Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6223841B2 - - Google Patents
[go: Go Back, main page]

JPS6223841B2 - - Google Patents

Info

Publication number
JPS6223841B2
JPS6223841B2 JP364879A JP364879A JPS6223841B2 JP S6223841 B2 JPS6223841 B2 JP S6223841B2 JP 364879 A JP364879 A JP 364879A JP 364879 A JP364879 A JP 364879A JP S6223841 B2 JPS6223841 B2 JP S6223841B2
Authority
JP
Japan
Prior art keywords
incident
prism
output
ray
ordinary
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.)
Expired
Application number
JP364879A
Other languages
Japanese (ja)
Other versions
JPS5595914A (en
Inventor
Satoru Iguchi
Mitsuaki Nishe
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.)
Sumitomo Electric Industries Ltd
Original Assignee
Sumitomo Electric Industries 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 Sumitomo Electric Industries Ltd filed Critical Sumitomo Electric Industries Ltd
Priority to JP364879A priority Critical patent/JPS5595914A/en
Publication of JPS5595914A publication Critical patent/JPS5595914A/en
Publication of JPS6223841B2 publication Critical patent/JPS6223841B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Optical Elements Other Than Lenses (AREA)

Description

【発明の詳細な説明】 本発明は特殊加工プリズムを用いた光スイツチ
及びそのプリズムに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical switch using a specially processed prism and its prism.

従来の光スイツチは第1図イに示す如くそれぞ
れ直交する偏波面を持つ常光線と異常光線から成
る二つの入射ビームA,Bを各別に偏光プリズム
1,2を通した後、これを電気光学効果等を有す
る光学結晶3に導き、前記結晶3を外部から4に
て示す如く電気的に制御し、さらに前記2光線を
検光プリズム5に導き、前記結晶3の制御により
出力側6にビームA又はBのいづれかを出力させ
る。また第1図ロに示す如く、入射ビームAを偏
光プリズム1により特定の偏光成分だけを取り出
し、これを光学結晶3に導き4に示す如く外部よ
り制御して偏光面を回転し、さらに偏波面により
出射方向を異にする検光プリズム5に導いて前記
光学結晶3を制御することにより、出射ビーム
C、出射ビームDのいずれかを出射する。
In a conventional optical switch, two incident beams A and B consisting of an ordinary ray and an extraordinary ray each having orthogonal polarization planes are passed through polarizing prisms 1 and 2, respectively, as shown in Fig. 1A. The two light beams are guided to an optical crystal 3 having effects, etc., and the crystal 3 is electrically controlled from the outside as shown at 4.The two light beams are then guided to an analyzing prism 5, and a beam is outputted to the output side 6 by controlling the crystal 3. Output either A or B. Further, as shown in FIG. By controlling the optical crystal 3 by guiding the beam to the analyzing prism 5 which has a different output direction, either the output beam C or the output beam D is output.

上記のイ,ロはいづれも直交する偏波面を持つ
偏光プリズム1を使用しているためこの偏光プリ
ズムにより3dBの損失を生ずる欠点がある。
In both A and B above, since the polarizing prism 1 having orthogonal polarization planes is used, this polarizing prism has the disadvantage of causing a loss of 3 dB.

本発明は上記の欠点を解消することを目的と
し、第1の発明は偏光子を使用することなく、光
スイツチを実現するためのプリズムである。該プ
リズムは、複屈折を有するプリズムの一対角隅に
傾斜反射面を形成し、前記反射面を除く入射面か
らそれぞれ直交する偏波面を有する常光線と異常
光線とより成る第1及び第2の光ビームを入射せ
しめ、且つ前記の常光線の一つを前記反射面にて
反射せしめ、対向面の反射面を除く出射面から第
1入射ビームの異常光線と第2入射ビームの常光
線、第2入射ビームの異常光線と第1ビームの常
光線とをそれぞれ合成して第1、第2出射ビーム
を出射せしめるものである。
The present invention aims to eliminate the above-mentioned drawbacks, and the first invention is a prism for realizing an optical switch without using a polarizer. The prism has an inclined reflective surface formed at one diagonal corner of the prism having birefringence, and has first and second rays each consisting of an ordinary ray and an extraordinary ray each having a plane of polarization perpendicular to an incident surface other than the reflective surface. A light beam is made incident, and one of the ordinary rays is reflected by the reflecting surface, and the extraordinary ray of the first incident beam, the ordinary ray of the second incident beam, and the The extraordinary rays of the two incident beams and the ordinary rays of the first beam are respectively combined to output the first and second output beams.

