Patent Application
20100162769
1. Technical Field
The present invention relates to a method and an apparatus for manufacturing an optical fiber preform using a high frequency induction thermal plasma torch. The present application claims priority from a Japanese Patent Application No. 2008-333749 filed on Dec. 26, 2008, the contents of which are incorporated herein by reference.
2. Related Art
A high frequency induction thermal plasma torch is an apparatus provided with a high frequency coil on a periphery of a gas flow tube, and a high frequency current is applied to ionize the gas therein and emit the resulting plasma from a nozzle. Such a high frequency induction thermal plasma torch can achieve extremely high temperatures around 10,000 degrees, has relatively low plasma velocity, and enables free selection of oxidation and reduction atmosphere, and is therefore used as an ultra-high temperature reaction field.
An optical fiber formed by covering a pure silica glass core with a fluorine-doped silica glass cladding is more durable with regard to UV rays and radiation than a commonly used optical fiber that is formed by covering a germanium-doped silica glass core with a pure silica glass cladding. This greater durability is due to the absence of Ge—O bonding, which has low bonding energy.
Two methods that are known for providing the fluorine-doped silica glass cladding on the core glass include (1) forming a porous glass layer by depositing pure silica glass particles on the periphery of a pure silica glass rod and converting the glass particles into transparent glass in a fluorine atmosphere, as disclosed in Japanese Examined Patent Application Publication No. 4-79981, and (2) using a plasma flame on a periphery of a pure silica glass rod to directly deposit fluorine-doped silica glass, as disclosed in Japanese Examined Patent Application Publication No. 2-47414.
In method (1), the relative refractive index difference Δ is limited to less than approximately 0.7%, and so method (1) is suitable for achieving favorable throughput and providing a thick cladding layer. Method (2) has inferior throughput compared to method (1), but can acheive a relative refractive index difference Δ greater than 0.7%. Here, the relative refractive index difference Δ is defined below in Expression 1.
Δ=(ncore−nclad)/ncore Expression 1:
Here, ncore and nclad represent the refractive indices of the core and the cladding.
Method (2) is described using
Fluorine-doped glass particles are generated in the plasma flame 4, and these fluorine-doped glass particles are deposited on a surface of a glass rod 6, i.e. a target, that moves up and down while rotating in a reaction chamber 5. Exhaust gas and glass particles that are not affixed to the glass rod 6 are expelled from the system via an exhaust outlet 7. By repeatedly depositing a thin film of the fluorine-doped glass particles in this way, an optical fiber preform is manufactured having a cladding layer with a desired thickness.
Japanese Patent Application No. 2007-142423 discloses a technique that involves supplying glass particles to a glass rod 6 moving symmetrically forward and backward over a plasma torch 1, only when the glass rod 6 moves forward. The supply of glass raw material is stopped while the glass rod 6 moves backward, and the plasma temperature is lowered and then quickly returned to the original temperature. As a result, the refractive index of the cladding can be stabilized in a longitudinal direction.
The numerical aperture NA of an optical fiber obtained by heating, melting, and drawing a preform is shown below in Expression 2.
NA=(ncore2−nclad2)1/2 Expression 2:
Here, NA is a parameter representing a spread angle of light that can be received by the optical fiber, and so a higher value for NA means that the optical fiber can transmit light received from a larger range of directions. In the optical fiber formed from a pure silica core and fluorine-doped cladding dealt with here, ncore is approximately 1.457 and nclad changes according to the fluorine concentration. NA and relative refractive index difference Δ are correlated with each other, such that NA increases when the relative refractive index difference is greater.
SUMMARY
The method for manufacturing an optical fiber preform according to the present invention involves supplying a high-frequency induction thermal plasma torch with at least glass raw material, dopant raw material, and oxygen, and depositing the glass particles synthesized in the plasma flame onto a surface of a glass rod that moves backward and forward relative to the plasma torch while rotating, wherein deposition of the glass particles is performed while cooling the glass rod.
Examples of techniques for depositing the glass particles while cooling the glass rod include (i) cooling the glass rod by blowing gas on the glass rod and (ii) lowering the temperature around the glass rod by drawing a cool gas into the reaction chamber.
The apparatus for manufacturing an optical fiber preform according to the present invention comprises a rotating and hanging mechanism that hangs and rotates the glass rod in the reaction chamber, a high frequency induction thermal plasma torch that synthesizes glass particles and deposits the glass particles on the glass rod, an exhaust opening that is provided on a side facing the high frequency induction thermal plasma torch and that expels exhaust gas and unaffixed glass particles, and a cooling means that cools the glass rod during deposition.
The cooling means may be forced cooling nozzles positioned at heights above and below the plasma flame to blow a gas on the glass rod, or may be cool air induction apertures position at the top and/or bottom of the reaction chamber. It is desirable that the glass particle deposition occur with the manufacturing apparatus being oriented vertically and the glass rod hanging down inside the reaction chamber.
By depositing the glass particles while cooling the glass rod, the present invention can continuously deposit glass doped with a high concentration of fluorine to form a cladding layer having a high fluorine concentration, which improves the relative refractive index of the preform.
