Optical fiber coupler and its manufacturing method

Abstract: In an optical fiber coupler there is provided in an optical coupling portion (21) between cores (13a, 13b) of two partly fused together and extended optical fibers an optical coupling control portion (21) which has a refractive index different from those of claddings (12a, 12b) covering the cores. With the provision of such a coupling control portion (21) which has a refractive index higher than those of the claddings (12a) and (12b), the optical coupling between the cores (13a) and (13b) is equivalently tighter than in the case where the coupling control portion (21) is not provided. Moreover, the coupling control portion (21) reduces the propagation wavelength of light therethrough and increases the effective coupling length (the length of the optical coupling portion converted to wavelength) as compared with that when the coupling control portion (21) is not provided. Thus, in the case of obtaining the same coupling coefficient as in the past, the length of the optical coupling portion (11) can be decreased. Since the length of the optical coupling portion (11) can be reduced and since the coupling coefficient C can be made large, it is possible to construct a WDM optical fiber coupler in which the core diameter is not so small, that is, to such an extent as not to increase the excess loss and which has a branching ratio narrow in the wavelength spacing between its peaks, that is, has high wavelength dependence (i.e. a narrow wavelength band).

Description: BACKGROUND OF THE INVENTION The present invention relates to an optical fiber coupler which performs optical coupling between a plurality of cores through claddings at an optical coupling portion and particularly an optical fiber coupler of a wavelength division multiplex/demultiplex type. The invention also pertains a method for the manufacture of such an optical fiber coupler. Fig. 1 shows a conventional optical fiber coupler (JP-A-60-51685). An optical coupling portion 11 includes two cores 13a and 13b in a common cladding 12 as depicted in Fig. 2 which is a cross-sectional view taken on the line 2-2 in Fig. 1. Reference numerals 15 and 16 denote optical fibers having cores continuous with both ends of the core 13a, and 17 and 18 optical fibers similarly having cores continuous with both ends of the core 13b. Usually, one optical fiber forming the optical fibers 15 and 16 and another optical fiber forming the optical fibers 17 and 18 have their intermediate portions fused together by heating and the fused portion is elongated or stretched to from the optical coupling portion 11. In this way the optical fibers 15, 16 and 17, 18 are optically coupled together at the optical coupling portion 11. A refractive index n along a straight line Ox passing through the centers of the cores 13a and 13b and perpendicular to the optical coupling portion 11 is high in the cores 13a, 13b as indicated by N CR in Fig. 3 and low and constant in the cladding 12 as indicated by N CL . The characteristics of the optical fiber coupler are dependent upon parameters such as the difference between the refractive indexes of the cores 13a, 13b and the cladding 12, the diameters of the cores 13a and 13b, their spacing and the length of the optical coupling portion 11. The conventional optical fiber coupler encounters a difficulty in reducing the length of the optical coupling portion 11. The branching ration CR in the optical fiber coupler is expressed by the following equations: CR = cos 2 (C) C = 0 L c(z)dz , where c(z) is a coupling coefficient in the z coordinates, z is a coordinate in the longitudinal direction of the optical coupling portion 11 and L is the length of the optical coupling portion 11. It is well-known in the art that the coupling coefficient C needs to be large in the case of fabricating a coupler which is used as a so-called WDM (wavelength division multiplex/demultiplex) coupler in particular, a coupler of a branching ratio narrow in the wavelength spacing of adjacent peaks, i.e. a highly wavelength dependent coupler. To make the coupling coefficient C large, it is necessary to maximize the coupling coefficient c(z). This can be accomplished by decreasing the core diameter in the optical coupling portion to facilitate the leakage of light from each core and by reducing the core spacing in that portion to facilitate the coupling of light. With too small a core diameter in the optical coupling portion as compared with the core diameter at the end of each optical fiber, however, the coupling coefficient c(z) becomes large but the discontinuity in the core diameter increases, causing an increase in an excess loss of the optical fiber coupler as a whole. Accordingly, it is customary in the prior art to increase the length L of the optical coupling portion 11 to make the coupling coefficient C large without abruptly decreasing the core diameter. Hence, the optical coupling portion 11 is long in the prior art optical fiber coupler. Thus, no WDM coupler with a short optical coupling portion could have been implemented