JPS6055377A - Formation of magnetic latent image - Google Patents

Formation of magnetic latent image

Info

Publication number
JPS6055377A
JPS6055377A JP16316383A JP16316383A JPS6055377A JP S6055377 A JPS6055377 A JP S6055377A JP 16316383 A JP16316383 A JP 16316383A JP 16316383 A JP16316383 A JP 16316383A JP S6055377 A JPS6055377 A JP S6055377A
Authority
JP
Japan
Prior art keywords
magnetic
latent image
magnetic field
length
magnetic latent
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
JP16316383A
Other languages
Japanese (ja)
Inventor
Koichi Saito
孝一 斉藤
Yoshihiko Fujimura
義彦 藤村
Yuji Suemitsu
末光 裕治
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.)
Fujifilm Business Innovation Corp
Original Assignee
Fuji Xerox 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 Fuji Xerox Co Ltd filed Critical Fuji Xerox Co Ltd
Priority to JP16316383A priority Critical patent/JPS6055377A/en
Publication of JPS6055377A publication Critical patent/JPS6055377A/en
Pending 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)

Abstract

PURPOSE:To obtain the more uniform reproducibility of a solid and a dot image by impressing dot-shaped heat input such as thermal head and laser light so that they overlap each other spatially on a magnetic latent image carrier, and making an external impressed magnetic field opposite in direction synchronously. CONSTITUTION:The magnetic latent image carrier moves as shown by an arrow 8 to draw a track shown by a chain line 9. Simultaneously, an external magnetic field 7 is impressed firstly and then an external magnetic field 7' in the opposite direction is impressed; and the direction of the external magnetic field is inverted repeatedly to form magnetic latent images 5a, 5b... on the magnetic latent image carrier in alternate directions. An integral multiple of the length of magnetism produced in one heat cycle is one magnetic latent image unit, which is formed to an optional multiple of magnetism length. The solid image, therefore, consists of magnetic latent image units having a sufficiently large multiple of magnetisum length, and a magnetic field which has the magnetism length as basic repetition in free space is established in the solid, so the uniform sticking of magnetic toner and magnetic ink is possible.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は磁気複写方法、詳しく言えば磁化しつる磁性体
に、サーマルヘッド、L/−f−f、にトの熱入力によ
って磁気潜像を形成する方法に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a magnetic copying method, more specifically, a method for forming a magnetic latent image on a magnetized magnetic material by heat input from a thermal head, L/-ff, and Ni. Regarding how to.

従来技術 従来、磁気複写に於ける磁気潜像形成方法として種々の
方法が提案されている。それらのなかで磁化しつる磁性
体薔こ比較的室温に近い高温ニキ、 −IJ一温度を有
する二酸クロム(Cr0z )などの熱磁気材料を用い
、サーマルヘッドやレーザー光などでドツト状の熱像を
加えながら、外部磁界を印加して熱残留磁化現象ζこよ
り、熱と磁界の協同作用によって磁気潜像を形成する方
法が知られている。この方法では場合によっては熱磁気
材料が予め所定の一方向に一様磁化されているものを用
いて、熱入力部で磁化の向きが反転するように外部磁界
を印加Tる事もできる。
BACKGROUND OF THE INVENTION Conventionally, various methods have been proposed as methods for forming magnetic latent images in magnetic copying. Among them, thermomagnetic materials such as chromium dioxide (Cr0z), which has a high temperature relatively close to room temperature and -IJ temperature, are used to generate dot-shaped heat using a thermal head or laser beam. A method is known in which a magnetic latent image is formed by the cooperative action of heat and magnetic field by applying an external magnetic field while applying an image, thereby causing a thermal residual magnetization phenomenon ζ. In this method, depending on the case, it is also possible to use a thermomagnetic material that has been uniformly magnetized in one predetermined direction and apply an external magnetic field so that the direction of magnetization is reversed at the heat input section.

この方法は磁気ヘッドを用いる磁気潜像形成方法に較べ
、長尺に必要画素密度だけ発熱体が並べられたサーマル
ヘッドや非接触で高密度に熱像を入力できるレーザー光
学系が使えるので磁気潜像の密度増大や低価格化の点で
優れている。
Compared to the magnetic latent image forming method that uses a magnetic head, this method uses a thermal head in which heating elements are arranged in a long length with the required pixel density, and a laser optical system that can input thermal images at high density without contact. It is superior in terms of increased image density and lower cost.

