High Bandwidth Optical Waveguides and Method of Fabrication

This invention relates to optical filament transmission media and, more particularly, to high band width optical waveguides.

Waveguides used in optical communication systems are herein referred to as optical waveguides, and are normally constructed from a transparent dielectric material, such as glass or plastic.

Gradient index optical waveguides have a radially varying composition and consequently a radially varying refractive index. Reference is made to U.S. Pat. Nos. 3,823,995 to Carpenter and 3,711,262 to Keck and Schultz as examples of gradient index optical waveguides as well as examples of formation of optical waveguides by inside vapor phase oxidation processes. Both of these patents are expressly incorporated herein by reference. The inside vapor phase oxidation processes include chemical vapor deposition, flame hydrolysis and any other processes by which vaporous material is directed into a heated tube, reacted with oxygen under the influence of heat and deposited on the inside wall surface of said tube. The material is deposited within the tube in successive layers and the tube is then removed from the heat to leave a fused blank. As will be understood, the central hole may be collapsed at the end of the deposition process, the blank may subsequently be reheated and the hole collapsed, or the hole may be collapsed during the drawing process. In any event, the blank or preform is subsequently heated and drawn into an elongated, fine strand. Inasmuch as the structure of the drawn strand or filament reflects the structure of the drawing blank or preform, it is important that the physical characteristics of the blank be carefully controlled.

As is familiar to those skilled in the art, gradient index optical waveguides commonly exhibit a higher index of refraction in the core at center thereof; and lower indices of refraction at points radially outward from the core center. The gradient index of refraction may, however, be varied continuously or discontinuously, and may exhibit a linear, parabolic, or any other desired characteristic. Information concerning the construction and use of optical waveguides may be found in "Fiber Optics Principles and Applications" by N. S. Kapany, Academic Press, 1967; "Geometrical Optics of Parabolic Index Gradient Cylindrical Lenses" by F. P. Kapron, Journal of the Optical Society of America, Vol. 60, No. 11, pages 1433-1436, November, 1970; and "Cylindrical Dielectric Waveguide Mode" by E. Snitzer, Journal of the Optical Society of America, Vol. 51, No. 5, pages 491-498, May, 1961.

In order to effect such change of the index of refraction of a blank or preform being formed by an inside vapor phase oxidation process, the chemical composition of the source materials, which, after reaction, comprise the ultimate material deposited on the inside surface of the tube, may be varied. The vapor mixture is hydrolyzed or oxidized and deposited on the inside surface of the tube and subsequently fused to form a high quality and purity glass. At the same time, one or more additional vapors can be supplied to the tube, each vapor being constituted of a chemical termed a "dopant" whose presence affects the index of refraction or other characteristics of the glass being formed.

In general, optical waveguide blanks or preforms formed by the inside vapor phase oxidation process include forming a barrier layer on the inside of the support or substrate tube prior to the deposition of the core glass with the substrate tube being the cladding. The principal function of the barrier layer is to minimize interface scattering and absorption losses by removing the core-cladding interface which would exist between deposited layers of high purity, low attenuation glasses and the substrate tube inner surface. The barrier layer is conventionally a borosilicate glass composition since doping silica, which is generally the base glass, with boron reduces the deposition temperature and thereby minimizes shrinkage of the substrate tube. Other advantages of doping silica with boron is that it reduces the refractive index of the glass and it acts as a barrier to the diffusion of hydroxyl ions, commonly referred to as hydrogen or water, from the substrate tube to the deposited core glass at the elevated processing and drawing temperatures.

It is well known that the information bandwith of an optical waveguide filament can be substantially increased by grading the index of refraction profile. The bandwidth of a graded index of refraction optical waveguide can be from about 10 to 10.sup.3 times greater than the bandwidth of a filament with an ungraded index profile. The increase in bandwidth is very dependent on the shape of the index of refraction profile.

