JP2727232B2 - Magneto-optical recording medium and method of manufacturing the same - Google Patents

Magneto-optical recording medium and method of manufacturing the same

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Publication number
JP2727232B2
JP2727232B2 JP1146568A JP14656889A JP2727232B2 JP 2727232 B2 JP2727232 B2 JP 2727232B2 JP 1146568 A JP1146568 A JP 1146568A JP 14656889 A JP14656889 A JP 14656889A JP 2727232 B2 JP2727232 B2 JP 2727232B2
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JP
Japan
Prior art keywords
dielectric film
based dielectric
target material
magneto
optical 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.)
Expired - Fee Related
Application number
JP1146568A
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Japanese (ja)
Other versions
JPH0312841A (en
Inventor
伸 浅利
久三 中村
敬司 宮本
賀文 太田
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.)
Ulvac Inc
Original Assignee
Nihon Shinku Gijutsu KK
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Priority to JP1146568A priority Critical patent/JP2727232B2/en
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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、Si系誘電体を磁性膜の片面或いは両面にエ
ンハンス膜および保護膜として被膜した光磁気記録体お
よびその製造方法に関する。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magneto-optical recording medium in which a Si-based dielectric is coated on one or both sides of a magnetic film as an enhancement film and a protective film, and a method for manufacturing the same.

(従来の技術) 従来、この種の光磁気記録体として、例えばTbFeCoか
ら成る磁性膜の片面或いは両面にSiNX、SiOX、SiNXOY
の透明でかつ屈折率の高いSi系誘電体膜を被膜したもの
は知られている。
(Prior art) Conventionally, as this type of magneto-optical recording material, a transparent and high-refractive-index Si-based dielectric material such as SiN x , SiO x , SiN x O y is provided on one or both sides of a magnetic film made of, for example, TbFeCo. Coated films are known.

また、該光磁気記録体の製造方法として、Si系ターゲ
ット材を用い例えばN2のような反応ガスを含む雰囲気中
で該ターゲット材を反応性スパッタ法によりスパッタ
し、スパッタされたターゲット材を反応ガスと反応させ
て例えばSiNXから成る磁性膜の片面或いは両面にSi系誘
電体膜を形成する方法が知られている。
Further, as a method for manufacturing a magneto-optical recording medium, the target material is sputtered by reactive sputtering in an atmosphere containing a reactive gas such as using a Si-based target for example N 2, the reaction of the sputtered target material It is known to form a Si-based dielectric film on one or both sides of a magnetic film made of, for example, SiN X by reacting with a gas.

(発明が解決しようとする課題) Si系誘電体膜の内部応力の大きさは該Si系誘電体のチ
ルト角に影響を与え、内部応力が高い程該チルト角は大
きくなる。また、チルト角が大きいとヘッドのサーボ不
良や信号の誤読等の原因となる。
(Problems to be Solved by the Invention) The magnitude of the internal stress of the Si-based dielectric film affects the tilt angle of the Si-based dielectric, and the higher the internal stress, the larger the tilt angle. In addition, a large tilt angle causes a servo failure of the head and erroneous reading of a signal.

しかしながら、前記方法で成膜されたSi系誘電体膜は
一般に高純度であるので、高い内部応力を有することと
なり、その結果該チルト角が大きくなってヘッドのサー
ボ不良や信号の誤読等が生じる等の問題がある。
However, since the Si-based dielectric film formed by the above method is generally of high purity, it has a high internal stress, and as a result, the tilt angle becomes large, causing a servo failure of the head or erroneous reading of a signal. There are problems such as.

また、形成される膜の内部応力が大きいとスパッタ中
に成膜装置内のカソード等の周辺に付着したターゲット
材料が剥離しやすくなり、該ターゲット材料が成膜中に
成膜装置内に飛散し、これが基板上に成膜中のSi系誘電
体膜に付着したりしてダストの原因となる等の問題があ
る。
Further, if the internal stress of the film to be formed is large, the target material attached to the periphery of the cathode or the like in the film forming apparatus during sputtering is likely to peel off, and the target material is scattered into the film forming apparatus during film formation. However, there is a problem that this adheres to the Si-based dielectric film being formed on the substrate and causes dust.

そこで内部応力の低いSi系誘電体膜を備えた光磁気記
録体が要望されていた。
Therefore, a magneto-optical recording medium provided with a Si-based dielectric film having low internal stress has been demanded.

