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JP3465804B2 - Method for measuring light transmission characteristics of wedge-type birefringent plate - Google Patents
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JP3465804B2 - Method for measuring light transmission characteristics of wedge-type birefringent plate - Google Patents

Method for measuring light transmission characteristics of wedge-type birefringent plate

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Publication number
JP3465804B2
JP3465804B2 JP18985695A JP18985695A JP3465804B2 JP 3465804 B2 JP3465804 B2 JP 3465804B2 JP 18985695 A JP18985695 A JP 18985695A JP 18985695 A JP18985695 A JP 18985695A JP 3465804 B2 JP3465804 B2 JP 3465804B2
Authority
JP
Japan
Prior art keywords
wedge
shaped birefringent
light
birefringent plate
shaped
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 - Fee Related
Application number
JP18985695A
Other languages
Japanese (ja)
Other versions
JPH0915092A (en
Inventor
利光 稲垣
明夫 高橋
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.)
FDK Corp
Original Assignee
FDK 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 FDK Corp filed Critical FDK Corp
Priority to JP18985695A priority Critical patent/JP3465804B2/en
Publication of JPH0915092A publication Critical patent/JPH0915092A/en
Application granted granted Critical
Publication of JP3465804B2 publication Critical patent/JP3465804B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Testing Of Optical Devices Or Fibers (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、光アイソレータの
構成部品である楔型複屈折板の製作後に行われる楔型複
屈折板の光透過特性を測定する方法の改良に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a method for measuring light transmission characteristics of a wedge-shaped birefringent plate, which is performed after manufacturing a wedge-shaped birefringent plate which is a component of an optical isolator.

【0002】[0002]

【従来の技術】光アイソレータの代表的なものとして、
次のような構成が知られている(例えば特公昭61−5
8809号公報等)。図3に示すように、偏光子および
検光子となる2枚の楔型複屈折板1a,1bの間に45
度ファラデー回転子2を配設し、入力側の光ファイバ3
とカップリングレンズ4を楔型複屈折板1aの側に組み
合わせ、出力側の光ファイバ5とカップリングレンズ6
を楔型複屈折板1bの側に組み合わせている。
2. Description of the Related Art As a typical optical isolator,
The following structure is known (for example, Japanese Patent Publication No. 61-5).
8809 publication). As shown in FIG. 3, between the two wedge-shaped birefringent plates 1a and 1b, which serve as a polarizer and an analyzer, 45
The Faraday rotator 2 is installed, and the optical fiber 3 on the input side is provided.
And the coupling lens 4 on the side of the wedge-shaped birefringent plate 1a, and the optical fiber 5 on the output side and the coupling lens 6 are combined.
On the side of the wedge-shaped birefringent plate 1b.

【0003】偏光子としての楔型複屈折板1aの光学軸
に対して検光子としての楔型複屈折板1bの光学軸がな
す角度を、ファラデー回転子2による偏光面の回転方向
に45度に設定している。なお、2枚の楔型複屈折板1
a,1bは同じ構成であるので、本明細書では以下両者
を区別しないときには楔型複屈折板1と記す。
The angle formed by the optical axis of the wedge type birefringent plate 1b as an analyzer with respect to the optical axis of the wedge type birefringent plate 1a as a polarizer is 45 degrees in the rotation direction of the plane of polarization by the Faraday rotator 2. Is set to. Two wedge-shaped birefringent plates 1
Since a and 1b have the same structure, they are referred to as wedge-shaped birefringent plate 1 in the following description when they are not distinguished from each other.

【0004】よく知られているように、複屈折結晶の大
きなインゴットから多数の楔型複屈折板1が切り出され
て仕上げ加工される。その形状を図4に詳しく示してい
る。この例の楔型複屈折板1は外形がほぼ正方形の薄板
であり、光学軸Qと平行な主平面Rと、この主平面Rに
対して適宜角度傾斜した傾斜平面Sとで挟まれた楔型に
加工されている。そして主平面Rと傾斜平面Sは鏡面仕
上げされ、さらに反射防止膜がコーティングされる。
As is well known, a large number of wedge-shaped birefringent plates 1 are cut out from a large ingot of a birefringent crystal and finished. The shape is shown in detail in FIG. The wedge-shaped birefringent plate 1 of this example is a thin plate having a substantially square outer shape, and is wedged between a main plane R parallel to the optical axis Q and an inclined plane S inclined at an appropriate angle with respect to the main plane R. It is processed into a mold. Then, the main plane R and the inclined plane S are mirror-finished and further coated with an antireflection film.

