Multicore fiber and optical cable

Abstract

A multicore fiber that includes: three or more cores that transmit in single-mode transmission; a common clad that covers a periphery of the three or more cores; and a low-refractive index portion that has a refractive index lower than a refractive index of the clad. The multicore fiber further includes a region having the three or more cores arranged annularly on a cross-section perpendicular to a longitudinal direction. At least a portion of the low-refractive index portion is arranged inside a minimum inscribed circle of two adjacent cores within the region.

Claims

1. A multicore fiber comprising: three or more cores that transmit in single-mode transmission; a common clad that covers a periphery of the three or more cores; and a low-refractive index portion that has a refractive index lower than a refractive index of the clad, wherein the multicore fiber includes two or more regions, the three or more cores are arranged annularly in a cross-section perpendicular to a longitudinal direction, each of the three or more cores is disposed in one of the two or more regions, a plurality of cores of the three or more cores in a same region are coupled cores, transmission modes are mutually independent of each other between the regions, and at least a portion of the low-refractive index portion is arranged inside a minimum inscribed circle of two adjacent cores within the same region.

2. The multicore fiber according to claim 1, wherein the multicore fiber is a coupled type multicore fiber.

3. The multicore fiber according to claim 2, wherein the low-refractive index portion is a hole.

4. An optical cable comprising the multicore fiber according to claim 2 in at least a portion thereof.

5. An optical cable comprising the multicore fiber according to claim 3 in at least a portion thereof.

6. The multicore fiber according to claim 1, wherein the low-refractive index portion is a hole.

7. An optical cable comprising the multicore fiber according to claim 6 in at least a portion thereof.

8. An optical cable comprising the multicore fiber according to claim 1 in at least a portion thereof.

9. The multicore fiber according to claim 1, wherein the low-refractive index portion is a hole.

10. An optical cable comprising the multicore fiber according to claim 9 in at least a portion thereof.

11. An optical cable comprising the multicore fiber according to claim 1 in at least a portion thereof.

Description

BRIEF DESCRIPTION OF DRAWINGS

(1) FIG. 1 is a cross-sectional view illustrating an example of a multicore fiber according to one or more embodiments of the present invention.

(2) FIG. 2A is a schematic diagram (photograph in substitution for a drawing) illustrating a first supermode in the field distribution of a 6-core C-MCF according to one or more embodiments.

(3) FIG. 2B is a schematic diagram (photograph in substitution for a drawing) illustrating a sixth supermode in the field distribution of the 6-core C-MCF according to one or more embodiments.

(4) FIG. 3 is a graph illustrating an example of the hole radius dependency of n.sub.eff in a hole-addition 6-core C-MCF according to one or more embodiments.

(5) FIG. 4 is a graph illustrating an example of the hole radius dependency of DGD in the hole-addition 6-core C-MCF according to one or more embodiments.

DETAILED DESCRIPTION

(6) Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings.

(7) FIG. 1 is a cross-sectional view of a coupled multicore fiber (C-MCF: hereinafter, called a multicore fiber) 10 according to one or more embodiments. The multicore fiber 10 according to one or more embodiments is constituted by six cores 11, a clad 12, and six low-refractive index portions 13.

(8) As shown in FIG. 1, the radius of the core 11 is set to a, the distance between cores (distance between centers of the core) is set to , and the radius of the low-refractive index portion 13 is set to r. In addition, the refractive index of the core 11 is set to n.sub.core, and the refractive index of the clad 12 is set to n.sub.clad. The refractive index n.sub.core of the core 11 is larger than the refractive index n.sub.clad of the clad 12. In addition, in FIG. 1, the distance between the centers of the core 11 and the low-refractive index portion 13 is /2.

(9) In all the cores 11, single-mode transmission can be performed in a transmission band. The cores 11 are all constituted by an identical type of core. The effective refractive indexes of the cores 11 may be nearly equal to each other. The number of cores 11 is not limited to six, and, for example, three or more cores may be arranged.

(10) The clad 12 is a common clad that covers the periphery of all the cores 11.

(11) The low-refractive index portion 13 is constituted by a medium such as, for example, a hole which has a refractive index lower than that of the clad 12. The medium constituting the low-refractive index portion 13 may be solid, liquid, and gaseous. In a case where low-refractive index portion 13 is solid, the low-refractive index portion can be formed by inserting a rod-shaped member into the clad. In a case where the low-refractive index portion 13 is fluid (liquid or gaseous), the low-refractive index portion can be formed as a hole of the clad 12. Gas within the hole may be air, and the outer air of the MCF may be introduced into the hole. The inside of the hole may be vacuum.

