WO2020108141A1 - Bending-resistant wide band multimode optical fiber - Google Patents
Bending-resistant wide band multimode optical fiber Download PDFInfo
- Publication number
- WO2020108141A1 WO2020108141A1 PCT/CN2019/111387 CN2019111387W WO2020108141A1 WO 2020108141 A1 WO2020108141 A1 WO 2020108141A1 CN 2019111387 W CN2019111387 W CN 2019111387W WO 2020108141 A1 WO2020108141 A1 WO 2020108141A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- core layer
- refractive index
- cladding
- optical fiber
- bending
- Prior art date
Links
- 238000005452 bending Methods 0.000 title claims abstract description 59
- 239000013307 optical fiber Substances 0.000 title claims abstract description 46
- 239000012792 core layer Substances 0.000 claims abstract description 111
- 238000005253 cladding Methods 0.000 claims abstract description 93
- 230000000994 depressogenic effect Effects 0.000 claims description 44
- 239000010410 layer Substances 0.000 claims description 26
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 18
- 235000012239 silicon dioxide Nutrition 0.000 claims description 15
- 229910005793 GeO 2 Inorganic materials 0.000 claims description 9
- 238000009826 distribution Methods 0.000 claims description 8
- 239000010453 quartz Substances 0.000 claims description 8
- 239000000377 silicon dioxide Substances 0.000 claims description 5
- 229910052681 coesite Inorganic materials 0.000 claims description 4
- 229910052906 cristobalite Inorganic materials 0.000 claims description 4
- 229910052682 stishovite Inorganic materials 0.000 claims description 4
- 229910052905 tridymite Inorganic materials 0.000 claims description 4
- 238000004364 calculation method Methods 0.000 claims description 3
- 239000011248 coating agent Substances 0.000 claims 1
- 238000000576 coating method Methods 0.000 claims 1
- YBMRDBCBODYGJE-UHFFFAOYSA-N germanium dioxide Chemical compound O=[Ge]=O YBMRDBCBODYGJE-UHFFFAOYSA-N 0.000 abstract description 8
- 239000000835 fiber Substances 0.000 description 17
- 238000012360 testing method Methods 0.000 description 13
- 238000000034 method Methods 0.000 description 11
- 239000006185 dispersion Substances 0.000 description 6
- 230000008021 deposition Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 230000005540 biological transmission Effects 0.000 description 4
- 238000007665 sagging Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
Images
Classifications
-
- 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
-
- 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
-
- 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
- G02B6/0288—Multimode fibre, e.g. graded index core for compensating modal dispersion
Definitions
- the invention relates to the field of optical communication, in particular to a broadband bending-resistant multimode optical fiber.
- the traditional bending-resistant multimode optical fiber is manufactured by the in-tube method, in which the core layer is deposited with quartz doped with GeO 2 , the outer surface is deposited with a deep-dipped cladding of quartz doped with F, and the outer layer is covered with a pure quartz sleeve.
- the deposition core layer of the multimode optical fiber itself is large, and the deposition rate of the multimode preform is much lower than that of the single mode preform, the price of the multimode optical fiber in the market is much higher than that of the single mode optical fiber.
- the invention provides a broadband anti-bending multimode optical fiber, which includes a core layer, a base tube, a depressed cladding and an outer cladding.
- the radial cross-sections of the base tube, the depressed cladding and the outer cladding are all rings.
- the core layer is doped with GeO 2 , P 2 O 5 and F, the core layer is a gradient refractive index region, the core layer radius is R1, the base tube is sleeved outside the core layer, the core
- the distance from the center of the layer to the boundary of the base tube is R2, the width of the base tube is R2-R1, the depressed cladding is disposed outside the base tube, and the center of the core layer to the boundary of the depressed cladding
- the distance is R3, the width of the depressed cladding is R3-R2, the outer cladding is sleeved on the outside of the depressed cladding, the distance from the center of the core layer to the boundary of the outer cladding is Rmax, the The width of the outer cladding layer is Rmax-R3, and the molar concentration of F in the core layer varies with the radius of the core layer, satisfying the following formula:
- M F0 is the molar concentration of F in the center of the core layer, and the value range of ⁇ F is 6-10, and the M F (r) represents the radial distance r of the F at the center axis of the core layer The molar concentration at.
- ⁇ F is preferably 7-9.
- the molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer, satisfying the following formula:
- M P0 is the molar concentration of P 2 O 5 in the center of the core layer
- ⁇ p has a value range of 2.0-4.5
- M P (r) represents the diameter of the P 2 O 5 at the central axis of the core layer To the molar concentration at distance r.
- ⁇ p is preferably 2.5-3.5.
- the refractive index difference ⁇ n 0 at the center of the core layer is 0.0127-0.0167
- the radius R1 of the core layer is 22-26 ⁇ m
- the width R2-R1 of the base tube is 5.5-10.5 ⁇ m
- the center of the core layer The distance Rmax to the outer cladding edge is 62.5 ⁇ 2.5 ⁇ m.
- the radius R1 of the core layer is preferably 23-24 ⁇ m, and the width of the base tube is preferably 6.5-9.5 ⁇ m.
- the depressed cladding layer is deposited on the outer wall of the base pipe or formed on the outer side of the base pipe by a fluorine-doped quartz.
- the width R3-R2 of the depressed cladding layer is 3.5-5.5 ⁇ m
- the refractive index difference ⁇ n 2 of the depressed cladding layer is -0.007 ⁇ -0.004
- K ⁇ n 2 *(R3-R2), and satisfy -0.025 ⁇ K ⁇ -0.022.
- the refractive index profile of the core layer is distributed as a power exponential function
- ⁇ is the distribution parameter of the refractive index profile of the gradient region, wherein the central refractive index of the core layer is n 0 , and the boundary refractive index of the core layer
- the rate is n 1
- the refractive index of the base tube is n sio2
- the refractive index of the depressed cladding is n 2
- the refractive index of the outer cladding is n C
- the calculation formula of the refractive index of the optical fiber is:
- ⁇ ranges from 1.90 to 2.10
- r is the radial distance from any point on the core layer to the center of the core layer
- n 1 n SiO2
- nc n SiO2
- ⁇ is the center of the core layer
- the relative refractive index difference ⁇ (n 0 2 -n 1 2 )/(2n 0 2 ) with the boundary of the core layer.
- the broadband anti-bending multimode optical fiber provided by the present invention, because it does not need to deposit the concave part, removes the high-cost depressed cladding deposit layer, and uses a cheap method to prepare a depressed layer/or coat an inexpensive F-doped quartz on the outer wall of the base tube
- the optical fiber produced by the preform is increased by 20% or more compared with other bending multimode optical fiber preforms with the same deposition amount, which reduces the cost of the manufactured bending multimode optical fiber and has good bending performance.