In the prior art formation of inside vapor phase oxidation gradient index optical waveguide preforms or blanks and the subsequent glass filaments, the filaments exhibit a combination step-graded index of refraction profile which causes pulse spreading of higher order modes resulting in lower bandwidth. Such a profile is illustrated in FIG. 1 where the gradient portion is indicated by curve 10 while the stepped portion is indicated by the substantially straight vertical portion 12.

Although not known to exist in the prior art, another example of a combination step-graded index of refraction profile which is believed to cause pulse spreading of higher order modes is illustrated in FIG. 2 where the gradient portion is indicated by curve 14 while the stepped portion is indicated by step 16.

There are at least two causes of the step-graded profile illustrated in FIGS. 1 and 2. A high boron level is desired in the barrier layer for reasons discussed above. A low boron level is desired in the core to minimize Rayleigh scattering and to eliminate the infrared absorption of the B-O vibrational bands in the spectral range between 1.2 and 1.5 micrometers. The second reason for such a step-graded profile is that at the barrier layer-core interface a dopant such as GeO.sub.2 and/or P.sub.2 O.sub.5, or the like, must be introduced at a finite level set by the capability of the source material vapor delivery system. It should be noted that in the illustrations of both FIGS. 1 and 2, the index of refraction of the core at the barrier layer-core interface is higher, by value of .DELTA.n, than the index of refraction of the substrate tube material or cladding. In each example, silica is shown as the substrate tube material having an index of refraction of 1.4570, with the index of refraction at the central axis 18 and 20 of the filaments of FIGS. 1 and 2 respectively being 1.4766. As will be understood, the indices of refraction are at a wavelength of about 630 nm. for a filament having a numerical aperture of about 0.24.

Curve 48 of FIG. 13 illustrates the pulse broadening which has been observed in a typical step-graded profile made by the prior art. The tall narrow portion of the pulse is produced by the graded part of the index of refraction profile, while the wide base extending to the right is caused by the step part of the profile. The bandwidth of the filament illustrated by curve 48 of FIG. 13 has been measured to be 260 mHz for a one kilometer length.

The method of the present invention avoids formation of the step part of the profile and results in the fabrication of pure graded index of refraction profiles such as those illustrated in FIGS. 6 or 7. As shown by curve 52 of FIG. 13, a filament formed by the method of the present invention has much less broadening and a measured bandwidth of 910 mHz for a one kilometer length. The reduced pulse broadening and high bandwidth have been achieved by elimination of the step portion of the step-graded profile.

A commonly used method of fabricating, for example, GeO.sub.2 -SiO.sub.2 -B.sub.2 O.sub.3 or SiO.sub.2 -GeO.sub.2 -B.sub.2 O.sub.3 -P.sub.2 O.sub.5 core gradient index optical waveguides is illustrated in FIGS. 3 and 4 wherein the simultaneous reduction of the B.sub.2 O.sub.3 level and the introduction of finite levels of GeO.sub.2 and/or P.sub.2 O.sub.5 causes a step increase in the refractive index at the edge of the core and leads to the step-gradient profile of FIG. 1 as hereinabove described. On the other hand, the method illustrated by FIG. 5, showing the second type of undesirable step-gradientprofile illustrated in FIG. 2, results when finite levels of GeO.sub.2 and/or P.sub.2 O.sub.5 are used in the barrier layer together with B.sub.2 O.sub.3, and the amount of B.sub.2 O.sub.3 in the barrier layer is insufficient to compensate for the increase in the refractive index due to the amount of GeO.sub.2 and/or P.sub.2 O.sub.5 present. In such a situation, a step increase in the index of refraction is caused at the cladding-barrier layer interface which leads to the step-gradient index profile of FIG. 2.

