TECHNOLOGICAL FIELD

[0001] The foi lowing disclosure relates to systems and methods for depositing chemicals onto workpieces, and the products therefrom.. More particularly, systems arsd methods for depositing silica soot on a start rod for fabricating optical fiber preforms, fused silica rods, and other optical components are disclosed.

BACKGROUND

0 j Today 's communications grade optical fiber of fused silica, S;0 is manufactured according to three basic steps: 1) core preform or "start rod ^" fabrication, 2) core-wilh~cl.ad.ding preform febricalion, and 3) fiber drawing. The core and cladding of a preform correspond m ratios and geometry to those of the ultimate glass fiber that is drawn from the preform.

[0003] The first step is to build up a start rod, forming it into a glass that will eventually become the fiber ^' s core, and in some cases, also part of the fiber's cladding layer. The start rod is a glass rod made of silica, Si0 ₂ , with the portion of the start rod that comprises the core being doped with a small amount of a dopant, typically Gerrnania, GeO?. The presence of the dopant in the core increases the refractive index of the glass material compared to the surrounding outer (cladding) layer. In the second step, a cl adding layer is built up on the start rod . The result of this step is a. preform havin g a core and a cladding, which is conventionally a.bont 160mm in diameter and about one meler long. The third slep is fiber drawing, where the preform is heated and strelehec, and typically yields about 400 km. of optical fiber.

[00Θ4] The primary raw ingredient to fabricating the glass preform, is silico tetrachloride, SiCL, which generally comes in a liquid form. As noted above, however, SK> ·. typically in the form of glass soot, is deposited on the start rod. The chemical reactions invol ved, in the formation of the glass soot are complex, involving, SiCL, oxygen, Ο.·. and the fuel gas combustion products. In all of the techniques, the silica, SiO? comprises the cla dding of the preform according, generally , to the reaction: SiCLs + 0 ₂ = Si0 ₂ + 2Ck

[0005] Generally, there are four distinct technologies for fabricating core preforms. These technologies include Modified Chemical Vapor Deposition (MCVD), Outside Vapor Deposition (OVD), Vapor Axial Deposition (VAD), and Plasma Chemical Vapor Deposition (PCVD). The resulting product for all of these technologies is generally the same: a. ''start rod" tha t is generally on the order of one meter long and 20 mm in diameter. The core is generally about 5 um in diameter.

[0006] Similarly, there are generally four technologies for performing the step of adding the cladding. These technologies include tube sleeving (concepiually paralleling MCVD), OVD soot overcladdmg (conceptually paralleling OVD), VAD soot

overcladdmg (conceptually paralleling VAD), and plasma (conceptually paralleling PCVD ). In this step, additional cladding layers of pure or substantially pure fused silica are deposited on the start rod to make a final preform that can be prepared for fiber drawing.

[0007] Irs MC VD, the step of manufacturing the start rod is performed inside of a tube. Similarly, when the cladding step is performed, a larger tube is sleeved onto and fused to the start rod. Presently, the company, Heraeus, ma ufactures tubes used for producing start rods and for sleeving onto arsd fusing with the start rods to make preforms.

[0008] In OVD, when fabr cat ng start rods, glass is deposited onto a rotating mandrel in a "soof ^* deposition process. The start rod is slowly built up by first depositing the gennaniu -doped core, and then the pure silica layers. When the core deposition is completed, typically the mandrel is removed and then the remaining body is sintered into a start rod of glass.

[00091 fo foe process of OVD soot overcladdmg, where a cladding is deposited onto a. fabricated start rod, the start rod is rotating and traversing on a. lathe such that many thin layers of soot are deposited on the rod in a stream from a chemical deposition burner over a period of time. Although the SiO? is not deposited onto the start rod as a vapor, but rather as SiO · particles, the process is known in the art as a "chemical vapor deposition ^{1 *} process because the SiCi ₄ , which reacts in the stream between the burner and the start rod to form Si0 ₂ , is input to the burner as a vapor. The porous preform that results from the OVD soot overciadding process typically is then sintered in a helium atmosphere at about 1500°C, into a solid, bubble-free glass blank, U.S. Patent No. 4,599,098, issued to Sarkar, whic is incorporated by reference as though fudy set forth herein, provides further background on systems and techniques for OVD and OVD soot overciadding.

[00.1.Θ] For the above-referenced technologies, typically any one of the core fabrication technologies may be combined with any one of the cladding fabrication technologies to generate a preform that may be used for dr win fiber.

{00111 In the OV D soot overciadding processes, one of the key measures of economic viability in comparison to the other available techniques is the deposition rate of the S:() · on the workpiece. For example, some companies involved in optical fiber manufacturing opt for the most cost-effective method of performing the step of overciadding the start rod in the fiber manufacturing process. With respect to this step m the process, the choice is either to purchase the cladding tiroes or to perform a deposttiou process to add the cladding.

