JPS62170902A - Wavelength plate - Google Patents

Wavelength plate

Info

Publication number
JPS62170902A
JPS62170902A JP1238086A JP1238086A JPS62170902A JP S62170902 A JPS62170902 A JP S62170902A JP 1238086 A JP1238086 A JP 1238086A JP 1238086 A JP1238086 A JP 1238086A JP S62170902 A JPS62170902 A JP S62170902A
Authority
JP
Japan
Prior art keywords
grating
lambda
wavelength
satisfying
groove
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
JP1238086A
Other languages
Japanese (ja)
Inventor
Yasuo Kimura
靖夫 木村
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 JP1238086A priority Critical patent/JPS62170902A/en
Publication of JPS62170902A publication Critical patent/JPS62170902A/en
Pending legal-status Critical Current

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  • Diffracting Gratings Or Hologram Optical Elements (AREA)

Abstract

PURPOSE:To easily form a surface releaf grating type wavelength plate by forming a surface releaf grating satisfying 2>lambda/d>=1.472 on a dielectric body when using wavelength is lambda and a grating pitch is (d). CONSTITUTION:The grating 2 is formed on the dielectric body 1, and when rays of light are made incident upon the surface of the grating from the direction of an arrow 3, different diffractive indexes are generated respectively in vertical and horizontal directions to the grating. When a He-Cd laser beam with wavelength lambda=441.6nm is made incident upon the grating having a pitch d=0.3mum satisfying lambda/d>2 for a He-Ne laser beam with wavelength 632.8nm e.g., the grating shows double refracting property and lambda/d=1.472 is obtained. Thereby, the grating satisfying the condition of at least 2>lambda/d>=1.472 indicates the double refracting property. When the ratio of the crest of the grating to its trough is set up to 1 to 1 in such kind of grating, the width l of the groove can be set up to lambda/4<l<=lambda/2.944, so that the width l of the groove can be expanded. Thus, the grating can be easily formed.

Description

【発明の詳細な説明】 (産業上の利用分野) この発明は、直交する2つの直線偏光の間に位相差を生
せしめる1/4波長板、1/2波長板、全波長板等の波
長板に関するものである。
Detailed Description of the Invention (Industrial Field of Application) This invention relates to a wavelength control device such as a quarter-wave plate, a half-wave plate, a full-wave plate, etc. that produces a phase difference between two orthogonal linearly polarized lights. It's about the board.

(従来の技術) 従来、波長板は水晶の結晶を研磨して、常光と異常光の
位相差が、1/4波長板では(N + 1/4)波長(
Nは整数)、172波長板では(N +1/2)波長、
全波長板ではN波長になるような厚さに調整して製作さ
れている。このような結晶研磨による方法以外に誘電体
に形成した高密度の表面レリーフ格子が複屈折を示すこ
とから、格子を用いる方法も提案されている。表面レリ
ーフ格子を用いた波長板の提案と実験は、アプライド・
フィジックス・レターズ(Applied Physi
cs Letters)誌第42巻第6号(1983年
3月15日発行)第492〜494頁掲載の論文及びア
プライド・オプティックス(Applied 0pti
cs)誌第22巻第20号(1983年10月15日発
行)第3220〜3228頁掲載の論文に述べられてい
る。格子を用いた波長板は、格子のピッチをd、使用波
長をλとすると、λがdに比べて十分大きい領域では格
子の溝に平行な方向と直交する方向で屈折率が異なるこ
とを利用している。
(Prior art) Conventionally, a wave plate is made by polishing a quartz crystal, and the phase difference between ordinary light and extraordinary light is changed to (N + 1/4) wavelength (
N is an integer), (N + 1/2) wavelength for a 172-wave plate,
A full-wavelength plate is manufactured by adjusting the thickness so that it has N wavelengths. In addition to such a method using crystal polishing, a method using a grating has also been proposed because a high-density surface relief grating formed on a dielectric exhibits birefringence. The proposal and experiment of a wave plate using surface relief gratings was carried out by Applied
Physics Letters (Applied Physi
cs Letters, Vol. 42, No. 6 (published March 15, 1983), pp. 492-494, and Applied Optics (Applied Optics).
cs), Vol. 22, No. 20 (published October 15, 1983), pp. 3220-3228. A wavelength plate using a grating takes advantage of the fact that, where the pitch of the grating is d and the wavelength used is λ, the refractive index differs in the direction parallel to and perpendicular to the grooves of the grating in a region where λ is sufficiently large compared to d. are doing.

