CA2356712A1 - Optical fiber and optical communication system using this optical fiber - Google Patents
Optical fiber and optical communication system using this optical fiber Download PDFInfo
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- CA2356712A1 CA2356712A1 CA002356712A CA2356712A CA2356712A1 CA 2356712 A1 CA2356712 A1 CA 2356712A1 CA 002356712 A CA002356712 A CA 002356712A CA 2356712 A CA2356712 A CA 2356712A CA 2356712 A1 CA2356712 A1 CA 2356712A1
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02004—Optical fibres with cladding with or without a coating characterised by the core effective area or mode field radius
- G02B6/02009—Large effective area or mode field radius, e.g. to reduce nonlinear effects in single mode fibres
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02214—Optical fibres with cladding with or without a coating tailored to obtain the desired dispersion, e.g. dispersion shifted, dispersion flattened
- G02B6/02219—Characterised by the wavelength dispersion properties in the silica low loss window around 1550 nm, i.e. S, C, L and U bands from 1460-1675 nm
- G02B6/02228—Dispersion flattened fibres, i.e. having a low dispersion variation over an extended wavelength range
- G02B6/02238—Low dispersion slope fibres
- G02B6/02242—Low dispersion slope fibres having a dispersion slope <0.06 ps/km/nm2
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02214—Optical fibres with cladding with or without a coating tailored to obtain the desired dispersion, e.g. dispersion shifted, dispersion flattened
- G02B6/02219—Characterised by the wavelength dispersion properties in the silica low loss window around 1550 nm, i.e. S, C, L and U bands from 1460-1675 nm
- G02B6/02266—Positive dispersion fibres at 1550 nm
- G02B6/02271—Non-zero dispersion shifted fibres, i.e. having a small positive dispersion at 1550 nm, e.g. ITU-T G.655 dispersion between 1.0 to 10 ps/nm.km for avoiding nonlinear effects
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03638—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only
- G02B6/03644—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 3 layers only arranged - + -
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03661—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only
- G02B6/03666—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 4 layers only arranged - + - +
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03688—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 5 or more layers
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2203/00—Fibre product details, e.g. structure, shape
- C03B2203/10—Internal structure or shape details
- C03B2203/22—Radial profile of refractive index, composition or softening point
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2203/00—Fibre product details, e.g. structure, shape
- C03B2203/36—Dispersion modified fibres, e.g. wavelength or polarisation shifted, flattened or compensating fibres (DSF, DFF, DCF)
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/028—Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
- G02B6/0281—Graded index region forming part of the central core segment, e.g. alpha profile, triangular, trapezoidal core
Abstract
The present invention resides in an optical fiber able to form an optical transmitting line for wavelength division multiplexing transmission in a wavelength band of 1.5 µm using a Raman amplifier, and an optical communication system using this optical fiber. The optical fiber has an effective core area from 40 µm2 to 60 µm2 in a set wavelength band of at least one portion of a wavelength band of 1.5 µm; a dispersion value from 4 to 10 ps/nm/km at a wavelength of 1.55 µm; a dispersion slope set to a positive value equal to or smaller than 0.04 ps/nm2/km in a wavelength band of 1.55 µm; and a zero dispersion wavelength equal to or smaller than 1.4 µm. Further, a cutoff wavelength is set to be equal to or smaller than 1.5 µm at a length of 2 m, and a bending loss is set to be equal to or smaller than 5 dB/m at a diameter of 20 mm in the wavelength band of 1.5 µm. In a refractive index profile of the optical fiber, for example, a relative refractive index difference .DELTA.1 of a first glass layer as an innermost layer with respect to a reference layer, and a relative refractive index difference .DELTA.3 of the refractive index of a third glass layer as a third layer from an inner side with respect to the reference layer are set to be positive. Further, a relative refractive index difference .DELTA.2 of a second glass layer as a second layer from the inner side with respect to the reference layer is set to be negative.
Description
OPTICAL FIBER AND OPTICAL COMMUNICATION SYSTEM
USING THIS OPTICAL FIBER
Field of the Invention This invention relates to an optical fiber used in optical transmission such as wavelength division multiplexing (WDM) transmission, etc. in a wavelength band of e. g. , 1. 5 Nm, etc., and optical communication systems using this optical fiber.
Background of the Invention A communication information capacity tends to be greatly increased as information society is developed. Techniques of the wavelength division multiplexing transmission (WDM
transmission) and time division multiplexing (TDM) transmission are noticed as such information is increased.
This wavelength division multiplexing transmission uses a system for transmitting signals of plural wavelengths by one optical fiber. Therefore, this system is an optical transmitting system suitable for high capacity and high bit-rate transmission. The wavelength division multiplexing transmission technique is vigorously studied at present.
It is considered at present that the wavelength division multiplexing transmission is performed in a wavelength band of 1.55 ~m as a gain band of an erbium-doped optical fiber amplifier. The wavelength band of 1. 55 ~m is a wavelength band with 1550 nm in wavelength approximately as a center, e.g., as in a wavelength band from 1530 nm to 1570 nm.
However, there are problems of an increase in power of an optical signal and a non-linear phenomenon due to an interaction between signals, etc. to perform the wavelength division multiplexing transmission. Therefore, for example, it is reported in a society report document OFC' 97 TuNlb of Japan, etc. to consider that a non-linear refractive index difference (n2) is reduced and restrained to restrain the non-linear phenomenon.
It is also noticed to consider that an effective core area (Aeff) of the optical fiber is increased together with this reduction in the non-linear refractive index difference.
Distortion ~NL of a signal due to the non-linear phenomenon is generally represented by the followingformula (1). Therefore, when the effective core area of the optical fiber is increased, the waveform distortion of a signal due to the non-linear phenomenon can be reduced.
TNL- ( 27CXn2Xheffxp ) I ( ~XAeff ) --- ~ 1 ) In the formula ( 1 ) , ~, n2, Leffi P and ~, respectively designate a ratio of the circumference of a circle to its diameter, a non-linear refractive index, an effective optical fiber length, signal power and a signal optical wavelength.
Accordingly, it is very important to enlarge the effective core area in the optical fiber used for e.g. the wavelength multiplexing transmission, and this enlargement is very noticed as reported in society report documents OFC'96 WK15 and OFC'97 YuN2 of Japan.
Summary of the Invention The present invention provides an optical fiber and an optical communication system using this optical fiber.
The optical fiber of the invention comprises:
an effective core area from 40 Eun2 to 60 Eun2 in a set wavelength band of at least one portion of a wavelength band of 1.5 Vim;
a dispersion value set to 4 ps/nm/km or more and 10 ps/nm/km or less at a wavelength of 1.55 Eun;
a dispersion slope set to a positive value equal to or smaller than 0.04 ps/nm2/km in a wavelength band of 1.55 N.m;
and a zero dispersion wavelength equal to or smaller than 1. 4 ~,m .
Brief Description of the Drawings Exemplary embodiments of the invention will now be described in conjunction with drawings, in which:
Fig, lA is an explanatory view showing the construction of a refractive index profile in a first embodiment of an optical fiber in the invention.
Fig. 1B is an explanatory view showing a sectional construction of the optical fiber in the first embodiment of the optical fiber in the invention.
Fig. 2 is an explanatory view showing a refractive index profile construction in a second embodiment of the optical fiber in the invention.
Fig. 3 is an explanatory view showing a refractive index profile construction in a third embodiment of the optical fiber in the invention.
Detailed Description In an optical fiber, a diffusion slope is generally increased when an effective core area is enlarged. The problem of a difference in chromatic dispersion every wavelength is caused by the increase in dispersion slope, and becomes a great obstacle in wavelength division multiplexing transmission.
