Optical fiber with a radially varying index of refraction and related methods

Information

  • Patent Grant
  • 6807350
  • Patent Number
    6,807,350
  • Date Filed
    Wednesday, May 15, 2002
    22 years ago
  • Date Issued
    Tuesday, October 19, 2004
    20 years ago
Abstract
An optical fiber has a core with a diameter dc and a reflective index nc; a primary cladding concentrically surrounding the core and having an outer diameter dpc and a refractive index npc less than the core refractive index nc; and a secondary cladding concentrically surrounding the primary cladding and having an outer diameter dsc and a refractive index nsc less than the primary cladding refractive index npc.
Description




FIELD OF THE INVENTION




The invention relates generally to optical fibers and more specifically to optical fibers with a controlled refractive index profile.




BACKGROUND OF THE INVENTION




Beam splitters and combiners are widely used today in optical communications systems. Optical splitters divide a single light beam into a plurality of light beams. Conversely, combiners take a plurality of light beams and combine them into a fewer number of beams (e.g. eight to one). Combiners and splitters generally introduce two losses into the overall system performance, “insertion loss” and “excess loss.” Insertion loss is the loss in a transmission line that results from inserting (i.e., introducing) the component in the transmission line (e.g., a 3 dB 2×2 coupler inserted into a line will introduce a 50% or 3 dB loss in the line). Excess loss is the internal loss attributable to the specific component itself.




Excess loss arises, for example, from fiber fusion and/or tapering of the fiber, and is generally related to the number of splits or combinations of fibers made in the component. (Fusion refers to localized heating and softening of two or more fibers to attach them together; tapering relates to reduction in the size of the fiber geometry, e.g., as a result of fusion or polishing.) For example, an 8-to-1 splitter will generally have a higher excess loss than a 4-to-1 splitter designed for the same operation band, with the same fibers. Fibers can be joined by means of cladding-fused and cladding-polished couplers.




With reference to

FIG. 1

, a typical single mode optical fiber


100


used to create either a cladding-polished or cladding-fused coupler includes a core


110


and a cladding


120


. In a cladding-fused coupler, shown in

FIG. 2

, the claddings of two single mode fibers


100




a


,


100




b


are fused together, thereby fixing cores


110




a


,


110




b


in close proximity to each other at the region of joinder. Cross-talk between cores


110




a


,


100




b


results in transfer of a portion of the signal propagating through one of the cores to the other core. In cladding-polished couplers, the core


110


of each fiber is polished flat and mechanically aligned to the other core


110


, thereby inducing cross-talk between the cores.




The coupling efficiency of both cladding-fused and cladding-polished couplers is reduced because a portion of the signal propagating in the core is transferred to cladding


120


at the point of coupling, thereby increasing the excess loss of the device incorporating the coupled fibers.




Accordingly, there exists a need for an optical fiber with reduced or minimal excess loss resulting from coupling.




SUMMARY OF THE INVENTION




The present invention is directed to improving the coupling efficiency of both cladding-fused and cladding-polished optical couplers thereby reducing excess loss.




One aspect of the invention is directed to an optical fiber including a core having a diameter d


c


and a refractive index n


c


, a primary cladding concentrically surrounding the core and having an outer diameter d


pc


, and a refractive index n


pc


that is less than the core refractive index n


c


and a secondary cladding concentrically surrounding the primary cladding. The secondary cladding has an outer diameter d


sc


and a refractive index n


sc


that is less than the primary cladding refractive index n


pc


. The primary cladding outer diameter d


pc


is a fraction of the secondary cladding outer diameter d


sc


. The difference between the primary cladding refractive index n


pc


and the secondary cladding refractive index n


sc


is greater than or equal to a constant and less than or equal to the core refractive index n


c


less the constant.




In other embodiments, the primary cladding is updoped or the secondary cladding is downdoped. The primary cladding outer diameter is a fraction of the secondary cladding outer diameter. The fraction may range from >0% to 75%; is desirably 10% to 50%; and is most preferably around 20%. The above-mentioned constant relating the refractive indices of the primary and secondary claddings is preferably equal to or greater than 0.0002.




