JPS5852670A - Magnetic recording method - Google Patents

Magnetic recording method

Info

Publication number
JPS5852670A
JPS5852670A JP15112681A JP15112681A JPS5852670A JP S5852670 A JPS5852670 A JP S5852670A JP 15112681 A JP15112681 A JP 15112681A JP 15112681 A JP15112681 A JP 15112681A JP S5852670 A JPS5852670 A JP S5852670A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic recording
layer
magnetic field
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
Application number
JP15112681A
Other languages
Japanese (ja)
Other versions
JPH038549B2 (en
Inventor
Hajime Machida
元 町田
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP15112681A priority Critical patent/JPS5852670A/en
Publication of JPS5852670A publication Critical patent/JPS5852670A/en
Publication of JPH038549B2 publication Critical patent/JPH038549B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G19/00Processes using magnetic patterns; Apparatus therefor, i.e. magnetography

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Photoreceptors In Electrophotography (AREA)
  • Recording Or Reproducing By Magnetic Means (AREA)
  • Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)

Abstract

PURPOSE:To obtain a magnetic recording method which performs high-density recording with simplified constitution and is suitable for high-speed recording. CONSTITUTION:On a nonmagnetic base 1a, a magnetic recording layer 1b is laminated and on this magnetic recording layer 1b, a semiconductor layer 1c with 10<3>-10<6> surface resistance is laminated to obtain a magnetic recording medium 1. This medium is heated by a heater 2 and also placed in a magnetic field produced by a magnet 3 to direct the magnetic field of the magnetic recording layer 1b in a specified layer direction of the magnetic recording medium 1. Then, the magnetic recording medium 1 is applied by a magnet 4 with a magnetic field in the opposite direction to the magnetic field of the magnetic recording layer 1b. A recording electrode 5 is brought into contact with the semiconductor layer IC of the medium 1 so that it is in the magnetic field of the magnet 4, and a return circuit electrode 6 arranged at a prescribed interval from said recording electrode 5 is also brought into contact; and an impulsive image signal voltage from an image signal voltage applying circuit 7 is applied between those recording electrode 5 and return circuit electrode 6 to power up the semiconductor layer 1c, and thus Joule heat is generated to invert the direction of the magnetic field of the magnetic recording layer 1b facing the recording electrode 5, thereby forming a magnetic latent image.

Description

【発明の詳細な説明】 本発明は、磁気記録媒体に磁気潜像を形成する磁気記録
方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic recording method for forming a magnetic latent image on a magnetic recording medium.

従来から、磁気記録方法として、磁気記録媒体の近くに
ヘッドにコイルを巻回したものを配置し、このコイルに
信号電流を流して形成される磁界で磁気記録媒体に磁気
潜像を形成するものが知られている。しかし、この磁気
記録方法は、多数のヘッドを用いて高速記録を行う場合
に、各ヘッドごとにコイルを巻く必要があるのでその製
作が複雑となるため高密度の記録がむずかしい。
Traditionally, magnetic recording methods involve placing a coil wound around a head near the magnetic recording medium, and forming a magnetic latent image on the magnetic recording medium using the magnetic field created by passing a signal current through the coil. It has been known. However, in this magnetic recording method, when performing high-speed recording using a large number of heads, it is necessary to wind a coil for each head, which complicates manufacturing and makes high-density recording difficult.

また、レーザー光を磁気記録媒体に照射してレーザー光
のエネルギーで磁気記録媒体を加熱して磁気潜像を形成
する磁気記録方法も知られている。
Also known is a magnetic recording method in which a magnetic recording medium is irradiated with laser light and the magnetic recording medium is heated by the energy of the laser light to form a magnetic latent image.

しかし、この磁気記録方法は、レーザー光の変調および
走査が複雑であり、かつ、光学系を配置する空間が大き
く必要であるため小型化に適していないという欠点があ
る。
However, this magnetic recording method has disadvantages in that modulation and scanning of the laser beam are complicated, and a large space is required for arranging the optical system, making it unsuitable for miniaturization.

