CN201314957Y - Improved non-zero dispersion shifted single-mode fiber with large mode field distribution - Google Patents

Improved non-zero dispersion shifted single-mode fiber with large mode field distribution Download PDF

Info

Publication number
CN201314957Y
CN201314957Y CNU2008201664635U CN200820166463U CN201314957Y CN 201314957 Y CN201314957 Y CN 201314957Y CN U2008201664635 U CNU2008201664635 U CN U2008201664635U CN 200820166463 U CN200820166463 U CN 200820166463U CN 201314957 Y CN201314957 Y CN 201314957Y
Authority
CN
China
Prior art keywords
sandwich layer
layer
refractive index
dispersion
cladding layer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CNU2008201664635U
Other languages
Chinese (zh)
Inventor
吴金东
卢卫民
吴海港
张立永
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Futong Group Co Ltd
Original Assignee
Futong Group Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Futong Group Co Ltd filed Critical Futong Group Co Ltd
Priority to CNU2008201664635U priority Critical patent/CN201314957Y/en
Application granted granted Critical
Publication of CN201314957Y publication Critical patent/CN201314957Y/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Abstract

The utility model relates to an improved non-zero dispersion shifted single-mode fiber with large mode field distribution, which comprises a fiber core layer and a cladding layer. The cladding layer is wrapped on the fiber core layer; the fiber core layer comprises inner core layers with different refractive indexes and outer core layers which are wrapped on the inner core layers; the outer core layers are distributed based on the gradual changes of the refractive indexes; the cladding layer comprises an inner cladding layer, a ring core cladding layer and an outer cladding layer which are provided with different refractive indexes and are arranged from the inner to the outer; the outer cladding layer is a pure silica glass layer; the refractive indexes of the fiber core layers are arranged in the sequence that n1 is more than n2 and n2 is more than n<c>; and the refractive indexes of the cladding layer are arranged in the sequence that n4 is more than n3 and n3 is more than n<c>, or in the sequence that n4 is more than n<c> and n<c> is more than n3. The utility model has the characteristics of the low nonlinear color effect, namely, large effective area, optimized dispersion and lower dispersion slope. The utility model can effectively solve the nonlinear problem and the polarization mode dispersion problem affecting the high-speed communication, reduce the cost for the management of the system dispersion, and lead to the low splicing loss. Therefore, the utility model is applicable to the large-capacity, high-speed and long-distance transmission system.