【0005】光アイソレータの製造・組立プロセスにお
いては、不良部品を排除するなどの目的で、仕上げ加工
された楔型複屈折板の光透過率を測定することが望まし
い。その測定方法の一例を説明すると、図5に示すよう
に、測定光を発する投光器7と光検出器8とを光軸を合
せて対向配置し(二点鎖線参照)、その中間位置に測定
しようとする楔型複屈折板1を置く。この状態で投光器
7からの測定光を楔型複屈折板1の主平面Rに垂直に入
射し、傾斜平面Sからの出射光を光検出器8で受光する
ようにする。これにより、入射光と出射光の光度差等を
求めることにより楔型複屈折板1の光透過率を求めるこ
とができる。
In the process of manufacturing and assembling the optical isolator, it is desirable to measure the light transmittance of the finished wedge-type birefringent plate for the purpose of eliminating defective parts. Explaining an example of the measuring method, as shown in FIG. 5, the light projector 7 and the photodetector 8 which emit the measuring light are arranged so as to face each other with their optical axes aligned (see the chain double-dashed line), and measure at an intermediate position therebetween. The wedge-shaped birefringent plate 1 is placed. In this state, the measurement light from the light projector 7 is vertically incident on the main plane R of the wedge-shaped birefringent plate 1, and the light emitted from the inclined plane S is received by the photodetector 8. Thereby, the light transmittance of the wedge-shaped birefringent plate 1 can be obtained by obtaining the difference in luminous intensity between the incident light and the emitted light.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、上記し
た従来の測定方法では、楔型複屈折板1の透過光を光検
出器8により高精度に測定できないという問題がある。
つまり図5に示すように、楔型複屈折板1の主平面Rに
垂直に測定光を入射しても、傾斜平面Sから出射する光
は入射光と平行ではなく、しかも常光と異常光とに分れ
て異なる角度で互いに離れる方向に出射する。したがっ
て、図3に示すように、単純に楔型複屈折板1の設置前
の状態で投光器7と光検出器8の光軸を一致させたとし
ても、図中破線で示すように楔型複屈折板1を透過した
出射光の全部を光検出器8で受光することはできず、し
かも受光している部分も光検出器8の最高感度ポイント
ではなく、正確な測定はできない。
However, the above-mentioned conventional measuring method has a problem that the transmitted light of the wedge-shaped birefringent plate 1 cannot be measured with high accuracy by the photodetector 8.
That is, as shown in FIG. 5, even if the measurement light is incident perpendicularly to the main plane R of the wedge-shaped birefringent plate 1, the light emitted from the inclined plane S is not parallel to the incident light, and is an ordinary ray and an extraordinary ray. And are emitted in directions away from each other at different angles. Therefore, as shown in FIG. 3, even if the optical axes of the projector 7 and the photodetector 8 are simply made to coincide with each other in a state before the wedge-shaped birefringent plate 1 is installed, the wedge-shaped birefringent plate 1 as shown by the broken line in FIG. The emitted light transmitted through the refraction plate 1 cannot be entirely received by the photodetector 8, and the receiving portion is not the highest sensitivity point of the photodetector 8 and accurate measurement cannot be performed.

【0007】したがって、このように常光と異常光とに
分れて広がる出射光を光検出器8の最高感度ポイントで
受光して高精度に測定するためには、ある測定対象物
(楔型複屈折板1)をセットし、その出射光に対して最
大の感度を示すように光検出器8の位置を微調整する必
要がある。こうすれば正確に測定できるが、次の測定対
象物に交換したときには、また光検出器8の位置調整を
行わなければならない。これでは多量の楔型複屈折板を
次々と能率よく測定できず、このような全数試験はほと
んど行われていないのが実情である。
Therefore, in order to receive the emitted light that is divided into ordinary light and extraordinary light and spread at the highest sensitivity point of the photodetector 8 and measure it with high accuracy, a certain object to be measured (a wedge-shaped compound) It is necessary to set the refraction plate 1) and finely adjust the position of the photodetector 8 so as to show the maximum sensitivity to the emitted light. Although accurate measurement can be performed in this way, the position of the photodetector 8 must be adjusted again when the object to be measured is replaced next time. This makes it impossible to measure a large number of wedge-shaped birefringent plates one after another efficiently, and it is the actual situation that such an exhaustive test is hardly conducted.

