OPTICAL FIBER

Abstract

An optical fiber that communicates in a predetermined communication band includes: a signal light propagation core that propagates light beams of up to (x+1)-th order LP mode, where x is an integer of two or more; and a coupler that propagates a light beam that is: coupled with a light beam of the (x+1)-th order LP mode propagating through the signal light propagation core, and suppressed from being coupled with light beams of up to the x-th order LP mode propagating through the signal light propagation core, wherein, mode coupling of the light beams of up to the x-th order LP mode propagating through the signal light propagation core is performed, and mode coupling between the light beam of the x-th order LP mode and the light beam of (x+1)-th order LP mode is suppressed.

Claims

1. An optical fiber that communicates in a predetermined communication band, the optical fiber comprising: a signal light propagation core that propagates light beams of up to (x+1)-th order LP mode, where x is an integer of two or more; and a coupler that propagates a light beam that is: coupled with a light beam of the (x+1)-th order LP mode propagating through the signal light propagation core, and suppressed from being coupled with light beams of up to the x-th order LP mode propagating through the signal light propagation core, wherein, mode coupling of the light beams of up to the x-th order LP mode propagating through the signal light propagation core is performed, and mode coupling between the light beam of the x-th order LP mode and the light beam of (x+1)-th order LP mode is suppressed.

2. An optical fiber that communicates in a predetermined communication band, the optical fiber comprising: a signal light propagation core that propagates light beams of (x+2)-th order LP mode and higher, where x is an integer of two or more; and a coupler that propagates a light beam that is: coupled with a light beam of any of (x+1)-th order LP mode and higher propagating through the signal light propagation core, and suppressed from being coupled with light beams of up to the x-th order LP mode propagating through the signal light propagation core, wherein, mode coupling of the light beams of up to the x-th order LP mode propagating through the signal light propagation core is performed, mode coupling between the light beam of the x-th order LP mode and the light beam of (x+1)-th order LP mode is suppressed, and mode coupling of the light beams of the (x+1)-th order LP mode and higher propagating through the signal light propagation core is performed.

3. The optical fiber according to claim 1, wherein the signal light propagation core comprises: an inner core having a center axis; and an outer core that surrounds an outer circumferential surface of the inner core and has a refractive index higher than that of the inner core.

4. The optical fiber according to claim 1, wherein the coupler loses more of a light beam propagating therethrough than the signal light propagation core.

5. The optical fiber according to claim 1, wherein the coupler is a clad that surrounds an outer circumferential surface of the signal light propagation core.

6. The optical fiber according to claim 5, wherein relationships (1) and (2) below are satisfied:
n.sub.effa<n.sub.effc; and (1):
n.sub.effb<n.sub.effc, where (2): n.sub.effa is a maximum value among effective refractive index differences between light beams of LP modes having effective refractive indexes that are adjacent to each other except for the x-th order LP mode and the (x+1)-th order LP mode, n.sub.effb is a difference between an effective refractive index of a light beam of the highest order LP mode propagating through the signal light propagation core and a refractive index of the clad, and n.sub.effc is a difference between an effective refractive index of the light beam of the x-th order LP mode and an effective refractive index of the light beam of (x+1)-th order LP mode.

7. The optical fiber according to claim 6, wherein relationship (3) below is satisfied:
n.sub.effb<n.sub.effa. (3):

8. The optical fiber according to claim 1, wherein the coupler is a side core that is parallel to the signal light propagation core.

9. The optical fiber according to claim 8, wherein relationships (1) to (4) below are satisfied:
n.sub.effa<n.sub.effc; (1):
n.sub.effa<n.sub.effd; (2):
n.sub.effb<n.sub.effc; and (3):
n.sub.effb<n.sub.effd, where (4): n.sub.effa is a maximum value among effective refractive index differences between light beams of LP modes having effective refractive indexes that are adjacent to each other except for the x-th order LP mode and the (x+1)-th order LP mode, n.sub.effb is a minimum value among differences between the effective refractive indexes of the light beams of (x+1)-th order LP mode and higher propagating through the signal light propagation core and an effective refractive index of a light beam of at least one mode propagating through the side core, n.sub.effc is a difference between an effective refractive index of the light beam of the x-th order LP mode and an effective refractive index of the light beam of (x+1)-th order LP mode, and n.sub.effd is a minimum value among differences between the effective refractive index of the light beam of the x-th order LP mode and the effective refractive indexes of the light beams of the modes propagating through the side core.

