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JP4750678B2 - Negative dispersion optical fiber, broadband optical transmission line and optical transmission system - Google Patents

Negative dispersion optical fiber, broadband optical transmission line and optical transmission system Download PDF

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JP4750678B2
JP4750678B2 JP2006318447A JP2006318447A JP4750678B2 JP 4750678 B2 JP4750678 B2 JP 4750678B2 JP 2006318447 A JP2006318447 A JP 2006318447A JP 2006318447 A JP2006318447 A JP 2006318447A JP 4750678 B2 JP4750678 B2 JP 4750678B2
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和秀 中島
隆 松井
克介 田嶋
泉 三川
和之 白木
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Description

本発明は単一モード光ファイバを用いた大容量光通信に関し、特に波長1310nm帯及び波長1550nm帯の2波長帯域を同時に用いた高速光通信を可能とする、負分散光ファイバ、及び当該負分散光ファイバを用いた広帯域光伝送路の構成法、並びに当該広帯域光伝送路を用いた光通信システムに関する。   The present invention relates to large-capacity optical communication using a single-mode optical fiber, and in particular, a negative dispersion optical fiber that enables high-speed optical communication using two wavelength bands of a wavelength 1310 nm band and a wavelength 1550 nm band simultaneously, and the negative dispersion The present invention relates to a configuration method of a broadband optical transmission line using an optical fiber and an optical communication system using the broadband optical transmission line.

広帯域データ通信サービスの普及に伴い、光通信システムに要求される伝送容量は飛躍的に増大している。このため、単一モード光ファイバ1芯当たりの伝送容量の拡大を目的として、同一の光ファイバ中に複数の波長の光を伝搬させる波長分割多重(WDM:Wavelength Division Multiplexing)技術が広く普及している。また、1波長当たりの伝送容量の拡大を目的とし、伝送速度10Gbit/s以上の高速光通信技術も利用されている。一般に、このような高速WDM伝送では光ファイバ中の累積分散による伝送特性の劣化が問題となる。このため、光伝送路中における累積分散の低減を目的とし、光伝送路で使用される光ファイバと逆符号の波長分散特性を有する分散補償ファイバ(DCF:Dispersion Compensating Fiber)が開発されている。   With the widespread use of broadband data communication services, the transmission capacity required for optical communication systems has increased dramatically. For this reason, wavelength division multiplexing (WDM) technology for propagating light of a plurality of wavelengths in the same optical fiber has been widely used for the purpose of increasing the transmission capacity per single-mode optical fiber. Yes. High-speed optical communication technology with a transmission speed of 10 Gbit / s or more is also used for the purpose of expanding the transmission capacity per wavelength. In general, in such high-speed WDM transmission, degradation of transmission characteristics due to cumulative dispersion in an optical fiber becomes a problem. For this reason, for the purpose of reducing the accumulated dispersion in the optical transmission line, a dispersion compensating fiber (DCF) having a chromatic dispersion characteristic opposite in sign to that of the optical fiber used in the optical transmission line has been developed.

一方近年、複数の空孔が、光ファイバ断面において均一な大きさ及び間隔で光ファイバの伝搬軸方向に開けられた構造(空孔構造)を有する空孔ファイバが開発されており、その広帯域性、並びに波長分散特性の柔軟な制御性の観点から注目を集めている。一般に光ファイバ断面で均一な大きさ及び間隔の空孔構造を有する空孔ファイバは、従来の空孔構造を有さない光ファイバに比べ大きな正の波長分散を有し、その零分散波長は1300nm以下にシフトすることが知られている(例えば、非特許文献1) 。従って、空孔ファイバを用いた高速光伝送においても、信号光波長帯域における累積分散の低減が必要不可欠となり、非特許文献2では、従来のDCFを用いた波長1550nm帯における累積分散低減の実現性が開示されている。
しかしながら、従来のDCFは波長1550nm帯、最大でも波長1460〜1625nmの波長帯域での使用を目的としており、従来のDCFを用い、特に前記正の波長分散を有する空孔ファイバの、波長1310及び1550nm帯の累積分散を同時に低減することは困難であるという課題があった。
On the other hand, in recent years, a hole fiber having a structure (hole structure) in which a plurality of holes are opened in the optical fiber propagation axis direction at a uniform size and interval in the cross section of the optical fiber has been developed. In addition, it has attracted attention from the viewpoint of flexible controllability of chromatic dispersion characteristics. In general, a holey fiber having a hole structure with a uniform size and interval in the cross section of the optical fiber has a larger positive wavelength dispersion than an optical fiber without a conventional hole structure, and its zero dispersion wavelength is 1300 nm. It is known to shift to the following (for example, Non-Patent Document 1). Therefore, even in high-speed optical transmission using holey fibers, it is essential to reduce the accumulated dispersion in the signal light wavelength band. In Non-Patent Document 2, the possibility of reducing the accumulated dispersion in the wavelength 1550 nm band using the conventional DCF is required. Is disclosed.
However, the conventional DCF is intended for use in the wavelength band of 1550 nm, and at the maximum, the wavelength band of 1460 to 1625 nm. The conventional DCF is used, and in particular, the holes 1310 and 1550 nm of the holey fiber having the positive wavelength dispersion are used. There is a problem that it is difficult to simultaneously reduce the cumulative dispersion of bands.

J.C.Knight, et al., “Anomalous dispersion in photonic crystal fiber, ”Photon. Technol. Lett., vol.12, no.7,pp.807-809, 2000.J.C.Knight, et al., “Anomalous dispersion in photonic crystal fiber,” Photon. Technol. Lett., Vol.12, no.7, pp.807-809, 2000. 中島 他,“PCFの1550nm帯40Gbit/s×8波DWDM伝送特性,”信総大,B−13−17,p.501,2006.Nakajima et al., “PCF 1550nm Band 40Gbit / s × 8 Wave DWDM Transmission Characteristics,” Shinso Univ., B-13-17, p.501, 2006.

以上のような背景に鑑み、本発明では波長1310及び1550nm帯で正の波長分散特性を有する光ファイバの、当該波長帯域における累積分散を同時に低減する負分散光ファイバ、及び当該負分散光ファイバを用いた広帯域光伝送路、並びに当該広帯域光伝送路を用いた光伝送システムを提供することを目的とする。   In view of the above background, in the present invention, an optical fiber having positive chromatic dispersion characteristics in the wavelength 1310 and 1550 nm bands, a negative dispersion optical fiber that simultaneously reduces cumulative dispersion in the wavelength band, and the negative dispersion optical fiber are provided. It is an object of the present invention to provide a broadband optical transmission line used and an optical transmission system using the broadband optical transmission line.