1 In considering the different approaches, the economics often are reduced to a question of whether a particular vapor deposition system that a company is considering maximizes the deposition rate--to-cost ratio. ^" The deposition rate may be characterized, for example, by the average grams/minute of silica soot that can be deposited o ? the start rod until completion (I.e., an optical fiber preform, ready for sintering). Above a certain average deposition rate, performing the soot overciadding process is likely to be economically more attractive to the company than purchasing cladding tubes. Companies that manufacture systems for performing soot overciadding focus on achieving the highest possible deposition rates nd being cost effective, but without compromising the quality of the preform thai is produced for fiber drawing, [0013] The factors that determine a deposition system's deposition rate are the chemical vapor delivery rate and the efficiency of chemical vapor deposition onto the workpiece. With respect to vapor delivery, key issues generally revolve around continuously aud efficiently maintaining a high (e.g., greater than 200 grams/minute) delivery rate over a prolonged period (e.g., greater than 2 hours). Several methods have been described in I he prior art for supplying a hydrolyzing burner with a substantially constant flow of vaporized source material entrained in a carrier gas. For example, in U.S. Patent No. 4, 14,837 issued io B!aiikenship ("the B!aiikenship reference"), a system is described that includes several enclosed reservoirs each containing liq id for the reaction product constituent The liquids are heated io a temperature sufficient to maintain a predetermined vapor pressure within each resei oir. Metering devices are coupled to each reservoir for delivering vapors of the liquids at a controlled flow rate. ^" The respective vapors from each reseivoir are then combined before they are delivered to the burner.

0014] With respect to enhancing the deposition efficiency of Si02 on the orkpiece to improve the effective deposition rate, studies have been performed, to characterize the flow of chemical vapor from, the burners io the surface of the workpiece in the reaction chamber. One reference directed to this issue is Li, Tingye, Fiber

Fabrication, pp. 75-77, Optical Fiber Communications, (Academic Press, Inc. 1985), As discussed in. the above reference, because of the small size of the formed glass particles, momentum does not cause an impaction of the particles onto the surface of the workpiece. The small sizes of the glass particles would fend to force them to follow the gas stream around, instead of at the preform surface. Rather, the phenomenon of thermophoresis is the dominant mechanism for collection on the surface of the preform. As the hot gas stream and glass particles travel around, the workpiece, a thermal gradient is established near the surface of the preform. Preferably, the thermal gradient is steep, effectively pulling the glass particles by a therrnophoretic force towards the preform..

[0015] Various methods have been proposed to increase deposition efficiency based on establishing and maintaining the thermophoretic force. One method is to vary the distance between the burner and the workpiece. See H. C, Tsai, R. Greif and S. Job, "A Study of Therrnophoretic Transport In a Reacting Flow With Application To Externa! Chemical Vapor Deposition Processes," Int. J. Heat Mass Transfer, v. 38, pp. 1901-1910 (1995). Another set of methods, disclosed in US Patent Nos, 6,789,401, 7,451,623 and 7,451 ,624 issued to Dabby et a!., which are i corporated herein by reference as though ful ly set forth, herein, involves selectively translating the burners relative to the workpiece above various threshold velocities, e.g., greater than 1.4 meters per minute. Higher velocities mean that less heat is applied to any given spot on the workpiece, ^" The workpiece is therefore kept cooler, which tends to increase the thermal gradient.

Nevertheless, even applying these methods, demand for even higher deposition rates has gone unmet,

[0016] To further increase deposition rate, s me have suggested providing an array of numerous soot-depositing burners. These additional burners are proposed to be positioned for example, on a burner block along the longitudinal axis of the lathe, where each burner deposits chemical soot on the workpiece. Specifically, U.S. Patent No.

6,047,564 issued to Schaper et ah, and incorporated herein by reference as though ml ly set forth herein, discloses a vapor deposition system in which a row of twelve equally- spaced chemical burners is mounted on a burner block, each such burner depositing soot. ^' The barrier block moves forward arid backward along the longitudinal axis of the workpiece. The amplitude of the motion of the burner block general ly corresponds to the distance between the burners such that each burner is deposits soot on a designated segment of the entire workpiece.

(00.1.7] Similarly, U.S. Patent Nos. 5,116,400 and 5,21 1 ,732 issued to Abbott et al. nd incorporated herein by reference as though fully set forth herein, disclose a deposition system comprising an array of chemical burners. Like in the Schaper et al . patent, the Abbott et al. patents disclose a deposition process in which each burner in the chemical burner array deposits soot on only portion of the usabl e length of the preform, ^' The Abbott patents disclose an array of eleven burners preferably equally spaced from, each other by about four inches. The burner array is oscillated through a total distance 2,1, with a distance J in each directio f m the burner array's center position. he Abbott el al. patents disclose that preferably the oscillation amplitude is equal to or slightly greater than the burner spacing d in order to insure uniformity of deposition.

Accordingly, each burner traverses approximately 20% of the length of the preform. In discussing varying the number of burners and their spacing to improve deposition efficiency, the Abbott et al, patents disclose that for its con iguration, deposition efficiency should improve as the number of burners is increased.

