JPH02173613A - Polarizing device - Google Patents

Polarizing device

Info

Publication number
JPH02173613A
JPH02173613A JP32797788A JP32797788A JPH02173613A JP H02173613 A JPH02173613 A JP H02173613A JP 32797788 A JP32797788 A JP 32797788A JP 32797788 A JP32797788 A JP 32797788A JP H02173613 A JPH02173613 A JP H02173613A
Authority
JP
Japan
Prior art keywords
light
polarization
lens
polarizing device
plane
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
JP32797788A
Other languages
Japanese (ja)
Inventor
Toru Shiraki
徹 白木
Tsugio Tokumasu
次雄 徳増
Yoichi Suzuki
洋一 鈴木
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 JP32797788A priority Critical patent/JPH02173613A/en
Publication of JPH02173613A publication Critical patent/JPH02173613A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a low-loss, efficient polarizing device by disposing a 1/2- wavelength plate between a polarized light separating plate and a 2nd lens and on the path of only ordinary or abnormal light passing between them, thereby projecting linear polarized light regardless of the polarized state of incident light. CONSTITUTION:Light which is emitted by a single-mode fiber 1 is collimated by a 1st lens 11 into parallel luminous flux, which is made incident on the polarized light separating plate 12 and separated into the ordinary light E0 and abnormal light Ex. Both the light beams have their planes of polarization deviating by 90 deg., but the ordinary light E0 is made incident on a 2nd lens 13 as it is and the abnormal light Ex is made incident on the 2nd lens 13 through the 1/2-wavelength plate 14; and the abnormal light Ex passing through the 1/2-wavelength plate 14 has the plane of polarization rotated by 90 deg., so the plane of polarization is coincident with the plane of polarization of the extraordinary light E0. Consequently, light which is converted after passing through the 2nd lens 13 becomes linear polarized light and the polarization angle of a constant polarization fiber 2 is made coincident with that of the linear polarized light to obtain the polarizing device which has extremely small loss.

Description

【発明の詳細な説明】 (産業上の利用分野) この発明は、偏光装置に関するもので、より具体的には
、偏光装置内での光量の損失の低減を図る偏光装置に関
する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to a polarizing device, and more specifically to a polarizing device that aims to reduce loss of light amount within the polarizing device.

(従来の技術) 振動面が一つの平面内に限られた直線偏光の光を得るた
めの偏光子(偏光装置)として、従来から種々の構成の
ものがあるが、その中の一つとして複屈折を利用したも
のがある。これは、ルチル等の複屈折性物質の中に光が
入射すると、屈折方向を異にする2つの直線偏光に分か
れて進むという性質を利用し、分離後の2つの光のうち
、一方を遮ったり、或いは2つの光の進路を充分に離し
て出射させることにより直線偏光を得る構造としている
(Prior art) There have been various configurations of polarizers (polarizers) for obtaining linearly polarized light whose vibration plane is limited to one plane. There are some that use refraction. This utilizes the property that when light enters a birefringent material such as rutile, it splits into two linearly polarized lights with different refraction directions, and blocks one of the two separated lights. Alternatively, the structure is such that linearly polarized light can be obtained by emitting two light beams with their paths sufficiently separated.

(発明が解決しようとする課題) しかしながら、上記した従来の偏光装置では、偏光装置
に入射される光のうち、偏光装置の軸に平行な偏波面を
持つ光のみを通過させ、それ以外の光は通過できずに損
失分となってしまう。
(Problem to be Solved by the Invention) However, in the above-mentioned conventional polarizing device, among the light incident on the polarizing device, only light having a polarization plane parallel to the axis of the polarizing device passes through, and other light cannot pass through, resulting in a loss.

そして、偏光装置を用いるということは、通常楕円偏光
のように異なる偏波面を有する光を、単一の偏波面を有
する光にすることを、目的として行われるため、上記損
失は必ず生じてしまい、しかも、入射する光の偏光状態
によって、その損失分が変化するなどの種々の問題を有
している。
The purpose of using a polarizer is to convert light with different planes of polarization, such as elliptically polarized light, into light with a single plane of polarization, so the above-mentioned loss always occurs. Moreover, there are various problems such as the amount of loss varies depending on the polarization state of the incident light.