【0008】上記した問題に鑑み、本発明者らは従来、
次のような光透過率試験を行っている。楔型複屈折板の
素材である複屈折結晶インゴットから光透過率試験用の
試料を切り出す。その試料は実際の製品のように楔型で
はなく、表面と裏面が平行な平板とする。しかも光学軸
が表裏面と垂直になるように加工する。そしてこの試料
を図5のような投光器7と光検出器8の間に測定光に対
して垂直に配置する。この場合、入射光と光軸の方向が
一致しているので、内部で常光と異常光に分離されるこ
とはなくそのまま試料内を直進し、そのまま出射する。
よって、入射光と出射光が同一直線状に位置するので、
投光器7と光検出器8の光軸を一致させておけば出射光
のすべてを受光することができる。しかしながら、この
試験はあくまでも素材インゴットの光透過率を測定して
いるのであり、このインゴットから加工された多数の個
々の楔型複屈折板の不良を見つけるための試験としては
不適切である。
In view of the above problems, the present inventors have
The following light transmittance tests are conducted. A sample for a light transmittance test is cut out from a birefringent crystal ingot which is a material for a wedge-shaped birefringent plate. The sample is not a wedge type like the actual product, but a flat plate whose front and back surfaces are parallel. Moreover, processing is performed so that the optical axis is perpendicular to the front and back surfaces. Then, this sample is arranged perpendicular to the measurement light between the light projector 7 and the photodetector 8 as shown in FIG. In this case, since the incident light and the direction of the optical axis coincide with each other, the ordinary light and the extraordinary light are not separated inside and the light travels straight through the sample and is emitted as it is.
Therefore, since the incident light and the emitted light are located on the same straight line,
If the optical axes of the projector 7 and the photodetector 8 are aligned with each other, all the emitted light can be received. However, this test only measures the light transmittance of the material ingot, and is unsuitable as a test for finding defects in a large number of individual wedge-shaped birefringent plates processed from this ingot.

【0009】本発明は、上記した背景に鑑みてなされた
もので、その目的とするところは、上記した問題点を解
決し、測定対象物を交換するごとに測定機器の位置調整
などを行わずに、個々の楔型複屈折板の光透過特性を能
率よく高精度に測定する楔型複屈折板の光透過特性の測
定方法を提供することにある。
The present invention has been made in view of the above background, and an object of the present invention is to solve the above-mentioned problems and to adjust the position of the measuring device every time the object to be measured is replaced. Another object of the present invention is to provide a method for measuring the light transmission characteristics of each wedge-shaped birefringent plate that efficiently and accurately measures the light transmission characteristics of each wedge-shaped birefringence plate.

【0010】[0010]

【課題を解決するための手段】上記した目的を達成する
ため、本発明に係る楔型複屈折板の光透過特性の測定方
法では、光学軸Qと平行な主平面Rと、この主平面Rに
対して適宜角度傾斜した傾斜平面Sとで挟まれた形状の
楔型複屈折板の光透過特性を測定するにあたり、2枚の
楔型複屈折板を用意する。そして、一方の楔型複屈折板
の傾斜平面Sと他方の楔型複屈折板の主平面Rとを対向
させるとともに、両楔型複屈折板の光学軸を合わせるよ
うに両者を配置する。この状態で、一方の楔型複屈折板
の主平面Rまたは他方の楔型複屈折板の傾斜平面Sに測
定光を入射させ、その出射光を光検出器で受光するよう
にした(請求項1)。
In order to achieve the above object, in the method for measuring the light transmission characteristics of a wedge-shaped birefringent plate according to the present invention, a main plane R parallel to the optical axis Q and this main plane R On the other hand, two wedge-shaped birefringent plates are prepared in order to measure the light transmission characteristics of the wedge-shaped birefringent plate which is sandwiched between the inclined plane S inclined by an appropriate angle. Then, the inclined plane S of one wedge-shaped birefringent plate and the main plane R of the other wedge-shaped birefringent plate are opposed to each other, and both are arranged so that the optical axes of both wedge-shaped birefringent plates are aligned. In this state, the measuring light is made incident on the main plane R of one wedge-shaped birefringent plate or the inclined plane S of the other wedge-shaped birefringent plate, and the emitted light is received by the photodetector (claim 3). 1).