しかしながら本発明者等の検討によれば、前記の方法で
は磁性トナーや磁性インクなどlこよる顕像化の際に完
全なソリッド像が得られないこと、或いは熱ドツトをそ
のままドツトの形で再現してしまい画像品位を落として
しまうこと等の欠点がある事がわかった。
However, according to studies conducted by the present inventors, it has been found that with the above method, a complete solid image cannot be obtained during visualization due to magnetic toner, magnetic ink, etc., or that thermal dots cannot be reproduced as they are in the form of dots. It has been found that there are drawbacks such as a decrease in image quality.

これは、前述の磁気潜像形成方法に於(・では、加熱ド
ツト部に於ける磁化の向き力S一方向に揃えられてしま
うことによると考えられる。すなわち磁気複写では磁気
潜像から自由空間にあられれる磁界に対応して磁性トナ
ーや磁性インクの付着がおきるので、加熱ドツトサイズ
が大きすぎると加熱ドツトの周辺部でのみ磁界があられ
れ、加熱ドツトの中央部が中ぬけしたりして、ドツト性
が残る再現性になったり〔第1図(、)参照〕、或いは
ソリッドをドツトサイズに分割して加熱磁化して再現し
ようとすると第1図(b)の如(、ソリッドの周辺部だ
けが再現される。
This is thought to be due to the fact that in the above-mentioned method of forming a magnetic latent image, the direction force S of magnetization in the heated dot part is aligned in one direction. In other words, in magnetic copying, the magnetic latent image is transferred from the free space. Adhesion of magnetic toner and magnetic ink occurs in response to the magnetic field generated by the heating dot, so if the heating dot size is too large, the magnetic field will only form around the periphery of the heating dot, and the center of the heating dot may become hollow. If the reproducibility is such that the dot nature remains [see Figure 1 (, )], or if you try to reproduce it by dividing the solid into dot-sized pieces and heating and magnetizing them, as shown in Figure 1 (b) (see Figure 1 ()), only the periphery of the solid is reproduced.

発明の目的 従って、この発明は前述の熱による磁気潜像形成方法に
於ける画像再現性の欠点を改良し、ソリッドの均−再現
性及びドツト像をより均一な再現性に優れた改良された
磁気潜像形成方法を提供することを目的とする。
OBJECTS OF THE INVENTION Accordingly, the present invention improves the drawbacks of image reproducibility in the above-mentioned thermal magnetic latent image forming method, and provides improved reproducibility of solid and dot images with more uniform reproducibility. An object of the present invention is to provide a method for forming a magnetic latent image.

発明の構成 すなわち、本発明の磁気潜像形成方法はサーマルヘッド
やレーザー光などのドツト状の熱入力を磁気潜像担体上
で空間的に重なるように印加し、この熱入力印加と同期
して外部印加磁界の向きを逆転する事を特徴とするもの
である。。
In other words, the magnetic latent image forming method of the present invention applies dot-shaped thermal input from a thermal head or laser beam so as to spatially overlap on a magnetic latent image carrier, and in synchronization with this thermal input application. This is characterized by reversing the direction of the externally applied magnetic field. .

以下、図面に従って本発明の詳細な説明する。Hereinafter, the present invention will be described in detail with reference to the drawings.

第2図に於いて、1は磁性体ベース層、2は熱磁気記録
体層、3はドツト状の熱入力部領域、4は予め形成され
ている背景部磁化である。
In FIG. 2, 1 is a magnetic base layer, 2 is a thermomagnetic recording layer, 3 is a dot-shaped heat input region, and 4 is a previously formed background magnetization.

磁気潜像担体は矢印8の向きで移動する。移動はステ、
ピンダモータを使って間欠的Gこ行才〕れても、連続的
に行われてもよい。まず第2図(、)に示したように、
外部磁界7の印加のもとで、5−aのように熱磁化する
The magnetic latent image carrier moves in the direction of arrow 8. Move to Ste.
G may be performed intermittently using a pin motor or continuously. First, as shown in Figure 2 (,),
Under the application of an external magnetic field 7, it becomes thermally magnetized as shown in 5-a.

