JPS6326604A - Polarization beam splitter - Google Patents

Polarization beam splitter

Info

Publication number
JPS6326604A
JPS6326604A JP61170244A JP17024486A JPS6326604A JP S6326604 A JPS6326604 A JP S6326604A JP 61170244 A JP61170244 A JP 61170244A JP 17024486 A JP17024486 A JP 17024486A JP S6326604 A JPS6326604 A JP S6326604A
Authority
JP
Japan
Prior art keywords
light
refractive index
grating
ordinary
birefringent medium
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.)
Granted
Application number
JP61170244A
Other languages
Japanese (ja)
Other versions
JP2594548B2 (en
Inventor
Yuzo Ono
小野 雄三
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP61170244A priority Critical patent/JP2594548B2/en
Priority to EP87110372A priority patent/EP0253403B1/en
Priority to DE87110372T priority patent/DE3786497T2/en
Priority to US07/075,456 priority patent/US4885734A/en
Publication of JPS6326604A publication Critical patent/JPS6326604A/en
Application granted granted Critical
Publication of JP2594548B2 publication Critical patent/JP2594548B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To eliminate the need for a prism which requires vapor deposition or sticking by charging a material whose refractive index is nearly equal to the ordinary or extraordinary light refractive index of a birefringent medium in at least recessed parts of the formed surface projection and recess grating of the birefringent medium. CONSTITUTION:When calcite 1 is used as the birefringent medium, the photoresist pattern of the grating is formed on the surface of the calcite 1 by photolithography and the surface projection and recess grating is formed by ion etching. Then, acrylic resin 2 which has the refractive index N=1.49 almost equal to the extraordinary light refractive index Ne=1.485 is applied as the filling material in grating grooves and the surface is flattened. When a polarization beam splitter is irradiated with incident light 3, a phase grating with a 0.005 refractive index difference to extraordinary light is obtained, so almost no diffracted light is generated and nearly all of extraordinary light components become 0th-order light 4. The refractive index difference to ordinary light, on the other hand, becomes No-N=1.6544-1.49=0.1644, so this grating operates as the phase grating, so that ordinary light components generate refracted light 5. The diffraction efficiency, however, is not 100%, so the ordinary light components generate 0th-order light 4 as well.

Description

【発明の詳細な説明】 この発明は、偏光ビームスプリッタに関し、特にビデオ
ディスク、ディジタル・オーディオ・ディスク(コンパ
クト・ディスク)、光デイスク用の光と・ツクアップや
、光アイソレータの検光子として用いられる、この種の
偏光ビームスプリ・ツタに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a polarizing beam splitter, which is used in particular for optical pickup for video discs, digital audio discs (compact discs), and optical discs, and as an analyzer for optical isolators. This type of polarized beam splitter is concerned.

(従来技術) ビデオディスク、ディジタル・オーディオディスク、光
ディスクの従来のピックア・ツブでは、直角プリズムを
2枚はり合わせ、そのはり合わせ面に誘電体多層膜をコ
ートした偏光ビームスプリッタが用いられている。又、
光アイソレータの検光子としては方解石で製作された検
光子が用いられている。光デイスク光学系への使用例は
、例えば、下記の文献に見ることができる。
(Prior Art) Conventional pick-up tubes for video disks, digital audio disks, and optical disks use a polarizing beam splitter in which two right-angle prisms are bonded together and the bonded surfaces are coated with a dielectric multilayer film. or,
An analyzer made of calcite is used as an analyzer for the optical isolator. Examples of use in optical disk optical systems can be found, for example, in the following documents.

官本、尾島、立野著の「光学」誌第11巻第6号第62
9〜633頁掲載の論文「光デイスク光学系における半
導体レーザーの特性」 (発明が解決しようとしている問題点)上述の従来技術
で、1i)T磨、多層膜蒸着、はり合わせの工程が必要
のため量産性に乏しく、高価であるという問題点があっ
た。又、プリズム分用いるため薄型化が困難であるとい
う問題かぁ−)な。
Kanmoto, Ojima, and Tateno, “Optics” magazine, Vol. 11, No. 6, No. 62
The paper published on pages 9 to 633, "Characteristics of semiconductor lasers in optical disk optical systems" (Problems to be solved by the invention) The above-mentioned conventional technology does not require the steps of 1i) T-polishing, multilayer film deposition, and bonding. Therefore, there were problems in that it was difficult to mass produce and was expensive. Another problem is that it is difficult to make it thinner because it uses the same amount as a prism.

