JP2015045704A - Optical fiber - Google Patents
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- JP2015045704A JP2015045704A JP2013175954A JP2013175954A JP2015045704A JP 2015045704 A JP2015045704 A JP 2015045704A JP 2013175954 A JP2013175954 A JP 2013175954A JP 2013175954 A JP2013175954 A JP 2013175954A JP 2015045704 A JP2015045704 A JP 2015045704A
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- 239000013307 optical fiber Substances 0.000 title claims abstract description 39
- 238000005253 cladding Methods 0.000 claims abstract description 47
- 230000002093 peripheral effect Effects 0.000 claims description 14
- 239000011248 coating agent Substances 0.000 claims description 6
- 238000000576 coating method Methods 0.000 claims description 6
- 238000005452 bending Methods 0.000 description 8
- 230000007423 decrease Effects 0.000 description 8
- 239000000835 fiber Substances 0.000 description 7
- 230000001965 increasing effect Effects 0.000 description 7
- 230000007704 transition Effects 0.000 description 7
- 230000005540 biological transmission Effects 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 5
- 238000004891 communication Methods 0.000 description 4
- 230000005684 electric field Effects 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000012535 impurity Substances 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- PXGOKWXKJXAPGV-UHFFFAOYSA-N Fluorine Chemical compound FF PXGOKWXKJXAPGV-UHFFFAOYSA-N 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 230000002708 enhancing effect Effects 0.000 description 1
- 229910052731 fluorine Inorganic materials 0.000 description 1
- 239000011737 fluorine Substances 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- -1 germanium (Ge) Chemical compound 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000009022 nonlinear effect Effects 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
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Abstract
Description
本発明は、漏洩損失の小さい光ファイバに関する。 The present invention relates to an optical fiber with small leakage loss.
光損失低減のため、漏洩損失の小さい光ファイバが検討されている(例えば、非特許文献1〜2参照。)。
In order to reduce optical loss, optical fibers with low leakage loss have been studied (for example, see Non-Patent
また、伝送容量の拡大のために、複数の異なる波長の光を波長多重した光ファイバ通信システムでは、光ファイバ中で発生する非線形効果やファイバヒューズが問題となり、伝送の大容量化が制限されている。これらの制限を緩和するために、1本の光ファイバ中に複数のコアを有するマルチコアファイバが検討されている(例えば、非特許文献3〜7参照。)。 In addition, in order to expand transmission capacity, optical fiber communication systems in which multiple wavelengths of light are wavelength-multiplexed have problems with nonlinear effects and fiber fuses that occur in the optical fiber, limiting transmission capacity. Yes. In order to alleviate these restrictions, a multi-core fiber having a plurality of cores in one optical fiber has been studied (for example, see Non-Patent Documents 3 to 7).
漏洩損失を小さくするために、コア部の中心からクラッド部の外周端までのクラッド厚を厚くすると、クラッド部の外径が大きくなるという問題がある。クラッド部の外径が大きくなると、光ファイバの曲げに対する機械的信頼性が劣化してしまう。 If the cladding thickness from the center of the core part to the outer peripheral end of the cladding part is increased in order to reduce leakage loss, there is a problem that the outer diameter of the cladding part increases. When the outer diameter of the clad portion is increased, the mechanical reliability against bending of the optical fiber is deteriorated.
マルチコア光ファイバでも、漏洩損失を小さくするために、クラッド部の外周端に最も近い位置にあるコア部の中心からクラッド部の外周端までのクラッド厚を厚くすると、クラッド部の外径が大きくなるという問題がある。クラッド部の外径が大きくなると、クラッド部の断面の単位面積当たりに存在するコア部の数が低下し、空間利用効率が低下してしまう。また、光ファイバの曲げに対する機械的信頼性が劣化するだけでなく、マルチコア光ファイバ同士の接続の際、接続損失を一定以下とするために許容される角度ずれが小さくなってしまう。 Even in a multi-core optical fiber, in order to reduce leakage loss, increasing the cladding thickness from the center of the core closest to the outer periphery of the cladding to the outer periphery of the cladding increases the outer diameter of the cladding. There is a problem. When the outer diameter of the clad portion increases, the number of core portions existing per unit area of the cross section of the clad portion decreases, and space utilization efficiency decreases. Further, not only the mechanical reliability against bending of the optical fiber is deteriorated, but also when the multi-core optical fibers are connected to each other, an allowable angular deviation is reduced in order to keep the connection loss below a certain level.