この発明は上記した背景に鑑みてなさたれもので、その
目的とするところは入射される光の偏光状態のいかんに
かかわらず、出射される光は直線偏光となり、これによ
り損失が少なく効率のよい偏光装置を提供することにあ
る。
This invention was made in view of the above-mentioned background, and its purpose is to produce linearly polarized light that is emitted regardless of the polarization state of the incident light, thereby achieving low loss and high efficiency. An object of the present invention is to provide a polarizing device.

(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、本発明に係る偏光装置で
は、光の順方向に沿って光を平行光束とする第1のレン
ズと、該平行光束を常光と異常光とに分離する偏光分離
板と、該偏光分離板を通過した光を収束して該定偏波フ
ァイバに入力させる第2のレンズとを配置し、かつ、該
偏光分離板と該第2のレンズとの間であって、かつ両者
間を通過する常光と異常光の一方のみの通路上に1/2
波長板を配設した。
(Means for Solving the Problems) In order to achieve the above object, the polarizer according to the present invention includes a first lens that converts light into a parallel light beam along the forward direction of the light, and a first lens that converts the parallel light beam into an ordinary light beam. A polarization separation plate that separates the light into extraordinary light, and a second lens that converges the light that has passed through the polarization separation plate and inputs it into the polarization constant fiber are arranged, and the polarization separation plate and the second lens are arranged. 1/2 on the path of only one of the ordinary light and the extraordinary light passing between the two lenses.
A wave plate was installed.

(作 用) 本偏光装置に入射された光は、第1のレンズ、偏光分離
板を通過することにより偏波面が90度ずれた2つの平
行光束となって出射される。
(Function) The light incident on the present polarizing device passes through the first lens and the polarization separation plate, and is emitted as two parallel beams with polarization planes shifted by 90 degrees.

そして、その2つの光の内、一方はそのまま第2のレン
ズに入射するが、他方の光は1/2波長板を介して第2
のレンズに入射することになる。
Of the two lights, one enters the second lens as is, but the other light passes through the 1/2 wavelength plate and enters the second lens.
will be incident on the lens.

すると、1/2波長板を通過する際に、その光の偏波面
が90度回転され、一方の光の偏波面と一致する。
Then, when passing through the 1/2 wavelength plate, the plane of polarization of the light is rotated by 90 degrees and coincides with the plane of polarization of one of the lights.

従って、偏光装置から出射される光は、直線偏光となり
、しかもその直線偏光が偏光分離板で分離された2つの
光を合成して形成されているため損失の極めて少ない偏
光装置となる。
Therefore, the light emitted from the polarizer becomes linearly polarized light, and since the linearly polarized light is formed by combining two lights separated by the polarization separation plate, the polarizer has extremely low loss.

(実 施 例) 以下、本発明に係る偏光装置の好適な実施例について添
附図面を参照にして詳述する。
(Embodiments) Hereinafter, preferred embodiments of the polarizing device according to the present invention will be described in detail with reference to the accompanying drawings.

第1図は本発明に係る偏光装置の一実施例を示す概略構
成図である。
FIG. 1 is a schematic diagram showing an embodiment of a polarizing device according to the present invention.

同図に示すように、この実施例では、2つのファイバ間
に装着される例で有る。具体的にはシングルモードファ
イバ1と、定偏波ファイバ2とを略同−線上に配置し、
それら両ファイバ1,2間に本発明の偏光装置10を挿
入配置する。この、偏光装置10は、基本的には第1の
レンズ11、偏光分離板12、並びに第2のレンズ13
を、光の順方向に沿って同軸上に配置した構造となって
いる。
As shown in the figure, this embodiment is an example in which the fiber is installed between two fibers. Specifically, a single mode fiber 1 and a polarization constant fiber 2 are arranged approximately on the same line,
A polarizing device 10 of the present invention is inserted between both fibers 1 and 2. This polarizing device 10 basically includes a first lens 11, a polarization separation plate 12, and a second lens 13.
are arranged coaxially along the forward direction of light.