As will be noted, FIGS. 3, 4 and 5 illustrate the starting source materials namely the chlorides or the like of boron, silicon, germania, and phosphorous. As will be understood these source materials, under the influence of oxygen and heat, react to produce the respective oxides. As used herein, inside vapor phase oxidation includes "chemical vapor deposition" and other vapor phase oxidation methods. The phrase "chemical vapor deposition" means the formation of deposits by chemical reactions which take place on, at, or near the deposition surface, a definition set forth on page 3 of the text "Vapor Deposition" edited by C. F. Powell et al., New York, John Wiley & Sons, Inc., 1966, which text is hereby wholly expressly incorporated by reference. Any of the procedural variations well known in the art may be employed to effect the deposition of the suitable coating of glass by the chemical vapor deposition process, such as, for example that described on page 263 of the aforementioned Powell et al. text which states: "Another means of obtaining uniform coverage which also can give high deposition efficiency, and which is especially applicable to the coating of the inside surfaces of small bore tubing, is to heat only a small portion of the tubing to the deposition temperature . . . The section heated to the deposition temperature is slowly moved over the total length of the tube or the total area to be coated." In this connection, reference is also made to U.S. Pat. No. 3,031,338 issued on Apr. 24, 1962 to R. G. Bourdeau.

Another effective means of applying coatings by vapor phase oxidation is to sinter a soot layer of the desired material applied by flame hydrolysis process similar to that described in U.S. Pat. No. 2,272,342 issued to J. F. Hyde or U.S. Pat. No. 2,326,059 issued to M. E. Nordberg, both of which patents are expressly incorporated herein by reference.

It is an object of this invention to provide a method of forming a preform for a high bandwidth gradient index optical filament, the preform itself, and the resulting optical filament.

Another object of this invention is to provide a high bandwidth gradient index optical waveguide having low signal attenuation and one which overcomes the disadvantages heretofore noted.

Briefly, according to this invention, a method of forming a preform for a high bandwidth gradient index optical filament, the preform itself, and the resulting optical filament is disclosed wherein a barrier layer is formed of a base glass, a first dopant B.sub.2 O.sub.3, and at least one other dopant which is maintained substantially constant in the barrier layer and then gradually varied during the formation of the core, the quantity of B.sub.2 O.sub.3 being maintained substantially constant in the barrier layer but gradually decreased during the formation of the core. The barrier layer is formed on the inside surface of a tubular starting member which will comprise the cladding and will be disposed between the starting member and the core, the index of refraction of the barrier layer being equal to or less than the index of refraction of the starting member; there being no step increase in the index of refraction of the barrier layer at the barrier layer-cladding interface nor of the core at the core-barrier layer interface of the optical filament.

These and additional objects, features and advantages of the present invention will become apparent to those skilled in the art from the following detailed description and the attached drawings, on which, by way of example, only the preferred embodiments of this invention are illustrated.

FIG. 1 is a graphical illustration of a prior art step-gradient index of refraction profile waveguide.

FIG. 2 is a graphical illustration of another step-gradient index of refraction profile, low bandwidth waveguide.

FIGS. 3 and 4 are graphical illustrations of the methods of prior art introduction of source vapor materials in the formation of step-gradient index of refraction profile optical waveguides.

FIG. 5 is a graphical illustration of a method of introducing source vapor materials in the formation of the step-gradient index of refraction profile waveguide of FIG. 2.

FIGS. 6 and 7 are graphical illustrations of high bandwidth gradient index optical filaments formed in accordance with the present invention.

FIG. 8 is an oblique view of an optical waveguide in accordance with this invention.

FIGS. 9 and 10 are graphical illustrations of the methods for introducing source vapor materials in the formation of high bandwidth optical filaments in accordance with the present invention.

FIG. 11 is a graphical illustration of another method of introducing source vapor materials in the formation of high bandwidth optical filaments in accordance with the present invention.

FIG. 12 is a graphical illustration of the principal mode number vs delay time of an optical waveguide formed by the present invention as compared to a waveguide of the prior art.