そこで、前記課題を解決するために、本発明は、クラッド部の外径を大きくすることなく、漏洩損失の小さい光ファイバを提供することを目的とする。 Therefore, in order to solve the above-described problems, an object of the present invention is to provide an optical fiber having a small leakage loss without increasing the outer diameter of the cladding portion.
上記目的を達成するために、クラッド部の外周端を包囲する被覆部の屈折率を所定の範囲内の光ファイバとした。 In order to achieve the above object, the refractive index of the covering portion surrounding the outer peripheral end of the cladding portion is an optical fiber within a predetermined range.
具体的には、本発明は、
コア部と、
前記コア部を包囲し、屈折率が前記コア部の屈折率より小さいクラッド部と、
前記クラッド部の外周端を包囲し、屈折率が前記クラッドの屈折率より大きく、前記コア部の導波モードの実効屈折率より小さい被覆部と、
を備えることを特徴とする光ファイバ
である。
この構成によれば、クラッド部の外径を大きくすることなく、漏洩損失の小さい光ファイバを提供することが可能である。
Specifically, the present invention provides:
The core,
A cladding that surrounds the core and has a refractive index less than the refractive index of the core;
Surrounding the outer peripheral edge of the cladding part, a coating part having a refractive index larger than the refractive index of the cladding part and smaller than the effective refractive index of the waveguide mode of the core part;
An optical fiber comprising:
According to this configuration, it is possible to provide an optical fiber with a small leakage loss without increasing the outer diameter of the cladding portion.
また、本発明の光ファイバは、前記コア部の中心から前記クラッド部の外周端までのクラッド厚が35μm以下としてもよい。
この構成によれば、漏洩損失が小さく、クラッド厚の薄い光ファイバを提供することが可能である
In the optical fiber of the present invention, the cladding thickness from the center of the core part to the outer peripheral end of the cladding part may be 35 μm or less.
According to this configuration, it is possible to provide an optical fiber having a small leakage loss and a thin cladding thickness.
また、本発明の光ファイバは、前記コア部を複数有してもよい。
この構成によれば、クラッド部の外径を大きくすることなく、漏洩損失が小さいマルチコア光ファイバを提供することが可能である。
The optical fiber of the present invention may have a plurality of the core portions.
According to this configuration, it is possible to provide a multi-core optical fiber with a small leakage loss without increasing the outer diameter of the cladding portion.
また、本発明の光ファイバは、前記複数のコア部のうち、前記クラッド部の外周端に最も近い位置にあるコア部の中心から前記クラッド部の外周端までのクラッド厚が35μm以下としてもよい。
この構成によれば、漏洩損失が小さく、クラッド厚の薄いマルチコア光ファイバを提供することが可能である
The optical fiber of the present invention may have a cladding thickness of 35 μm or less from the center of the core portion closest to the outer peripheral end of the cladding portion to the outer peripheral end of the cladding portion among the plurality of core portions. .
According to this configuration, it is possible to provide a multi-core optical fiber having a small leakage loss and a thin cladding thickness.
本発明の光ファイバは、クラッド部の外径を大きくすることなく、漏洩損失を小さくすることができる。 The optical fiber of the present invention can reduce the leakage loss without increasing the outer diameter of the cladding.
添付の図面を参照して本発明の実施形態を説明する。以下に説明する実施形態は本発明の実施の例であり、本発明は以下の実施形態に制限されるものではない。なお、本明細書及び図面において符号が同じ構成要素は、相互に同一のものを示すものとする。 Embodiments of the present invention will be described with reference to the accompanying drawings. The embodiments described below are examples of the present invention, and the present invention is not limited to the following embodiments. In the present specification and drawings, the same reference numerals denote the same components.