Description

A kind of improved non-zero dispersion displacement single mode optical fibre with big mould field distribution
Technical field
The utility model relates to a kind of non-zero dispersion displacement single mode optical fibre that designs for high capacity, two-forty, long haul transmission system.This optical fiber has improved low nonlinear effects characteristic, it is big mould field distribution (useful area), optimize chromatic dispersion and lower chromatic dispersion gradient, have simultaneously that polarization mode dispersion is low, low-loss and excellent bending resistance, have advantages such as low welding loss during with fused fiber splice, be applicable to the dense wave division multipurpose dwdm system transmission of high capacity, two-forty, long distance, big useful area helps reducing nonlinear effect, low chromatic dispersion gradient helps chromatic dispersion is comprehensively managed, and satisfies the transmission of the long distance of C+L and S+C+L wave band.
Background technology
Development along with Fibre Optical Communication Technology, particularly the maturation of fiber amplifier and wavelength-division multiplex technique is used, what restrict optical fiber communication no longer is the loss of optical fiber, the fast development of global IT application needs high capacity, the two-forty optical fiber telecommunications system, from technology and consideration economically, the Fibre Optical Communication Technology development mainly contains 2 directions, one for improving the single-channel transfer rate of wavelength-division multiplex, two channel quantity and increase service bands for the increase wavelength-division multiplex, so high capacity, two-forty, long haul transmission system proposes new demand to the characteristic and the development of optical fiber, for wavelength-division multiplex technique, the principal element of restriction Optical Fiber Transmission capacity and distance is a nonlinear effect at present, chromatic dispersion and Optical Signal To Noise Ratio (English of Optical Signal To Noise Ratio abbreviates OSNR as).
In dwdm system, along with the increase of capacity, constantly reduce thereupon the wavelength interval, and the optical nonlinear effect between each wavelength (comprise four-wave mixing, from phase modulation (PM), cross-phase modulation etc.) has limited the capacity and the distance of light transmission.Therefore the Optical Signal To Noise Ratio of system requirements requires higher signal light power along with single-channel speed improves and the increase that is directly proportional, and this makes fiber nonlinear effect more become serious.And because the expansion of wavelength division multiplexed channel wave band, chromatic dispersion gradient causes the chromatic dispersion accumulation of long and short wavelength edges channel uneven, if this chromatic dispersion accumulation imbalance can not get good compensation, the regenerative repeating distance of the remarkable shortening of meeting system, this makes dispersion management complicated more, has increased system dispersion compensation cost.As for the 40Gbit/s system, the bandwidth of each channel reaches the nearly 0.8nm of 80GHz, chromatic dispersion gradient becomes remarkable to the influence of each frequency component in each channel, requirement is near 100% dispersion slope compensation efficient, this just requires the relative dispersion slope (the English RDS of abbreviation of the relative dispersion slope of optical fiber) of optical fiber as far as possible little, and its effective method is to reduce chromatic dispersion gradient and suitably increase chromatic dispersion.The effective way that the addresses these problems optical fiber technology of constantly bringing forth new ideas exactly, the new optical fiber that exploitation has low nonlinear effects and chromatic dispersion optimized light-guide.
In order to suppress effect of nonlinear in the dwdm system, need suitable dispersion values and reduce optical power density at the transmission wave band, people have developed non-zero dispersion displacement optical fiber and large effective area non-zero dispersion displacement optical fiber on the basis of dispersion shifted optical fiber.The design and production patent (application) scheme of a series of this type optical fiber have been announced at present.Be applicable to the optical fiber of C+L wave band, as a kind of large effective area non-zero dispersion displacement optical fiber and manufacture method that No. 98121639.0 Chinese utility application (publication number is CN1220402A) are announced, its typical chromatic dispersion gradient is 0.09ps/ (nm 2Km), useful area is at 80um 2More than, 1550nm loss representative value is 0.205dB/km; As the patent No. be 03125210.9, Granted publication number is to design 8 fibre core layerings by the disclosed a kind of positive non-zero dispersion displacement optical fiber of Chinese utility model patent of CN1219227C, the 1550nm chromatic dispersion gradient is reduced to 0.085ps/ (nm 2Km), useful area is adjusted into 70um 2More than; The optical fiber of the central concave core structure of announcing as No. 00806764.3 Chinese utility application (publication number is CN1348548A), the about 70um of optical fiber effective area 2, chromatic dispersion gradient is 0.09-0.08ps/ (nm 2Km); Or the like.A kind of parabolic distribution core structure optical fiber of US2002/0154876A1 U.S. Patent Application Publication, useful area is