JP2510292B2 - Laser printing method for magnetic recording media - Google Patents

Laser printing method for magnetic recording media

Info

Publication number
JP2510292B2
JP2510292B2 JP1215643A JP21564389A JP2510292B2 JP 2510292 B2 JP2510292 B2 JP 2510292B2 JP 1215643 A JP1215643 A JP 1215643A JP 21564389 A JP21564389 A JP 21564389A JP 2510292 B2 JP2510292 B2 JP 2510292B2
Authority
JP
Japan
Prior art keywords
magnetic recording
printing
laser
recording medium
laser printing
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 - Lifetime
Application number
JP1215643A
Other languages
Japanese (ja)
Other versions
JPH0379361A (en
Inventor
正一 長村
孝好 林
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP1215643A priority Critical patent/JP2510292B2/en
Publication of JPH0379361A publication Critical patent/JPH0379361A/en
Application granted granted Critical
Publication of JP2510292B2 publication Critical patent/JP2510292B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Laser Beam Processing (AREA)
  • Manufacturing Of Magnetic Record Carriers (AREA)
  • Lasers (AREA)
  • Dot-Matrix Printers And Others (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明はコンピュータの外部記憶装置であるハード
デイスク装置等に使用される磁気記録媒体のレーザ印字
方法に関する。
The present invention relates to a laser printing method for a magnetic recording medium used in a hard disk device or the like which is an external storage device of a computer.

〔従来の技術〕[Conventional technology]

レーザ光を用いて金属等へ印字する方法は一般的に知
られている。レーザ印字は例えばYAGレーザ光をパルス
状に照射して所定のパルス周波数,印字速度で数字,記
号等を刻印する。所定ランプ電流がクリプトンランプに
流され、クリプトンランプの光によってイツトリウムア
ルミニウムガーネツト結晶が励起され、レーザ光を発振
する。1.06μmのYAGレーザ光はパルス状に照射されて
第3図に示すようにX−Y軸偏光ミラーによりX−Y方
向に走査される。レーザ光は例えばAl基板上にNi−P
層,Cr層,Co合金層,カーボン層の積層された磁気記録媒
体に照射され印字が行われる。媒体はNi−P層を形成し
たあとで研磨され媒体表面は平均あらさRa 0.1μm最大
あらさRmax 0.8μm位になっている。
A method of printing on a metal or the like using laser light is generally known. Laser printing is performed by, for example, irradiating a pulse of YAG laser light to engrave numbers, symbols, etc. at a predetermined pulse frequency and printing speed. A predetermined lamp current is passed through the krypton lamp, the yttrium aluminum garnet crystal is excited by the light of the krypton lamp, and oscillates a laser beam. A 1.06 μm YAG laser beam is applied in a pulsed form and scanned in the XY directions by an XY axis polarization mirror as shown in FIG. The laser light is, for example, Ni-P on the Al substrate.
Printing is performed by irradiating a magnetic recording medium in which a layer, a Cr layer, a Co alloy layer, and a carbon layer are laminated. The medium is polished after forming a Ni-P layer, and the surface of the medium has an average roughness Ra of 0.1 μm and a maximum roughness Rmax of 0.8 μm.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