[0018] Such, multiple burner configurations as disclosed in the Schaper et al. and

Abbott et al. patents are not commercially attractive in part because anticipated improvements in deposition rate have not beers realized. The close proximity of the chemical burners to each other compromises the theniiophoretie effect such that the deposition efficiency significantly reduced . The close proximity of chemical barriers positioned over the length of a workpiece prevents regions of the workpiece from having sufficient time to cool before another burner is delivering soot on that same region. Furthermore, the amount of heat and number of chemical streams generated in the chamber caused by having a. large number of burners depositing soot compromises die desired laminar flow around the workpiece, which thereby reduces the needed thermal gradient for therrnophoresis to occur. Without the optimal temperature gradient between a burner arid the workpiece, thermophoresis is weakened, which reduces the deposition efficiency, and thereby, the overall deposition rate,

[0019] The costs associated with such multiple burner configurations are also prohibitive. These costs include not only the costs associated with the additional chemical burners, but the costs of the vaporizers, preheaters and other equipment needed to support them, as well as the scrubbers and other equipment needed io handle the additional wasted deposition material and heat that the burners produce. Furthennore, because these burner configurations require vast amounts of chemtcal to achieve acceptable deposition rates, the cost of Ihe chemical needed to manufacture each preform is increased. These multiple-burner configurations can therefore be fairly characterized as "brute force" approaches that are unduly wasteful of material and unnecessarily expensive.

[0020] As a result, a need exists for systems and methods that offer f rther improvements to deposition efficiency, chemical delivery and, thereby, the overall deposition rate of chemical vapor. A need f rther exists for systems and methods that offer cost effective manufacturing of optical fiber preforms, including the manufacture of larger preforms in the same deposition space, and accordingly, cost-effective optical fiber. A need further exists for multiple-burner configurations in chemical vapor deposition systems and processes that maintain the necessary thermophoresis to provide higher deposition rates and efficiencies. SUMMARY OF THE DISCLOSURE

[00211 The following disclosure generally provides, in one aspect, systems and methods for enhancing the effective deposition rate of chemicals onto a workpiece, such as the deposition of Si0 ₂ from a Si<¾ vapor onto a start rod for making a preform usable for drawing into optical fiber.

[0022] In a second separate aspect as described herein, systems and methods for manufacturing pure fused silica, optica! fiber preforms, silica tubes, optical fiber, and silica rods, including fused silica rods, are disclosed.

[0023] In a third separate aspect as described herein, a deposition system for depositing silica particles onto a workpiece includes a first set of burners for depositing silica particles onto a first portion of the workpiece, a second set of burners for depositing silica particles onto a second portion of the workpiece, and a lathe for holding the workpiece and for rotating the workpiece relative to the first and second sets of burners. The first and second portions of the workpiece overlap each other to form an overlap segment. Preferably, the longest distance between deposition burners within any set of two proximate burners is less than the shortest distance between burners in different sets, [0024] In a fourth separate aspect as described herein, a method of manufacturing optical fiber includes the steps of obtaining a start rod, and depositing fused silica on the start rod to produce an optical fiber preform. The depositing step includes steps of depositing silica on a first portion of the start rod using a first pair of burners separated from each other by a distance of about d, and. depositing silica on a second portion of the start rod using a second pair of burners separated from each other by a distance of about d. The first and second portions overlap each other and the overlap preferably has a width of about d. Furthermore, the first pair and second pair of burners are preferably separated by a distance T, where T is preferably greater than three times d.

[0025] In a fifth separate aspect as described herein, a deposition system for depositing silica particles onto a workpiece includes a first set of burners for depositing silica particles onto a first portion of the workpiece, a second set of burners for deposking silica particles onto a second portion of the workpiece, a third set of burners for depositing silica particles onto a third portion of the workpiece, and a lathe for holding the workpiece and for rotating the workpiece relative to the first, second and third sets of burners. The first and second portions of the workpiece preferably overlap each other to form a first overlap segment, onto which one burner from the first set burners and a second burner from, the second set of burners substantially deposits silica particles. Similarly, the second and third portions of the workpiece preferably overlap each other to form a second overlap segment onto which one burner from each of the second set and third set of burners substantially deposits siiica particles. In this configuration, the furthest, distance between deposition burners within any set of burners is less than the shortest distance between burners in different sets.

[0026] in a sixth separa te aspect as described herein, a method of manufacturing optical fiber includes the steps of obtaining a start rod, and depositing fused silica on the start rod to produce an optical fiber preform. The depositing step preferably includes the steps of depositing silica on first, second and third portions of the start rod using first, second and third pairs of burners, respectively. The burners in each pair are preferably separated from each other by a distance of about d, where d is preferably greater than about 80 rnrn. The first and second portions of the start rod overlap each other and the overlap has a width of about, d, and the second and third, portions overlap each other and that overlap also has a width of about d. In ibis configuration, the shortest distance between a burner of the first pair of burners and a burner of the second pair burners is greater than d, and the shortest distance between a burner of the second pair of burners and a burner of the third pair burners is also greater than d.

[0027] Further embodiments as well as modifications, variations and

enhancements are also described herein.

BRIEF DESCRIPTION OF THE DRAWINGS

[0028] FIG. 1 is a schematic diagram, of a perspective view of a re (erred embodiment of a chemical, vapor deposition system;

[0029] FIG. 2 is a funcdori-orierited diagram of a preferred embodiment of a chemical vapor deposition system;

[0030] FIG. 3 is a diagram of a functional representation of a chemical burner;

[0031 ] FIG. 4 is a schematic diagram, providing a perspective view of a preferred embodiment of a lathe, such as is generally depicted, in FIG, 2, for holding and. moving a workpiece m a chemical vapor deposition system as is depicted in FIGS. 1 and 2; {0032] FIG. 5 depicts a conventional configuration 500 of chemical burners relative to a workpiece;

[0033] FIG. 6A depicts a preferred embodiment of a niu I tip le -burner

configuration 600 in a chemical vapor deposition process;

[0034] FIG. 6B depicts another preferred embodiment of a multiple-burner configuration 600 in a chemical vapor deposition process; and

[0035] FIG. 7 is a process flow diagram illustrating a preferred embodiment of a process of performing chemical vapor deposition such as may be performed by the chemical vapor deposition system illustrated in FIG. 1 .