これを第2図にて具体的に説明すると第1図と
同一符号は同一部分を示し第2図中7は前記の特
殊加工を施こして対角隅に反射面を形成せる複屈
折を有するプリズム例えばカルサイトプリズムで
あつて、従来ビームセパレータとして用いられて
いるプリズムの二つの対角隅にそれぞれ傾斜反射
面8,9を加工研磨し、反射コーテイング又は金
属蒸着によつて鏡面を形成する。10,11は他
の対角隅の非加工部即ち非反射部分で光ビームを
透過する。
This will be explained in detail in Fig. 2. The same reference numerals as in Fig. 1 indicate the same parts, and 7 in Fig. 2 has birefringence that has been subjected to the above-mentioned special processing to form a reflective surface at the diagonal corner. The prism is, for example, a calcite prism, which is conventionally used as a beam separator, and two diagonal reflective surfaces 8 and 9 are machined and polished, respectively, and mirror surfaces are formed by reflective coating or metal vapor deposition. Reference numerals 10 and 11 are non-processed portions, that is, non-reflective portions at other diagonal corners, and transmit the light beam.

第1入射ビームAはプリズム7の非反射面即ち
透過面10に入射するとAの異常光線A2とAの
常光線A1に分れてそれぞれ対向非反射面11か
らそのままA2,A1として出射する。第2入射ビ
ームBはプリズム7の非反射面10に入射してB
の常光線B1とBの異常光線B2と分れる。この中
異常光線B2は非反射面11からそのまま出射し
第1入射ビームの常光線A1と合成されて第1出
射ビームDとなる。常光線B1は一対角隅傾斜反
射面9にて反射しさらに他の対角隅傾斜反射面8
にて再反射して非反射面11から出射して第1入
射ビームAの異常光線A2と合成されて第2出射
ビームCとなる。第1入射ビームAと第2入射ビ
ームBとの入射面に対する入射位置を上記の場合
と反対にしてもよい。
When the first incident beam A enters the non-reflecting surface, that is, the transmitting surface 10 of the prism 7, it is split into an extraordinary ray A 2 of A and an ordinary ray A 1 of A, which are then directly transmitted from the opposing non-reflecting surface 11 as A 2 and A 1 , respectively. Emits light. The second incident beam B is incident on the non-reflecting surface 10 of the prism 7 and
It is divided into the ordinary ray B1 of B and the extraordinary ray B2 of B. This medium extraordinary ray B 2 exits as it is from the non-reflecting surface 11 and is combined with the ordinary ray A 1 of the first incident beam to become the first outgoing beam D. The ordinary ray B 1 is reflected by one diagonal corner inclined reflecting surface 9 and then reflected by another diagonal corner inclined reflecting surface 8.
It is re-reflected at , exits from the non-reflective surface 11, and is combined with the extraordinary ray A2 of the first incident beam A to become a second outgoing beam C. The positions of incidence of the first incident beam A and the second incident beam B on the incident surface may be reversed from the above case.

上記のそれぞれ直交する偏波面を持つ二つの入
射ビームをプリズム内にて4本のビームに分離
し、前記4本のビームの中の任意のビームをプリ
ズム内で反射させて2本の出射ビームに合成する
ように反射面の傾斜角、傾斜面の長さ及び面積等
を調整加工することが望ましい。
The above two incident beams with orthogonal polarization planes are separated into four beams within the prism, and any beam among the four beams is reflected within the prism to form two output beams. It is desirable to adjust the angle of inclination of the reflecting surface, the length and area of the inclined surface, etc. so as to combine them.