- FIG. 1 is a schematic diagram of the refractive index profile of an optical fiber according to an embodiment of the present invention.
- FIG. 2 is a schematic diagram of the variation of the doping amount of F with the radius of the core layer according to an embodiment of the present invention.
- FIG. 3 is a schematic diagram of the variation of the doping amount of F with the radius of the core layer in another embodiment of the present invention.
- FIG. 4 is a schematic diagram of the variation of the doping amount of P 2 O 5 with the radius of the core layer in the embodiment of FIG. 3.
- FIG. 1 is a schematic diagram of the refractive index profile of a broadband anti-bending multimode optical fiber according to an embodiment of the present invention.
- the optical fiber is used for data transmission.
- the optical fiber includes a core layer and a base tube in order from inside to outside. , Sagging cladding and outer cladding.
- the core layer uses silicon dioxide as a matrix, and the core layer is doped with GeO 2 , P 2 O 5 and F, the core layer is a graded refractive index region, and the cross section of the core layer is circular.
- the radius is R1, that is, the radius of the gradient area is R1.
- the radius R1 of the gradient region is 22-26 ⁇ m, preferably 23-24 ⁇ m.
- the refractive index profile of the core layer is distributed as a power exponential function, and ⁇ is the distribution parameter of the refractive index profile of the gradient region, and its ⁇ value is 1.90-2.10.
- the central refractive index of the core layer is n 0
- the refractive index difference ⁇ n 0 of the core layer ranges from 0.0127 to 0.0167
- the boundary refractive index of the core layer is n 1 .
- the base pipe is sleeved on the outer side of the core layer.
- the radial cross section of the base pipe is annular, the inner diameter is R1, the outer diameter is R2, and the width of the base pipe is R2-R1.
- the width R2-R1 of the base tube is 5.5-10.5 ⁇ m, preferably 6.5-9.5 ⁇ m.
- the refractive index of the base tube is n sio2
- the boundary refractive index n 1 of the core layer is the same as the refractive index n sio2 of the base tube.
- the base tube is a pure silica sleeve
- the refractive index difference between the boundary of the core layer and the outer cladding layer is 0.
- the sagging cladding is sleeved on the outside of the base pipe, and the radial cross-section of the sagging cladding is ring-shaped.
- the sagging cladding is deposited on the outer wall of the base pipe or outside the base pipe
- the outer casing is formed of fluorine-doped quartz.
- the depressed cladding layer is deposited on the outer wall of the base tube by plasma outer cladding.
- the inner diameter of the depressed cladding is R2, the outer diameter is R3, and the width of the depressed cladding is R3-R2.
- the width of the depressed cladding R3-R2 is 3.5-5.5 ⁇ m, refractive
- the rate is n 2 .
- the outer cladding is sleeved on the outer side of the depressed cladding, the radial cross-section of the outer cladding is annular, the inner diameter of the outer cladding is R3, the outer diameter is Rmax, and the refractive index of the outer cladding is n C In this embodiment, the Rmax is set between 60-65 ⁇ m.
- the outer cladding is a pure silica sleeve, the outer cladding refractive index n C and the core layer
- the boundary refractive index n 1 and the refractive index n sio2 of the substrate tube are the same.
- the refractive index distribution of the optical fiber meets the requirements of formula (1):
- ⁇ is the distribution parameter of the refractive index profile of the gradient region
- r is the radial distance from any point A on the core layer to the core axis
- M F0 is the molar concentration of F in the center of the core layer
- the value range of ⁇ F is 6-10, preferably 7-9
- the M F (r) indicates that F is in the center of the core layer
- the center of the core layer is doped with GeO 2 with a molar concentration of 13% to 14% and F with a molar concentration of 0.2% to 0.8%.
- the boundary of the gradient region is doped with GeO 2 with a molar concentration of 1.4% to 8% and F with a molar concentration of 5% to 7%.
- the molar concentration of F in the core layer changes with the radius of the core layer, satisfying formula (2), the concentration of F in the base tube and the outer cladding is 0, and the concentration of F in the depressed cladding M Fd is a constant.
- the inter-mode dispersion must be minimized, that is, an optimal profile refractive index distribution parameter must be selected, and ⁇ opt (850- 950nm) is 0.05, indicating that the optical fiber can achieve the maximum effective mode bandwidth (EMB) in the wideband range of 850nm to 950nm, and it can satisfy the choice of four wavelengths for wavelength division multiplexing at 850nm to 950nm.
- EMB effective mode bandwidth
- the molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer, satisfying the following formula:
- M P0 as the center core layer P 2 O 5 molar concentration of the M P (r) represents the P 2 O 5 molar concentration of the radial distance r from the central axis of the core, ⁇ p
- the value range is 2.0-4.5, preferably 2.5-3.5.
- the center of the core layer is doped with GeO 2 with a molar concentration of 9.6% to 10.8% and F and 3.2% with a molar concentration of 0.4% to 1.5% 3.5% of P 2 O 5 .
- the boundary of the gradient region is doped with GeO 2 with a molar concentration of 8% to 9%, F with a molar concentration of 4.5% to 5%, and P 2 O 5 with a molar concentration of 0% to 1.2%.
- the molar concentration of F in the core layer varies with the radius of the core layer and satisfies formula (2), where M F0 is the molar concentration of F in the center of the core layer, and ⁇ F has a value range of 6.5 to 9, preferably From 7 to 8.5, the concentration of F in the base tube and the outer cladding is 0, and the concentration M Fd in the depressed cladding is constant.
- the molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer and satisfies formula (3).
- the ⁇ opt (850-950nm) is 0.005
- EMB effective mode bandwidth in the wideband range of 850nm to 950nm
- a PCVD process is used to prepare an optical fiber preform.
- the optical fiber preform is prepared by the MCVD process.
- an optical fiber preform is prepared by the MCVD process.
- the optical fiber preform is prepared by the MCVD process.
- the difference between the central refractive index of the core layer and the outer cladding layer n 0 -nc is 0.0143, and the difference between the boundary refractive index of the core layer and the outer cladding layer n 1 -nc is 0, the refractive index difference n 2 -nc of the depressed cladding and the outer cladding is -0.0062, the radius R1 of the gradient region is 24.9 ⁇ m, the width of the substrate tube R2-R1 is 8.9 ⁇ m, the depressed cladding
- the core layer is doped with GeO2, F and P2O5, the doped F and P2O5 meet the requirements of formula (2)(3), the The doping concentration of the depressed cladding F is 15.45%, the dispersion in the center of the fiber is -96.2ps/(nm ⁇ km
- the optical fibers have Effective mode bandwidth and good bending resistance.