(問題点を解決するための手段) この発明の偏光ビームスアリツタは、複屈折媒体の形成
した表面凹凸格子の少なくとら凹部を前記複屈折媒体の
常光屈折率又は異常光屈折率にほぼ等1−1い屈折率の
物質で充てんして構成されている。
(Means for Solving the Problems) The polarizing beam sparitor of the present invention has at least the concave portions of the surface unevenness grating formed by the birefringent medium that is approximately equal to the ordinary refractive index or the extraordinary refractive index of the birefringent medium. It is filled with a material with a -1 refractive index.

(作用) 複屈折媒体に形成した表面凹凸格子の凹部を例えばその
常光屈折率にほぼ等しい屈折率の物質で充てんすると常
光に対しては、この格子は、屈折率マツチングしてもは
や格子として作用せず、単に屈折率が常光屈折率の媒体
となる。一方、異常光に対しては、異常光屈折率と充て
ん物質の屈折率とから成る位相格子として作用し、異常
光を回折して実効的に光路を変える。以上が本発明の作
用原理である。このように、本構成では、回折現象を用
いて−いるので、素子の表面近傍の薄い格子部でビーム
スプリッタ機能を持っており、これにより、プリズムを
用いない薄型の素子が実現できる。又、充てん物質に、
後の実施例で述べるように樹脂を用いることで、蒸着、
やはり合わせによらず、スビンコー1−等の簡単なプロ
セスで製造ができ、量産性とコストを改善できる。
(Function) If the concave portions of a surface uneven grating formed on a birefringent medium are filled with, for example, a substance with a refractive index approximately equal to the refractive index of the ordinary light, this grating will match the refractive index for ordinary light and will no longer function as a grating. First, it simply becomes a medium whose refractive index is the ordinary refractive index. On the other hand, for extraordinary light, it acts as a phase grating consisting of the refractive index of the extraordinary light and the refractive index of the filling material, diffracts the extraordinary light, and effectively changes the optical path. The above is the principle of operation of the present invention. In this way, since the present configuration uses the diffraction phenomenon, the thin grating near the surface of the element has a beam splitter function, thereby realizing a thin element without using a prism. Also, for the filling material,
As described in later examples, by using resin, vapor deposition,
After all, it can be manufactured by a simple process such as Subinko 1-, regardless of alignment, and mass productivity and cost can be improved.

(実施例) 第1図は本発明の実施例の基本構成を示す斜視断面図で
ある。本実施例では複屈折媒体としてカルサイト1を用
いた。カルサイI−1の表面にフォトリソグラフィで格
子のフオトレジス1−パターンを形成し、これをマスク
にイ6オンエッチングで表面凹凸格子をまず形成した。
(Embodiment) FIG. 1 is a perspective sectional view showing the basic configuration of an embodiment of the present invention. In this example, Calcite 1 was used as the birefringent medium. A lattice photoresist 1-pattern was formed on the surface of Calci I-1 by photolithography, and using this as a mask, a surface uneven lattice was first formed by I6 ion etching.