【0011】そして好ましくは、前記両楔型複屈折板を
配置するに際し、前記一方の楔型複屈折板の主平面Rと
前記他方の楔型複屈折板の傾斜平面Sとが平行になるよ
うにすることである(請求項2)。
Preferably, when disposing the both wedge-shaped birefringent plates, the main plane R of the one wedge-shaped birefringent plate and the inclined plane S of the other wedge-shaped birefringent plate are parallel to each other. (Claim 2).

【0012】所定の相対位置関係で重なった2枚の楔型
複屈折板に対し、たとえば垂直に測定光を入射すると、
入射側の楔型複屈折板内ではそのまま直進するが、その
楔型複屈折板から出射する際に、常光と異常光に分離さ
れて進む。そして、本発明では両楔型複屈折板の光学軸
を合わせていたため、上記常光と異常光は、次の楔型複
屈折番においても同様に常光と異常光の状態を保持す
る。したがって、上記のように一度分離されて互いに離
れる方向に進んだ常光と異常光は次の楔型複屈折板内を
進む間に互いに接近する方向に進む。よってそれぞれの
楔型複屈折板で生じる複屈折が相殺され、出射する光は
入射光と平行になる。したがって出射光を光検出器で正
確に受光・測定される。
When the measuring light is vertically incident on the two wedge-shaped birefringent plates which are superposed in a predetermined relative positional relationship,
In the wedge-shaped birefringent plate on the incident side, it goes straight as it is, but when it exits from the wedge-shaped birefringent plate, it is separated into ordinary light and extraordinary light. Further, in the present invention, since the optical axes of both wedge-shaped birefringent plates are aligned with each other, the ordinary light and the extraordinary light similarly maintain the ordinary light and the extraordinary light in the next wedge-shaped birefringence number. Therefore, as described above, the ordinary light and the extraordinary light, which are once separated and proceed in a direction away from each other, proceed in a direction approaching each other while proceeding in the next wedge-shaped birefringent plate. Therefore, the birefringence generated in each wedge-shaped birefringent plate is canceled, and the emitted light becomes parallel to the incident light. Therefore, the emitted light can be accurately received and measured by the photodetector.

【0013】[0013]

【発明の実施の形態】以下、本発明に係る楔型複屈折板
の光透過特性の測定方法の好適な実施例を添付図面を参
照にして詳述する。図1,図2は本発明の測定方法の一
実施例を示している。同図に示すように、光学軸Qと平
行な主平面Rと、この主平面Rに対して適宜角度傾斜し
た傾斜平面Sとで挟まれた形状の楔型複屈折板1の光透
過特性を測定するにあたり、2枚の楔型複屈折板1a,
1bを用意する。そして、一方の楔型複屈折板1aの傾
斜平面Sと他方の楔型複屈折板1bの主平面Rとを対向
させ、しかも、楔型複屈折板1aの主平面Rと楔型複屈
折板1bの傾斜平面Sとが平行になるように両者を重ね
合わせる。測定対象の2つの楔型複屈折板1a,1bは
素材インゴットの光学軸に対して同じ方向性条件で切り
出されているので、楔型複屈折板1aの主平面Rと垂直
方向に見て両楔型複屈折板の光学軸Qは平行に揃う。
BEST MODE FOR CARRYING OUT THE INVENTION Preferred embodiments of a method for measuring light transmission characteristics of a wedge-shaped birefringent plate according to the present invention will be described in detail below with reference to the accompanying drawings. 1 and 2 show an embodiment of the measuring method of the present invention. As shown in the figure, the light transmission characteristic of the wedge-shaped birefringent plate 1 having a shape sandwiched between a main plane R parallel to the optical axis Q and an inclined plane S inclined at an appropriate angle with respect to the main plane R is shown. In measuring, two wedge-shaped birefringent plates 1a,
Prepare 1b. The inclined plane S of the one wedge-shaped birefringent plate 1a and the main plane R of the other wedge-shaped birefringent plate 1b are opposed to each other, and the main plane R of the wedge-shaped birefringent plate 1a and the wedge-shaped birefringent plate 1a. Both are superposed so that the inclined plane S of 1b is parallel. Since the two wedge-shaped birefringent plates 1a and 1b to be measured are cut out under the same directional condition with respect to the optical axis of the material ingot, both are seen in the direction perpendicular to the main plane R of the wedge-shaped birefringent plate 1a. The optical axes Q of the wedge-shaped birefringent plates are aligned in parallel.

