FIBRE-OPTIC CONNECTOR EMPLOYING MODE FIELD MODIFICATION

Abstract: Disclosed is a mode field modifier (40) for use with an optical fibre (54) having a core (56) and a cladding (58) of outside diameter d. The modifier comprises a modifier core (42) having a refractive index n₁. Surrounding the modifier core is first cladding layer (44) having a refractive index n₂ that is less than n₁. On the surface of the first cladding layer is a second cladding layer (46) having a refractive index n₃ which is less than n₂. The modifier is tapered intermediate its ends whereby it has a large diameter end and a small diameter end. The diameters of at least the core and first cladding layer at the large diameter end are greater than the corresponding diameters at the small diameter end. The diameter D₁ of the first cladding layer at the large diameter end is greater than d. An axially disposed hole (52) in the large diameter end receives a fiber (54) which is held in such alignment with the mode field modifier (40) that it is in light coupling relationship with the modifier core (42). The mode field of a signal coupled from the fiber to the mode field modifier expands as it propagates through the tapered portion of the modifier to the small diameter end. An in-line coupler between two optical fibers is effected by connecting together in axial alignment two such mode field modifiers with their small diameter ends adjacent one another.

Description: This invention relates to optical fiber connectors, and, more particularly, to connectors which are capable of connecting an optical fiber to a source or to another optical fiber with very little sensitivity to lateral misalignment. Although the present invention finds utility in the coupling of light from a source to an optical fiber, the present discussion concerning connector alignment problems will be limited to fiber-to-fiber connectors. The butt connection between the ends of two fibers will result in an insertion loss that is caused by various optical fiber misalignment parameters. Examples of such misalignment parameters are as follows: (a) lateral misalignment between the axes of the two fibers, (b) longitudinal misalignment between the endfaces of the two fibers, and (c) angular misalignment between the axes of the two fibers. The usual approach to fiber coupling is the butted end coupler in which fibers which have had their end-faces prepared are brought into angular, lateral and axial alignment. Such alignment is difficult to achieve outside the laboratory. Since the butted fiber arrangement is particularly sensitive to lateral displacement, this type of connector is difficult to use in field applications. Beam expanders employing lenses or tapered fibers have been employed in in-line single-mode fiber connectors which, due to the small core diameter of such fibers, are extremely sensitive to lateral misalignment. Although such beam expanders exhibit a reduced sensitivity to lateral displacement, they are generally very sensitive to angular misalignment. The art of aligning two connector halves is sufficiently advanced that angular misalignment is not a primary concern. Expanded beam connectors are therefore receiving a considerable amount of attention. The basic principal of expanded beam connectors is described in the publication K. P. Jedrzejewski et al. "Tapered-Beam Expander for Single-Mode Optical-Fiber Gap Devices", Electronics Letters , 16th January 1986, vol. 22, No. 2, pp. 105-106. That publication teaches a connector of the type wherein the end of a single-mode fiber having a core refractive index n₁ and a cladding refractive index n₂ is inserted into a tube of glass having a refractive index n₃ which is lower than n₂. The refractive index of the tube is slightly lower than cladding n₂. The capillary tube is uniformly heated to collapse it about the fiber. The central region of the combined fiber and capillary is then tapered to a minimum neck diameter of 40 µm, which is appropriate for fiber handling and cleaving. A taper ratio of 4:1 is said to be adequate for minimizing insertion loss. Since the end of the fiber forms the central portion of the connector, no means need be provided for attaching the fiber to the connector half. However, that fiber cannot be easily disconnected from the connector half and replaced by another fiber. Furthermore, by employing the fiber as the internal portion of the connector half, the maximum spot size is limited. A three layer mode field modifier is also disclosed in DE-A-35 44 136. That modifier comprises a tapered modifier core having a refractive index n₁, surrounded by first and second cladding layers having refractive indices n₂ and n₃, respectively, where n₁>n₂>n₃. The modifier is tapered intermediate its ends whereby it modifies the mode field of an optical signal propagating therethrough. An optical fiber is positioned at the large diameter end of the modifier in light coupling relationship with the modifier core. The diameter D₁ of the first cladding layer at the large diameter end of the modifier is smaller than the outside diameter d of the optical fiber, whereby the maximum spot size of a signal propagating in the modifier toward the small diameter end thereof is limited. Summary of the Invention Briefly, the present invention relates to a mode field modifier connected to an