- the broadband anti-bending multimode optical fiber provided by the present invention, because it does not need to deposit the concave part, removes the high-cost depressed cladding deposit layer, and uses a cheap method to prepare a depressed layer/or coat an inexpensive F-doped quartz on the outer wall of the base tube
- the optical fiber produced by the preform is increased by 20% or more compared with other bending multimode optical fiber preforms with the same deposition amount, which reduces the cost of the manufactured bending multimode optical fiber and has good bending performance.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Manufacture, Treatment Of Glass Fibers (AREA)
- Glass Compositions (AREA)
Abstract
Description
本发明涉及光通信领域,尤其涉及一种宽带抗弯多模光纤。The invention relates to the field of optical communication, in particular to a broadband bending-resistant multimode optical fiber.
传统的抗弯多模光纤采用管内法制造,其中芯层沉积掺GeO 2的石英,外面再沉积掺F的石英深下陷包层,外层再套纯石英套管。但是由于多模光纤本身的沉积芯层很大,且多模预制棒的沉积速率远低于单模预制棒的沉积速率,造成多模光纤在市场上的售价远高于单模光纤。目前,降低多模光纤的制造成本的方法不多,主要是采用提高沉积速率、增大芯棒尺寸以及廉价的原材料,但是这些方法受到工艺的局限,也带来多模光纤衰耗的略微增大为代价。 The traditional bending-resistant multimode optical fiber is manufactured by the in-tube method, in which the core layer is deposited with quartz doped with GeO 2 , the outer surface is deposited with a deep-dipped cladding of quartz doped with F, and the outer layer is covered with a pure quartz sleeve. However, because the deposition core layer of the multimode optical fiber itself is large, and the deposition rate of the multimode preform is much lower than that of the single mode preform, the price of the multimode optical fiber in the market is much higher than that of the single mode optical fiber. At present, there are not many methods to reduce the manufacturing cost of multimode fiber, mainly to increase the deposition rate, increase the size of the core rod and cheap raw materials, but these methods are limited by the process, but also bring a slight increase in the loss of multimode fiber Big price.
发明内容Summary of the invention
有鉴于此,有必要提供一种宽带抗弯多模光纤,其降低了生产成本且具有良好的抗弯性能。In view of this, it is necessary to provide a broadband bending-resistant multimode optical fiber, which reduces the production cost and has good bending resistance.
本发明提供一种宽带抗弯多模光纤,包括芯层、基管、下陷包层及外包层,所述基管、下陷包层及外包层沿径向的横截面均为圆环,所述芯层中掺杂有GeO 2,P 2O 5和F,所述芯层为折射率渐变区,所述芯层半径为R1,所述基管套设于所述芯层外侧,所述芯层中心到所述基管边界的距离为R2,所述基管的宽度为R2-R1,所述下陷包层设置在所述基管的外侧,所述芯层中心到所述下陷包层边界的距离为R3,所述下陷包层的宽度为R3-R2,所述外包层套设于所述下陷包层的外侧,所述芯层中心到所述外包层边界的距离为Rmax,所述外包层的宽度为Rmax-R3,所述芯层中的F的摩尔浓度随所述芯层的半径变化,满足如下公式: The invention provides a broadband anti-bending multimode optical fiber, which includes a core layer, a base tube, a depressed cladding and an outer cladding. The radial cross-sections of the base tube, the depressed cladding and the outer cladding are all rings. The core layer is doped with GeO 2 , P 2 O 5 and F, the core layer is a gradient refractive index region, the core layer radius is R1, the base tube is sleeved outside the core layer, the core The distance from the center of the layer to the boundary of the base tube is R2, the width of the base tube is R2-R1, the depressed cladding is disposed outside the base tube, and the center of the core layer to the boundary of the depressed cladding The distance is R3, the width of the depressed cladding is R3-R2, the outer cladding is sleeved on the outside of the depressed cladding, the distance from the center of the core layer to the boundary of the outer cladding is Rmax, the The width of the outer cladding layer is Rmax-R3, and the molar concentration of F in the core layer varies with the radius of the core layer, satisfying the following formula:
其中,M F0为所述芯层中心的F的摩尔浓度,β F的取值范围为6-10,所述M F(r)表示所述F在所述芯层中心轴的径向距离r处的摩尔浓度。 Where, M F0 is the molar concentration of F in the center of the core layer, and the value range of β F is 6-10, and the M F (r) represents the radial distance r of the F at the center axis of the core layer The molar concentration at.
进一步的,所述β F的取值范围优选为7-9。 Further, the value range of β F is preferably 7-9.
进一步的,所述芯层中的P 2O 5的摩尔浓度随所述芯层的半径变化,满足如下公式: Further, the molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer, satisfying the following formula:
其中,M P0为纤芯层中心P 2O 5的摩尔浓度,β p取值范围为2.0-4.5,所述M P(r)表示所述P 2O 5在所述芯层中心轴的径向距离r处的摩尔浓度。 Where, M P0 is the molar concentration of P 2 O 5 in the center of the core layer, β p has a value range of 2.0-4.5, and M P (r) represents the diameter of the P 2 O 5 at the central axis of the core layer To the molar concentration at distance r.
进一步的,所述β p的取值范围优选为2.5-3.5。 Further, the value range of β p is preferably 2.5-3.5.
进一步的,所述芯层中心的折射率差Δn 0为0.0127-0.0167,所述芯层半径R1为22-26μm,所述基管的宽度R2-R1为5.5-10.5μm,所述芯层中心至所述外包层边缘距离Rmax为62.5±2.5μm。 Further, the refractive index difference Δn 0 at the center of the core layer is 0.0127-0.0167, the radius R1 of the core layer is 22-26 μm, the width R2-R1 of the base tube is 5.5-10.5 μm, and the center of the core layer The distance Rmax to the outer cladding edge is 62.5±2.5 μm.
进一步的,所述芯层半径R1优选为23-24μm,所述基管的宽度,优选6.5-9.5μm。Further, the radius R1 of the core layer is preferably 23-24 μm, and the width of the base tube is preferably 6.5-9.5 μm.
进一步的,所述下陷包层沉积在所述基管外壁或在所述基管外侧外套一掺氟石英形成。Further, the depressed cladding layer is deposited on the outer wall of the base pipe or formed on the outer side of the base pipe by a fluorine-doped quartz.
进一步的,所述下陷包层的宽度R3-R2为3.5-5.5μm,所述下陷包层的折射率差Δn 2为-0.007~-0.004,K=Δn 2*(R3-R2),并且满足-0.025<K<-0.022。 Further, the width R3-R2 of the depressed cladding layer is 3.5-5.5 μm, the refractive index difference Δn 2 of the depressed cladding layer is -0.007~-0.004, K=Δn 2 *(R3-R2), and satisfy -0.025<K<-0.022.