本発明は内部応力の低いSi系誘電体膜を備えた光磁気
記録体およびその製造方法を提供することを目的とす
る。
SUMMARY OF THE INVENTION An object of the present invention is to provide a magneto-optical recording medium having a Si-based dielectric film having a low internal stress and a method for manufacturing the same.

(課題を解決するための手段) 本発明者らは、前記目的を達成すべく鋭意検討した結
果、Si系誘電体膜に不純物を混入することにより内部応
力が低減することを知見した。
(Means for Solving the Problems) As a result of intensive studies to achieve the above object, the present inventors have found that the internal stress is reduced by mixing impurities into the Si-based dielectric film.

本発明の光磁気記録体は、前記知見に基づいてなされ
たものであって、磁性膜の片面或いは両面に形成された
Si系誘電体膜中にPを1014atoms/cm3以上含有せしめた
ことを特徴とする。
The magneto-optical recording medium of the present invention is based on the above findings, and is formed on one side or both sides of a magnetic film.
It is characterized in that P is contained in a Si-based dielectric film at 10 14 atoms / cm 3 or more.

本発明においてSi系誘電体膜中のPの含有量を1014at
oms/cm3以上としたのは、Pの含有量が1014atoms/cm3
満たない場合は、該膜の内部応力の低下効果が得られな
いからである。
In the present invention, the content of P in the Si-based dielectric film is set to 10 14 at.
The reason for setting it to oms / cm 3 or more is that if the P content is less than 10 14 atoms / cm 3 , the effect of lowering the internal stress of the film cannot be obtained.

また、光磁気記録体の製造方法は、Si系ターゲット材
を用い、反応性スパッタ法により磁性膜の片面或いは両
面にSi系誘電体膜を形成する方法において、該Si系ター
ゲット材としてPを1014atoms/cm3以上ドープしたSi系
ターゲット材を用いることを特徴とする。
Further, a method for manufacturing a magneto-optical recording medium is a method of forming a Si-based dielectric film on one or both sides of a magnetic film by a reactive sputtering method using a Si-based target material. It is characterized by using a Si-based target material doped with 14 atoms / cm 3 or more.

本発明法で用いるPドープされたSi系ターゲット材は
Si単独ターゲット材、或いはSiに例えばAl等を添加した
ターゲット材に公知の溶解法によりPをドープすればよ
く、該ターゲット材へのPドープ量の調整は溶解度で行
えばよく、そのPドープ量は一般に1014〜1020atmos/cm
3程度とする。
The P-doped Si-based target material used in the method of the present invention is
The P material may be doped into the Si target material or the target material obtained by adding Al or the like to Si by a known dissolving method, and the P doping amount in the target material may be adjusted by the solubility. Is generally 10 14 to 10 20 atmos / cm
About 3

また、反応性スパッタ法としては、N2ガス、O2ガス、
N2+O2ガス等の反応性スパッタガスを用いたRFスパッタ
法、DCスパッタ法等が挙げられる。そして前記ターゲッ
ト材をスパッタする際のスパッタガス圧は1×10-3〜1
×10-1Torr程度に設定する。
As the reactive sputtering method, N 2 gas, O 2 gas,
An RF sputtering method and a DC sputtering method using a reactive sputtering gas such as N 2 + O 2 gas are exemplified. The sputtering gas pressure for sputtering the target material is 1 × 10 -3 to 1
Set to about × 10 -1 Torr.

(作 用) Si系誘電体膜中にPを1014atoms/cm3以上含有せしめ
ることによって、PはSiのネットワーク中に入るなどし
て、膜の歪みを緩和して内部応力を低下する。
(Operation) By including P in the Si-based dielectric film at 10 14 atoms / cm 3 or more, P enters into the network of Si, etc., thereby relaxing the strain of the film and lowering the internal stress.

Pが1014atoms/cm3以上ドープされたSi系ターゲット
材を用いることによって反応性スパッタ法により成膜さ
れるSi系誘電体膜中のP含有量を調節する。
By using a Si-based target material doped with P at 10 14 atoms / cm 3 or more, the P content in the Si-based dielectric film formed by the reactive sputtering method is adjusted.

(実施例) 次に本発明の具体的な実施例につき説明する。(Example) Next, a specific example of the present invention will be described.