Therefore, a reduction in dispersion slope is a very important.
It is studied in recent years that a Raman amplifier is applied instead of the wavelength division multiplexing transmission using the erbium-doped optical fiber amplifier, and the wavelength division multiplexing transmission is performed in e. g. , a wavelength band of 1. 5 ~.tm. The wavelength band of 1.5 ~m is a wavelength band with 1500 nm in wavelength approximately as a center, e.g. as in a wavelength band from 1500 nm to 1650 nm. Hereafter, the term of the wavelength band of 1.5 N,m is used as this meaning.
The Raman amplifier is an optical amplifier utilizing Raman amplification described below. The Raman amplification is an amplifying method of an optical signal utilizing a so-called Raman amplifying phenomenon. In the Raman amplifying phenomenon, when pumping light as strong light is incident to the optical fiber, a gain appears about 100 nm on a long wavelength side from a pumping light wavelength by induced Raman scattering, and signal light in a wavelength area having this gain is amplified when this signal light is incident to the optical fiber in this pumped state.
Therefore, when the wavelength division multiplexing transmission in a wavelength band of 1.5 Eun is performed by using the Raman amplifier, pumping light having about 1.4 Eun in wavelength is incident to the optical fiber.
However, in the optical fiber conventionally considered for the wavelength division multiplexing transmission, wavelength dispersion at a wavelength of 1.55 Eun approximately ranges from -4 ps/nm/km to +6 ps/nm/km, and its dispersion slope is 0.05 ps/nm2/km or more. Therefore, in the optical fiber conventionally considered for the wavelength division multiplexing transmission, a zero dispersion wavelength becomes 1.4 ~tm or more so that an interference of the pumping light of about 1.4 pm in wavelength and four-wave mixing, etc.
is caused.
In an optical fiber and an optical communication system in one aspect of the invention, no problem of an interference with pumping light, etc. is almost caused even when the wavelength division multiplexing transmission in a wavelength band of 1.5 ~m is performed by using e.g., the Raman amplifier, and the optical fiber and the optical communication system have a low dispersion slope with low non-linearity.
Concrete embodiments of the invention will next be explained on the basis of the drawings. Fig. lA shows a refractive index distribution profile in a first embodiment of an optical fiber in the invention. The profile of the refractive index distribution of the optical fiber can be set to refractive index profiles in various modes. However, in the first embodiment, a refractive index profile as shown in Fig. lA is adopted. This refractive index profile is relatively simple in structure, and is easily designed and controlled in refractive index structure.
The optical fiber of the first embodiment has multiple (four layers here) glass layers (a first glass layer 1, a second glass layer 2, a third glass layer 3 and a reference layer 6) adjacent to each other and having different compositions. As shown in Fig. 1B, these glass layers are formed in a concentric shape. The reference layer 6 as an outermost layer is a layer constituting a reference of the refractive index distribution among the four glass layers. Three glass layers constructed by the first glass layer 1, the second glass layer 2 and the third glass layer 3 are formed insides this reference layer 6.
In the optical fiber of the first embodiment, a maximum refractive index of the first glass layer 1 formed on an innermost side of the optical fiber, end a maximum refractive index of the third glass layer 3 as a third layer from an inner side are set to be higher than the refractive index of the reference layer 6. Further, in the optical fiber of the first embodiment, a minimum refractive index of the second glass layer 2 as a second layer from the inner side of the optical fiber is set to be lower than the refractive index of the reference layer 6. A refractive index distribution shape of the first glass layer 1 is formed irk a shape.
In the optical fiber of the first embodiment, D1>03>02 is formed when a maximum relative refractive index difference of the first glass layer 1 with respect to the reference layer 6 is set to 01, a minimum relative refractive index difference of the second glass layer 2 with respect to the reference layer 6 is set to D2, and a maximum relative refractive index difference of the third glass layer' 3 with respect to the reference layer 6 is set to 03.
In this specification, the refractive index of a maximum refractive index portion of the first glass layer is set to nl, the refractive index of a minimum refractive index portion of the second glass layer is set to n2, the refractive index of a maximum refractive index portion of the third glass layer is set to n3, and the refractive index of the reference layer is set to n6. The respective relative refractive index differences 01, O2 and 03 are respectively defined by the following approximate formulas (2) to (4).
~1=((nl-n6)/n6}x100 --- (2) ~2={(n2-n6)/n6}x100 --- (3) ~3-((n3-n6)/n6}x100 --- (9) The optical fiber of the first embodiment has the refractive index profile shown in Fig. lA, and also has the following construction. Namely, the optical fiber of the first embodiment has a construction in which an effective core area ranges from 90 Eun2 to 60 Eun2 in a set wavelength band of at least one portion of a wavelength band of 1.5 Eun. This optical fiber also has a construction in which a dispersion value at a wavelength of 1.55 Eun is set to 4 ps/nm/km or more and is set to 10 ps/nm/km or less. This optical fiber also has a construction in which a dispersion slope in the wavelength band of 1.55 ~m is set to a positive value equal to or smaller than 0.04 ps/nm2/km. This optical fiber further has a construction in which a zero dispersion wavelength is set to 1.4 ~m or less. For example, the set wavelength band is a wavelength band of 1.55 ~.un.
Further, the optical fiber of the first embodiment has a construction in which a cutoff wavelength at a length of 2 m is set to 1.5 Eun or less, and a bending loss at a diameter of 20 mm in the wavelength band of 1.5 ~m is set to 5 dB/m or less.
The present inventors have considered that the optical fiber of the first embodiment is applied to wavelength division multiplexing transmission in the wavelength band of 1.5 Eun, and the following consideration is taken into account with respect to the refractive index profile shown in Fig. lA.
Namely, respective relative refractive indexes O1, 02, D3, a and respective diameters a, b, c are set to parameters, and these values are set to various values . When a single mode condition is satisfied, a profile range is searched such that the dispersion slope (an average value of the dispersion slope) in the wavelength band of 1.55 ~.un among the wavelength band of 1.5 ~.m becomes a positive value equal to or smaller than 0: 03 ps/nm2/km. An optimum profile of the first embodiment is calculated from the relation of the effective core area and a bending loss value in this profile range.
As a result, when no relative refractive index difference 01 is set to lie within a range equal to or smaller than 0.6 0, it has been found that it is difficult to set the effective core area to 40 Eun2 or more when the dispersion slope is set to a positive value equal to or smaller than 0.03 ps/nm2/km.
Further, it has been found that the bending loss becomes a value greater than 5 dB/m when the relative refractive index difference O1 is set to be smaller than 0.5 ~. Therefore, the range of the relative refractive index difference D1 is set to a range from 0.5 ~ to 0.6 The relative refractive index difference 01 is set to lie within the above range and the constant a not increasing the dispersion slope is calculated when the effective core area is enlarged. It is then judged that the constant a is suitably set to 5.0 or more. In this condition, the refractive index profile is calculated such that the effective core area can be set to 40 ~tm2 or more and 60 ~,un2 or less, and the dispersion slope can be set to a positive value equal to or smaller than 0.04 ps/nm2/km while the bending loss value at the diameter of 20 mm is held to be equal to or smaller than 5 dB/m.
As a result, when the relative refractive index difference 02 is set to be smaller than -0.4 $, it is difficult to set the effective core area to be equal to or greater than 40 ~m2, and the bending loss value at the diameter of 20 mm also becomes a value greater than 5 dB/m. Further, when the relative refractive index difference D2 is set to be greater than -0.1 ~, the dispersion slope becomes a value greater than 0.04 ps/nm2/km. Therefore, the range of the relative refractive index difference 02 is set to a range from -0.4 ~
to -0.1 ~.
