JPS5913224A - Polarizing element - Google Patents

Polarizing element

Info

Publication number
JPS5913224A
JPS5913224A JP12264182A JP12264182A JPS5913224A JP S5913224 A JPS5913224 A JP S5913224A JP 12264182 A JP12264182 A JP 12264182A JP 12264182 A JP12264182 A JP 12264182A JP S5913224 A JPS5913224 A JP S5913224A
Authority
JP
Japan
Prior art keywords
film
polarizing element
light
separated
polarizing
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
JP12264182A
Other languages
Japanese (ja)
Other versions
JPH0372961B2 (en
Inventor
Masataka Shirasaki
白崎 正孝
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP12264182A priority Critical patent/JPS5913224A/en
Priority to EP83304027A priority patent/EP0100178B1/en
Priority to DE8383304027T priority patent/DE3378140D1/en
Publication of JPS5913224A publication Critical patent/JPS5913224A/en
Priority to US06/815,279 priority patent/US4641926A/en
Publication of JPH0372961B2 publication Critical patent/JPH0372961B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/30Polarising elements
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/28Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising
    • G02B27/283Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising used for beam splitting or combining

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)

Abstract

PURPOSE:To reduce the distance between separated projected light beams, to improve operation efficiency, and to perform high-speed operation by providing a polarizing separation film at part of one surface of a transparent flat plate which has parallel planes and a light reflecting film at part of the other surface. CONSTITUTION:The polarizing separation film 32 made of a dielectric multilayered film is formed at part of one surface of the parallelplane glass plate 31 with about 1mm. thickness, and the reflecting film 33 (thin metallic film or dielectric multilayered film) is formed at part of the other surface. Incident light in a direction X3 is separated by the polarizing element into a horizontal polarized wave Y3 and a vertical polarized wave Y4. In this case, the distance (dl) between the emitted light beams Y3 and Y4 is as shown by an equation, where (i) is the angle of incidence of the light in the direction X3, (t) is the thickness of the plate 31, and (n) is a refractive index. Consequently, the distance between the emitted light beams separated by the polarizing element is reduced, a Faraday rotating element is reduced in size, and high-speed operation is realized.

Description

【発明の詳細な説明】 (a)発明の技術分野 本発明は、光回路素子に係り、とくに光スィッチ、光サ
ーキュレータ−等に用いられる偏光素子□に関する。
DETAILED DESCRIPTION OF THE INVENTION (a) Technical Field of the Invention The present invention relates to optical circuit elements, and particularly to polarizing elements □ used in optical switches, optical circulators, and the like.

(b)技術の背景 現在実用化されている光回路においては、第1図に示す
ような偏光素子1および2とファラデー回転素子3から
成る光スィッチが用いられている。
(b) Background of the Technology In optical circuits currently in practical use, an optical switch consisting of polarizing elements 1 and 2 and a Faraday rotation element 3 as shown in FIG. 1 is used.

またこれらの組合・Uを基本として成る光サーキュレー
タ−等も用いられている。
Optical circulators based on a combination of these U are also used.

第1図において、偏光素子lにXiの方向から入射した
光は偏光分離膜11によって水平偏波と垂直偏波とに分
離される。
In FIG. 1, light incident on the polarizing element 1 from the direction of Xi is separated by a polarization separation film 11 into horizontally polarized light and vertically polarized light.

すなわち、通當、入射光に含まれる水平偏波は偏光分離
膜を透過するのに対し、垂直偏波は該偏光分IIII!
l!!によって反射されるためである。
That is, generally, horizontally polarized waves contained in incident light are transmitted through the polarization separation film, whereas vertically polarized waves are transmitted by the polarized light component III!
l! ! This is because it is reflected by

第1図において、水平偏波は偏光分離膜11を透過し、
偏光素子1の反射面12によって反射された後、ファラ
デー回転素子3に入射し、−力、垂直偏波は偏光分離膜
11によって反射されファラデー回転素子3に入射する
In FIG. 1, the horizontally polarized wave passes through the polarization separation film 11,
After being reflected by the reflective surface 12 of the polarizing element 1 , it enters the Faraday rotation element 3 , and the -power and vertically polarized waves are reflected by the polarization separation film 11 and enter the Faraday rotation element 3 .

どれら分離された光は、ファラデー回転素子3によって
その偏光面を回転されない時にはファラデー偏光回転素
子3をそのまま透過し、偏光素子2に入射する。この場
合、偏光素子2の偏光分離膜21に入射した前記水平偏
波はこれを透過し、vlの方向に出射し、また前記垂直
偏波は偏光素子2の反射面22により反射され偏光分離
膜21に入射するが、ここで再び反射されMlの方向に
出射する。
When the polarization plane of any of the separated lights is not rotated by the Faraday rotation element 3, it passes through the Faraday polarization rotation element 3 as it is and enters the polarization element 2. In this case, the horizontally polarized wave that has entered the polarization separation film 21 of the polarization element 2 is transmitted through it and exits in the direction of vl, and the vertically polarized wave is reflected by the reflection surface 22 of the polarization element 2 and is reflected by the polarization separation film 21. The light enters 21, but is reflected again and exits in the direction of Ml.

