomes about mm, the head output sharply decreases. The degree of this decrease becomes greater as the track width of the head becomes smaller.
課題を解決するための手段
主磁気コアが金属磁性膜を非磁性基板で挟持した構造か
らなり、磁気ギャップをはさんで巻線窓の無い■型コア
の記録媒体走行方向の長さが巻線窓を有するC型コアの
長さより短い構造の磁気ヘッドにおいて、前記■型コア
の巻線窓と反対の端面に金属磁性体が形成された構造と
する。Means for solving the problem The main magnetic core has a structure in which a metal magnetic film is sandwiched between non-magnetic substrates, and the length of the ■-shaped core with no winding window across the magnetic gap in the recording medium running direction is the length of the winding. In a magnetic head having a structure shorter than the length of a C-shaped core having a window, a metal magnetic material is formed on the end face of the ■-shaped core opposite to the winding window.
作用
上述の構成により、I型コアの長さLが短(でも端部に
形成された金属磁性体が磁路に並列に加わるのでI型コ
ア部分の磁気抵抗を低くでき、再生効率の低下を防ぎ高
い効率で信号を記録再生できる磁気ヘッドが得られるも
のである。Effect With the above-mentioned configuration, the length L of the I-shaped core is short (although the metal magnetic material formed at the end is applied in parallel to the magnetic path, so the magnetic resistance of the I-shaped core part can be lowered, reducing the reduction in regeneration efficiency. This provides a magnetic head that can record and reproduce signals with high efficiency.
実施例
本発明の一実施例の斜視図を第1図に示す。図において
、1は非晶質合金やセンダスト合金等の金属磁性膜であ
り、チタン酸カルシウム系セラミックス等の非磁性基板
2で挟持されて主磁気コアを構成している。磁気コアは
巻線窓3を有するC型コアと記録媒体走行方向の長さが
約0.2mm程度のI型コアとからなり、非磁性膜を介
して対向しボンディングガラス4によって接合されて磁
気ギャップ5を形成している。又、I型コアの巻線窓と
反対側の側面には5iOzなどの非磁性絶縁膜を介して
非晶質合金やセンダスト合金等の金属磁性膜6が形成さ
れている。このような構造lこすることによって例えば
金属磁気コア幅30μm、チップ幅130μmのI型コ
アに対して約45μm厚の金属磁性膜を形成すれば■型
コアの磁気抵抗は金属磁性膜の無い場合の約半分になり
、1型コアの長さが0.2mm程度になっても従来見ら
れたようなヘッド出力の低下はほとんど無くなる。なお
ヘッド端部に金属磁性膜が露出していると疑似ギャップ
となり不要な信号を発生することになるので、端部は削
り落として金属磁11膜がテープと接触しない構造にす
るのが望ましい。Embodiment A perspective view of an embodiment of the present invention is shown in FIG. In the figure, reference numeral 1 denotes a metal magnetic film such as an amorphous alloy or Sendust alloy, which is sandwiched between non-magnetic substrates 2 such as calcium titanate ceramics to form a main magnetic core. The magnetic core consists of a C-shaped core with a winding window 3 and an I-shaped core with a length of about 0.2 mm in the recording medium running direction, which are opposed to each other with a non-magnetic film in between and bonded by a bonding glass 4 to form a magnetic core. A gap 5 is formed. Further, on the side surface of the I-shaped core opposite to the winding window, a metal magnetic film 6 made of an amorphous alloy, sendust alloy, etc. is formed with a non-magnetic insulating film made of 5iOz or the like interposed therebetween. If a metal magnetic film with a thickness of about 45 μm is formed on an I-type core with a metal magnetic core width of 30 μm and a chip width of 130 μm by rubbing such a structure, the magnetic resistance of the ■-type core will be the same as that without the metal magnetic film. Even if the length of the type 1 core becomes about 0.2 mm, the decrease in head output that has been seen in the past almost disappears. Note that if the metal magnetic film is exposed at the end of the head, it will create a pseudo gap and generate unnecessary signals, so it is desirable to shave off the end so that the metal magnetic film 11 does not come into contact with the tape.
このような磁気ヘッドの製造方法としては、先ず非磁性
基板上に金属磁性膜をスパッタリングで形成し、これを
複数枚積み重ねて結晶化ガラス等で接着し切断すること
によって金属磁性膜と非磁性基板が交互に積層された一
対のコアブロックができる。この一対のコアブロックの
うち一方は巻線窓を形成してC型コアブロックとし、他
方はそのままの形状で■型コアブロックとする。その後
両コアブロックのギャップ面を鏡面に研磨し、ガラス等
の非磁性薄膜をスパッタリングで所定膜厚形成した後突
き合わせてボンディングガラスで接着する。その後1型
コア側を切断、研磨で約0゜2 m mの長さに仕上げ
る。次にこの研磨したI型コアの面に金属磁性膜をスパ
ッタリングで形成する。その後これを所定の厚みで切断
して前面をテープラッピングすることによって第1図に
示す磁気ヘッドが製造出来る。特に非晶質合金を用いる
場合は熱処理に制限が加わることから1コア側面に形成
する金属磁性膜は飽和磁束密度が磁気コア部と比べて低
く、比較的低温でアニルしても高い透磁率が得られる組
成を選ぶのが良い。The manufacturing method for such a magnetic head is to first form a metal magnetic film on a non-magnetic substrate by sputtering, stack multiple sheets, adhere them with crystallized glass, etc., and cut them. This creates a pair of core blocks in which the core blocks are alternately stacked. One of the pair of core blocks forms a winding window to form a C-shaped core block, while the other remains in the same shape as a ■-shaped core block. Thereafter, the gap surfaces of both core blocks are polished to a mirror surface, a non-magnetic thin film such as glass is formed to a predetermined thickness by sputtering, and the core blocks are butted together and bonded with bonding glass. After that, the type 1 core side is cut and polished to a length of approximately 0°2 mm. Next, a metal magnetic film is formed on the surface of this polished I-type core by sputtering. Thereafter, the magnetic head shown in FIG. 1 can be manufactured by cutting this to a predetermined thickness and wrapping the front surface with tape. In particular, when using an amorphous alloy, there are restrictions on heat treatment, so the metal magnetic film formed on the side surface of one core has a lower saturation magnetic flux density than the magnetic core, and even if annealed at a relatively low temperature, it has high magnetic permeability. It is better to choose the composition that is obtained.