実験例1 反応ガスとしてN2ガス雰囲気下で、ターゲット材とし
てSi(純度99.999%)にPを1014atoms/cm3、2×1015a
toms/cm3、2×1019atoms/cm3を夫々ドープしたSi系タ
ーゲット材を用い、各ターゲット材をRFスパッタ法によ
りスパッタし、膜厚900ÅのSiNXPY膜(以下Si系誘電体
膜という)を形成して光磁気記録体を作成した。
Experimental Example 1 In a N 2 gas atmosphere as a reaction gas, P was added to Si (purity: 99.999%) as a target material at 10 14 atoms / cm 3 and 2 × 10 15 a.
Each target material is sputtered by an RF sputtering method using a Si-based target material doped with toms / cm 3 and 2 × 10 19 atoms / cm 3 , respectively, and a 900-nm-thick SiN X P Y film (hereinafter referred to as a Si-based dielectric material). A film was formed to form a magneto-optical recording medium.

作成された各Si系誘電体膜中のPの含有量(atoms/cm
3)を二次イオン質量分析法で測定した。得られた結果
を第1図に示す。
The P content (atoms / cm) in each of the formed Si-based dielectric films
3 ) was measured by secondary ion mass spectrometry. The results obtained are shown in FIG.

尚、スパッタガス圧力は1×10-2Torrとし、またスパ
ッタ電力は2.2KWとし、また析出速度は500Å/minとし
た。尚、基板上に形成されるSi系誘電体膜の屈折率nは
2.3となるように調整した。
The sputtering gas pressure was 1 × 10 −2 Torr, the sputtering power was 2.2 KW, and the deposition rate was 500 ° / min. Incidentally, the refractive index n of the Si-based dielectric film formed on the substrate is
Adjusted to 2.3.

第1図から明らかなようにSi系ターゲット材中のPド
ープ量と、基板上に形成されたSi系誘電体膜中のP含有
量とはほぼ同じ値を示している。従って、ターゲット材
中のPドープ量と成膜されたSi系誘電体膜中のP量とは
比例関係にあるので、ターゲット材中のPドープ量によ
り成膜されるSi系誘電体膜中のPの含有量を調節出来る
ことが確認された。
As is clear from FIG. 1, the P doping amount in the Si-based target material and the P content in the Si-based dielectric film formed on the substrate show almost the same value. Therefore, since the amount of P dope in the target material and the amount of P in the formed Si-based dielectric film are in a proportional relationship, the amount of P-doped Si film in the target material is not proportional to the amount of P in the target material. It was confirmed that the P content could be adjusted.

実験例2 前記実験例1で作成した各光磁気記録体の内部応力を
薄いカバーガラス基板の変形を測定することにより測定
した。得られた結果を第2図に示す。
Experimental Example 2 The internal stress of each magneto-optical recording medium prepared in Experimental Example 1 was measured by measuring the deformation of a thin cover glass substrate. The results obtained are shown in FIG.

比較実験例1 ターゲット材にSi(純度99.999%)単独のターゲット
材(Pを全くドープされていないターゲット材)を用い
た以外は前記実験例1と同様の方法でSi系誘電体膜を作
成した。
Comparative Experimental Example 1 An Si-based dielectric film was formed in the same manner as in Experimental Example 1 except that a target material containing only Si (99.999% purity) (a target material not doped with P at all) was used as the target material. .

作成されたPを含まないSi系誘電体膜の内部応力を前
記実験例2と同様の方法で測定した。得られた結果を第
2図に示す。
The internal stress of the prepared Si-based dielectric film not containing P was measured in the same manner as in Experimental Example 2. The results obtained are shown in FIG.

第2図から明らかなようにSi系誘電体膜中にPが1014
atoms/cm3含有されていることによって、従来のPを全
く含有していないSi系誘電体膜の内部応力−3.5×109dy
n/cm2に比して内部応力は−8×108dyn/cm2に減少し、
更にP含有量が増加するに伴って該内部応力も減少傾向
を示し、またP含有量が1015atoms/cm3以上に達すると
該内部応力はほぼ一定状態となる傾向を示した。特にSi
系誘電体膜中にPを5×1015atoms/cm3含有させること
によって従来のPを全く含まないSi系誘電体膜に比して
内部応力が1桁以上減少した。従って、Si系誘電体膜中
にPを1014atoms/cm3以上含有させることによって該膜
の内部応力が減少することが確認された。
As is apparent from FIG. 2, P is 10 14 in the Si-based dielectric film.
By containing atoms / cm 3, the internal stress of the conventional Si-based dielectric film containing no P at all -3.5 × 10 9 dy
The internal stress is reduced to −8 × 10 8 dyn / cm 2 compared to n / cm 2 ,
Further, as the P content increased, the internal stress also tended to decrease, and when the P content reached 10 15 atoms / cm 3 or more, the internal stress tended to be substantially constant. Especially Si
By containing 5 × 10 15 atoms / cm 3 of P in the system dielectric film, the internal stress was reduced by one digit or more as compared with the conventional Si system dielectric film containing no P at all. Therefore, it was confirmed that the internal stress of the Si-based dielectric film was reduced by including P at 10 14 atoms / cm 3 or more.

