In the reactive deposition of the core material from a gas which is passed through the tube onto the inner wall of the tube by means of a plasma zone, while a relative motion is effected in the axial direction between the tube and a plasma-producing device, the rate of precipitation is increased without impairing the quality of the core material coat, the reactive deposition being effected at a pressure of from 1 to 100 Torr and a temperature zone being superimposed on the plasma zone.
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1. A method of producing internally coated glass tubes for drawing fiber optic light conductors which consists of a core and a jacket of glasses which have a mutually different refractive index, comprising the steps of introducing into a glass tube surrounded by a resonator a reactive gas mixture consisting of SiCl4 and oxygen at a pressure of about 1 to 100 Torr, adding GeCl4 to the gas mixture moving the tube relative to the resonator to form a non-isothermal plasma zone within the tube, and heating the tube to a temperature between 800°C-1200° C. to form a coating free of soot-like particles and consisting of a plurality of layers of sio2 doped with an increasing content of geo2.
2. A method as claimed in
3. A method as claimed in
4. A method of producing internally coated glass tubes, for drawing fibre-optic light conductors which consist of a core and a jacket of glasses which have a mutually different refractive index, comprising the steps of introducing into a glass tube surrounded by a resonator a reactive gas mixture comprising SiCl4 and oxygen at a pressure of about 1 to 100 Torr, moving the tube relative to the resonator 2 and heating the tube to a temperature between 800°C-1200°C while activating the resonator to form a nonisothermal plasma zone within the tube, whereby a coating free of soot-like particles and consisting of a plurality of layers of sio2 is formed. 5. A method of producing internally coated glass tubes, as claimed in
A method of producing internally coated glass tubes, as claimed in claim 9, wherein the dopant-forming compound is added to the gas mixture at an increasing rate. 9. A method of producing internally coated glass tubes, as claimed in claim 5 or 6 wherein the dopant-forming compound is added to the gas mixture at a varying rate. 10. A method of producing internally coated glass tubes, as claimed in claim 9, wherein the dopant-forming compound is added to the gas mixture at a decreasing rate. 11. A method of producing internally coated glass tubes, as claimed in claim 9, wherein the dopant-forming compound is added to the gas mixture at a rate which will produce a coating whose index of refraction increases toward a central axis of the tube. 12. A method of producing coatings on walls of glass comprising the steps of: contacting at least a portion of the wall of the glass with a mixture of a gaseous glass-forming compound and gaseous oxygen at a pressure of about 1 to 100 Torr; forming a plasma zone in the gas mixture in contact with the glass wall portion; heating the glass wall portion, to a temperature which is above the temperature necessary to produce substantially stress-free coating layers on the heated tube wall portion but which is below the temperature at which there is substantial reaction of the mixture in the gas phase, to produce a nonisothermal plasma zone; and thereby causing a heterogeneous reaction to occur on the glass wall resulting in the deposit on the glass wall of a glass coating. 13. A method as claimed in claim 12, characterized in that the glass wall is in the form of a tube and further comprising the step of causing relative movement between the plasma zone and the tube. 14. A method as claimed in claim 13, characterized in that the coating and the gas mixture are on the inside of the tube, and the glass-forming compound is a silicon tetrahalide. 15. A method as claimed in claim 14, characterized in that the tube is heated to a temperature which is not greater than 1200°C and not below 800°C 16. A method as claimed in claim 15, characterized in that the plasma is formed by means of a high frequency field or a microware resonator. 17. A method as claimed in claim 16, characterized in that a dopant-forming compound is added to the gas mixture. 18. A method of producing a fiber-optic light conductor comprising the steps of: producing an internally coated glass tube as claimed in claim 17; and drawing the internally coated glass tube to form a a fiber-optic light conductor. |
This is a continuation of application Ser. No. 610,570, filed Sept. 5, 1975, now abandoned.
The invention relates to a method for producing internally coated glass tubes, consisting of a core and a jacket of glasses which have a mutually different refractive index, by means of a reactive deposition of the coating from a gas mixture which is passed through the tube and which is brought to reaction in the tube.
The tubes produced in this manner are heated to a temperature which is suitable for drawing and thereafter drawn to such an extent that the diameter is reduced until the coating is brought to coincidence and a light conductor of the required diameter is obtained.
Light conductors consist of a light-conducting core which is embedded in a jacket of a lower refractive index. The core may, for example, consist of quartz glass which has been doped with a few percent of a metal oxide which increases the refractive index and the jacket of undoped quartz glass.
For the doping of the core glass TiO2, GeO2 and Al2 O3 may, for example, be used. In the so-called self-focussing fibre optic light conductors a parabolic change in the refractive index across the radius is obtained by means of a continuous change in the grades of doping. According to a known method such internally coated quartz glass tubes are produced in which gaseous SiCl4 and oxygen or a mixture of SiCl4, TiCl4 and oxygen are passed through a tube brought there to reaction in the gas phase by means of high frequency energization and probably precipitated at least partly as a soot-like glass coat, which must thereafter be melted or sintered. There is a danger that gases are trapped which later on might form light-scattering centers. The heat treatment makes the formation of a doping profile as required for self-focussing fibre optic light conductors difficult, owing to blurring due to diffusion.
The tube may consist of non-doped quartz glass. In this method a uniform relative motion in . The resonator 3 was moved forward and backward along the tube in this test at 60 cm/min.
A mixture of 0.4 volume % AlCl3, 4 volume % SiCl4 and .Badd.95.6 volume % oxygen was passed through the quartz tube at a throughput of 42 scm3 per minute (length and diameter as in Example I). The pressure in the tube 1 was 15 Torr. The wall temperature of the tube 1 was kept at 950°C A plasma 4 as in Example I was produced. (Power 180 W, frequency 2.45 GHz). The reaction efficiency was approximately 100%. The tube was passed through the device 2-3 at a speed of 60 cm per minute while the resonator 3 was moved forward and backward along the tube 1. A homogeneous, adhering coat 5 was obtained. The total thickness of the coating was 150 μm.
FIG. 2 shows the total attenuation in dB per km as a function of the wavelength in micrometer of a fiber optic light conductor which was obtained by drawing at 1900°C of an internally coated tube according to Example II. The core diameter was 25 μm and the fiber diameter was 100 μm. The difference in the refractive indexes were approximately 5 o/oo.
By means of the method according to the invention a coating profile which has a certain refractive index in proportion to the doping can be obtained as shown above at a progressive change of the doping share. When a suitable profile is chosen the tube forms in an ideal manner a basic product for the production of monomode, multimode and self-focussing fiber optics.
Dopant-forming compounds which may be used in the method according to the invention are, for example, GeCl4, TiCl4, and AlCl3 which oxidize to form the dopants GeO2, TiO2, and Al2 O3, respectively.
Rehder, Ludwig, Kuppers, Dieter, Lydtin, Hans
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