【0014】係る2枚重ねの楔型複屈折板1a,1bを
投光器7と光検出器8の中間に配置し、楔型複屈折板1
aの主平面Rに垂直に測定光を入射し、楔型複屈折板1
bの傾斜平面Sからの出射光を光検出器8で受光する。
The two wedge-shaped birefringent plates 1a and 1b are placed in the middle of the projector 7 and the photodetector 8 to form the wedge-shaped birefringent plate 1.
The measurement light is incident perpendicularly to the main plane R of a, and the wedge-shaped birefringent plate 1
Light emitted from the inclined plane S of b is received by the photodetector 8.

【0015】すると、最初に照射される一方の楔型複屈
折板1aに対しての入射光の入射方向は、水平面Rの法
線方向と等しい(入射角が0)ので、常光と異常光はそ
のまま直進する。そして、傾斜平面Sから出射する際に
は、楔型複屈折板1a内を進む常光及び異常光はその傾
斜平面Sの法線に対して所定角度で入射されるので、そ
の出射光は常光は法線に近づく方向に屈折し、異常光は
法線から離れる方向に屈折するので、出射した常光及び
異常光は、図1中に示すように互いに離れるように進
む。
Then, since the incident direction of the incident light on the one wedge-shaped birefringent plate 1a which is first irradiated is equal to the normal direction of the horizontal plane R (incident angle is 0), the ordinary ray and the extraordinary ray are Continue straight ahead. Then, when the ordinary light and the extraordinary light traveling in the wedge-shaped birefringent plate 1a are incident on the inclined plane S at a predetermined angle with respect to the normal line of the inclined plane S, the emitted light is the ordinary light. Since the extraordinary light is refracted in a direction approaching the normal line and the extraordinary light is refracted in a direction away from the normal line, the emitted ordinary light and extraordinary light travel away from each other as shown in FIG.

【0016】そして、そのまま次の他方の楔型複屈折板
1bに入射する。すると、その主平面Rを通過する際に
各光は所定方向に屈折するが、両楔型複屈折板1a,1
bは光学軸を合わせているので、楔型複屈折板1bに入
射する際の常光及び異常光はそのままの状態を保持する
ので、異常光の方が屈折角が大きくしかも境界面の前後
の屈折率の大小関係が楔型複屈折板1aの傾斜平面Sに
おけるそれと逆であるので、結局楔型複屈折板1aで生
じる複屈折による2光線の分離作用が相殺される方向に
屈折し、楔型複屈折板1b内を進む。さらに、本実施例
では、両楔型複屈折板1a,1bの対向面を平行に配置
したため、楔型複屈折板1bの出射面である傾斜平面S
に到達した際には、常光と異常光は一点に収束し、その
後両光は一致(合成)した状態で出射される。そしてこ
のときの出射光は入射光と平行で同一直線上となる。
Then, the light enters the other wedge-shaped birefringent plate 1b as it is. Then, while each light is refracted in a predetermined direction when passing through the main plane R, the two wedge-shaped birefringent plates 1a, 1
Since b has its optical axis aligned, the ordinary light and the extraordinary light when entering the wedge-shaped birefringent plate 1b maintain the same state, so that the extraordinary light has a larger refraction angle and refraction before and after the boundary surface. Since the magnitude relationship of the indices is opposite to that in the inclined plane S of the wedge-shaped birefringent plate 1a, the two-ray splitting effect due to the birefringence generated in the wedge-shaped birefringent plate 1a is refracted in a direction canceling the wedge-shaped birefringent plate 1a. Proceed inside the birefringent plate 1b. Further, in this embodiment, since the opposing surfaces of the wedge-shaped birefringent plates 1a and 1b are arranged in parallel, the inclined plane S which is the emission surface of the wedge-shaped birefringent plate 1b.
When the light reaches, the ordinary light and the extraordinary light converge to one point, and then both lights are emitted in a state of being coincident (combined). The emitted light at this time is parallel to the incident light and is on the same straight line.

