JPH0590129A - Method of forming diffraction grating - Google Patents
Method of forming diffraction gratingInfo
- Publication number
- JPH0590129A JPH0590129A JP3182026A JP18202691A JPH0590129A JP H0590129 A JPH0590129 A JP H0590129A JP 3182026 A JP3182026 A JP 3182026A JP 18202691 A JP18202691 A JP 18202691A JP H0590129 A JPH0590129 A JP H0590129A
- Authority
- JP
- Japan
- Prior art keywords
- resist
- light
- substrate
- film thickness
- diffraction grating
- 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
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
- G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
- G03F7/70—Microphotolithographic exposure; Apparatus therefor
- G03F7/70408—Interferometric lithography; Holographic lithography; Self-imaging lithography, e.g. utilizing the Talbot effect
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Exposure Of Semiconductors, Excluding Electron Or Ion Beam Exposure (AREA)
- Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
- Diffracting Gratings Or Hologram Optical Elements (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は回折格子の形成方法に
関し、特に、面内均一性に優れた形状を有する回折格子
を得る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 forming a diffraction grating, and more particularly to a method for obtaining a diffraction grating having a shape with excellent in-plane uniformity.
【0002】[0002]
【従来の技術】回折格子が組み込まれた半導体レーザと
して分布帰還型レーザがある。これは、単一縦モード発
振を達成するために考えられた半導体レーザであり、こ
の半導体レーサのレーザ特性は回折格子の形状によって
大きく変化する。このため、回折格子の形状をできるだ
け均一にすることが望まれている。2. Description of the Related Art A distributed feedback laser is a semiconductor laser incorporating a diffraction grating. This is a semiconductor laser designed to achieve single longitudinal mode oscillation, and the laser characteristics of this semiconductor laser greatly change depending on the shape of the diffraction grating. Therefore, it is desired to make the shape of the diffraction grating as uniform as possible.
【0003】図2は、従来の回折格子の形成方法を模式
的に示す工程断面図であり、図において、1は基板、2
はレジスト、2aはレジスト2の未露光部、2bはレジ
スト2の露光部、3は干渉縞の光強度分布、4は二光束
干渉光である。2A to 2C are process sectional views schematically showing a conventional method of forming a diffraction grating, in which 1 is a substrate and 2 is a substrate.
Is a resist, 2a is an unexposed portion of the resist 2, 2b is an exposed portion of the resist 2, 3 is a light intensity distribution of interference fringes, and 4 is two-beam interference light.
【0004】以下、形成工程を説明する。先ず、基板1
上にレジスト2を均一な膜厚に塗布する。そして、図1
(a) に示すように露光用光源として単一波長のArイオ
ンレーザを使用し、このレーザ光をビームエキスパンダ
により光を拡張した後、二光束に分割して、レジスト2
上に干渉縞を形成した二光束干渉光4を照射し、レジス
ト2が露光される。その結果、レジスト2には上記干渉
縞に対応した露光部2aと未露光部2bが形成される。
ここで使用される二光束干渉光4の光束の径は約60m
m(φ)程度で、中心から15mm離れると光強度が5
%程度低下し、中心から離れるにつれてガウス分布に従
って光強度が低下している。続いて、二光束干渉光によ
る露光が行われた上記レジスト2の現像を行うと、レジ
スト露光部2aは溶解し、レジスト未露光部2aは溶解
せず、図2(b) に示すように基板1上にレジスト未露光
部2aによるレジストパターンが形成される。次いで、
図2(c) に示すように上記レジストパターンをマスクと
して基板1のエッチングを行うと、図2(d) に示すよう
な回折格子が形成される。The forming process will be described below. First, substrate 1
The resist 2 is applied on top of it to a uniform film thickness. And FIG.
As shown in (a), an Ar ion laser having a single wavelength is used as a light source for exposure, the laser light is expanded by a beam expander, and then split into two light fluxes.
The resist 2 is exposed by irradiating the two-beam interference light 4 on which interference fringes are formed. As a result, an exposed portion 2a and an unexposed portion 2b corresponding to the interference fringes are formed on the resist 2.
The diameter of the two-beam interference light 4 used here is about 60 m.