10. The optical fiber according to claim 9, wherein relationship (5) below is satisfied:
n.sub.effb<n.sub.effa (5):

11. The optical fiber according to claim 8, wherein the side core is a single mode core.

12. The optical fiber according to claim 1 comprising a plurality of the signal light propagation cores.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0031] FIG. 1 is a sectional view perpendicular to the longitudinal direction of an optical fiber according to one or more embodiments.

[0032] FIG. 2 is a diagram illustrating an example of a refractive index profile and effective refractive indexes of the optical fiber of FIG. 1.

[0033] FIG. 3 is a sectional view perpendicular to the longitudinal direction of an optical fiber according to one or more embodiments.

[0034] FIG. 4 is a diagram illustrating an example of a refractive index profile and effective refractive indexes of the optical fiber of FIG. 3.

[0035] FIG. 5 is a diagram illustrating another example of a refractive index profile and effective refractive indexes of the optical fiber of FIG. 3.

[0036] FIG. 6 is a sectional view perpendicular to the longitudinal direction of an optical fiber according to one or more embodiments.

[0037] FIG. 7 is a sectional view perpendicular to the longitudinal direction of an optical fiber according to one or more embodiments.

DESCRIPTION

[0038] Hereinafter, embodiments of an optical fiber according to the present invention will be described in detail with reference to the drawings. In order to facilitate understanding, the scales in the drawings may be different from the scales described in the following description.

[0039] FIG. 1 is a sectional view that is perpendicular to the longitudinal direction of an optical fiber according to one or more embodiments. As illustrated in FIG. 1, an optical fiber 1 includes a core 10 through which signal light propagates, a clad 20 that surrounds the outer circumferential surface of the core 10 with no gap, and a coating layer 30 that coats the outer circumferential surface of the clad 20. The core 10 includes an inner core 11 including the center axis of the core 10, and an outer core 12 surrounding the outer circumferential surface of the inner core 11 with no gap. The core 10 is a signal light propagation core through which signal light propagates.

[0040] FIG. 2 is a diagram illustrating an example of a refractive index profile and effective refractive indexes of the optical fiber 1 of FIG. 1. As illustrated in FIG. 2, the outer core 12 has a refractive index higher than the refractive index of the inner core 11 and the refractive index of the clad 20, and has a refractive index profile of a ring type. In one or more embodiments, the inner core 11 is made to have a refractive index that is substantially identical to that of the clad 20. Further, in FIG. 2, the effective refractive indexes of light beams of LP modes propagating through the cores 10 and the refractive index of the clad are indicated by broken lines.

[0041] The optical fiber 1 is an optical fiber that communicates using light beams of up to x-th order LP mode (x is an integer of two or more) in a predetermined communication band. However, in this communication band, the core 10 allows propagation of light beams of (x+1)-th order LP mode and higher. FIG. 2 illustrates an example where x is three, and light beams of five LP modes propagate. In FIG. 2, the five LP modes are indicated as mode 1 to mode 5. Mode 1 is indicated as LP.sub.01 mode, mode 2 is indicated as LP.sub.11 mode, mode 3 is indicated as LP.sub.21 mode, mode 4 is indicated as LP.sub.02 mode, and mode 5 is indicated as LP.sub.31 mode. However, the mode 3 may be indicated as LP.sub.02 mode, and the mode 4 may be indicated as LP.sub.21 mode. As described above, through the optical fiber 1 of the example illustrated in FIG. 2, the light beams of five LP modes propagate in the communication band. However, since x is set to three as described above, the optical fiber 1 communicates using only the light beams of three LP modes: mode 1 to mode 3, and the light beams of mode 4 and mode 5 propagating through the optical fiber 1 are regarded as unnecessary light beams that are not used for communication. In the present specification, when a light beam of x-th order LP mode is referred, LP modes are referred as the first order LP mode (mode 1), the second order LP mode (mode 2), and the third order LP mode (mode 3), in the descending order of the effective refractive index.

