JPS592016A - Optical isolator - Google Patents
Optical isolatorInfo
- Publication number
- JPS592016A JPS592016A JP10991282A JP10991282A JPS592016A JP S592016 A JPS592016 A JP S592016A JP 10991282 A JP10991282 A JP 10991282A JP 10991282 A JP10991282 A JP 10991282A JP S592016 A JPS592016 A JP S592016A
- Authority
- JP
- Japan
- Prior art keywords
- optical
- wavelength
- rotator
- dependency
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/09—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on magneto-optical elements, e.g. exhibiting Faraday effect
- G02F1/093—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on magneto-optical elements, e.g. exhibiting Faraday effect used as non-reciprocal devices, e.g. optical isolators, circulators
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
Abstract
Description
【発明の詳細な説明】
(1) 発明の技術分野
本発明は光アイソレータに関するもQ〕であり特に波長
依存性を減少せしめ友改喪された光アイソレータに関す
るものである。DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to an optical isolator, and particularly relates to an optical isolator that reduces wavelength dependence and is improved.
鰺) 従来技術と問題点
本発明者は先に順方向に対して100−透過すべく2つ
σ】テーパー状の複屈折物質板管偏光分離合成素子に用
いる光アイソレータを提案し、更に又、上述の偏光分離
合成素子間に配置される460フアラデ一回転子に近接
して’/2 徒長板による旋光子を配設し、光を順方向
に透過せしめる光アイソレータを提案した。しかしなが
らこれらのアイソレータでは約2%以上の波長のずれが
あると。Prior Art and Problems The present inventor has previously proposed an optical isolator for use in a tapered birefringent material plate tube polarization separation/synthesis element that transmits 100 - 2 σ in the forward direction, and furthermore, An optical isolator was proposed in which an optical rotator formed by a '/2 elongated plate is disposed close to the 460 Falade single rotator disposed between the above-mentioned polarization separation/synthesis elements to transmit light in the forward direction. However, these isolators have a wavelength shift of about 2% or more.
逆方向からの光が除去されずに透過するという元アイソ
レータのアイソレージコンの劣化を招いていた。This caused deterioration of the original isolator's isolator, in which light from the opposite direction was transmitted through without being removed.
(3) 発明の目的
上記欠点を鑑み本発明9)帛Jの目的は逆方向損失の波
長依存性を減少せしめた元アイソレータを提供すること
である。(3) Object of the Invention In view of the above drawbacks, the object of the present invention 9) is to provide an original isolator in which the wavelength dependence of reverse loss is reduced.
本発明の他の目的は小さな旋光子を用いることが可能な
光アイソレータを提供することである。Another object of the invention is to provide an optical isolator that allows the use of small optical polarizers.
(4) 発明の構成
本発明の目的はテーパー状の複屈折物質板からなる第1
クツ偏光分離素子、旋光子%45077ラデ一回転子そ
して更にテーパー状の複屈折物質板からなる第2の偏光
合成素子Pこ(7J順序に含む、光アイソレータにおい
て前記旋光子が2枚Q)位相差板を組み合わせた旋光子
であり1且つ駁旋光子の旋光角の波長依存性が45°
ファラデー回転子の波長依存性と同じで、且つ該45°
7アラデ一回転子Q〕波長依存性を打ち消すようにし
て作用せしめ1ζことを特徴とする光アイソレータによ
って達成することが出来る。(4) Structure of the Invention The object of the present invention is to provide a first structure comprising a tapered birefringent material plate.
A second polarization combining element P consisting of a Kutsu polarization separation element, an optical rotator % 45077 Rade rotator, and a tapered birefringent material plate (included in the order 7J, the optical isolator has two optical polarizers Q). It is an optical rotator that combines a retardation plate, and the wavelength dependence of the optical rotation angle of the optical rotation photon is 45°.
Same as the wavelength dependence of Faraday rotator, and the 45°
7 Alade one rotator Q] This can be achieved by an optical isolator characterized in that it acts so as to cancel the wavelength dependence.
(5) 発明C/J笑施例
第1図及び第2図は本発明に係る元アイソレータ2示す
概略図であ1v特に第1図は順方向の光の透過状態を示
し、第2図は逆方向の光GjJ透過状態を示したもので
ある。(5) Example of Invention C/J Figures 1 and 2 are schematic diagrams showing the original isolator 2 according to the present invention. Particularly, Figure 1 shows the state of transmission of light in the forward direction, and Figure 2 shows the state of transmission of light in the forward direction. It shows the transmission state of light GjJ in the opposite direction.
第1図に示すように45° ファラデー回転子5の左側
にテーパー状の第1の複屈折物質(偏光分離素子)3.