上記において、偏光素子lにより分離された光がファラ
デー回転素子3によってその偏光面を90度回転される
時には、ファラデー回転素子3に入射した水平偏波は垂
直偏波になり、これは偏光素子2の偏光分離膜21によ
り反射されv2の方向に出射し、同様にしてファラデー
回転素子3に入射した垂直偏波ば水平偏波になり、これ
は偏光素子2゛の反射面22で反射された後偏光分離膜
21を透過してY2’(71力向に出射する。
In the above, when the light separated by the polarizing element 1 has its plane of polarization rotated by 90 degrees by the Faraday rotator 3, the horizontally polarized wave incident on the Faraday rotator 3 becomes vertically polarized wave, and this The vertically polarized wave reflected by the polarization separating film 21 and emitted in the direction of v2, and similarly incident on the Faraday rotator 3, becomes a horizontally polarized wave, which is reflected by the reflective surface 22 of the polarizer 2. The light passes through the polarization separation film 21 and is emitted in the Y2' (71) force direction.

このように、偏光素子lにより入射光を分離し、ファラ
デー回転素子3によりこれら分離された光の偏光面を回
転制御することによって偏光素子2からの光の出射方向
を切り換えることができる。
In this way, the direction of light emitted from the polarizing element 2 can be switched by separating the incident light by the polarizing element 1 and controlling the rotation of the polarization plane of the separated lights by the Faraday rotation element 3.

また、偏光素子lに×2の方向から入射する光について
も同様のことが可能であり、これによって入射方向の異
なる2つの光を選択的に取り出すこともできる。
Furthermore, the same thing can be done for the light that enters the polarizing element l from the x2 direction, and thereby it is also possible to selectively extract two lights that have different incident directions.

(C)従来技術と問題点 従来、上記偏光素子lにより分離された水平偏波と垂直
偏波の光路間の距Md (第1図参照)は105m 1
iii l&であづた。
(C) Prior art and problems Conventionally, the distance Md (see Figure 1) between the optical paths of horizontally polarized waves and vertically polarized waves separated by the polarizing element l is 105 m 1
iii l & azuta.

これは偏光素子1の幾何学的−1法、すなわら偏光分離
膜11の面と反射面12との間の距離に基づくものであ
って、従来の偏光素子の構造およびその製造方法ではこ
の距離をl龍以下にすることはきわめて困難であり、ま
たこれを実現するためには、製造コストが高くなる欠点
があった。
This is based on the geometrical -1 method of the polarizing element 1, that is, the distance between the surface of the polarization separation film 11 and the reflecting surface 12. It is extremely difficult to reduce the distance to less than one length, and achieving this has the drawback of increasing manufacturing costs.

すなわち、従来の構造の偏光素子は、第2図に示すAの
部分とBの部分とから成り、これらは別箇に製作され、
への部分に偏光分離膜11を設りた後Bの部分と貼り合
わせることによって製作されていた。しかも、これらに
おいて、面4と面5は正確に平行が保たれ、また面6と
面7は正確に同一平面上に在るように組立られ、かつ面
6.7.8および9には精密平面研摩加工が施されてい
ることが必要であり、このような構造によれば、偏光素
子が小型になる程取り扱いおよび精度の維持が困難にな
るためである。
That is, a polarizing element with a conventional structure consists of a part A and a part B shown in FIG. 2, which are manufactured separately.
It was manufactured by providing a polarization separation film 11 on the part B and then bonding it to the part B. Moreover, in these, surfaces 4 and 5 are precisely kept parallel, surfaces 6 and 7 are assembled so as to be exactly on the same plane, and surfaces 6, 7, 8, and 9 are precisely It is necessary that the polarizing element be subjected to surface polishing, and with such a structure, the smaller the polarizing element becomes, the more difficult it becomes to handle and maintain accuracy.

(d)発明の目的 本発明は、従来の偏光素子とは異なって、小型化、低コ
スト化が可能な新規な構造を有する偏光素子を提供する
ことを目的とする。
(d) Purpose of the Invention An object of the present invention is to provide a polarizing element having a novel structure that can be made smaller and lower in cost, unlike conventional polarizing elements.