greater than 90um 2But the chromatic dispersion of 1550nm is excessive, is 14-20ps/ (nmkm); U.S. US6459839B1 patent is announced has large effective area fiber trapezoidal and the fibre core depression, and useful area reaches 100um 2More than, chromatic dispersion gradient is 0.08; A kind of optical fiber that U.S. US6396987B1 patent is announced, fiber core layer refractive index adopt distribution trapezoidal and the sagging step change type in center, and its chromatic dispersion gradient is less than 0.07ps/ (nm 2Km), but useful area only reach to 60um 2A kind of step change type index distribution optical fiber that No. 00802639.4 patented claim of China (publication number is CN1337010A) is announced, the about 0.09ps/ (nm of chromatic dispersion gradient 2Km), the chromatic dispersion of 1550nm is at 7-15ps/ (nmkm), and useful area reaches 60-150um 2The optical fiber of the sagging annular core structure of the SMIS that No. 03119080.4 patented claim of China (publication number is CN1450369A) is announced, optical fiber effective area is greater than 95um 2, chromatic dispersion gradient is less than 0.065ps/ (nm 2Km); All can be used for the S+C+L wave band, but the welding added losses height of optical fiber.
Though G..655 optical fiber kind is numerous now, in the most large effective area G..655 optical fiber, chromatic dispersion gradient still is bigger than normal, and perhaps structure is too complicated, is unfavorable for system dispersion management and optical fiber production technology controlling and process.In the former technological operation, the chromatic dispersion gradient of large effective area fiber that is used for long haul transmission system is big, therefore causes the dwdm system performance degradation, and repeater span is limited.Transmission system for wide operation wavelength, chromatic dispersion gradient direct harm bigger than normal is exactly to cause the chromatic dispersion difference of long and short wavelength side bandgap wavelength big, the transmission wavelength scope is wide more, this chromatic dispersion difference is big more, and dispersion compensation difficulty and cost are big more, especially requires the High Speed System of accurate dispersion management like this for 40Gbit/s, its influence just becomes very big problem, need more complicated dispersion management in actual applications, increased system cost, the interests that do not meet Virtual network operator are selected.Therefore, in order to make full use of the bandwidth of an optical fiber resource, to increase message capacity, these application requirements are optimized chromatic dispersion, reduce chromatic dispersion gradient, are improved the flatness of service band chromatic dispersion when keeping the large effective area characteristic.
Desirable CHROMATIC DISPERSION IN FIBER OPTICS should have a constant at whole service band, but refractive index changes along with wavelength variations, and chromatic dispersion has dependence to wavelength.On the fibre-optic waveguide structural design, useful area and chromatic dispersion gradient mutual restriction need be considered the various characteristics balance when optical fiber designs.
In actual fiber optic transmission system long haul, usually different fiber need be connected to form communication link, non-zero dispersion displacement optical fiber is more complicated than standard single-mode fiber index distribution, together the time,, often cause reflection to increase non-zero dispersion displacement optical fiber and other dissimilar fused fiber splice because long diameter of mould each other and optical fiber geometric parameter etc. do not match, added losses increase, the long more contact of link is many more, and the effect of accumulation is big more, and serious may cause the unacceptable bit error rate.Therefore the welding characteristic is the problem that can not be ignored in the optical fiber manufacturing, need take measures to reduce the splice loss, splice attenuation of optical fiber, and the restriction splice loss, splice attenuation is to the illeffects of transmission system.
The utility model content
The purpose of this utility model provides a kind of low nonlinearity chromatic effect characteristic that has, it is large effective area, chromatic dispersion of optimizing and lower chromatic dispersion gradient, thereby can effectively solve the nonlinear problem and the polarization mode dispersion problem that influence high-speed communication, the dispersion management cost of minimizing system, and the improved non-zero dispersion displacement single mode optical fibre with big mould field distribution with low splice loss, splice attenuation is to be applicable to high capacity, two-forty, long haul transmission system.For this reason, the utility model is by the following technical solutions:
A kind of improved non-zero dispersion displacement single mode optical fibre with big mould field distribution, it comprises fiber core layer and the covering that is enclosed on the fiber core layer, it is characterized in that described fiber core layer comprises inner sandwich layer with different refractivity and the outer sandwich layer that surrounds described inner sandwich layer, the refractive index of described outer sandwich layer is a graded profile, covering comprises the inner cladding from inside to outside with different refractivity, ring core covering and surrounding layer, surrounding layer is the pure silicon dioxide glassy layer, the index distribution of described fiber core layer is n1〉n2〉nc, described cladding index is distributed as n4〉n3〉nc or n4〉nc〉n3, wherein: n1 is the refractive index of inner sandwich layer, n2 is the largest refractive index of outer sandwich layer, n3 is the refractive index of inner cladding, n4 is the refractive index of ring core covering, and nc is the refractive index of surrounding layer, the refractive index of outer sandwich layer by the n2 gradual change to n3.