FIG. 13 is a graphical illustration of bandwidth represented by time vs power of an optical waveguide formed by the present invention as compared to a waveguide of the prior art.

It is to be noted that the drawings are illustrative and symbolic of the present invention and there is no intention to indicate scale or relative proportions of the elements shown therein. For purposes of simplicity, the present invention will be described in connection with the formation of high bandwidth gradient index optical waveguide preforms and the waveguides themselves wherein the base glass is silica although this invention is not intended to be limited thereto.

Two examples of high bandwidth gradient index optical filaments made from preforms or blanks formed in accordance with the present invention are illustrated by FIGS. 6 and 7. FIG. 8 illustrates a typical optical waveguide 22 formed in accordance with the present invention. Referring to FIGS. 6 and 8, gradient index of refraction core 24 is indicated in FIG. 6 by curve 26 while the barrier layer 28 is indicated by flat portion 30. The starting member or substrate tube 32, which ultimately forms the waveguide cladding, is illustrated by flat portion 34 in FIG. 6. As will be understood, the barrier layer comprises the first deposited material on the inside surface of the substrate tube and is sometimes referred to as the deposited cladding. The base glass and substrate tube material used in the description of the present invention is silica, wherefore, the index of refraction of the cladding portion illustrated in FIG. 6 is 1.4570. This is true for each of the illustrations set out in FIGS. 1, 2, 6, and 7 for purposes of simplicity of description and easy comparison. To further these aims, the index of refraction in each of these examples at the central axes 18, 20, 36 and 38 of the optical waveguides of FIGS. 1, 2, 6 and 7 respectively is approximately 1.4766, while the barrier layer thickness "b" of each is approximately 1 micrometer and the core radius "a" is approximately 31.25 micrometers.

The method of forming a preform or blank of the present invention as well as the optical filament itself may be any of various methods, such as for example, those described in the heretofore noted U.S. Pat. Nos. 3,823,995 and 3,711,262 which patents are hereby expressly incorporated by reference. Any other methods of forming gradient index optical waveguides are also suitable for the purpose of the present invention.

Referring to FIGS. 9 and 10, there are illustrated two methods of forming the high bandwidth gradient index optical waveguide of FIG. 6. As will be noted, FIGS. 9 and 10 illustrate the starting source materials, namely the chlorides or the like, of boron, silicon, phosphorous, and germania, which under the influence of oxygen and heat, react to produce the respective oxides. The base glass illustrated in FIGS. 9 and 10 is silica to which is added B.sub.2 O.sub.3, and GeO.sub.2 and/or P.sub.2 O.sub.5. The starting member or substrate in each example is silica.

The barrier layer is formed by applying a plurality of layers of materials to the inside surface of the substrate tube, the composition of the barrier layer being substantially uniform throughout having a substantially constant proportion of silica, B.sub.2 O.sub.3, and GeO.sub.2 and/or P.sub.2 O.sub.5. As illustrated in FIG. 9, the levels of B.sub.2 O.sub.3 and GeO.sub.2 in the barrier layer are maintained at levels whereby the barrier layer index of refraction is less than that of silica as shown by flat portion 30 of FIG. 6. Specifically, the index of refraction of the barrier layer in the example illustrated in FIG. 6 is from approximately 0.002 to 0.010 lower than the index of refraction of the cladding. To obtain the gradient index core as illustrated by curve 26 of FIG. 6, the amount of B.sub.2 O.sub.3 in the core material composition deposited over the barrier layer is gradually decreased as each successive layer of core material is deposited, while the amount of GeO.sub.2 in the core composition is gradually increased in each successive layer. As will be understood, the core may be formed by the application of a plurality of layers of core material until the desired thickness of the core layer is achieved.