上述の論文を含め従来、格子が複屈折性を示す条件は、
実験的にA/d>2であるとされており、これは回折光
が生じない条件でもある。
Conventionally, including the above-mentioned paper, the conditions for a grating to exhibit birefringence are:
It has been experimentally determined that A/d>2, which is also a condition under which no diffracted light is generated.

(発明が解決しようとする問題点) 、Vd>2すなわちd<)J2の高密度格子では、格子
の山と谷の比を1対1とした場合、溝の幅1は1<后4
となり、微細な加工が必要となる。また、格子を用いた
波長板の位相差は、複屈折の屈折率差をΔnとすると、
Δn−tで与えられる。ここに、tは格子の溝深さであ
る。屈折率1.5〜2.0の材料で格子を製作するとΔ
n−0,2程度となるため、必要な溝深さが、1/4波
長板でもt=1.25λとなる。したがって微細な溝幅
で、溝幅に対して非常に深い格子となり、製作が困難に
なる問題点があった。表面レリーフ格子の最も安価で簡
便な方法は、プラスチック板に型押しで製作する方法で
あるが、上述の格子は型押しで製作するのが困難である
という問題もある。本発明の目的は以上述べた問題点を
解決した表面レリーフ格子型の波長板を提供することに
ある。
(Problem to be Solved by the Invention) In a high-density grid with Vd>2, that is, d<)J2, when the ratio of peaks and valleys of the grid is 1:1, the width 1 of the groove is 1<4
Therefore, fine processing is required. Furthermore, the phase difference of a wavelength plate using a grating is given by Δn, which is the refractive index difference of birefringence.
It is given by Δn-t. Here, t is the groove depth of the grating. When a grating is made of a material with a refractive index of 1.5 to 2.0, Δ
Since it is about n-0.2, the required groove depth is t=1.25λ even for a quarter-wave plate. Therefore, the fine groove width results in a grating that is very deep relative to the groove width, making it difficult to manufacture. The cheapest and simplest method for producing a surface relief grating is to fabricate it by stamping it onto a plastic plate, but there is also the problem that the above-mentioned gratings are difficult to fabricate by stamping. An object of the present invention is to provide a surface relief grating type wave plate that solves the above-mentioned problems.

(問題点を解決するための手段) 前述の問題点を解決するために本発明が提供する手段は
、誘電体に、使用波長をλ、格子ピッチをdとして、2
>Vd≧1.472なる表面レリーフ格子を形成したこ
とを特徴とする。
(Means for Solving the Problems) In order to solve the above-mentioned problems, the present invention provides means for solving the problems described above.
>Vd≧1.472.

(作用) 波長632.8nmのHe−Neレーザ光に対してVd
>2を満足するピッチd = 0.3pmとした格子に
対して波長λ=441.6nmのHe−Cdレーザ光を
入射させたところ、格子は複屈折性を示すことを見い出
した。この場合)Jd=1.472となる。したがって
、少くとも2>Vd>1.472の条件を満足する格子
は複屈折性を示す。このような格子では、格子の山と谷
の比を1対1とした場合溝の幅lはA/4<1≦l/2
.944となり、)Jd≧2の格子に比べて溝幅を広く
することができる゛ので製作が容易になる。また、型押
しによる格子の製作も容易になる。
(Function) Vd for He-Ne laser light with a wavelength of 632.8 nm
When a He-Cd laser beam with a wavelength λ = 441.6 nm was incident on a grating with a pitch d = 0.3 pm satisfying >2, it was found that the grating exhibited birefringence. In this case) Jd=1.472. Therefore, a grating that satisfies at least the condition 2>Vd>1.472 exhibits birefringence. In such a lattice, when the ratio of peaks to valleys of the lattice is 1:1, the width l of the groove is A/4<1≦l/2.
.. 944), and the groove width can be made wider than in the case of a lattice with Jd≧2, making manufacturing easier. Furthermore, it becomes easy to manufacture the grid by stamping.