尚、前記SiにPをドープしたターゲット材の代わり
に、Si・AlにPを1015atoms/cm3ドープしたターゲット
材を用いても同様の効果が得られることが確認された。
また、反応スパッタガスをN2ガスに代えてO2ガス、N2
O2ガスを用いても同様の効果が得られることが確認され
た。
It was confirmed that the same effect could be obtained by using a target material in which Si · Al was doped with P at 10 15 atoms / cm 3 instead of the target material in which Si was doped with P.
Further, the reaction sputtering gas in place of the N 2 gas O 2 gas, N 2 +
It was confirmed that the same effect was obtained even when O 2 gas was used.

実験例3 ターゲット材にPを2×1015atoms/cm3ドープしたSi
系ターゲット材を用い、スパッタ法をDCスパッタ法(ス
パッタ電力3KW)とした以外は前記実験例1と同様の方
法で光磁気記録体を作成した。作成された光磁気記録体
のSi系誘電体膜の内部応力を前記実験例2と同様の方法
で測定したところ、該膜の内部応力は−1.6×108dyn/cm
2であった。
Experimental Example 3 Si doped with 2 × 10 15 atoms / cm 3 of P as a target material
A magneto-optical recording medium was prepared in the same manner as in Experimental Example 1 except that a DC sputtering method (sputter power: 3 KW) was used as the sputtering method, using a system target material. When the internal stress of the Si-based dielectric film of the created magneto-optical recording medium was measured by the same method as in Experimental Example 2, the internal stress of the film was −1.6 × 10 8 dyn / cm.
Was 2 .

実験例4 ターゲット材にPを2×1015atoms/cm3ドープしたSi
系ターゲット材を用い、またポリカーボネートから成る
径5.25inchのディスクを用い、該ディスクの片面に膜厚
900ÅのSi系誘電体膜を形成し、その上に膜厚800ÅのTb
FeCoから成る磁性膜を形成し、更に膜厚900ÅのSi系誘
電体膜を形成してディスク媒体を作成した。作成された
ディスク媒体の該Si系誘電体膜のチルト角を測定したと
ころ、3mrad.であった。また、該Si系誘電体膜の内部応
力は−4.2×108dyn/cm2であった。
Experimental Example 4 Si doped with 2 × 10 15 atoms / cm 3 of P as a target material
A 5.25 inch diameter disk made of polycarbonate was used, and a film was formed on one side of the disk.
A 900 mm thick Si-based dielectric film is formed, and an 800 mm thick Tb
A magnetic film made of FeCo was formed, and a Si-based dielectric film having a thickness of 900 mm was further formed to produce a disk medium. The tilt angle of the Si-based dielectric film of the produced disk medium was measured and found to be 3 mrad. The internal stress of the Si-based dielectric film was −4.2 × 10 8 dyn / cm 2 .

比較実験例2 ターゲット材にPを全くドープされていないSi単独タ
ーゲット材を用い、またポリカーボネートから成る径5.
25inchのディスクを用いた以外は前記実験例4と同様の
方法で該ディスクの片面に膜厚900ÅのPを全く含まな
いSi誘電体膜および膜厚800ÅのTbFeCoの磁性膜、更に
膜厚900ÅのPを全く含まないSi系誘電体膜を形成して
ディスク媒体を作成した。作成されたディスク媒体の該
Si系誘電体膜のチルト角を測定したところ、6mrad.であ
った。また、該Si系誘電体膜の内部応力は−3.5×109dy
n/cm2であった。
Comparative Experimental Example 2 The target material used was a single Si target material not doped with P at all, and had a diameter of 5.
Except that a 25-inch disk was used, the same method as in Experimental Example 4 was used except that a 900-nm thick P-free Si dielectric film and a 800-mm thick TbFeCo magnetic film were formed on one surface of the disk, and a 900-mm-thick magnetic film was further formed. A disk medium was prepared by forming a Si-based dielectric film containing no P at all. Of the created disk medium
When the tilt angle of the Si-based dielectric film was measured, it was 6 mrad. The internal stress of the Si-based dielectric film is −3.5 × 10 9 dy
n / cm 2 .