进一步的,所述芯层的折射率剖面呈α幂指数函数分布,α为所述渐变区折射率剖面分布参数,其中所述芯层的中心折射率为n 0,所述芯层的边界折射率为n 1,所述基管的折射率为n sio2,所述下陷包层的折射率为n 2,所述外包层 折射率为n C,所述光纤的折射率计算公式为: Further, the refractive index profile of the core layer is distributed as a power exponential function, α is the distribution parameter of the refractive index profile of the gradient region, wherein the central refractive index of the core layer is n 0 , and the boundary refractive index of the core layer The rate is n 1 , the refractive index of the base tube is n sio2 , the refractive index of the depressed cladding is n 2 , the refractive index of the outer cladding is n C , and the calculation formula of the refractive index of the optical fiber is:
其中,α取值范围为1.90-2.10,r为所述芯层上任意一点位置到所述芯层中心的径向距离,n 1=n SiO2,nc=n SiO2,Δ为所述芯层中心和芯层边界的相对折射率差Δ=(n 0 2-n 1 2)/(2n 0 2)。 Where α ranges from 1.90 to 2.10, r is the radial distance from any point on the core layer to the center of the core layer, n 1 = n SiO2 , nc = n SiO2 , and Δ is the center of the core layer The relative refractive index difference Δ=(n 0 2 -n 1 2 )/(2n 0 2 ) with the boundary of the core layer.
本发明提供的宽带抗弯多模光纤,因其不需要沉积凹陷部分,将高成本的下陷包层沉积层去掉,在基管外壁采用廉价方法制备一个下陷层/或外套一根廉价掺F石英,预制棒生产的光纤比同样沉积量的其它抗弯多模光纤预制棒增加20%或以上,降低了所制造的抗弯多模光纤的成本并且具有良好的抗弯性能。The broadband anti-bending multimode optical fiber provided by the present invention, because it does not need to deposit the concave part, removes the high-cost depressed cladding deposit layer, and uses a cheap method to prepare a depressed layer/or coat an inexpensive F-doped quartz on the outer wall of the base tube The optical fiber produced by the preform is increased by 20% or more compared with other bending multimode optical fiber preforms with the same deposition amount, which reduces the cost of the manufactured bending multimode optical fiber and has good bending performance.
图1为本发明一实施方式中的光纤折射率剖面示意图。FIG. 1 is a schematic diagram of the refractive index profile of an optical fiber according to an embodiment of the present invention.
图2为本发明一实施方式中的F的掺杂量随芯层半径的变化示意图。FIG. 2 is a schematic diagram of the variation of the doping amount of F with the radius of the core layer according to an embodiment of the present invention.
图3为本发明另一实施方式中的F的掺杂量随芯层半径的变化示意图。FIG. 3 is a schematic diagram of the variation of the doping amount of F with the radius of the core layer in another embodiment of the present invention.
图4为图3实施方式中的P 2O 5的掺杂量随芯层半径的变化示意图。 FIG. 4 is a schematic diagram of the variation of the doping amount of P 2 O 5 with the radius of the core layer in the embodiment of FIG. 3.
如下具体实施方式将结合上述附图进一步说明本发明。The following specific embodiments will further illustrate the present invention with reference to the above drawings.
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be described clearly and completely in conjunction with the drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, but not all the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by a person of ordinary skill in the art without making creative efforts fall within the protection scope of the present invention.
除非另有定义,本文所使用的所有的技术和科学术语与属于本发明的技术 领域的技术人员通常理解的含义相同。本文中在本发明的说明书中所使用的术语只是为了描述具体的实施例的目的,不是旨在于限制本发明。本文所使用的术语“或/及”包括一个或多个相关的所列项目的任意的和所有的组合。Unless otherwise defined, all technical and scientific terms used herein have the same meaning as commonly understood by those skilled in the technical field of the present invention. The terminology used in the description of the present invention herein is for the purpose of describing specific embodiments, and is not intended to limit the present invention. The term "or/and" as used herein includes any and all combinations of one or more related listed items.
请参阅图1,图1为本发明一实施方式中的宽带抗弯多模光纤的折射率剖面示意图,所述光纤用于数据的传输,所述光纤包括由内向外依次包括芯层、基管、下陷包层及外包层。Please refer to FIG. 1. FIG. 1 is a schematic diagram of the refractive index profile of a broadband anti-bending multimode optical fiber according to an embodiment of the present invention. The optical fiber is used for data transmission. The optical fiber includes a core layer and a base tube in order from inside to outside. , Sagging cladding and outer cladding.
所述芯层以二氧化硅为基质,在所述芯层中掺杂GeO 2,P 2O 5及F,所述芯层为折射率渐变区,所述芯层横截面为圆形,其半径为R1,即所述渐变区的半径为R1。在本实施方式中,所述渐变区半径R1为22-26μm,优选为23-24μm。所述芯层的折射率剖面呈α幂指数函数分布,α为所述渐变区折射率剖面分布参数,其α值为1.90-2.10。所述芯层的中心折射率为n 0,其与所述外包层的折射率差Δn 0取值范围为0.0127-0.0167,所述芯层的边界折射率为n 1。 The core layer uses silicon dioxide as a matrix, and the core layer is doped with GeO 2 , P 2 O 5 and F, the core layer is a graded refractive index region, and the cross section of the core layer is circular. The radius is R1, that is, the radius of the gradient area is R1. In this embodiment, the radius R1 of the gradient region is 22-26 μm, preferably 23-24 μm. The refractive index profile of the core layer is distributed as a power exponential function, and α is the distribution parameter of the refractive index profile of the gradient region, and its α value is 1.90-2.10. The central refractive index of the core layer is n 0 , and the refractive index difference Δn 0 of the core layer ranges from 0.0127 to 0.0167, and the boundary refractive index of the core layer is n 1 .
所述基管套设于所述芯层外侧,所述基管沿径向的横截面为环形,内径为R1,外径为R2,所述基管的宽度为R2-R1。通过软件模拟,发现当基管的宽度大于5.5um时该抗弯多模光纤所有模式都可被限制在芯层渐变区内传输,且绝大部分能量都分布在芯层区域,基管区和下陷区没有发现传输模式;当基管的宽度小于5.5um,基管开始存在传输模式,将导致测试的光纤芯层直径大于52.5um,即标准纤芯直径的上限;当平台区大于10.5um时,本专利设计的多模光纤的弯曲性能变差,或不满足同类抗弯曲多模光纤的抗弯曲性能标准。因此,在本实施方式中,所述基管的宽度R2-R1为5.5-10.5μm,优选6.5-9.5μm。所述基管的折射率为n sio2,所述芯层的边界折射率n 1与所述基管的折射率n sio2相同,在本实施方式中,所述基管为纯二氧化硅套管,其与所述芯层边界和外包层的折射率差为0。 The base pipe is sleeved on the outer side of the core layer. The radial cross section of the base pipe is annular, the inner diameter is R1, the outer diameter is R2, and the width of the base pipe is R2-R1. Through software simulation, it is found that when the width of the base tube is greater than 5.5um, all modes of the bending-resistant multimode fiber can be restricted to be transmitted in the core layer gradient area, and most of the energy is distributed in the core layer area, the base tube area and the sag There is no transmission mode found in the area; when the width of the base tube is less than 5.5um, the base tube begins to have a transmission mode, which will result in the test fiber core diameter greater than 52.5um, which is the upper limit of the standard core diameter; when the platform area is greater than 10.5um, The bending performance of the multimode optical fiber designed by this patent becomes poor, or does not meet the bending resistance performance standards of similar bending-resistant multimode optical fibers. Therefore, in this embodiment, the width R2-R1 of the base tube is 5.5-10.5 μm, preferably 6.5-9.5 μm. The refractive index of the base tube is n sio2 , and the boundary refractive index n 1 of the core layer is the same as the refractive index n sio2 of the base tube. In this embodiment, the base tube is a pure silica sleeve , The refractive index difference between the boundary of the core layer and the outer cladding layer is 0.