optical fiber having an outside diameter d. The mode field modifier comprises a tapered modifier core having a refractive index n₁ and a first cladding layer surrounding the modifier core, the first cladding layer refractive index n₂ being less than n₁. On the surface of the first cladding layer is a second cladding layer, the refractive index n₃ of which is less than n₂. The modifier is tapered intermediate its ends whereby it has a large diameter end and a small diameter end. The diameters of at least the core and the first cladding layer at the large diameter end are greater than the corresponding diameters at the small diameter end, whereby the mode field of an optical signal propagating in one end of the modifier is modified as the signal propagates through the tapered portion of the modifier. Means are provided for positioning the fiber at the large diameter end in light coupling relationship with the modifier core. The mode field modifier of the present invention is characterized in that the diameter D₁ of the first cladding layer at the large diameter end is greater than d. The mode field diameter can be increased by forming a modifier in which the ratio (n₂-n₃)/n₂ has been minimized. The means for positioning a fiber can be a recess in the large diameter end of the mode field modifier. In one embodiment the first cladding layer consists of an inner and an outer layer of glass, the inner layer being more soluble in a given solvent than the outer layer. The recess is formed by immersing the large diameter end in a solvent to dissolve the inner layer to a sufficient depth. The refractive index of the outer layer can be equal to or less than that of the inner layer. The fiber can be properly positioned with respect to the modifier by incorporating an end of the fiber in the modifier as the central region thereof. In this embodiment the end of the fiber is surrounded by a tube comprising concentric regions, the refractive index of the outer region being lower than that of the inner region. The small diameter ends of two such mode field modifiers can be connected end-to-end to effect a low loss connection between fibers attached to the large diameter ends of such modifiers. Such mode field modifiers are especially useful for connecting single-mode fibers. The present mode field modifier is also useful for connecting an optical fiber to a light source or detector. Fig. 1 is a cross-sectional view of an in-line fiber connector employing two mode field modifiers. Fig. 2 is a cross-sectional view of a mode field modifier connection between an optical fiber and a light source. Fig. 3 is a cross-sectional view of the mode field modifier of the present invention. Fig. 4 is a cross-sectional view taken along lines 4-4 of Fig. 3. Fig. 5 is the refractive index profile of the large diameter end of the mode field modifier of Fig. 3. Fig. 6 is a graph of spot size versus draw ratio for different values of cladding diameter D₁. Fig. 7 is a graph of spot size versus draw ratio for different values of percent Δ₂₋₃. Figs. 8 and 9 illustrate one embodiment of the invention whereby a fiber alignment hole is formed by dissolving a glass layer. Fig. 10 is a cross-sectional view of a further embodiment Fig. 1 shows an in-line fiber connector of the mode field diameter modification type. Two connector halves 12 and 14 are secured together in axial alignment by sleeve 16. Means to be discussed later are provided for securing fibers 18 and 20 in axial alignment with the large diameter ends of connector halves 12 and 14, respectively. An optical signal propagating in fiber 18 is coupled to the core of connector half 12. As this signal propagates toward the small diameter end of coupler 12 the mode field diameter expands, the expanded beam coupling into the small diameter end of connector half 14. Because of the large size of the beam at the small diameter ends, this type of connector is much less sensitive to lateral misalignment. This type of expanded-beam connector is a rugged alternative to lens beam-expanders in connectors and other in-line fiber devices. Fig. 2 illustrates that a similar connector half 24 may be employed to connect the output from light emitting diode 26 to fiber 28. Housing 30 contains cavities for receiving the diode and connector half. Means 32 located at the large diameter end of the connector half 24 contains an aperture for receiving fiber 28 in alignment with the core of mode field modifier 24. The mode field modifier of the present invention is shown in greater detail in Figs. 3 and 4, and the refractive index profile of the large diameter end thereof is shown in Fig. 5. Modifier 40 comprises a core 42 of refractive index n₁ surrounded by a layer 44 of cladding material having a refractive index n₂ which is less than n₁. A second cladding layer 46 on the surface of layer 44 has a refractive index n₃ which is less than n₂. For device 40 to function as a mode field modifier, the diameters of at least the core 42 and first cladding layer 44 must change intermediate ends 48 and 50. In the illustrated embodiment, modifier 40 is tapered intermediate ends 48 and 50 such that the diameter of layer 44 decreases over length l from D₁ to D₂. A fiber 54 having core 56 and cladding 58 is positioned at the large diameter end of modifier 40 in light coupling relationship therewith. In