As to further the improving and replenishing of technique scheme, the utility model also comprises following additional technical feature, so that technical characterictics that these are additional combine individually or arbitrarily and are applied in the technique scheme when stating technical scheme on the implementation:
The waveguiding structure parameter of described inner sandwich layer, outer sandwich layer, inner cladding, ring core covering is:
0.53%≤Δn1≤0.65%,3.0um≤R1≤4.0um,
0.15%≤Δn2≤0.40%,6.4um≤R2≤8.4um,
-0.1%≤Δn3≤0.03%,11.6um≤R3≤14.6um,
0.15%≤Δn4≤0.25%,17.6um≤R4≤19.8um,
Wherein Δ n1, Δ n2, Δ n3, Δ n4 are respectively inner sandwich layer, outer sandwich layer, inner cladding, ring core covering with the refractive index contrast of nc as the reference refractive index, and R1, R2, R3, R4 are respectively the diameter of inner sandwich layer, outer sandwich layer, inner cladding, ring core covering.Surrounding layer is pure silica glass layer, and its refractive index is the refractive index n c of pure silicon dioxide glass, its refractive index contrast Δ nc=0.From R1 to R2, the refractive index of outer sandwich layer by Δ n2 gradual change to Δ n3.
Described outer sandwich layer gradually changed refractive index distributes and satisfies formula:
N (r)=nc*[1-2 Δ (r/r2) α] 1/2, r1≤r≤r2 wherein, r is the radius variable of outer sandwich layer, and r1 is the radius of inner sandwich layer, and r2 is the radius of outer sandwich layer, and α is a gradual change rule coefficient.
Outside described, mix at least a of germanium, fluorine, three kinds of elements of phosphorus in sandwich layer, inner cladding, the ring core covering respectively.In order to the index distribution of adjusting optical fiber product, and make viscosity and stress coupling, reduce unrelieved stress in the optical fiber, equilibrium stress distributes, stable fiber polarization mode dispersion performance.
By accurate adjustment to Refractive Index Profile o, the gradual change factor alpha of the refractive index of especially outer sandwich layer, can obtain the mould field distribution (useful area) and the dispersion characteristics of needs, be dispersion values, chromatic dispersion gradient, and have lower polarization mode dispersion, loss, excellent bending property and welding performance, therefore optical fiber of the present utility model has following feature especially
1550nm chromatic dispersion gradient≤0.073ps/ (nm 2Km);
Zero-dispersion wavelength≤1500nm;
Useful area is 70~75um 2
Chromatic dispersion in 1530nm~1565nm scope is 2.5~6.5ps/ (nmkm);
Chromatic dispersion in 1565nm~1625nm scope is 6~12ps/ (nmkm);
Loss≤0.22dB/km of 1550 is at the loss≤0.22dB/km of 1530nm~1565nm wave band.
According to the fibre-optical bending performance measurement method, φ 60mm mandrel around 100 the circle tests in, the added losses that bending causes at 1550nm and 1625nm place all less than 0.05dB, at φ 32mm mandrel in the test of 1 circle, the added losses that bending causes at 1550nm and 1625nm place all less than 0.5dB.The polarization mode look of optical fiber
Figure Y200820166463D0008135534QIETU
Fiber core layer of the present utility model can adopt but be not limited to technologies such as MCVD, PCVD or OVD and be made, to realize the fibre-optic waveguide structural design of regulation.
The beneficial effects of the utility model are:
1, compares with non-zero dispersion displacement single mode waveguiding structure in the past, structure of the present utility model is simple relatively, not only can obtain easily, and waveguiding structure has corresponding dispersion characteristics in the numerical value interval of regulation, accurate control ability in conjunction with the distribution of technology refractive index such as MCVD, PCVD, OVD, produce easily and quality control, can obtain designed optical fiber property expeditiously.
2, optical fiber of the present utility model has big mould field distribution, and chromatic dispersion gradient is lower, and the characteristic of optical fiber is enough to satisfy the requirement that suppresses nonlinear effect, reduces the system dispersion management costs, is applicable to the DWDM transmission needs of C+L wave band or S+C+L wave band.
3, the utility model is taken into account the composition design of fiber optic materials in waveguide design, and viscosity and stress are optimized coupling, improves stress distribution, and the PMD performance of optical fiber is improved.In the utility model,, reach the optimization internal stress distribution, make the fiber PMD stable performance by to suitably the choosing of prefabricated rod cladding doping composition.
4, optical fiber of the present utility model and other non-zero dispersion displacement optical fiber NZ-DSF welding have low splice loss, splice attenuation, and the welding performance is fabulous.
Description of drawings
Fig. 1 be among the utility model embodiment 1 the relative index of refraction Δ to the distribution curve synoptic diagram of diameter.
Fig. 2 be among the utility model embodiment 2 the relative index of refraction Δ to the distribution curve synoptic diagram of diameter.