Since the barrier layer and the core each contain B.sub.2 O.sub.3 and GeO.sub.2 and there is no abrupt change in the amounts of these dopants, nor the abrupt introduction of a new dopant as the core is formed over the barrier layer, the resultant waveguide profile as illustrated in FIG. 6 does not have the step-gradient index profile of prior art waveguides. It will be understood that the change in the quantity of B.sub.2 O.sub.3 and GeO.sub.2 within the core thickness is programmed in a predetermined manner so as to obtain a predetermined desired cross-sectional profile of the ultimate optical waveguide.

A second example of a method of forming the waveguide illustrated in FIG. 6 is shown in FIG. 10. In this example, the base glass is silica and the barrier layer contains B.sub.2 O.sub.3, GeO.sub.2, and P.sub.2 O.sub.5 in constant amounts throughout the thickness of the barrier layer. These same three dopants are contained in the core with the GeO.sub.2 and P.sub.2 O.sub.5 constituents increasing from the barrier layer-core interface towards the center of the core, while the amount of B.sub.2 O.sub.3 decreases from said interface towards the center of the core. The proportion of the silica base glass is substantially constant throughout the barrier layer and core thicknesses. As described in connection with the example of FIG. 9, the respective dopant levels are programmed to provide a predetermined change in index of refraction within the core so as to produce a predetermined index of refraction profile as illustrated in FIG. 6. As is evident from the profile indicated in FIG. 6, the process illustrated by FIG. 10 produces a high bandwidth gradient index optical filament without a step-gradient index profile.

Referring to FIG. 11, there is illustrated a method of forming the high bandwidth gradient index optical waveguide of FIG. 7. Referring additionally to FIG. 8, gradient index of refraction core 24 is indicated in FIG. 7 by curve 40, while the barrier layer 28 is indicated by flat portion 42. The starting member or substrate tube 32, which ultimately forms the waveguide cladding, is illustrated by flat portion 44 in FIG. 7. As illustrated in FIG. 11, the levels of B.sub.2 O.sub.3 and GeO.sub.2 in the barrier layer are maintained at levels whereby the barrier layer index of refraction is substantially equal to that of silica as shown by flat portion 42 of FIG. 7. To obtain the gradient index core as illustrated by curve 40 of FIG. 7, the amount of B.sub.2 O.sub.3 in the core material composition deposited over the barrier layer is gradually decreased as each successive layer of core material is deposited, while the amount of GeO.sub.2 in the core composition is gradually increased in each successive layer. As will be understood, the core may be formed by the application of a plurality of layers of core material until the desired thickness of the core layer is achieved. Since the barrier layer and the core each contain B.sub.2 O.sub.3 and GeO.sub.2 and there is no abrupt change in the amounts of these dopants, nor the abrupt introduction of a new dopant as the core is formed over the barrier layer, the resultant waveguide profile as illustrated in FIG. 7 does not have the step-gradient index profile of prior art waveguides. It will be understood that the change in the quantity of B.sub.2 O.sub.3 and GeO.sub.2 within the core thickness is programmed in a predetermined manner so as to obtain a predetermined desired cross-sectional profile of the ultimate optical waveguide. It will also be understood that although the method illustrated by FIGS. 9, 10 and 11 to produce the optical waveguides of FIGS. 6 and 7 have been described in connection with B.sub.2 O.sub.3, P.sub.2 O.sub.5 and GeO.sub.2 as dopants, other dopants or combinations thereof may be used. When other dopants or combinations thereof are used, the amounts of each must be properly programmed, as will be understood, so as to obtain a predetermined desired cross-sectional profile.