this embodiment, fiber 54 extends into a hole 52 that is formed in large diameter end 48. Hole 52 is centered about the axis of modifier 40 so that fiber core 56 is aligned with modifier core 42. The difference between n₁ and n₂ should be similar to the Δ value of fiber 54. A loss will occur if the diameter of core 42 is not the same as that of core 56. A single-mode or multimode signal propagating in fiber 54 is coupled to the optical waveguide comprising core 42 and first cladding layer 44. In a multimode system, the term "mode field" refers to the summation of the mode fields of all modes. The tapered region along length l has a significant affect on the propagating optical field. Initially the field is guided by, and substantially confined to core 42. As the core diameter decreases the field spreads out, and spot sized increases. Eventually a point is reached when the field is no longer guided by the core but is effectively guided by the waveguide consisting of first cladding 44 and second cladding 46. The small end diameter D₂ of layer 44 is greater than the diameter of core 56. Because of the large diameter spot size at end 50 of modifier 40, light can be coupled to the small diameter end of a like modifier as illustrated in Fig. 1. Although this device is useful for the in-line connection of multimode fibers, it is especially useful in single-mode systems wherein the spot size at the endface of the single-mode fiber is extremely small. It is the larger spot size at small diameter end 50 which renders the connector of Fig. 1 less sensitive to lateral misalignment. It has been discovered that an even greater enlargement of the spot size can be achieved if the diameter D₁ of first cladding layer 44 is greater than diameter d of fiber 54. This relationship is illustrated in the graph of Fig. 6 wherein spot size is plotted as a function of draw ratio for different values of cladding diameter D₁. For this experiment fiber 54 was a single-mode fiber having a diameter d of 125µm. Curve 64 is the spot size versus draw ratio curve for a modifier having an inner cladding diameter D₁ which is also equal to 125µm. Curves 66, 68, 70 and 72 illustrate the spot size versus draw ratio relationship which exists when the diameter D₁ is equal to 140µm, 160µm, 180µm and 200µm, respectively. Spot size is related to a lesser degree to % Δ₂₋₃ which is equal to (n₂-n₃)/n₂ x 100%. The graph of Fig. 7 illustrates the relationship between spot size and draw ratio for different values of % Δ₂₋₃. Curves 78, 80 and 82 were generated from devices wherein the diameter d of single-mode fiber 54 and the diameter D₁ of inner cladding layer 44 were 125µm. Curve 78, which is identical with curve 64 of Fig. 6, is for a mode field modifier wherein % Δ₂₋₃ is 0.15%. Curves 80 and 82 represent devices wherein % Δ₂₋₃ is equal to 0.10% and 0.05%, respectively. Fig. 7 shows that for draw ratios between 3.5 and 4 an increase in spot size of about 1µm can be achieved by reducing % Δ₂₋₃ from 0.15% to 0.05%. If a mode field modifier is to be used in a connector for multimode optical fibers, the Δ-value of the mode field modifier should be on the order of that of the fiber, or higher order modes will be lost. Therefore, a mode field modifier having a % Δ of 0.05% would be useful for only single-mode fibers. The spot size for curve 82 is about 17µm for a draw ratio of about 14. However, since operation in this region of the curve is more susceptible to loss, a draw ratio between about 3.5 and 4.0 may be preferred. It is noted that if the taper rate is sufficiently small, there will be negligible loss due to mode coupling. Thus, it is possible to form very low loss connectors having draw ratios greater than 10:1. By very low loss is ment a loss that is much lower than the 1 dB loss that is usually considered to be tolerable. A method of forming the fiber positioning hole 52 is illustrated in Figs. 8 and 9. In this embodiment, mode field modifier 86 comprises a core 88 and a second cladding layer 90 having optical characteristics similar to core 42 and second cladding 46 of Fig. 3. The first cladding layer comprises concentric layers 92 and 94, the refractive index of layer 94 being equal to or less than that of layer 92. The compositions of layers 92 and 94 differ, the glass of layer 92 being more soluble in a given solvent than that of layer 94. Cladding 96 must also be resistant to being dissolved in the given solvent. For example, the various glasses which comprise modifier 86 could consist essentially, expressed in weight percent on the oxide basis, of the compositions specified in the following table. When end 96 of modifier 86 is immersed in nitric acid, layer 92 is more readily etched so that hole 98 of Fig. 9 is formed. The mode field modifier could also be fabricated in the manner illustrated in Fig. 10 wherein elements similar to those of Fig. 3 are represented by primed reference numerals. The end of fiber 54′ is inserted into an aperture 102 in a tube comprising concentric regions 101 and 46′. The refractive index of region 101 is preferably the same as that of fiber cladding 58′ and is greater than that of region 46′. The tube is symmetrically heated to collapse it uniformly about fiber 54′. The combined fiber and tube is then tapered and the small diameter end is cleaved to form mode field modifier 40′.