続いて、第21図(b)に示す状態に移る。この時磁気
潜像担体は第2図一点鎖線9で示さり、るような軌跡を
えかく。一方(b)では外部磁界の向きが7′のように
反転され、熱残留磁化は5−bのように5−aとは逆向
きになる。
Subsequently, the state shifts to the state shown in FIG. 21(b). At this time, the magnetic latent image carrier traces a trajectory as shown by the dashed line 9 in FIG. On the other hand, in (b), the direction of the external magnetic field is reversed as shown in 7', and the thermal residual magnetization becomes opposite to that in 5-a, as shown in 5-b.

以下、(c) 、(d)に示すように外部磁界の向きの
反転を繰り返す事により、磁気潜像担体には5−a、 
5−b、 5−cのような磁気潜像が形成される。この
場合、磁気潜像形成の最終段階では〔第2図(d) )
 、背景部と同方向の熱磁化が残留f6ようなサイクル
である必要がある。
Hereinafter, as shown in (c) and (d), by repeatedly reversing the direction of the external magnetic field, the magnetic latent image carrier has 5-a,
Magnetic latent images such as 5-b and 5-c are formed. In this case, in the final stage of magnetic latent image formation [Figure 2 (d)]
, the cycle must be such that the thermal magnetization in the same direction as the background part remains f6.

従って、例えば第2図に示すように5−a、5−b、5
−cの磁化反転で磁気潜像を形成する場合には第1加熱
サイクルを背景部と逆向きの磁化ができるように揃える
ならば、必ず4回の加熱サイクルが必要である。
Therefore, for example, as shown in FIG.
In the case of forming a magnetic latent image by magnetization reversal of -c, four heating cycles are always required if the first heating cycle is aligned so that magnetization is in the opposite direction to the background part.

1加熱サイクルで形成される磁化の長さく5−息又は5
−b又は5−c)の整数倍が1つの磁気潜像単位となる
が、磁気潜像単位は任意の倍数(一般に奇数)の磁化長
さで形成される。従って、ソリッド画像は十分大きな磁
化長さの倍数から成る磁気潜像単位から成り、ソリッド
中でも、自由空間中に磁化長さを基本(り返しとする磁
界が発生するので均一な磁性トナー、磁性インクの付着
が可能となる。
The length of magnetization formed in one heating cycle is 5-breath or 5
An integral multiple of -b or 5-c) constitutes one magnetic latent image unit, and a magnetic latent image unit is formed with an arbitrary multiple (generally an odd number) of magnetization length. Therefore, a solid image consists of a magnetic latent image unit consisting of a sufficiently large multiple of the magnetization length, and even in a solid, a magnetic field is generated in free space with the magnetization length basically (repetitively), so uniform magnetic toner and magnetic ink are generated. can be attached.

l加熱サイクルで形成される磁化長さは磁気潜像担体の
送り速度で決定する事ができるが、ソリッドやドツトの
均一な再現性が確保されるよう任意に選択される。
The length of magnetization formed in one heating cycle can be determined by the feeding speed of the magnetic latent image carrier, and is arbitrarily selected so as to ensure uniform reproducibility of solids and dots.

顕像化手段として、平均粒径10μm程度の磁性トナー
粒子を用いる場合には前記の磁化憂さは5μm乃至は2
00μm1好ましくは30μm乃至120μm程度であ
る。すなわち一般に顕像化粒子の平均粒径をdとすると
、前期磁化長さはd/2乃至20d程度にする事が好ま
しい。
When using magnetic toner particles with an average particle diameter of about 10 μm as the visualization means, the magnetization depth is 5 μm to 2 μm.
00 μm1 is preferably about 30 μm to 120 μm. That is, in general, if the average particle diameter of the visualization particles is d, it is preferable that the initial magnetization length is about d/2 to 20 d.

次に実施例により本発明の磁気潜像形成方法を説明する
Next, the method for forming a magnetic latent image of the present invention will be explained with reference to Examples.

実施例 磁気潜像担体として市販の二酸化クロムテープ(米国D
upou’を社製商品名CROLYN )を用いた。こ
のテープの磁性体層を市販のサーマルヘッド(富士ゼロ
ックス社製テレコピア490用ン10に接触するように
配置し、二酸化クロムテープを介しサーマルヘッド10
と対向する位置に30tynのトラック幅を有し、ギャ
ップ長さが200μmのセンダスト長尺磁気ヘッド(巻
数300ターン)11を配置した(第3図(a)参照)
Examples Commercially available chromium dioxide tape (US D
Upou' (trade name: CROLYN) was used. The magnetic layer of this tape was placed in contact with a commercially available thermal head (Telecopier 490 manufactured by Fuji Xerox Co., Ltd.), and the thermal head 10 was placed through the chromium dioxide tape.
A Sendust long magnetic head (number of turns: 300 turns) 11 having a track width of 30 tin and a gap length of 200 μm was placed at a position facing the magnetic head (see Fig. 3(a)).
.