所述下陷包层套设于所述基管外侧,所述下陷包层沿径向的横截面为环形,具体的,所述下陷包层沉积在所述基管外壁或在所述基管外侧外套一掺氟石英形成,在本实施方式中,所述下陷包层采用等离子外包的方式沉积在所述基管外壁。所述下陷包层的内径为R2,外径为R3,所述下陷包层的宽度为R3-R2,在本实施方式中,所述下陷包层的宽度R3-R2为3.5-5.5μm,折射率为n 2。所述下陷包层的折射率差Δn 2设定在-0.007~-0.004之间,定义K=Δn 2*(R3-R2), 并且满足-0.025<K<-0.022,引入K值用于保证抗弯多模光纤的弯曲损耗满足标准,同时保证所述基管区没有传输模式和能量。 The sagging cladding is sleeved on the outside of the base pipe, and the radial cross-section of the sagging cladding is ring-shaped. Specifically, the sagging cladding is deposited on the outer wall of the base pipe or outside the base pipe The outer casing is formed of fluorine-doped quartz. In this embodiment, the depressed cladding layer is deposited on the outer wall of the base tube by plasma outer cladding. The inner diameter of the depressed cladding is R2, the outer diameter is R3, and the width of the depressed cladding is R3-R2. In this embodiment, the width of the depressed cladding R3-R2 is 3.5-5.5 μm, refractive The rate is n 2 . The refractive index difference Δn 2 of the depressed cladding is set between -0.007~-0.004, and K=Δn 2 *(R3-R2) is defined, and it satisfies -0.025<K<-0.022, and the K value is introduced to ensure The bending loss of the bending-resistant multimode optical fiber meets the standard, and at the same time, it is ensured that the base tube region has no transmission mode and energy.
所述外包层套设于所述下陷包层外侧,所述外包层沿径向的横截面为环形,所述外包层的内径为R3,外径为Rmax,所述外包层折射率为n C,在本实施方式中,所述Rmax设定在60-65μm之间,在本实施方式中,所述外包层为纯二氧化硅套管,所述外包层折射率n C和所述芯层的边界折射率n 1以及所述基管的折射率n sio2相同。 The outer cladding is sleeved on the outer side of the depressed cladding, the radial cross-section of the outer cladding is annular, the inner diameter of the outer cladding is R3, the outer diameter is Rmax, and the refractive index of the outer cladding is n C In this embodiment, the Rmax is set between 60-65 μm. In this embodiment, the outer cladding is a pure silica sleeve, the outer cladding refractive index n C and the core layer The boundary refractive index n 1 and the refractive index n sio2 of the substrate tube are the same.
所述光纤的折射率分布满足公式(1)要求:The refractive index distribution of the optical fiber meets the requirements of formula (1):
其中,α为所述渐变区折射率剖面分布参数,r为所述芯层上任意一点A到所述芯轴的径向距离,Δ为所述芯层中心和芯层边界的相对折射率差,Δ=(n 0 2-n 1 2)/(2n 0 2)。 Where α is the distribution parameter of the refractive index profile of the gradient region, r is the radial distance from any point A on the core layer to the core axis, and Δ is the relative refractive index difference between the center of the core layer and the boundary of the core layer , Δ=(n 0 2 -n 1 2 )/(2n 0 2 ).
所述芯层中的F的摩尔浓度随所述芯层的半径变化,满足公式(2):The molar concentration of F in the core layer changes with the radius of the core layer, satisfying formula (2):
其中,M F0为所述芯层中心的F的摩尔浓度,β F的取值范围为6-10,优选为7-9,所述M F(r)表示所述F在所述芯层中心轴的径向距离r处的摩尔浓度。 Where, M F0 is the molar concentration of F in the center of the core layer, and the value range of β F is 6-10, preferably 7-9, and the M F (r) indicates that F is in the center of the core layer The molar concentration at the radial distance r of the axis.
如图2所示,本发明一实施方式中,所述芯层中心掺杂有摩尔浓度为13%~14%的GeO 2以及摩尔浓度为0.2%~0.8%的F。所述渐变区的边界掺杂有摩尔浓度为1.4%~8%的GeO 2以及摩尔浓度为5%~7%的F。其中,F在所述芯层的摩尔浓度随所述芯层的半径变化,满足公式(2),在所述基管和外包层的F的浓度为0,所述下陷包层中F的浓度M Fd为恒量。要实现多模光纤的带宽最大化,必须使其模间色散最小,即要选择一个最佳剖面折射率分布参数,根据最佳剖面折射率分布参数差值的计算公式得出Δα opt(850-950nm)为0.05,说明 所述光纤可以实现在850nm到950nm宽带范围内的有效模式带宽(EMB)可以达到最大,并满足在850nm到950nm任意选择四个波长进行波分复用。 As shown in FIG. 2, in an embodiment of the present invention, the center of the core layer is doped with GeO 2 with a molar concentration of 13% to 14% and F with a molar concentration of 0.2% to 0.8%. The boundary of the gradient region is doped with GeO 2 with a molar concentration of 1.4% to 8% and F with a molar concentration of 5% to 7%. Wherein, the molar concentration of F in the core layer changes with the radius of the core layer, satisfying formula (2), the concentration of F in the base tube and the outer cladding is 0, and the concentration of F in the depressed cladding M Fd is a constant. To maximize the bandwidth of the multimode fiber, the inter-mode dispersion must be minimized, that is, an optimal profile refractive index distribution parameter must be selected, and Δα opt (850- 950nm) is 0.05, indicating that the optical fiber can achieve the maximum effective mode bandwidth (EMB) in the wideband range of 850nm to 950nm, and it can satisfy the choice of four wavelengths for wavelength division multiplexing at 850nm to 950nm.