さらKまた、熱ヘッドで磁気記録媒体を直接に加熱して
磁気潜像を形成する磁気記録方法も知られている。しか
し、この磁気記録方法は、記録に必要なエネルギーが大
きく、かつ、熱ヘッドを冷却する工程が必要であるため
高速記録に適していないという欠点がある。
Further, a magnetic recording method is also known in which a magnetic recording medium is directly heated with a thermal head to form a magnetic latent image. However, this magnetic recording method has the disadvantage that it is not suitable for high-speed recording because it requires a large amount of energy for recording and requires a step to cool the thermal head.

本発明の目的は、構成が簡単であって高密度の記録が可
能であり、かつ、高速記録に適している磁気記録方法を
提供することにある。
An object of the present invention is to provide a magnetic recording method that has a simple configuration, enables high-density recording, and is suitable for high-speed recording.

本発明は、非磁性支持体に磁性記録層を積層し、かつ、
この磁性記録層に半導電層を積層してなる磁気記録媒体
に熱および外部磁界を加えて磁気記録層の磁界の方向を
磁気記録媒体の一定の層方向とし、次に磁気記録層の磁
界の方向と反対方向の外部磁界を磁気記録媒体に加えた
状態で、磁気記録媒体の半導電層に記録電極と帰路電極
とを接触させ、かつ、これらの記録電極と帰路電極との
間に追択的に画像信号電圧を印加して半導電層に通電し
てジュール熱を発生させることにより記録電極に対向す
る磁気記録層の磁界の方向を反転させて磁気潜像を形成
することを特徴とする。
The present invention comprises laminating a magnetic recording layer on a non-magnetic support, and
Heat and an external magnetic field are applied to the magnetic recording medium formed by stacking a semiconducting layer on this magnetic recording layer to make the direction of the magnetic field in the magnetic recording layer a certain layer direction of the magnetic recording medium, and then the direction of the magnetic field in the magnetic recording layer is A recording electrode and a return electrode are brought into contact with the semiconducting layer of the magnetic recording medium while an external magnetic field in the opposite direction is applied to the magnetic recording medium, and an additional electrode is added between the recording electrode and the return electrode. A magnetic latent image is formed by reversing the direction of the magnetic field in the magnetic recording layer facing the recording electrode by applying current to the semiconducting layer by applying an image signal voltage to generate Joule heat. .

以下に図面を参照しながら本発明の詳細な説明する。The present invention will be described in detail below with reference to the drawings.

第1図において符号】は磁気記録媒体を示l〜て(3) いる。この磁気記録媒体1は、非磁性支持体1aに磁気
記録層1bを積層し、かつ、この磁気記録層11)に半
導電層ICを積層【〜でなる。
In FIG. 1, the symbols ] indicate magnetic recording media. This magnetic recording medium 1 consists of a magnetic recording layer 1b laminated on a non-magnetic support 1a, and a semiconducting layer IC laminated on this magnetic recording layer 11).

上記非磁性支持体1aは、Cu土たけプラスチックフィ
ル、ポリカーボネート、マイラーおよびポリイミドフィ
ルなどで5〜100μmの膜厚に形成される。
The non-magnetic support 1a is formed of Cu clay plastic fill, polycarbonate, Mylar, polyimide fill, etc. to a thickness of 5 to 100 μm.

