JPH06259816A - Method for measuring thickness of stamper - Google Patents

Method for measuring thickness of stamper

Info

Publication number
JPH06259816A
JPH06259816A JP6743093A JP6743093A JPH06259816A JP H06259816 A JPH06259816 A JP H06259816A JP 6743093 A JP6743093 A JP 6743093A JP 6743093 A JP6743093 A JP 6743093A JP H06259816 A JPH06259816 A JP H06259816A
Authority
JP
Japan
Prior art keywords
stamper
thickness
measured
measuring
laser
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
JP6743093A
Other languages
Japanese (ja)
Inventor
Masataka Yashima
正孝 八島
Osamu Shikame
修 鹿目
Hirofumi Kamitakahara
弘文 上高原
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP6743093A priority Critical patent/JPH06259816A/en
Publication of JPH06259816A publication Critical patent/JPH06259816A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To exactly measure the thickness of a stamper with high precision by measuring the thickness of the stamper after the influence due to the inclination in the stamper being a subject to be measured is eliminated. CONSTITUTION:The stamper formed on a glass plate is set to a movable stage 7. Then, the movable stage 7 is moved and a measuring position is aligned. A laser displacement gage 1 and the laser displacement gage (measuring istrument) 1a are rotated around a central line 4, and a rotation angle where the displacement becomes maximum or minimum is obtained. The value of the displacement gage when the meter is rotated by 90 deg. from the rotation angle becomes a real value. The operation is performed by the laser displacement gages 1 and 1a independently, and the thickness of the stamper is obtained from these values.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、光記録媒体用基板を製
造する為のスタンパーの厚みの測定方法に関するもので
ある。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring the thickness of a stamper for manufacturing a substrate for an optical recording medium.

【0002】[0002]

【従来の技術】光記録媒体は、照射したレーザービーム
の反射によりピットの有無を検出し、情報を記録再生す
るものである。したがって、目的の情報をすばやく記録
再生する為には、レーザー光を所定の場所にすばやく移
動する(高速アクセス)為に、案内溝が必要となる。案
内溝の幅や深さは、レーザーのビーム径や制御方法によ
り異なるが、通常、光ディスクの場合には、溝幅0.8
μm、溝ピッチ1.6μm、溝深さ700Å前後であ
り、光カードの場合には、溝幅2.5〜3.0μm、溝
ピッチ12μm、溝深さ1000〜3000Åぐらいで
ある。
2. Description of the Related Art An optical recording medium is for recording / reproducing information by detecting the presence or absence of pits by the reflection of an irradiated laser beam. Therefore, in order to quickly record and reproduce desired information, the guide groove is required to quickly move the laser light to a predetermined place (high speed access). The width and depth of the guide groove vary depending on the laser beam diameter and control method, but in the case of an optical disk, the groove width is usually 0.8
The groove width is about 2.5 μm, the groove pitch is about 12 μm, and the groove depth is about 1000 to 3000 Å.

【0003】このように微細な凹凸パターンは、硬い材
質であるニッケルのスタンパーにより基板に転写され
る。その方法はインジェクション法や、押し出し成形法
等様々であるが、ほとんど、数十μmから数百μmの厚
さのスタンパーを使用している。
Such a fine concavo-convex pattern is transferred to the substrate by a nickel stamper which is a hard material. There are various methods such as an injection method and an extrusion molding method, but most of them use a stamper having a thickness of several tens μm to several hundreds μm.