上記目的を達成する発明の負分散光ファイバは、波長1310nm帯及び波長1550nm帯で負の波長分散特性を有し、前記波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバの、少なくとも前記波長1310nm帯及び波長1550nm帯を含む2波長帯域における累積分散を同時に低減する負分散光ファイバであって、
波長1625nmにおける波長分散D 1625 と波長1550nmにおける波長分散D 1550 との比率D 1625 /D 1550 が1.1〜1.2であり、波長1310nmにおける波長分散D 1310 と前記波長分散D 1550 との比率D 1310 /D 1550 が0.3〜0.6であることと、
屈折率が均一なクラッド部と、前記クラッド部よりも高い屈折率を有する第1コア部と、前記クラッド部よりも低い屈折率を有する第2コア部とを有し、
前記第2コア部の半径aに対する前記第1コア部の半径a1の比率Ra=a1/aが0.24〜0.70の範囲であり、前記第2コア部の前記クラッド部に対する比屈折率差Δ1と、前記第1コア部の前記クラッド部に対する比屈折率差Δとの比率RΔ=Δ1/Δが−0.13〜−1.73の範囲であり、かつ前記第2コア部の半径a及び第1コア部の比屈折率差Δが、それぞれ2.3〜6.0μm及び0.3〜1.5%の範囲であることを特徴とする。
The negative dispersion optical fiber of the first invention that achieves the above object has negative chromatic dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band, and has positive chromatic dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band. A negative dispersion optical fiber that simultaneously reduces cumulative dispersion in two wavelength bands including at least the wavelength 1310 nm band and the wavelength 1550 nm band,
Ratio D 1625 / D 1550 of the chromatic dispersion D 1550 at a wavelength dispersion D 1625 and the wavelength 1550nm in wavelength 1625nm is 1.1 to 1.2, the ratio of the chromatic dispersion D 1550 and the wavelength dispersion D 1310 at a wavelength of 1310nm D 1310 / D 1550 is 0.3 to 0.6,
A clad part having a uniform refractive index, a first core part having a higher refractive index than the clad part, and a second core part having a lower refractive index than the clad part,
The ratio Ra = a1 / a of the radius a1 of the first core portion to the radius a of the second core portion is in the range of 0.24 to 0.70, and the relative refractive index of the second core portion to the cladding portion. The ratio RΔ = Δ1 / Δ between the difference Δ1 and the relative refractive index difference Δ of the first core portion with respect to the cladding portion is in the range of −0.13 to −1.73, and the radius of the second core portion The relative refractive index difference Δ between a and the first core part is in the range of 2.3 to 6.0 μm and 0.3 to 1.5%, respectively.

また、第発明の負分散光ファイバは、第発明の負分散光ファイバにおいて、
前記クラッド部に、前記第1コア部の中心から距離Λの円周に外接するように配置された、直径dの少なくとも6個以上の空孔を有し、
前記距離Λと前記第2コア部の半径aとの比率Λ/aが2.0以上であり、かつ前記空孔直径dと前記第2コア部の直径2aとの比率d/2aが0.5以上であることを特徴とする。
The negative dispersion optical fiber of the second invention is the negative dispersion optical fiber of the first invention.
The clad portion has at least six holes having a diameter d, which are arranged so as to circumscribe a circumference of a distance Λ from the center of the first core portion,
The ratio Λ / a between the distance Λ and the radius a of the second core part is 2.0 or more, and the ratio d / 2a between the hole diameter d and the diameter 2a of the second core part is 0. It is 5 or more.

また、第発明の広帯域光伝送路は、第1又は第2発明の負分散光ファイバと、
波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバとを用いて構成されることを特徴とする。
Further, the broadband optical transmission line of the third invention includes the negative dispersion optical fiber of the first or second invention,
An optical fiber having positive wavelength dispersion characteristics in a wavelength 1310 nm band and a wavelength 1550 nm band is used.

また、第発明の広帯域光伝送路は、第発明の広帯域光伝送路において、
前記波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバが、複数の空孔が軸方向に開けられた構造を有する空孔ファイバであることを特徴とする。
The broadband optical transmission line of the fourth invention is the broadband optical transmission line of the third invention.
The optical fiber having positive wavelength dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band is a hole fiber having a structure in which a plurality of holes are opened in the axial direction.

また、第発明の光伝送システムは、第又は第発明の広帯域光伝送路を用い、少なくとも波長1310nm帯及び波長1550nm帯を含む2波長帯を信号伝送帯域として使用することを特徴とする。 An optical transmission system according to a fifth aspect of the invention uses the broadband optical transmission line of the third or fourth aspect of the invention, and uses at least two wavelength bands including a wavelength band of 1310 nm and a wavelength of 1550 nm as a signal transmission band. .

以上説明したように本発明の負分散光ファイバによれば、波長1310及び1550nm帯で正の波長分散特性を有する光ファイバの、当該波長帯域における累積分散を同時に低減することを可能とするため、従来のDCFに比べ累積分散の低減帯域を飛躍的に拡大できるといった効果を奏する。
また本発明の広帯域光伝送路及び光伝送システムによれば、波長1310及び1550nm帯の少なくとも2波長帯域以上を同時に用いた、広帯域かつ高速な光伝送を実現できるため、光ファイバ1芯当たりの伝送容量を飛躍的に拡大できるといった効果も奏する。
As described above, according to the negative dispersion optical fiber of the present invention, it is possible to simultaneously reduce the accumulated dispersion in the wavelength band of the optical fiber having positive wavelength dispersion characteristics in the wavelength 1310 and 1550 nm bands. As compared with the conventional DCF, there is an effect that the reduction band of the cumulative dispersion can be dramatically expanded.
Further, according to the broadband optical transmission line and the optical transmission system of the present invention, it is possible to realize broadband and high-speed optical transmission using at least two wavelength bands of the wavelength 1310 and 1550 nm bands at the same time. There is also an effect that the capacity can be dramatically increased.

以下では本発明の実施の形態例について図面を用いて説明する。   Hereinafter, embodiments of the present invention will be described with reference to the drawings.

図1は本発明の実施の形態例に係る広帯域光伝送路及び光伝送システムの1構成例を示す概念図である。図1に示すように、本実施の形態例の光伝送システムは、送信部11、受信部14及び広帯域光伝送路15により構成されており、送信部11と受信部14とが広帯域光伝送路15を介して接続されている。   FIG. 1 is a conceptual diagram showing one configuration example of a broadband optical transmission line and an optical transmission system according to an embodiment of the present invention. As shown in FIG. 1, the optical transmission system according to the present embodiment includes a transmission unit 11, a reception unit 14, and a broadband optical transmission line 15, and the transmission unit 11 and the reception unit 14 include a broadband optical transmission line. 15 is connected.

送信部11は、波長1310及び1550nm帯の少なくとも2波長帯域を含む波長帯域の光信号を生成し、広帯域光伝送路15に送出する機能を有する。同様に受信部14は、送信部11から広帯域光伝送路15を介して伝送されてくる当該波長帯域における光信号を受信する機能を有する。   The transmission unit 11 has a function of generating an optical signal in a wavelength band including at least two wavelength bands of the wavelength 1310 and the 1550 nm band and sending it to the broadband optical transmission line 15. Similarly, the receiving unit 14 has a function of receiving an optical signal in the wavelength band transmitted from the transmitting unit 11 via the broadband optical transmission line 15.

また、広帯域光伝送路15は、波長1310及び1550nm帯で正の波長分散特性を有する光ファイバ12、及び当該波長帯で負の波長分散特性を有する負分散光ファイバ13により構成される。ここで前記光ファイバ12は、例えば複数の空孔が、光ファイバ断面において均一な大きさ及び間隔で光ファイバの伝搬軸方向に開けられた構造(空孔構造)を有する空孔ファイバにより構成することができる。また、前記光ファイバ12及び負分散光ファイバ13、もしくはその一方のファイバ長を適切に調整することにより、前記波長1310及び1550nm帯における広帯域光伝送路15全長での累積分散を同時に低減することが可能となる。   The broadband optical transmission line 15 includes an optical fiber 12 having positive chromatic dispersion characteristics in the wavelengths 1310 and 1550 nm, and a negative dispersion optical fiber 13 having negative chromatic dispersion characteristics in the wavelength bands. Here, the optical fiber 12 is constituted by, for example, a hole fiber having a structure (hole structure) in which a plurality of holes are opened in the propagation axis direction of the optical fiber at a uniform size and interval in the cross section of the optical fiber. be able to. In addition, by appropriately adjusting the length of the optical fiber 12 and the negative dispersion optical fiber 13 or one of them, the cumulative dispersion over the entire length of the broadband optical transmission line 15 in the wavelength 1310 and 1550 nm bands can be simultaneously reduced. It becomes possible.