上記磁気記録層11)は、熱と外部磁界を加えることに
より磁界の方向を反転百」能な物乍」で0.5〜50μ
nlの膜厚に形成されろ。上記磁気記録層11)を形成
する物質としては、キュリ一温度が約130′Cである
rl、I))ipe1キュリ一温度が約601?である
FeDy、補償点が30[であるFeQd、補償点が8
0UであるGdCo、キュリ一温度が160′C:であ
る(TbF’e)Gdおよび(’、f’bFe)’Dy
などの重金属と遷移金属との合金が良い。」二部磁気記
録層1bは、スパッター法、蒸着法またはメッキ法で形
成される。
The magnetic recording layer 11) is a material capable of reversing the direction of the magnetic field by applying heat and an external magnetic field, and has a thickness of 0.5 to 50 μm.
It should be formed to a film thickness of nl. The materials forming the magnetic recording layer 11) include rl, which has a Curie temperature of about 130'C, I)) ipe1, which has a Curie temperature of about 601? FeDy, compensation point is 30 [FeQd, compensation point is 8
GdCo which is 0U, Curie temperature is 160'C: (TbF'e)Gd and (',f'bFe)'Dy
Alloys of heavy metals and transition metals such as The two-part magnetic recording layer 1b is formed by sputtering, vapor deposition, or plating.

上記半導電層ICは、10〜10 Ωの表面抵抗を有す
ると共に軟化点が180 tG以上である物(4( 質で1〜50μmの膜厚に形成される。上記半導電層1
cは、絶縁性バインダー用樹脂に導電粉末を均一に分散
して形成される。半導電層ICの絶縁性バインダー用樹
脂としては、ポリカーボネート、ポリエチレン、ポリエ
ステル、マイラー、ポリイミド、および、塩化ビニルな
どが用いられる。半導電層ICの導電粉末としては、金
属粉末、導電性カーボンおよび導電性プラスチック粉末
が用いられる。
The semiconducting layer IC has a surface resistance of 10 to 10 Ω and a softening point of 180 tG or more.
c is formed by uniformly dispersing conductive powder in an insulating binder resin. As the resin for the insulating binder of the semiconductive layer IC, polycarbonate, polyethylene, polyester, mylar, polyimide, vinyl chloride, etc. are used. As the conductive powder of the semiconductive layer IC, metal powder, conductive carbon, and conductive plastic powder are used.

先ず、第1図に示すように、上記磁気記録媒体1をヒー
タ2で加熱すると共に磁石3の磁界中に磁気記録媒体1
を配置して、磁気記録層1bの磁界を磁気記録媒体1の
一定の層方向へ向ける。
First, as shown in FIG. 1, the magnetic recording medium 1 is heated by the heater 2 and placed in the magnetic field of the magnet 3.
is arranged to direct the magnetic field of the magnetic recording layer 1b in a certain layer direction of the magnetic recording medium 1.

次に、第2図に示すように、上記磁気記録媒体1の磁気
記録層1bの磁界の方向と反対方向の磁界を磁石4によ
り磁気記録媒体1に加える。上記磁気記録媒体10半導
電層1cに、上記磁石4の磁界中に位Rするように記録
層&5を接触′1″ると共にこの記録電極5から所定間
隔をおいて配置された帰路電極6を接触し、かつ、これ
らの記録電極5と帰路′「汀イク6との間に画像信号電
圧印加回路7によりパルス状の画像信号電圧を印加して
半導電層1Cに通電してジュール熱を発生させることに
より記録電極5に対向する磁気記録層1+)の磁界の方
向を反転させて磁気潜像を形成する。
Next, as shown in FIG. 2, a magnetic field is applied to the magnetic recording medium 1 by the magnet 4 in a direction opposite to that of the magnetic recording layer 1b of the magnetic recording medium 1. As shown in FIG. A recording layer &5 is brought into contact with the semiconductive layer 1c of the magnetic recording medium 10 so as to be positioned R in the magnetic field of the magnet 4, and a return electrode 6 is placed at a predetermined distance from the recording electrode 5. A pulsed image signal voltage is applied by the image signal voltage applying circuit 7 between the recording electrode 5 and the return path 6, and the semiconductive layer 1C is energized to generate Joule heat. By doing so, the direction of the magnetic field of the magnetic recording layer 1+) facing the recording electrode 5 is reversed to form a magnetic latent image.

