JPS6053285B2 - Constant polarization optical fiber - Google Patents

Constant polarization optical fiber

Info

Publication number
JPS6053285B2
JPS6053285B2 JP56101710A JP10171081A JPS6053285B2 JP S6053285 B2 JPS6053285 B2 JP S6053285B2 JP 56101710 A JP56101710 A JP 56101710A JP 10171081 A JP10171081 A JP 10171081A JP S6053285 B2 JPS6053285 B2 JP S6053285B2
Authority
JP
Japan
Prior art keywords
cladding
optical fiber
core
refractive index
polarization
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
JP56101710A
Other languages
Japanese (ja)
Other versions
JPS5816203A (en
Inventor
博 梶岡
利秀 徳永
久典 中居
晃一 御子柴
一徳 石川
順吉 中川
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.)
Hitachi Cable Ltd
Original Assignee
Hitachi Cable 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 Hitachi Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP56101710A priority Critical patent/JPS6053285B2/en
Publication of JPS5816203A publication Critical patent/JPS5816203A/en
Publication of JPS6053285B2 publication Critical patent/JPS6053285B2/en
Expired legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C3/00Glass compositions
    • C03C3/04Glass compositions containing silica
    • C03C3/06Glass compositions containing silica with more than 90% silica by weight, e.g. quartz
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C13/00Fibre or filament compositions
    • C03C13/04Fibre optics, e.g. core and clad fibre compositions
    • C03C13/045Silica-containing oxide glass compositions
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C2201/00Glass compositions
    • C03C2201/06Doped silica-based glasses
    • C03C2201/08Doped silica-based glasses containing boron or halide
    • C03C2201/10Doped silica-based glasses containing boron or halide containing boron
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C2201/00Glass compositions
    • C03C2201/06Doped silica-based glasses
    • C03C2201/30Doped silica-based glasses containing metals
    • C03C2201/31Doped silica-based glasses containing metals containing germanium

Landscapes

  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
  • Glass Compositions (AREA)

Description

【発明の詳細な説明】 本発明は、光伝送用光ファイバに低損失定偏波型光フ
ァイバに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a low-loss constant polarization type optical fiber for optical transmission.

クラッドを楕円にし、コアに異方性歪を起こし、光弾
性効果によつて長軸、短軸方向の屈折率、従つて伝搬定
数の差を大きくし、長軸、短軸の偏波を保存するいわゆ
る定偏波型光ファイバとしては従来、λ■0.63μm
用のものが多く用いられている。
The cladding is made into an ellipse, causing anisotropic strain in the core, and the photoelastic effect increases the difference in refractive index and propagation constant in the major and minor axis directions, preserving polarization in the major and minor axes. Conventionally, the so-called constant polarization type optical fiber has a wavelength of λ■0.63 μm.
Many things are used for this purpose.

異方性歪をおこすクラッド材料としてはB、0。が有力
とされているが、B、O。は1.3μm帯以上の長波波
長帯で大きな吸収損失を受けることが、従来定偏波型光
ファイバの使用を短波長帯に限つていた大きな理由であ
る。 本発明の目的は、前記した従来技術の九色を解消
し、長波長帯で低損失となる定偏波型光ファイバの損失
を提供することにある。
The cladding material that causes anisotropic strain is B, 0. is said to be the most likely, but B and O. suffers from a large absorption loss in the long wavelength band of 1.3 μm or more, which is a major reason why the use of polarization-controlled optical fibers has conventionally been limited to short wavelength bands. An object of the present invention is to eliminate the nine colors of the prior art described above and to provide a constant polarization type optical fiber with low loss in a long wavelength band.

すなわち、本発明の要旨は、断面を4層構造とし、コ
ア周辺の低屈折率層の幅をコア半径以上とし、楕円クラ
ッド層の屈折率をコアと低屈折率層からなる第1クラッ
ドの間にあるように屈折率分布をつけたことにある。
That is, the gist of the present invention is that the cross section has a four-layer structure, the width of the low refractive index layer around the core is equal to or larger than the core radius, and the refractive index of the elliptical cladding layer is set between the core and the first cladding consisting of the low refractive index layer. The reason is that the refractive index distribution is added as shown in .

第1図に本発明定偏波型光ファイバの一実施例の断面
構造を、また、その屈折率分布を第2図に示す。
FIG. 1 shows a cross-sectional structure of an embodiment of the polarization constant optical fiber of the present invention, and FIG. 2 shows its refractive index distribution.