尚、図1の構成例では前記光ファイバ12の後段に負分散光ファイバ13が接続される形態を図示しているが、負分散光ファイバ13の後段に光ファイバ12が接続される構成であっても構わない。また、前記光ファイバ12及び負分散光ファイバ13は、任意の長さの複数区間に分割して任意の順番で接続される構成であっても構わない。更には、前記負分散光ファイバ13の全長、もしくはその一部は、前記送信部11及び受信部14、もしくはその一方に組み込まれる構成であっても構わない。   In the configuration example of FIG. 1, a configuration in which the negative dispersion optical fiber 13 is connected to the subsequent stage of the optical fiber 12 is illustrated, but the optical fiber 12 is connected to the subsequent stage of the negative dispersion optical fiber 13. It doesn't matter. The optical fiber 12 and the negative dispersion optical fiber 13 may be divided into a plurality of sections having an arbitrary length and connected in an arbitrary order. Further, the entire length of the negative dispersion optical fiber 13 or a part thereof may be incorporated in the transmission unit 11 and the reception unit 14 or one of them.

以下では本発明の実施例について図面を用いて説明する。   Hereinafter, embodiments of the present invention will be described with reference to the drawings.

[実施例1]
本発明の実施例1では、図1に示した実施の形態において、波長1310及び1550nm帯で正の波長分散を有する光ファイバに、複数の空孔が、光ファイバ断面において均一な大きさ及び間隔で光ファイバの伝搬軸方向に開けられた構造(空孔構造)を有する空孔ファイバを用いた場合に対する、負分散光ファイバ及び広帯域光伝送路について図面を用いて説明する。
[Example 1]
In Example 1 of the present invention, in the embodiment shown in FIG. 1, a plurality of holes are formed in an optical fiber having positive chromatic dispersion in the wavelength 1310 and 1550 nm bands, with a uniform size and spacing in the cross section of the optical fiber. A negative dispersion optical fiber and a broadband optical transmission line for a case where a hole fiber having a structure (hole structure) opened in the propagation axis direction of the optical fiber will be described with reference to the drawings.

図2の(a)及び(b)は本発明の実施例で用いた負分散光ファイバの屈折率分布を示す概念図及び断面図である。図2に示すように、本発明の負分散光ファイバは、屈折率が均一なクラッド部21と、前記クラッド部に対する比屈折率差がΔで半径がa1の第1コア部22と、前記クラッド部に対する比屈折率差がΔ1で半径がaの第2コア部23とにより構成される。尚、前記比屈折率差Δ及びΔ1(単位%)は、前記クラッド部の屈折率n0及び、第1コア部もしくは第2コア部の屈折率nを用いて次式(1)の関係で記述される。

Figure 0004750678
2A and 2B are a conceptual diagram and a cross-sectional view showing the refractive index distribution of the negative dispersion optical fiber used in the example of the present invention. As shown in FIG. 2, the negative dispersion optical fiber of the present invention includes a clad part 21 having a uniform refractive index, a first core part 22 having a relative refractive index difference Δ and a radius a1 with respect to the clad part, and the clad And a second core portion 23 having a relative refractive index difference Δ1 and a radius a. The relative refractive index differences Δ and Δ1 (unit%) are described by the relationship of the following equation (1) using the refractive index n0 of the cladding part and the refractive index n of the first core part or the second core part. Is done.
Figure 0004750678

またここで、前記第1コア部及び第2コア部の半径、及び比屈折率差の比率を、それぞれRa及びRΔとして、次式(2)及び(3)により定義する。

Figure 0004750678
Further, here, the radii of the first core part and the second core part and the ratio of the relative refractive index difference are defined by the following expressions (2) and (3) as Ra and RΔ, respectively.
Figure 0004750678

図3の(a),(b)及び(c)は本発明の実施例で用いた空孔ファイバの波長分散特性を表す図、側面図及び断面図である。図3(a)中の実線及び破線は、空孔構造(規格化空孔直径d0/Λ0、及び空孔間隔Λ0)の異なる2種類の空孔ファイバ1,2に対する測定結果を示している。図3(b),(c)に示す空孔ファイバにおいて、31はクラッド部、32は複数の空孔である。これらの図3(b),(c)に示すようにd0及びΛ0は空孔32の直径及び間隔であり、空孔32は空孔ファイバ断面において均一な大きさ(直径d0)及び間隔Λ0を有し、空孔ファイバの伝搬軸方向に開けられている。図示例では60個の空孔が6角形状に配置されているが、空孔の個数は任意(一般に数十〜数百)であり、空孔の配置パターンも任意の回転対象の形状(4角形状、8角形状、同心円状など)が可能である。尚、図3(a)中の空孔ファイバ1はd0/Λ0=0.5及びΛ0=7.5μm、空孔ファイバ2はd0/Λ0=0.6及びΛ0=5.5μmの空孔構造を有する。図3(a)より、空孔ファイバ1及び2は、ともに波長1310及び1550nm帯で正の波長分散特性を有しており、前記図1に記載の広帯域光伝送路(15)における光ファイバ(12)として適用できることが分かる。   3A, 3B, and 3C are a diagram, a side view, and a cross-sectional view showing wavelength dispersion characteristics of the holey fiber used in the embodiment of the present invention. The solid line and the broken line in FIG. 3A show the measurement results for two types of hole fibers 1 and 2 having different hole structures (standardized hole diameter d0 / Λ0 and hole interval Λ0). In the hole fibers shown in FIGS. 3B and 3C, 31 is a cladding part, and 32 is a plurality of holes. As shown in FIGS. 3B and 3C, d0 and Λ0 are the diameter and interval of the hole 32, and the hole 32 has a uniform size (diameter d0) and interval Λ0 in the hole fiber cross section. And open in the propagation axis direction of the holey fiber. In the illustrated example, 60 holes are arranged in a hexagonal shape, but the number of holes is arbitrary (generally several tens to several hundreds), and the hole arrangement pattern is also an arbitrary shape to be rotated (4 (A rectangular shape, an octagonal shape, a concentric circular shape, etc.) are possible. In FIG. 3A, the hole fiber 1 has a hole structure of d0 / Λ0 = 0.5 and Λ0 = 7.5 μm, and the hole fiber 2 has a hole structure of d0 / Λ0 = 0.6 and Λ0 = 5.5 μm. Have As shown in FIG. 3A, the holey fibers 1 and 2 both have positive chromatic dispersion characteristics in the wavelength 1310 and 1550 nm bands, and the optical fiber (15) in the broadband optical transmission line (15) shown in FIG. It can be seen that it is applicable as 12).

表1は図3(a)に示した空孔ファイバ1,2の測定結果から、図3(a)に示した空孔ファイバ1,2の、波長1310、1625、及び1460nmにおける波長分散と、波長1550nmにおける波長分散の比率、それぞれD1310/D1550、D1625/D1550、及びD1460/D1550を計算した一覧表である。

Figure 0004750678
Table 1 shows the chromatic dispersion at the wavelengths 1310, 1625 and 1460 nm of the hole fibers 1 and 2 shown in FIG. 3A from the measurement results of the hole fibers 1 and 2 shown in FIG. It is the list which computed the ratio of chromatic dispersion in wavelength 1550nm, D1310 / D1550 , D1625 / D1550 , and D1460 / D1550 , respectively.
Figure 0004750678

表1から波長1310と1550nmにおける波長分散の比率D1310/D1550、及び波長1625と1550nmにおける波長分散の比率D1625/D1550は、それぞれ0.4〜0.5、及び1.15程度の関係を有することが確認できる。 From Table 1, the chromatic dispersion ratio D 1310 / D 1550 at wavelengths 1310 and 1550 nm and the chromatic dispersion ratio D 1625 / D 1550 at wavelengths 1625 and 1550 nm are about 0.4 to 0.5 and 1.15, respectively. It can be confirmed that there is a relationship.