そして本願特有の2枚の位相差板を組み合わせた旋光子
4を配設し、右側にテーパー状の第2の複屈折物質(偏
光合成素子)6が配設されている。テーパー状の第1σ
】偏光分離素子に光を順方向(第1図において左から右
)に入射させると偏光によって屈折率が異なるので常光
及び異常光と別れて別方向に屈折し旋光子4に入射、透
過され、更に45° ファラデー回転子5に入射される
。テーパー状の第2の偏光合成素子6の光学軸はテーパ
ー状σノ第1の偏光分離素子3の光学軸に対して光線方
向Vノ14ジに45°回転したものを用いている力で偏
光台H,禦子6を透過した常光と異常光は互いに・平行
となって出射され共にレンズ7で光ファイバ8に集束す
る。一方逆方向(第2図番こおいて右から左)への光線
はテーパー状の偏光分離素子6に入射し一7C後常光と
異常光に別れて別方向に屈折し45° ファラデー回転
子5に入射し、偏光面が450回転させられて出射され
る。As shown in FIG. 1, a tapered first birefringent material (polarization splitting element) 3. is provided on the left side of the 45° Faraday rotator 5.
An optical rotator 4 which is a combination of two retardation plates unique to the present invention is disposed, and a tapered second birefringent material (polarization combining element) 6 is disposed on the right side. Tapered first σ
] When light is incident on the polarization separation element in the forward direction (from left to right in Figure 1), the refractive index differs depending on the polarization, so it is separated from the ordinary light and extraordinary light and refracted in a different direction, and is incident on the optical rotator 4 and transmitted. The light is further incident on the 45° Faraday rotator 5. The optical axis of the tapered second polarization combining element 6 is rotated by 45 degrees in the light beam direction V with respect to the optical axis of the tapered first polarization separating element 3. The ordinary light and the extraordinary light that have passed through the stand H and the Satoru 6 are emitted parallel to each other, and both are focused onto the optical fiber 8 by the lens 7. On the other hand, the light beam in the opposite direction (from right to left in Figure 2) enters the tapered polarization separation element 6, and after 17C, it separates into ordinary light and extraordinary light and is refracted in different directions at 45° Faraday rotator 5. The plane of polarization is rotated by 450 and the light is emitted.
偏光面が45°回転した5の常光は旋光子4に入射され
る。この場合ある波長λで入射されるものがΔλの波長
Q】ずれがあるとファラデー回転子θ、の波長依存△θ
、が生ずるが、このΔθし入。The ordinary light 5 whose polarization plane has been rotated by 45° is incident on the optical rotator 4 . In this case, if the incident wavelength λ is Δλ wavelength Q], the wavelength dependence of the Faraday rotator θ, Δθ
, but this Δθ is input.
に等しい60ムλの組を有し、且りファラデー回転子と
は逆向きに作用する旋光子4と用いる。こ(7J工うな
旋光子に↓って、ファラデー回転子において波長ワ]変
化によって生じたファラデー回転角度のずれが補償され
る。従って旋光子4を出射した異常光は第】の偏光合成
の光学軸に対し90゜回転した偏光となり異常としての
屈折を受ける。is used with an optical rotator 4 having a set of 60 μm λ equal to , and acting in the opposite direction to the Faraday rotator. The deviation of the Faraday rotation angle caused by the change in the wavelength in the Faraday rotator is compensated for. Therefore, the extraordinary light emitted from the optical rotator 4 is the polarization synthesis optical The polarized light is rotated by 90 degrees with respect to the axis and undergoes anomalous refraction.
一方偏光面が6の常光(波線で示す)は同様にして第J
の偏光台H,素子3に対して異常光としてジノ[折を受
ける。このためにレンズ2によってファイバに絞り込む
時に逆方向光はファイバ1に入らない。On the other hand, the ordinary light with a polarization plane of 6 (shown by a wavy line) is similarly
The polarizing table H and the element 3 receive the Zino [reflection] as extraordinary light. For this reason, when the light is focused into the fiber by the lens 2, the backward light does not enter the fiber 1.
該旋光子4は小さくさせるために2枚の組合せ位相板に
したもので、材質祉水晶等の複屈折物質板でぶくその厚
みは30〜100μm直径は3〜5■でよい。その−例
として、1/2波長板とJ/4波長板の組み会せかあり
、直線偏光e′/2波長板で旋光した後、1/4波長板
の主軸をその偏光方向とすることに工ってΔλによる楕
円偏光化を旋光角の変化に変換することができる。The optical rotator 4 is made of a combination of two phase plates in order to be small, and is made of a birefringent material plate such as quartz, and may have a thickness of 30 to 100 .mu.m and a diameter of 3 to 5 .mu.m. As an example, there is a combination of a 1/2 wavelength plate and a J/4 wavelength plate, and after linearly polarized light is rotated by the e'/2 wavelength plate, the main axis of the 1/4 wavelength plate is set as the polarization direction. It is possible to convert the elliptical polarization caused by Δλ into a change in the angle of optical rotation.