For a better understanding of the advantages produced by the present invention, reference is made to FIGS. 12 and 13. Curve 46 in FIG. 12 and curve 48 in FIG. 13 represent prior art data of an optical waveguide of the prior art such as is represented by FIG. 1, while curves 50 of FIG. 12 and 52 of FIG. 13 represent data of an optical waveguide of the present invention such as is represented by FIG. 6. Referring first to FIG. 12, the delay time in nanoseconds per kilometer is shown as a function of the principal mode number (m) for optical waveguides whose measured data is represented by curves 46 and 50. As additional information for better understanding of the representation of FIG. 12, reference is made to an article entitled "Differential Mode Attenuation in Graded-Index Optical Waveguides" by Robert Olshanksy, published at page 423 of the Technical Digest of the 1977 International Conference on Integrated Optics and Optical Fiber Communications, Tokyo, Japan, which article is hereby expressly incorporated by reference. The principal mode number "m" is related to the launch position "r" of a laser spot at the input end of a fiber by the equation

where "a" is the core radius and "M" is the maximum value of the principal mode number, given by

where "n.sub.1 " is the on-axis index of refraction, "k" is equal to 2.pi./.lambda., .lambda. is the free space wavelength (799 nm for the data shown in FIG. 12), "n.sub.2 " is the index of refraction of the cladding, and .DELTA. equals (n.sub.1 -n.sub.2)/(n.sub.1).

Because of the step in the index of refraction profile at the core-barrier layer interface of the waveguide represented by FIG. 1, a large delay time shift results for high order modes transmitted through such a waveguide and consequently a large rms pulse width of 0.69 ns is produced as seen from curve 46 of FIG. 12. When the index of refraction profile shape is corrected according to the present invention as represented by FIG. 6, the delay shift as shown by curve 46 of FIG. 12 is eliminated as demonstrated by curve 50. It is seen that the pulse broadening as represented by the curve 50 of FIG. 12 is reduced to 0.21 ns.

Referring additionally to FIG. 13 where curve 48 represents data of the prior art optical waveguide illustrated by FIG. 1, the pulse width ".pi." of 0.69 ns is mathematically translated to a bandwidth of 0.28 GHz. The measured bandwidth was 260 mHz. On the other hand, the optical waveguide of the present invention of FIG. 6 represented by curve 50 of FIG. 12 and curve 52 of FIG. 13 having a pulse width ".pi." of 0.21 ns is mathematically translated to a bandwidth of 0.95 GHz. The measured bandwidth was 910 mHz.

For comparison and informational purposes, the chemical vapor deposition process data represented by FIGS. 3 and 4 which produced optical waveguides of the prior art represented by FIG. 1, and the calculated process data represented by FIG. 5 which is believed to produce an optical waveguide represented by FIG. 2, is set out in Table I, following. The data of the example of FIGS. 1 and 4 is illustrated by curve 46 of FIG. 12 and curve 48 of FIG. 13.

For each of the examples of Table I the excess oxygen is 1000 scc/min, temperature is 1750.degree. C. and the transverse rate of layer application is 15 cm/min for both the barrier layer and core; the barrier layer is formed by 3 passes or layers while the core is formed by 60 passes or layers. The resulting optical waveguides has an outside diameter of about 125 micrometers, a core diameter of about 62.5 micrometers, and a barrier layer thickness of about 1 micrometer, although the barrier layer may range from about 1 to 10 micrometers if desired.

The following is a typical example of producing an optical waveguide having a profile as illustrated in FIG. 6 and produced by the method represented in FIG. 10 of the present invention. A silica substrate tube having an outside diameter of 25 millimeters and a wall thickness of 1.275 millimeters is mounted in a deposition lathe. The constituent reactants SiCl.sub.4, GeCl.sub.4, POCl.sub.3, and BCl.sub.3 were delivered to the substrate tube by a chemical vapor deposition system well known to one familiar with the art, specifically, reference is made in this regard to the teaching of the Aslami application noted heretofore, Application Ser. No. 855,215 by M. G. Blankenship which is incorporated herein by reference, and copending patent application entitled "Method of Making Large Diameter Optical Waveguide Preforms" by A. Sarkar, Ser. No. 913,754, which copending application is also incorporated herein by reference. The parameters of the process of this example are set out in Table II following.