When the relative refractive index difference O3 is set to be smaller than 0.1 $, it is difficult to set the effective core area to be equal to or greater than 40 Wn2, and the bending loss value at the diameter of 20 mm also becomes a value greater than 5 dB/m. Further, when the relative refractive index difference O3 is set to be greater than 0.4 $, a cutoff wavelength ~,c becomes larger than 1. 5 Eun. Therefore, the range of the relative refractive index difference 03 is set to a range from 0.1 ~ to 0.4 ~k.
The refractive index profile in each of concrete examples 1 to 4 shown in table 1 is determined from the above consideration results.
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The table 1 shows setting examples of the respective relative refractive index differences D1, D2, 03, and examples of the value of the constant a, and a ratio of a:b:c, a core diameter and simulation results of characteristics of the optical fiber when an outside diameter of the first glass layer 1 is set to a, an outside diameter of the second glass layer 2 is set to b, and an outside diameter of the third glass layer 3 is set to c.
In the table 1 and tables shown below, respective values of the core diameter and the optical fiber characteristics show the following values. Namely, the core diameter shows the outside diameter of the second layer (the value of b in a corresponding figure among Figs. 1 to 3). Dispersion shows a dispersion value at a wavelength of 1.55 ~.un. Slope shows an average value of the dispersion slope (dispersion gradient) in a wavelength band of 1.55 ~.un, and becomes a value equal to the dispersion slope in a wavelength band of 1.5 ~tm. Aeff shows an effective core area when 1.55 Etm signal is propagated. ~,c shows a cutoff wavelength at a length of 2 m. Bending loss shows a value of the bending loss at a diameter of 20 mm with respect to light of 1.55 dun in wavelength. ~,o shows a zero dispersion wavelength.
In the optical fiber of the first embodiment, the zero dispersion wavelength can be set to be equal to or smaller than 1.4 ~m by the refractive index profile shown in Fig. lA and the table 1, and this optical fiber has characteristics shown in the table 1 at a wavelength of 1.55 Eun and in a wavelength band including this wavelength 1. 55 Eun. Namely, in the optical fiber of the first embodiment, the dispersion value at the wavelength of 1.55 Eun is set to 4 ps/nm/km or more, and 10 ps/nm/km or less, and the dispersion slope in the wavelength band of 1.55 dun is set to a positive value equal to or smaller than 0.04 ps/nm2/km so that the zero dispersion wavelength can be set to be equal to or smaller than 1.4 N.m.
Accordingly, in the optical fiber of the first embodiment, when Raman amplification is performed in the wavelength band of 1.5 Vim, it is possible to restrain the generation of an interference of pumping light of about 1.4 ~m in wavelength and four-wave mixing, etc.
Further, since the dispersion value at the wavelength of 1.55 Eun is set to be equal to or smaller than 10 ps/nm/km as mentioned above, no optical fiber of the first embodiment has large local dispersion as in a case in which the dispersion value is set to be greater than 10 ps/nm/km. Accordingly, the optical fiber of the first embodiment can restrain distortion due to dispersion, and can also reduce the difference in dispersion between wavelengths.
Further, the optical fiber of the first embodiment can reduce the difference in dispersion between wavelengths since an absolute value of the dispersion slope is reduced by setting the dispersion slope in the wavelength band of 1.55 ~,m to a positive value equal to or smaller than 0.04 ps/nm2/km.
Accordingly, the optical fiber of the first embodiment becomes an optical fiber suitable for the wavelength division multiplexing transmission in the wavelength band of 1.5 ~m to which the Raman amplifier is applied.
Further, since the absolute value of the dispersion slope in the optical fiber of the first embodiment is small, the dispersion slope of the optical fiber of the first embodiment can be easily compensated by connecting e.g., a dispersion slope compensating fiber (DSCF), etc. conventionally developed to the optical fiber of the first embodiment.
As is well known, there are a Raman amplifier of a distribution type and a Raman amplifier of a concentration type in the Raman amplifier. When the Raman amplifier of the concentration constant type is applied to the wavelength division multiplexing transmission, no nonlinear phenomenon within the optical fiber can be neglected. In this case, in the optical fiber of the first embodiment, the effective core area is set to 90 E.tm2 or more equal to or greater than that of the conventional optical fiber for the wavelength division multiplexing transmission in the set wavelength band of at least one portion of the wavelength band of 1. 5 ~.m. Accordingly, the optical fiber of the first embodiment can also restrain signal light distortion due to the nonlinear phenomenon by performing the wavelength division multiplexing transmission in this set wavelength band.
Further, when the Raman amplifier of the distribution constant type is applied, maximum input power of the optical fiber can be reduced and restrained so that the signal light distortion due to the nonlinear phenomenon within the optical fiber can be reliably restrained.
When the effective core area is too large, a reduction in efficiency of the Raman amplifier is caused. However, in the optical fiber of the first embodiment, the effective core area is set to 60 Eun2 or less in the set wavelength band of at least one portion of the wavelength band of 1.5 Vim.
Accordingly, in the optical fiber of the first embodiment, the reduction in efficiency of the Raman amplifier can be restrained by performing the wavelength division multiplexing transmission using the Raman amplifier in this set wavelength band.
Since the cutoff wavelength is set to 1. 5 dun in wavelength or less in the optical fiber of the first embodiment, a single mode operation can be precisely performed in a wavelength band equal to or greater than 1.5 Eun in wavelength. Further, the optical fiber of the first embodiment can also restrain the bending loss when the optical fiber is formed as a cable.
Accordingly, the optical fiber of the first embodiment becomes an optical fiber suitable for the wavelength division multiplexing transmission in the wavelength band of 1.5 ~.m and able to efficiently perform the Kaman amplification. An optical communication system applying the optical fiber of the first embodiment thereto as an optical transmission line can be set to a wavelength division multiplexing transmission system in the wavelength band of 1.5 E.tm, etc. using e.g. the Kaman amplification with high quality.
When the restriction of an influence of the four-wave mixing is seriously considered in the first embodiment and second and third embodiments shown below, it is desirable to set the dispersion value to 6 ps/nm/km or more as shown in each table.
Fig. 2 shows a refractive index profile in a second embodiment of the optical fiber in the invention. The second embodiment approximately has a construction similar to that of the first embodiment. The second embodiment characteristically differs from the first embodiment in that a glass layer having a refractive index lower than that of a reference layer 6 is arranged between a third glass layer 3 and the reference layer 6. This glass layer having the low refractive index is a fourth glass layer 4. The fourth glass layer 4 is adjacently arranged on an outer circumferential side of the third glass layer 3.
In this specification, a relative refractive index difference O4 of the fourth glass layer 4 with respect to the reference layer 6 is defined by an approximate formula (5) shown below when the refractive index of a minimum refractive index portion of the fourth glass layer 4 is set to n4. In the second embodiment, the relative refractive index difference D4 is set to approximately range from -0.2 ~ to -0.1 O4.((n4-n6)/n6?x100 --- (5) Table 2 shows the relative refractive index difference 04 of the optical fiber in each of concrete examples 5 to 8 of the second embodiment, an outside diameter ratio a:b:c:d of the first to fourth glass layers, and characteristics of the optical fiber. In the concrete examples 5 to 8, relative refractive index differences Dl, ~2, 03 and constant a are set to values similar to those in the optical fiber of the concrete example 2 shown in the table 1. The outside diameter ratio a:b:c:d of the first to fourth glass layers is a ratio when the outside diameter of the first glass layer 1 is a, the outside diameter of the second glass layer 2 is b, the outside diameter of the third glass layer 3 is c, and the outside diameter of the fourth glass layer 4 is d.