上記記録電極5の平導箱′層1c[対する接触面積は帰
路電極6の半導電層1cに対する接触面積より非常に小
さいように設定されている1、記録電極5の直径をdと
し、帰路電極6の半導電層1cに対する接触面が一辺が
Dの正方形とした場合に10 d ((Dの条件を満足
する必要がある。
The contact area of the recording electrode 5 with the flat conducting box layer 1c is set to be much smaller than the contact area of the return electrode 6 with the semiconductive layer 1c.The diameter of the recording electrode 5 is d, and the return electrode When the contact surface of No. 6 to the semiconductive layer 1c is a square with sides D, 10 d ((It is necessary to satisfy the condition D.

また、上記半導電層1cの強度を一定以上に保つために
その厚さは、171m以上とする必要があり、かつ、5
0μmを超えると記録以外に消費される通電エネルギー
が大きくなるので50μtn以下とすることが好ましい
In addition, in order to maintain the strength of the semiconductive layer 1c above a certain level, its thickness must be 171 m or more, and
If it exceeds 0 μm, the energy consumed for purposes other than recording increases, so it is preferable to set it to 50 μtn or less.

そ1.て、上記記録電極5と帰路電極6との距離をLと
すると、2d’:)Lである場合には記録電極5と帰路
電極6との間の磁気記録層1bの部分まで磁界の方向が
反転してしまう可能性があるので、2d≦T、という条
件を満足する必要がある。Lが大きくなると、記録部分
以外の通電経路で消費されろエネルギーが大きくなるか
ら、dとLの関係のさらに好ましい条件は5d≦L≦8
0dである。
Part 1. If the distance between the recording electrode 5 and the return electrode 6 is L, then if it is 2d':)L, the direction of the magnetic field will reach the part of the magnetic recording layer 1b between the recording electrode 5 and the return electrode 6. Since there is a possibility of inversion, it is necessary to satisfy the condition 2d≦T. As L becomes larger, more energy is consumed in the energizing path other than the recording part, so a more preferable condition for the relationship between d and L is 5d≦L≦8.
It is 0d.

また、解像力の実用上の範囲は8〜16ドツト/罰であ
るから、50μm≦d≦150/ln1であることが必
要である〇 さらに、上記半導電層ICの厚さをlとし、田作を満足
する必要があり、その理由を次に説明する。
In addition, since the practical range of resolution is 8 to 16 dots/penalty, it is necessary that 50 μm≦d≦150/ln1〇Furthermore, the thickness of the semiconductive layer IC is 1, and Tasaku The reason for this is explained below.

上記半導電層ICの体積固有抵抗をρVとし、半導電層
ICの厚さ方向の抵抗をRtとし、平面方向の抵抗をR
pとすると、R1およびRpは次の式で表わされる。
The volume resistivity of the above semiconducting layer IC is ρV, the resistance in the thickness direction of the semiconducting layer IC is Rt, and the resistance in the planar direction is R.
When p is R1 and Rp are expressed by the following formula.

1 it t−ρ■×−5□ ・・・・・・(1)上記(1
) 、 (2)式からupとrttとの比KEを求め(
7) ると、KEは次の式で表わされる。
1 it t-ρ■×-5□ ・・・・・・(1) Above (1
), Find the ratio KE of up and rtt from equation (2) (
7) Then, KE is expressed by the following formula.

K E一旦・−リ上・・・・・・(3)R,t”412 上記りを主して変化させてKEを5〜10”の範囲で変
化させて記録エネルギーの変化および磁気記録層1 b
の磁界の方向が反転した部分の記録電極5の面積に対す
る拡大率を調べたところ、記録エネルギーはKEの増大
にともなって増大し、また、上記拡大率はKEの増大に
ともなって減少した。そして、実用上記録エネルギーは
20rnJ/ドツト以下であることが望ましく、かつ、
拡大率は−20チ〜+100%であることが望ましいの
で、10≦K I≦105の条件を満足する必要がある
Once KE...... (3) R, t''412 Mainly changing the above, KE is changed in the range of 5 to 10'' to change the recording energy and the magnetic recording layer. 1 b
When the magnification ratio with respect to the area of the recording electrode 5 at the portion where the direction of the magnetic field was reversed was investigated, it was found that the recording energy increased as KE increased, and the magnification ratio decreased as KE increased. In practical terms, it is desirable that the recording energy be 20 rnJ/dot or less, and
Since the magnification ratio is preferably -20% to +100%, it is necessary to satisfy the following conditions: 10≦K I≦105.