Fig. 3 be among the utility model embodiment 3 the relative index of refraction Δ to the distribution curve synoptic diagram of diameter.
Fig. 4 is the optical fiber and existing dispersion curve synoptic diagram with the type optical fiber commodity of the utility model embodiment.
Embodiment
The improved non-zero dispersion displacement single mode optical fibre of the utility model with big mould field distribution, comprise fiber core layer and the covering that is enclosed on the fiber core layer, fiber core layer comprises inner sandwich layer with different refractivity and the outer sandwich layer that surrounds inner sandwich layer, the refractive index of described outer sandwich layer is a graded profile, covering comprises inner cladding from inside to outside, ring core covering and the surrounding layer with different refractivity, and surrounding layer is the pure silicon dioxide glassy layer.Below by several specific embodiments it is elaborated.
Embodiment 1:
Be a kind of fibre-optic waveguide refractive index distribution curve of the present utility model as shown in Figure 1, following is one group of refractive index contrast distribution parameter:
The parameter of inner sandwich layer Core1 is: Δ n1 is about 0.60%, and R1 is about 3.6um,
The parameter of outer sandwich layer Core2 is: Δ n2 is about 0.25%, and R2 is about 7.6um,
The parameter of inner cladding Clad1 is: Δ n3 is about 0.02%, and R3 is about 12.8um,
The parameter of ring core covering Clad2 is: Δ n4 is about 0.21%, and R4 is about 17.2um,
The parameter of surrounding layer (being outermost layer) Clad3 is: Δ nc is about 0.00%, and R5 is 125um,
Surrounding layer Clad3 is the pure silicon dioxide glassy layer, and its refractive index is nc (Δ nc=0),
Outer sandwich layer Core2 gradually changed refractive index distributes and satisfies formula: n (r)=nc*[1-2 Δ (r/r2) α] 1/2, r1≤r≤r2 wherein, r is the radius variable of outer sandwich layer, and r1 is the radius of inner sandwich layer, and r2 is the radius of outer sandwich layer, and gradual change rule factor alpha gets 1; The refractive index of outer sandwich layer Core2 is gradient to Δ n3 by Δ n2 from R1 to R2.
The characteristic of gained optical fiber is as follows:
1550nm useful area: 74um 2,
Zero-dispersion wavelength: 1487nm,
At 1550nm chromatic dispersion: 4.45ps/ (nmkm),
At the 1550nm chromatic dispersion gradient: 0.0714ps/ (nm 2Km),
At 1530nm chromatic dispersion: 3.03ps/ (nmkm),
At 1625nm chromatic dispersion: 9.866ps/ (nmkm),
Cable cut-off wavelength: 1330nm,
At 1550 losses: 0.20dB/km,
Macrobend φ 60mm is around 100 circles, at the maximal value of the added losses of 1550nm and 1625nm: 0.04dB.
Macrobend φ 32mm is around 1 circle, at the maximal value of the added losses of 1550nm and 1625nm: 0.05dB.
The described optic fibre characteristic of this embodiment at the chromatic dispersion gradient of 1550nm less than 0.073ps/ (nm 2Km), useful area is 74um 2, and decay and bending property excellence, the splice loss, splice attenuation of different batches optical fiber self is less than 0.03dB, with the splice loss, splice attenuation of other NZ-DSF optical fiber less than 0.06dB.Optic fibre characteristic can be applicable to the dwdm system transmission needs of C+L wave band.
Embodiment 2:
According to fibre-optic waveguide refractive index distribution curve shown in Figure 2, following is one group of refractive index contrast distribution parameter:
The parameter of inner sandwich layer Core1 is: Δ n1 is about 0.58%, and R1 is about 3.8um,
The parameter of outer sandwich layer Core2 is: Δ n2 is about 0.24%, and R2 is about 7.8um,
The parameter of inner cladding Clad1 is: Δ n3 is about-0.05%, and R3 is about 13.0um,
The parameter of ring core covering Clad2 is: Δ n4 is about 0.23%, and R4 is about 18.2um,
The parameter of surrounding layer Clad3 is: Δ nc is about 0.00%, and R5 is about 125um,
Surrounding layer Clad3 is the pure silicon dioxide glassy layer, and its refractive index is nc,
Outer sandwich layer Core2 gradually changed refractive index distributes and satisfies formula: n (r)=nc*[1-2 Δ (r/r2) α] 1/2, r1≤r≤r2 wherein, r is the radius variable of outer sandwich layer, and r1 is the radius of inner sandwich layer, and r2 is the radius of outer sandwich layer, and gradual change rule factor alpha gets 1; The refractive index of outer sandwich layer Core2 is gradient to Δ n3 by Δ n2 from R1 to R2.
The characteristic of gained optical fiber is as follows:
1550nm useful area: 72um 2,
Zero-dispersion wavelength: 1470nm,
At 1550nm chromatic dispersion: 5.29ps/ (nmkm),
At the 1550nm chromatic dispersion gradient: 0.068ps/ (nm 2Km),
At 1530nm chromatic dispersion: 3.94ps/ (nmkm),
At 1565nm chromatic dispersion: 6.29ps/ (nmkm),
At 1625nm chromatic dispersion: 10.48ps/ (nmkm),
Cable cut-off wavelength: 1330nm,
At 1550 losses: 0.20dB/km,
Macrobend φ 60mm is around 100 circles, at the maximal value of the added losses of 1550nm and 1625nm: 0.035dB.
Macrobend φ 32mm is around 1 circle, at the maximal value of the added losses of 1550nm and 1625nm: 0.045dB.
The described optic fibre characteristic of this embodiment at the chromatic dispersion gradient of 1550nm less than 0.07ps/ (nm 2Km), useful area 72um 2, and decay and bending property excellence, the splice loss, splice attenuation of different batches optical fiber self is less than 0.03dB, with the splice loss, splice attenuation of other NZ-DSF optical fiber less than 0.06dB.Optic fibre characteristic can be applicable to the dwdm system transmission needs of C+L wave band.