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As shown in the table 2, in the optical fiber of the second embodiment, the cutoff wavelength can be reduced, and it is possible to set an optical fiber also able to cope with wavelength multiplexing transmission in a wavelength band of 1.31 ~m as well as a wavelength band of 1.55 ~.m.
Fig. 3 shows a refractive index profile of a third embodiment of the optical fiber in the invention. The third embodiment approximately has a construction similar to that of the first embodiment. The third embodiment characteristically differs from the first embodiment in that a glass layer having a refractive index higher than that of a reference layer 6 is arranged between a third glass layer 3 and the reference layer 6. This glass layer having the high refractive index is a fifth glass layer 5.
In the third embodiment, a fourth glass layer 4 is adjacently arranged on an outer circumferential side of the third glass layer 3, and has a refractive index equal to that of the reference layer 6. The fifth glass layer 5 is adjacently arranged on an outer circumferential side of the fourth glass layer 4.
In this specification, a relative refractive index difference D5 of the fifth glass layer 5 with respect to the reference layer 6 is defined by an approximate formula ( 6) shown below when the refractive index of a maximum refractive index portion of the fifth glass layer is set to n5. In the third embodiment, the relative refractive index difference d5 is set to approximately range from 0.1 ~ to 0.2 ~.
~5-((n5-n6)/n6)x100 --- (6) Table 3 shows the relative refractive index difference D5 of the optical fiber in each of concrete examples 9 to 12 of the third embodiment, an outside diameter ratio a:b:c:d:e of the first to fifth glass layers, and characteristics of the optical fiber. In the concrete examples 9 to 12, relative refractive index differences D1, D2, D3 and constant a are set to values similar to those in the optical fiber of the concrete example 3 shown in the table 1. The outside diameter ratio a:b:c:d:e of the first to fifth glass layers is a ratio when the outside diameter of the first glass layer 1 is a, the outside diameter of the second glass layer 2 is b, the outside diameter of the third glass layer 3 is c, the outside diameter of the fourth glass layer 4 is d, and the outside diameter of the fifth glass layer 5 is e.
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As shown in the table 3, the optical fiber of the third embodiment can have effects similar to those in the first embodiment.
A fabrication example of the optical fiber actually fabricated on the basis of the above simulation results will next be explained. The present inventors fabricated the actual optical fiber on the basis of a design of the optical fiber of the concrete example 2 of the table 1. Table 4 shows results of this fabrication.
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m m As clearly seen from the table 4, similar to design values, the optical fiber of each fabrication example has low dispersion and a low dispersion slope, and has low transmission loss. Further, in the optical fiber of each fabrication example, since the zero dispersion wavelength (~,o) is equal to or smaller than 1400 nm, no problem of an interference with pumping light, etc. is caused even when the wavelength division multiplexing transmission is performed in a wavelength band of 1.5 Eun by using e.g. the Raman amplifier.
The invention is not limited to each of the above embodiments, but various kinds of embodiment modes can be adopted. For example, the optical fiber of the invention may have a refractive index profile except for the refractive index profile shown in each of the above embodiments. Namely, in the optical fiber of the invention, it is sufficient to set the effective core area, the dispersion value and the dispersion slope at least at a set wavelength or in a set wavelength band in the wavelength band of 1.5 Eun to e.g.
suitable values as shown in each of the above embodiments, and set the zero dispersion wavelength to 1. 4 Eun or less . In this construction, it is possible to construct an optical fiber and an optical communication system using this optical fiber in which the wavelength division multiplexing transmission in the wavelength band of 1 . 5 ~m using the Raman amplifier is performed with high quality.
In the above examples, the optical fiber and the optical communication system are applied to the wavelength division multiplexing transmission in the wavelength band of 1.5 ~,m using the Raman amplifier. However, the optical fiber and the optical communication system of the invention can be also applied to the wavelength division multiplexing transmission using e. g. an erbium-doped optical fiber amplifier except for the Raman amplifier. Further, in accordance with the construction of the optical fiber, the optical fiber and the optical communication system can be also applied to the wavelength division multiplexing transmission in a wavelength band except for the wavelength band of 1.5 ~.un in addition to this wavelength band of 1.5 Eun.
Further, in the above examples, the wavelength band is set to the wavelength band of 1.55 ~,tm. However, the set wavelength band is not particularly limited, but is suitably set in conformity with the wavelength band applied to the wavelength division multiplexing transmission, etc.
USING THIS OPTICAL FIBER
Field of the Invention This invention relates to an optical fiber used in optical transmission such as wavelength division multiplexing (WDM) transmission, etc. in a wavelength band of e. g. , 1. 5 Nm, etc., and optical communication systems using this optical fiber.
Background of the Invention A communication information capacity tends to be greatly increased as information society is developed. Techniques of the wavelength division multiplexing transmission (WDM
transmission) and time division multiplexing (TDM) transmission are noticed as such information is increased.
This wavelength division multiplexing transmission uses a system for transmitting signals of plural wavelengths by one optical fiber. Therefore, this system is an optical transmitting system suitable for high capacity and high bit-rate transmission. The wavelength division multiplexing transmission technique is vigorously studied at present.
It is considered at present that the wavelength division multiplexing transmission is performed in a wavelength band of 1.55 ~m as a gain band of an erbium-doped optical fiber amplifier. The wavelength band of 1. 55 ~m is a wavelength band with 1550 nm in wavelength approximately as a center, e.g., as in a wavelength band from 1530 nm to 1570 nm.
However, there are problems of an increase in power of an optical signal and a non-linear phenomenon due to an interaction between signals, etc. to perform the wavelength division multiplexing transmission. Therefore, for example, it is reported in a society report document OFC' 97 TuNlb of Japan, etc. to consider that a non-linear refractive index difference (n2) is reduced and restrained to restrain the non-linear phenomenon.
It is also noticed to consider that an effective core area (Aeff) of the optical fiber is increased together with this reduction in the non-linear refractive index difference.
Distortion ~NL of a signal due to the non-linear phenomenon is generally represented by the followingformula (1). Therefore, when the effective core area of the optical fiber is increased, the waveform distortion of a signal due to the non-linear phenomenon can be reduced.
TNL- ( 27CXn2Xheffxp ) I ( ~XAeff ) --- ~ 1 ) In the formula ( 1 ) , ~, n2, Leffi P and ~, respectively designate a ratio of the circumference of a circle to its diameter, a non-linear refractive index, an effective optical fiber length, signal power and a signal optical wavelength.
Accordingly, it is very important to enlarge the effective core area in the optical fiber used for e.g. the wavelength multiplexing transmission, and this enlargement is very noticed as reported in society report documents OFC'96 WK15 and OFC'97 YuN2 of Japan.
Summary of the Invention The present invention provides an optical fiber and an optical communication system using this optical fiber.
The optical fiber of the invention comprises:
an effective core area from 40 Eun2 to 60 Eun2 in a set wavelength band of at least one portion of a wavelength band of 1.5 Vim;
a dispersion value set to 4 ps/nm/km or more and 10 ps/nm/km or less at a wavelength of 1.55 Eun;
a dispersion slope set to a positive value equal to or smaller than 0.04 ps/nm2/km in a wavelength band of 1.55 N.m;
and a zero dispersion wavelength equal to or smaller than 1. 4 ~,m .
Brief Description of the Drawings Exemplary embodiments of the invention will now be described in conjunction with drawings, in which:
Fig, lA is an explanatory view showing the construction of a refractive index profile in a first embodiment of an optical fiber in the invention.