永久磁石(図示せず)により、磁気テープを予め一方向
iこ均一に磁化した後、サーマルヘッドで加熱すると共
に(加熱巾約160μm)磁気テープの磁化方向と逆向
きの磁化方向となる様、磁気ヘッドにより磁化し、約1
60μmの反転磁化部を形成した〔第2図(a)〕。
After uniformly magnetizing the magnetic tape in one direction with a permanent magnet (not shown), it is heated with a thermal head (heating width of about 160 μm) so that the magnetization direction is opposite to that of the magnetic tape. Magnetized by a magnetic head, approximately 1
A reverse magnetization part of 60 μm was formed [FIG. 2(a)].

次いで磁気テープのみを30μm移動させた後再びサー
マルヘッドで加熱すると共に磁気ヘッドによる磁界を前
の磁化と逆向きの熱残留磁化を形成する向き、即ち均一
磁化と同方向にして磁化し、30μmの反転磁化部を形
成した〔第2図(b)〕。
Next, after moving only the magnetic tape by 30 μm, it is heated again with a thermal head, and the magnetic field by the magnetic head is magnetized in a direction that forms thermal remanent magnetization in the opposite direction to the previous magnetization, that is, in the same direction as uniform magnetization. A reverse magnetization portion was formed [FIG. 2(b)].

更ζこ磁気テープのみを30μm移動させた後、再びサ
ーマルヘッドで加熱すると共に前の磁化と逆向き即ち均
一磁化と逆方向に磁化し、第2図(c)に示す磁化パタ
ーンを形成した。最後に、同様に磁気テープのみを30
μm移動させた後、加熱と共に前の磁化と逆向き即ち均
一磁化と同方向に磁化し、第2図(d)に示す磁化反転
単位30μmの磁化パターンが形成された。即ち予め一
方向に均一磁化された磁気テープを加熱、逆方向磁化し
た後、磁気テープを30μm移動させる毎に、加熱する
と共に外部磁界を均一磁化と同方向、逆方向、同方向に
逆転させ、4回の加熱サイクル及び4回の磁化反転を行
ない、磁化反転単位30μmを有する磁気潜像単位長9
0μmの磁気潜像を形成した。この磁気潜像を一成分磁
性トナーにより磁気ブラシ現像し、転写紙に転写後定着
したところ約100μm巾の線巾、濃度共均−な横線を
再現することができた。
After moving only the magnetic tape by 30 μm, it was heated again with a thermal head and magnetized in the opposite direction to the previous magnetization, that is, in the opposite direction to the uniform magnetization, to form the magnetization pattern shown in FIG. 2(c). Finally, in the same way, only the magnetic tape was used for 30 minutes.
After being moved by .mu.m, it was heated and magnetized in the opposite direction to the previous magnetization, that is, in the same direction as the uniform magnetization, forming a magnetization pattern with a magnetization reversal unit of 30 .mu.m as shown in FIG. 2(d). That is, after heating a magnetic tape that has been uniformly magnetized in one direction in advance and magnetizing it in the opposite direction, every time the magnetic tape is moved by 30 μm, the external magnetic field is heated and reversed to the same direction, the opposite direction, or the same direction as the uniform magnetization. Four heating cycles and four magnetization reversals were performed to form a magnetic latent image unit length 9 having a magnetization reversal unit of 30 μm.
A magnetic latent image of 0 μm was formed. When this magnetic latent image was developed with a magnetic brush using a one-component magnetic toner, transferred and fixed on transfer paper, it was possible to reproduce horizontal lines with a width of about 100 μm and uniform density.

同様に種々の単位長の磁気潜像を形成する為、加熱サイ
クル数及び送り長さを異ならせて実験を行なった。すな
わち、以下の表に示した組合わせで磁気潜像形成すると
共に、比較例として分割印字をしない、すなわち長−尺
磁気ヘッドからは一方向の磁界を印加する従来方法ζこ
よっても磁気潜像を形成した。
Similarly, in order to form magnetic latent images of various unit lengths, experiments were conducted by varying the number of heating cycles and feeding length. That is, in addition to forming a magnetic latent image using the combinations shown in the table below, as a comparative example, the conventional method of not performing divided printing, that is, applying a magnetic field in one direction from a long magnetic head, results in the formation of a magnetic latent image. was formed.