with the optical fiber coupler. Besides, the conventional optical fiber coupler has relatively high polarization dependence. Fig. 4 shows the branching ratio vs. wavelength characteristic of the conventional optical fiber coupler measured using random light. As is evident from Fig. 4, the branching ratio is not 0% but 7 to 8% at a wavelength of about 1534 nm and not 100% but 90% or so at a wavelength of about 1470 nm. This is considered to be caused by the polarization dependence of the optical fiber coupler. The dependence of the branching ration on polarization was ±9.3% at a wavelength of 1548 nm, which is relatively large. To realize an optical fiber coupler of low wavelength dependence, it is necessary to minimize the coupling coefficient C in contrast to the case of increasing the wavelength dependence. This can be accomplished by maximizing the core diameter and the core spacing, but they cannot be made larger than those of an optical fiber which is used to form the optical fiber coupler. Accordingly, there is a limit to the reduction of the wavelength dependence of the optical fiber coupler. In a conventional optical fiber coupler which has a branching ratio of 50% at a wavelength of 1.3 µm, it is difficult to make its wavelength dependence 0.2% or below. To obtain an optical fiber coupler of a wide wavelength band, it has also been proposed to employ a method according to which an optical fiber is fused and stretched and another optical fiber is fused and connected thereto and then stretched so that the core diameter of the one optical fiber is smaller than the core diameter of the other optical fiber. With this method, however, it is difficult to manufacture of optical fiber couplers of desired characteristics with a satisfactory yield of product. US-A-4,589,725 discloses an optical fiber coupler according to the precharacterizing clause of claim 1, wherein the optical coupling control portion comprises a vitreous layer of amorphous boron oxide having an index of refraction just slightly below the value of the index of refraction of the claddings. The coupler disclosed in this document is a wideband coupler said to provide insertion losses below 0.5 dB over a relatively wide bandwidth. SUMMARY OF THE INVENTION It is therefore an object of the present invention to provide an optical fiber coupler of a WDM type with which it is possible to obtain a branching ratio of desired wavelength dependence. Another object of the present invention is to provide a method for the manufacture of such an optical fiber coupler with a good production yield. These objects are achieved with an optical fiber coupler and a method as claimed in claims 1 and 3, respectively. When the refractive index of the coupling control portion is selected higher than the refractive indexes of the claddings, the coupling coefficient between the both cores increases, whereas when the refractive index of the coupling control portion is selected lower than the refractive indexes of the claddings, the coupling coefficient decreases. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a diagram schematically showing a conventional optical fiber coupler; Fig. 2 is an enlarged cross-sectional view taken on the line 2-2 in Fig. 1; Fig. 3 is a graph showing the refractive index distribution along a line Ox in Fig. 2; Fig. 4 is a graph showing the branching ratio-wavelength characteristic of the conventional optical fiber coupler; Fig. 5 is a cross-sectional view illustrating the optical fiber coupler according to an embodiment of the present invention; Fig. 6 is a graph showing the refractive index distribution of the optical fiber used in the coupler of Fig. 5; Fig. 7 is graph showing the refractive index distribution of the optical fiber coupler along the line Ox in Fig. 5; Fig. 8 is a graph showing the refractive index distribution of an optical fiber for use in the embodiment of Fig. 5; Fig. 9 is a graph showing the refractive index distribution in an example of an optical fibre coupler; Fig. 10 is a graph showing the refractive index distribution in still another example of an optical fibre coupler; and Fig. 11 is a diagram for explaining the optical fiber coupler manufacturing method of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS Fig. 5 illustrates in section the optical coupling portion 11 of the optical fiber coupler of a WDM type according to an embodiment of the present invention. Between a cladding 12a covering the core 13a and a cladding 12b covering the core 13b there is provided a coupling control portion 21 which has a refractive index different from those of the claddings 12a and 12b. In the Fig. 5 embodiment a pair of identical optical fibers, each of which has its cladding surrounded by an optical layer having a refractive index different from that of the cladding and has such a refractive index distribution as shown in Fig. 6 (in which the ordinate represents a refractive index difference Δn between the optical layer and the cladding), are partly fused together and the fused portion is extended to form the optical fiber