Fig. 1B is an explanatory view showing a sectional construction of the optical fiber in the first embodiment of the optical fiber in the invention.
Fig. 2 is an explanatory view showing a refractive index profile construction in a second embodiment of the optical fiber in the invention.
Fig. 3 is an explanatory view showing a refractive index profile construction in a third embodiment of the optical fiber in the invention.
Detailed Description In an optical fiber, a diffusion slope is generally increased when an effective core area is enlarged. The problem of a difference in chromatic dispersion every wavelength is caused by the increase in dispersion slope, and becomes a great obstacle in wavelength division multiplexing transmission.
Therefore, a reduction in dispersion slope is a very important.
It is studied in recent years that a Raman amplifier is applied instead of the wavelength division multiplexing transmission using the erbium-doped optical fiber amplifier, and the wavelength division multiplexing transmission is performed in e. g. , a wavelength band of 1. 5 ~.tm. The wavelength band of 1.5 ~m is a wavelength band with 1500 nm in wavelength approximately as a center, e.g. as in a wavelength band from 1500 nm to 1650 nm. Hereafter, the term of the wavelength band of 1.5 N,m is used as this meaning.
The Raman amplifier is an optical amplifier utilizing Raman amplification described below. The Raman amplification is an amplifying method of an optical signal utilizing a so-called Raman amplifying phenomenon. In the Raman amplifying phenomenon, when pumping light as strong light is incident to the optical fiber, a gain appears about 100 nm on a long wavelength side from a pumping light wavelength by induced Raman scattering, and signal light in a wavelength area having this gain is amplified when this signal light is incident to the optical fiber in this pumped state.
Therefore, when the wavelength division multiplexing transmission in a wavelength band of 1.5 Eun is performed by using the Raman amplifier, pumping light having about 1.4 Eun in wavelength is incident to the optical fiber.
However, in the optical fiber conventionally considered for the wavelength division multiplexing transmission, wavelength dispersion at a wavelength of 1.55 Eun approximately ranges from -4 ps/nm/km to +6 ps/nm/km, and its dispersion slope is 0.05 ps/nm2/km or more. Therefore, in the optical fiber conventionally considered for the wavelength division multiplexing transmission, a zero dispersion wavelength becomes 1.4 ~tm or more so that an interference of the pumping light of about 1.4 pm in wavelength and four-wave mixing, etc.
is caused.
In an optical fiber and an optical communication system in one aspect of the invention, no problem of an interference with pumping light, etc. is almost caused even when the wavelength division multiplexing transmission in a wavelength band of 1.5 ~m is performed by using e.g., the Raman amplifier, and the optical fiber and the optical communication system have a low dispersion slope with low non-linearity.
Concrete embodiments of the invention will next be explained on the basis of the drawings. Fig. lA shows a refractive index distribution profile in a first embodiment of an optical fiber in the invention. The profile of the refractive index distribution of the optical fiber can be set to refractive index profiles in various modes. However, in the first embodiment, a refractive index profile as shown in Fig. lA is adopted. This refractive index profile is relatively simple in structure, and is easily designed and controlled in refractive index structure.
The optical fiber of the first embodiment has multiple (four layers here) glass layers (a first glass layer 1, a second glass layer 2, a third glass layer 3 and a reference layer 6) adjacent to each other and having different compositions. As shown in Fig. 1B, these glass layers are formed in a concentric shape. The reference layer 6 as an outermost layer is a layer constituting a reference of the refractive index distribution among the four glass layers. Three glass layers constructed by the first glass layer 1, the second glass layer 2 and the third glass layer 3 are formed insides this reference layer 6.
In the optical fiber of the first embodiment, a maximum refractive index of the first glass layer 1 formed on an innermost side of the optical fiber, end a maximum refractive index of the third glass layer 3 as a third layer from an inner side are set to be higher than the refractive index of the reference layer 6. Further, in the optical fiber of the first embodiment, a minimum refractive index of the second glass layer 2 as a second layer from the inner side of the optical fiber is set to be lower than the refractive index of the reference layer 6. A refractive index distribution shape of the first glass layer 1 is formed irk a shape.
In the optical fiber of the first embodiment, D1>03>02 is formed when a maximum relative refractive index difference of the first glass layer 1 with respect to the reference layer 6 is set to 01, a minimum relative refractive index difference of the second glass layer 2 with respect to the reference layer 6 is set to D2, and a maximum relative refractive index difference of the third glass layer' 3 with respect to the reference layer 6 is set to 03.
In this specification, the refractive index of a maximum refractive index portion of the first glass layer is set to nl, the refractive index of a minimum refractive index portion of the second glass layer is set to n2, the refractive index of a maximum refractive index portion of the third glass layer is set to n3, and the refractive index of the reference layer is set to n6. The respective relative refractive index differences 01, O2 and 03 are respectively defined by the following approximate formulas (2) to (4).
~1=((nl-n6)/n6}x100 --- (2) ~2={(n2-n6)/n6}x100 --- (3) ~3-((n3-n6)/n6}x100 --- (9) The optical fiber of the first embodiment has the refractive index profile shown in Fig. lA, and also has the following construction. Namely, the optical fiber of the first embodiment has a construction in which an effective core area ranges from 90 Eun2 to 60 Eun2 in a set wavelength band of at least one portion of a wavelength band of 1.5 Eun. This optical fiber also has a construction in which a dispersion value at a wavelength of 1.55 Eun is set to 4 ps/nm/km or more and is set to 10 ps/nm/km or less. This optical fiber also has a construction in which a dispersion slope in the wavelength band of 1.55 ~m is set to a positive value equal to or smaller than 0.04 ps/nm2/km. This optical fiber further has a construction in which a zero dispersion wavelength is set to 1.4 ~m or less. For example, the set wavelength band is a wavelength band of 1.55 ~.un.
Further, the optical fiber of the first embodiment has a construction in which a cutoff wavelength at a length of 2 m is set to 1.5 Eun or less, and a bending loss at a diameter of 20 mm in the wavelength band of 1.5 ~m is set to 5 dB/m or less.
The present inventors have considered that the optical fiber of the first embodiment is applied to wavelength division multiplexing transmission in the wavelength band of 1.5 Eun, and the following consideration is taken into account with respect to the refractive index profile shown in Fig. lA.
Namely, respective relative refractive indexes O1, 02, D3, a and respective diameters a, b, c are set to parameters, and these values are set to various values . When a single mode condition is satisfied, a profile range is searched such that the dispersion slope (an average value of the dispersion slope) in the wavelength band of 1.55 ~.un among the wavelength band of 1.5 ~.m becomes a positive value equal to or smaller than 0: 03 ps/nm2/km. An optimum profile of the first embodiment is calculated from the relation of the effective core area and a bending loss value in this profile range.
As a result, when no relative refractive index difference 01 is set to lie within a range equal to or smaller than 0.6 0, it has been found that it is difficult to set the effective core area to 40 Eun2 or more when the dispersion slope is set to a positive value equal to or smaller than 0.03 ps/nm2/km.
Further, it has been found that the bending loss becomes a value greater than 5 dB/m when the relative refractive index difference O1 is set to be smaller than 0.5 ~. Therefore, the range of the relative refractive index difference D1 is set to a range from 0.5 ~ to 0.6 The relative refractive index difference 01 is set to lie within the above range and the constant a not increasing the dispersion slope is calculated when the effective core area is enlarged. It is then judged that the constant a is suitably set to 5.0 or more. In this condition, the refractive index profile is calculated such that the effective core area can be set to 40 ~tm2 or more and 60 ~,un2 or less, and the dispersion slope can be set to a positive value equal to or smaller than 0.04 ps/nm2/km while the bending loss value at the diameter of 20 mm is held to be equal to or smaller than 5 dB/m.