丈−マルヘッドは発熱体長さく第1図及び第2図中3)
が約160μmであり、磁気m像担体送り方向と直交す
る方向3tynに亘り同一の信号を印加した。
Length - The round head is the length of the heating element (3) in Figures 1 and 2.
was approximately 160 μm, and the same signal was applied over 3 tyn in a direction orthogonal to the magnetic image carrier feeding direction.

従来方式の場合には、磁気潜像単位の最小長さは丈−マ
ルヘッドの加熱ドツト長(160μm)であるので16
0μmX3cmの横線(加熱サイクル数l)、320μ
fnX311ffMの横線(加熱サイクル数2、送り1
60μm )、480/1m X 3 cmの横線(1
60μm加熱、160μm非加熱、160μm加熱;加
熱サイクル数2、送り320μm)、−、−3cIlt
X 36Nソリツド((160μm加熱、160μm非
加熱)×94、加熱サイクル数94、送り320μm)
の潜像を形成した。これを平均粒径10μmの電子写真
用−成分磁性トナーで現像した。これらの結果を表に記
す。
In the case of the conventional method, the minimum length of the magnetic latent image unit is 160 μm since it is the length of the heating dot of the long head (160 μm).
0 μm x 3 cm horizontal line (number of heating cycles 1), 320 μ
Horizontal line of fnX311ffM (number of heating cycles 2, feed 1
60μm), 480/1m x 3cm horizontal line (1
60μm heating, 160μm non-heating, 160μm heating; number of heating cycles: 2, feed: 320μm), -, -3cIlt
X 36N solid ((160μm heated, 160μm unheated) x 94, number of heating cycles 94, feed 320μm)
A latent image was formed. This was developed with an electrophotographic component magnetic toner having an average particle size of 10 μm. These results are shown in the table.

なお上記の実施例においては外部磁界印加を磁気ヘッド
により行う場合について説明したが、第4図に示すよう
に永久磁石を用いることもできる。
In the above embodiment, a case has been described in which the external magnetic field is applied by a magnetic head, but a permanent magnet may also be used as shown in FIG. 4.

図中、15はシリコーンゴム等の弾性体被覆であって、
サーマルヘッドと磁性体との密着を補助する。中空シリ
ンダー16中では、対称に着磁された円筒形永久磁石ロ
ールが一定速度で回転する。
In the figure, 15 is an elastic covering such as silicone rubber,
Assists in the close contact between the thermal head and the magnetic material. In the hollow cylinder 16, a symmetrically magnetized cylindrical permanent magnet roll rotates at a constant speed.

この永久磁石ロールには、ホール素子などの磁束検出手
段を設けて前磁化と逆向きの印加磁界となる加熱イネー
ブル(クロック)スタートのタイミング制御、十H,−
Hの印加磁界が熱残留磁化するのに十分な値になるスラ
イスレベル検出と加熱イネーブル制御、磁性体の送りタ
イミングを決定するクロック発生制御を行なう。
This permanent magnet roll is provided with a magnetic flux detection means such as a Hall element to control the timing of the heating enable (clock) start, which applies a magnetic field in the opposite direction to that of pre-magnetization.
Slice level detection and heating enable control are performed so that the applied magnetic field of H has a value sufficient to cause thermal residual magnetization, and clock generation control is performed to determine the feeding timing of the magnetic body.

この外部磁化印加方法によれば磁気ヘッドにより較べて
サーマルヘッドと磁界印加手段の位置合わせ精度が軽減
される。
According to this external magnetization application method, the alignment accuracy between the thermal head and the magnetic field application means is reduced compared to a magnetic head.

発明の詳細 な説明したように本発明は丈−マルヘッドやレーザー光
などによるドツト状の熱入力を磁気潜像担体上で空間的
に重なるように印加し、熱入力印加と同期して外部印加
磁界の向きを逆転する事によって行う磁気潜像形成法を
提供したものであり、ソリッドが均一に再現されること
、熱入力ドツトの大きさよりも小さな磁気潜像単位が形
成できることなどの特長を有する、ものである。
As described in detail, the present invention applies a dot-shaped thermal input using a long head or a laser beam so as to spatially overlap on a magnetic latent image carrier, and synchronizes with the application of the thermal input by applying an externally applied magnetic field. This method provides a method of forming a magnetic latent image by reversing the direction of the dot, and has the features of uniformly reproducing a solid and being able to form a magnetic latent image unit smaller than the size of the heat input dot. It is something.