図4は空孔ファイバにおける前記波長分散比D1310/D1550、D1625/D1550、及びD1460/D1550と、空孔間隔Λ0の関係を示す計算結果である。図中の実線及び破線は、それぞれ規格化空孔直径d0/Λ0が0.2及び0.5の時の結果を示す。図4より均一な空孔構造を有する空孔ファイバの波長分散比D1310/D1550、及びD1625/D1550は、それぞれ0.3〜0.6及び1.1〜1.2の範囲内であり、図3(a)及び表1に示した実際の空孔ファイバにおける測定結果と良く一致していることが分かる。また、波長分散比D1460/D1550は概ね0.8程度であることが分かる。 FIG. 4 is a calculation result showing a relationship between the chromatic dispersion ratios D 1310 / D 1550 , D 1625 / D 1550 , and D 1460 / D 1550 in the hole fiber and the hole interval Λ0. The solid and broken lines in the figure show the results when the normalized hole diameter d0 / Λ0 is 0.2 and 0.5, respectively. As shown in FIG. 4, the chromatic dispersion ratios D 1310 / D 1550 and D 1625 / D 1550 of the holey fiber having a uniform hole structure are in the range of 0.3 to 0.6 and 1.1 to 1.2, respectively. Thus, it can be seen that the measurement results for the actual holey fiber shown in FIG. It can also be seen that the chromatic dispersion ratio D 1460 / D 1550 is about 0.8.

表2は図4に示した均一な空孔構造を有する空孔ファイバ中における波長分散比D1310/D1550、D1625/D1550、及びD1460/D1550を纏めた一覧表である。

Figure 0004750678
Table 2 is a list that summarizes the chromatic dispersion ratios D 1310 / D 1550 , D 1625 / D 1550 , and D 1460 / D 1550 in the holey fiber having the uniform hole structure shown in FIG.
Figure 0004750678

従って、本発明の実施の形態の図1に示した構成例において、負分散光ファイバ(13)において、次式(4)及び(5)の関係を満足する波長分散特性を実現することにより、当該空孔ファイバの波長1310、1550nm及び1625nm帯における累積分散を同時に低減することが可能となる。更に好ましくは、波長1460及び1550nmにおける波長分散の比率D1460/D1550を0.8の近傍とすることにより、波長1460nm帯を含むより広帯域での累積分散の低減が実現できることが分かる。

Figure 0004750678
Therefore, in the configuration example shown in FIG. 1 of the embodiment of the present invention, in the negative dispersion optical fiber (13), by realizing chromatic dispersion characteristics satisfying the relations of the following expressions (4) and (5), It is possible to simultaneously reduce the accumulated dispersion in the wavelength 1310, 1550 nm, and 1625 nm bands of the hole fiber. More preferably, by setting the ratio of chromatic dispersion D 1460 / D 1550 at wavelengths 1460 and 1550 nm to be close to 0.8, it is possible to realize a reduction in cumulative dispersion in a wider band including the wavelength 1460 nm band.
Figure 0004750678

図5は、本発明の実施例の図2に示した屈折率分布を有する負分散光ファイバにおいて、前記式(4)及び(5)の関係を同時に満足する、半径の比率Raと比屈折率差の比率RΔの領域を表す図面である。図中の2本の曲線で囲まれた領域で、前記式(4)及び(5)の関係を同時に満たす波長分散特性を有する負分散光ファイバが実現できる。   FIG. 5 shows a radius ratio Ra and a relative refractive index satisfying the relations of the expressions (4) and (5) at the same time in the negative dispersion optical fiber having the refractive index distribution shown in FIG. 2 of the embodiment of the present invention. It is a drawing showing a region of a difference ratio RΔ. In the region surrounded by the two curves in the figure, a negative dispersion optical fiber having a wavelength dispersion characteristic that simultaneously satisfies the relations of the expressions (4) and (5) can be realized.

図6は、前記図5に示したRa及びRΔの設計領域を満足する、前記第2コア部の比屈折率差Δ1の最大値(符号を含む)と半径の比率Raの関係を示す図面である。図6より、Δ1の最大値はRaの増加と伴に減少する傾向にあることが分かる。一般に、クラッド部を純石英ガラスで形成する場合、クラッド部よりも低い屈折率を得るためには純石英ガラスにフッ素を添加する手法が用いられるが、実際の光ファイバでは損失増加や製造上の困難性の観点から、フッ素による比屈折率差の変化範囲は−0.5%程度までが限界となる。即ち、Raが0.7を超える領域では実際に負分散光ファイバを実現することは困難になると考えられる。   FIG. 6 is a diagram showing the relationship between the maximum value (including the sign) of the relative refractive index difference Δ1 of the second core portion and the radius ratio Ra, which satisfies the design area of Ra and RΔ shown in FIG. is there. From FIG. 6, it can be seen that the maximum value of Δ1 tends to decrease as Ra increases. In general, when the cladding is made of pure silica glass, a technique of adding fluorine to the pure silica glass is used to obtain a lower refractive index than that of the cladding. From the viewpoint of difficulty, the range of change in the relative refractive index difference due to fluorine is limited to about -0.5%. That is, it is considered difficult to actually realize a negative dispersion optical fiber in a region where Ra exceeds 0.7.

従って、図5及び6より、本発明の実施例の図2に示した屈折率分布を有する負分散光ファイバにおいて、半径の比率Ra及び比屈折率差の比率RΔを、それぞれ次式(6)及び(7)の領域で制御することにより、前記式(4)及び(5)の関係を満足する波長分散特性が実現できることが分かる。本実施例の図2に示した屈折率分布を有する負分散光ファイバの第1コア、第2コア部を純石英ガラスにゲルマニウム及びフッ素を添加して形成することで屈折率を変化させることができる。

Figure 0004750678
Therefore, from FIGS. 5 and 6, in the negative dispersion optical fiber having the refractive index distribution shown in FIG. 2 of the embodiment of the present invention, the radius ratio Ra and the relative refractive index difference ratio RΔ are respectively expressed by the following equations (6). And it can be seen that by controlling in the region of (7), chromatic dispersion characteristics satisfying the relations of the equations (4) and (5) can be realized. The first and second cores of the negative dispersion optical fiber having the refractive index distribution shown in FIG. 2 of the present embodiment can be formed by adding germanium and fluorine to pure silica glass to change the refractive index. it can.
Figure 0004750678

図7は、前記図5に示したRa及びRΔの設計領域において実現可能な、波長1460及び1550nmにおける波長分散の比率D1460/D1550の最大値と半径の比率Raとの関係を表す図面である。図7よりD1460/D1550はRaと伴に増加する傾向にあることが分かる。また、前記式(6)及び(7)に示した関係において、更に好ましくはRaを0.35〜0.51の範囲とすることにより、D1460/D1550を0.8近傍の0.78〜0.82のより好ましい特性に設定できることが分かる。 FIG. 7 is a diagram showing the relationship between the maximum value of the chromatic dispersion ratio D 1460 / D 1550 at the wavelengths 1460 and 1550 nm and the radius ratio Ra that can be realized in the design region of Ra and RΔ shown in FIG. is there. It can be seen from FIG. 7 that D 1460 / D 1550 tends to increase with Ra. In the relationship shown in the above formulas (6) and (7), it is more preferable that Ra is in the range of 0.35 to 0.51, so that D 1460 / D 1550 is 0.78 near 0.8. It can be seen that a more preferable characteristic of ˜0.82 can be set.

