JPS61198101A - Polarizing separation element - Google Patents
Polarizing separation elementInfo
- Publication number
- JPS61198101A JPS61198101A JP3799485A JP3799485A JPS61198101A JP S61198101 A JPS61198101 A JP S61198101A JP 3799485 A JP3799485 A JP 3799485A JP 3799485 A JP3799485 A JP 3799485A JP S61198101 A JPS61198101 A JP S61198101A
- Authority
- JP
- Japan
- Prior art keywords
- substance
- prism
- refractive index
- reflecting surface
- light
- 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
Links
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は光通信システムを構成する光アイソレータに係
り、特に光アイソレータに利用される複屈折物質からな
る偏光分離素子に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optical isolator constituting an optical communication system, and particularly to a polarization splitting element made of a birefringent material used in an optical isolator.
光通信用回路網の形成において回路網の途中における反
射光等が光ファイバによって逆方向に伝送され、光源と
して用いられる半導体レーザに入射すると光信号にノイ
ズが混入する。そこで逆方向に伝送されてきた光が半導
体レーザに入射するのを防ぎ、半導体レーザの動作を安
定化するために半導体レーザの前に光アイソレータを挿
入し、順方向の光線は回路網を形成する光ファイバに入
射するが、逆方向の光線は光ファイバの外に逸らすとい
う操作を行っている。When forming an optical communication network, reflected light or the like in the middle of the network is transmitted in the opposite direction by an optical fiber, and when it enters a semiconductor laser used as a light source, noise is mixed into the optical signal. Therefore, in order to prevent the light transmitted in the opposite direction from entering the semiconductor laser and stabilize the operation of the semiconductor laser, an optical isolator is inserted in front of the semiconductor laser, and the light rays in the forward direction form a circuit network. The light beam enters the optical fiber, but the light rays in the opposite direction are deflected out of the optical fiber.
かかる光アイソレータには偏光分離素子が組込まれてお
り、偏光分離素子は常光線に対する屈折率と異常光線に
対する屈折率とが異なる、方解石の結晶や二酸化チタン
(T i 02 )の単結晶等の複屈折物質で構成され
る。また偏光分離素子には板状複屈折物質の表から裏に
光を透過させることによって分離する透過型偏光分離素
子と、複屈折物質で形成されたプリズムの一面から入射
した光が反射面で全反射され、そこで偏光分離されて他
面から出射するプリズム型偏光分離棄子等がある。Such an optical isolator incorporates a polarization separation element, and the polarization separation element is made of a composite material such as a calcite crystal or a single crystal of titanium dioxide (T i 02 ), which has a different refractive index for ordinary rays and for extraordinary rays. Composed of refractive material. In addition, the polarization separation element includes a transmission type polarization separation element that separates light by transmitting it from the front side of a plate-shaped birefringent material to the back side, and a transmission type polarization separation element that separates the light by transmitting it from the front to the back side of a plate-shaped birefringent material. There is a prism-type polarization separation element, etc., in which the light is reflected, the polarization is separated, and the light is emitted from the other surface.
中でも二酸化チタンの単結晶で形成されたプリズム型の
偏光分離素子は屈折率および分離角が大きく、且つ光デ
バイスを小型化できるために極めて有効な偏光分離素子
として利用されている。Among them, a prism-type polarization splitting element made of a single crystal of titanium dioxide has a large refractive index and a large separation angle, and is used as an extremely effective polarization splitting element because it allows miniaturization of optical devices.
第2図は二酸化チタンの単結晶で形成されたプリズム型
偏光分離素子の従来例を示す断面斜視図である。FIG. 2 is a cross-sectional perspective view showing a conventional example of a prism-type polarization splitting element made of a single crystal of titanium dioxide.
図においてプリズム1は二酸化チタンの単結晶で形成さ
れており、プリズム1の入射面2から入射した矢印で図
示する光は、プリズム1と空気の境界に形成された反射
面3で反射され出射面4から出射する。二酸化チタン単
結晶は屈折率が高く常光線に対して2.463、異常光
線に対して2.721である。したがって入射面2から
入射する光は反射面3で全反射され、そこで偏光方向の
異なる二つの光線は分離されて出射面4から出射する。In the figure, the prism 1 is made of a single crystal of titanium dioxide, and the light shown by the arrow that enters from the entrance surface 2 of the prism 1 is reflected by the reflection surface 3 formed at the boundary between the prism 1 and air, and is reflected from the exit surface. It emits from 4. Titanium dioxide single crystal has a high refractive index of 2.463 for ordinary rays and 2.721 for extraordinary rays. Therefore, the light incident from the entrance surface 2 is totally reflected by the reflection surface 3, and the two light beams having different polarization directions are separated and exit from the exit surface 4.