Embodiment 3:
According to fibre-optic waveguide refractive index distribution curve shown in Figure 3, following is one group of refractive index contrast distribution parameter:
The parameter of inner sandwich layer Core1 is: Δ n1 is about 0.56%, and R1 is about 4.0um,
The parameter of outer sandwich layer Core2 is: Δ n2 is about 0.22%, and R2 is about 8.0um,
The parameter of inner cladding Clad1 is: Δ n3 is about-0.07%, and R3 is about 13.6um,
The parameter of the first ring core covering Clad2 is: Δ n4 is about 0.22%, and R4 is about 19.2um,
The parameter of the second ring core covering Clad3 is: Δ n5 is about 0.-08%, and R5 is about 20.8um,
Outermost layer is that the parameter of surrounding layer Clad4 is: Δ nc is about 0.00%, and R6 is 125um,
Covering layering Clad4 is the pure silicon dioxide glassy layer, and its refractive index is nc (Δ nc=0),
Described outer sandwich layer gradually changed refractive index distributes and satisfies formula: n (r)=nc*[1-2 Δ (r/r2) α] 1/2, r1≤r≤r2 wherein, r is the radius variable of outer sandwich layer, and r1 is the radius of inner sandwich layer, and r2 is the radius of outer sandwich layer, and gradual change rule factor alpha gets 1; The refractive index of outer sandwich layer Core2 is gradient to Δ n3 by Δ n2 from R1 to R2.
The characteristic of gained optical fiber is as follows:
1550nm useful area: 73um 2,
Zero-dispersion wavelength: 1450nm,
At 1550nm chromatic dispersion: 6.6ps/ (nmkm),
At the 1550nm chromatic dispersion gradient: 0.068ps/ (nm 2Km),
At 1530nm chromatic dispersion: 5.3ps/ (nmkm),
At 1625nm chromatic dispersion: 11.5ps/ (nmkm),
Cable cut-off wavelength: 1320nm,
At 1550 losses: 0.20dB/km,
Macrobend φ 60mm is around 100 circles, at the maximal value of the added losses of 1550nm and 1625nm: 0.04dB.
Macrobend φ 32mm is around 1 circle, at the maximal value of the added losses of 1550nm and 1625nm: 0.045dB.
These embodiment 3 described optic fibre characteristics at the chromatic dispersion gradient of 1550nm less than 0.07ps/ (nm 2Km), useful area 73um 2, and decay and bending property excellence, the splice loss, splice attenuation of different batches optical fiber self is less than 0.03dB, with the splice loss, splice attenuation of other NZ-DSF optical fiber less than 0.06dB.Optic fibre characteristic can be applicable to the dwdm system transmission needs of S+C+L wave band.
The definition of some terms in the utility model:
Refractive indices is defined by following equation:
Refractive index contrast Δ ni%=[(ni 2-nc 2)/2ni 2] (1)
Wherein ni is the optical fibre refractivity of i layer, and nc is the refractive index of surrounding layer pure silicon dioxide glass part, and it is as the reference refractive index in this application.
The definition of index distribution is meant the relation of on the selected part of optical fiber refractive index n i or the relative fiber optic hub with it of Δ ni position ri (radius).
Gradually changed refractive index distributes, and satisfies formula: n (r)=nc*[1-2 Δ (r/a) α] 1/2, 0≤r≤a
Wherein: r is the radius variable; α is a gradual change rule coefficient, the shape of its decision change curve, can value (0, ∞); A is a constant, can be defined as different constants when the various refractive index of design.
Total dispersion is defined as the algebraic sum of fiber optic materials chromatic dispersion and waveguide dispersion, and in technical field of optical fiber communication, CHROMATIC DISPERSION IN FIBER OPTICS just is meant total dispersion, and its unit is ps/ (nmkm).
Chromatic dispersion gradient is represented the correlativity of chromatic dispersion to wavelength, owing to refractive index along with wavelength variations changes, fibre-optical dispersion numerical value also changes along with wavelength variations, chromatic dispersion gradient is represented this variability, it is to be abscissa with the wavelength, dispersion values is described slope of a curve by ordinate, and its unit is ps/ (nm 2Km).
Ds=dD/dλ
In wavelength-division multiplex system, if the chromatic dispersion gradient of transmission link is big, then the difference of the dispersion values between each wavelength becomes big, will reduce the transport property of system or the cost of increase dispersion compensation.
Useful area Aeff=2 π (∫ E 2Rdr) 2/ (∫ E 4Rdr) (2)
Integration is limited to 0 to ∞ in the formula, and E is and propagates relevant electric field.
DWDM is the abbreviation of dense wavelength division multiplexing system.
PMD is the abbreviation of optic fiber polarization mould dispersion.
The bending resistance of optical fiber is meant the added losses under the regulation test condition.Test process is, the loss of measuring fiber under normal operation, again according to standard-required with optical fiber on mandrel, measure loss value, the difference of two kinds of measurements is the addition bend loss that bending causes.Its specified standard test condition is included on the mandrel of diameter 75mm on 100 circles and the mandrel at 32mm around 1 circle etc.Usually, the maximum permissive waste that bending causes is as the criterion with the annex bending loss of 1310nm and 1550nm, and unit is dB.Adopt mandrel 60mm and 32mm respectively around 100 circles and the conditioned measurement 1550nm of 1 circle and the added losses of 1625nm wavelength among the application, and get maximal value as measurement result.
Splice loss, splice attenuation is to average at 1550nm place bidirectional measurement with OTDR.