本発明の光ファイバの断面構造を示す概略を図1に示す。図1において、コア部11の周囲にクラッド部12が配置され、クラッド部12の周囲が被覆部13で覆われている。コア部11、クラッド部12及び被覆部13の屈折率は、それぞれ、n1、n2及びn3である。クラッド厚は、コア部11の中心からクラッド部12の外周端までの距離CTで定義される。
FIG. 1 schematically shows the cross-sectional structure of the optical fiber of the present invention. In FIG. 1, a cladding portion 12 is disposed around a core portion 11, and the periphery of the cladding portion 12 is covered with a covering portion 13. Refractive index of the core portion 11, the clad portion 12 and the covering portion 13, respectively, is
また、本発明のマルチコア光ファイバの断面構造を示す概略を図2に示す。図2において、複数のコア部11の周囲にクラッド部12が配置され、クラッド部12の周囲が被覆部13で覆われている。コア部11、クラッド部12及び被覆部13の屈折率は、それぞれ、n1、n2及びn3である。クラッド厚は、コア部11のうち、クラッド部12の外周端に最も近い位置にあるコア部11の中心からクラッド部12の外周端までの距離CTで定義される。
Moreover, the outline which shows the cross-section of the multi-core optical fiber of this invention is shown in FIG. In FIG. 2, a clad part 12 is disposed around a plurality of core parts 11, and the clad part 12 is covered with a covering part 13. Refractive index of the core portion 11, the clad portion 12 and the covering portion 13, respectively, is
以下の説明は、図1に示す光ファイバ及び図2に示すマルチコア光ファイバに共通する。 The following description is common to the optical fiber shown in FIG. 1 and the multi-core optical fiber shown in FIG.
ここで、コア部11のクラッド部12に対する比屈折率差Δcore及び被覆部13のクラッド部12に対する比屈折率差Δcoatは以下の式であらわされる。
Δcore=(n1 2−n2 2)/(2n1 2) (1)
Δcoat=(n3 2−n2 2)/(2n3 2) (2)
上記式(1)、式(2)において、n1>n2であり、被覆部13の屈折率を1.5程度にすれば、コア部11の比屈折率差は高くても1%程度であることから、n3>n1>n2の関係を実現できる。
Here, the relative refractive index difference Δcore of the core portion 11 with respect to the cladding portion 12 and the relative refractive index difference Δcoat of the covering portion 13 with respect to the cladding portion 12 are expressed by the following equations.
Δ core = (n 1 2 −n 2 2 ) / (2n 1 2 ) (1)
Δ coat = (n 3 2 −n 2 2 ) / (2n 3 2 ) (2)
In the above formulas (1) and (2), if n 1 > n 2 and the refractive index of the covering portion 13 is about 1.5, the relative refractive index difference of the core portion 11 is at most about 1%. Therefore, the relationship of n 3 > n 1 > n 2 can be realized.
なお、n1>n2の条件は、コア部11及びクラッド部12の材料を純石英ガラス、またはゲルマニウム(Ge)やアルミニウム(Al)、リン(P)などの屈折率を増加させる不純物や、フッ素(F)、ボロン(B)などの屈折率を低減させる不純物を添加した石英ガラスを用いることで実現できる。 The condition of n 1 > n 2 is that the material of the core portion 11 and the cladding portion 12 is pure quartz glass, or impurities such as germanium (Ge), aluminum (Al), phosphorus (P), or the like that increase the refractive index, This can be realized by using quartz glass to which an impurity such as fluorine (F) or boron (B) is added to reduce the refractive index.
被覆部13の比屈折率差に対する漏洩損失の関係を計算したものを図3に示す。図3では、コア部11の中心からクラッド部12の外周端までの距離であるクラッド厚CTを20〜40μmの範囲で変化させている。波長については1550nmであり、コア部11の半径は4.5μm、Δcoreは0.35%、漏洩損失は光ファイバの曲げ半径140mmのときの損失としている。この光ファイバの構造においては、コア部11の導波モードの実効屈折率neffは、クラッド部12に対する導波モードの比屈折率差Δneffが0.169%となる値である。 FIG. 3 shows a calculation of the relationship between the leakage loss and the relative refractive index difference of the covering portion 13. In FIG. 3, the cladding thickness CT, which is the distance from the center of the core portion 11 to the outer peripheral end of the cladding portion 12, is changed in the range of 20 to 40 μm. The wavelength is 1550 nm, the radius of the core 11 is 4.5 μm, Δcore is 0.35%, and the leakage loss is the loss when the bending radius of the optical fiber is 140 mm. In this optical fiber structure, the effective refractive index neff of the waveguide mode of the core portion 11 is such that the relative refractive index difference Δneff of the waveguide mode with respect to the cladding portion 12 is 0.169%.