DETAILED DESCRIPTION OF PREFERRED EMBODIM ENTS

[0036] FIG . 1 depicts a preferred embodiment of a chemical vapor deposition system 100, usable in the manufacture of optical fiber preforms, optical fiber, pure fused silica, fused silica tubes, core preforms, silica wafers, ilica substrates and silica ingots. The chemical vapor deposition system 100 preferably includes a reaction or deposition chamber 102, and an enclosure 104 for the deposition chamber 102, a computer 106 and other electronic components, an enclosure 108 for the computer 106 and the other electronic components, a power distribution subsystem 1 10, an enclosure 1 12 for the power distribution subsystem 1 10, a gas panel 1 .14. a gas panel enclosure 1 16 and an intake and exhaust subsystem, including a main exhaust 1 18 and secondary exhausts 122, 123.

[0037] The deposition chamber 102 is structured to house a process of deposition of particles (e.g., particles of Silica soot) onto a workpiece or start rod. The deposition chamber 102 and the deposition system 100 generally may be used to produce an optical fiber preform that, in a subsequent drawing process, -nay be used to manufacture optical fiber. The deposition system 100 may also be used to manufacture fused silica rods, including pure fused silica rods. For this application, the deposition system 100 generally applies sihca sooi to an initial start rod of substantially pure fused Silica, The product of this deposition process, a pure fused silica preform, is then sintered to form the pure fused silica rod and may be used to manufacture (e.g., by drawing, slicing or otherwise reforming the pure fused silica rod) silica wafers or substrates, multi-mode optical fiber, and other optical components for a variety of applications. {0038} The other subsystems arid components of the deposition chamber 102 are generally provided to su port, the deposition process. In one embodiment, deposition material generally comprising a vapor of silicon tetrachloride (SIC14) ami oxygen (02) is emitted from a chemical burner in a, process of fabricating optical fiber preforms in a deposition region 146 of ihe deposition chamber 102, in the deposition region 146 are the chemical burner, a chemical stream from the burner, and. the workpiece, where the stream is directed towards the workpiece from the burner. The burner also preferably issues and ignites streams of hydrogen and oxygen. The resulting flame heats the chemical constituents to temperatures generally exceeding about 1000 °C. A. chemical reaction with the hydrogen, oxygen and SiC14 occurs in the stream, in which the SiG4 in the stream is oxidized producing particles of silicon dioxide (that are then deposited on the workpiece) and a. byproduct of hydrogen chloride (FIG). Optionally, methane may be used to generate the hear necessary in the deposition chamber 102, and octamethyl silica and siiane (octomethycyciotetrasiloxane) for a source of silicon to produce silicon dioxide,

[0039] The deposition chamber 102 preferably provides a laminar flow of air in the deposition region around the workpiece. The provided laminar flow preferably assists in maintaining a hocused stream, of heat and chemical vapor from the burner towards the workpiece. A narrow and tight stream of flame enhances the mermophoretic effect that attracts the Si0 ₂ particles to the workpiece because the Si0 ₂ particles get hotter while the surface of the workpiece remains relatively cooler,

[0040] barge quantities of oxygen (0 ₂ ) and fuel gas, typically in the form of hydrogen (H ₂ ) or natural gas, are passed through the deposition chamber 102 to enable the deposition process of converting S-C i _; into SiO? soot thai is deposited in layers onto a workpiece.

[0041 ] FIG. 2 is a diagram depicting a functional view of the chemical vapor deposition system 100 generally shown in FIG. 1 , As depicted m FIG. 2, the chemical vapor deposition system 200 preferably includes a SiCL source 202, a nitrogen (N2) source 204, an oxygen (0 ₂ ) source 206, and an 1 1 · source 208 as raw materials for the vapor deposition system 200. Alternatively, the N , 0 _2? and FL sources 204, 206, 208 may be piped in from an external location. The deposition system 200 preferably further includes a computer 2 0, a gas panel 2 12, a preheaier 214, arid a vaporizer 216 for control ling the flow of the materials used for the deposition process.

[0042] The deposition system 200 preferably includes a deposition chamber or cabinet 218, enclosing preferably four or more chemical deposition burners 220, a lathe 222 for holding a workpiece 224 nd for moving the workpiece 224 rotational !y and, optionally, translation a fly relative to the four or mote chemical burners 220, The deposition chamber 218 preferably encloses one or more end-torches (not shown) positioned near the ends of the workpiece 224. and which preferably move (or remain stationary } with, the workpiece 224. The end torches preferably direct heat to the ends of the workpiece 224 to prevent it 224 from breaking and/or cracking. Preferably, the workpiece 224 and the end torches move so that the exhaust around the chemical burner 220 is maintained relatively constant. Alternatively, the chemical barriers 220 are moving and the workpiece 224 and end torches are stationary (except for the rotation of the workpiece 224), The deposition system 200 preferably further includes an air intake and exhaust subsystem. 226 including scrubbers (not shown).