The light intensity is about 5 m at a distance of 15 mm from the center.
%, And the light intensity decreases according to a Gaussian distribution as the distance from the center decreases. Subsequently, when the resist 2 exposed by the two-beam interference light is developed, the resist exposed portion 2a is dissolved, the resist unexposed portion 2a is not dissolved, and the substrate is exposed as shown in FIG. 2 (b). A resist pattern is formed on the resist pattern 1 by the resist unexposed portion 2a. Then
When the substrate 1 is etched using the resist pattern as a mask as shown in FIG. 2C, a diffraction grating as shown in FIG. 2D is formed.
【0005】[0005]
【発明が解決しようとする課題】従来の回折格子の形成
工程では、上記のように基板1のレジスト全面にレーザ
光が露光されるように、レーザ光をビームエキスパンダ
によって拡張して二光束干渉光4を形成している。しか
しながら、上記ビームエキスパンダによって光束を拡張
して形成した二光束干渉光4は干渉縞の光強度分布3を
有するため、レジスト2への露光強度にも分布が生じ、
現像して得られるレジストパターンは基板1の中心から
端部に向けてレジスト未露光部2aが多く残り、その結
果、このようなレジストパターンをマスクとしたエッチ
ング処理によって得られる基板1上の溝は形状が不揃い
となり、形成された回折格子の形状は面内均一性の乏し
いものになるという問題点があった。In the conventional diffraction grating forming process, the laser beam is expanded by the beam expander so that the entire surface of the resist on the substrate 1 is exposed to the two-beam interference as described above. Forming light 4. However, since the two-beam interference light 4 formed by expanding the light beam by the beam expander has the light intensity distribution 3 of the interference fringes, the exposure intensity on the resist 2 also has a distribution.
The resist pattern obtained by development has many resist unexposed portions 2a from the center to the end of the substrate 1, and as a result, the groove on the substrate 1 obtained by the etching process using such a resist pattern as a mask is There is a problem that the shapes are not uniform and the formed diffraction grating has poor in-plane uniformity.
【0006】この発明は上記のような問題点を解消する
ためになされたもので、面内均一性に優れた形状を有す
る回折格子を形成する方法を得ることにある。The present invention has been made to solve the above problems, and an object thereof is to obtain a method for forming a diffraction grating having a shape excellent in in-plane uniformity.
【0007】[0007]
【課題を解決するための手段】この発明にかかる回折格
子の形成方法は、レジストの膜厚の膜厚分布をレジスト
を照射する二光束干渉の干渉縞の光強度分布に近づけ、
基板中心から基板周辺に向かう光強度が弱くなる領域の
レジストの膜厚を薄くするようにしたものである。In the method of forming a diffraction grating according to the present invention, the film thickness distribution of the resist film thickness is brought close to the light intensity distribution of the interference fringes of two-beam interference for irradiating the resist,
The thickness of the resist is thinned in the region where the light intensity from the center of the substrate to the periphery of the substrate becomes weak.
【0008】[0008]
【作用】この発明においては、光強度の強い干渉光が照
射される部分のレジストの膜厚を厚く、光強度の弱い干
渉光が照射される部分のレジストの膜厚を薄くしたた
め、現像後のレジストパターンによるマスクの程度が基
板全体でほぼ均一になり、上記レジストパターンをマス
クとしたエッチング処理にて得られる基板上の溝の形状
をほぼ均一にすることができる。According to the present invention, the resist is thicker in the portion irradiated with the interference light having a high light intensity and thinner in the portion irradiated with the interference light having a weak light intensity. The degree of masking by the resist pattern becomes substantially uniform over the entire substrate, and the shape of the groove on the substrate obtained by the etching process using the resist pattern as a mask can be made substantially uniform.
【0009】[0009]
【実施例】以下、この発明の一実施例を図について説明
する。図1はこの発明の一実施例による回折格子の形成
方法の工程を模式的に示す断面図であり、図2と同一符
号は同一または相当する部分を示し、基板1上のレジス
ト2の膜厚は基板の中心から基板の端に向けて薄くなる
膜厚分布を有している。DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a cross-sectional view schematically showing steps of a method of forming a diffraction grating according to an embodiment of the present invention. The same reference numerals as those in FIG. Has a film thickness distribution that becomes thinner from the center of the substrate toward the edge of the substrate.