ここで、曲げ半径140mmとした理由は、非特許文献1に記載の通り遮断波長の測定に曲げ半径140mmが用いられており、光ケーブル敷設時に光ファイバが受ける曲げの実効的な半径が140mmとなるからである。
Here, the reason for setting the bending radius to 140 mm is that, as described in
図3に示す計算結果から、漏洩損失は被覆部13の屈折率が大きい領域ではほとんど変化せず、ある値を閾値として漏洩損失が下がる。このコア部11においては、導波モードの実効屈折率をneffとし、クラッド部12に対する導波モードの比屈折率差は次式で表される。
Δneff=(nneff 2−n2 2)/(2nneff 2) (3)
前述のように、比屈折率差Δneffが0.169%であったが、計算の結果、図3の閾値がこのΔneffに対応することがわかった。つまり、被覆部13の屈折率n3がコア部11の導波モードの実効屈折率neffより大きい領域では漏洩損失は変化しないが、被覆部13の屈折率n3が導波モードの実効屈折率neffより小さくなると漏洩損失が低減されることがわかった。
From the calculation results shown in FIG. 3, the leakage loss hardly changes in the region where the refractive index of the covering portion 13 is large, and the leakage loss decreases with a certain value as a threshold value. In the core portion 11, the effective refractive index of the waveguide mode is neff, and the relative refractive index difference of the waveguide mode with respect to the cladding portion 12 is expressed by the following equation.
Δ neff = (n neff 2 −n 2 2 ) / (2n neff 2 ) (3)
As described above, the relative refractive index difference Δneff was 0.169%. As a result of calculation, it was found that the threshold value in FIG. 3 corresponds to this Δneff. That is, the refractive index n 3 of the cover portion 13 is leakage loss in the effective refractive index neff larger area of the guided mode of the core portion 11 does not change, the effective refractive index refractive index n 3 is guided modes of the cover portion 13 It has been found that leakage loss is reduced when it is smaller than neff.
これは、図4に示すようにΔcoat>Δneffの場合、転移点rc(被覆の屈折率がneffを上回る位置)はΔcoatに依存しないため、曲げ損失の値は、クラッド厚CTが一定であればΔcoatに依存しないが、図5に示すようにΔcoat<Δneffの場合、Δcoatが小さくなるほど転移点rcは大きくなり、クラッド厚CTが一定であれば、Δcoatの値が小さいほど曲げ損失の値は小さくなるからである。非特許文献2に記載の通り、転移点を超えた位置の電界は振動特性を示し、放射成分となる。転移点がファイバ中心からクラッド部12の側に移動することで、転移点以降に存在する電界強度が小さくなり、放射する電界パワーの量が小さくなるためである。 As shown in FIG. 4, when Δcoat> Δneff, the transition point r c (the position where the refractive index of the coating exceeds neff) does not depend on Δcoat. Therefore, the bending loss value should be constant for the cladding thickness CT. If does not depend on Derutacoat, when the Δcoat <Δneff as shown in FIG. 5, as the transition point r c Δcoat decreases increases, if the cladding thickness CT is constant, the value of bending loss as the value of Derutacoat small This is because becomes smaller. As described in Non-Patent Document 2, an electric field at a position exceeding the transition point shows vibration characteristics and becomes a radiation component. This is because when the transition point moves from the center of the fiber to the clad portion 12 side, the electric field strength existing after the transition point decreases, and the amount of electric field power to be radiated decreases.
また、被覆部13の屈折率差n3がクラッド部12の屈折率n2より小さくなると、クラッド部12をコアとし、被覆部13をクラッドとした多数の伝搬モードが発生し、マルチモード化することから好ましくない。 When the refractive index difference n 3 of the covering portion 13 is smaller than the refractive index n 2 of the cladding portion 12, a large number of propagation modes are generated with the cladding portion 12 as a core and the covering portion 13 as a cladding. That is not preferable.