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

第1図(a)及び(b)は従来の熱による磁気潜像形成
方法の説明図、第2図(、)〜(d)は本発明の磁気潜
像形成方法の説明図、第3図(a)、(b)及び第4図
(a)、(b)は外部磁界印加手段としてそれぞれ磁気
ヘッド及び永久磁石を使った実施例の構成図と制御の概
要図である。 図中符号: l・・・支持体層;2・・・磁性体Pi: 3・・・加
熱ドツト部;4・・・背景部磁化;5・・・潜像磁化′
、6・・・磁性トナー;7・・・外部磁界;7′・・・
反転外部磁界;8・・・移動方向;9・・・移動軌跡;
10・・・サーマルヘッド;11・・・長尺磁気ヘッド
;12・・・長尺磁気ヘッドドライブ電流;13・・・
サーマルヘッド加熱イネーブル;14・・・磁気m像担
体送り信号;15・・・弾性被覆体層:16・・・中空
支持体;17・−・永久磁石ロール;18・・・磁界検
出手段。 111 図 第 2 図 第 3 図
FIGS. 1(a) and (b) are explanatory diagrams of a conventional method for forming a magnetic latent image using heat; FIGS. 2(a) to (d) are explanatory diagrams of a method for forming a magnetic latent image according to the present invention; FIG. (a), (b) and FIG. 4 (a), (b) are block diagrams and schematic diagrams of control of an embodiment using a magnetic head and a permanent magnet as external magnetic field applying means, respectively. Symbols in the figure: l... Support layer; 2... Magnetic material Pi: 3... Heating dot part; 4... Background magnetization; 5... Latent image magnetization'
, 6... Magnetic toner; 7... External magnetic field; 7'...
Reversal external magnetic field; 8...Movement direction; 9...Movement trajectory;
10... Thermal head; 11... Long magnetic head; 12... Long magnetic head drive current; 13...
Thermal head heating enable; 14...Magnetic image carrier feeding signal; 15...Elastic coating layer; 16...Hollow support; 17...Permanent magnet roll; 18...Magnetic field detection means. 111 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] 支持体上に熱残留磁化可能な磁気層を有する磁気記録体
を画像状に加熱すると共に磁界を作用させて磁気潜像を
形成する方法において、画像状に加熱する毎に磁界の向
きを逆転させることを特徴とする磁気潜像形成方法。
A method of forming a magnetic latent image by imagewise heating a magnetic recording body having a magnetic layer capable of thermoremanent magnetization on a support and applying a magnetic field, in which the direction of the magnetic field is reversed each time it is imagewise heated. A method for forming a magnetic latent image, characterized in that:
JP16316383A 1983-09-07 1983-09-07 Formation of magnetic latent image Pending JPS6055377A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16316383A JPS6055377A (en) 1983-09-07 1983-09-07 Formation of magnetic latent image

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16316383A JPS6055377A (en) 1983-09-07 1983-09-07 Formation of magnetic latent image

Publications (1)

Publication Number Publication Date
JPS6055377A true JPS6055377A (en) 1985-03-30

Family

ID=15768427

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16316383A Pending JPS6055377A (en) 1983-09-07 1983-09-07 Formation of magnetic latent image

Country Status (1)

Country Link
JP (1) JPS6055377A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57176080A (en) * 1981-04-21 1982-10-29 Iwatsu Electric Co Ltd Method and device for forming latent image
JPS589176A (en) * 1981-07-10 1983-01-19 Fuji Xerox Co Ltd Magnetic recording medium
JPS5811178A (en) * 1981-07-15 1983-01-21 Fuji Xerox Co Ltd Magnetic recording method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57176080A (en) * 1981-04-21 1982-10-29 Iwatsu Electric Co Ltd Method and device for forming latent image
JPS589176A (en) * 1981-07-10 1983-01-19 Fuji Xerox Co Ltd Magnetic recording medium
JPS5811178A (en) * 1981-07-15 1983-01-21 Fuji Xerox Co Ltd Magnetic recording method

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