【0017】したがって、投光器7と光検出器8の光軸
を一致させておくことで、正確に透過光を測定でき、測
定対象物を交換しても測定系の位置調整をしなおす必要
はない。これにより、実際の製品である楔型に加工した
状態の最終製品の状態でその透過率等の特性の良否の判
定が連続して短時間で行える。
Therefore, by making the optical axes of the light projector 7 and the photodetector 8 coincident with each other, the transmitted light can be measured accurately, and it is not necessary to readjust the position of the measuring system even if the object to be measured is replaced. . As a result, the quality of the characteristics such as the transmittance can be continuously determined in a short time in the state of the final product, which is an actual product processed into a wedge shape.

【0018】なお、同一インゴットから同一条件で加工
されたものであれば、2枚とも未知の楔型複屈折板1
a,1bを測定対象としてもよいし、測定済みの既知の
複屈折板と未知の楔型複屈折板とを組み合わせて測定し
てもよい。いずれでも楔型複屈折板の良品・不良品の判
定は問題なく行える。
If the same ingot is processed under the same conditions, both wedge-shaped birefringent plates 1 are unknown.
The measurement target may be a and 1b, or the measurement may be performed by combining a known birefringent plate that has been measured and an unknown wedge-shaped birefringent plate. In either case, it is possible to judge whether the wedge-shaped birefringent plate is good or defective without any problem.

【0019】*実験結果 複屈折結晶インゴットより任意にウェハを抜き取り、こ
のウェハから2枚の楔型複屈折板と、1枚の平行平板を
製作した。この平行平板の厚さは、2枚の楔型複屈折板
を所定の位置関係で重ね合わせたときの厚さの半分にな
るようにした。なお、各板の表面は鏡面加工をした。
* Experimental Results A wafer was arbitrarily extracted from the birefringent crystal ingot, and two wedge-shaped birefringent plates and one parallel plate were manufactured from this wafer. The thickness of this parallel plate was set to be half the thickness when two wedge-shaped birefringent plates were superposed in a predetermined positional relationship. The surface of each plate was mirror-finished.

【0020】そして、平行平板単独及び2枚の楔型複屈
折板を対向配置したものをそれぞれ投光器7と光検出器
8の間に挿入配置し、光透過率を測定した。すると、平
行平板の光透過率は0.01dBであるのに対し、2枚
分の楔型複屈折板の光透過率は0.02dBとなり、平
行平板の2倍となり、厚さの比と等しくなる。これによ
り楔型複屈折板の光透過率を正確に測定できることが確
認できた。
Then, the parallel flat plate alone and the two wedge-shaped birefringent plates arranged facing each other were inserted between the light projector 7 and the photodetector 8 to measure the light transmittance. Then, while the light transmittance of the parallel plate is 0.01 dB, the light transmittance of the two wedge-shaped birefringent plates is 0.02 dB, which is twice that of the parallel plate, which is equal to the thickness ratio. Become. This confirmed that the light transmittance of the wedge-shaped birefringent plate can be accurately measured.

【0021】なお、上記した実施例では、楔型複屈折板
1a,1bの対向面を平行に配置したが、本発明は必ず
しも平行に配置しなくても良く、主平面と傾斜平面とが
対向しているとともに光学軸が一致していれば、その角
度は任意である。また、入射光の入射面に対する角度も
必ずしも垂直にしなくてもよく、所定角度傾斜していて
もよい。但し、両板の平行度がずれていたり、入射光が
垂直に照射しない場合には、一対の楔型複屈折板から出
射された出射光は、入射光と平行になるものの、常光と
異常光とが分離された状態で出射されることになる。但
し、その出射光は入射光と同一直線上に近い位置にあ
り、しかも両光が平行で広がっていかないので、投光器
と光検出器を図1に示すような位置関係においたとして
も、すべての出射光を検出感度の高い光検出器の中央部
分で受光することができる。
Although the opposing surfaces of the wedge-shaped birefringent plates 1a and 1b are arranged in parallel in the above embodiment, the present invention does not necessarily have to be arranged in parallel, and the main plane and the inclined plane are opposed to each other. If the optical axes coincide with each other, the angle is arbitrary. Further, the angle of the incident light with respect to the incident surface does not necessarily have to be vertical, and may be inclined by a predetermined angle. However, when the parallelism between the two plates is deviated or the incident light is not radiated vertically, the emitted light emitted from the pair of wedge-shaped birefringent plates becomes parallel to the incident light, but the ordinary light and the extraordinary light. And will be emitted in a separated state. However, the emitted light is in a position close to the same straight line as the incident light, and both lights are not parallel and do not spread. Therefore, even if the projector and the photodetector are placed in the positional relationship as shown in FIG. The emitted light can be received by the central portion of the photodetector with high detection sensitivity.