コア1、第1クラッド2、楕円形第2クラッド3、最外
層第3クラッド4の組成はそれぞれ、GeO2+SlO
2,slO2,GeO2+B3,O3+SiO2,Si
O,である。
The composition of the core 1, first cladding 2, elliptical second cladding 3, and outermost third cladding 4 is GeO2+SlO.
2, slO2, GeO2+B3, O3+SiO2, Si
O.

コア1と第3クラッド4との屈折率差Δn1〜0.5%
、楕円形第2クラッド3と第3クラッド4との屈折率差
ΔN2〜0.1%であり、第1クラッド2の屈折率は第
3クラッド4と等しい。
Refractive index difference Δn1 to 0.5% between core 1 and third cladding 4
, the refractive index difference between the elliptical second cladding 3 and the third cladding 4 is ΔN2 to 0.1%, and the refractive index of the first cladding 2 is equal to that of the third cladding 4.

コア径6μm第1クラッド2の厚さ3μm1外径125
μmでカットオフ波長1.1μmの単一モード光ファイ
バを得た。単一モード光ファイバの場合には多モード光
ファイバと異なり規格化周波数によりクラッドまで電磁
界成分がしみ出すため、第1クラッドはコアの半径分の
厚さを与えた。
Core diameter: 6 μm, first cladding 2 thickness: 3 μm, outer diameter: 125
A single mode optical fiber with a cutoff wavelength of 1.1 μm was obtained. In the case of a single mode optical fiber, unlike a multimode optical fiber, the electromagnetic field components seep into the cladding due to the normalized frequency, so the first cladding was given a thickness equivalent to the radius of the core.

さて、定偏波性を決定するファクターは楕円クラッドの
楕円率とボロンの量であり、一般にボロンの量増すと定
偏波性が改善される。
Now, the factors that determine polarization stability are the ellipticity of the elliptical cladding and the amount of boron, and generally, as the amount of boron increases, polarization stability improves.

単一モード光ファイバでは上記のように第1クラッドの
厚さを設定しても、わずかのコア径、屈折率の変化によ
つてカットオフ波長が変化し、それによつて動作波長に
おける規格化周波数が変化するため時によつて電磁界成
分が楕円形第2クラッドまでしみ出す場合がある。この
ような電磁界成分は導波モードである場合には波動エネ
ルギーの一部が楕円形第2クラッド部で吸収され伝送損
失の増加となる。これを防ぐ目的でかかる導波モードを
漏洩モードとし、コア中心部に電磁界成分が集中するよ
うな低損失なモードのみを導波しうるように楕円形第2
クラッドの屈折率を第1クラッドよりも大一きくする。
このような光ファイバはλ=1.2μmで1pB/Km
,λ=1.3μmでも1〜2dB/k程度の低損失にす
ることが可能であつた。
In a single mode optical fiber, even if the thickness of the first cladding is set as described above, the cutoff wavelength changes due to slight changes in the core diameter and refractive index, and this causes the normalized frequency at the operating wavelength to change. Because of this change, the electromagnetic field component may sometimes seep into the second elliptical cladding. When such an electromagnetic field component is in a waveguide mode, part of the wave energy is absorbed by the elliptical second cladding portion, resulting in an increase in transmission loss. In order to prevent this, the waveguide mode is made into a leaky mode, and an elliptical second
The refractive index of the cladding is made larger than that of the first cladding.
Such an optical fiber is 1pB/Km at λ=1.2μm.
, it was possible to achieve a low loss of about 1 to 2 dB/k even when λ=1.3 μm.

試作した光ファイバの楕円率Eは、ε=60%で結合が
約4m(λ=1.3μm)であつた。
The ellipticity E of the prototype optical fiber was ε=60%, and the coupling was about 4 m (λ=1.3 μm).

長径一短径なお、ε=?×100(%)であ
る。
The major axis and the minor axis, ε=? ×100(%).

!唇予キ短径 ここで、比較のため屈折率分布を第3図のようにした場
合について述べる。
! For comparison, a case where the refractive index distribution is as shown in FIG. 3 will be described.

このような屈折率分布の場合には、第1クラッドもコア
の一部であるかの如く動作し、クラッドモードが立ちや
すい。
In the case of such a refractive index distribution, the first cladding also operates as if it were part of the core, and a cladding mode is likely to occur.