[0043] The computer 210 preferably includes electronic connections to the vaporizer 2 1 6, the gas parse! 212, and the deposition cabinet 218 for automatically controlling functions of each component. The computer 106, 210 preferably further includes a connection to a user-input device such as a keyboard, touch screen, knobs, buttons, switches, mouse and/or microphone for voice activated command, input for providing operational control of the deposition system. 200 to a. user. Moreover, the computer 210 preferably includes a user output device, such, as a display monitor or speaker for presenting a status of the system.

[0044] The raw deposition materials' sources 202, 204, 206, 208 are preferably reservoirs, which ma be commercial ly available pressurized, tanks for containing each constituent material. The SiC preferably is contained in a reservoir in liquid form, preferably at room, temperature. The S1C14 source 202 preferably is connected by a pipe or line to the preheaier 214, such that SrC14 may be conveyed as a liquid into the preheaier 214. Preferably, positioned above the SiCU source 202 is an exhaust port 203 to convey SiCl to a pollution control system (not shown) m event of a leak of SiCl from. its source 202, The preheaier 214 is connected io the vaporizer 216 for transferring the heated S1CI4 liquid out of the preheaier 214 and into the vaporizer 216,

[0045] The vaporizer 21 comprises a container for containing a substantial volume of SiCL, a heating element to heat the SR i ·. in the container, and numerous valves (not shown) to regulate the flow of materials into and out of the vaporizer 216. The vaporizer 216 is preferably electronically connected to the computer 210. Through this electronic connection, the volume of SiCL¾ in the vaporizer 216 is preferably regulated and maintained between a predetermined minimum and maximum level. The computer 210 preierably controls the flow of SiCU liquid from the SiCL source 202 to the vaporizer 216 from a solenoid valve 217. The vaporizer 216 is also preferably pneumatically connected by a line to the N-? source 204. Through control from the c m uter 210, the SiCL source 202, the preheaier 214 and the vaporizer 216 preferably provide a constant, automatic and prolonged flow of vaporized SR i ·. from the vaporizer 216 to the burners 220 in the deposition cabinet 2 1 8.

101146] The gas sources 204, 206, 208 are preferably pneumatically connected to the gas panel 212. The gas panel 212 includes valves and mass flow controllers to regulate the flow of gasses from the gas sources 204, 206, 208. Conirol of the valves in the gas panel 212 is provided by the computer 210, which is electronically connected to the gas panel 212. Lines for 0 and I I · are provided to preferably pneumatically connect the gas panel 212 and the burner 220 in the deposition cabinet 218. Further, a separate line is preferably provided to convey (32 to the line carrying the vaporized SiCL to the burner 220, Thus, at a "T" fitting 21 , the vaporized SR i ·. and O? are mixed, and continue as a mixture m their transport to the burners 220.

|0047] Accordingly, four separate lines are preferably input to the burners 220: a line conveying a mixture of vaporized SiCL; and 0 \ a. line conveying I ; · or another convenient fuel gas, a line conveying 02 for the combustion of hydrogen, and a line conveying O · to shield the SiCL and O? mixture. This configuration preferably assures at least close to the same volume of SiCL particles from each of the four chemical burners 220 at any given point in time.

[0048] F!G, 3 depicts a preferred embodiment of a burner 300 for use in the deposition system. The burner 300 preierably receives the four streams (one for each input line), aad emits preferably four streams from a burner face 302. each stream being emitted from one of at least four concentric rings 304, 306, 308, 310 of emission holes.

[0049] As the constituents are emitted from the burner 300, the fuel gas and the oxygen are ignited. The SiC!.4 particles react in the flame at a controlled distance away from the face of the burrser 300. The SiCk particles passing through the flame are oxidized to form silica soot that continue in a directed stream toward a workpiece 224 that may initial ly be in the form or a start rod.. As silica soot approaches the workpiece 224, the si lica soot has a temperature on the order of about 1 1 00 C . The chlorine is preferably separated from the other materials and combines with hydrogen to ultimately form hydrochloric fumes (HQ). These reactions generally apply to the deposition process for a cladding on an optical fiber preform. Other constituents may be used for chemical apor deposition tor other applications applying the different embodiments and aspects of the chemical vapor deposition system, described herein,

[0050] Referring again to FIG. 2, the silica soot is deposited in layers on a continuously moving workpiece 224. The workpiece 224 is mounted on the lathe 222, which preferably rotates and translates the workpiece 224 relative to the burners 220. As shown in FIG, 4, the lathe 400 preferably includes end holders 402 into which the ends of the workpiece 224 (e.g., the start rod) are inserted. The lathe 400 further includes at least one and optionall two motors 404 and 406 for moving the workpiece 224 relative to the burners 220 both rotationaliy, and optionally, translationally. The motors 404, 406 are preferably controlled by a computer 2 1 0, such as that depicted in FIG. 2, for controlling the speed of rotation and translation of the workpiece 224 throughout the course of the deposition process on the workpiece 224.