【0004】厚さ数十μmから数百μmのスタンパーは
次の様にして製造される。厚さ10mm程度のガラスに
レジスト等により案内溝パターンを形成し、この面にス
パッタリングにより、ニッケルの導電化膜を厚さ数千Å
程度に成膜する。この面に電鋳を行ないニッケルの膜厚
を数十μmから数百μmにする。このニッケルを所定の
厚さまで研磨し、ガラスから剥離してスタンパーを得
る。この研磨の際、ニッケルスタンパーの厚さは、ガラ
スから剥離できない為直接測定することはできない。こ
の為、例えばレーザー変位計でスタンパーの研磨面側と
ガラス面側を測定し、その差からスタンパーの厚さを算
出していた。
A stamper having a thickness of several tens of μm to several hundreds of μm is manufactured as follows. A guide groove pattern is formed on the glass with a thickness of about 10 mm with resist or the like, and a nickel conductive film is formed on this surface by sputtering to a thickness of several thousand Å.
The film is formed to a degree. Electroforming is performed on this surface to change the nickel film thickness from several tens of μm to several hundreds of μm. This nickel is polished to a predetermined thickness and peeled from the glass to obtain a stamper. During this polishing, the thickness of the nickel stamper cannot be directly measured because it cannot be separated from the glass. Therefore, for example, a laser displacement meter was used to measure the polished surface side and the glass surface side of the stamper, and the thickness of the stamper was calculated from the difference.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、上記従
来例では、ニッケルスタンパーの厚さを正確に測定する
事は難しかった。この理由は以下の通りである。
However, in the above conventional example, it was difficult to accurately measure the thickness of the nickel stamper. The reason for this is as follows.

【0006】レーザー変位計は、図2に示す様にレーザ
ー光の入射光(照射光)11を被測定物12に照射し、
その反射光13の受光センサー14の受光面での位置か
ら、被測定物の変位を測定するものである。したがっ
て、照射光の進行方向の単位ベクトル
The laser displacement meter irradiates an object to be measured 12 with incident light (irradiation light) 11 of laser light as shown in FIG.
The displacement of the object to be measured is measured from the position of the reflected light 13 on the light receiving surface of the light receiving sensor 14. Therefore, the unit vector of the traveling direction of the irradiation light

【0007】[0007]

【外1】 [Outer 1]

【0008】と受光面を含む平面(図2における紙面)
に被測定物の法線ベクトルを斜影した単位ベクトル
And a plane including the light receiving surface (paper surface in FIG. 2)
A unit vector that is the normal vector of the DUT

【0009】[0009]

【外2】 は照射光の進行方向の単位ベクトル[Outside 2] Is the unit vector in the direction of travel of the irradiation light

【0010】[0010]

【外3】 と常に次の(I)式の関係が成り立たなければ正確な測
定はできない事になる。
[Outside 3] If the relation of the following formula (I) is not always satisfied, accurate measurement cannot be performed.

【0011】[0011]

【数1】 [Equation 1]

【0012】ところが、ガラスにニッケルをスパッタリ
ングおよび電鋳する際、多かれ少なかれ応力が生じるの
が通常である。その結果、ガラスは多少ゆがみをもつこ
とになる。このゆがみは、被測定面の法線ベクトルの向
きを変化させる事になり、その結果レーザー変位計の値
は真の値からずれる事になる。
However, when nickel is sputtered and electroformed on glass, more or less stress is usually generated. As a result, the glass will be somewhat distorted. This distortion changes the direction of the normal vector of the surface to be measured, and as a result, the laser displacement meter value deviates from the true value.

【0013】本発明は、この様な従来技術の欠点を改善
するためになされたものであり、測定用レーザー及び受
光面をもつ測定器を回転させる機溝を設け、前記(I)
式が成成する様にして、スタンパーの傾きの影響をとり
のぞいた状態にして測定する事により、スタンパーの厚
さを正確に精度良く測定する事を目的とする。
The present invention has been made in order to remedy the above drawbacks of the prior art. A machine groove for rotating a measuring laser and a measuring instrument having a light receiving surface is provided, and the above (I) is provided.
The purpose is to measure the thickness of the stamper accurately and accurately by measuring the condition with the effect of the tilt of the stamper removed so that the formula is satisfied.

【0014】[0014]

【課題を解決するための手段】即ち、本発明は、スタン
パーの製造方法におけるガラス板上に成膜されたスタン
パーの厚みを測定する際、レーザー光を照射する部分と
被測定物からの反射光を受光する部分とを配置してあ
り、その反射光の受光位置から被測定物の変位を測定す
るレーザー変位計をスタンパーの両側に配置してスタン
パーの厚みを測定する方法において、被測定物であるス
タンパーの傾きの影響を無くした状態でスタンパーの厚
さを測定することを特徴とするスタンパーの厚み測定方
法である。
That is, according to the present invention, when measuring the thickness of a stamper formed on a glass plate in a method of manufacturing a stamper, a portion irradiated with laser light and reflected light from an object to be measured are measured. In the method of measuring the thickness of the stamper by arranging laser displacement gauges on both sides of the stamper that measures the displacement of the measured object from the position where the reflected light is received, The stamper thickness measuring method is characterized in that the thickness of the stamper is measured in a state where the influence of the inclination of a certain stamper is eliminated.