coupler. Consequently, the coupling control portion 21 is extended so that the claddings 12a and 12b are surrounded by optical layers 21a and 21b, respectively. In short, the coupling control portion 21 needs to be provided in an area defined by the opposed claddings 12a and 12b between the cores 13a and 13b. Fig. 7 shows an example of the refractive index distribution along the straight line Ox passing through the centers of the cores 13a and 13b in Fig. 5, inferred from Fig. 6. (The actual diameter of the stretched optical coupling portion 11 was as small as 30 µm or so, and hence the refractive index distribution along the diameter could not be measured.) In Fig. 7, N CL represents the refractive indexes of the claddings 12a and 12b and N CR the refractive indexes of the cores 13a and 13b. In this embodiment the refractive index 21N of the coupling control portion 21 is higher than the refractive indexes N CL of the claddings 12a and 12b. With the provision of such a coupling control portion 21 which has a refractive index higher than those of the claddings 12a and 12b, the optical coupling between the cores 13a and 13b is equivalently tighter than in the case where the coupling control portion 21 is not provided. Moreover, the coupling control portion 21 reduces the propagation wavelength of light therethrough and increases the effective coupling length (the length of the optical coupling portion converted to wavelength) as compared with that when the coupling control portion 21 is not provided. Thus, in the case of obtaining the same coupling coefficient as in the past, the length of the optical coupling portion 11 can be decreased. Fig. 8 shows the branching ratio-wavelength characteristic of the optical fiber coupler with respect to randomly polarized light. The optical coupling portion 11 of this optical fiber coupler is 9.8 mm long, whereas the optical coupling portion 11 of the conventional optical fiber coupler which has a peak at the same wavelength as in Fig. 8 is 16.5 mm. Since the length of the optical coupling portion 11 can be reduced and since the coupling coefficient C can be made large, it is possible to construct a WDM optical fiber coupler in which the core diameter is not so small, that is, to such an extent as not to increase the excess loss and which has a branching ratio narrow in the wavelength spacing between its peaks, that is, has high wavelength dependence (i.e. a narrow wavelength band). The coupling coefficient C can be controlled or adjusted by selecting the refractive index of the coupling control portion 21, the distance between the cores 13a and 13b, and so forth. The branching ratio of the optical fiber coupler of the present invention, shown in Fig. 8, is around 2% at a wavelength of 1550 nm and about 98% at 1470 nm. This demonstrates that the optical fiber coupler of the present invention is less polarization-dependent than the conventional optical fiber coupler depicted in Fig. 4. The polarization dependence of the branching ratio is ± 1% at a wavelength of 1555 nm, which is appreciably better than in the prior art. The reason for which the polarization dependence can be reduced is that the length of the optical coupling portion 11 can be decreased. In the optical fibre coupler of Fig. 5 the refractive index 21N of the coupling control portion 21 between the cores 13a and 13b may also be chosen lower than the refractive indexes N CL of the claddings 12a and 12b as shown in Fig. 9, thus getting a device as known from US-A-4 589 725. In this instance, the coupling coefficient C between the cores 13a and 13b becomes equivalently smaller than in the case where the coupling control portion 21 is not provided and the effective coupling length of the optical coupling portion 11 becomes short, hence an optical fiber coupler of low wavelength dependence is obtained. Thus, the degree of effective coupling between the cores 13a and 13b can be reduced irrespective of the size and shape of each optical fiber which is used to fabricate the optical fiber coupler. The coupling control portion 21 may also be located apart from the center between the cores 13a and 13b, as shown in terms of the refractive index distribution in Fig. 10, by fusing together two optical fibers of different diameters and having the optical layers 21a and 21b, respectively, and stretching them under the same condition or by fusing together two optical fibers of the same diameter and having the optical layers 21a and 21b, respectively, and stretching them under different conditions. By locating the coupling control portion 21 off the center between the cores 13a and 13b as mentioned above, it is possible to obtain an optical fiber coupler which has an asymetrical optical coupling portion, that is, an optical fiber coupler of a wide wavelength band. The manufacture of the optical fiber coupler which has the above-described coupling control 21 starts with the preparation of an optical fiber 22a which has the optical layer 21a formed around the outer periphery of the cladding 12a covering the core 13a and having a refractive index different