(12) The cores 11 are arranged annularly on a cross-section perpendicular to the longitudinal direction of the multicore fiber 10. In one or more embodiments, the multicore fiber 10 is a 6-core C-MCF, and has six cores. FIGS. 2A and 2B illustrate the field distribution of the 6-core C-MCF. In the 6-core C-MCF, in a case where the respective cores operate in a single mode, six supermodes are present. Among the supermodes, FIG. 2A illustrates a first supermode (1st), and FIG. 2B illustrates a sixth supermode (6th). The electric fields of six cores have the same sign in the basic (first) supermode. On the other hand, nodes are formed in which the sign of an electric field (field) is reversed between the cores in the higher-order (second to sixth) supermode. In the sixth supermode, respective nodes are formed between two cores adjacent to each other. Among these nodes, the effective refractive index n.sub.eff of the basic supermode is highest, and n.sub.eff of the higher-order supermode is lower than n.sub.eff of the basic supermode.

(13) The first supermode has an even-symmetric field distribution between cores adjacent to each other, whereas the sixth supermode has an odd-symmetric field distribution between cores adjacent to each other. That is, the sixth supermode is less in the localization of power than the first supermode, in a region between cores adjacent to each other. Consequently, when a low-refractive index portion is provided in a region in which the power of the first supermode is localized as compared with the power of the sixth supermode, n.sub.eff of the first supermode decreases more greatly than n.sub.eff of the sixth supermode. Thereby, the difference n.sub.eff of n.sub.eff between supermodes decreases, and thus it is possible to enhance coupling between supermodes. As a result, in a case where the same degree of DGD as that of a C-MCF not including a low-refractive index portion is attempted to be obtained, the distance between cores is made smaller, and thus it is possible to improve the degree of spatial multiplexing. In addition, in a case where the same degree of the distance between cores as that of the C-MCF not including a low-refractive index portion is provided, it is possible to further reduce the DGD. The DGD of a MCF may be, for example, equal to or less than 500 ps/km, and may be equal to or less than 200 ps/km.

(14) Here, a relationship between the first supermode and the highest-order (sixth) supermode of the 6-core C-MCF will be described. The relationship between the first supermode and the highest-order (sixth) supermode of 3 or more-core MCF is same as the 6-core C-MCF. The number of cores included annularly may be an odd number (3, 5, 7, . . . ) equal to or greater than 3, and may be an even number (4, 6, 8, . . . ) equal to or greater than 4. In addition, even in higher-order supermodes (second to fifth supermodes in a case of 6 cores) rather than the highest-order supermode, points having an odd-symmetric field distribution between cores adjacent to each other are present, and thus an effect is obtained with respect to the second or higher-order supermodes.

(15) At least a portion of the low-refractive index portion 13 may be arranged inside the minimum inscribed circle which contacts with adjacent two cores to each other among a plurality of cores arranged annularly. Here, the minimum inscribed circle refers to a circle in which a shortest distance between two regions (cores) is set to a diameter. In the case of FIG. 1, a radius of each inscribed circle is (/2)a. The low-refractive index portion 13 may include the center of the inscribed circle. The entire low-refractive index portion 13 may be arranged inside the inscribed circle. The center of the low-refractive index portion 13 may be coincident with the center of inscribed circle. The low-refractive index portion 13 may not be in contact with the core, and the clad may cover the periphery of the low-refractive index portion 13. The radius r of the low-refractive index portion 13 may be smaller than (/2)a which is the radius of the minimum inscribed circle of two cores adjacent to each other. In a case where distances A which is between cores are not constant with respect to all the cores (outer circumferences) arranged annularly, a inscribed circle having a different radius may be set for each of two cores adjacent to each other.

(16) In the example shown in FIG. 1, a case is shown in which the MCF has one region (coupled core region) including a plurality of cores arranged annularly, but the present invention is not limited to this case. The respective cores may have an identical type or different types. The MCF may have two or more coupled core regions, and may have one or more coupled core region and one or more uncoupled cores. Here, the coupled core region refers to a region in which supermodes occurring between a plurality of cores included in the region can be used in transmission. In addition, the uncoupled core refers to a core, having a single core included therein, in which transmission modes are independent of each other between the core and other cores.

(17) In a MCF including two or more coupled core regions, transmission modes are mutually independent of each other between coupled core regions (that is, the respective regions are not coupled to each other). In the MCF including two or more coupled core regions, a low-refractive index portion may be provided in one or more coupled core regions. Thereby, in the coupled core region having a low-refractive index portion provided therein, the distance between cores within the region can be reduced. As a result, the distance between a core in one region and a core in another region is increased, and thus it is possible to reduce crosstalk between the regions.

(18) Hereinbefore, although the embodiments of the present invention have been described, the present invention is not limited to the above-described embodiments, and can be modified variously without departing from the scope of the embodiments of the present invention.

(19) According to one or more embodiments, the MCF can be used as a portion or the entirety of an optical fiber which is used in an optical transmission line, an optical waveguide, an optical cable, or the like. The optical cable may include the MCF in at least a portion thereof.