For the example of Table II the excess oxygen provided was about 1000 scc/min, the forming temperature was about 1750.degree. C., and the transverse rate of layer application was about 15 cm/min for both the barrier layer and core; the barrier layer was formed by 3 passes or layers while the core was formed by 60 passes or layers.

The blank or preform so formed was then heated to a temperature of about 2200.degree. C., rotated at a speed of 60-90 rpm, and the central hole was collapsed to form a solid preform. The solid preform was then mounted in a drawing apparatus as well known in the art, the end thereof heated to a temperature of about 2000.degree. C. and drawn into an optical waveguide filament having the cross-sectional profile as illustrated in FIG. 6 and data as illustrated by curve 50 of FIG. 12 and curve 52 of FIG. 13. The resulting optical waveguide had an outside diameter of about 125 micrometers, a core diameter of about 62.5 micrometers, and a barrier layer thickness of about 1 micrometer.

The following is another typical example of producing an optical waveguide of the present invention having a profile as illustrated in FIG. 6 and produced by the method represented by FIG. 9. A silica substrate tube having an outside diameter of 25 millimeters and a wall thickness of 1.275 millimeters is mounted in a deposition lathe. The constituent reactants SiCl.sub.4, GeCl.sub.4, and BCl.sub.3 are delivered to the substrate tube by a chemical vapor deposition system well known to one familiar with the art as described in the previous example. The mathematically calculated and estimated parameters of the process of this example are set out in Table III following.

For the example of Table III the excess oxygen provided is about 1000 scc/min, the forming temperature is about 1750.degree. C., and the transverse rate of layer application is about 15 cm/min for both the barrier layer and core; the barrier layer being formed by 3 passes or layers while the core is formed by 60 passes or layers.

The blank or preform so formed is then heated to a temperature of about 2200.degree. C., rotated at a speed of 60-90 rpm, and the central hole is collapsed to form a solid preform. The solid preform is then mounted in a drawing apparatus as well known in the art, the end thereof heated to a temperature of about 2000.degree. C. and drawn into an optical waveguide filament having the cross-sectional profile similar to that illustrated in FIG. 6.

The resulting optical waveguide of this example should have an outside diameter of about 125 micrometers, a core diameter of about 32.5 micrometers, and a barrier layer thickness of about 1 micrometer.

Still another example of the present invention employs the same delivery system and chemical vapor deposition lathe as described in connection with the previous examples. A silica tube having a 25 millimeter outside diameter and a 1.275 millimeter wall thickness is provided and mounted in said lathe. The method parameters for forming an optical waveguide having an index of refraction profile as illustrated in FIG. 7 by the process illustrated by FIG. 11 have been mathematically calculated and estimated to be as set out in Table IV following.

For the example of Table IV the excess oxygen provided is about 1000 scc/min, the forming temperature is about 1750.degree. C., and the transverse rate of layer application is about 15 cm/min for both the barrier layer and core; the barrier layer being formed by 3 passes or layers while the core is formed by 60 passes or layers.

After the preform or blank is fabricated as heretofore described, it is heated to a temperature of about 2200.degree. C., rotated at a speed of 60-90 rpm, and the central hole is collapsed to form a solid preform. The article so formed is subsequently placed in a drawing apparatus known to one familiar with the art, the end thereof heated and a fiber having an outside diameter of about 125 micrometers, a core diameter of about 62.5 micrometers, and a barrier layer thickness of about 1 micrometer is drawn in a manner well known in the art. The waveguide so formed should have an index of refraction profile as illustrated by FIG. 7.

As will be understood, the central hole of any of the waveguide preforms or blanks of the preceding examples may be collapsed at the end of the deposition process as described, or the blank may be subsequently reheated and the hole collapsed, or the hole may be collapsed during the drawing process as desired.

Although the present invention has been described with respect to specific details of certain embodiments thereof, it is not intended that such details be limitations upon the scope of the invention except insofar as set forth in the following claims.