In another embodiment, the cladding and/or the core includes a material inducing photosensitivity, such that exposure to radiation creates a refractive-index modulation within the cladding and/or the core.




In another aspect, the invention is directed to a method of coupling a pair of optical fibers. The method includes the steps of providing a pair of fibers and fusing the fibers along a portion of their longitudinal extents to couple them.




The primary claddings may or may not be fused. Thus, in some embodiments, the primary claddings are fused, while in other embodiments, the primary claddings are not fused but the secondary claddings are fused proximate to the primary claddings.











BRIEF DESCRIPTION OF THE DRAWINGS




The invention is pointed out with particularity in the appended claims. The advantages of the invention may be better understood by referring to the following description taken in conjunction with the accompanying drawing in which:





FIG. 1

is an end view of a prior art single mode optical fiber and a graph showing the radial variation of the fiber's refractive index;





FIG. 2

is a plan view of a prior art cladding fused optical coupler;





FIG. 3

is an end view of an embodiment of the present invention; and





FIG. 4

graphically depicts the refractive index profile of an optical fiber in accordance with the principles of the present invention.











DETAILED DESCRIPTION OF THE INVENTION




With reference to

FIG. 3

, one embodiment of the present invention, indicated generally at


200


, includes a core


210


having an outer diameter d


c


and a refractive index n


c


, a primary cladding


220


, which concentrically surrounds core


210


, having an outer diameter d


pc


, an annular thickness t


pc


that is substantially equal to (d


pc


−d


c


)/2, and a refractive index n


pc


; and a secondary cladding


230


, which concentrically surrounds primary cladding


220


, having an outer diameter d


sc


, an annular thickness t


sc


that is substantially equal to (d


sc


−d


pc


)/2, and a refractive index n


sc


. The relationship among the refractive indices mentioned above is n


c


>n


pc


>n


sc


. Thicknesses t


pc


and t


sc


are related in that t


pc


≦t


sc


. In one embodiment, annular thickness t


sc


is substantially 125 μm. In another embodiment, annular thickness t


sc


is substantially 80 μm.




Both primary cladding


220


and secondary cladding


230


are typically composed of silica-based glass material. Primary cladding


220


is selected or treated to slightly elevate the refractive index n


pc


; for example, one of the primary or secondary claddings may be pure silica and the other doped such that primary cladding


220


exhibits a slightly higher index (that is, primary cladding


220


may be pure silica and secondary cladding


230


“downdoped” to lower its index, or secondary cladding


230


may be pure silica and primary cladding


220


“updoped” to raise its index); or both the primary and secondary claddings may be doped, with primary cladding


220


doped as appropriate to achieve the desired index elevation. As used herein, the term “downdope” refers to the addition of one or more dopants that lower the refractive index or to the use of a dopant concentration or combination which, relative to an adjacent layer, achieves a lower index than that layer (e.g., through use of a lower concentration of an index-raising dopant, or a higher concentration of an index-decreasing dopant); similarly, the term “updope” refers to the addition of one or more dopants that raise the refractive index or to the use of a dopant concentration or combination which, relative to an adjacent layer, achieves a higher index than that layer. Typical index-raising dopants include, for example, germanium, phosphorus, titanium and aluminum, while fluorine and boron are common index-lowering dopants. The dopants are added during the manufacturing process, for example, the modified chemical vapor deposition process (MCVD) or another process such as, but not limited to, outside vapor deposition (OVD), vapor axial deposition (VAD), and plasma vapor deposition (PVD).