【0015】本発明においては、変位を測定する為のレ
ーザー光照射部分とその反射光受光部分を備えたレーザ
ー変位計が、その対称中心軸のまわりに回転させる手段
と被測定物の傾きを検知する手段を有し、被測定物の傾
きが測定に影響しないような配置に上記レーザー変位計
を回転させて測定するのが好ましい。
In the present invention, a laser displacement meter having a laser light irradiation portion for measuring displacement and a reflected light receiving portion thereof detects a means for rotating about a central axis of symmetry and an inclination of an object to be measured. It is preferable that the laser displacement meter is rotated so that the inclination of the object to be measured does not affect the measurement.

【0016】また、被測定物の傾きを検知する手段が、
レーザー変位計を回転させた時の受光位置の分布である
か、または被測定物の傾きを検知する手段が、レーザー
変位計の回転中心軸と平行にレーザー光を被測定物に照
射する手段と、その反射光を受光する手段であり、その
受光した反射光の位置により被測定物の傾きを検知する
方法であることが好ましい。
The means for detecting the inclination of the object to be measured is
The means for detecting the distribution of the light receiving position when the laser displacement meter is rotated or the inclination of the object to be measured is a means for irradiating the object to be measured with a laser beam parallel to the central axis of rotation of the laser displacement meter. A means for receiving the reflected light, and a method for detecting the inclination of the object to be measured by the position of the received reflected light are preferable.

【0017】[0017]

【実施例】以下に図面に示す実施例を挙げて本発明を具
体的に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be specifically described below with reference to the embodiments shown in the drawings.

【0018】実施例1 図1は本発明のスタンパーの厚み測定方法の一実施態様
を示す説明図である。図1において、1はレーザー変位
計(測定器)であり、2はニッケルスタンパー、3はガ
ラス板である。1のレーザー変位計の測定器は、その中
心線4を軸に回転できる手段を有する。被測定物である
スタンパーに傾きがある場合、受光センサー14の受光
面での反射光位置21は1のレーザー変位計測定器を回
転させると図3のように変化する。図3において、22
及び22aの位置は、図2で示した
Example 1 FIG. 1 is an explanatory view showing one embodiment of a stamper thickness measuring method of the present invention. In FIG. 1, 1 is a laser displacement meter (measuring instrument), 2 is a nickel stamper, and 3 is a glass plate. The measuring instrument of the laser displacement meter of No. 1 has means capable of rotating about its center line 4. When the stamper that is the object to be measured has an inclination, the reflected light position 21 on the light receiving surface of the light receiving sensor 14 changes as shown in FIG. 3 when the laser displacement gauge measuring device 1 is rotated. In FIG. 3, 22
The positions of 22a and 22a are shown in FIG.

【0019】[0019]

【外4】 の値が最大、最小になった時の位置であり、そこからレ
ーザー変位計(測定器)1を90°回転させ、
[Outside 4] Is the position when the value of becomes maximum and minimum, from which the laser displacement meter (measuring device) 1 is rotated by 90 °,

【0020】[0020]

【数2】 が成り立つ様にした時、反射光の受光面上の位置は、図
3における23の位置にくる。被測定物(スタンパー)
との距離は、この23の位置から算出した値が真の値と
なる。
[Equation 2] When the above condition is satisfied, the position of the reflected light on the light receiving surface comes to the position of 23 in FIG. DUT (Stamper)
As for the distance between and, the value calculated from these 23 positions is the true value.