そして、上記偏光分離板12は、矩形状のルチル単結晶
板等の一軸性複屈折板で形成されるとともに、その光学
軸Xを境界面に対して30度傾斜配置している。
The polarization splitting plate 12 is formed of a uniaxial birefringent plate such as a rectangular rutile single crystal plate, and its optical axis X is inclined at 30 degrees with respect to the boundary surface.

さらに本発明では、上記偏光分離板12と第2のレンズ
13との間に1/2波長板14を配置させる。このとき
、その1/2波長板14は、偏光分離板12から出射さ
れる常光EOと異常光Exの内、一方の通路上のみ(本
実施例では異常光EX上)に位置させている。
Furthermore, in the present invention, a 1/2 wavelength plate 14 is disposed between the polarization splitting plate 12 and the second lens 13. At this time, the 1/2 wavelength plate 14 is positioned only on one path (on the extraordinary light EX in this embodiment) of the ordinary light EO and the extraordinary light Ex emitted from the polarization separation plate 12.

また、この1/2波長板14もルチル単結晶板から形成
されており、その光学軸yは、光の進路と直交する方向
に位置するように配設している。
Further, this 1/2 wavelength plate 14 is also formed from a rutile single crystal plate, and is disposed so that its optical axis y is located in a direction perpendicular to the path of light.

次ぎに上記実施例の作用について説明すると、先ず、シ
ングルモードファイバ1から波長λ−1゜55珈の光を
出射する。すると、第1のレンズ11により平行光束と
なり、その平行光束が偏光分離板12に入射され、その
通過途中で偏光分離板12の境界面で光学軸に垂直な偏
波面を持つ常光Eoと、平行な偏波面を持つ異常光Ex
とに分離され(両光の偏波面は90度ずれている)、常
光Eoは光軸に沿って直進し、異常光Exはθ−9゜8
5度で屈折し、離反する方向に沿って進む。さらに本実
施例では偏光分離板12の肉厚を10mmとしたため、
偏光分離板12を出射後の異常光EXは常光Eoに対し
て1.74m+sずれた状態で平行に進む。
Next, the operation of the above embodiment will be explained. First, light having a wavelength of λ-1°55 C is emitted from the single mode fiber 1. Then, the first lens 11 converts the parallel light beam into a parallel light beam, which enters the polarization separation plate 12. On the way of its passage, it meets the ordinary light Eo, which has a plane of polarization perpendicular to the optical axis, at the boundary surface of the polarization separation plate 12. Extraordinary light Ex with a plane of polarization
(the planes of polarization of both lights are 90 degrees apart), the ordinary light Eo travels straight along the optical axis, and the extraordinary light Ex travels straight along the optical axis at θ-9°8.
It refracts at 5 degrees and moves along the direction of separation. Furthermore, in this embodiment, since the thickness of the polarization splitting plate 12 was set to 10 mm,
After exiting the polarization separation plate 12, the extraordinary light EX travels parallel to the ordinary light Eo with a deviation of 1.74 m+s.

次いで、その出射された2つの光のうち、常光Eoはそ
のまま第2のレンズ13に入射されるが、異常光Exは
1/2波長板14を介して第2のレンズ13に入射され
ることになる。従って、1/2波長板14を通過する異
常光Exは、その通過の際に偏光面が90度回転される
ため、常光E。
Next, of the two emitted lights, the ordinary light Eo is incident on the second lens 13 as it is, but the extraordinary light Ex is incident on the second lens 13 via the 1/2 wavelength plate 14. become. Therefore, the extraordinary light Ex passing through the 1/2 wavelength plate 14 becomes ordinary light E because the plane of polarization is rotated by 90 degrees during the passage.

の偏光面に一致する。coincides with the plane of polarization.