なお、複数の記録電極5を1列状に配置してもよく、ま
た、複数の記録電極5を複数列状に配置すると共に各列
の記録電極5を他の列の記録電極5の中間に位置させて
もよい。
Note that a plurality of recording electrodes 5 may be arranged in a single row, or a plurality of recording electrodes 5 may be arranged in a plurality of rows and the recording electrodes 5 in each row may be placed between the recording electrodes 5 in other rows. It may be located.

第3図に本発明を実施する装置の1実施例が示されてい
るので、次にこれを説明する。
FIG. 3 shows one embodiment of an apparatus for carrying out the present invention, which will now be described.

(8) 第3図において符号8,9はそれぞれ搬送ローラーを示
しており、これらの搬送ローラー8,9はそれぞれ図示
してない駆動手段により矢印a。
(8) In FIG. 3, reference numerals 8 and 9 indicate conveyance rollers, and these conveyance rollers 8 and 9 are driven by driving means (not shown) in the direction of arrow a.

b方向へ回転される。これらの搬送ローラー8゜9には
エンドレスの磁気記録媒体1が取り掛けられている。こ
の磁気記録媒体1は、非磁性支持体1aが外側に位置し
半導電層ICが内側に位置するように搬送ローラー8,
9に取り掛けられて(・て、搬送ローラー8,9により
矢印C方向へ移動される。
It is rotated in direction b. An endless magnetic recording medium 1 is hung on these transport rollers 8.9. This magnetic recording medium 1 is moved by transport rollers 8, so that the nonmagnetic support 1a is located on the outside and the semiconductive layer IC is located on the inside.
9 and is moved in the direction of arrow C by conveyance rollers 8 and 9.

上記搬送ローラー8の近くの上側に位置する磁気記録媒
体1の上にはヒータ2および磁石3が配置されている。
A heater 2 and a magnet 3 are arranged above the magnetic recording medium 1 located above the transport roller 8.

このヒータ2により磁気記録層1bを加熱すると共に磁
石3により磁気記録層1bに磁界を加えて磁気記録層1
blC磁気記録媒体1の一定の層方向の磁界を形成する
。上記搬送ローラー9の近くの上側に位置する磁気記録
媒体1の半導電層ICに接触するように複数の記録電極
5および帰路電極6が配置されている。これらの記録電
極5と帰路電極6とには画像信号電圧印加回路7が接続
されている。上記記録電極5と対向する磁気記録媒体1
の上には磁石4が配置されろ。
The heater 2 heats the magnetic recording layer 1b, and the magnet 3 applies a magnetic field to the magnetic recording layer 1b.
A magnetic field is formed in a certain layer direction of the blC magnetic recording medium 1. A plurality of recording electrodes 5 and return electrodes 6 are arranged so as to contact the semiconductive layer IC of the magnetic recording medium 1 located above the transport roller 9. An image signal voltage applying circuit 7 is connected to these recording electrodes 5 and return electrodes 6. Magnetic recording medium 1 facing the recording electrode 5
A magnet 4 is placed above it.

上記磁石3の磁界の方向と磁石4の磁界の方向とは反対
である。上記画像信号電圧印加回路7により記録電極5
と帰路電極6との間に選択的圧パルス状の画像信号電圧
を印加することにより、上述のように磁気配録層1bに
磁気潜像が形成される。
The direction of the magnetic field of the magnet 3 and the direction of the magnetic field of the magnet 4 are opposite. The recording electrode 5 is controlled by the image signal voltage application circuit 7.
By applying an image signal voltage in the form of a selective pressure pulse between the magnetic recording layer 1b and the return electrode 6, a magnetic latent image is formed on the magnetic recording layer 1b as described above.