しかしながらこのレーザ印字を磁気記録媒体に適用す
る場合には次に述べるような問題点があった。即ちレー
ザ印字は磁気記録媒体のクランピング領域に行われるが
その場合レーザ照射時の発熱により磁気記録媒体の表面
平滑性やクランピング領域の耐食性が損われる。例えば
クランピング領域において刻印部からバリを発生し媒体
をそのクランピング領域を介してスペーサによりハード
デイスク装置に装着する場合に磁気記録媒体の基板が変
形しあるいは媒体回転時に面振れが発生する。また磁気
記録媒体はAl基板上に無電解メッキによりNi−P非磁性
層が形成されるが、この非磁性層がレーザ照射時の発熱
により再結晶して結晶粒が大きくなり耐食性が低下す
る。クランピング領域に発生したNi−Pの腐食は進行し
て記録層に達し入力情報を損傷する。
However, when this laser printing is applied to a magnetic recording medium, there are the following problems. That is, laser printing is performed on the clamping area of the magnetic recording medium, in which case the surface smoothness of the magnetic recording medium and the corrosion resistance of the clamping area are impaired by the heat generated during laser irradiation. For example, burrs are generated from the marking portion in the clamping area, and when the medium is mounted on the hard disk device by the spacer through the clamping area, the substrate of the magnetic recording medium is deformed or surface wobbling occurs when the medium rotates. Further, in the magnetic recording medium, a Ni-P non-magnetic layer is formed on the Al substrate by electroless plating, but this non-magnetic layer is recrystallized by heat generated during laser irradiation, resulting in large crystal grains and reduced corrosion resistance. Corrosion of Ni-P generated in the clamping area progresses to reach the recording layer and damage the input information.

この発明は上述の点に鑑みてなされその目的はレーザ
印字の際の条件設定を最適にして信頼性に優れる磁気記
録媒体を得ることが可能なレーザ印字方法を提供するこ
とにある。
The present invention has been made in view of the above points, and an object thereof is to provide a laser printing method capable of obtaining a magnetic recording medium having excellent reliability by optimizing the condition setting in laser printing.

〔課題を解決するための手段〕[Means for solving the problem]

本発明者等は磁気記録媒体のレーザ印字について鋭意
研究を重ねた結果、媒体の表面あらさが光反射率を大き
く左右することを見出し、この知見に基いて本発明をな
すに至った。
As a result of intensive studies on the laser printing of a magnetic recording medium, the present inventors have found that the surface roughness of the medium has a great influence on the light reflectance, and have completed the present invention based on this finding.

上述の目的は、この発明によれば、クリプトンランプ
にランプ電流を流してYAGレーザパルスを所定の印字速
度で照射することにより磁気記録媒体に印字する方法で
あって、前記YAGレーザパルスのパルス周波数を16〜20k
Hzの範囲内に設定し、前記ランプ電流を10〜14Aの範囲
内に設定し、前記印字速度を100〜200mm/sの範囲内に設
定することにより達成される。
According to the present invention, the above-mentioned object is a method of printing on a magnetic recording medium by applying a lamp current to a krypton lamp and irradiating a YAG laser pulse at a predetermined printing speed, and a pulse frequency of the YAG laser pulse. 16-20k
It is achieved by setting within the range of Hz, the lamp current within the range of 10 to 14 A, and the printing speed within the range of 100 to 200 mm / s.

〔作用〕[Action]

レーザ印字の最適条件を満足するときは磁気記録媒体
の表面層が溶融して初期の媒体表面あらさが平滑化され
る。
When the optimum conditions for laser printing are satisfied, the surface layer of the magnetic recording medium is melted and the initial surface roughness of the medium is smoothed.