図8は、前記図5に示したRa及びRΔの設計領域を満足する、前記第2コア部の半径aと前記第1コア部の比屈折率差Δの関係を示す図面である。図中の6本の曲線は、それぞれRaが0.24、0.3、0.4、0.5、0.6及び0.7の条件におけるaとΔの関係を示している。図8より比屈折率差Δが一定の場合、コア半径aはRaの増加と伴に減少する傾向にあることが分かる。一方、コア半径aが一定の場合、比屈折率差ΔはRaの増加とともに減少する傾向にあることが分かる。従って、本発明の実施例の図2に示した屈折率分布において、第2コア部のコア半径a及び第1コア部の比屈折率差Δを、図8の実線及び破線で囲まれる領域、即ち以下の関係式(8)及び(9)を満たす領域で設計することにより、前記関係式(4)及び(5)を満足する負分散光ファイバが実現できることが分かる。

Figure 0004750678
FIG. 8 is a view showing the relationship between the radius a of the second core portion and the relative refractive index difference Δ of the first core portion, which satisfies the design area of Ra and RΔ shown in FIG. The six curves in the figure show the relationship between a and Δ under the conditions where Ra is 0.24, 0.3, 0.4, 0.5, 0.6 and 0.7, respectively. It can be seen from FIG. 8 that when the relative refractive index difference Δ is constant, the core radius a tends to decrease as Ra increases. On the other hand, when the core radius a is constant, it can be seen that the relative refractive index difference Δ tends to decrease as Ra increases. Therefore, in the refractive index profile shown in FIG. 2 of the embodiment of the present invention, the core radius a of the second core part and the relative refractive index difference Δ of the first core part are indicated by a region surrounded by a solid line and a broken line in FIG. That is, it can be seen that a negative dispersion optical fiber satisfying the relational expressions (4) and (5) can be realized by designing in a region satisfying the following relational expressions (8) and (9).
Figure 0004750678

図9は、前記図8に示したコア半径aと比屈折率差Δの関係を満たす負分散光ファイバと、前記図3(a)に示した空孔ファイバ1とを用いて構成した、本発明の広帯域光伝送路の全長における実効的な波長分散特性を示す図面である。図中の実線、破線及び一点鎖線は、それぞれ前記図2の屈折率分布における(Ra、RΔ、a、Δ)が、(0.40、−0.34、3.4μm、1.35%)、(0.50、−0.56、3.8μm、0.80%)及び(0.60、−0.90、3.6μm、0.70%)で設計された負分散光ファイバに対する結果を示す。また、点線(細い破線)は従来のDCF、即ち前記関係式(4)及び(5)を満足しないDCFを用いた時の結果を示す。図9より従来のDCFでは、波長1550nm帯以外の波長帯域における波長分散が負の符号側に増大する傾向にあることが分かる。一方、本発明の負分散光ファイバを用いた場合、波長1310、1550及び1625nm帯における波長分散の絶対値が低減されていることが分かる。従って、図2に示した屈折率分布を用い、前記関係式(4)〜(7)及び(8)並びに(9)を満足する負分散光ファイバを実現し、実施例の図3に示した複数の空孔が、光ファイバ断面において均一な大きさ及び間隔で光ファイバ断面の伝搬軸方向に開けられた構造を有する空孔ファイバと組み合わせることにより、少なくとも波長1310及び1550nmの2波長帯域における累積分散を同時に低減する、本発明の広帯域光伝送路が実現できることが分かる。   FIG. 9 is a diagram showing the configuration of the negative dispersion optical fiber satisfying the relationship between the core radius a and the relative refractive index difference Δ shown in FIG. 8 and the hole fiber 1 shown in FIG. It is drawing which shows the effective chromatic dispersion characteristic in the full length of the broadband optical transmission line of invention. In the figure, the solid line, the broken line, and the alternate long and short dash line indicate that (Ra, RΔ, a, Δ) in the refractive index distribution of FIG. 2 is (0.40, −0.34, 3.4 μm, 1.35%), respectively. , (0.50, -0.56, 3.8 μm, 0.80%) and (0.60, −0.90, 3.6 μm, 0.70%) designed results for negative dispersion optical fibers Indicates. A dotted line (thin broken line) shows a result when a conventional DCF, that is, a DCF that does not satisfy the relational expressions (4) and (5) is used. From FIG. 9, it can be seen that in the conventional DCF, the chromatic dispersion in the wavelength band other than the wavelength 1550 nm band tends to increase toward the negative sign side. On the other hand, when the negative dispersion optical fiber of the present invention is used, it can be seen that the absolute value of chromatic dispersion in the wavelengths 1310, 1550 and 1625 nm bands is reduced. Therefore, using the refractive index distribution shown in FIG. 2, a negative dispersion optical fiber satisfying the relational expressions (4) to (7), (8) and (9) is realized, and shown in FIG. 3 of the embodiment. By combining a plurality of holes with a hole fiber having a structure opened in the propagation axis direction of the cross section of the optical fiber at a uniform size and interval in the cross section of the optical fiber, accumulation in at least two wavelengths of wavelengths 1310 and 1550 nm is achieved. It can be seen that the broadband optical transmission line of the present invention that simultaneously reduces dispersion can be realized.

尚、本発明の実施例では、図2に示した、屈折率が均一なクラッド部と、クラッド部よりも高い屈折率を有する第1コア部と、クラッド部よりも低い屈折率を有する第2コア部とを有する負分散光ファイバを用いて説明したが、任意の屈折率分布を有する負分散光ファイバ、例えば、前記第2コア部の外側に前記クラッド部よりも高い屈折率を有する第3コア部と、前記クラッド部よりも低い屈折率を有する第4コア部(第3コア部の外側)とを有する屈折率分布、を用いても良く、当該屈折率分布を有する光ファイバにおいて、前記関係式(4)及び(5)を満足することにより、本発明の実施例と同等の作用効果を実現することも可能である。   In the embodiment of the present invention, as shown in FIG. 2, a clad portion having a uniform refractive index, a first core portion having a higher refractive index than the clad portion, and a second refractive index lower than that of the clad portion. Although a negative dispersion optical fiber having a core portion has been described, a negative dispersion optical fiber having an arbitrary refractive index distribution, for example, a third having a higher refractive index than the cladding portion outside the second core portion. A refractive index distribution having a core part and a fourth core part (outside the third core part) having a lower refractive index than the cladding part may be used. In the optical fiber having the refractive index distribution, By satisfying the relational expressions (4) and (5), it is possible to achieve the same operation and effect as the embodiment of the present invention.

[実施例2]
本発明の第2の実施例では、負分散光ファイバに空孔構造を用いた場合について図面を用いて説明する。
[Example 2]
In the second embodiment of the present invention, a case where a hole structure is used in a negative dispersion optical fiber will be described with reference to the drawings.