【0021】実際のスタンパーの厚みの測定は以下の手
順による。はじめにガラス板上に成膜されたスタンパー
を移動ステージ7にセットする。次に、前記可動ステー
ジを移動して測定場所を合わせる。1および1aのレー
ザー変位計(測定器)を中心線4を軸に回転させ、変位
が最大もしくは最小になる(図3の22もしくは23の
位置に反射光がくる)回転角をさがす。その回転角から
90°回転させた時の変位計の値が真の値となる。レー
ザー変位計1および1aでこの動作を独立で行い、それ
らの値からスタンパー厚みが求められる。このあとステ
ージを次の測定ポイントに移動し再度上記作業を行う。
The actual thickness of the stamper is measured by the following procedure. First, the stamper formed on the glass plate is set on the moving stage 7. Next, the movable stage is moved to match the measurement location. The laser displacement gauges (measuring instruments) 1 and 1a are rotated about the center line 4 to find the rotation angle at which the displacement becomes maximum or minimum (the reflected light comes to the position 22 or 23 in FIG. 3). The true value is the value of the displacement meter when it is rotated 90 ° from the rotation angle. This operation is independently performed by the laser displacement meters 1 and 1a, and the stamper thickness is obtained from those values. After that, the stage is moved to the next measurement point and the above work is performed again.

【0022】ここでは、1のレーザー変位計としてキー
エンス社製のレーザー変位計(LD−2510)を用
い、パルスモーター付ステージ(シグマ光機社製、KS
H−80PM)で回転制御した、また1のレーザー変位
計(測定器)の出力を変換演算する変換演算器5はキー
エンス社製のLD−2500を用いた。
Here, a laser displacement meter (LD-2510) manufactured by Keyence Corporation is used as one laser displacement meter, and a stage with a pulse motor (KS manufactured by Sigma Optical Co., Ltd., KS) is used.
LD-2500 manufactured by KEYENCE CORPORATION was used as the conversion calculator 5 which controls the rotation of the laser displacement meter (measuring device) No. 1 by rotation control at H-80PM).

【0023】実施例2 図4に示すように、変位測定用レーザー10及び受光セ
ンサー14の他に被測定物12の法線ベクトルの向きを
検知する為の傾き検知用レーザー16と傾き検知用受光
センサー17が設けてある装置を用いた。
Embodiment 2 As shown in FIG. 4, in addition to the displacement measuring laser 10 and the light receiving sensor 14, a tilt detecting laser 16 for detecting the direction of the normal vector of the object to be measured 12 and a tilt detecting light receiving. A device provided with the sensor 17 was used.

【0024】コリメーター付半導体レーザーの傾き検知
用レーザー16から出射されたレーザー光は被測定物1
2の測定ポイントに照射される。その反射光の進行方向
を示す単位ベクトル
The laser light emitted from the laser 16 for detecting the tilt of the semiconductor laser with a collimator is the object to be measured 1
The two measurement points are illuminated. A unit vector indicating the traveling direction of the reflected light

【0025】[0025]

【外5】 は、被測定面の法線ベクトルを[Outside 5] Is the normal vector of the surface to be measured

【0026】[0026]

【外6】 、入射光の進行方向を示す単位ベクトルを[Outside 6] , A unit vector indicating the traveling direction of the incident light

【0027】[0027]

【外7】 とすると、下記の(II)式を満足する。[Outside 7] Then, the following expression (II) is satisfied.

【0028】[0028]

【数3】 [Equation 3]

【0029】すなわち、被測定面の法線べクトルの向き
で反射光の進行方向が決定される。したがって、図4
(a)において、被測定面の向きを調べる傾き検知用反
射光20を測定用の照射光の進行方向を示す単位ベクト
That is, the traveling direction of the reflected light is determined by the direction of the normal vector of the surface to be measured. Therefore, FIG.
In (a), a unit vector indicating the traveling direction of the tilt detection reflected light 20 for checking the direction of the surface to be measured

【0030】[0030]

【外8】 と受光面を含む平面(図4(a)における紙面)に斜影
した時、その斜影した傾き検知用反射光20が入射光と
一致すれば、前記(I)式が成り立つことになる。
[Outside 8] When the shaded reflected light 20 for tilt detection coincides with the incident light when shaded on a plane including the light receiving surface (the paper surface in FIG. 4A), the above formula (I) is established.