〔実施例〕〔Example〕

次にこの発明の実施例を図面に基いて説明する。第1
図はレーザ周波数(kHz)と刻印部の表面あらさとの関
係を示す線図である。こは磁気記録媒体のクランピング
領域の表面であるカーボン層に0.3mm巾の直線をレーザ
印字し、直線に直角方向に1mmの間を走査して、その領
域の表面あらさ(Rmax,Ra)を測定したものである。Rma
xはあらさの最大値であり、Raは平均値である。印字速
度は50mm/s、ランプ電流は10Aと14Aに設定した。ランプ
電流は10Aより小さいときは印字が不能であるので最小
値として10Aが選定される。曲線11と曲線12はRa(μ
m)に対応し、曲線13と曲線14はRmax(μm)に対応す
る。また曲線11の曲線13はランプ電流14A,曲線12と曲線
14はランプ電流10Aの場合である。YAGレーザパルスのパ
ルス周波数が増すにつれ平均あらさと最大あらさが共に
初期の値よりも減少していることがわかる。これはレー
ザ印字の際の発熱によって媒体表面が溶融し、表面平滑
性が増したことを意味する。そのために平滑化されたカ
ーボン層から光照射率が増大し刻印された印字を明瞭に
区別することができる。磁気記録媒体の場合はレーザ印
字によってカーボン層がこげ茶色より銀白色へと変化す
る。周波数を20kHzを越えて30kHzにすると、印字の際の
発熱量が大き過ぎて、刻印吹からバリが発生したり、Ni
−P層が腐食を示すようになる。ランプ電流が14Aを越
えるとRmax,Raともに大きくなるのでランプ電流として
は10〜14Aが適当である。また周波数の範囲としては16
〜20kHzがRmaxとRaが小さく適当である。
Next, an embodiment of the present invention will be described with reference to the drawings. First
The figure is a diagram showing the relationship between the laser frequency (kHz) and the surface roughness of the marking portion. This laser prints a 0.3 mm wide straight line on the carbon layer, which is the surface of the clamping area of the magnetic recording medium, and scans 1 mm in the direction perpendicular to the straight line to determine the surface roughness (Rmax, Ra) of that area. It was measured. Rma
x is the maximum value of roughness and Ra is the average value. The printing speed was set to 50 mm / s and the lamp current was set to 10A and 14A. When the lamp current is less than 10A, printing is impossible, so 10A is selected as the minimum value. Curves 11 and 12 are Ra (μ
m) and curves 13 and 14 correspond to Rmax (μm). Curve 11 of curve 11 is lamp current 14A, curve 12 and curve
14 is for a lamp current of 10A. It can be seen that both the average roughness and the maximum roughness decrease from the initial values as the pulse frequency of the YAG laser pulse increases. This means that the surface of the medium was melted by the heat generated during the laser printing and the surface smoothness was increased. Therefore, the light irradiation rate is increased from the smoothed carbon layer, and it is possible to clearly distinguish the imprinted print. In the case of a magnetic recording medium, the carbon layer changes from dark brown to silvery white by laser printing. If the frequency exceeds 20kHz and becomes 30kHz, the amount of heat generated during printing will be too large, and burrs will occur from the marking and the Ni
The P layer becomes corrosive. When the lamp current exceeds 14A, both Rmax and Ra increase, so 10-14A is suitable as the lamp current. The frequency range is 16
~ 20kHz is suitable because Rmax and Ra are small.

第2図は印字速度と表面あらさとの関係を示す線図で
ある。ランプ電流は10A,周波数は12kHzに設定された。
曲線15は表面あらさRaに対応し曲線16は表面あらさRmax
に対応する。印字速度が増大するにつれ表面平滑性は増
している。印字速度が50mm/sのときに表面平滑性が100
〜200mm/sの印字速度の場合よりわるくなるのは、発熱
が過剰で逆効果になったものと考えられる。印字速度が
200mm/sを越えるときは発熱不足で媒体表面が溶融せず
表面あらさは増大の方向に向かう。従って印字速度とし
ては100〜200mm/sが最適範囲となる。Ni−P層の腐食の
問題は、上記表面あらさの平滑化される条件で解消され
る。最適条件を満足するときは磁気記録媒体を80℃,相
対湿度80%の環境下に1000h放置しても腐食が発生しな
い。
FIG. 2 is a diagram showing the relationship between the printing speed and the surface roughness. The lamp current was set to 10 A and the frequency was set to 12 kHz.
Curve 15 corresponds to surface roughness Ra and curve 16 corresponds to surface roughness Rmax
Corresponding to. The surface smoothness increases as the printing speed increases. Surface smoothness is 100 when printing speed is 50 mm / s
The reason why the print speed becomes worse than the print speed of ~ 200 mm / s is considered to be the excessive heat generation and the adverse effect. Printing speed
When it exceeds 200 mm / s, the heat generation is insufficient and the surface of the medium does not melt and the surface roughness tends to increase. Therefore, the optimum printing speed is 100 to 200 mm / s. The problem of corrosion of the Ni-P layer is solved under the condition that the surface roughness is smoothed. When the optimum conditions are satisfied, corrosion does not occur even if the magnetic recording medium is left for 1000 hours in an environment of 80 ° C and 80% relative humidity.