【0010】次に、上記回折格子の形成工程を説明す
る。先ず、図1に示すように、基板1上に基板1の中心
から離れるにつれて膜厚が減少する膜厚分布をもつよう
にレジスト2を塗布し、次に、露光用光源として単一波
長のArイオンレーザを使用し、このレーザ光をビーム
エキスパンダにより光を拡げた後、二光束に分割し、干
渉縞が形成された二光束干渉光4にてレジスト2を露光
する。この時、上記二光束干渉光4の干渉縞の光強度3
はガウス分布にしたがって基板1の中心から端部に向け
て光強度が低下しているが、上記のような膜厚分布に形
成されたレジスト2は基板の中心から端に向けて膜厚が
薄くなっているため、基板1の表面部のレジストまで露
光するために必要な露光エネルギーが少なくて済み、何
れの部分においても基板1の表面部のレジストまで二光
束干渉光4を露光することができる。次に、現像を行う
と、図1(b) に示すように、レジスト露光部2bは溶解
して除去され、レジスト未露光部2aが基板1上に残
り、更に、このレジスト2aをマスクとした基板1のエ
ッチングを行うと、図1(c) に示すように基板1の何れ
の領域にも均一な形状の溝が形成できる。そして、最後
に基板1上のレジスト2aを除去すると、図1(d) に示
す回折格子が形成される。Next, the process of forming the diffraction grating will be described. First, as shown in FIG. 1, a resist 2 is applied on a substrate 1 so as to have a film thickness distribution in which the film thickness decreases as the distance from the center of the substrate 1 increases. This laser light is expanded by a beam expander using an ion laser, then divided into two light beams, and the resist 2 is exposed by the two light beam interference light 4 in which interference fringes are formed. At this time, the light intensity 3 of the interference fringes of the two-beam interference light 4
Shows that the light intensity decreases from the center of the substrate 1 toward the edges according to the Gaussian distribution, but the resist 2 formed with the above-described thickness distribution has a thinner thickness from the center of the substrate toward the edges. Therefore, the exposure energy required to expose the resist on the surface portion of the substrate 1 is small, and the two-beam interference light 4 can be exposed to the resist on the surface portion of the substrate 1 at any portion. .. Next, when development is performed, as shown in FIG. 1 (b), the resist exposed portion 2b is dissolved and removed, the resist unexposed portion 2a remains on the substrate 1, and the resist 2a is used as a mask. When the substrate 1 is etched, grooves having a uniform shape can be formed in any region of the substrate 1 as shown in FIG. 1 (c). Finally, when the resist 2a on the substrate 1 is removed, the diffraction grating shown in FIG. 1 (d) is formed.
【0011】このような本実施例による回折格子の形成
工程では、レジスト2の膜厚分布の形態と二光束干渉光
4の干渉縞の光強度分布3の形態が一致しているため、
膜厚の大きいところに光強度の大きい干渉光が照射さ
れ、膜厚の小さいところに光強度の小さい干渉光が照射
され、これによって、レジスト2への露光の程度がレジ
スト2全体で平均化し、基板1上の何れの部分において
もマスクの程度が同程度のマスクパターンを作成するこ
とができ、エッチングにより得られる基板1上の溝の形
状が揃い、面内均一性に優れた形状を有する回折格子が
得られる。In the step of forming the diffraction grating according to the present embodiment, since the form of the film thickness distribution of the resist 2 and the form of the light intensity distribution 3 of the interference fringes of the two-beam interference light 4 match.
Interference light having a high light intensity is irradiated to a portion having a large film thickness, and interference light having a low light intensity is irradiated to a portion having a small film thickness, whereby the degree of exposure to the resist 2 is averaged over the entire resist 2, It is possible to form a mask pattern having the same degree of masking on any portion of the substrate 1, the grooves on the substrate 1 obtained by etching are aligned, and the diffraction having a shape with excellent in-plane uniformity is obtained. A lattice is obtained.