【0031】すなわち、傾き検知用反射光20を検知す
る受光センサーとして、例えば図4(C)のような縦形
の2分割の傾き検知用受光センサー17を用い、その左
右(17A、17B)での光量が等しくなるように測定
器のレーザー変位計を中心線4を軸にして回転して合わ
せたとき、前記(1)式が成立する。図4においては、
傾き検知用受光センサー17の設置場所を得るために、
18の偏光ビームスプリッターを利用している。
That is, as a light receiving sensor for detecting the reflected light 20 for tilt detection, for example, a vertical two-divided light receiving sensor 17 for tilt detection as shown in FIG. 4C is used, and the left and right (17A, 17B) thereof are used. When the laser displacement meter of the measuring instrument is rotated about the center line 4 and aligned so that the light amounts become equal, the above formula (1) is established. In FIG.
To obtain the installation location of the light receiving sensor 17 for tilt detection,
18 polarization beam splitters are used.

【0032】スタンパーの厚みの測定方法は実施例1と
ほとんど同じであり厚み測定の際、上述したように17
の受光センサーの差(17A−17B)が0になるよう
に1の測定器のレーザー変位計を回転させる。したがっ
て、実施例1に比べて1の測定器のレーザー変位計の回
転の時間が大幅に短縮され、測定時間が短くなるという
効果もある。
The method of measuring the thickness of the stamper is almost the same as that of the first embodiment.
The laser displacement meter of the measuring instrument of 1 is rotated so that the difference (17A-17B) of the light receiving sensors of 1 is 0. Therefore, compared with the first embodiment, there is an effect that the rotation time of the laser displacement meter of the measuring instrument 1 is significantly shortened and the measurement time is shortened.

【0033】[0033]

【発明の効果】以上説明した様に、本発明によれば、ス
タンパーの厚みをスタンパーの傾きの影響をとりのぞい
た状態にして測定する事により、スタンパーの厚みを精
度良く測定する事ができる効果がある。
As described above, according to the present invention, the thickness of the stamper can be accurately measured by measuring the thickness of the stamper without the influence of the inclination of the stamper. There is.

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

【図1】本発明のスタンパーの厚み測定方法の一実施態
様を示す説明図である。
FIG. 1 is an explanatory view showing an embodiment of a stamper thickness measuring method of the present invention.

【図2】変位測定の原理図[Fig.2] Principle diagram of displacement measurement

【図3】レーザー変位計を回転させた時の反射光位置[Fig. 3] Position of reflected light when the laser displacement meter is rotated

【図4】本発明のスタンパーの厚み測定方法の他の実施
態様を示す説明図である。
FIG. 4 is an explanatory view showing another embodiment of the stamper thickness measuring method of the present invention.

【符号の説明】[Explanation of symbols]

1,1a レーザー変位計 2 ニッケルスタンパー 3 ガラス板 4 中心軸 5 変位演算器 6 変位・厚み変換器 7 可動ステージ 10 変位測定用レーザー(コリメータ付) 11 入射光(照射光) 12,12a 被測定物 13,13a 反射光 14 受光センサー 15 被測定面の法線ベクトル 16 傾き検知用レーザー 17 傾き検知受光センサー 18 偏光ビームスプリッター 19 傾き検知用入射光 20 傾き検知用反射光 21 反射光の軌跡 1, 1a Laser displacement meter 2 Nickel stamper 3 Glass plate 4 Center axis 5 Displacement calculator 6 Displacement / thickness converter 7 Movable stage 10 Laser for displacement measurement (with collimator) 11 Incident light (irradiation light) 12, 12a DUT 13, 13a Reflected light 14 Light receiving sensor 15 Normal vector 16 of the surface to be measured 16 Tilt detection laser 17 Tilt detection light receiving sensor 18 Polarization beam splitter 19 Tilt detection incident light 20 Tilt detection reflected light 21 Reflected light trajectory

