KR20010046512A - Non-zero dispersion shifted fiber manufacturing method - Google Patents

Abstract

PURPOSE: A method of manufacturing preform of non-zero dispersion shifted fiber is provided to transmit mass signals to a long distance on a DWDM system by minimizing compensation for dispersion along the wide bandwidth. CONSTITUTION: In a method of manufacturing preform of non-zero dispersion shifted fiber, in step (one), a suite deposit for cradding is produced by depositing porous glass particles on a glass load while hydrolyzing glass under heats. In step (two), The suite deposit is dehydrated and the OH is eliminated. In step (three), the suite deposit without the OH is deadburned at an adequate temperature, producing transparent glass. In step (four), the glass is extruded to make a glass stick for core layer. In step (five), the glass stick is again hydrolyzed under heat to produce another suite deposit. In step (six), The suite deposit is again deadburned to produce the final product.

Description

Non-zero dispersion shifted fiber manufacturing method

The present invention relates to a method for manufacturing a mother agent for a non-zero dispersion shifted fiber, and in particular, when producing a soot deposit, a raw material of SiCl ₄ , GeCl ₄ and fuel fibers, which are optical fiber raw materials, at the bottom of the outer surface of the seed rod. By applying a gas mixture of H ₂ , O _{2, which} is a gas, with the flame of the burner as appropriate,

The refractive index profile of the secondary core has a trapezoidal shape, and the ratio of the length to the radius of the upper and lower base layers of the secondary core of the profile is about 0.3 to 0.8, and the difference in specific refractive index between the primary fiber and the cladding is 0.5 to 0.8. The difference in specific refractive index between charcoal and cladding is about 0.05 to 0.3, minimizing the FWM (Four Wave Mixing) phenomenon in the wavelength division area, while the dispersion slope becomes smaller than that of the existing non-zero dispersion transition optical fiber, and thus the usable wavelength range is expanded. The present invention relates to a method for manufacturing a base material for an optical fiber capable of transmitting a large amount of high speed information in the wavelength range of 1620 nm.

In general, optical fiber transmits a laser signal containing information through a core to transmit at an arbitrary wavelength and forms a cladding on the outer circumferential surface of the core so that a signal having an arbitrary wavelength is lost while transmitting to minimize the loss. It is well known that it is able to transmit to a stable place.

In the prior art, when an optical fiber is manufactured into a single mode optical fiber by a VAD method (Vapor-axial deposition method),

As shown in Figure 1 the glass raw material

Through a primary burner (3a) is installed at the lower end is properly with the fiber raw material gas of SiCl _4, GeCl ₄ and the fuel gas in the gas mixture (4a) of H _2, O ₂ and the flame, and a second burner (3b) through may fixes this laminate (2 by for core deposition on a seed rod (1) to a hydrolysis reaction by appropriate application of mixed gas (4b) of the SiCl ₄ with the fuel gas, H _2, O _2, an optical fiber raw material gas with the flame ),

Removing OH ions from the soot deposit (2) in a furnace containing Cl ₂ gas (dehydration),

Sintering the core soot deposits (2) from which the OH ions have been removed at a suitable temperature to transparent vitrify,

A process of making the glass rod for core by stretching the vitrified core suot deposits to the designed outer diameter;

Depositing a cladding suit by subjecting the glass material to a flame hydrolysis reaction again on the outer circumference of the core glass rod;

The optical fiber was manufactured by sintering the cladding suit.

As described above, in the single mode optical fiber manufactured by the conventional manufacturing method, the specific refractive index difference (△ = n ₁ -n ₂ / n ₁ , where n ₁ is the core refractive index and n ₂ is the cladding refractive index) is about △ = 0.34. As shown in FIG. 2, the dispersion of the single mode optical fiber is 17ps / km as shown in b-2 of FIG. 3 at a wavelength range of 1550 nm, which is a WDM (Wavelength Division Multiplexing) wavelength range, in a stepped structure. very high in nm. Therefore, long distance transmission of broadband is impossible in the WDM region of more than 1530nm without compensating for dispersion.

In addition, the dispersion transition optical fiber manufactured by the conventional manufacturing method has zero dispersion in the vicinity of the wavelength of 1550 nm, which is the WDM region, and the optical fiber effective area is small, as shown in b-2 of FIG. There was a difficulty in WDM transmission system due to mixing phenomenon.