上記搬送ローラー9の下側に位置する磁気記録媒体1の
外側には現像装w10が配置されている。
A developing device w10 is arranged outside the magnetic recording medium 1 located below the transport roller 9.

この現像装置10は、容器10aとこの容器10aに収
容された磁性粉を含有したトナー10!〕と、このトナ
ー10bを磁気記録媒体1方向へ移動させるローラー]
Ocとからなる。上舊己トナー10bは、全体積の20
%以上の磁性粉を含有していると共に1μC/g以上の
電荷を有するものである。上記磁気記録層1bの磁界の
方向が反転した部分の磁界は非常に強いから、この部分
に上記トナー10bが吸引されて磁気記録媒体1の非磁
性支持体1aK付着して磁気潜像が可視化される。
This developing device 10 includes a container 10a and a toner 10 containing magnetic powder contained in the container 10a! ] and a roller that moves this toner 10b in one direction of the magnetic recording medium]
It consists of Oc. The Kamibake toner 10b has a total volume of 20
% or more of magnetic powder and has a charge of 1 μC/g or more. Since the magnetic field in the portion of the magnetic recording layer 1b where the direction of the magnetic field is reversed is very strong, the toner 10b is attracted to this portion and adheres to the non-magnetic support 1aK of the magnetic recording medium 1, making a magnetic latent image visible. Ru.

上記搬送ローラー8の下には磁気記録媒体1の外側に転
写装置11が配置されていると共に転写媒体12を搬送
するローラー13が配置されている。」1記転写装置1
1と磁気記録媒体1の間に転写媒体12が挿入されると
、転写装置11の放電により磁気記録媒体1のトナーが
クーロン力により転写媒体12に転移される。上記搬送
ローラー80近くには、転写後の磁気記録方法工に残留
しているトナーを除去するためのクリーニング装置14
が配置されている。このクリーニング装置14は、外周
面に毛が植えられたマグネットローラー14aと、この
マグネットローラー14aに接触しているl・ナー分離
ローラー14bと、l・ナーを収容する容器14cと、
この容器1.4 cの下に配置されたトナー回収容器1
4. dとからなる。
Below the conveyance roller 8, a transfer device 11 is disposed outside the magnetic recording medium 1, and a roller 13 for conveying the transfer medium 12 is disposed. "1 Transfer device 1
When the transfer medium 12 is inserted between the transfer device 1 and the magnetic recording medium 1, the toner on the magnetic recording medium 1 is transferred to the transfer medium 12 by the Coulomb force due to the discharge of the transfer device 11. A cleaning device 14 is provided near the conveyance roller 80 for removing toner remaining on the magnetic recording method after transfer.
is located. This cleaning device 14 includes a magnetic roller 14a with hair planted on the outer peripheral surface, an l/ner separation roller 14b in contact with the magnetic roller 14a, and a container 14c containing l/ner.
Toner collection container 1 placed under this container 1.4 c
4. It consists of d.

上記マグネットローラー14aの毛が磁気記録媒体1の
残留トナーに接触して残留トナーを磁気記録媒体1から
分離させると共にマグネットローラー14aは磁力によ
り残留トナーを吸引して磁気記録媒体1から残留トナー
を除去する。このマグネットローラー14aに何着した
トナーはI・ナー分離ローラー14bにより分離されて
容器1.4 cへ落下される。
The hairs of the magnetic roller 14a come into contact with the residual toner on the magnetic recording medium 1 and separate the residual toner from the magnetic recording medium 1, and the magnetic roller 14a attracts the residual toner by magnetic force and removes the residual toner from the magnetic recording medium 1. do. The toner that has landed on this magnetic roller 14a is separated by an I/toner separation roller 14b and dropped into a container 1.4c.

上記クリーニング装@14により残留トナーを除去され
た磁気記録媒体1はヒータ2により加熱された後に磁石
3により一定方向の磁界を加えられて再度記録が可能な
状態となる。
The magnetic recording medium 1 from which residual toner has been removed by the cleaning device @ 14 is heated by the heater 2, and then a magnetic field is applied in a certain direction by the magnet 3, so that it becomes ready for recording again.