所述芯层中的P 2O 5的摩尔浓度随所述芯层的半径变化,满足如下公式: The molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer, satisfying the following formula:
其中,M P0为纤芯层中心P 2O 5的摩尔浓度,所述M P(r)表示所述P 2O 5在所述芯层中心轴的径向距离r处的摩尔浓度,β p取值范围为2.0-4.5,优选为2.5-3.5。 Wherein, M P0 as the center core layer P 2 O 5 molar concentration of the M P (r) represents the P 2 O 5 molar concentration of the radial distance r from the central axis of the core, β p The value range is 2.0-4.5, preferably 2.5-3.5.
请参阅图3和图4,本发明另一实施方式中,所述芯层中心掺杂有摩尔浓度为9.6%~10.8%的GeO 2以及摩尔浓度为0.4%~1.5%的F和3.2%~3.5%的P 2O 5。所述渐变区的边界掺杂有摩尔浓度为8%~9%的GeO 2以及摩尔浓度为4.5%~5%的F和0%~1.2%的P 2O 5。所述芯层中的F的摩尔浓度随所述芯层的半径变化并且满足公式(2),其中M F0为纤芯层中心F的摩尔浓度,β F取值范围为6.5~9,优选为7~8.5,在所述基管和外包层的F的浓度为0,在下陷包层中F的浓度M Fd为恒量。所述芯层中的P 2O 5的摩尔浓度随所述芯层的半径变化并且满足公式(3),要实现多模光纤的带宽最大化,必须使其模间色散最小,即要选择一个最佳剖面折射率分布参数,根据最佳剖面折射率分布参数差值的计算公式得出Δα opt(850-950nm)为0.005,说明所述光纤可以实现在850nm到950nm宽带范围内的有效模式带宽(EMB)可以达到最大,并满足在850nm到950nm任意选择四个波长进行波分复用。 3 and 4, in another embodiment of the present invention, the center of the core layer is doped with GeO 2 with a molar concentration of 9.6% to 10.8% and F and 3.2% with a molar concentration of 0.4% to 1.5% 3.5% of P 2 O 5 . The boundary of the gradient region is doped with GeO 2 with a molar concentration of 8% to 9%, F with a molar concentration of 4.5% to 5%, and P 2 O 5 with a molar concentration of 0% to 1.2%. The molar concentration of F in the core layer varies with the radius of the core layer and satisfies formula (2), where M F0 is the molar concentration of F in the center of the core layer, and β F has a value range of 6.5 to 9, preferably From 7 to 8.5, the concentration of F in the base tube and the outer cladding is 0, and the concentration M Fd in the depressed cladding is constant. The molar concentration of P 2 O 5 in the core layer varies with the radius of the core layer and satisfies formula (3). To maximize the bandwidth of the multimode fiber, it is necessary to minimize the dispersion between the modes, that is, to select one The best profile refractive index distribution parameter, according to the calculation formula of the difference of the best profile refractive index distribution parameter, the Δα opt (850-950nm) is 0.005, indicating that the optical fiber can achieve an effective mode bandwidth in the wideband range of 850nm to 950nm (EMB) can reach the maximum, and meet the arbitrary selection of four wavelengths for wavelength division multiplexing from 850nm to 950nm.
下面将结合具体的实施例对本发明做进一步说明。The present invention will be further described below in conjunction with specific embodiments.
例子1Example 1
该例子采用PCVD工艺制备光纤预制棒,所述芯层的中心折射率与外包层折射率差n 0-nc为0.0145,所述芯层的边界折射率与外包层折射率差n 1-nc为0,所述下陷包层与外包层的折射率差n 2-nc为-0.005,所述渐变区半径R1为24.3μm,所述基管的宽度R2-R1为8.1μm,所述下陷包层的宽度R3-R2为4.9μm,Rmax为62.5μm,k=-0.0245,所述芯层掺杂GeO 2和F,掺杂的F满足公式(2) 的要求,所述下陷包层F的掺杂浓度为1.3%,光纤中心的色散为-97ps/(nm·km),测试多模光纤的芯直径为49.4um,光纤的数值孔径NA为0.1995,以R7.5mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.01dB,在1300nm波长的弯曲损耗为0.1dB;以R15mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.04dB,在1300nm波长的弯曲损耗为0.02dB。 In this example, a PCVD process is used to prepare an optical fiber preform. The difference between the central refractive index of the core layer and the outer cladding layer n 0 -nc is 0.0145, and the difference between the boundary refractive index of the core layer and the outer cladding layer n 1 -nc is 0, the refractive index difference n 2 -nc of the depressed cladding and the outer cladding is -0.005, the radius R1 of the gradient region is 24.3 μm, the width of the base tube R2-R1 is 8.1 μm, the depressed cladding The width of R3-R2 is 4.9μm, Rmax is 62.5μm, k=-0.0245, the core layer is doped with GeO 2 and F, the doped F meets the requirements of formula (2), the doping of the depressed cladding layer F The impurity concentration is 1.3%, the dispersion in the center of the fiber is -97ps/(nm·km), the core diameter of the test multimode fiber is 49.4um, the numerical aperture of the fiber is 0.1995, and the bending loss test with R7.5mm for 2 turns Value: bending loss at 850nm wavelength is 0.01dB, bending loss at 1300nm wavelength is 0.1dB; bending loss at 2 turns with R15mm test value: bending loss at 850nm wavelength is 0.04dB, bending loss at 1300nm wavelength is 0.02dB.
例子2Example 2
该例子采用MCVD工艺制备光纤预制棒,所述芯层的中心折射率与外包层折射率差n 0-nc为0.0139,所述芯层的边界折射率与外包层折射率差n 1-nc为0,所述下陷包层与外包层的折射率差n 2-nc为-0.0056,所述渐变区半径R1为24.85μm,所述基管的宽度R2-R1为8.5μm,所述下陷包层的宽度R3-R2为4.15μm,Rmax为62.5μm,k=-0.02296,所述芯层掺杂GeO2、F及P2O5,掺杂的F和P2O5满足公式(2)(3)的要求,所述下陷包层F的掺杂浓度为15.45%,光纤中心的色散为-96.2ps/(nm·km),测试多模光纤的芯直径为50.3um,光纤的数值孔径NA为0.1953,以R7.5mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.13dB,在1300nm波长的弯曲损耗为0.29dB;以R15mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.01dB,在1300nm波长的弯曲损耗为0.05dB。 In this example, the optical fiber preform is prepared by the MCVD process. The difference between the central refractive index of the core layer and the outer cladding layer n 0 -nc is 0.0139, and the difference between the boundary refractive index of the core layer and the outer cladding layer n 1 -nc is 0, the refractive index difference n 2 -nc of the depressed cladding and the outer cladding is -0.0056, the radius R1 of the gradient region is 24.85 μm, the width of the base tube R2-R1 is 8.5 μm, the depressed cladding The width R3-R2 is 4.15μm, Rmax is 62.5μm, k=-0.02296, the core layer is doped with GeO2, F and P2O5, the doped F and P2O5 meet the requirements of formula (2)(3), the The doping concentration of the depressed cladding F is 15.45%, the dispersion of the fiber center is -96.2ps/(nm·km), the core diameter of the test multimode fiber is 50.3um, the numerical aperture NA of the fiber is 0.1953, and R7.5mm Test value of bending loss around 2 turns: bending loss at 850nm wavelength is 0.13dB, bending loss at 1300nm wavelength is 0.29dB; testing value of bending loss at 2 turns with R15mm: bending loss at 850nm wavelength is 0.01dB, The bending loss at 1300nm wavelength is 0.05dB.