As a result, when the relative refractive index difference 02 is set to be smaller than -0.4 $, it is difficult to set the effective core area to be equal to or greater than 40 ~m2, and the bending loss value at the diameter of 20 mm also becomes a value greater than 5 dB/m. Further, when the relative refractive index difference D2 is set to be greater than -0.1 ~, the dispersion slope becomes a value greater than 0.04 ps/nm2/km. Therefore, the range of the relative refractive index difference 02 is set to a range from -0.4 ~
to -0.1 ~.
When the relative refractive index difference O3 is set to be smaller than 0.1 $, it is difficult to set the effective core area to be equal to or greater than 40 Wn2, and the bending loss value at the diameter of 20 mm also becomes a value greater than 5 dB/m. Further, when the relative refractive index difference O3 is set to be greater than 0.4 $, a cutoff wavelength ~,c becomes larger than 1. 5 Eun. Therefore, the range of the relative refractive index difference 03 is set to a range from 0.1 ~ to 0.4 ~k.
The refractive index profile in each of concrete examples 1 to 4 shown in table 1 is determined from the above consideration results.
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The table 1 shows setting examples of the respective relative refractive index differences D1, D2, 03, and examples of the value of the constant a, and a ratio of a:b:c, a core diameter and simulation results of characteristics of the optical fiber when an outside diameter of the first glass layer 1 is set to a, an outside diameter of the second glass layer 2 is set to b, and an outside diameter of the third glass layer 3 is set to c.
In the table 1 and tables shown below, respective values of the core diameter and the optical fiber characteristics show the following values. Namely, the core diameter shows the outside diameter of the second layer (the value of b in a corresponding figure among Figs. 1 to 3). Dispersion shows a dispersion value at a wavelength of 1.55 ~.un. Slope shows an average value of the dispersion slope (dispersion gradient) in a wavelength band of 1.55 ~.un, and becomes a value equal to the dispersion slope in a wavelength band of 1.5 ~tm. Aeff shows an effective core area when 1.55 Etm signal is propagated. ~,c shows a cutoff wavelength at a length of 2 m. Bending loss shows a value of the bending loss at a diameter of 20 mm with respect to light of 1.55 dun in wavelength. ~,o shows a zero dispersion wavelength.
In the optical fiber of the first embodiment, the zero dispersion wavelength can be set to be equal to or smaller than 1.4 ~m by the refractive index profile shown in Fig. lA and the table 1, and this optical fiber has characteristics shown in the table 1 at a wavelength of 1.55 Eun and in a wavelength band including this wavelength 1. 55 Eun. Namely, in the optical fiber of the first embodiment, the dispersion value at the wavelength of 1.55 Eun is set to 4 ps/nm/km or more, and 10 ps/nm/km or less, and the dispersion slope in the wavelength band of 1.55 dun is set to a positive value equal to or smaller than 0.04 ps/nm2/km so that the zero dispersion wavelength can be set to be equal to or smaller than 1.4 N.m.
Accordingly, in the optical fiber of the first embodiment, when Raman amplification is performed in the wavelength band of 1.5 Vim, it is possible to restrain the generation of an interference of pumping light of about 1.4 ~m in wavelength and four-wave mixing, etc.
Further, since the dispersion value at the wavelength of 1.55 Eun is set to be equal to or smaller than 10 ps/nm/km as mentioned above, no optical fiber of the first embodiment has large local dispersion as in a case in which the dispersion value is set to be greater than 10 ps/nm/km. Accordingly, the optical fiber of the first embodiment can restrain distortion due to dispersion, and can also reduce the difference in dispersion between wavelengths.
Further, the optical fiber of the first embodiment can reduce the difference in dispersion between wavelengths since an absolute value of the dispersion slope is reduced by setting the dispersion slope in the wavelength band of 1.55 ~,m to a positive value equal to or smaller than 0.04 ps/nm2/km.
Accordingly, the optical fiber of the first embodiment becomes an optical fiber suitable for the wavelength division multiplexing transmission in the wavelength band of 1.5 ~m to which the Raman amplifier is applied.
Further, since the absolute value of the dispersion slope in the optical fiber of the first embodiment is small, the dispersion slope of the optical fiber of the first embodiment can be easily compensated by connecting e.g., a dispersion slope compensating fiber (DSCF), etc. conventionally developed to the optical fiber of the first embodiment.
As is well known, there are a Raman amplifier of a distribution type and a Raman amplifier of a concentration type in the Raman amplifier. When the Raman amplifier of the concentration constant type is applied to the wavelength division multiplexing transmission, no nonlinear phenomenon within the optical fiber can be neglected. In this case, in the optical fiber of the first embodiment, the effective core area is set to 90 E.tm2 or more equal to or greater than that of the conventional optical fiber for the wavelength division multiplexing transmission in the set wavelength band of at least one portion of the wavelength band of 1. 5 ~.m. Accordingly, the optical fiber of the first embodiment can also restrain signal light distortion due to the nonlinear phenomenon by performing the wavelength division multiplexing transmission in this set wavelength band.
Further, when the Raman amplifier of the distribution constant type is applied, maximum input power of the optical fiber can be reduced and restrained so that the signal light distortion due to the nonlinear phenomenon within the optical fiber can be reliably restrained.
When the effective core area is too large, a reduction in efficiency of the Raman amplifier is caused. However, in the optical fiber of the first embodiment, the effective core area is set to 60 Eun2 or less in the set wavelength band of at least one portion of the wavelength band of 1.5 Vim.
Accordingly, in the optical fiber of the first embodiment, the reduction in efficiency of the Raman amplifier can be restrained by performing the wavelength division multiplexing transmission using the Raman amplifier in this set wavelength band.
Since the cutoff wavelength is set to 1. 5 dun in wavelength or less in the optical fiber of the first embodiment, a single mode operation can be precisely performed in a wavelength band equal to or greater than 1.5 Eun in wavelength. Further, the optical fiber of the first embodiment can also restrain the bending loss when the optical fiber is formed as a cable.
Accordingly, the optical fiber of the first embodiment becomes an optical fiber suitable for the wavelength division multiplexing transmission in the wavelength band of 1.5 ~.m and able to efficiently perform the Kaman amplification. An optical communication system applying the optical fiber of the first embodiment thereto as an optical transmission line can be set to a wavelength division multiplexing transmission system in the wavelength band of 1.5 E.tm, etc. using e.g. the Kaman amplification with high quality.
When the restriction of an influence of the four-wave mixing is seriously considered in the first embodiment and second and third embodiments shown below, it is desirable to set the dispersion value to 6 ps/nm/km or more as shown in each table.
Fig. 2 shows a refractive index profile in a second embodiment of the optical fiber in the invention. The second embodiment approximately has a construction similar to that of the first embodiment. The second embodiment characteristically differs from the first embodiment in that a glass layer having a refractive index lower than that of a reference layer 6 is arranged between a third glass layer 3 and the reference layer 6. This glass layer having the low refractive index is a fourth glass layer 4. The fourth glass layer 4 is adjacently arranged on an outer circumferential side of the third glass layer 3.