〔発明の効果〕〔The invention's effect〕

この発明によれば、クリプトンランプにランプ電流を
流してYAGレーザパルスを所定の印字速度で照射するこ
とにより磁気記録媒体に印字する方法であって、前記YA
Gレーザパルスのパルス周波数を16〜20kHzの範囲内に設
定し、前記ランプ電流を10〜14Aの範囲内に設定し、前
記印字速度を100〜200mm/sの範囲内に設定して行うので
磁気記録媒体の初期表面あらさが平滑化され、光反射率
が増大して従来の印字とは異なる原理で刻印部の識別が
可能となるのみならず、Ni−Pの腐食の問題や媒体基板
の変形等の問題が解消され、信頼性に優れる磁気記録媒
体が得られる。
According to the present invention, there is provided a method of printing on a magnetic recording medium by passing a lamp current through a krypton lamp and irradiating a YAG laser pulse at a predetermined printing speed, wherein the YA
The pulse frequency of the G laser pulse is set within the range of 16 to 20 kHz, the lamp current is set within the range of 10 to 14 A, and the printing speed is set within the range of 100 to 200 mm / s. The initial surface roughness of the recording medium is smoothed, the light reflectance is increased, and the marking part can be identified by a principle different from the conventional printing. In addition, the problem of Ni-P corrosion and the deformation of the medium substrate It is possible to obtain a magnetic recording medium having excellent reliability by solving the above problems.

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

第1図はレーザ印字方法につき周波数と表面あらさとの
関係を示す線図、第2図はレーザ印字方法につき印字速
度と表面あらさとの関係を示す線図、第3図はレーザ印
字装置の原理図である。
FIG. 1 is a diagram showing the relationship between frequency and surface roughness for the laser printing method, FIG. 2 is a diagram showing the relationship between printing speed and surface roughness for the laser printing method, and FIG. 3 is the principle of the laser printing device. It is a figure.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】クリプトンランプにランプ電流を流してYA
Gレーザパルスを所定の印字速度で照射することにより
磁気記録媒体に印字する方法であって、前記YAGレーザ
パルスのパルス周波数を16〜20kHzの範囲内に設定し、
前記ランプ電流を10〜14Aの範囲内に設定し、前記印字
速度を100〜200mm/sの範囲内に設定することを特徴とす
る磁気記録媒体のレーザ印字方法。
1. A lamp current is applied to a krypton lamp to YA.
A method of printing on a magnetic recording medium by irradiating a G laser pulse at a predetermined printing speed, wherein the pulse frequency of the YAG laser pulse is set within a range of 16 to 20 kHz,
A laser printing method for a magnetic recording medium, wherein the lamp current is set within a range of 10 to 14 A, and the printing speed is set within a range of 100 to 200 mm / s.
JP1215643A 1989-08-22 1989-08-22 Laser printing method for magnetic recording media Expired - Lifetime JP2510292B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1215643A JP2510292B2 (en) 1989-08-22 1989-08-22 Laser printing method for magnetic recording media

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1215643A JP2510292B2 (en) 1989-08-22 1989-08-22 Laser printing method for magnetic recording media

Publications (2)

Publication Number Publication Date
JPH0379361A JPH0379361A (en) 1991-04-04
JP2510292B2 true JP2510292B2 (en) 1996-06-26

Family

ID=16675805

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1215643A Expired - Lifetime JP2510292B2 (en) 1989-08-22 1989-08-22 Laser printing method for magnetic recording media

Country Status (1)

Country Link
JP (1) JP2510292B2 (en)

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
レーザー応用技術ハンドブック第196ページ及び第197ページ1984年3月10日初版第1刷編集レーザ協会発行朝倉書店

Also Published As

Publication number Publication date
JPH0379361A (en) 1991-04-04

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