【0022】但し、平行に出射される常光と異常光の離
反距離は、平行度のずれが大きくなるほど、また、入射
角度が大きくなるほど大きくなるので、上記した実施例
のように、平行に設定するとともに垂直入射させるのが
最もよい。また、換言すれば、平行度からのずれ量や、
入射角度の上限は、光検出器の受光範囲により決定され
る。
However, the separation distance between the ordinary ray and the extraordinary ray emitted in parallel becomes larger as the deviation of the parallelism becomes larger and the incident angle becomes larger, so that they are set to be parallel as in the above-mentioned embodiment. It is best to make it vertically incident with. In other words, the amount of deviation from parallelism,
The upper limit of the incident angle is determined by the light receiving range of the photodetector.

【0023】さらに、両楔型複屈折板1a,1bを配置
するに際し、図示した例では両板を離して設置したが、
その離反距離は任意であり、一度出射された2本の光が
ともに次の楔型複屈折板に入射できるようになっていれ
ばその幅の広狭は問わない。
Further, in disposing the both wedge-shaped birefringent plates 1a and 1b, in the example shown in the figure, the both plates are separated from each other.
The separation distance is arbitrary, and the width may be wide or narrow as long as the two lights emitted once can enter the next wedge-shaped birefringent plate.

【0024】[0024]

【発明の効果】本発明の測定方法によれば、前記のよう
に2枚重ねした楔型複屈折板に所定角度で測定光が入射
すると、それぞれの楔型複屈折板で生じる複屈折が相殺
され、出射する光は入射光と平行になる。したがって、
投光器と光検出器の光軸を一致させておくことで、正確
に透過光を測定でき、測定対象物を交換しても測定系の
位置調整をしなおす必要はない。そのため、個々の楔型
複屈折板の光透過特性を能率よく高精度に測定できる。
According to the measuring method of the present invention, when the measuring light is incident on the two wedge-shaped birefringent plates which are stacked as described above at a predetermined angle, the birefringence generated in each wedge-shaped birefringent plate is canceled. The emitted light becomes parallel to the incident light. Therefore,
By making the optical axes of the light projector and the photodetector coincide with each other, the transmitted light can be accurately measured, and it is not necessary to readjust the position of the measurement system even if the measurement object is replaced. Therefore, the light transmission characteristics of each wedge-shaped birefringent plate can be measured efficiently and highly accurately.

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

【図1】本発明に係る楔型複屈折板の光透過特性の測定
方法の一実施例を示す概略図である。
FIG. 1 is a schematic view showing an example of a method for measuring light transmission characteristics of a wedge-shaped birefringent plate according to the present invention.

【図2】図1に示す2枚の楔型複屈折板の組み合わせ方
を示す斜視図である。
FIG. 2 is a perspective view showing how to combine the two wedge-shaped birefringent plates shown in FIG.

【図3】本発明の対象となる楔型複屈折板を使用した光
アイソレータの概略構成図である。
FIG. 3 is a schematic configuration diagram of an optical isolator using a wedge-shaped birefringent plate which is an object of the present invention.

【図4】楔型複屈折板の一例を示す斜視図である。FIG. 4 is a perspective view showing an example of a wedge-shaped birefringent plate.

【図5】楔型複屈折板の光透過特性を測定する従来の方
法を示す概略図である。
FIG. 5 is a schematic view showing a conventional method for measuring the light transmission characteristics of a wedge-shaped birefringent plate.