プリズムの反射面が清浄な間はプリズムに入射した光は
反射面で全反射される。しかし反射面に保護膜等の防塵
対策を施していないため、空気中に浮遊している塵埃等
が露出している反射面に付着する。塵埃等が反射面に付
着するとプリズムに入射した光は塵埃等によって乱反射
し、反射面における光の損失を増大させると共に偏光分
離素子の特性を悪化させるという問題がある。As long as the reflective surface of the prism is clean, the light incident on the prism is totally reflected by the reflective surface. However, since no dust-proofing measures such as a protective film are applied to the reflective surface, dust particles floating in the air adhere to the exposed reflective surface. When dust or the like adheres to the reflective surface, light incident on the prism is diffusely reflected by the dust or the like, which increases the loss of light at the reflective surface and deteriorates the characteristics of the polarization separation element.
上記問題点は複屈折物質からなるプリズムの反射面を、
屈折率が該複屈折物質よりも低い物質で被覆してなる本
発明の偏光分離素子によって解決される。The above problem is that the reflective surface of the prism made of birefringent material
This problem is solved by the polarization splitting element of the present invention, which is coated with a substance whose refractive index is lower than that of the birefringent substance.
複屈折物質からなるプリズムの反射面を、屈折率が該複
屈折物質よりも低い物質で被覆することにより、プリズ
ムに入射した光は反射面で全反射させると共に、塵埃等
が反射面に付着して反射面における光の損失を増大させ
ると共に偏光分離素子の特性を悪化させる等の問題を回
避することができる。By coating the reflective surface of a prism made of a birefringent material with a material whose refractive index is lower than that of the birefringent material, the light incident on the prism is totally reflected on the reflective surface, and dust and other particles are prevented from adhering to the reflective surface. This makes it possible to avoid problems such as increasing light loss at the reflecting surface and deteriorating the characteristics of the polarization separation element.
以下添付図により本発明の実施例について説明する。第
1図は本発明になる偏光分離素子の一実施例を示す断面
斜視図であり、第2図と同じ対象物は同一記号で表して
いる。Embodiments of the present invention will be described below with reference to the accompanying drawings. FIG. 1 is a cross-sectional perspective view showing one embodiment of a polarization splitting element according to the present invention, and the same objects as in FIG. 2 are represented by the same symbols.
図において複屈折物質からなるプリズム1の反射面3に
は、屈折率が複屈折物質よりも低い物質5が蒸着されて
おり、反射面3では複屈折物質と蒸着された物質の屈折
率の差により全反射が行われている。例えば二酸化チタ
ンの単結晶は屈折率が高く常光線に対して2.463、
異常光線に対して2.721であり、二酸化チタンの単
結晶で形成されたプリズム1の反射面3に、屈折率が1
.5の二酸化シリコン(Si02)を蒸着すると、二酸
化チタンの単結晶の屈折率と二酸化シリコンの屈折率の
差により十分全反射させることができる。In the figure, a substance 5 whose refractive index is lower than that of the birefringent material is deposited on the reflective surface 3 of a prism 1 made of a birefringent material, and the difference in refractive index between the birefringent material and the deposited material is total internal reflection is performed. For example, a single crystal of titanium dioxide has a high refractive index of 2.463 for ordinary rays.
2.721 for extraordinary rays, and the reflective surface 3 of the prism 1 made of a single crystal of titanium dioxide has a refractive index of 1.
.. When silicon dioxide (Si02) of No. 5 is vapor-deposited, sufficient total reflection can be achieved due to the difference between the refractive index of the single crystal of titanium dioxide and the refractive index of silicon dioxide.
しかもプリズム1の反射面3の表面は蒸着された物質5
によって完全に被覆されており、空気中に浮遊している
塵埃等が反射面に付着して、反射面における光の損失を
増大させると共に偏光分離素子の特性を悪化させる等の
問題を回避することができる。Moreover, the surface of the reflective surface 3 of the prism 1 is covered with a deposited material 5.