1005 ! ] In the deposition process, the translation speed of the workpiece 224 relative to the burner may alternate (e.g., velocity to the right versus to the left) between slow (e.g., I meter per rnrnute) and fast (e.g., more than rive meters per minute). The last pass may be performed so that the deposition at the end of a slow pass (e.g., at the left end portion of the workpiece), effectively resumes with a slow pass that commences at the right end-portion of the workpiece. Such a motion profile may be advantageous because at the concl usion of a slow pass to the left, the theniiophoreiic force wi ll be strongest where the workpiece is the coolest, which, in this example, would be at the right end, which has been afforded the most time to cool, A very fast pass (e.g., greater than 20 meters per minute) may be employed primarily for the purpose of quickly positioning the burners for another slow pass that starts at the coolest point on the workpiece. This approach also helps to minimize the "footballing ^' ' effect that is discussed in the Dabby et a!. patents referenced herein.

[0052] FIG. 5 depicts a conventional configuration 500 of chemical burners relative to a workpiece onto which silica soot is deposited. Two burners 502 are separated by a distance d and traverse a longitudinal path relative to a workpiece 504. The configuration a lso preferably includes torches (not shown) drat heat and solidify the ends of workpiece to prevent it from bending or cracking. The torches are distinguished from the burners, in that the torches do not typically deposit soot on the workpiece. in the deposition process, the pair of burners 502 traverses a distance T along the longitudinal length of the workpiece 504, while the workpiece is rotating on a lathe. The pair of burners 502 reaches the endpomt 503 of a traversal in one direction. Then, the pair of burners 502 returns along the essentially sarne longitudinal path in the opposite direction. Over the course of a deposition process, the endpoint 503 may vary slightly from pass to pass, to avoid producing a rippling effect on the surface of the preform. At the endpoints 503 of the traversal, a portion of the workpiece having a width of approximately d, where d is the distance between the chemical burners 502, receives deposition from one of the two burners 502 in the pair, but not both burners 502. As a result of having only one burner deposit soot onto the ends of the workpiece, any tapering of the wor kpiece at its endpoints may be amplified, as depicted by the tapered regions 506.

0053] A configuration of two burners in relatively close proximity is suitable from the standpoint of therrnophoresis because two burners so configured typically will not deposit on the same region of the workpiece. During the deposition process, because the workpiece is continuously rotating, the second burner in a pair will typically deposit on the radial side of the workpiece that opposes the side on which the first burner in the pair has deposited. Once a third close-proximity burner is added to the burner configuration, therrnophoresis is impacted because the third burner will typically generally deposit on the same region on which the first burner deposited soot. Because of the third burner's close proximity to the other two burners, that region of the preform has not yet had sufficient time to cool for thermophoresis to adequately take place.

[0054] FIG, 6A depicts a mult le-burner configuration 600 in a chemical vapor deposition process that overcomes the prior art's shortcomings of a weakened

thermophore^ e force as a result of rising three or more burners in close proxinnty to each other while providing an enhanced deposition rate through the use of additional burners. In the new multiple-burner configuration, thermophoresis is not materiall compromised, leading to enhanced deposition efficiency and greatly enhanced deposition rate, as well as a actical use of deposition material, FIG. 6A depicts a first set of chemical burners 602 and 604 and a second set of chemical burners 606 and 608. The burners in each set are preferably spaced from each other by a distance dl (e.g., 80 mm · 150 mm), and. dl is preferably the same for both sets of chemical burners. The mean distance between sets of burners is T, where T preferably is a distance (e.g., 40 cm) sufficient for thermophoresis to take place when one pair of burners deposits on a region of the preform following a deposition on that region by the other pair of burners. To establish a consistent therrnophoretie force, the distance between pairs of burners must be above a. certain threshold so that enough time elapses between depositions by the different pairs of burners. Preferably, the distance, T, between pairs of burners is generally greater than (e.g., three times) di. Jn this configuration, the distance T is also approximately equal to the distance that the burners 602, 604, 606, 608 traverse ionginidinaliy is each direction. The value of T represents only a portion of the length, L, of the workpiece 610, such that each of the two sets of burners is responsible for depositing on approximately half of the workpiece 610, In the middle of the workpiece 610, both sets of burners responsible for an overlap segment 612, with each set of burners contributing to the deposition generally in accordance with the triangles shown in FIG. 6A. In this multiple-burner configuration, L is generally equal to about 2T + d. In FIG. 6A, each portion of the workpiece 610 ibr which a set of burners is responsible is shown, purely for clarity of explanation, separately. Of course, in practice the two portions form one continuous workpiece 610.

[0055] in the deposition process, the chemical burners generally remain fixed distances fiom each other whi le they traverse the workpiece 610. For example, while chemical burners 602 and 604 traverse to the right along the left side of the workpiece 610, chemical burners 606 and 60S traverse to the right along the right half of the workpiece 610. Similarly, while chemical burners 602 and 604 traverse to the left along the left side of the workpiece 610, chemical burners 606 and 608 traverse to the left along the right half of the workpiece 610. In this manner, each set of burners do not interfere with the other set as they deposit soot on the portion of the workpiece 10 for winch each is responsible.