In this specification, a relative refractive index difference O4 of the fourth glass layer 4 with respect to the reference layer 6 is defined by an approximate formula (5) shown below when the refractive index of a minimum refractive index portion of the fourth glass layer 4 is set to n4. In the second embodiment, the relative refractive index difference D4 is set to approximately range from -0.2 ~ to -0.1 O4.((n4-n6)/n6?x100 --- (5) Table 2 shows the relative refractive index difference 04 of the optical fiber in each of concrete examples 5 to 8 of the second embodiment, an outside diameter ratio a:b:c:d of the first to fourth glass layers, and characteristics of the optical fiber. In the concrete examples 5 to 8, relative refractive index differences Dl, ~2, 03 and constant a are set to values similar to those in the optical fiber of the concrete example 2 shown in the table 1. The outside diameter ratio a:b:c:d of the first to fourth glass layers is a ratio when the outside diameter of the first glass layer 1 is a, the outside diameter of the second glass layer 2 is b, the outside diameter of the third glass layer 3 is c, and the outside diameter of the fourth glass layer 4 is d.
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As shown in the table 2, in the optical fiber of the second embodiment, the cutoff wavelength can be reduced, and it is possible to set an optical fiber also able to cope with wavelength multiplexing transmission in a wavelength band of 1.31 ~m as well as a wavelength band of 1.55 ~.m.
Fig. 3 shows a refractive index profile of a third embodiment of the optical fiber in the invention. The third embodiment approximately has a construction similar to that of the first embodiment. The third embodiment characteristically differs from the first embodiment in that a glass layer having a refractive index higher than that of a reference layer 6 is arranged between a third glass layer 3 and the reference layer 6. This glass layer having the high refractive index is a fifth glass layer 5.
In the third embodiment, a fourth glass layer 4 is adjacently arranged on an outer circumferential side of the third glass layer 3, and has a refractive index equal to that of the reference layer 6. The fifth glass layer 5 is adjacently arranged on an outer circumferential side of the fourth glass layer 4.
In this specification, a relative refractive index difference D5 of the fifth glass layer 5 with respect to the reference layer 6 is defined by an approximate formula ( 6) shown below when the refractive index of a maximum refractive index portion of the fifth glass layer is set to n5. In the third embodiment, the relative refractive index difference d5 is set to approximately range from 0.1 ~ to 0.2 ~.
~5-((n5-n6)/n6)x100 --- (6) Table 3 shows the relative refractive index difference D5 of the optical fiber in each of concrete examples 9 to 12 of the third embodiment, an outside diameter ratio a:b:c:d:e of the first to fifth glass layers, and characteristics of the optical fiber. In the concrete examples 9 to 12, relative refractive index differences D1, D2, D3 and constant a are set to values similar to those in the optical fiber of the concrete example 3 shown in the table 1. The outside diameter ratio a:b:c:d:e of the first to fifth glass layers is a ratio when the outside diameter of the first glass layer 1 is a, the outside diameter of the second glass layer 2 is b, the outside diameter of the third glass layer 3 is c, the outside diameter of the fourth glass layer 4 is d, and the outside diameter of the fifth glass layer 5 is e.
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As shown in the table 3, the optical fiber of the third embodiment can have effects similar to those in the first embodiment.
A fabrication example of the optical fiber actually fabricated on the basis of the above simulation results will next be explained. The present inventors fabricated the actual optical fiber on the basis of a design of the optical fiber of the concrete example 2 of the table 1. Table 4 shows results of this fabrication.
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The invention is not limited to each of the above embodiments, but various kinds of embodiment modes can be adopted. For example, the optical fiber of the invention may have a refractive index profile except for the refractive index profile shown in each of the above embodiments. Namely, in the optical fiber of the invention, it is sufficient to set the effective core area, the dispersion value and the dispersion slope at least at a set wavelength or in a set wavelength band in the wavelength band of 1.5 Eun to e.g.
suitable values as shown in each of the above embodiments, and set the zero dispersion wavelength to 1. 4 Eun or less . In this construction, it is possible to construct an optical fiber and an optical communication system using this optical fiber in which the wavelength division multiplexing transmission in the wavelength band of 1 . 5 ~m using the Raman amplifier is performed with high quality.
In the above examples, the optical fiber and the optical communication system are applied to the wavelength division multiplexing transmission in the wavelength band of 1.5 ~,m using the Raman amplifier. However, the optical fiber and the optical communication system of the invention can be also applied to the wavelength division multiplexing transmission using e. g. an erbium-doped optical fiber amplifier except for the Raman amplifier. Further, in accordance with the construction of the optical fiber, the optical fiber and the optical communication system can be also applied to the wavelength division multiplexing transmission in a wavelength band except for the wavelength band of 1.5 ~.un in addition to this wavelength band of 1.5 Eun.
Further, in the above examples, the wavelength band is set to the wavelength band of 1.55 ~,tm. However, the set wavelength band is not particularly limited, but is suitably set in conformity with the wavelength band applied to the wavelength division multiplexing transmission, etc.
Claims (7)
1. An optical fiber comprising:
an effective core area from 40 µm2 to 60 µm2 in a set wavelength band of at least one portion of a wavelength band of 1.5 µm;
a dispersion value set to 4 ps/nm/km or more and 10 ps/nm/km or less at a wavelength of 1.55 µm;
a dispersion slope set to a positive value equal to or smaller than 0.04 ps/nm2/km in a wavelength band of 1.55 µm;
and a zero dispersion wavelength equal to or smaller than 1.4 µm.
an effective core area from 40 µm2 to 60 µm2 in a set wavelength band of at least one portion of a wavelength band of 1.5 µm;
a dispersion value set to 4 ps/nm/km or more and 10 ps/nm/km or less at a wavelength of 1.55 µm;
a dispersion slope set to a positive value equal to or smaller than 0.04 ps/nm2/km in a wavelength band of 1.55 µm;
and a zero dispersion wavelength equal to or smaller than 1.4 µm.
2. An optical fiber according to claim 1, wherein a cutoff wavelength is set to be equal to or smaller than 1.5 µm at a length of 2 m, and a bending loss is set to be equal to or smaller than 5 dB/m at a diameter of 20 mm in the wavelength band of 1.5 µm.
3. An optical fiber according to claim 1, wherein the optical fiber comprises:
multiple glass layers adjacent to each other and having different compositions; and at least three glass layers formed inside a reference layer as a reference of a refractive index distribution among these multiple glass layers;
wherein a maximum refractive index of a first glass layer formed on an innermost side of the optical fiber is set to be higher than the refractive index of said reference layer, a minimum refractive index of a second glass layer as a second layer from an inner side of said optical fiber is set to be lower than the refractive index of said reference layer, and a maximum refractive index of a third glass layer as a third layer from the inner side of said optical fiber is set to be higher than the refractive index of said reference layer.
multiple glass layers adjacent to each other and having different compositions; and at least three glass layers formed inside a reference layer as a reference of a refractive index distribution among these multiple glass layers;
wherein a maximum refractive index of a first glass layer formed on an innermost side of the optical fiber is set to be higher than the refractive index of said reference layer, a minimum refractive index of a second glass layer as a second layer from an inner side of said optical fiber is set to be lower than the refractive index of said reference layer, and a maximum refractive index of a third glass layer as a third layer from the inner side of said optical fiber is set to be higher than the refractive index of said reference layer.
4. An optical fiber according to claim 3, wherein a glass layer having a refractive index higher than that of the reference layer is arranged between the third glass layer and the reference layer.
5. An optical fiber according to claim 3, wherein a glass layer having a refractive index lower than that of the reference layer is arranged between the third glass layer and the reference layer.
6. An optical fiber according to claim 3, wherein a relative refractive index difference .DELTA.1 of the maximum refractive index of the first glass layer with respect to the reference layer is set to 0.5 % or more and 0.6 % or less, a relative refractive index difference .DELTA.2 of the minimum refractive index of the second glass layer with respect to said reference layer is set to -0.4 % or more and -0.1 % or less, and a relative refractive index difference .DELTA.3 of the maximum refractive index of the third glass layer with respect to said reference layer is set to 0.1 % or more and 0.4 % or less.