本発明の磁気記録方法は、構成がTll1i君今であっ
て高密度の記録が可能であり、かつ、高速記録に適して
いる。
The magnetic recording method of the present invention has the same configuration as Tll1i, and is capable of high-density recording and is suitable for high-speed recording.

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

第1図および第2図は本発明を訣明するための図、並び
に、第3図は本発明を実施する装置の1実施例を示すシ
1である。 1・・・磁気記録媒体、1a・・・非磁性支す体、■b
・・・磁気記録層、1c・・・半導′酸層、2・・・ヒ
ータ、3,4・・・磁石、5・・・記録電極、6・・・
帰路Tli極、7・・・画像信号電圧印加回路 \                     \−4
4:
1 and 2 are diagrams for explaining the present invention, and FIG. 3 is a diagram illustrating an embodiment of an apparatus for carrying out the present invention. 1...Magnetic recording medium, 1a...Nonmagnetic supporting body, ■b
... Magnetic recording layer, 1c... Semiconductor acid layer, 2... Heater, 3, 4... Magnet, 5... Recording electrode, 6...
Return path Tli pole, 7... Image signal voltage application circuit\\-4
4:

Claims (1)

【特許請求の範囲】[Claims] 熱および外部磁界によって磁界方向を反転可能な磁気記
録層を非磁性支持体に積層し、かつ、上記磁気記録層に
10〜10 Ωの表面抵抗を有する半導電層を積層して
なる磁気記録媒体に熱および外部磁界を加えて磁気記録
層の磁界の方向を磁気記録媒体の一定の層方向とし、次
に磁気記録層の磁界の方向と反対方向の外部磁界を磁気
記録媒体に加えた状態で、磁気記録媒体の半導電層に記
録電接とこれから所定間隔をおいて配置された帰路電極
を接触させ、かつ、これらの記録電極と帰路電極との間
に選択的に画像信号電圧を印加して半導電層に通電して
ジュール熱を発生させることにより記録電極に対向する
磁気記録層の磁界の方向を反転させて磁気潜像を形成す
ることを特徴とする磁気記録方法。
A magnetic recording medium in which a magnetic recording layer whose magnetic field direction can be reversed by heat and an external magnetic field is laminated on a non-magnetic support, and a semiconducting layer having a surface resistance of 10 to 10 Ω is laminated on the magnetic recording layer. Heat and an external magnetic field are applied to the magnetic recording layer so that the direction of the magnetic field is in a certain layer direction of the magnetic recording medium, and then an external magnetic field is applied to the magnetic recording medium in the opposite direction to the magnetic field direction of the magnetic recording layer. , a recording electrical contact and a return electrode arranged at a predetermined interval from the semiconductive layer of the magnetic recording medium are brought into contact with each other, and an image signal voltage is selectively applied between these recording electrodes and the return electrode. A magnetic recording method characterized in that a magnetic latent image is formed by reversing the direction of a magnetic field in a magnetic recording layer facing a recording electrode by passing current through a semiconductive layer to generate Joule heat.
JP15112681A 1981-09-22 1981-09-22 Magnetic recording method Granted JPS5852670A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15112681A JPS5852670A (en) 1981-09-22 1981-09-22 Magnetic recording method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15112681A JPS5852670A (en) 1981-09-22 1981-09-22 Magnetic recording method

Publications (2)

Publication Number Publication Date
JPS5852670A true JPS5852670A (en) 1983-03-28
JPH038549B2 JPH038549B2 (en) 1991-02-06

Family

ID=15511926

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15112681A Granted JPS5852670A (en) 1981-09-22 1981-09-22 Magnetic recording method

Country Status (1)

Country Link
JP (1) JPS5852670A (en)

Also Published As

Publication number Publication date
JPH038549B2 (en) 1991-02-06

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