The summary clause does not necessarily describe all necessary features of the embodiments of the present invention. The present invention may also be a sub-combination of the features described above. The above and other features and advantages of the present invention will become more apparent from the following description of the embodiments taken in conjunction with the accompanying drawings.
Hereinafter, some embodiments of the present invention will be described. The embodiments do not limit the invention according to the claims, and all the combinations of the features described in the embodiments are not necessarily essential to means provided by aspects of the invention.
The inventors discovered that the refractive index of a glass film deposited on a glass rod is closely related to plasma power and temperature of the glass rod. In other words, as shown in
As the plasma power increases, deposition of the transparent glass becomes easier. However, the temperature of the glass rod rises after deposition, and so it is difficult to achieve high-density fluorine doping when depositing the next layer.
Therefore, the present invention is capable of continuously doping with a high fluorine concentration by performing glass particle deposition with relatively high plasma power while forcefully cooling the glass rod.
One example of forced cooling of the glass rod 6 involves providing a cooling means, as shown in
The same effect can be achieved by using a gas containing fluorine other than the silicon tetrafluoride as the dopant, such as ethane hexafluoride, sulfur hexafluoride, or the like. Even if a dopant other than fluorine is used, similar effects can be achieved as long as the indaction amount of the dopant depends on the temperature of the rod and the plasma power. Hereinafter, some embodiments and a comparative example of the present invention will be described, but the invention is not limited to these embodiments.
A fluorine-doped quartz glass layer was formed by using a high frequency induction thermal plasma torch to deposit glass particles on a quartz glass rod that has an outer diameter of 50 mm and a length of 1,100 mm and that moves up and down vertically while rotating.
The velocity of the glass rod relative to the plasma torch during forward movement was set to 75 mm/min, and the plasma torch was supplied with argon, oxygen, silicon tetrachloride, and silicon tetrafluoride. Forced cooling nozzles 8 were provided at positions opposite the upper and lower edges of the plasma torch, i.e. near the upper and lower edges of the exhaust outlet 7 provided across from the plasma torch, and each forced cooling nozzle blows room-temperature air at a rate of 30 L/min to cool the upper and lower edges of the portion undergoing deposition. The power supplied to the plasma torch 1 was set to 61 kW, which is the minimum power needed to convert the glass raw material into glass.
The velocity of the glass rod relative to the plasma torch during backward movement was set to 500 mm/min, and the plasma torch was supplied with argon and oxygen, but the silicon tetrachloride and the silicon tetrafluoride, which are the glass raw material and the fluorine source, were not supplied. The power supplied to the plasma torch 1 during the backward movement was set to 8 kW, which is the minimum power needed to safely maintain the plasma.
Under these conditions, a fluorine-doped glass layer was formed by repeated deposition over the course of 50 full trips of the glass rod backward and forward over the plasma torch. Upon analyzing the refractive index distribution of the resulting preform, the relative refractive index difference was found to be 1.62%.
The same apparatus as used in the first embodiment was used, but cool air induction apertures 9 were provided at the top and bottom of the reaction chamber 5, and each cool air induction chamber supply air cooled to 10 degrees Celsius at a rate of 200 L/min. Aside from this feature, the same process described in the First Embodiment was used to form a fluorine-doped quartz glass layer on the quartz glass rod. Upon analyzing the refractive index distribution of the resulting preform, the relative refractive index difference was found to be 1.62%.
A fluorine-doped quartz glass layer was formed by using a high frequency induction thermal plasma torch to deposit glass particles on a quartz glass rod that has an outer diameter of 50 mm and a length of 1,100 mm and that moves up and down vertically while rotating.
The velocity of the glass rod relative to the plasma torch during forward movement was set to 75 mm/min, and the plasma torch was supplied with argon, oxygen, silicon tetrachloride, and silicon tetrafluoride. The forced cooling nozzles were not provided near the upper and lower borders of the exhaust outlet 7, and room-temperature air flowed into the reaction chamber 5 from the Rip and bottom thereof at a rate of 100 L/min. The power supplied to the plasma torch was set to 61 kW, which is the minimum power needed to convert the glass raw material into glass.
The velocity of the glass rod relative to the plasma torch during backward movement was set to 500 mm/min, and the plasma torch was supplied with argon and oxygen, but the silicon tetrachloride and the silicon tetrafluoride, which are the glass raw material and the fluorine source, were not supplied. The power supplied to the plasma torch 1 during the backward movement was set to 8 kW, which is the minimum power needed to safely maintain the plasma.
Under these conditions, a fluorine-doped glass layer was formed by repeated deposition over the course of 50 full trips of the glass rod backward and forward over the plasma torch. Upon analyzing the refractive index distribution of the resulting preform, the relative refractive index difference was found to be 1.42%, which is lower than that of the First Embodiment and the Second Embodiment.
As made clear form the above, the present invention can be used to obtain an optical fiber with a large relative refractive index difference Δ.
While the embodiments of the present invention have been described, the technical scope of the invention is not limited to the above described embodiments. It is apparent to persons skilled in the art that various alterations and improvements can be added to the above-described embodiments. It is also apparent from the scope of the claims that the embodiments added with such alterations or improvements can be included in the technical scope of the invention.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2008-333749 | Dec 2008 | JP | national |