例子3Example 3
该例子采用MCVD工艺制备光纤预制棒,所述芯层的中心折射率与外包层折射率差n 0-nc为0.0141,所述芯层的边界折射率与外包层折射率差n 1-nc为0,所述下陷包层与外包层的折射率差n 2-nc为-0.0052,所述渐变区半径R1为25.05μm,所述基管的宽度R2-R1为6.4μm,所述下陷包层的宽度R3-R2为4.5μm,Rmax为62.5μm,k=-0.0234,所述芯层掺杂GeO2、F及P2O5,掺杂的F和P2O5满足公式(2)(3)的要求,所述下陷包层F的掺杂浓度为15.45%,光纤中心的色散为-96.2ps/(nm·km),测试多模光纤的芯直径为50.9um,光纤的数值孔径NA为0.1967,以R7.5mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.06dB,在1300nm波长的弯曲损耗为0.2dB;以R15mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.006dB,在1300nm波长的弯曲损耗为0.07dB。 In this example, an optical fiber preform is prepared by the MCVD process. The difference between the central refractive index of the core layer and the outer cladding layer n 0 -nc is 0.0141, and the difference between the boundary refractive index of the core layer and the outer cladding layer n 1 -nc is 0, the refractive index difference n 2 -nc of the depressed cladding and the outer cladding is -0.0052, the radius R1 of the gradient region is 25.05 μm, the width of the base tube R2-R1 is 6.4 μm, the depressed cladding The width R3-R2 is 4.5μm, Rmax is 62.5μm, k=-0.0234, the core layer is doped with GeO2, F and P2O5, the doped F and P2O5 meet the requirements of formula (2)(3), the The doping concentration of the depressed cladding F is 15.45%, the dispersion in the center of the fiber is -96.2ps/(nm·km), the core diameter of the test multimode fiber is 50.9um, the numerical aperture of the fiber is 0.1967, with R7.5mm Test value of bending loss around 2 turns: bending loss at 850nm wavelength is 0.06dB, bending loss at 1300nm wavelength is 0.2dB; testing value of bending loss at 2 turns with R15mm: bending loss at 850nm wavelength is 0.006dB, The bending loss at 1300nm wavelength is 0.07dB.
例子4Example 4
该例子采用MCVD工艺制备光纤预制棒,所述芯层的中心折射率与外包层折射率差n 0-nc为0.0143,所述芯层的边界折射率与外包层折射率差n 1-nc为0,所述下陷包层与外包层的折射率差n 2-nc为-0.0062,所述渐变区半径R1为24.9μm,所述基管的宽度R2-R1为8.9μm,所述下陷包层的宽度R3-R2为3.7μm,Rmax为62.5μm,k=-0.02232,所述芯层掺杂GeO2、F及P2O5,掺杂的F和P2O5满足公式(2)(3)的要求,所述下陷包层F的掺杂浓度为15.45%,光纤中心的色散为-96.2ps/(nm·km),测试多模光纤的芯直径为50.6um,光纤的数值孔径NA为0.1981,以R7.5mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.18dB,在1300nm波长的弯曲损耗为0.37dB;以R15mm绕2圈的弯曲损耗测试值:在850nm波长的弯曲损耗为0.03dB,在1300nm波长的弯曲损耗为0.1dB。 In this example, the optical fiber preform is prepared by the MCVD process. The difference between the central refractive index of the core layer and the outer cladding layer n 0 -nc is 0.0143, and the difference between the boundary refractive index of the core layer and the outer cladding layer n 1 -nc is 0, the refractive index difference n 2 -nc of the depressed cladding and the outer cladding is -0.0062, the radius R1 of the gradient region is 24.9 μm, the width of the substrate tube R2-R1 is 8.9 μm, the depressed cladding The width R3-R2 is 3.7μm, Rmax is 62.5μm, k=-0.02232, the core layer is doped with GeO2, F and P2O5, the doped F and P2O5 meet the requirements of formula (2)(3), the The doping concentration of the depressed cladding F is 15.45%, the dispersion in the center of the fiber is -96.2ps/(nm·km), the core diameter of the test multimode fiber is 50.6um, the numerical aperture of the fiber is 0.1981, with R7.5mm Test value of bending loss around 2 turns: bending loss at 850nm wavelength is 0.18dB, bending loss at 1300nm wavelength is 0.37dB; testing value of bending loss at 2 turns with R15mm: bending loss at 850nm wavelength is 0.03dB, The bending loss at 1300nm wavelength is 0.1dB.
有上述例子可知,所述光纤在850nm波长,以7.5mm半径弯曲绕2圈的附加损耗不超过0.18dB,以15mm半径弯曲绕2圈的附加损耗不超过0.01dB;在1300nm波长,以7.5mm半径弯曲绕2圈的附加损耗不超过0.37dB,以15mm半径弯曲绕2圈的附加损耗不超过0.1dB,所述光纤在850nm到950nm宽带范围内的有介于5700MHz-km~2500MHz-km的有效模式带宽,具有良好的抗弯性能。It can be seen from the above example that the additional loss of the optical fiber at a wavelength of 850 nm and two turns around a radius of 7.5 mm does not exceed 0.18 dB, and the additional loss of a two-turn curve at a radius of 15 mm does not exceed 0.01 dB; The additional loss of 2 turns around the radius bend does not exceed 0.37dB, and the additional loss of 2 turns around the radius of 15mm does not exceed 0.1dB. In the wideband range of 850nm to 950nm, the optical fibers have Effective mode bandwidth and good bending resistance.
本发明提供的宽带抗弯多模光纤,因其不需要沉积凹陷部分,将高成本的下陷包层沉积层去掉,在基管外壁采用廉价方法制备一个下陷层/或外套一根廉价掺F石英,预制棒生产的光纤比同样沉积量的其它抗弯多模光纤预制棒增加20%或以上,降低了所制造的抗弯多模光纤的成本并且具有良好的抗弯性能。The broadband anti-bending multimode optical fiber provided by the present invention, because it does not need to deposit the concave part, removes the high-cost depressed cladding deposit layer, and uses a cheap method to prepare a depressed layer/or coat an inexpensive F-doped quartz on the outer wall of the base tube The optical fiber produced by the preform is increased by 20% or more compared with other bending multimode optical fiber preforms with the same deposition amount, which reduces the cost of the manufactured bending multimode optical fiber and has good bending performance.