[0056] Irs the burner configuration depicted in FIG. 6 A, each of the four chemical burners 602, 604, 606, 608 preferably streams about the same amount of silica soot at any given point in time. Indeed, both sets of burners preferably receive chemical from the same supply, so as to help insure that both sets of burners stream the same volume of silica soot at any given time. At any givers point on the workpiece 610, generally two burners are capable of depositing silica soot on the workpiece 610, except at the ends of the workpiece 610, where at the left end-portion, only the leftmost burner 602 will deposit silica soot, and at the right end-portion, where only the rightmost burner 608 will deposit soot, tiowever, between the end-portions, two burners deposit silica soot ors the workpiece 610. At the interface of the deposition between the two sets of burners, burner 604 of the left burner set and burner 606 of the right burner set deposit Silica soot, so that even at the interface, two burners are depositing silica soot on the workpiece. Such a deposition enables the creation of a preform with generally a seamless transition between the portions of the preform formed by the depositions from each respective set of chemical burners. The result of this process is the formation of a preform, with a fully usable portion, A, as depicted in FIG, 6A between the end-portions of the workpiece 610.

[0057] FIG. 6B depicts another multiple burner configuration 640 that overcomes the prior art's shortcomings of a weakened thermophoretic force when using multiple burners. In this alternative multiple-burner configuration, thermophoresis is not compromised, which accordingly provides enhanced deposition efficiency. FIG. 6B depicts a set of chemical burners 642 and 644, a second set of chemical burners 646 and 648, and a third set of chemical burners 650 and 652. The burners in each set are preferably spaced from each other by a distance dl (e.g., 80 mm · 150 mm), and. dl is preferably the same for each set of chemical burners. The mean distance, T _s , between the first set of burners and the second set of burners is preferably the same as the mean distance, T ₂ , between the second set of burners and the third set of burners, such thai Ti ^:::: TV Also, shortest distance between burners in different sets is longer than the longest distance between deposition burners iu the same set. The parameters Ύ-. and 1 · are distances (e.g. , 30 ere ) generally significantly greater than (e.g., 3 times) d _ls and Tj and T ₂ represent only a portion of the length, L, of the workpieee 654 such thai preferably L is equal to about Vk + d; (or 3T ÷ (!■). As with the previous configuration, the longitudinal distance traveled by the burners in each direction relative to the workpieee is equal to about the mean distance between nearest sets of burners.

[0058] In the deposition process, the burners generall remain these fixed distances from each other while traversing the workpieee 654, For example, while chemical burners 642 and 644 traverse ΐο the right along the leftmost portion of the workpieee 654, chemical burners 646 and 648 traverse to the right along a middle portion of the workpieee 654 and chemical burners 650 and 652 traverse to the right along the rightmost portion of the workpieee 654. Similarly, while chemical burners 642 and 644 traverse to the left along the left side of the workpieee 654, chemical burners 646 and 648 traverse to the left along the middle portion of the workpieee 654, and chemical burners 650 and 652 traverse to the left along the rightmost portion of the workpieee 654, In this maimer, the three sets of burners do not interfere with each other while depositing on the portion of the workpieee 654 for which each set is responsible.

[0059] in this configuration, each of the six chemical burners preferably streams the same amount of si lica soot at any given time. Again, as in the previous embodiment, the three sets of burners preferably receive chemical from the same supply. At any particular point on the workpieee 654, generally two burners wi ll deposit silica soot on the workpieee 654, except at the ends of the workpieee 654, where at the left end-portion 656, only the leftmost burner 642 will deposit silica soot, and at the right end-portion 658, the rightmost burner 652 will solely deposit on that portion of the workpieee 654. However, between the end-portions, two burners deposit silica soot o the workpieee. At the interfaces 660, 662 of the deposition between each set of burners, two burners generally will deposit soot. At interface 660, burner 64 of the left burner set and burner 646 of the middle burner set deposit si lica soot, so that at the interface, two burners are depositing silica soot on the workpieee 654 , Similarly, burner 648 of the middle burner sci and bnnier 650 of the right burner set deposit silica soot, so that at that interface 662, two burners are depositing silica soot on the workpiece 654. Such a deposition enables the creation of a preform with generally a seamless transition between the portions of the preform formed by the depositions from each respective set of chemical burners. The result of tins process is the formation of a preform with a fully usable portion A as depicted in FIG. 6B between the end-portions of the workpiece.

[006Θ] In an alternative configuration, four burners such as burners 602, 604, 606, and 606 of F!G, 6A may be used to produce a preform of length ) .. where L is equal to about 3T + di, as depicted in FIG . 6B. in this configuration, the four burners travel relative to the workpiece a distance of preferably about 2T.

[0061] In the design of a deposition system, there are different issues and constraints associated with the choice of whether the workpiece is physically translated to pass in front of stationary (or nearly stationary) burners or whether the burners are translated to pass along a stationary (or nearly stationary) workpiece. In the case of physically moving burners, serious (generally surmountable but costly) Issues exist relating to maintaining a consistent exhaust of heat and deposition material from the deposition chamber due to the fact t.hat the sources of the heat and deposition material are moving within the chamber. On the other hand, physically translating the workpiece relative to stationary burners causes the anticipated size of the workpiece and the distance of its translation within the chamber to define the minimum length of the chamber itself A longer and bigger chamber not only has a larger footprint. It Is also more expensive to manufacture. Although both alternatives have tradeoffs, manufacturers typically design the deposition chamber to provide for some amount of translation of the workpiece so as to minimize exhaust and other design issues associated with having moving deposition burners. Using the burner configura tions disclosed herein, the minimum length of the deposition chamber may be reduced, because the necessary translation distance of the workpiece is significantly reduced in comparison with conventional configurations, such as the configuration depicted in FIG. 5. For example, using the configuration of FIG . 5, a two-meter workpiece would have to be translated two meters in each direction to allow for the pair of burners 502 to deposit on the entire workpiece. As a result, the translation distance and length of the workpiece would effectively require a chamber having a length of no less than four meters.