That is, in a Dense Wavelength Division Multiplexing (DWDM) region where dispersion is close to "0", when three wavelengths are transmitted through one optical fiber, the three wavelengths interfere with each other to generate a fourth wavelength. The fourth wavelength generated causes distortion of the transmission signal, degrades the transmission quality, and is recognized as noise during transmission. As a result, the fourth color wavelength cannot be recolored and the usable wavelength range is limited.

In addition, as shown in (b) in the graph of Figure 3 has a disadvantage such that the area of the available wavelength becomes small due to the relatively large slope. In the figure, b-1 is a dispersion characteristic graph of a single mode (SM) optical fiber and b-2 is a dispersion characteristic graph of a dispersion transition (DSF) optical fiber.

The cause of the fourth wavelength that causes the FWM phenomenon is expressed by the following equation in "JOURNAL OF QUANTUM ELECTRONICS, VOL, QE-23".

Here, P _ijk (L): the strength of the new power

D _c : fiber dispersion

A _eff : effective area of optical fiber

Therefore, in order to suppress the FWM phenomenon, it is preferable that the zero dispersion of the optical fiber basically does not exist in the WDM use area, and it is desirable to form the effective area of the optical fiber as large as possible.

The present invention has been made to solve the above problems, the object of the present invention,

Existing by prepared by applying as appropriate with a gas mixture of fiber material gas of SiCl _4, GeCl ₄ and the fuel gas, H _2, O ₂ and the flame of the burner from the outer surface of the lower end of a seed rod to produce a number of fixes this deposited material for the core The non-dispersion transition is less than 0.085 less than the dispersion slope of the base material for the optical fiber, and the ratio of the distance between the trapezoidal primary cladding and the secondary cladding from 0.3 to 0.8 is 0.3 to 0.8 so that the zero dispersion point is less than 1530 nm wavelength. Thus, the refractive index difference of the optical fiber is 0.5 to 0.8, and the refractive index difference of the primary cladding is 0.1 to 0.3, so as to suppress the FWM phenomenon in the DWDM area and to expand the usable area in the DWDM area than the conventional non-zero dispersion transition optical fiber base material. DWDM allows small signals to be transmitted over long distances with minimal or no compensation for dispersion over broadband It is to provide a method for manufacturing a non-disperse transition optical fiber that can be used in the system.

1 is a schematic view of a soot deposit for cores prepared by a conventional method.

2 is a schematic diagram showing a conventional single-mode optical fiber refractive index distribution.

3 is a graph of dispersion characteristics of optical fibers according to the conventional and the present invention.

4 is a flow chart showing the manufacturing process of the present invention.

5 is a schematic representation of a soot deposit according to one embodiment made by the method of the present invention.

6 is a schematic representation of a soot deposit according to another embodiment produced by the method of the present invention.

7 is a schematic view of a furnace used for dehydration and sintering of the present invention.

8 is a schematic view of a clad soot deposit prepared by the method of the present invention;

9 is a graph showing the refractive index distribution of the optical fiber produced by the present invention.

* Nomenclature for the main parts of the drawings

10: seed road 12: the suot sediment

13 burner 14 mixed gas

15: core core 16: heater

18: glass rod 20: crouting suit pile

In order to achieve the above object, the present invention provides a first deposition process in which a glass raw material having a core and a cladding composition is deposited on a prepared glass rod by flame hydrolysis reaction of a glass material to form a core suot deposit. The primary dewatering process of dewatering OH groups while dewatering the core soot deposits in a furnace containing Cl ₂ gas, and sintering the core soot deposits from which the OH groups were removed at an appropriate temperature for transparent vitrification The primary sintering process, stretching the vitrified core suot deposits to the designed outer diameter to make the core glass rods, and subjecting the hydrolysis reaction to the outer periphery of the core glass rods The secondary deposition process for depositing the wort (hereinafter referred to as cladding suout) and the secondary sintering process for sintering the cladding soot deposits described above. The ratio of the distance between the trapezoidal primary cladding from the center of the core and the distance between the core of the core and the secondary cladding is 0.3 to 0.8, with the zero dispersion point below the wavelength of 1530 nm and the refractive index difference between the core and the cladding being 0.5 to 0.8. By making it so that the loss of the optical fiber in the wavelength range of 1550nm is less than 0.23 dB / Km, the FWM phenomenon does not occur in the DWDM region, and the slope of the optical fiber is smaller than 0.085 or less compared to the base material for the conventional non-zero dispersion Cheonah fiber To extend the range of usable wavelengths.