This avoids problems such as dust floating in the air adhering to the reflective surface, increasing light loss on the reflective surface and deteriorating the characteristics of the polarization separation element. I can do it.
上述の如く本発明によれば空気中に浮遊している塵埃等
が反射面に付着して、特性を悪化させることを防止した
偏光分離素子を提供することができる。As described above, according to the present invention, it is possible to provide a polarization separation element that prevents dust and the like floating in the air from adhering to the reflecting surface and deteriorating the characteristics.
第1図は二酸化チタンの単結晶で形成された本発明にな
る、プリズム型偏光分離素子
の一実施例を示す断面斜視図、
第2図はプリズム型偏光分離素子の従来例を示す断面斜
視図、
である。図において
1はプリズム、 2は入射面、
3は反射面、 4は出射面、
5は蒸着物質、
をそれぞれ表す。FIG. 1 is a cross-sectional perspective view showing an example of a prism-type polarized light splitting element according to the present invention formed of a single crystal of titanium dioxide. FIG. 2 is a cross-sectional perspective view showing a conventional example of a prism-type polarized light splitting element. , is. In the figure, 1 represents a prism, 2 represents an entrance surface, 3 represents a reflection surface, 4 represents an exit surface, and 5 represents a deposited material.
Claims (1)
該複屈折物質よりも低い物質で被覆してなることを特徴
とする偏光分離素子。 2)複屈折物質として二酸化チタンの単結晶を用いた特
許請求の範囲第1項記載の偏光分離素子。[Scope of Claims] 1) A polarization separation element characterized in that the reflecting surface of a prism made of a birefringent substance is coated with a substance whose refractive index is lower than that of the birefringent substance. 2) A polarization splitting element according to claim 1, which uses a single crystal of titanium dioxide as the birefringent substance.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3799485A JPS61198101A (en) | 1985-02-27 | 1985-02-27 | Polarizing separation element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3799485A JPS61198101A (en) | 1985-02-27 | 1985-02-27 | Polarizing separation element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS61198101A true JPS61198101A (en) | 1986-09-02 |
Family
ID=12513124
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3799485A Pending JPS61198101A (en) | 1985-02-27 | 1985-02-27 | Polarizing separation element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61198101A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5299059A (en) * | 1991-04-30 | 1994-03-29 | Canon Kabushiki Kaisha | Plural-beam optical head including a uniaxial crystal right triangular prism beam divider |
-
1985
- 1985-02-27 JP JP3799485A patent/JPS61198101A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5299059A (en) * | 1991-04-30 | 1994-03-29 | Canon Kabushiki Kaisha | Plural-beam optical head including a uniaxial crystal right triangular prism beam divider |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5076675A (en) | Polarizing separating device and optical isolator employing the same | |
| KR940701548A (en) | Retroreflective polarizer | |
| US6128133A (en) | Optical beamsplitter | |
| JPS6118481Y2 (en) | ||
| US6246518B1 (en) | Reflection type optical isolator | |
| US5559633A (en) | Optical isolator with reduced relative walk-off | |
| US5574809A (en) | Optical fiber type part for optical systems | |
| JPS61198101A (en) | Polarizing separation element | |
| US6476967B2 (en) | Compact optical circulator with three ports | |
| JP3290578B2 (en) | Optical isolator with Fabry-Perot ripple reducer | |
| JP2000180789A (en) | Optical isolator | |
| US6633428B2 (en) | Optical module | |
| JPH0246419A (en) | Optical isolator | |
| JP2611352B2 (en) | Chromatic dispersion compensation method for optical transmission line | |
| JP2775103B2 (en) | Polarizing prism | |
| JPS61167912A (en) | Optical coupling device | |
| JPS597312A (en) | Optical isolator | |
| JP2686453B2 (en) | Optical isolator | |
| JP2644314B2 (en) | Optical branching / coupling device | |
| JP2560058Y2 (en) | Optical fixed attenuator | |
| JP3006687B2 (en) | Optical isolator | |
| JPS6324457Y2 (en) | ||
| JPH06160771A (en) | Optical isolator | |
| JPH0784124A (en) | Beam splitter | |
| JPS6097309A (en) | Optical coupling method to thin dielectric film |