[0062] In contrast, using the configuration of FIG. 6A having two pairs of deposition burners, a two-meter workpiece may only have to be translated one meter in each direction. The translation distance and length of the workpiece would effectively reduce the minimum length of the deposition chamber three meters. For the

configuration of FIG. 6B, which has three pairs of deposition burners, the two-meter workpiece would require a translation of approximately one half-meter in each direction. ^; he translation distance and length of the workpiece would effectively reduce the minimum length of the deposition chamber 2,5 meters. Conversely, given a

predetermined length of a deposition chamber, the maximum lengths of the preforms that can be manufactured within it are increased by Implementing the new burner

configurations disclosed herein.

[0063] i ll s. 7 depicts a preferred embodiment of a process 700 of performing chemical vapor deposition such as may be performed by the chemical vapor deposition system 100 illustrated in FIG. 1. Optionally, in a first step 702, a start rod is obtained. In the deposition process, a length lor a start rod is set. In different runs of the vapor deposition system, start rods of various lengths, preferably between about 0.8 meters and about 4 meters, may be used. Preferably, a length of a star! rod is input at an operator terminal and transmitted to a computer. The computer then communicates with components of the deposition system that o c functions dependent on the start rod length. Specifically, the lat he may be programmed according the length of the start rod that is used for a particular run of the deposition process 700. When the lathe receives the length value from the computer, the torch at one end of the lathe is preferably automatically repositioned to apply heat to one end of the rod. The other torch is preferably stationary. Furthermore, the motor controlling the translation of the rod executes a traverse motion profile tha reflects the entered length of the start rod.

[0064] In a next step 704, silica soot Is deposited in passes along a workpiece, with each of the two, three or more sets of burners (depending on the maximum possible length of the workpiece) depositing soot on respective portions of the workpiece, including the overlap segments. The first pass of depositing silica soot preferably is performed with a high flow of fuel gas arid oxygen from the chemical burner relative to the flow of SiCLj. Furthermore, on this first pass the traverse speed is relatively low (e.g., one meter per minute). The resulting high heat of the soot stream and of the workpiece on this first pass hardens the initial interracial layers between the start rod and the cladding layers that are subsequently deposited, preferably preventing interface defects and slippage of the soo t over the start rod.

[0065] During the first pass and. throughout a run of die deposition process 700, certain parameters are preferably fixed throughout the run. Specifically, the end torches at each end of the start rod provide a flame that preferably provides a souree of heat. The end torches provide heat at the ends of the workpiece to prevent the soot from cracking and to eliminate the soot slippage over the start rod during sintering, by keeping the ends denser and tightly adhered to the handle glass. The rod should be hot enough to affix the ends of the soot to a particular point on the start rod. However, if the end burners provide too much heat, then generally the start rod bends. Furthermore, to enhance die effective deposition rate, the distance between the burners / torches and the workpiece is preferably permitted, to close as the workpiece increases in diameter throughout the run. This closing of the distance between the burners / torches and the workpiece via the workpiece's natural, increase in diameter typically effectively meets the need for increasing the amount of heat applied to the workpiece due to its continuously increasing size and mass. Thus, as the workpiece increases in diameter, the chemical burners preferably remain stationary,

[0066] In the deposition process, and in accordance with the embodiments discussed herein, one set of burners deposits soot on one portion of the workpiece while at the same time another set of burners deposits on another portion of the workpiece. Throughout the deposition process, the sets of burners remain generally equidistant from each other, and indeed may be affixed to the same burner block which may perform the translation of the burners relative to the workpiece. Via such a configuration where the sets of burners are relatively distant from each other, when one burner has deposited on the overlap portion, sufficient time passes before a burner of the other set deposits on that same portion. That time allows the overlap segment to cool sufficiently to facilitate a strong thennophoretic force each time deposition is performed on that segment. 101167] Orsce the deposition process is completed to form an optical fiber preform, in a next step 706, the preform is sintered in a furnace and then drawn in a next step 708 into optical fiber, in a next step 710, a protective coating preferably comprised of aery late is applied to the drawn optical fiber, which is then preferably UV-eured to harden the coating, in a final step, the protected optical fiber is general ly placed into tubes that may hold 100 or more optica! fibers to form an optica! fiber cable that is ready for use in telecommunications applications.

100681 While preferred embodiments of the invention have been described herein, arid are further explained in the accompanying materials, many variations are possible which remain withm the concept and scope of the invention. Such variations would become clear to one of ordinary skill in the art alter inspection of the specification and the drawings. The invention therefore is not to be restricted except within the spirit and scope of any appended claims.