(実施例) 次に図面を参照してこの発明の詳細な説明する。図はこ
の発明の波長板の構造を説明するための斜視図で、わか
りやすくするために、格子を実際よりもはるかに大きく
模式的に描いである。誘電体1上に格子2が形成されて
おり、格子面に矢印3の方向から光を入射すると格子に
垂直な方向と平行な方向で屈折率が異なり、溝深さtに
より位相差を受け、矢印4の方向に透過光が出射し、波
長板として作用する。また、本発明による波長板ではA
/d<2であるため、回折光が空気中に生じる。実際の
製作は、He−Cdレーザの波長441.6nmの光ビ
ームを用いて干渉計を構成し、ホログラフィックにピッ
チ0.3pmの格子をホトレジストに形成した。ホトレ
ジスト現像後の表面レリーフ格子からニッケル電鋳法で
スタンパ−を製作し、このスタンパ−を用いてアクリル
板に加熱プレスで型押しして波長板を形成した。
(Example) Next, the present invention will be described in detail with reference to the drawings. The figure is a perspective view for explaining the structure of the wavelength plate of the present invention, and for the sake of clarity, the grating is schematically drawn much larger than it actually is. A grating 2 is formed on a dielectric 1, and when light is incident on the grating surface from the direction of arrow 3, the refractive index is different in the direction perpendicular to the grating and the direction parallel to it, and there is a phase difference due to the groove depth t. The transmitted light is emitted in the direction of arrow 4 and acts as a wave plate. Furthermore, in the wave plate according to the present invention, A
Since /d<2, diffracted light is generated in the air. In actual production, an interferometer was constructed using a light beam of a He-Cd laser with a wavelength of 441.6 nm, and a holographic grating with a pitch of 0.3 pm was formed on a photoresist. A stamper was produced from the surface relief grating after photoresist development using a nickel electroforming method, and this stamper was used to stamp an acrylic plate with a hot press to form a wavelength plate.

(発明の効果) 本発明により製作の容易な表面レリーフ格子型の波長板
が得られる。
(Effects of the Invention) The present invention provides a surface relief grating type wave plate that is easy to manufacture.

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

図は本発明の実施例を模式的に示す斜視図である。 The figure is a perspective view schematically showing an embodiment of the present invention.

Claims (1)

【特許請求の範囲】[Claims] 誘電体に、使用波長をλ、格子ピッチをdとして2>λ
/d■1.472なる表面レリーフ格子を形成したこと
を特徴とする波長板。
For the dielectric material, 2>λ, where the wavelength used is λ and the grating pitch is d.
A wavelength plate characterized by forming a surface relief grating of /d■1.472.
JP1238086A 1986-01-22 1986-01-22 Wavelength plate Pending JPS62170902A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1238086A JPS62170902A (en) 1986-01-22 1986-01-22 Wavelength plate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1238086A JPS62170902A (en) 1986-01-22 1986-01-22 Wavelength plate

Publications (1)

Publication Number Publication Date
JPS62170902A true JPS62170902A (en) 1987-07-28

Family

ID=11803665

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1238086A Pending JPS62170902A (en) 1986-01-22 1986-01-22 Wavelength plate

Country Status (1)

Country Link
JP (1) JPS62170902A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0396902A (en) * 1989-09-08 1991-04-22 Sharp Corp Optical element
US6922516B2 (en) 2002-01-15 2005-07-26 Sumitomo Electric Industries, Ltd. Releasing mechanism of an optical module from a host board
WO2007142179A1 (en) * 2006-06-07 2007-12-13 Konica Minolta Holdings, Inc. Quarter-wave plate, and optical pickup device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0396902A (en) * 1989-09-08 1991-04-22 Sharp Corp Optical element
US6922516B2 (en) 2002-01-15 2005-07-26 Sumitomo Electric Industries, Ltd. Releasing mechanism of an optical module from a host board
US7108429B2 (en) 2002-01-15 2006-09-19 Sumitomo Electric Industries, Ltd. Releasing mechanism of an optical module from a host board
WO2007142179A1 (en) * 2006-06-07 2007-12-13 Konica Minolta Holdings, Inc. Quarter-wave plate, and optical pickup device
US8000210B2 (en) 2006-06-07 2011-08-16 Konica Minolta Holdings, Inc. Quarter-wave plate, and optical pickup device

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