その結果、消光比や曲げ損″失値が劣化し、また第2ク
ラッドに含まれているB2O,の影響も現われてしまう
ことになる。第1クラッドと第2クラッドとを等しくす
れば、ほぼ本発明と同様の効果が期待できるが、現実の
工業生産において厳密な意味で等しく製造することは極
めて困難であり、本発明を採用しない限り、第3図の比
較例のようになる可能性が大きい。以上説明したような
本発明光ファイバであれば次のような顕著な効果を奏す
る。
As a result, the extinction ratio and bending loss value deteriorate, and the influence of B2O contained in the second cladding also appears.If the first cladding and the second cladding are made equal, approximately Although the same effects as the present invention can be expected, it is extremely difficult to produce the same in a strict sense in actual industrial production, and unless the present invention is adopted, there is a possibility that the result will be like the comparative example in Figure 3. The optical fiber of the present invention as described above has the following remarkable effects.

(1)第1クラッドを高純際102とし、楕円形第2ク
ラッドの屈折率を第1クラッドより高くしたので、長波
長帯まで低損失で偏波特性の優れた光ファイバが得られ
る。
(1) Since the first cladding is made of high purity 102 and the refractive index of the elliptical second cladding is made higher than that of the first cladding, an optical fiber with low loss and excellent polarization characteristics up to a long wavelength band can be obtained.

(2)規格化周波数の変化に起因した電磁界のクラッド
へのしみ出しによる損失増加量が少ないので、コア径や
屈折率差に長手方向の変動があつても低損失特性が安定
している。
(2) Since the increase in loss due to the electromagnetic field seeping into the cladding due to changes in the normalized frequency is small, the low-loss characteristics are stable even if the core diameter or refractive index difference varies in the longitudinal direction. .

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

第1図は本発明の一実施例を示す断面図、第2図はその
屈折率分布を示す線図であり、第3図は比較例の屈折率
分布を示す線図である。 1・・・・・コア、2・・・・・・第1クラッド、3・
・・・・・第2クラッド、4・・・・・・第3クラッド
FIG. 1 is a sectional view showing an example of the present invention, FIG. 2 is a diagram showing its refractive index distribution, and FIG. 3 is a diagram showing the refractive index distribution of a comparative example. 1... Core, 2... First cladding, 3...
...Second cladding, 4...Third cladding.

Claims (1)

【特許請求の範囲】[Claims] 1 光ファイバの中心にガラスコア1を有し、該ガラス
コアの外周に高純度SiO_2からなり厚さが該コア半
径以上であり屈曲率が該コアより小さい同心円状の第1
クラッド2を有し、該第1クラッド2の外周に屈折率が
前記コアより小さくかつ、該第1クラッドより大きい断
面楕円形の第2クラッド3を有し、該第2クラッド3の
外周に屈折率が該第2クラッドより小さい第3クラッド
4を有することを特徴とする定偏波型光ファイバ。
1 A glass core 1 is provided at the center of the optical fiber, and a first concentric ring made of high-purity SiO_2 is formed on the outer periphery of the glass core and has a thickness greater than or equal to the core radius and a curvature smaller than that of the core.
A second cladding 3 having a refractive index smaller than the core and larger than the first cladding and having an elliptical cross section is provided on the outer periphery of the first cladding 2. 1. A polarization-constant optical fiber characterized in that it has a third cladding 4 having a smaller index than the second cladding.
JP56101710A 1981-06-30 1981-06-30 Constant polarization optical fiber Expired JPS6053285B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56101710A JPS6053285B2 (en) 1981-06-30 1981-06-30 Constant polarization optical fiber

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56101710A JPS6053285B2 (en) 1981-06-30 1981-06-30 Constant polarization optical fiber

Publications (2)

Publication Number Publication Date
JPS5816203A JPS5816203A (en) 1983-01-29
JPS6053285B2 true JPS6053285B2 (en) 1985-11-25

Family

ID=14307858

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56101710A Expired JPS6053285B2 (en) 1981-06-30 1981-06-30 Constant polarization optical fiber

Country Status (1)

Country Link
JP (1) JPS6053285B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2542358B2 (en) * 1985-02-14 1996-10-09 住友電気工業株式会社 Absolute single polarization type constant polarization optical fiber
JPS61200509A (en) * 1985-03-01 1986-09-05 Sumitomo Electric Ind Ltd Constant polarization fiber with absolute single polarization band
JPS61267707A (en) * 1985-05-22 1986-11-27 Sumitomo Electric Ind Ltd Side tunnel type constant polarization optical fiber
JPH07281044A (en) * 1995-04-05 1995-10-27 Sumitomo Electric Ind Ltd Constant polarization optical fiber
US6954575B2 (en) * 2001-03-16 2005-10-11 Imra America, Inc. Single-polarization high power fiber lasers and amplifiers

Also Published As

Publication number Publication date
JPS5816203A (en) 1983-01-29

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