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 スタンパーの製造方法におけるガラス板
上に成膜されたスタンパーの厚みを測定する際、レーザ
ー光を照射する部分と被測定物からの反射光を受光する
部分とを配置してあり、その反射光の受光位置から被測
定物の変位を測定するレーザー変位計をスタンパーの両
側に配置してスタンパーの厚みを測定する方法におい
て、被測定物であるスタンパーの傾きの影響を無くした
状態でスタンパーの厚さを測定することを特徴とするス
タンパーの厚み測定方法。
1. When measuring the thickness of a stamper formed on a glass plate in the method of manufacturing a stamper, a portion for irradiating laser light and a portion for receiving reflected light from an object to be measured are arranged. , In the method of measuring the thickness of the stamper by arranging the laser displacement gauges on both sides of the stamper to measure the displacement of the measured object from the position where the reflected light is received, the effect of the inclination of the stamper that is the measured object is eliminated. A method for measuring the thickness of a stamper, which comprises measuring the thickness of the stamper with.
【請求項2】 変位を測定する為のレーザー光照射部分
とその反射光受光部分を備えたレーザー変位計が、その
対称中心軸のまわりに回転させる手段と被測定物の傾き
を検知する手段を有し、被測定物の傾きが測定に影響し
ないような配置に上記レーザー変位計を回転させて測定
することを特徴とする請求項1記載のスタンパーの厚み
測定方法。
2. A laser displacement meter provided with a laser light irradiation portion for measuring displacement and a reflected light receiving portion thereof has means for rotating about a central axis of symmetry and means for detecting inclination of an object to be measured. The method for measuring the thickness of a stamper according to claim 1, wherein the laser displacement meter is rotated in such a position that the inclination of the object to be measured does not affect the measurement.
【請求項3】 被測定物の傾きを検知する手段が、レー
ザー変位計を回転させた時の受光位置の分布であること
を特徴とする請求項2記載のスタンパーの厚み測定方
法。
3. The stamper thickness measuring method according to claim 2, wherein the means for detecting the inclination of the object to be measured is a distribution of light receiving positions when the laser displacement meter is rotated.
【請求項4】 被測定物の傾きを検知する手段が、レー
ザー変位計の回転中心軸と平行にレーザー光を被測定物
に照射する手段と、その反射光を受光する手段であり、
その受光した反射光の位置により被測定物の傾きを検知
することを特徴とする請求項2記載のスタンパーの厚み
測定方法。
4. The means for detecting the inclination of the object to be measured is means for irradiating the object to be measured with laser light parallel to the central axis of rotation of the laser displacement meter, and means for receiving the reflected light thereof.
The stamper thickness measuring method according to claim 2, wherein the inclination of the object to be measured is detected by the position of the received reflected light.
JP6743093A 1993-03-04 1993-03-04 Method for measuring thickness of stamper Pending JPH06259816A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6743093A JPH06259816A (en) 1993-03-04 1993-03-04 Method for measuring thickness of stamper

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6743093A JPH06259816A (en) 1993-03-04 1993-03-04 Method for measuring thickness of stamper

Publications (1)

Publication Number Publication Date
JPH06259816A true JPH06259816A (en) 1994-09-16

Family

ID=13344693

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6743093A Pending JPH06259816A (en) 1993-03-04 1993-03-04 Method for measuring thickness of stamper

Country Status (1)

Country Link
JP (1) JPH06259816A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20020016446A (en) * 2000-08-25 2002-03-04 신현준 Measuring system for width or thickness using laser sensors and optics
EP1655572A1 (en) * 2004-11-05 2006-05-10 DaTARIUS Technologies GmbH Device for measuring surface properties of optical media stampers
EP1655571A1 (en) * 2004-11-05 2006-05-10 DaTARIUS Technologies GmbH Device for measuring the thickness of optical media stampers
KR100867951B1 (en) * 2007-07-16 2008-11-11 삼성전기주식회사 Imprinting method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20020016446A (en) * 2000-08-25 2002-03-04 신현준 Measuring system for width or thickness using laser sensors and optics
EP1655572A1 (en) * 2004-11-05 2006-05-10 DaTARIUS Technologies GmbH Device for measuring surface properties of optical media stampers
EP1655571A1 (en) * 2004-11-05 2006-05-10 DaTARIUS Technologies GmbH Device for measuring the thickness of optical media stampers
KR100867951B1 (en) * 2007-07-16 2008-11-11 삼성전기주식회사 Imprinting method

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