Hereinafter, the present invention will be described in detail with reference to the accompanying drawings.

4 shows a manufacturing process according to an embodiment of the present invention,

A first process of primary deposition in which a porous glass fine particle having a core and a cladding composition is deposited on a prepared glass rod while flame-hydrolyzing a glass raw material, to form a core soot deposit;

A second step of removing the OH group while first dehydrating the core soot deposit in a furnace containing Cl ₂ gas;

A third process of firstly sintering the core soot deposits from which the OH groups have been removed and transparent vitrification at an appropriate temperature;

A fourth process of stretching the vitrified core suot deposits to a designed outer diameter to produce a glass rod for cores,

A fifth process of secondary deposition in which a flame hydrolysis reaction is again performed on the outer peripheral portion of the glass rod for cores to deposit the cladding suits;

By the sixth process of secondary sintering the cladding soot deposits, the ratio of the distance between the primary cladding where the base material for the optical fiber is trapezoidal from the center of the core and the distance of the secondary cladding from the center of the core is 0.3 to 0.8. The zero dispersion point is below 1530 nm wavelength while the refractive index difference between core and cladding is 0.5 to 0.8.

The base material for the optical fiber formed by such a manufacturing process is as shown in Figure 5 of the glass rod seed rod 10 of the lower surface of the outer surface of SiCl ₄ , GeCl ₄ and the fuel gas H ₂ , O ₂ of the fuel gas The primary gas 12a and the secondary core are applied to the outer surface of the seed rod 10 by appropriately applying the mixed gas 14a and 14b together with the flames of the primary burner 13a and the secondary burner 13b. (12b) causes a soot deposit 12 consisting of SiO ₂ and GeO ₂ to be produced.

6 is another embodiment according to the present invention.

Fiber raw material gas from the lower outer surface of the glass rod of the seed rod 10 is SiCl _4, GeCl ₄ and the fuel gas in the gas mixture (14a), (14b), the first burner (13a) and a second burner of H _2, O _2, (13b) to properly apply the flames together, and the mixed gas (14c) of SiCl ₄ , which is an optical fiber raw material gas, and H ₂ , O ₂ , which is a fuel gas, is properly applied together with the flame by the tertiary burner 13c. the outer surface of the seed rod 10 the first core (12a) and the second core (12b) is SiO _2, is made of GeO _2, the buffer size raeding (12c) on the outer surface of the second core (12b) is SiO ₂ The soot deposition body 12 produced | generated is formed.

As shown in FIG. 7, the soot deposition body 12 produced by the present invention as described above is provided with a gas 17 of Cl ₂ or SiCl _{4 in} the core tube 15 having the heater 16 mounted on the outer surface thereof. While injecting He 10-20 L / min, Cl ₂ 300 ~ 1200 ㏄ / min, the process of the primary dehydration to remove the OH group under the conditions of 900 ~ 1400 ℃ temperature.

The primary sintering is performed to transparent vitrify the OH group-removed soot deposit 12 at a temperature of 1300 to 1900 ° C. and He 15 to 35 L / min.

The soot deposits 12 formed to a diameter of 70 mm in length are stretched to a diameter of 20 mm and a length of 500 mm using an acid / hydrogen flame to produce a glass rod 18 for cores.

The glass rod 18 for cores manufactured as described above has a mixed gas 19 of SiCl ₄ , which is an optical fiber raw material gas, and H ₂ , O ₂ , which is a fuel gas, at the bottom of the burner 13, as shown in FIG. 8. The flame is appropriately applied to allow the secondary deposition so that the cladding suit deposit 20 made of SiO ₂ is formed on the outer circumferential surface by a flame hydrolysis reaction.

In addition, the cladding suitor body 20 and the glass bar 18 for cores are secondary sintered at a temperature of 1300 to 1900 ° C. to form a base material of the optical fiber.