(20) An example of a medium constituting cores and a clad of the MCF includes silica-based glass (silica glass), multicomponent glass, plastic, or the like. An example of the silica-based glass includes pure silica glass having no additives contained therein, and silica-based glass having additives contained therein. An example of the additives includes Ge, Al, P, B, F, Cl, and one type or two types of alkali metal or the like.

(21) In the C-MCF, similarly to a case of the FMF, coupling between modes occurs due to various perturbations (micro-bend, twist or the like) in a transmission line, and thus it is considered that MIMO processing is required similarly to normal MDM transmission on the receiving side. In that case, it is possible to achieve a reduction in the load of signal processing of MIMO or the like by using the multicore fiber which is obtained by reducing the DGD.

(22) A wavelength band which is used in transmission in the MCF is not particularly limited, and an example thereof includes a C band (1,530 to 1,565 nm), an L band (1,565 to 1,625 nm), or the like. In single-mode operation conditions in use wavelength band, single-mode operation conditions of v2.405 as a normalized frequency v=2a(n.sub.core.sup.2n.sub.clad.sup.2).sup.1/2/ may be satisfied. A relative refractive index difference =(n.sub.core.sup.2n.sub.clad.sup.2)/(2n.sub.core.sup.2) is equal to or greater than 0.05%, and the upper limit of the core radius in which v2.405 is establish in a C+L band is approximately 13 m. The value of in which v2.405 is established in each core radius can be automatically determined. is a wavelength, and 2/ is a wavenumber k.sub.0.

(23) In addition, in the value a or having a relation of v2.405, a transmission loss in a higher-order mode equal to or greater than an LP.sub.11 mode may be equal to or greater than .sub.Loss. In this case, a relation of .sub.Loss>0 dB/m is established, and an example of this value includes 0.1 dB/m, 0.5 dB/m, 1.0 dB/m, 2.0 dB/m, or the like. An example of the cable cutoff wavelength .sub.cc of a fiber includes 1,260 nm or less, 1,000 nm or less, or the like.

(24) As shown in Reference Literature 1 (Okamoto, Foundation of Optical Waveguide, Corona Publishing Co., Ltd.), in a case where a, and are fixed, the coupling constant of a fiber-type directional coupler is dependent on the normalized frequency v (the same is true of V). In a case where the wavelength is changed in the range of a C+L band, a change in the v value is a maximum of approximately 0.15, and the value of the coupling constant does not much change. In a case where the core diameter a and the relative refractive index difference are fixed, the coupling constant of the fiber-type directional coupler decreases approximately exponentially with an increase in /a.

(25) From the above, it is considered to be close to a normal FMF in a case where /a is excessively small, and to be close to an uncoupled MCF in a case where /a is excessively large. An example of the lower limit of /a includes 2.0, 2.2, 2.4, 2.6, 2.8, 3.0, or the like. In addition, an example of the upper limit of /a includes 5.0, 5.2, 5.4, 5.6, 5.8, 6.0, or the like. An example of the value of /a includes an appropriate value such as 3.2, 3.5, 4.0, 4.5, 4.8, or 5.0.

(26) The shortest distance (-2a) between cores adjacent to each other has a relation of -2a0 m, and an example thereof includes 0.1 m, 0.3 m, 0.5 m, 0.7 m, 1.0 m, 2.0 m, 5.0 m, 10.0 m, 15.0 m, 17.0 m, or the like.

(27) The radius r of the low-refractive index medium (such as a hole) is not particularly limited, and has a relation of r>0 m. An example of the lower limit of r includes 0.1 m, 0.25 m, 0.5 m, 0.7 m, 1.0 m, 1.5 m, 2.0 m, 2.5 m, 3.0 m, or the like.

(28) The shortest distance ((/2)ar, for example, in a case where the center of the low-refractive index portion is located at the central point between cores adjacent to each other) between the core and the low-refractive index portion has a relation of raa.sub.20 m, and an example thereof includes 0.1 m, 0.3 m, 0.5 m, 0.7 m, 1.0 m, 1.5 m, 2.0 m, 2.5 m, 3.0 m, or the like.

Example

(29) Here, the transmission characteristics of a hole-addition 6-core coupled fiber for mode division multiplexing transmission are analyzed, and the supermode characteristics (effective refractive index and group delay) of the MCF are evaluated by full-vectorial finite-element scheme analysis (Reference Literature 2: K. Saitoh and M. Koshiba, Full-vectorial imaginary-distance beam propagation method based on a finite element scheme: application to photonic crystal fibers, IEEE J. Quantum Electronics, vol. 38, no. 7, pp. 927-933, July 2002). By adding holes between cores adjacent to each other, an effective refractive index difference between supermodes is reduced and coupling between modes is enhanced. Thereby, even in a case where the distance between cores is reduced, it is possible to reduce the effective refractive index difference between supermodes, and simultaneously to reduce differential mode group delay.