【0012】尚、上記実施例ではポジレジストを使用し
た場合について説明したが、ネガレジストを使用した場
合も同様の効果を得ることができる。In the above embodiments, the case where the positive resist is used has been described, but the same effect can be obtained when the negative resist is used.
【0013】[0013]
【発明の効果】以上のように、この発明にかかる回折格
子の形成方法によれば、レジストを照射するレーザ光の
光強度分布に合わせてレジストの膜厚に分布を持たせ、
基板周辺に向かう光強度が弱くなる領域に対応するレジ
ストの膜厚を薄く形成したので、基板上の何れの部分に
もほぼ同一な形状の溝を形成することができ、面内均一
性に優れた形状を有する回折格子を得ることができる効
果がある。As described above, according to the method for forming a diffraction grating of the present invention, the resist film thickness is made to have a distribution in accordance with the light intensity distribution of the laser beam for irradiating the resist,
Since the film thickness of the resist corresponding to the region where the light intensity toward the periphery of the substrate becomes weak is formed thin, grooves of almost the same shape can be formed on any part of the substrate, and excellent in-plane uniformity is achieved. There is an effect that a diffraction grating having a curved shape can be obtained.
【図1】この発明の一実施例による回折格子の形成方法
の工程を模式的に示す断面図である。FIG. 1 is a sectional view schematically showing a step of a method of forming a diffraction grating according to an embodiment of the present invention.
【図2】従来の回折格子の形成工程を模式的に示す断面
図である。FIG. 2 is a cross-sectional view schematically showing a conventional diffraction grating forming process.
1 基板 2 レジスト 2a レジスト未露光部 2b レジスト露光部 3 干渉縞光強度分布 4 二光束干渉光 1 substrate 2 resist 2a resist unexposed part 2b resist exposed part 3 interference fringe light intensity distribution 4 two-beam interference light
Claims (2)
束干渉光を露光する工程と、露光後のレジストを現像し
てレジストパターンを形成する工程と、該レジストパタ
ーンをマスクとして上記基板をエッチング処理する工程
とを含む回折格子の形成方法において、 上記レジストの膜厚分布は上記干渉縞の光強度分布に近
似したものであることを特徴とする回折格子の形成方
法。1. A step of exposing a resist on a substrate to two-beam interference light having interference fringes, a step of developing the exposed resist to form a resist pattern, and etching the substrate using the resist pattern as a mask. A method of forming a diffraction grating including a step of processing, wherein the film thickness distribution of the resist is similar to the light intensity distribution of the interference fringes.
あって、 上記レジストは上記基板の中心から周辺部に向けて膜厚
を薄くしたことを特徴とする回折格子の形成方法。2. The method for forming a diffraction grating according to claim 1, wherein the resist has a film thickness that is reduced from a center of the substrate toward a peripheral portion thereof.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3182026A JPH0590129A (en) | 1991-06-24 | 1991-06-24 | Method of forming diffraction grating |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3182026A JPH0590129A (en) | 1991-06-24 | 1991-06-24 | Method of forming diffraction grating |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0590129A true JPH0590129A (en) | 1993-04-09 |
Family
ID=16111046
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3182026A Pending JPH0590129A (en) | 1991-06-24 | 1991-06-24 | Method of forming diffraction grating |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0590129A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN110320582A (en) * | 2019-07-15 | 2019-10-11 | 英诺激光科技股份有限公司 | Interfere the method for production diffraction optical device using multi-beam laser |
| CN117410168A (en) * | 2023-12-13 | 2024-01-16 | 江西兆驰半导体有限公司 | Patterned sapphire substrate and preparation method thereof |
-
1991
- 1991-06-24 JP JP3182026A patent/JPH0590129A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN110320582A (en) * | 2019-07-15 | 2019-10-11 | 英诺激光科技股份有限公司 | Interfere the method for production diffraction optical device using multi-beam laser |
| CN117410168A (en) * | 2023-12-13 | 2024-01-16 | 江西兆驰半导体有限公司 | Patterned sapphire substrate and preparation method thereof |
| CN117410168B (en) * | 2023-12-13 | 2024-03-29 | 江西兆驰半导体有限公司 | Patterned sapphire substrate and preparation method thereof |
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