図10は空孔構造を用いた負分散光ファイバの断面構造を示す概念図である。図10に示すように本発明の空孔構造を有する負分散光ファイバは、コア部81の中心から距離Λの円周に外接し、屈折率が均一なクラッド部82に等間隔(円周方向に等間隔)に配置された少なくとも6個以上の直径dの空孔83を有する構造(空孔構造)を有している。ここで、図10中のコア部81は、実施例1の図2に示した、第1コア部及び第2コア部を含むコア領域に対応し、図10中のコア半径aは、図2中の第2コア部の半径aと等しい。   FIG. 10 is a conceptual diagram showing a cross-sectional structure of a negative dispersion optical fiber using a hole structure. As shown in FIG. 10, the negative dispersion optical fiber having a hole structure according to the present invention circumscribes the circumference at a distance Λ from the center of the core portion 81, and is evenly spaced (circumferential direction) in the cladding portion 82 having a uniform refractive index. And a structure (hole structure) having at least six holes 83 with a diameter d arranged at equal intervals. Here, the core part 81 in FIG. 10 corresponds to the core region including the first core part and the second core part shown in FIG. 2 of Example 1, and the core radius a in FIG. It is equal to the radius a of the second core part inside.

図11は、空孔構造を有する負分散光ファイバにおける、波長分散比の変化量と空孔までの距離Λをコア部の半径aで規格化した規格化空孔位置Λ/aの関係を示す図面である。ここで、縦軸は空孔構造を付与する前に対する、空孔構造付与後の波長分散比、D1310/D1550、D1460/D1550及びD1625/D1550の変化量を示す。また、図中の実線、破線及び一点鎖線は、空孔直径dをコア部の直径2aで規格化した規格化空孔直径d/2aが、それぞれ0.2、0.6及び1.0の場合の計算結果を示す。図11より波長分散比D1310/D1550及びD1460/D1550の変化量は、規格化空孔位置Λ/aの減少と伴に増加する傾向にあることが分かる。一方、D1625/D1550の変化量はΛ/aと伴に減少する傾向にあることが分かる。また、規格化空孔位置Λ/aが2.0以上であれば、何れの波長分散比の変化量も0.1以下に低減できることが分かる。更に好ましくは、規格化空孔位置Λ/aを2.3以上とすることにより、空孔の付与に伴う波長分散比D1460/D1550及びD1625/D1550の変化量をほぼ零とすることが可能となる。 FIG. 11 shows the relationship between the amount of change in the chromatic dispersion ratio and the normalized hole position Λ / a in which the distance Λ to the hole is normalized by the radius a of the core in a negative dispersion optical fiber having a hole structure. It is a drawing. Here, the vertical axis indicates the amount of change in the chromatic dispersion ratio, D 1310 / D 1550 , D 1460 / D 1550, and D 1625 / D 1550 after the hole structure is imparted before the pore structure is imparted. The solid line, the broken line, and the alternate long and short dash line in the figure indicate that the normalized hole diameter d / 2a obtained by normalizing the hole diameter d with the core diameter 2a is 0.2, 0.6, and 1.0, respectively. The calculation result is shown. From FIG. 11, it can be seen that the amount of change in the chromatic dispersion ratios D 1310 / D 1550 and D 1460 / D 1550 tends to increase as the normalized hole position Λ / a decreases. On the other hand, it can be seen that the amount of change of D 1625 / D 1550 tends to decrease with Λ / a. It can also be seen that if the normalized hole position Λ / a is 2.0 or more, the amount of change in the chromatic dispersion ratio can be reduced to 0.1 or less. More preferably, by setting the normalized hole position Λ / a to 2.3 or more, the amount of change in the chromatic dispersion ratios D 1460 / D 1550 and D 1625 / D 1550 accompanying the addition of the holes is made substantially zero. It becomes possible.

図12は、規格化空孔位置Λ/aが2.0の空孔構造を有する負分散光ファイバにおける、波長分散比の変化量と規格化空孔直径d/2aの関係を示す図面である。図中の実線、破線、及び一点鎖線は、それぞれ波長分散比D1310/D1550、D1460/D1550及びD1625/D1550に対する結果を示す。図12より波長分散比の変化量の、規格化空孔直径d/2aに対する依存性は、図11で示した規格化空孔位置Λ/aに対する依存性に比べ比較的小さく、d/2aが0.5以上の領域ではほぼ一定の変化量に収束する傾向にあることが分かる。 FIG. 12 is a drawing showing the relationship between the amount of change in the chromatic dispersion ratio and the normalized hole diameter d / 2a in a negative dispersion optical fiber having a hole structure with a normalized hole position Λ / a of 2.0. . The solid line, broken line, and alternate long and short dash line in the figure indicate the results for the chromatic dispersion ratios D 1310 / D 1550 , D 1460 / D 1550 and D 1625 / D 1550 , respectively. As shown in FIG. 12, the dependence of the change amount of the chromatic dispersion ratio on the normalized hole diameter d / 2a is relatively smaller than the dependence on the normalized hole position Λ / a shown in FIG. It can be seen that in the region of 0.5 or more, there is a tendency to converge to a substantially constant change amount.

従って、図11及び図12の結果から、実施例1で述べた手順で好適とした屈折率分布において、規格化空孔位置Λ/aが2.0以上の位置に空孔を付与することにより、波長分散比の変化量を低減し、実施例1の関係式(4)及び(5)に示した好適な波長分散比条件を保持することが可能となる。更に好ましくは、実施例1に示した手順において、波長分散比D1310/D1550の条件に次式(10)を用いることにより、空孔付与後においても実施例1で示した好適な波長分散比の関係式(4)及び(5)を満たすことが可能となる。

Figure 0004750678
Therefore, from the results shown in FIGS. 11 and 12, in the refractive index distribution suitable for the procedure described in Example 1, by providing holes at positions where the normalized hole position Λ / a is 2.0 or more. Thus, it is possible to reduce the amount of change in the chromatic dispersion ratio and to maintain the preferred chromatic dispersion ratio conditions shown in the relational expressions (4) and (5) of the first embodiment. More preferably, in the procedure shown in Example 1, the following equation (10) is used as the condition of the chromatic dispersion ratio D 1310 / D 1550 , so that the suitable chromatic dispersion shown in Example 1 can be obtained even after the formation of holes. It becomes possible to satisfy the relational expressions (4) and (5) of the ratio.
Figure 0004750678

図13は、空孔構造を有する負分散光ファイバにおける、曲げ損失の低減量と規格化空孔直径d/2aの関係を示す図面である。ここで縦軸は、空孔の付与に伴う曲げ損失の低減量を表す。図中の実線、破線、及び一点鎖線は、それぞれ規格化空孔位置Λ/aが2.0、2.2及び2.4の時の結果を表す。図13より、負分散光ファイバの曲げ損失は、空孔の付与に伴い改善され、その効果は規格化空孔直径d/2aに対し指数関数的に増大することが分かる。又、曲げ損失の低減効果は規格化空孔位置Λ/aが小さいほど増大するが、曲げ損失の低減効果のΛ/aに対する依存性は、d/2aに対する依存性に比べ比較的小さいことが分かる、従って、実施例1に示した手順で好適とされた屈折率分布を有する負分散光ファイバにおいて、規格化空孔直径d/2aが0.5以上となる空孔構造を付与することにより、空孔付与前に比べ曲げ損失を1桁以上改善できることが分かる。更に好ましくは、規格化空孔位置Λ/aを2.0〜2.4の範囲、規格化空孔直径d/2aを1.1以上とすることにより、空孔構造の付与による曲げ損失の低減効果を2桁以上とすることが可能となる。   FIG. 13 is a diagram showing the relationship between the reduction amount of bending loss and the normalized hole diameter d / 2a in a negative dispersion optical fiber having a hole structure. Here, the vertical axis represents the amount of reduction in bending loss accompanying the provision of holes. The solid line, broken line, and alternate long and short dash line in the figure represent the results when the normalized hole positions Λ / a are 2.0, 2.2, and 2.4, respectively. From FIG. 13, it can be seen that the bending loss of the negative dispersion optical fiber is improved with the provision of the holes, and the effect increases exponentially with respect to the normalized hole diameter d / 2a. Also, the bending loss reduction effect increases as the normalized hole position Λ / a decreases, but the dependency of the bending loss reduction effect on Λ / a is relatively small compared to the dependency on d / 2a. As can be seen, in the negative dispersion optical fiber having a refractive index profile suitable for the procedure shown in Example 1, by providing a hole structure in which the normalized hole diameter d / 2a is 0.5 or more. It can be seen that the bending loss can be improved by an order of magnitude or more compared to before the formation of holes. More preferably, when the normalized hole position Λ / a is in the range of 2.0 to 2.4 and the normalized hole diameter d / 2a is 1.1 or more, the bending loss due to the provision of the hole structure is reduced. The reduction effect can be made two digits or more.