(30) Regarding an identical type of 6-core C-MCF not including a low-refractive index portion, and an identical type of 6-core C-MCF provided with a hole as the low-refractive index portion between cores adjacent to each other, as shown in FIG. 1, analyses are performed as follows. Here, the radius of the core 11 is set to a, the refractive index of the core 11 is set to n.sub.core, and the refractive index of the clad 12 is set to n.sub.clad. In the shown example, each core 11 is arranged on the peak of a regular hexagon of which the centroid is set to the center of a fiber.

(31) The refractive indexes of the core and the clad are calculated by the Sellmeier equation, in consideration of wavelength dependency. In a case where holes are added, the radius of the holes is set to r, and the refractive index of the holes is set to 1.0. in a case where no hole is added, the radius r of the hole is set to 0 m. In addition, the distance between the centers of cores is set to .

(32) In the disposition of a regular hexagon, the distance from the center of a fiber to the center of each core is also set to . Further, the relative refractive index difference of the core with respect to the clad is set to =(n.sub.core.sup.2n.sub.clad.sup.2)/(2n.sub.core.sup.2). The value of the normalized frequency V is V=k.sub.0a(n.sub.core.sup.2n.sub.clad.sup.2).sup.1/2. Here, k.sub.0 is a free-space wavenumber.

(33) In the present example, is set to be equal to or less than 28 m. This is a value which is the same as or smaller than the distance A=28 m between cores of Non-Patent Document 3 (ECOC2014, PD.3.2) which is an identical type of 6-core C-MCF not including a low-refractive index portion in the center. As parameters of the 6-core C-MCF common to the respective analysis examples, a is set to 5.55 m, is set to 0.32 m, the wavelength is set to 1,550 nm, and the clad diameter is set to 125 m. In addition, as described above, the number of propagation modes in the 6-core C-MCF is six, and the propagation modes are called the first to sixth supermodes (1.sup.st, 2.sup.nd, 3.sup.rd, 4.sup.th, 5.sup.th, and 6.sup.th, respectively, in FIGS. 2A to 4), respectively.

(34) DGD between the first and m.sup.th supermodes of this fiber and n.sub.eff are defined as DGD=.sub.mth.sub.1st and n.sub.eff=n.sub.eff.sub._.sub.mthn.sub.eff.sub._.sub.1st, respectively. Here, .sub.1st and .sub.mth indicate group delay times of the first and m.sup.th modes, respectively, and n.sub.eff.sub._.sub.1st and n.sub.eff.sub._.sub.mth indicate effective refractive indexes of the first and m.sup.th modes, respectively.

(35) Regarding the fiber, as shown in FIG. 1, holes are added between cores, and thus n.sub.eff is reduced even in a case where the distance between cores is reduced. Therefore, it is shown that the coupling between modes is enhanced, and that the DGD can be reduced.

(36) In the sixth supermode, an electric field is constantly set to 0 between cores due to its symmetry, as shown in FIG. 2B, regardless of the presence or absence of a hole. On the other hand, in the basic supermode, it can be understood from FIG. 2A that the electric field between cores has a large value. That is, when focused on two cores adjacent to each other, these cores are even-symmetric in the first supermode, and are odd-symmetric in the sixth supermode. Thus, with little influence on the sixth supermode by adding a hole between cores, it is possible to reduce n.sub.eff of the first supermode, and to reduce the effective refractive index difference n.sub.eff between the basic (first) supermode and the higher-order (sixth) supermode.

(37) FIG. 3 shows the hole radius dependency of n.sub.eff in the second to sixth supermodes of an identical type of 6-core C-MCF. In this case, the distance A between cores is 28.0 m. From FIG. 3, it can be understood that it is possible to reduce each n.sub.eff between the first and higher-order (second to sixth) supermodes by enlarging the holes.

(38) In addition, FIG. 4 shows the hole radius dependency of the DGD between the first supermode and the sixth supermode in a case where A is 20 m, 24 m, or 28 m. From FIG. 4, it can be understood that it is possible to reduce the DGD by increasing a hole.

(39) From the above, it can be understood that a hole is added between the cores of the 6-core C-MCF, and thus it is possible to reduce the effective refractive index difference n.sub.eff between the supermodes, to enhance coupling between modes, and to reduce the differential mode group delay DGD.

REFERENCE SIGNS LIST

(40) 10: multicore fiber 11: core 12: clad 13: low-refractive index portion

(41) Although the disclosure has been described with respect to only a limited number of embodiments, those skilled in the art, having benefit of this disclosure, will appreciate that various other embodiments may be devised without departing from the scope of the present invention. Accordingly, the scope of the invention should be limited only by the attached claims.