FIG. 4

depicts the refractive index profile and the differences among the refractive indices of an embodiment of the present invention. Core refractive index n


c


is the largest, and generally constant until outer core diameter d


c


is reached. Primary cladding


220


begins where core


210


ends, thus the refractive index transitions to that of primary cladding


220


(i.e., n


pc


). Primary cladding refractive index n


pc


is less than that of core


210


. Again, the primary cladding refractive index n


pc


is substantially constant until primary cladding outer diameter d


pc


is reached. Secondary cladding refractive index n


sc


is slightly less than primary cladding refractive index n


pc


and remains substantially constant until the secondary cladding outer diameter d


sc


is reached. The difference between primary cladding refractive index n


pc


and secondary cladding refractive index n


sc


is indicated in

FIG. 4

by Δn


clad


. The quantity Δn


clad


generally remains in a range between a constant and the core refractive index n


c


less the constant (i.e., k≦Δn


clad


≦n


c


−k). In one embodiment, k≧0.0002. The quantity Δn


clad


is determined before fabrication and may be selected to provide the desired performance for a given wavelength of light and coupling application. In use, two fibers are coupled so that the primary claddings fuse; alternatively, the fibers may be coupled so that only the secondary claddings fuse, but the primary claddings are in close proximity. The two fibers may be constructed in accordance with the principles of the present invention, or a fiber of the present invention may be fused with a traditional or other custom fiber. Additionally, principles of the present invention can be embodied in other fused devices, such as, splitters, combiners, add-drop filters, and mulitplexers.




Generally, the dimension of the primary cladding outer diameter d


pc


is a fraction of the secondary cladding outer diameter d


rc


. The fraction d


pc


/d


sc


may range from >0 to 0.75; is desirably 0.1 to 0.5; and is most preferably around 0.2 (i.e., d


pc


≈0.2d


sc


). The dimensions of primary cladding outer diameter d


pc


and secondary cladding outer diameter d


sc


are also determined prior to fabrication and are selected to provide the desired performance for a given wavelength of light and coupling application.




Therefore, by controlling the dimensions of outer diameters d


pc


and d


sc


, and the difference Δn


clad


, the present invention provides improved coupling efficiency.




It should be noted that the core and/or cladding layers may be made photosensitive to facilitate production of fiber Bragg gratings. These devices, which are used to filter, reflect and/or demultiplex wavelength-division multiplexed signals, are implemented within the fiber itself by providing a refractive-index modulation within the core. Fiber Bragg gratings may be obtained by, for example, rendering the core photosensitive to a certain form of radiation (typically ultraviolet light) and then exposing the fiber to such radiation, thereby altering the refractive index of the core where so exposed. Photosensitivity may be achieved, e.g., by doping a silica core with germanium and/or boron. Creating the pattern of index variations characteristic of a fiber Bragg grating may be achieved using any of various techniques, including holographic approaches, exposure of the fiber to radiation through a phase mask, etc.




The present invention is amenable to this treatment; that is, photosensitivity may be imparted to a fiber produced in accordance herewith so long as the necessary refractive-index relationships are maintained.




Having shown the preferred embodiments, one skilled in the art will realize that many variations are possible within the scope and spirit of the claimed invention. It is therefore the intention to limit the invention only by the scope of the claims.