以上により、実施例1に示した手順で好適とされた屈折率分布を有する負分散光ファイバにおいて、規格化空孔位置Λ/aが2.0以上、かつ規格化空孔直径d/2aが0.5以上の条件で、実施例2の図10に示した空孔構造を付与することにより、本発明の負分散光ファイバに好適な波長分散比の条件を満たし、かつ曲げ損失を飛躍的に低減した負分散光ファイバを実現することが可能となる。   As described above, in the negative dispersion optical fiber having the refractive index distribution suitable for the procedure shown in Example 1, the normalized hole position Λ / a is 2.0 or more and the normalized hole diameter d / 2a is By providing the hole structure shown in FIG. 10 of Example 2 under the condition of 0.5 or more, the condition of the chromatic dispersion ratio suitable for the negative dispersion optical fiber of the present invention is satisfied, and the bending loss is remarkably increased. It is possible to realize a negative dispersion optical fiber that is reduced to a very low level.

尚、空孔の付与に伴う波長分散比の変化は、空孔部が光ファイバ断面中の電界分布に変化を与えることにより生じるものであり、一般に光ファイバ中の電界分布はその半径方向で減少する特性を有する。従って、前記図11及び12に示したように、波長分散比の変化は主に空孔部までの距離により制御することが可能となり、空孔の個数には殆ど依存しない。また、空孔の付与に伴う曲げ損失の改善効果は、曲げ付与に伴う電界分布のクラッド部への浸み出しを、空孔部が遮断することにより得られるものであり、6個以上の空孔が付与された場合には、空孔界面が電界分布を遮断する領域が増加することにより、より強い曲げ損失の低減効果が実現可能となる。従って、本発明の実施例2では、空孔数が6個の場合について説明したが、6個を超える空孔構造を付与した場合においても、前記規格化空孔位置Λ/a及び規格化空孔直径d/2aを、それぞれ2.0以上及び0.5以上とすることにより、空孔数が6個の場合と同等、もしくはそれ以上の波長分散比の保持効果と曲げ損失の低減効果を実現することが可能となる。   Note that the change in the chromatic dispersion ratio associated with the provision of holes is caused by the holes changing the electric field distribution in the cross section of the optical fiber, and generally the electric field distribution in the optical fiber decreases in the radial direction. It has the characteristic to do. Therefore, as shown in FIGS. 11 and 12, the change in the chromatic dispersion ratio can be controlled mainly by the distance to the hole, and hardly depends on the number of holes. In addition, the effect of improving the bending loss associated with the provision of the holes is obtained by blocking the leaching of the electric field distribution accompanying the provision of the bending into the cladding part. When holes are provided, a stronger bending loss reduction effect can be realized by increasing the region where the hole interface blocks the electric field distribution. Therefore, in the second embodiment of the present invention, the case where the number of holes is six has been described. However, even when a hole structure having more than six holes is provided, the normalized hole position Λ / a and the normalized holes are also described. By setting the hole diameter d / 2a to 2.0 or more and 0.5 or more, respectively, the effect of maintaining the chromatic dispersion ratio and the effect of reducing the bending loss equal to or more than the case of 6 holes are obtained. It can be realized.

本発明は、特に波長1310nm帯及び波長1550nm帯の2波長帯域を同時に用いた高速光通信を可能とする、負分散光ファイバ、及び当該負分散光ファイバを用いた広帯域光伝送路、並びに当該広帯域光伝送路を用いた光通信システムに適用して有用なものである。   In particular, the present invention provides a negative dispersion optical fiber, a broadband optical transmission line using the negative dispersion optical fiber, and the broadband, which enable high-speed optical communication using two wavelength bands of a wavelength 1310 nm band and a wavelength 1550 nm band simultaneously. The present invention is useful when applied to an optical communication system using an optical transmission line.

本発明の実施の形態例に係る広帯域光伝送路及び光伝送システムの構成例を示す概念図である。It is a conceptual diagram which shows the structural example of the broadband optical transmission line and optical transmission system which concern on the embodiment of this invention. 本発明の実施例で用いた負分散光ファイバの屈折率分布を示す概念図及び断面図である。It is the conceptual diagram and sectional drawing which show the refractive index distribution of the negative dispersion optical fiber used in the Example of this invention. 本発明の実施例で用いた空孔ファイバの波長分散特性を示す図、側面図及び断面図である。It is a figure which shows the wavelength dispersion characteristic of the holey fiber used in the Example of this invention, a side view, and sectional drawing. 本発明の実施例で考慮した、均一な空孔構造を有する空孔ファイバにおける波長分散比と空孔間隔Λ0の関係を示す図面である。6 is a diagram illustrating a relationship between a wavelength dispersion ratio and a hole interval Λ0 in a holey fiber having a uniform hole structure, which is considered in an example of the present invention. 本発明の負分散光ファイバにおいて波長分散の比率D1310/D1550及びD1625/D1550の要求条件を満足する半径の比率Raと比屈折率差の比率RΔの領域を表す図面である。5 is a diagram showing a region of a radius ratio Ra and a relative refractive index difference ratio RΔ that satisfies the requirements of the chromatic dispersion ratios D 1310 / D 1550 and D 1625 / D 1550 in the negative dispersion optical fiber of the present invention. 本発明の実施例の図5に示したRaとRΔの関係を用いて実現可能な、第2コア部の比屈折率差Δ1の最大値と半径の比率Raの関係を示す図面である。6 is a diagram illustrating the relationship between the maximum value of the relative refractive index difference Δ1 of the second core portion and the radius ratio Ra that can be realized using the relationship between Ra and RΔ shown in FIG. 5 according to the embodiment of the present invention. 本発明の実施例の図5に示したRaとRΔの関係を用いて実現可能な、波長1460及び1550nmにおける波長分散比D1460/D1550と半径の比率Raの関係を示す図面である。Achievable using embodiments Figure 5 the relationship Ra and RΔ shown in the of the present invention, is a view showing a relationship between the wavelength dispersion ratio D 1460 / D 1550 and the radius ratio Ra at the wavelength 1460 and 1550 nm. 本発明の実施例の図5に示したRaとRΔの関係を満足する第2コア部の半径aと第1コア部の比屈折率差Δの関係を示す図面である。6 is a diagram illustrating a relationship between a radius a of the second core portion and a relative refractive index difference Δ of the first core portion satisfying the relationship between Ra and RΔ illustrated in FIG. 5 according to the embodiment of the present invention. 本発明の実施例の図8に示したa及びΔの関係を満たす負分散光ファイバと、実施例の図3に示した空孔ファイバ1とを用いて構成した本発明の広帯域光伝送路の実効的な波長分散特性を示す図面である。The broadband optical transmission line of the present invention constructed using the negative dispersion optical fiber satisfying the relationship between a and Δ shown in FIG. 8 of the embodiment of the present invention and the holey fiber 1 shown in FIG. 3 of the embodiment. It is drawing which shows an effective wavelength dispersion characteristic. 空孔構造を用いた負分散光ファイバの断面構造を示す概念図である。It is a conceptual diagram which shows the cross-section of the negative dispersion optical fiber using a void structure. 空孔構造を有する負分散光ファイバにおける、波長分散比の変化量と規格化空孔位置Λ/aの関係を示す図面である。6 is a drawing showing the relationship between the amount of change in wavelength dispersion ratio and the normalized hole position Λ / a in a negative dispersion optical fiber having a hole structure. 規格化空孔位置Λ/aが2.0の空孔構造を有する負分散光ファイバにおける、波長分散比の変化量と規格化空孔直径d/2aの関係を示す図面である。6 is a drawing showing the relationship between the amount of change in wavelength dispersion ratio and the normalized hole diameter d / 2a in a negative dispersion optical fiber having a hole structure with a normalized hole position Λ / a of 2.0. 空孔構造を有する負分散光ファイバにおける、曲げ損失の低減量と規格化空孔直径の関係を示す図面である。It is drawing which shows the relationship between the reduction amount of a bending loss and the normalized hole diameter in the negative dispersion optical fiber which has a hole structure.