第3図は本発明の特殊加工プリズムによる偏波
面を有する光ビームの合成方法を使用して構成せ
る2入力2出力の光スイツチを示すものであつ
て、第1図及び第2図と同一符号は同一部分を示
し、7,7′は複屈折を有するプリズム例えばカ
ルサイトプリズムで光学結晶を挾んでその前後に
配設し、前記プリズム7にそれぞれ直交する偏光
面を持つ第1入射ビームA及び第2入射ビームB
を入射せしめると、第1入射ビームAは2本のビ
ームに分離され光学結晶3により偏光面を回転さ
せられ再びプリズム7′によつて合成されて第1
出射C又は第2出射Dに出力される。第2入射ビ
ームBについても同様である。上記の2入力、2
出力の光スイツチに於ては偏光子を全然使用して
いないのでそれによる損失は発生しない。
FIG. 3 shows a 2-input, 2-output optical switch constructed using the method of synthesizing light beams having a polarization plane using a specially processed prism according to the present invention, and shows the same reference numerals as in FIGS. 1 and 2. 7 and 7' indicate the same part, and 7 and 7' are birefringent prisms, such as calcite prisms, which are placed in front and behind the optical crystal, and the first incident beams A and 7' have polarization planes perpendicular to the prism 7, respectively. Second incident beam B
When the first incident beam A is made incident, the first incident beam A is separated into two beams, the plane of polarization is rotated by the optical crystal 3, and the first incident beam A is combined by the prism 7' again.
It is output to the output C or the second output D. The same applies to the second incident beam B. 2 inputs above, 2
Since no polarizer is used in the output optical switch, no loss occurs due to it.

本発明の特殊加工プリズムによる偏波面を有す
る光ビームの合成方法は偏光子を全然使用してい
ないのでそれによる損失を発生せず、極めて能率
良く光の合成を行うことが出来る。
The method of synthesizing light beams having polarization planes using a specially processed prism of the present invention does not use any polarizers, so there is no loss due to polarizers, and light can be synthesized extremely efficiently.

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

第1図イ,ロは従来の偏光子を使用する偏波面
を有する光ビームの光スイツチの説明図、第2図
は本発明の特殊加工を施こしたプリズムによる偏
波面を有する光ビームの合成方法の実施の態様を
示す正面図、第3図は本発明に使用せるプリズム
を使用せる光スイツチの説明図である。 1,2は偏光子、3は光学結晶、4は外部制御
手段、5は検光子、6は出力、7,7′は反射面
を形成せるカルサイトプリズム、8,8′,9,
9′は対角隅傾斜反射面、10,11は前記反射
面を除く入射面、A,Bは入射ビーム、C,Dは
出射ビーム。
Figure 1 A and B are explanatory diagrams of an optical switch for a light beam with a polarization plane using a conventional polarizer, and Figure 2 is a synthesis of a light beam with a polarization plane using a specially processed prism according to the present invention. FIG. 3 is a front view showing an embodiment of the method, and is an explanatory diagram of an optical switch using a prism used in the present invention. 1 and 2 are polarizers, 3 is an optical crystal, 4 is an external control means, 5 is an analyzer, 6 is an output, 7 and 7' are calcite prisms that form reflective surfaces, 8, 8', 9,
9' is a diagonal corner inclined reflecting surface, 10 and 11 are incident surfaces excluding the reflecting surface, A and B are incident beams, and C and D are output beams.

Claims (1)