Claims (4)

1, a kind of improved non-zero dispersion displacement single mode optical fibre with big mould field distribution, it comprises fiber core layer and the covering that is enclosed on the fiber core layer, it is characterized in that described fiber core layer comprises inner sandwich layer with different refractivity and the outer sandwich layer that surrounds described inner sandwich layer, the refractive index of described outer sandwich layer is a graded profile, covering comprises the inner cladding from inside to outside with different refractivity, ring core covering and surrounding layer, surrounding layer is the pure silicon dioxide glassy layer, the index distribution of described fiber core layer is n1〉n2〉nc, described cladding index is distributed as n4〉n3〉nc or n4〉nc〉n3, wherein: n1 is the refractive index of inner sandwich layer, n2 is the largest refractive index of outer sandwich layer, n3 is the refractive index of inner cladding, n4 is the refractive index of ring core covering, and nc is the refractive index of surrounding layer.
2, a kind of improved non-zero dispersion displacement single mode optical fibre with big mould field distribution according to claim 1 is characterized in that the waveguiding structure parameter of described inner sandwich layer, outer sandwich layer, inner cladding, ring core covering is:
53%≤Δn1≤0.65%,3.0um≤R1≤4.0um,
15%≤Δn2≤0.40%,6.4um≤R2≤8.4um,
-0.1%≤Δn3≤0.03%,11.6um≤R3≤14.6um,
15%≤Δn4≤0.25%,17.6um≤R4≤19.8um,
Wherein Δ n1, Δ n2, Δ n3, Δ n4 are respectively inner sandwich layer, outer sandwich layer, inner cladding, ring core covering with the refractive index contrast of nc as the reference refractive index, R1, R2, R3, R4 are respectively the diameter of inner sandwich layer, outer sandwich layer, inner cladding, ring core covering, from R1 to R2, the refractive index of outer sandwich layer by Δ n2 gradual change to Δ n3.
3, a kind of improved non-zero dispersion displacement single mode optical fibre according to claim 1 with big mould field distribution, it is characterized in that described outer sandwich layer gradually changed refractive index distributes satisfies formula:
N (r)=nc*[1-2 Δ (r/r2) α] 1/2, r1≤r≤r2 wherein, r is the radius variable of outer sandwich layer, and r1 is the radius of inner sandwich layer, and r2 is the radius of outer sandwich layer, and α is a gradual change rule coefficient.
4, a kind of improved non-zero dispersion displacement single mode optical fibre with big mould field distribution according to claim 1 is characterized in that:
1550nm chromatic dispersion gradient≤0.073ps/ (nm 2Km);
Zero-dispersion wavelength≤1500nm;
Useful area is 70~75um 2
Chromatic dispersion in 1530nm~1565nm scope is 2.5~6.5ps/ (nmkm);
Chromatic dispersion in 1565nm~1625nm scope is 6~12ps/ (nmkm);
Loss≤0.22dB/km of 1550 is at the loss≤0.22dB/km of 1530nm~1565nm wave band.
CNU2008201664635U 2008-11-13 2008-11-13 Improved non-zero dispersion shifted single-mode fiber with large mode field distribution Expired - Fee Related CN201314957Y (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNU2008201664635U CN201314957Y (en) 2008-11-13 2008-11-13 Improved non-zero dispersion shifted single-mode fiber with large mode field distribution