本技术领域的普通技术人员应当认识到,以上的实施方式仅是用来说明本发明,而并非用作为对本发明的限定,只要在本发明的实质精神范围内,对以上实施方式所作的适当改变和变化都落在本发明要求保护的范围内。Persons of ordinary skill in the art should realize that the above embodiments are only used to illustrate the present invention, and are not intended to limit the present invention, as long as they make appropriate changes to the above embodiments within the spirit and scope of the present invention And changes fall within the scope of the claimed invention.
Claims (9)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201811457678.7A CN111257994B (en) | 2018-11-30 | 2018-11-30 | Broadband bend-resistant multimode optical fiber |
CN201811457678.7 | 2018-11-30 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2020108141A1 true WO2020108141A1 (en) | 2020-06-04 |
Family
ID=70852369
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/CN2019/111387 WO2020108141A1 (en) | 2018-11-30 | 2019-10-16 | Bending-resistant wide band multimode optical fiber |
Country Status (2)
Country | Link |
---|---|
CN (1) | CN111257994B (en) |
WO (1) | WO2020108141A1 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113625390B (en) * | 2021-10-14 | 2021-12-31 | 长飞光纤光缆股份有限公司 | Dispersion optimization bending insensitive optical fiber |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20150023642A1 (en) * | 2013-07-16 | 2015-01-22 | Corning Incorporated | High bandwidth mmf and method of making |
CN105060701A (en) * | 2015-07-24 | 2015-11-18 | 长飞光纤光缆股份有限公司 | Preparation method for large-sized bended insensitive multimode optical fiber preform |
CN105334569A (en) * | 2015-12-17 | 2016-02-17 | 长飞光纤光缆股份有限公司 | High-bandwidth anti-bending multimode fiber |
CN106371167A (en) * | 2016-11-26 | 2017-02-01 | 长飞光纤光缆股份有限公司 | High-bandwidth multi-mode fiber |
CN106707407A (en) * | 2016-12-30 | 2017-05-24 | 中天科技精密材料有限公司 | Wideband semi-step type multimode optical fiber |
CN106842419A (en) * | 2016-12-30 | 2017-06-13 | 中天科技精密材料有限公司 | A kind of broadband bend-insensitive multimode fibre |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105759344B (en) * | 2016-03-23 | 2018-11-30 | 长飞光纤光缆股份有限公司 | A kind of anti-bending multimode fiber |
US10162109B2 (en) * | 2017-02-07 | 2018-12-25 | Corning Incorporated | Multimode optical fibers for attenuators |
CN209514123U (en) * | 2018-11-30 | 2019-10-18 | 中天科技精密材料有限公司 | Broadband bending resistance multimode fibre |
-
2018
- 2018-11-30 CN CN201811457678.7A patent/CN111257994B/en active Active
-
2019
- 2019-10-16 WO PCT/CN2019/111387 patent/WO2020108141A1/en active Application Filing
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20150023642A1 (en) * | 2013-07-16 | 2015-01-22 | Corning Incorporated | High bandwidth mmf and method of making |
CN105060701A (en) * | 2015-07-24 | 2015-11-18 | 长飞光纤光缆股份有限公司 | Preparation method for large-sized bended insensitive multimode optical fiber preform |
CN105334569A (en) * | 2015-12-17 | 2016-02-17 | 长飞光纤光缆股份有限公司 | High-bandwidth anti-bending multimode fiber |
CN106371167A (en) * | 2016-11-26 | 2017-02-01 | 长飞光纤光缆股份有限公司 | High-bandwidth multi-mode fiber |
CN106707407A (en) * | 2016-12-30 | 2017-05-24 | 中天科技精密材料有限公司 | Wideband semi-step type multimode optical fiber |
CN106842419A (en) * | 2016-12-30 | 2017-06-13 | 中天科技精密材料有限公司 | A kind of broadband bend-insensitive multimode fibre |
Also Published As
Publication number | Publication date |
---|---|
CN111257994B (en) | 2025-04-18 |
CN111257994A (en) | 2020-06-09 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP7190236B2 (en) | Low-loss optical fiber with core region co-doped with fluorine and chlorine | |
JP5685028B2 (en) | Multimode optical fiber with improved bending loss | |
CN101373238B (en) | Bending Loss Insensitive Single Mode Fiber | |
CN106772788B (en) | A cut-off wavelength shifted single-mode fiber | |
CN103048732B (en) | Bend insensitive fiber | |
JPH01163707A (en) | Optical fiber | |
US20190154911A1 (en) | Low loss optical fiber with core codoped with two or more halogens | |
CN110488411B (en) | Bending-resistant single-mode optical fiber | |
WO2013177996A1 (en) | Graded refractive index bending-resistant multimode optical fiber | |
WO2016173253A1 (en) | Ultralow-attenuation bend-insensitive single-mode optical fibre | |
CN108375815B (en) | High-bandwidth bending insensitive multimode optical fiber | |
CN112904474B (en) | Small-outer-diameter low-attenuation bending insensitive single-mode optical fiber | |
CN113608298B (en) | Large-mode-field-diameter bending insensitive single-mode fiber | |
WO2017101568A1 (en) | High-bandwidth anti-bending multimode optical fiber | |
WO2015007097A1 (en) | Bending insensitive single mode optical fibre | |
CN111399113B (en) | Small-outer-diameter bending insensitive single-mode optical fiber | |
US10564349B2 (en) | Low bend loss optical fiber with graded index core | |
WO2013177995A1 (en) | Graded refractive index bending-resistant multimode optical fiber | |
WO2022027796A1 (en) | Bend-resistant optical fiber manufacturing method and optical fiber corresponding thereto | |
WO2019122943A1 (en) | Bending-loss insensitve single mode fibre, with a shallow trench, and corresponding optical system | |
CN110749953B (en) | Low-dispersion single-mode optical fiber | |
CN114325928B (en) | Low-loss bending-resistant single-mode optical fiber | |
CN209514123U (en) | Broadband bending resistance multimode fibre | |
WO2020108141A1 (en) | Bending-resistant wide band multimode optical fiber | |
US10422948B2 (en) | Optical fiber and method of manufacturing the same |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
121 | Ep: the epo has been informed by wipo that ep was designated in this application |
Ref document number: 19891127 Country of ref document: EP Kind code of ref document: A1 |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
122 | Ep: pct application non-entry in european phase |
Ref document number: 19891127 Country of ref document: EP Kind code of ref document: A1 |