次に格子溝に異常光屈折率Ne−1,485にほぼ等し
い、屈折率N=1.49を持つアクリル系樹脂2を埋め
込み物質として塗布して、表面を平坦化した。完成した
漏光ビームスプリッタに入射光3を照射すると、異常光
に対しては、屈折率差が0.005の位相格子となるの
で、はとんど回折光を生じず、異常光成分のほとんどが
0次光4として生じる。−万雷光に対しては、屈折率差
がNo−N=1.6544−1.49=0.1644と
なるため、位相格子として作用して、常光成分は回折光
5を生じる。しかし、回折効率は100%ではないので
、常光成分は0次光4も生じる。回折効率を大きくする
ためには、格子がブラ・ソゲ回折格子として作用するよ
うに、渦深さを大きくし、かつ、格子が入射光と回折波
に対して鏡面の関係になるようにブラッグ配置として用
いればよいことはいう迄もない。
Next, acrylic resin 2 having a refractive index N=1.49, which is approximately equal to the extraordinary light refractive index Ne-1,485, was applied as a filling material to the grating grooves to flatten the surface. When the completed leakage beam splitter is irradiated with incident light 3, it becomes a phase grating with a refractive index difference of 0.005 for extraordinary light, so almost no diffracted light is generated, and most of the extraordinary light components are It is generated as zero-order light 4. - For lightning, the refractive index difference is No-N=1.6544-1.49=0.1644, so it acts as a phase grating, and the ordinary light component produces diffracted light 5. However, since the diffraction efficiency is not 100%, zero-order light 4 is also generated as the ordinary light component. In order to increase the diffraction efficiency, the vortex depth must be increased so that the grating acts as a Brass-Soget diffraction grating, and the Bragg arrangement must be arranged so that the grating has a mirror surface relationship with the incident light and diffracted waves. It goes without saying that it can be used as

本実施例では第1図に示すように、複屈折媒体の凸部も
アクリル系樹脂で覆ったが、このような構成とせず、凹
部のみに樹脂を埋めこんでも本質は変らない。また、凹
部のみに樹脂を埋め込んだ後、全面を複屈折媒体で覆っ
ても同様の効果が得られる。
In this embodiment, as shown in FIG. 1, the convex portions of the birefringent medium were also covered with acrylic resin, but the essence remains the same even if only the concave portions are filled with resin instead of such a structure. Furthermore, the same effect can be obtained by filling only the recesses with resin and then covering the entire surface with a birefringent medium.

(発明の効果) 本発明により従来のように高価な蒸着、はり合わせを必
要とするプリズムが不要になる。さらに、本発明の常光
ビームスプリッタは、薄板状に構成できるのでプリズム
に比べ薄型、軽量になる効果がある。
(Effects of the Invention) The present invention eliminates the need for prisms that require expensive vapor deposition and gluing as in the past. Furthermore, since the ordinary beam splitter of the present invention can be constructed in the form of a thin plate, it has the effect of being thinner and lighter than a prism.

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

第1図は本発明の実施例の斜視断面図を示す図である。 1・・・複屈折媒体   2・・・充てん物質3・・入
射光     4・・・0次回折光−゛−・、。 5・・・1次回折光           ■ニーZ−
代理人 弁理士 内厚 晋−コレ 第1図 複屈折媒体
FIG. 1 is a diagram showing a perspective sectional view of an embodiment of the present invention. 1... Birefringent medium 2... Filling material 3... Incident light 4... 0th order diffracted light -゛-...,. 5...1st order diffracted light ■Knee Z-
Agent: Susumu Uchiatsu, Patent Attorney - Figure 1: Birefringent medium

Claims (1)

【特許請求の範囲】[Claims] 複屈折媒体に形成した表面凹凸格子の少なくとも凹部を
前記複屈折媒体の常光屈折率又は異常光屈折率とほぼ等
しい屈折率の物質で充てんしたことを特徴とする偏光ビ
ームスプリッタ。
A polarizing beam splitter, characterized in that at least the concave portions of a surface uneven grating formed on a birefringent medium are filled with a material having a refractive index substantially equal to the ordinary or extraordinary refractive index of the birefringent medium.
JP61170244A 1986-07-18 1986-07-18 Polarizing beam splitter Expired - Lifetime JP2594548B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP61170244A JP2594548B2 (en) 1986-07-18 1986-07-18 Polarizing beam splitter
EP87110372A EP0253403B1 (en) 1986-07-18 1987-07-17 Diffraction grating using birefringence and optical head in which a linearly polarized beam is directed to a diffraction grating
DE87110372T DE3786497T2 (en) 1986-07-18 1987-07-17 Birefringent diffraction grating and optical head in which a linearly polarized beam is directed onto this grating.
US07/075,456 US4885734A (en) 1986-07-18 1987-07-20 Diffraction grating using birefringence and optical head in which a linearly polarized beam is directed to a diffraction grating

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61170244A JP2594548B2 (en) 1986-07-18 1986-07-18 Polarizing beam splitter

Publications (2)