【特許請求の範囲】 1 外部制御手段4を有する光学結晶3をはさん
で、その前後に複屈折を有するプリズムの一対角
隅に傾斜反射面8,9,8′,9′を付加して形成
されたプリズム7,7′が配置されて構成され、 光学結晶3の前に配置されたプリズム7の前記
反射面を除く入射面10からそれぞれ直交する偏
波面を有する常光線と異常光線とより成る第1及
び第2の光ビームA,A1,A2、B,B1,B2を入
射し、光学結晶3を通過した後、プリズム7′の
出射面11′から第1及び第2出射ビームC,
A1,A2、D,B1,B2を出射せしめ、 かつ、外部制御手段4によつて光学結晶3を通
過する光ビームの偏光面を回転することによつ
て、第1出射ビーム及び第2出射ビームの出射位
置が切替えられることを特徴とする光スイツチ。 2 複屈折を有するプリズムの一対角隅に傾斜反
射面8,9を付加して形成されたプリズム7に関
し、 前記反射面を除く入射面10からそれぞれ直交
する偏波面を有する常光線と異常光線とより成る
第1及び第2の光ビームA,A1,A2、B,B1
B2を入射せしめ、且つ前記常光線の一つB1を前
記反射面8,9にて反射せしめ、対向面の反射面
を除く出射面11から第1入射ビームの異常光線
A2と第2入射ビームの常光線B1、、第2入射ビー
ムの異常光線B2と第1入射ビームの常光線A1
をそれぞれ合成して、第1、第2出射ビームC,
A2,B1、D,A1,B2が出射することを特徴とす
る光スイツチのプリズム。
[Claims] 1. An optical crystal 3 having an external control means 4 is sandwiched therebetween, and inclined reflecting surfaces 8, 9, 8', and 9' are added to one diagonal corner of a prism having birefringence before and after the optical crystal 3. The formed prisms 7 and 7' are arranged to form an ordinary ray and an extraordinary ray, each having a plane of polarization perpendicular to the incident surface 10 excluding the reflecting surface of the prism 7 disposed in front of the optical crystal 3. The first and second light beams A, A 1 , A 2 , B, B 1 , B 2 are incident, and after passing through the optical crystal 3, the first and second light beams are Outgoing beam C,
The first output beam and An optical switch characterized in that the output position of the second output beam is switched. 2 Regarding the prism 7 formed by adding inclined reflective surfaces 8 and 9 to one diagonal corner of a prism having birefringence, ordinary rays and extraordinary rays having orthogonal polarization planes from the incident surface 10 excluding the reflective surface First and second light beams A, A 1 , A 2 , B, B 1 ,
B 2 is made incident, one of the ordinary rays B 1 is reflected by the reflecting surfaces 8 and 9, and an extraordinary ray of the first incident beam is made from the exit surface 11 excluding the reflecting surface of the opposing surface.
A 2 and the ordinary ray B 1 of the second incident beam, , the extraordinary ray B 2 of the second incident beam and the ordinary ray A 1 of the first incident beam are combined to form the first and second output beams C,
A prism for an optical switch, characterized in that A 2 , B 1 , D, A 1 , and B 2 are emitted.
JP364879A 1979-01-16 1979-01-16 Synthesizing method of light beam having plane of polarization by prism Granted JPS5595914A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP364879A JPS5595914A (en) 1979-01-16 1979-01-16 Synthesizing method of light beam having plane of polarization by prism

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP364879A JPS5595914A (en) 1979-01-16 1979-01-16 Synthesizing method of light beam having plane of polarization by prism

Publications (2)

Publication Number Publication Date
JPS5595914A JPS5595914A (en) 1980-07-21
JPS6223841B2 true JPS6223841B2 (en) 1987-05-26

Family

ID=11563289

Family Applications (1)

Application Number Title Priority Date Filing Date
JP364879A Granted JPS5595914A (en) 1979-01-16 1979-01-16 Synthesizing method of light beam having plane of polarization by prism

Country Status (1)

Country Link
JP (1) JPS5595914A (en)

Also Published As

Publication number Publication date
JPS5595914A (en) 1980-07-21

Similar Documents

Publication Publication Date Title
US5930038A (en) Optical isolator with polarization dispersion and differential transverse deflection correction
US6055104A (en) Optical attenuator
US5223975A (en) Polarization beam coupler including a splitter for producing an output monitor beam
US4917461A (en) Achromatic infrared retarder
US6545805B2 (en) Polarization-dependent retroreflection mirror device
US6246518B1 (en) Reflection type optical isolator
JPH07281128A (en) Optical isolator
JPH0219702A (en) Optical feedback isolator
US3442571A (en) Prismatic member for differentially changing directions of light beams incident thereon
JPS61122624A (en) Optical isolator
JPS6223841B2 (en)
JP2002296544A (en) 3-port miniaturized optical circulator
US5724184A (en) Polarizer with birefringent plate
JP2721879B2 (en) Self-temperature compensated optical isolator
JP2761141B2 (en) Polarization rotating mirror
JPH0820623B2 (en) Optical isolator
JPS6230607B2 (en)
US5864428A (en) Polarizing device
JP2775103B2 (en) Polarizing prism
JPS60238813A (en) Optical isolator
JPH0830789B2 (en) Polarization splitting prism
JP3492736B2 (en) Optical isolator
JPS63220109A (en) Deflection separating/synthesizing prism
JPS6264969A (en) Fiber optic current sensor
JPS61113003A (en) Dielectric multilayered film polarizer