7. An optical communication system characterized in that an optical fiber according to claim 1 is applied as an optical transmitting path.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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JP2000-361390 | 2000-11-28 | ||
JP2000361390A JP2002162529A (en) | 2000-11-28 | 2000-11-28 | Optical fiber, and optical communication system using the optical fiber |
Publications (1)
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CA2356712A1 true CA2356712A1 (en) | 2002-05-28 |
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ID=18832832
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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CA002356712A Abandoned CA2356712A1 (en) | 2000-11-28 | 2001-09-05 | Optical fiber and optical communication system using this optical fiber |
Country Status (9)
Country | Link |
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US (2) | US6640036B2 (en) |
EP (1) | EP1211533A3 (en) |
JP (1) | JP2002162529A (en) |
KR (1) | KR20020041746A (en) |
CN (1) | CN1178078C (en) |
BR (1) | BR0105528A (en) |
CA (1) | CA2356712A1 (en) |
HK (1) | HK1044380A1 (en) |
RU (1) | RU2001132143A (en) |
Families Citing this family (21)
Publication number | Priority date | Publication date | Assignee | Title |
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JP2002261366A (en) * | 2000-12-26 | 2002-09-13 | Sumitomo Electric Ind Ltd | Amplifying optical fiber, and optical fiber amplifier including the same |
FR2828939B1 (en) * | 2001-08-27 | 2004-01-16 | Cit Alcatel | OPTICAL FIBER FOR A WAVELENGTH MULTIPLEXED TRANSMISSION SYSTEM |
JP3886771B2 (en) | 2001-10-29 | 2007-02-28 | 株式会社フジクラ | Single mode optical fiber and composite optical line for WDM |
JP2003287642A (en) | 2002-01-22 | 2003-10-10 | Fujikura Ltd | Optical fiber and optical transmission line |
JP2003227959A (en) * | 2002-02-04 | 2003-08-15 | Furukawa Electric Co Ltd:The | Single mode optical fiber for wavelength multiplex transmission |
US6856744B2 (en) * | 2002-02-13 | 2005-02-15 | The Furukawa Electric Co., Ltd. | Optical fiber and optical transmission line and optical communication system including such optical fiber |
AU2003210934A1 (en) | 2002-02-15 | 2003-09-09 | Corning Incorporated | Low slope dispersion shifted optical fiber |
FR2842610B1 (en) * | 2002-07-18 | 2004-11-12 | Cit Alcatel | OPTICAL FIBER WITH DISPERSION MANAGEMENT |
JP2005534963A (en) * | 2002-07-31 | 2005-11-17 | コーニング・インコーポレーテッド | Non-zero dispersion shifted optical fiber with large effective area, low tilt and low zero dispersion |
US6707976B1 (en) * | 2002-09-04 | 2004-03-16 | Fitel Usa Corporation | Inverse dispersion compensating fiber |
CN1692429B (en) * | 2002-11-22 | 2012-05-09 | Lg电子有限公司 | recording and reproducing methods and apparatuses for managing reproduction of multiple reproduction path video data |
US7085463B2 (en) | 2002-12-18 | 2006-08-01 | The Furukawa Electric Co., Ltd. | Optical fiber and optical transmission line |
FR2849213B1 (en) * | 2002-12-24 | 2005-03-04 | Cit Alcatel | OPTICAL FIBER |
US7103251B2 (en) * | 2002-12-31 | 2006-09-05 | Corning Incorporated | Dispersion flattened NZDSF fiber |
US6904217B2 (en) * | 2003-01-29 | 2005-06-07 | Furukawa Electric North America | Method for the manufacture of optical fibers, improved optical fibers, and improved Raman fiber amplifier communication systems |
JP2005055795A (en) * | 2003-08-07 | 2005-03-03 | Furukawa Electric Co Ltd:The | Polarization holding optical fiber and optical wavelength converter using the same |
US6985662B2 (en) * | 2003-10-30 | 2006-01-10 | Corning Incorporated | Dispersion compensating fiber for moderate dispersion NZDSF and transmission system utilizing same |
US7024083B2 (en) * | 2004-02-20 | 2006-04-04 | Corning Incorporated | Non-zero dispersion shifted optical fiber |
KR101627830B1 (en) * | 2009-02-16 | 2016-06-08 | 엘에스전선 주식회사 | A non-zero dispersion shifted optical fiber and optical transmission line using the same, and optical transmission system |
CN106383379A (en) * | 2016-11-26 | 2017-02-08 | 长飞光纤光缆股份有限公司 | High-bandwidth bending insensitive multi-mode fiber |
US11435538B2 (en) | 2018-11-12 | 2022-09-06 | Panasonic Intellectual Property Management Co., Ltd. | Optical fiber structures and methods for beam shaping |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
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US5878182A (en) | 1997-06-05 | 1999-03-02 | Lucent Technologies Inc. | Optical fiber having a low-dispersion slope in the erbium amplifier region |
JPH1184159A (en) * | 1997-09-10 | 1999-03-26 | Furukawa Electric Co Ltd:The | Dispersion flat fiber |
EP1037074A4 (en) * | 1997-12-05 | 2001-01-17 | Sumitomo Electric Industries | Dispersion-shifted optical fiber |
CA2277332C (en) * | 1997-12-05 | 2003-03-25 | Sumitomo Electric Industries, Ltd. | Dispersion-flattened optical fiber |
US5905838A (en) * | 1998-02-18 | 1999-05-18 | Lucent Technologies Inc. | Dual window WDM optical fiber communication |
JP4134468B2 (en) | 1999-12-13 | 2008-08-20 | 住友電気工業株式会社 | Optical fiber |
US6477306B2 (en) * | 2000-04-11 | 2002-11-05 | Sumitomo Electric Industries, Ltd. | Dispersion-compensating optical fiber, and, optical transmission line and dispersion-compensating module respectively including the same |
-
2000
- 2000-11-28 JP JP2000361390A patent/JP2002162529A/en active Pending
-
2001
- 2001-09-05 CA CA002356712A patent/CA2356712A1/en not_active Abandoned
- 2001-09-07 EP EP01307637A patent/EP1211533A3/en not_active Withdrawn
- 2001-09-13 US US09/950,646 patent/US6640036B2/en not_active Expired - Lifetime
- 2001-10-29 KR KR1020010066614A patent/KR20020041746A/en not_active Application Discontinuation
- 2001-11-27 RU RU2001132143/28A patent/RU2001132143A/en not_active Application Discontinuation
- 2001-11-27 CN CNB011401397A patent/CN1178078C/en not_active Expired - Fee Related
- 2001-11-28 BR BR0105528-3A patent/BR0105528A/en not_active IP Right Cessation
-
2002
- 2002-08-16 HK HK02105999.8A patent/HK1044380A1/en unknown
-
2003
- 2003-08-19 US US10/642,630 patent/US6795629B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
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EP1211533A3 (en) | 2004-01-28 |
US20040033041A1 (en) | 2004-02-19 |
CN1178078C (en) | 2004-12-01 |
RU2001132143A (en) | 2003-08-27 |
HK1044380A1 (en) | 2002-10-18 |
US6795629B2 (en) | 2004-09-21 |
BR0105528A (en) | 2002-07-02 |
US20020097971A1 (en) | 2002-07-25 |
KR20020041746A (en) | 2002-06-03 |
EP1211533A2 (en) | 2002-06-05 |
US6640036B2 (en) | 2003-10-28 |
CN1356568A (en) | 2002-07-03 |
JP2002162529A (en) | 2002-06-07 |
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