(6)発明の効果
以上の説明から明らかなように450 ファラデー回
転子の波長依存性と同じ波長依存性を有する2枚の位相
差板を組み合わせた旋光子を用いることによって逆方向
損失の波長依存性を減少させ且つ小型化せしめた光アイ
ソレータを得ることが出来る。(6) Effects of the invention As is clear from the above explanation, the wavelength dependence of reverse loss can be achieved by using an optical rotator that combines two retardation plates that have the same wavelength dependence as that of a 450 Faraday rotator. Thus, it is possible to obtain an optical isolator with reduced thermal resistance and miniaturization.
w41図及び第2図は本発明を説明するための概略図で
ある。
J、8・・・・・・ファイバ% 2.7・・・・・・レ
ンズ、3.6・・・・・・テーパー状偏光分成素子、4
・・自・・旋光子、5・・・・・・45° ファラデー
回転子。
特許出願人
富士通株式会社
特許出願代理人
弁理士 青 木 朗
弁理士 西 舘 和 之
弁理士 内 1)幸 男
弁理士 山 口 昭 之Figure w41 and Figure 2 are schematic diagrams for explaining the present invention. J, 8...Fiber% 2.7...Lens, 3.6...Tapered polarization splitting element, 4
... Self... Rotator, 5...45° Faraday rotator. Patent applicant Fujitsu Ltd. Patent agent Akira Aoki Patent attorney Kazuyuki Nishidate 1) Yukio Patent attorney Akira Yamaguchi
Claims (1)
靜素J1旋光子、45° ファラデー回転子そして更に
テーパー状の複屈折物質板からなる第2の偏光會底累子
をこ内順序に含む元アイソレータにおいて; 前記旋光子が2枚の位相差板を組み会わせた旋光子であ
り、且つ該旋光子の旋光角シ〕波長依存性が45° フ
ァラデー回転子の波長依存性と同じで。 且つ該45° ファラデー回転子の波長依存性を打ち消
すようにして作用せしめたことを特徴とする光アイソレ
ータ。[Claims] A first +7J polarization polarizer J1 optical rotator made of a tapered birefringent material plate, a 45° Faraday rotator, and a second polarization rotator made of a tapered birefringent material plate. In the original isolator including in this order; the optical rotator is an optical rotator made by combining two retardation plates, and the optical rotation angle of the optical rotator has a wavelength dependence of 45°; the wavelength of the Faraday rotator; Same as dependence. An optical isolator characterized in that the optical isolator is operated to cancel the wavelength dependence of the 45° Faraday rotator.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10991282A JPS592016A (en) | 1982-06-28 | 1982-06-28 | Optical isolator |
CA000430872A CA1253726A (en) | 1982-06-28 | 1983-06-21 | Polarization rotation compensator and optical isolator using the same |
DE8383303738T DE3381840D1 (en) | 1982-06-28 | 1983-06-28 | POLARIZATION OPTICAL ROTATIONAL COMPENSATOR AND OPTICAL ISOLATOR WITH SUCH A COMPENSATOR. |
EP83303738A EP0098730B1 (en) | 1982-06-28 | 1983-06-28 | Polarization rotation compensator and optical isolator using the same |
US06/900,246 US4712880A (en) | 1982-06-28 | 1986-08-25 | Polarization rotation compensator and optical isolator using the same |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10991282A JPS592016A (en) | 1982-06-28 | 1982-06-28 | Optical isolator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS592016A true JPS592016A (en) | 1984-01-07 |
JPS6151299B2 JPS6151299B2 (en) | 1986-11-08 |
Family
ID=14522293
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10991282A Granted JPS592016A (en) | 1982-06-28 | 1982-06-28 | Optical isolator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS592016A (en) |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5478153A (en) * | 1977-12-05 | 1979-06-22 | Nippon Telegr & Teleph Corp <Ntt> | Light isolator |
JPS57100410A (en) * | 1980-12-15 | 1982-06-22 | Fujitsu Ltd | Optical isolator |
-
1982
- 1982-06-28 JP JP10991282A patent/JPS592016A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5478153A (en) * | 1977-12-05 | 1979-06-22 | Nippon Telegr & Teleph Corp <Ntt> | Light isolator |
JPS57100410A (en) * | 1980-12-15 | 1982-06-22 | Fujitsu Ltd | Optical isolator |
Also Published As
Publication number | Publication date |
---|---|
JPS6151299B2 (en) | 1986-11-08 |
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