(e)発明の構成 本発明は、平行平面を有する透明平板の片面、の一部に
偏光分離膜を、他の片面の一部に死反射膜を設けること
を特徴とする。        、(「)発明の実施例 以下本発明の実施例、を図面を参照して説明する。
(e) Structure of the Invention The present invention is characterized in that a polarized light separation film is provided on a part of one side of a transparent flat plate having parallel planes, and a dead reflection film is provided on a part of the other side. , (') Embodiments of the Invention Below, embodiments of the present invention will be described with reference to the drawings.

第゛3図は本発明による偏光素子の一実施例を示す模式
図である。
FIG. 3 is a schematic diagram showing an embodiment of a polarizing element according to the present invention.

同図において、31は厚さがl +n程度であり1.平
行平面を有するガラス板である。このガラス板31の一
力の面の一部に誘電体多層膜から成る偏光分離膜32を
形成し、他の面の一部に反射膜33(金属薄膜または誘
電体多層膜から成る)を形成する。
In the figure, 31 has a thickness of about l+n, and 1. It is a glass plate with parallel planes. A polarization separation film 32 made of a dielectric multilayer film is formed on a part of one side of the glass plate 31, and a reflective film 33 (made of a metal thin film or a dielectric multilayer film) is formed on a part of the other side. do.

これらの膜の形成は通糸の真空蒸着、あ番いはスパッタ
リングとフォトエツチングの技術を用いて行えばよい。
These films may be formed using thread vacuum deposition, sputtering, and photoetching techniques.

上記のようにして得られた偏光素子にx3の方向から入
射した光は、従来の偏光素子におりると同様に分離され
、同図の実線の径路にしたがって水平偏波はY3に、垂
直偏波はY4に出射する。
The light incident on the polarizing element obtained as described above from the direction The wave is emitted at Y4.

また、×4の方向から入射した光は、破線の径路にした
がって分離され、水平偏波はv4に、垂直偏波はY3に
出射する。
Further, the light incident from the x4 direction is separated according to the path indicated by the broken line, and the horizontally polarized wave is outputted to v4, and the vertically polarized wave is outputted to Y3.

これらの場合、出射光v3とv4の間の距1[dlは、
偏光素子に対するX3方向の光の入射角をi、ガラス板
31・の厚さをtまたその屈折率をnとするとdl=2
t−cosi−sini / (n” −5in’i 
芦であるから、t = l ma、1=45°、n=、
1.5とすると dl’= 1.26鶴 となる。
In these cases, the distance 1 [dl] between the output lights v3 and v4 is
If the incident angle of light in the X3 direction to the polarizing element is i, the thickness of the glass plate 31 is t, and its refractive index is n, then dl=2
t-cosi-sini / (n"-5in'i
Since it is a reed, t = l ma, 1 = 45°, n =,
If it is 1.5, then dl' = 1.26 cranes.

本発明によれば、ガラス板310両面の平行度が保たれ
ていればその厚さはさらに薄いものでも実施可能であり
、この厚さに比例してdlの値をさらに小さくすること
ができる。
According to the present invention, as long as the parallelism of both sides of the glass plate 310 is maintained, the thickness of the glass plate 310 can be even thinner, and the value of dl can be further reduced in proportion to this thickness.

第4図は本発明の他の実施例を示す模式図である。FIG. 4 is a schematic diagram showing another embodiment of the present invention.

同図に示す偏光素子は、第3図と同様にして偏光分離膜
32と反射111Ii33を設りられたガラス板31を
、該ガラス板31と同じ屈折率を有する直角プリズム4
1および42で両側から挾むようにして貼り合せ・体化
してものであり、同図(八)は貼り合せ前の斜視図、(
B)は貼り合せ後の断面図である。
The polarizing element shown in the same figure has a glass plate 31 provided with a polarization separation film 32 and a reflection 111Ii33 in the same manner as in FIG.
1 and 42 are attached and assembled from both sides, and Figure 8 (8) is a perspective view before attachment.
B) is a sectional view after bonding.

本構造の偏光素子の場合には、第4図(B)から明らか
なように、×5および×6から入射する光は偏光素子の
それぞれの面43および44に対しほぼ垂直に入射する
ために、入射面43あるいは44における反射損失が少
なくなり、また、偏光分M膜32とガラス板31との界
面における光の入射角および出射角が大きくなるために
、2つの偏波に対する分離性能を向上することができる
In the case of the polarizing element of this structure, as is clear from FIG. 4(B), the light incident from x5 and x6 is incident almost perpendicularly to the respective surfaces 43 and 44 of the polarizing element. , the reflection loss at the incident surface 43 or 44 is reduced, and the incident and exit angles of light at the interface between the polarization M film 32 and the glass plate 31 are increased, improving the separation performance for two polarized waves. can do.