【符号の説明】[Explanation of symbols]

1,1a,1b 楔型複屈折板 2 ファラデー回転子 3 入力側光ファイバ 4 カップリングレンズ 5 出力側光ファイバ 6 カップリングレンズ 7 投光器 8 光検出器 Q 光学軸 R 主平面 S 傾斜平面 1,1a, 1b Wedge type birefringent plate 2 Faraday rotator 3 Input side optical fiber 4 coupling lens 5 Output side optical fiber 6 coupling lens 7 Floodlight 8 Photodetector Q optical axis R main plane S inclined plane

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平6−34916(JP,A) 特開 平6−51244(JP,A) 実開 昭62−39229(JP,U) 特公 昭61−58809(JP,B2) (58)調査した分野(Int.Cl.7,DB名) G01M 11/00 - 11/08 G01N 21/23 G01N 21/59 G02B 27/00 - 27/64 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP-A-6-34916 (JP, A) JP-A-6-51244 (JP, A) Fukui Sho 62-39229 (JP, U) JP-B Sho 61- 58809 (JP, B2) (58) Fields investigated (Int.Cl. 7 , DB name) G01M 11/00-11/08 G01N 21/23 G01N 21/59 G02B 27/00-27/64

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 光学軸Qと平行な主平面Rと、この主平
面Rに対して適宜角度傾斜した傾斜平面Sとで挟まれた
形状の楔型複屈折板の光透過特性を測定するにあたり、
2枚の楔型複屈折板(1aと1b)を用意し、 一方の楔型複屈折板(1a)の傾斜平面Sと他方の楔型
複屈折板(1b)の主平面Rとを対向させるとともに、
両楔型複屈折板の光学軸を合わせるように両者を配置
し、 一方の楔型複屈折板(1a)の主平面Rまたは他方の楔
型複屈折板(1b)の傾斜平面Sに測定光を入射させ、
その出射光を光検出器(8)で受光することを特徴とす
る楔型複屈折板の光透過特性の測定方法。
1. When measuring a light transmission characteristic of a wedge-shaped birefringent plate having a shape sandwiched by a main plane R parallel to an optical axis Q and an inclined plane S inclined at an angle with respect to the main plane R. ,
Two wedge-shaped birefringent plates (1a and 1b) are prepared, and the inclined plane S of one wedge-shaped birefringent plate (1a) and the main plane R of the other wedge-shaped birefringent plate (1b) are opposed to each other. With
The two wedge-shaped birefringent plates are arranged so that their optical axes are aligned with each other, and the measurement light is placed on the main plane R of one wedge-shaped birefringent plate (1a) or the inclined plane S of the other wedge-shaped birefringent plate (1b). Incident,
A method for measuring light transmission characteristics of a wedge-shaped birefringent plate, characterized in that the emitted light is received by a photodetector (8).
【請求項2】 前記両楔型複屈折板を配置するに際し、
前記一方の楔型複屈折板(1a)の主平面Rと前記他方
の楔型複屈折板(1b)の傾斜平面Sとが平行になるよ
うにすることを特徴とする請求項1に記載の楔型複屈折
板の光透過特性の測定方法。
2. When disposing the both wedge-shaped birefringent plates,
The main plane R of the one wedge-shaped birefringent plate (1a) and the inclined plane S of the other wedge-shaped birefringent plate (1b) are made parallel to each other. Measuring method of light transmission characteristics of wedge-shaped birefringent plate.
JP18985695A 1995-07-03 1995-07-03 Method for measuring light transmission characteristics of wedge-type birefringent plate Expired - Fee Related JP3465804B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18985695A JP3465804B2 (en) 1995-07-03 1995-07-03 Method for measuring light transmission characteristics of wedge-type birefringent plate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18985695A JP3465804B2 (en) 1995-07-03 1995-07-03 Method for measuring light transmission characteristics of wedge-type birefringent plate

Publications (2)

Publication Number Publication Date
JPH0915092A JPH0915092A (en) 1997-01-17
JP3465804B2 true JP3465804B2 (en) 2003-11-10

Family

ID=16248331

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Country Status (1)

Country Link
JP (1) JP3465804B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6158809B2 (en) 2011-08-11 2017-07-05 マーレ インターナショナル ゲゼルシャフト ミット ベシュレンクテル ハフツングMAHLE International GmbH Plate heat exchanger

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6158809B2 (en) 2011-08-11 2017-07-05 マーレ インターナショナル ゲゼルシャフト ミット ベシュレンクテル ハフツングMAHLE International GmbH Plate heat exchanger

Also Published As

Publication number Publication date
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