その結果、第2のレンズ13を通過後収束される光は直
線偏光となり、その偏光角度に定偏波ファイバ2のそれ
を一致させることにより偏光装置10に入射された光で
偏光面が90度回転された成分も定偏波ファイバ2に入
射させることができる。
As a result, the light converged after passing through the second lens 13 becomes linearly polarized light, and by matching that polarization angle with that of the constant polarization fiber 2, the polarization plane of the light incident on the polarizer 10 becomes 90 degrees. The rotated component can also be made to enter the polarization constant fiber 2.

なお、上記した実施例では、入力側のファイバとしてシ
ングルモードの光ファイバを用いたが、本発明はこれに
限ることなく、種々のファイバを用いることができる。
In the above embodiments, a single mode optical fiber was used as the input fiber, but the present invention is not limited to this, and various types of fibers can be used.

さらに、偏光装置を装着する箇所はファイバ内に限られ
ない。
Furthermore, the location where the polarization device is attached is not limited to inside the fiber.

また、偏光分離板並びに1/2波長板として上記した実
施例ではルチル単結晶板を用いたが、本発明はこれに限
らずカルサイトその他−軸性の複屈折板であれば種々の
ものを用いることができる。
Further, although a rutile single crystal plate was used as the polarization splitting plate and the 1/2 wavelength plate in the above embodiment, the present invention is not limited to this, and various other axial birefringent plates such as calcite may be used. Can be used.

さらに、1/2波長板を設ける位置は、上記した異常光
の通路上でなく、常光の通路上に来るようにしても良い
Furthermore, the position where the 1/2 wavelength plate is provided may be on the ordinary light path instead of the above-mentioned extraordinary light path.

(発明の効果) 以上のように、本発明に係る偏光装置では、入射される
光の偏光状態に関係なく、出射する光は直線偏光とする
ことができる。
(Effects of the Invention) As described above, in the polarizing device according to the present invention, the emitted light can be linearly polarized light regardless of the polarization state of the incident light.

しかも、その直線偏光は、偏光分離板で分離された2つ
の光を合成することにより形成されるため、偏光装置内
での損失が極めて低くおさえることができる。
Furthermore, since the linearly polarized light is formed by combining two lights separated by a polarization separation plate, loss within the polarizer can be kept extremely low.

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

第1図は本発明に係る偏光装置の好適な一実施例を示す
概略構成図である。 1・・・シングルモードファイバ
FIG. 1 is a schematic diagram showing a preferred embodiment of a polarizing device according to the present invention. 1...Single mode fiber

Claims (1)

【特許請求の範囲】[Claims] 光の順方向に沿って光を平行光束とする第1のレンズと
、該平行光束を常光と異常光とに分離する偏光分離板と
、該偏光分離板を通過した光を収束して該定偏波ファイ
バに入力させる第2のレンズとを配置し、かつ、該偏光
分離板と該第2のレンズとの間であって、かつ両者間を
通過する常光と異常光の一方のみの通路上に1/2波長
板を配設してなることを特徴とする偏光装置。
A first lens that converts the light into a parallel beam along the forward direction of the light, a polarization splitter that separates the parallel beam into ordinary light and extraordinary light, and a polarization splitter that converges the light that has passed through the polarization splitter to determine the A second lens input to the polarization fiber is arranged between the polarization splitting plate and the second lens, and on the path of only one of ordinary light and extraordinary light passing between them. A polarizing device characterized in that a 1/2 wavelength plate is disposed in the polarizing device.
JP32797788A 1988-12-27 1988-12-27 Polarizing device Pending JPH02173613A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32797788A JPH02173613A (en) 1988-12-27 1988-12-27 Polarizing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32797788A JPH02173613A (en) 1988-12-27 1988-12-27 Polarizing device

Publications (1)

Publication Number Publication Date
JPH02173613A true JPH02173613A (en) 1990-07-05

Family

ID=18205130

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32797788A Pending JPH02173613A (en) 1988-12-27 1988-12-27 Polarizing device

Country Status (1)

Country Link
JP (1) JPH02173613A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011033914A (en) * 2009-08-04 2011-02-17 Ntt Electornics Corp Optical polarization diversity module and optical device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011033914A (en) * 2009-08-04 2011-02-17 Ntt Electornics Corp Optical polarization diversity module and optical device

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