Claims
  • 1. An optical fiber comprising:a core having a diameter dc and a refractive index nc; a primary cladding concentrically surrounding the core and having an outer diameter dpc and a refractive index npc less than the core refractive index nc, wherein the refractive index npc is substantially constant through the primary cladding; and a secondary cladding concentrically surrounding the primary cladding and having an outer diameter dsc and a refractive index nsc less than the primary cladding refractive index npc, wherein the primary cladding outer diameter dpc is a fraction of the secondary cladding outer diameter dsc, and wherein a difference between the primary cladding refractive index npc and the secondary cladding refractive index nsc is greater than or equal to a constant and less than or equal to the core refractive index nc less the constant.
  • 2. The optical fiber of claim 1, wherein the primary cladding is updoped.
  • 3. The optical fiber of claim 1, wherein the secondary cladding is downdoped.
  • 4. The optical fiber of claim 1, wherein the fraction ranges from >0 to 0.75.
  • 5. The optical fiber of claim 4, wherein the fraction ranges from 0.1 to 0.5.
  • 6. The optical fiber of claim 4, wherein the fraction is about 0.2.
  • 7. The optical fiber of claim 1, wherein the constant is about 0.0002.
  • 8. The fiber of claim 1, wherein the core further comprises a material rendering the core photosensitive, such that exposure of the core to radiation creates a refractive-index modulation within the core.
  • 9. The fiber of claim 1, wherein at least one of the primary and secondary cladding further comprises a material causing photosensitivity, such that exposure of the at least one cladding to radiation creates a refractive-index modulation therein.
  • 10. The fiber of claim 1, wherein the secondary cladding has an annular thickness tsc of substantially 125 μm.
  • 11. The fiber of claim 1, wherein the secondary cladding has an annular thickness tsc of substantially 80 μm.
  • 12. A method of coupling a pair of optical fibers, comprising the steps of:providing a pair of fibers, each of the fibers having a longitudinal extent and at least one of the fibers comprising (i) a core having a diameter dc and a refractive index nc; (ii) a primary cladding concentrically surrounding the core and having an outer diameter dpc and a refractive index npc less than the core refractive index nc; and (iii) a secondary cladding concentrically surrounding the primary cladding and having an outer diameter dsc and a refractive index nsc less than the primary cladding refractive index npc wherein the primary cladding outer diameter dpc is a fraction of the secondary cladding outer diameter dsc, and wherein a difference between the primary cladding refractive index npc and the secondary cladding refractive index nsc is greater than or equal to a constant and less than or equal to the core refractive index nc less the constant; and fusing the fibers along a portion of their longitudinal extents to couple them.
  • 13. The method of claim 12 wherein the primary claddings are fused.
  • 14. The method of claim 12 wherein the primary claddings are not fused but the secondary claddings are fused proximate to the primary claddings.
CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority to and the benefits of U.S. Provisional Patent Application Ser. No. 60/305,916 filed on Jul. 17, 2001, the entire disclosure of which is herein incorporated by reference.

US Referenced Citations (30)
Number Name Date Kind
3403955 Jueneman Oct 1968 A
3434774 Miller Mar 1969 A
3718383 Moore Feb 1973 A
3778132 Pinnow et al. Dec 1973 A
4053204 Miller Oct 1977 A
4053205 Miller Oct 1977 A
4076380 DiMarcello et al. Feb 1978 A
4106850 Marcatili Aug 1978 A
4111525 Kaminow et al. Sep 1978 A
4114980 Asam et al. Sep 1978 A
4152044 Liu May 1979 A
4203743 Suganuma et al. May 1980 A
4212660 Maurer Jul 1980 A
4440558 Nath et al. Apr 1984 A
4812153 Andrejco et al. Mar 1989 A
4968339 Miller et al. Nov 1990 A
5044724 Glodis et al. Sep 1991 A
5175785 Dabby Dec 1992 A
5217516 Ishiguro et al. Jun 1993 A
5364429 Le Sergent Nov 1994 A
5676725 Ito et al. Oct 1997 A
5746797 Noda May 1998 A
5761366 Oh et al. Jun 1998 A
5933743 New et al. Aug 1999 A
6062046 Terasawa et al. May 2000 A
6145344 Oyamada et al. Nov 2000 A
6157758 Abe et al. Dec 2000 A
6445855 Stowe et al. Sep 2002 B1
6597849 Ishikawa et al. Jul 2003 B2
6603913 Okuno Aug 2003 B1
Foreign Referenced Citations (3)
Number Date Country
WO 9829768 Jul 1998 WO
WO 0000860 Jan 2000 WO
WO 0073822 Dec 2000 WO
Non-Patent Literature Citations (1)
Entry
Patent Cooperation Treaty, International Search Report, International Application No. PCT/US02/15409, mailed on Nov. 21, 2002, 8 pages.
Provisional Applications (1)
Number Date Country
60/305916 Jul 2001 US