The loss characteristics of the optical fiber manufactured using the above base material are zero dispersion, outside the DWDM region, as shown in (a) in the graph of FIG. 3, and the slope is less than 0.085, manufactured by the present invention of FIG. As shown in the graph showing the refractive index distribution of the optical fiber, the refractive index profile of the optical fiber is trapezoidal. The profile becomes trapezoidal, and the refractive index difference △ ₁ (△ ₁ = n ₁ -n ₂ / n ₁ , n ₁ is the core refractive index and n ₂ is the cladding refractive index) between the optical fiber primary core and the cladding is 0.5 to 0.8, the refractive index difference △ ₂ (△ ₂ = n _3- n ₃ / n ₃ , n ₂ is the cladding refractive index, n ₃ is the core refractive index,) between the optical fiber secondary core and the cladding is about 0.05 ~ 0.3.

Therefore, the refractive index distribution of the non-zero dispersion optical fiber by the method for producing the non-zero dispersion transition optical fiber base material of the present invention has a length ratio of 0.3 to 0.8 with respect to the radius of the core upper base (a) and the lower base base (b) so that the profile is trapezoidal. The refractive index differences △ ₁ and △ ₂ of the optical fibers are 0.5 to 0.8 and 0.05 to 0.3, respectively, and the loss of the optical fiber is constant at 0.23 dB / Km or less in the wavelength range of 1550 nm, while the slope of the optical fiber is a conventional non-zero dispersion transition optical fiber. It is smaller than 0.085 in comparison with the base material, and the range of usable wavelengths is expanded.

Therefore, the zero-dispersion wavelength λ ₀ of the optical fiber made of such a base material is 1530 nm or less or 1560 nm or more as shown in FIG. 3A, and zero dispersion exists in the wavelength range of 1530-1560 nm, which is a wavelength division multiplexing (WDM) region. Even if three wavelengths are transmitted simultaneously, the signal can be transmitted without the Four Wavelength Mixing (FWM) phenomenon, in which a new fourth wave is generated. On the other hand, since the dispersion slope (S ₀ ) is very small, below 0.075ps / nm ² · km, it is possible to transmit a large amount of ultra-high speed information in a wide wavelength range of 1530-1620nm, thereby realizing the construction of a Dense Wavelength Division Multiplexing (DWDM) system. have.

Claims (1)

While the reaction of the glass raw material flame hydrolysis while applying the heating power of the core and greater than the porous glass fine particles for fiber raw material gas in the glass rod prepared with raeding composition of SiCl _4, GeCl ₄ and the mixed gas burner of the fuel gas, H _2, O ₂ The first process of primary deposition which deposits and forms the core soot deposit, The above-described core soot deposits are used to remove OH groups in the atmosphere containing He 10-20 L / min or Cl ₂ 300-1200 mW / min while dehydrating the primary in a furnace at 900-1400 ° C. 2 courses, A third process of primary sintering the OH group-removed core soot deposits by primary sintering at a furnace temperature of 1300 to 1900 ° C. and He 15 to 35 L / min to transparent vitrification, A fourth process of stretching the vitrified soot deposited body to a designed outer diameter to make a glass rod, The fifth secondary deposition which deposits a cladding suit by hydrolyzing the hydrolysis reaction of the mixed gas of SiCl ₄ which is an optical fiber raw material gas and H ₂ , O _{2 which} is a fuel gas, while applying a burner's flame to the outer peripheral part of the glass rod. Process, The base material of the optical fiber is produced by a sixth process of secondaryly sintering the cladding soot deposition body in a He gas atmosphere and a furnace temperature of 1300 to 1900 ° C. The optical fiber refractive index profile is trapezoidal, and the ratio (a / b) of the length in the radial direction of the trapezoidal upper base portion (a) and the lower base portion (b) is 0.3 to 0.8, and the optical fiber specific refractive index difference Δ ₁ (Δ ₁ = n ₁ -n ₂ / n ₁ , n ₁ is the core refractive index, n ₂ is the cladding refractive index) is 0.5 to 0.8, the specific refractive index difference △ ₂ (△ ₂ = n _3- n ₃ / n ₃ , n ₂ is the cladding refractive index, n ₃ is the core refractive index,) is 0.05 ~ 0.3, the zero dispersion wavelength is less than 1530nm or more than 1560nm, the zero dispersion slope is less than 0.075 ps / nm ² · km, in the 1550nm wavelength band A method for producing a base material for a non-zero dispersion transition optical fiber, which generates a base material of an optical fiber whose loss of an optical fiber is 0.23 dB / km or less.