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNU2008201664635U CN201314957Y (en) 2008-11-13 2008-11-13 Improved non-zero dispersion shifted single-mode fiber with large mode field distribution

Publications (1)

Publication Number Publication Date
CN201314957Y true CN201314957Y (en) 2009-09-23

Family

ID=41126757

Family Applications (1)

Application Number Title Priority Date Filing Date
CNU2008201664635U Expired - Fee Related CN201314957Y (en) 2008-11-13 2008-11-13 Improved non-zero dispersion shifted single-mode fiber with large mode field distribution

Country Status (1)

Country Link
CN (1) CN201314957Y (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102185238A (en) * 2011-04-01 2011-09-14 北京交通大学 Large-effective-area single mode optical fiber amplifier based on change of refractive index distribution of cladding
CN102183813A (en) * 2011-05-09 2011-09-14 北京交通大学 Optical fiber structure with spotlighting layer
CN102200610A (en) * 2011-05-27 2011-09-28 成都富通光通信技术有限公司 Dispersion optimization single-mode optical fibre for super-high-speed long-distance dense wave division multiplexing
CN102222855A (en) * 2011-05-09 2011-10-19 北京交通大学 Fiber laser with spotlighting layer structure
CN102255228A (en) * 2011-05-09 2011-11-23 北京交通大学 Optical fiber amplifier having light collecting layer structure
CN101764343B (en) * 2010-01-08 2012-04-25 北京交通大学 Optical fiber of coupling multilayer rare earth blending ring-shaped fiber core with single-mold fiber core
CN109839694A (en) * 2017-11-27 2019-06-04 中天科技精密材料有限公司 A kind of cutoff wavelength displacement single mode optical fiber

Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101764343B (en) * 2010-01-08 2012-04-25 北京交通大学 Optical fiber of coupling multilayer rare earth blending ring-shaped fiber core with single-mold fiber core
CN102185238A (en) * 2011-04-01 2011-09-14 北京交通大学 Large-effective-area single mode optical fiber amplifier based on change of refractive index distribution of cladding
CN102185238B (en) * 2011-04-01 2012-05-23 北京交通大学 Large-effective-area single mode optical fiber amplifier based on change of refractive index distribution of cladding
CN102183813A (en) * 2011-05-09 2011-09-14 北京交通大学 Optical fiber structure with spotlighting layer
CN102222855A (en) * 2011-05-09 2011-10-19 北京交通大学 Fiber laser with spotlighting layer structure
CN102255228A (en) * 2011-05-09 2011-11-23 北京交通大学 Optical fiber amplifier having light collecting layer structure
CN102255228B (en) * 2011-05-09 2012-05-30 北京交通大学 Optical fiber amplifier having light collecting layer structure
CN102183813B (en) * 2011-05-09 2012-05-30 北京交通大学 Optical fiber structure with spotlighting layer
CN102200610A (en) * 2011-05-27 2011-09-28 成都富通光通信技术有限公司 Dispersion optimization single-mode optical fibre for super-high-speed long-distance dense wave division multiplexing
CN102200610B (en) * 2011-05-27 2012-10-17 成都富通光通信技术有限公司 Dispersion optimization single-mode optical fibre for super-high-speed long-distance dense wave division multiplexing
CN109839694A (en) * 2017-11-27 2019-06-04 中天科技精密材料有限公司 A kind of cutoff wavelength displacement single mode optical fiber
CN109839694B (en) * 2017-11-27 2020-08-18 中天科技精密材料有限公司 Single mode fiber with cut-off wavelength displacement

Similar Documents

Publication Publication Date Title
CN101446663B (en) Improved nonzero dispersion-shifted single-mode optical fiber with large mode field distribution
US6483975B1 (en) Positive dispersion optical fiber having large effective area
CN103257397B (en) Single-mode fiber
US7620282B2 (en) Low bend loss single mode optical fiber
JP4247950B2 (en) Dispersion compensating optical fiber and wavelength division multiplexing optical transmission line using the dispersion compensating optical fiber
CN101551488B (en) Dispersion-shifted optical fiber
CN201314957Y (en) Improved non-zero dispersion shifted single-mode fiber with large mode field distribution
US6829423B2 (en) Low slope dispersion managed waveguide
CN104603652B (en) Optical fiber
CN105683790A (en) Few mode optical fibers for space division multiplexing
AU750557B2 (en) Low slope dispersion managed waveguide
US6633715B2 (en) Optical fiber having negative dispersion, negative dispersion slope and large effective area
JP4282235B2 (en) Dispersion shifted single mode optical fiber optimized for high data rates
CN102200610B (en) Dispersion optimization single-mode optical fibre for super-high-speed long-distance dense wave division multiplexing
US6650814B2 (en) Single mode dispersion compensating optical fiber
US6614973B2 (en) Monomode optical fiber for optical fiber cable transmission networks with wavelength division multiplexing
JP2004133373A (en) Optical fiber and optical transmission line using optical fiber
WO2007005332A2 (en) Non-zero dispersion shifted optical fiber
CN101373237B (en) Single-mode optical fiber optimizing dispersion characteristic
WO2002069005A1 (en) Waveguide fiber for dispersion and slope compensation
CN202171655U (en) Dispersion optimizing single mode fiber suitable for ultra high speed long-distance dense wavelength division multiplexing
CN1471256B (en) Single mode optical fiber and optica lcommunication system
CN100432720C (en) Single-mode optical fiber used for overlength distance fiber transit network
JP2002116338A (en) Optical fiber and optical transmission line using it
MXPA00008215A (en) Low slope dispersion managed waveguide

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20090923

Termination date: 20101113