0%<Δcoat<Δneff、つまり屈折率で表現して、n2<n3<neffとすることで、クラッド厚CTの減少に伴う漏洩損失の増加を抑圧することができ、従来の光ファイバよりクラッド厚CTを低減可能である。マルチコア光ファイバの場合は、小さな外径のクラッド部12に多数のコア部11を配置することができ、空間利用効率を向上させることができる。 By expressing 0% <Δcoat <Δneff, that is, refractive index, and n 2 < n 3 < neff, an increase in leakage loss due to a decrease in cladding thickness CT can be suppressed. The cladding thickness CT can be reduced. In the case of a multi-core optical fiber, a large number of core portions 11 can be arranged in the cladding portion 12 having a small outer diameter, and space utilization efficiency can be improved.
同様に、波長1625nmにおける被覆の比屈折率差に対する漏洩損失の関係を計算したものを図6に示す。波長以外の条件は、図3と同様である。この光ファイバの構造においては、コア部11の導波モードの実効屈折率neffは、クラッド部12に対する導波モードの比屈折率差Δneffが0.159%となる値である。一般的には、波長が長くなると漏洩損失が増加するため、1550nmの時の計算結果より漏洩損失が大きくなっているが、Δneffを境に漏洩損失が下がる傾向は同じである。 Similarly, FIG. 6 shows a calculation of the relationship of leakage loss to the relative refractive index difference of the coating at a wavelength of 1625 nm. Conditions other than the wavelength are the same as in FIG. In this optical fiber structure, the effective refractive index neff of the waveguide mode of the core portion 11 is such that the relative refractive index difference Δneff of the waveguide mode with respect to the cladding portion 12 is 0.159%. Generally, since the leakage loss increases as the wavelength becomes longer, the leakage loss is larger than the calculation result at 1550 nm, but the tendency of the leakage loss to decrease at Δneff is the same.
ITU−Tのファイバ勧告G.652において、光損失の上限が0.4dB/kmと規定されており、波長1625nmにおいて0.4dB/km以下であれば、一般的に用いられている1625nm以下の通信波長帯で漏洩損失を0.4dB/km以下とすることができる。被覆部13の屈折率を制限しない場合、つまりn3>n1>n2の関係にある時にはCT>35μmとしなければならないが、被覆部13の屈折率を0%<Δcoat<Δneffとすることで、CT<35μmの領域においても漏洩損失を0.4dB/km以下とすることができる。 ITU-T Fiber Recommendation G. In 652, the upper limit of optical loss is defined as 0.4 dB / km, and if the wavelength is 16 dB nm or less at 0.4 dB / km, the leakage loss is reduced to 0 in the communication wavelength band of 1625 nm or less that is generally used. .4 dB / km or less. When the refractive index of the covering portion 13 is not limited, that is, when n 3 > n 1 > n 2 , CT> 35 μm is required, but the refractive index of the covering portion 13 should be 0% <Δcoat <Δneff. Thus, the leakage loss can be 0.4 dB / km or less even in the region of CT <35 μm.
本発明は、光通信システムの伝送媒体として適用することができるため、光通信システムに利用することができる。 Since the present invention can be applied as a transmission medium of an optical communication system, it can be used for an optical communication system.
11:コア部
12:クラッド部
13:被覆部
11: Core part 12: Cladding part 13: Covering part
Claims (4)
前記コア部を包囲し、屈折率が前記コア部の屈折率より小さいクラッド部と、
前記クラッド部の外周端を包囲し、屈折率が前記クラッドの屈折率より大きく、前記コア部の導波モードの実効屈折率より小さい被覆部と、
を備えることを特徴とする光ファイバ。 The core,
A cladding that surrounds the core and has a refractive index less than the refractive index of the core;
Surrounding the outer peripheral edge of the cladding part, a coating part having a refractive index larger than the refractive index of the cladding part and smaller than the effective refractive index of the waveguide mode of the core part;
An optical fiber comprising:
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