Publication Number Publication Date
JPS6326604A true JPS6326604A (en) 1988-02-04
JP2594548B2 JP2594548B2 (en) 1997-03-26

Family

ID=15901343

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61170244A Expired - Lifetime JP2594548B2 (en) 1986-07-18 1986-07-18 Polarizing beam splitter

Country Status (1)

Country Link
JP (1) JP2594548B2 (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02156205A (en) * 1988-12-08 1990-06-15 Nec Corp Double refractive diffraction grating type polarizer and production thereof
US5272690A (en) * 1992-03-05 1993-12-21 International Business Machines Corporation Hologram element system
US5296694A (en) * 1992-03-31 1994-03-22 Matsushita Electric Industrial Co., Ltd. Optical pick-up head apparatus with optical means having polarization anisotropy
US5739952A (en) * 1994-04-14 1998-04-14 Kabushiki Kaisha Sankyo Seiki Seisakusho Polarizing beam splitter and optical head assembly
US5786911A (en) * 1995-03-20 1998-07-28 Fujitsu Limited Optical scanning apparatus utilizing linear polarized beams
WO1999018459A1 (en) * 1997-10-02 1999-04-15 Asahi Glass Company Ltd. Optical head device and a diffraction element suitable for the device, and a method of manufacturing the diffraction element and the optical head device
US6417941B1 (en) 1998-03-24 2002-07-09 Sharp Kabushiki Kaisha Hologram-type polarized-light splitting element
JP2006106726A (en) * 2004-09-13 2006-04-20 Hitachi Maxell Ltd Polarized light diffracting element
US7113472B2 (en) 2001-03-28 2006-09-26 Matsushita Electric Industrial Co., Ltd. Optical head including an active polymer film for switching voltage during recording and reproducing processes

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6186703A (en) * 1984-09-24 1986-05-02 ミネソタ マイニング アンド マニユフアクチユアリング コンパニー Transparent non-vitreous ceramic fine particle
JPS6186727A (en) * 1984-10-04 1986-05-02 Canon Inc Optical controlling element
JPS61201214A (en) * 1985-03-05 1986-09-05 Canon Inc Optical modulator

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6186703A (en) * 1984-09-24 1986-05-02 ミネソタ マイニング アンド マニユフアクチユアリング コンパニー Transparent non-vitreous ceramic fine particle
JPS6186727A (en) * 1984-10-04 1986-05-02 Canon Inc Optical controlling element
JPS61201214A (en) * 1985-03-05 1986-09-05 Canon Inc Optical modulator

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02156205A (en) * 1988-12-08 1990-06-15 Nec Corp Double refractive diffraction grating type polarizer and production thereof
US5272690A (en) * 1992-03-05 1993-12-21 International Business Machines Corporation Hologram element system
US5296694A (en) * 1992-03-31 1994-03-22 Matsushita Electric Industrial Co., Ltd. Optical pick-up head apparatus with optical means having polarization anisotropy
US5739952A (en) * 1994-04-14 1998-04-14 Kabushiki Kaisha Sankyo Seiki Seisakusho Polarizing beam splitter and optical head assembly
US5786911A (en) * 1995-03-20 1998-07-28 Fujitsu Limited Optical scanning apparatus utilizing linear polarized beams
WO1999018459A1 (en) * 1997-10-02 1999-04-15 Asahi Glass Company Ltd. Optical head device and a diffraction element suitable for the device, and a method of manufacturing the diffraction element and the optical head device
US6618116B1 (en) 1997-10-02 2003-09-09 Asahi Glass Company, Limited Optical head device and a diffraction element suitable for the device, and a method of manufacturing the diffraction element and the optical head device
US6417941B1 (en) 1998-03-24 2002-07-09 Sharp Kabushiki Kaisha Hologram-type polarized-light splitting element
US7113472B2 (en) 2001-03-28 2006-09-26 Matsushita Electric Industrial Co., Ltd. Optical head including an active polymer film for switching voltage during recording and reproducing processes
JP2006106726A (en) * 2004-09-13 2006-04-20 Hitachi Maxell Ltd Polarized light diffracting element

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Publication number Publication date
JP2594548B2 (en) 1997-03-26

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