from that of the cladding 12a and an optical fiber 22b which similarly has the optical layer 21b formed around the outer periphery of the cladding 12b covering the core 13b and having a refractive index different from that of the cladding 12b, as shown in Fig. 11. The optical fibers 22a and 22b may be obtained by the same method as an ordinary optical fiber manufacturing method, or by doping existing optical fibers with an impurity to form in their outer surface layers the optical layers 21a and 21b of refractive indexes different from those of the claddings 12a and 12b. In the case of the latter, it is also possible to form the optical layers 21a and 21b only in those portions of the optical fibers which will ultimately form the coupling control portion 21 of the optical coupling portion 11 between the two cores 13a and 13b. In the case where the claddings 12a and 12b are formed of pure quartz, the layers 21a and 21b are doped with titanium or gemanium, or boron, depending on whether their refractive indexes are made high or low. Such optical fibers 22a and 22b are held in contact with each other along their entire length and are partly fused together by heating and the fused portion is stretched or elongated to form the optical coupling portion. The fusion and stretching or elongation of the optical fibers can be carried out by the same techniques as those for the fabrication of conventional optical fiber couplers of this kind. While in the above the present invention has been described as being applied to the optical fiber coupler including the two cores 13a and 13b in the optical coupling portion 11, the invention is also applicable to an optical fiber coupler including three or more cores in the optical coupling portion 11 and its fabrication can be done by the same method as described above. In this instance, coupling between the plurality of cores may be effected by using different refractive indexes in the coupling control portion between them and the coupling control portion may be omitted in some part. That is, during manufacture at least one of the plurality of optical fibers may be one that has formed therearound a layer of a refractive index different from that of the cladding. Also in the case of fabricating an optical coupler with two optical fibers as shown in Fig. 11, it is possible to employ the one optical fiber 22a without the optical layer 21a and the other optical fiber 22b with the optical layer 21b. As described above, according to the present invention, since the coupling control portion having a refractive index higher than that of the claddings is provided between two optical fibres in the coupling region, it is possible to obtain an optical fiber coupler which has a short optical coupling portion, a branching ratio of narrow wavelength spacing, or low polarization dependence, by making the coupling coefficient C large. It was already known to obtain an optical fiber coupler of low wavelength dependence by selecting the coupling coefficient C small, and in this case, the optical fiber coupler is easy to manufacture and high in the production yield. It will be apparent that many modifications and variations may be effected without departing from the scope of the novel concepts of the present invention as claimed in the appended claims.

Claims: An optical fiber coupler obtainable by fusing together at least two optical fibers (12a, 13a, 12b, 13b) and stretching them, wherein claddings (12a, 12b) covering the cores (13a, 13b) of said at least two optical fibers are separated by an optical coupling control portion (21) inserted between the claddings of the fused optical fibers, the optical coupling control portion having a refractive index different from those of said claddings, characterized in that the refractive index of said optical coupling control portion (21) is higher than the refractive indexes of said claddings. The optical fiber coupler of claim 1 wherein said optical coupling control portion (21) is an optical layer formed around the cladding (12a, 12b) of at least one of said two optical fibers. A method of manufacturing an optical fiber coupler, according to claim 1 comprising the steps of: (a) preparing a plurality of optical fibers (12a, 13a, 12b, 13b), at least one of which has an optical medium(21a, 21b) around the outer periphery of its cladding (12a, 12b) said medium having a refractive index higher than that of the cladding, (b) holding said plurality of optical fibers partly in contact with each other lengthwise thereof, (c) fusing the optical fibers together by heating and (d) then stretching the fused portion.

Inventors: NAMIHIRA YOSHINORI, SASAKI HIROYUKI, SHIMAMURA MASATO, YOSHIDA YOSHIHIRO, NAMIHIRA, YOSHINORI, SASAKI, HIROYUKI, SHIMAMURA, MASATO, YOSHIDA, YOSHIHIRO, SASAKI, HIROYUKI, C/O JAPAN AVIATION ELECTRONICS, SHIMAMURA, MASATO, C/O JAPAN AVIATION ELECTRONICS
Applicants: JAPAN AVIATION ELECTRON, KOKUSAI DENSHIN DENWA CO LTD, JAPAN AVIATION ELECTRONICS INDUSTRY, LIMITED, KOKUSAI DENSHIN DENWA CO., LTD
Application year: 1992
Main classification: C03B37
IPC codes: G02B6