なお、特に高周波特性を必要とする場合は前記トラック
幅を構成する金属磁性膜を、SiO2等の絶縁層を介し
て積層して渦電流損失を考慮した厚みに分割すると良い
。この場合には、Iコア側面に形成した金属磁性膜で積
層膜を短絡しないように、Iコアとの界面に!t!!縁
層を形成し、端面に形成する金属磁性膜自体も積層構造
にしたほうが良好な特性が得られる。In addition, when particularly high frequency characteristics are required, it is preferable that the metal magnetic films constituting the track width are laminated via an insulating layer such as SiO2 and divided into thicknesses that take into account eddy current loss. In this case, be careful not to short-circuit the laminated film with the metal magnetic film formed on the side surface of the I-core at the interface with the I-core! T! ! Better characteristics can be obtained by forming the edge layer and forming the metal magnetic film itself formed on the end face into a laminated structure.
発明の効果
本発明によれば、高抗磁力媒体の性能を十分に引き出す
ことができ、且つ2個のヘッドが狭いギャップ間隔で配
置されるシステムにおいても十分その特長を発揮できる
磁気ヘッドが容易に得られるものである。Effects of the Invention According to the present invention, it is possible to easily create a magnetic head that can fully bring out the performance of a high coercive force medium and can fully exhibit its characteristics even in a system in which two heads are arranged with a narrow gap. That's what you get.
第1図は本発明の一実施例における磁気ヘットの斜視図
、第2図及び第3図は従来の磁気ヘッドの斜視図、第4
図は第3図に示した従来の磁はヘッドにおけるI型コア
の長さとヘッド出力の関係を示す図である。
1・・・・金属磁性膜、2・・・・非磁性基板、3・・
・・巻線窓、4・・・・ボンディングガラス、5・・・
・磁気ギャップ、6・・・・金属磁性膜、7・・・・酸
化物弓A、 磁性体。
代理人の氏名 弁理士 中尾敏男 ほか1名第1図
5罹気rぎツブ
箔 2 図
第3図
第4図
Iボア侵(m−t )FIG. 1 is a perspective view of a magnetic head according to an embodiment of the present invention, FIGS. 2 and 3 are perspective views of a conventional magnetic head, and FIG.
This figure is a diagram showing the relationship between the length of the I-shaped core in the conventional magnetic head shown in FIG. 3 and the head output. 1...Metal magnetic film, 2...Nonmagnetic substrate, 3...
...Wire-wound window, 4...Bonding glass, 5...
・Magnetic gap, 6...Metal magnetic film, 7...Oxide bow A, magnetic material. Name of agent: Patent attorney Toshio Nakao and one other person Figure 1 Figure 5 Figure 4 Figure I Bore Invasion (m-t)
Claims (3)
構造からなり、磁気ギャップをはさんで巻線窓の無いI
型コアの記録媒体走行方向の長さが巻線窓を有するC型
コアの長さより短い構造の磁気ヘッドにおいて、前記I
型コアの巻線窓と反対の端面に金属磁性体が形成された
構造からなることを特徴とする磁気ヘッド。(1) The main magnetic core has a structure in which a metal magnetic film is sandwiched between non-magnetic substrates, and an I
In a magnetic head having a structure in which the length of the recording medium running direction of the type core is shorter than the length of the C type core having a winding window, the I
A magnetic head characterized by having a structure in which a metal magnetic material is formed on an end surface of a mold core opposite to a winding window.
磁性体が金属磁性薄膜と絶縁薄膜とを交互に積層した多
層膜よりなることを特徴とする特許請求の範囲第1項記
載の磁気ヘッド。(2) Claim 1, characterized in that the metal magnetic material formed on the end face of the I-shaped core opposite to the winding window is made of a multilayer film in which metal magnetic thin films and insulating thin films are alternately laminated. The magnetic head described.
積層した多層膜磁気コアからなることを特徴とする特許
請求の範囲第1項または第2項記載の磁気ヘッド。(3) The magnetic head according to claim 1 or 2, wherein the main magnetic core is a multilayer magnetic core in which metal magnetic thin films and insulating thin films are alternately laminated.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6099088A JPH01235005A (en) | 1988-03-15 | 1988-03-15 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6099088A JPH01235005A (en) | 1988-03-15 | 1988-03-15 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01235005A true JPH01235005A (en) | 1989-09-20 |
Family
ID=13158381
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6099088A Pending JPH01235005A (en) | 1988-03-15 | 1988-03-15 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01235005A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1084906C (en) * | 1996-04-02 | 2002-05-15 | 日本胜利株式会社 | Magnetic head and magnetic head assembly |
-
1988
- 1988-03-15 JP JP6099088A patent/JPH01235005A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1084906C (en) * | 1996-04-02 | 2002-05-15 | 日本胜利株式会社 | Magnetic head and magnetic head assembly |
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