符号の説明Explanation of symbols

11 送信部
12 波長1310及び1550nm帯で正の波長分散特性を有する光ファイバ
13 負分散光ファイバ
14 受信部
15 広帯域光伝送路
21 クラッド部
22 第1コア部
23 第2コア部
31 クラッド部
32 空孔
81 コア部
82 クラッド部
83 空孔
DESCRIPTION OF SYMBOLS 11 Transmission part 12 Optical fiber which has positive wavelength dispersion characteristic in wavelength 1310 and 1550 nm band 13 Negative dispersion optical fiber 14 Reception part 15 Broadband optical transmission line 21 Cladding part 22 1st core part 23 2nd core part 31 Cladding part 32 Sky Hole 81 Core part 82 Clad part 83 Hole

Claims (5)

波長1310nm帯及び波長1550nm帯で負の波長分散特性を有し、前記波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバの、少なくとも前記波長1310nm帯及び波長1550nm帯を含む2波長帯域における累積分散を同時に低減する負分散光ファイバであって、
波長1625nmにおける波長分散D 1625 と波長1550nmにおける波長分散D 1550 との比率D 1625 /D 1550 が1.1〜1.2であり、波長1310nmにおける波長分散D 1310 と前記波長分散D 1550 との比率D 1310 /D 1550 が0.3〜0.6であることと、
屈折率が均一なクラッド部と、前記クラッド部よりも高い屈折率を有する第1コア部と、前記クラッド部よりも低い屈折率を有する第2コア部とを有し、
前記第2コア部の半径aに対する前記第1コア部の半径a1の比率Ra=a1/aが0.24〜0.70の範囲であり、前記第2コア部の前記クラッド部に対する比屈折率差Δ1と、前記第1コア部の前記クラッド部に対する比屈折率差Δとの比率RΔ=Δ1/Δが−0.13〜−1.73の範囲であり、かつ前記第2コア部の半径a及び第1コア部の比屈折率差Δが、それぞれ2.3〜6.0μm及び0.3〜1.5%の範囲であることを特徴とする負分散光ファイバ。
Two wavelengths including at least the wavelength 1310 nm band and the wavelength 1550 nm band of an optical fiber having negative wavelength dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band and having positive wavelength dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band A negative dispersion optical fiber that simultaneously reduces the cumulative dispersion in the band,
Ratio D 1625 / D 1550 of the chromatic dispersion D 1550 at a wavelength dispersion D 1625 and the wavelength 1550nm in wavelength 1625nm is 1.1 to 1.2, the ratio of the chromatic dispersion D 1550 and the wavelength dispersion D 1310 at a wavelength of 1310nm D 1310 / D 1550 is 0.3 to 0.6,
A clad part having a uniform refractive index, a first core part having a higher refractive index than the clad part, and a second core part having a lower refractive index than the clad part,
The ratio Ra = a1 / a of the radius a1 of the first core portion to the radius a of the second core portion is in the range of 0.24 to 0.70, and the relative refractive index of the second core portion to the cladding portion. The ratio RΔ = Δ1 / Δ between the difference Δ1 and the relative refractive index difference Δ of the first core portion with respect to the cladding portion is in the range of −0.13 to −1.73, and the radius of the second core portion A negative dispersion optical fiber, wherein the relative refractive index difference Δ between a and the first core portion is in the range of 2.3 to 6.0 μm and 0.3 to 1.5%, respectively.
請求項に記載の負分散光ファイバにおいて、
前記クラッド部に、前記第1コア部の中心から距離Λの円周に外接するように配置された、直径dの少なくとも6個以上の空孔を有し、
前記距離Λと前記第2コア部の半径aとの比率Λ/aが2.0以上であり、かつ前記空孔直径dと前記第2コア部の直径2aとの比率d/2aが0.5以上であることを特徴とする負分散光ファイバ。
The negative dispersion optical fiber according to claim 1 ,
The clad portion has at least six holes having a diameter d, which are arranged so as to circumscribe a circumference of a distance Λ from the center of the first core portion,
The ratio Λ / a between the distance Λ and the radius a of the second core part is 2.0 or more, and the ratio d / 2a between the hole diameter d and the diameter 2a of the second core part is 0. A negative dispersion optical fiber characterized by being 5 or more.
請求項1又は2に記載の負分散光ファイバと、
波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバとを用いて構成されることを特徴とする広帯域光伝送路。
The negative dispersion optical fiber according to claim 1 or 2 ,
A broadband optical transmission line comprising an optical fiber having positive chromatic dispersion characteristics in a wavelength 1310 nm band and a wavelength 1550 nm band.
請求項に記載の広帯域光伝送路において、
前記波長1310nm帯及び波長1550nm帯で正の波長分散特性を有する光ファイバが、複数の空孔が軸方向に開けられた構造を有する空孔ファイバであることを特徴とする広帯域光伝送路。
In the broadband optical transmission line according to claim 3 ,
A broadband optical transmission line, wherein the optical fiber having positive chromatic dispersion characteristics in the wavelength 1310 nm band and the wavelength 1550 nm band is a hole fiber having a structure in which a plurality of holes are opened in the axial direction.
請求項又はに記載の広帯域光伝送路を用い、少なくとも波長1310nm帯及び波長1550nm帯を含む2波長帯を信号伝送帯域として使用することを特徴とする光伝送システム。 5. An optical transmission system using the broadband optical transmission line according to claim 3 or 4 , wherein at least two wavelength bands including a wavelength 1310 nm band and a wavelength 1550 nm band are used as a signal transmission band.
JP2006318447A 2006-11-27 2006-11-27 Negative dispersion optical fiber, broadband optical transmission line and optical transmission system Expired - Fee Related JP4750678B2 (en)

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US5361319A (en) * 1992-02-04 1994-11-01 Corning Incorporated Dispersion compensating devices and systems
CA2340948A1 (en) * 1999-06-25 2001-01-04 The Furukawa Electric Co., Ltd. Dispersion compensation optical fiber and optical transmission line comprising the dispersion compensation optical fiber
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