(g)発明の効果 本発明によれば、偏光素子により分離された出射光の間
の距離を小さくすることが容易であり、これによってフ
ァラデー回転素子を小型化でき、その動作効率(一定の
印加電圧によって可能な偏光面の回転角の大さ)を向上
でき、また高速動作を可能にする効果がある。さらにま
た、構造およびその加工が比較的簡単であるため、低コ
ストで量産可能な偏光素子を提供できる効果がある。
(g) Effects of the Invention According to the present invention, it is easy to reduce the distance between the emitted lights separated by the polarizing element, thereby making it possible to miniaturize the Faraday rotator and its operating efficiency (constant applied voltage). This has the effect of increasing the degree of rotation angle of the plane of polarization that is possible depending on the voltage, and enabling high-speed operation. Furthermore, since the structure and processing thereof are relatively simple, it is possible to provide a polarizing element that can be mass-produced at low cost.

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

第1図は偏光素子を用いた光スィッチの概要を説明する
だめの図、第2図は従来の偏光素子の構造を示す図、第
3図および第4図は本発明による偏光素子の構造を示す
模式図である。 図においてlおよび2は偏光素子、3はファラデー回転
素子、4.5.6.7.8および9は面、11.21お
よび32は偏光分1i111N!ji、12および22
は反射面、3Iはガラス板、33は反射膜、4Iおよび
42は直角プリズム、43および44は入射面、45は
出射面、xl・・・×6は光の入射方向、v4・・・v
6は光の出射方向、dおよびdlは偏波間の距離である
。 第1図         α2I211乎5図 4 第4図 (A) 3 (B)
Figure 1 is a diagram for explaining the outline of an optical switch using a polarizing element, Figure 2 is a diagram showing the structure of a conventional polarizing element, and Figures 3 and 4 are diagrams showing the structure of a polarizing element according to the present invention. FIG. In the figure, l and 2 are polarization elements, 3 is a Faraday rotation element, 4.5.6.7.8 and 9 are planes, and 11.21 and 32 are polarization components 1i111N! ji, 12 and 22
is a reflective surface, 3I is a glass plate, 33 is a reflective film, 4I and 42 are right angle prisms, 43 and 44 are incident surfaces, 45 is an exit surface, xl...×6 is the incident direction of light, v4...v
6 is the light emission direction, and d and dl are the distances between polarized waves. Figure 1 α2I211义5Figure 4 Figure 4 (A) 3 (B)

Claims (1)

【特許請求の範囲】[Claims] 平行平面を有する透明平板の片面の一部に偏光分sum
を、他の片面の一部に光反射膜を設けることを特徴とす
る偏光素子
Polarized light component sum on a part of one side of a transparent flat plate with parallel planes
A polarizing element, characterized in that a light reflecting film is provided on a part of the other side.
JP12264182A 1982-07-14 1982-07-14 Polarizing element Granted JPS5913224A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP12264182A JPS5913224A (en) 1982-07-14 1982-07-14 Polarizing element
EP83304027A EP0100178B1 (en) 1982-07-14 1983-07-11 Polarizing elements
DE8383304027T DE3378140D1 (en) 1982-07-14 1983-07-11 Polarizing elements
US06/815,279 US4641926A (en) 1982-07-14 1985-12-26 Polarizing element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12264182A JPS5913224A (en) 1982-07-14 1982-07-14 Polarizing element

Publications (2)

Publication Number Publication Date
JPS5913224A true JPS5913224A (en) 1984-01-24
JPH0372961B2 JPH0372961B2 (en) 1991-11-20

Family

ID=14840992

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12264182A Granted JPS5913224A (en) 1982-07-14 1982-07-14 Polarizing element

Country Status (1)

Country Link
JP (1) JPS5913224A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6138934A (en) * 1984-07-30 1986-02-25 Yamaichi Electric Mfg Co Ltd Switch of optical path
JP2000249513A (en) * 1999-02-26 2000-09-14 Dr Johannes Heidenhain Gmbh Beam splitter structure group and interferometer with it

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5699538U (en) * 1979-12-27 1981-08-06
JPS56137329A (en) * 1980-03-28 1981-10-27 Fujitsu Ltd Polarized and separated light control device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5699538U (en) * 1979-12-27 1981-08-06
JPS56137329A (en) * 1980-03-28 1981-10-27 Fujitsu Ltd Polarized and separated light control device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6138934A (en) * 1984-07-30 1986-02-25 Yamaichi Electric Mfg Co Ltd Switch of optical path
JP2000249513A (en) * 1999-02-26 2000-09-14 Dr Johannes Heidenhain Gmbh Beam splitter structure group and interferometer with it

Also Published As

Publication number Publication date
JPH0372961B2 (en) 1991-11-20

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