実験例4および比較実験例2から明らかなようにSi系
誘電体膜にPを含有せしめることによって該Si系誘電体
膜のチルト角が小さくなることが確認された。
As is clear from Experimental Example 4 and Comparative Experimental Example 2, it was confirmed that the tilt angle of the Si-based dielectric film was reduced by adding P to the Si-based dielectric film.

(発明の効果) このように本発明の光磁気記録体によるときは、磁性
膜の片面或いは両面に形成されたSi系誘電体膜中にPを
1014atmos/cm3以上含有せしめるようにしたので、従来
のPを全く含まないSi系誘電体膜に比して内部応力を低
減させることが出来る効果を有する。
(Effect of the Invention) As described above, according to the magneto-optical recording medium of the present invention, P is contained in the Si-based dielectric film formed on one or both sides of the magnetic film.
Since 10 14 atmos / cm 3 or more is contained, the internal stress can be reduced as compared with a conventional Si-based dielectric film containing no P at all.

また、本発明の光磁気記録体の製造方法によるとき
は、Si系ターゲット材として1014atoms/cm3以上Pドー
プされたSi系ターゲット材を用いるようにしたので、磁
性膜の片面或いは両面に成膜されるSi系誘電体膜中のP
含有量の調節が容易であり、また、低内部応力でかつダ
ストのないSi系誘電体膜を磁性膜の片面或いは両面に備
えた光磁気記録体を容易に製造することが出来る等の効
果を有する。
In addition, when using the method for manufacturing a magneto-optical recording medium of the present invention, a Si-based target material that is P-doped at 10 14 atoms / cm 3 or more is used as the Si-based target material. P in Si-based dielectric film to be formed
The effect is that the content can be easily adjusted, and a magneto-optical recording medium having a low dielectric stress and a dust-free Si-based dielectric film on one or both sides of the magnetic film can be easily manufactured. Have.

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

第1図はターゲット材中のPドープ量変化とSi系誘電体
膜中のP含有量との関係を示す特性線図、第2図はSi系
誘電体膜中のP含有量変化と該Si系誘電体膜の内部応力
との関係を示す特性線図である。
FIG. 1 is a characteristic diagram showing the relationship between the change in the P doping amount in the target material and the P content in the Si-based dielectric film, and FIG. 2 is a graph showing the change in the P content in the Si-based dielectric film and the Si content. FIG. 4 is a characteristic diagram showing a relationship with an internal stress of a system dielectric film.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】磁性膜の片面或いは両面に形成されたSi系
誘電体膜中にPを1014atoms/cm3以上含有せしめたこと
を特徴とする光磁気記録体。
1. A magneto-optical recording medium characterized in that P is contained in an Si-based dielectric film formed on one side or both sides of a magnetic film at 10 14 atoms / cm 3 or more.
【請求項2】Si系ターゲット材を用い、反応性スパッタ
法により磁性膜の片面或いは両面にSi系誘電体膜を形成
する方法において、該Si系ターゲット材としてPを1014
atoms/cm3以上ドープしたSi系ターゲット材を用いるこ
とを特徴とする光磁気記録体の製造方法。
2. A Si system using a target material, reactive by sputtering in a method of forming a Si-based dielectric film on one side or both sides of the magnetic film, P 10 14 as the Si-based target
A method for producing a magneto-optical recording material, comprising using a Si-based target material doped with atoms / cm 3 or more.
JP1146568A 1989-06-12 1989-06-12 Magneto-optical recording medium and method of manufacturing the same Expired - Fee Related JP2727232B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1146568A JP2727232B2 (en) 1989-06-12 1989-06-12 Magneto-optical recording medium and method of manufacturing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1146568A JP2727232B2 (en) 1989-06-12 1989-06-12 Magneto-optical recording medium and method of manufacturing the same

Publications (2)

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JPH0312841A JPH0312841A (en) 1991-01-21
JP2727232B2 true JP2727232B2 (en) 1998-03-11

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JP1146568A Expired - Fee Related JP2727232B2 (en) 1989-06-12 1989-06-12 Magneto-optical recording medium and method of manufacturing the same

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Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62275338A (en) * 1986-02-17 1987-11-30 Brother Ind Ltd Magneto-optical disk and its production

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Publication number Publication date
JPH0312841A (en) 1991-01-21

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