Claims: A mode field modifier (40) connected to an optical fiber (54) having a core (56) and a cladding (58) of outside diameter d, said modifier comprising a tapered modifier core (42) having a refractive index n₁, a first cladding layer (44) surrounding said modifier core, said first cladding layer having a refractive index n₂ that is less than n₁, a second cladding layer (46) on the surface of said first cladding layer, the refractive index n₃ of said second cladding layer being less than n₂, said modifier being tapered intermediate its ends (48, 50) whereby it has a large diameter end and a small diameter end, the diameters of at least said core and said first cladding layer at said large diameter end are greater than the corresponding diameters at said small diameter end, whereby the mode field of an optical signal propagating in one end of said modifier is modified as said signal propagates through the tapered portion of said modifier, and means (52) for positioning said fiber (54) at said large diameter end in light coupling relationship with said modifier core (42), characterized in that the diameter D₁ of said first cladding layer (44) at said large diameter end is greater than d. A mode field modifier (40) in accordance with claim 1 wherein said means for positioning a fiber comprises a recess (52) in said large diameter end, said recess being concentric with said modifier core (42). A mode field modifier (86) in accordance with claim 2 wherein said first cladding layer comprises an inner (92) and an outer (94) layer of glass, the inner of said layers being more soluble in a given solvent than the outer of said layers. A mode field modifier in accordance with claim 3 wherein the refractive index of said outer layer (94) is substantially the same as that of said inner layer (92). A mode field modifier in accordance with claim 3 wherein the refractive index of said outer layer (94) is less than that of said inner layer (92). A mode field modifier in accordance with claim 1 wherein the ratio (n₂-n₃)/n₂ is no smaller than 0.5%. A mode field modifier in accordance with claim 1 wherein said fiber (54) forms the central portion of said mode field modifier and wherein said first cladding layer comprises the cladding (58') of said fiber and a further layer (101) on the surface of said fiber cladding, said further layer having a refractive index equal to or less than that of said fiber cladding. A device for connecting first and second optical fibers of outside diameter d, said device comprising first and second mode field modifiers (12, 14), each having a modifier core (42) having a refractive index n₁, a first cladding layer (44) surrounding said modifier core, said first cladding layer having a refractive index n₂ that is less than n₁, a second cladding layer (46) on the surface of said first cladding layer, the refractive index n₃ of said second cladding layer being less than n₂, said modifier being tapered intermediate its ends (48, 50) whereby it has a large diameter end and a small diameter end, the diameters of at least said core and said first cladding layer at said large diameter end are greater than the corresponding diameters at said small diameter end, whereby the mode field of an optical signal propagating in one end of said modifier is modified as said signal propagates through the tapered portion of said modifier, the diameter D₁ of said first cladding layer (44) at said large diameter end being greater than d, means (52) for positioning said first optical fiber at said large diameter end of said first modifier (12) in light coupling relationship with said first modifier core, means (52) for positioning said second optical fiber at said large diameter end of said second modifier (14) in light coupling relationship with said second modifier core, and said device further comprising means (16) for positioning the small diameter end of said first modifier adjacent the small diameter end of said second modifier with the axes of said first and second modifiers in substantial light coupling alignment.

Inventors: NOLAN, DANIEL ALOYSIUS, TRUESDALE, CARLTON MAURICE
Applicants: CORNING GLASS WORKS
Application year: 1988
Main classification: G02B6
IPC codes: G02B6