[0042] In addition, the optical fiber 1 is configured such that light beams of up to x-th order LP mode used for communication are mode coupled. In the example of FIG. 2, the optical fiber 1 is configured such that the light beam of mode 1, the light beam of mode 2, and the light beam of mode 3 are mode coupled with each other. That is, the effective refractive index of the light beam of mode 1 and the effective refractive index of the light beam of mode 2 are set to have a difference small enough to cause mode coupling, and the effective refractive index of the light beam of mode 2 and the effective refractive index of the light beam of mode 3 are set to have a difference small enough to cause mode coupling.

[0043] Further, the optical fiber 1 is configured such that the light beams of (x+1)-th order LP mode and higher propagating through the core 10 are mode coupled separately from the light beams of up to x-th order LP mode. In the example of FIG. 2, the effective refractive index of the light beam of mode 4 and the effective refractive index of the light beam of mode 5 are set to have a difference small enough to cause mode coupling of the light beam of mode 4 and the light beam of mode 5. Here, n.sub.effa is defined as the maximum value among the effective refractive index differences between light beams of LP modes having effective refractive indexes that are adjacent to each other except for x-th order LP mode and (x+1)-th order LP mode. In the example of FIG. 2, the maximum effective refractive index difference among the effective refractive index difference between the light beams of mode 1 and mode 2, the effective refractive index difference between the light beams of mode 2 and mode 3, and the effective refractive index difference between the light beams of mode 4 and of mode 5 is n.sub.effa. The value n.sub.effa is set small enough to cause mode coupling (for example, 1.010.sup.3 or less, 2.010.sup.3 or less, etc.).

[0044] As described above, the light beams of (x+1)-th order LP mode and higher cause mode coupling separately from the light beams of up to x-th order LP mode. Thus, mode coupling of the light beam of x-th order LP mode and the light beam of (x+1)-th order LP mode is suppressed. Here, n.sub.effc is defined as the difference between the effective refractive index of the light beam of x-th order LP mode, which is the highest order LP mode used for communication, and the effective refractive index of the light beam of (x+1)-th order LP mode, which is the lowest order LP mode not used for communication. The relationship:

n.sub.effa<n.sub.effc

is then satisfied. The value n.sub.effc is set large enough to suppress mode coupling between the light beam of x-th order LP mode and the light beam of (x+1)-th order LP mode. In the example of FIG. 2, the difference between the effective refractive index of the light beam of mode 3 and the effective refractive index of the light beam of mode 4 is n.sub.effc, and the mode coupling is suppressed between the light beam of mode 3 and the light beam of mode 4.

[0045] Further, any of the light beams of (x+1)-th order LP mode and higher propagating through the core 10 is coupled with the light beam of the clad mode propagating through the clad 20. A light beam that is most likely to be coupled with the light beam of the clad mode is the light beam of the highest order LP mode propagating through the core 10. Therefore, now n.sub.effb is defined as the difference between the effective refractive index of the light beam of the highest order LP mode propagating through the core 10 and the refractive index of the clad 20. In the example of FIG. 2, the difference between the effective refractive index of the light beam of mode 5 and the refractive index of the clad is n.sub.effb. Thus, the value n.sub.effb is made smaller than a predetermined value so that the light beam of mode 5 can be coupled with the light beam of the clad mode propagating through the clad 20. Specifically, the relationship:

n.sub.effb<n.sub.effc

is satisfied.

[0046] Further, the relationship:

n.sub.effb<n.sub.effa

may be satisfied.

[0047] Since the light beam of mode 1, the light beam of mode 2 and the light beam of mode 3 are mode coupled with each other as described above, if n.sub.effb is smaller than n.sub.effa, the light beam of the highest order LP mode propagating through the core 10 (the light beam of mode 5) can be more appropriately coupled with the light beam of the clad mode propagating through the clad 20. However, when n.sub.effa is sufficiently small, the light beam of mode 5 can be coupled with the light beam of the clad mode propagating through the clad 20.even when n.sub.effb is larger than n.sub.effa. As described above, in one or more embodiments, the clad 20 is a member through which a light beam to be coupled with light beams of unnecessary LP modes, which are not used for communication, propagates. Thus, the clad 20 can be regarded as a coupled member (or coupler). In addition, the clad 20 is coated with the coating layer 30, and the light beam propagating through the clad 20 is absorbed by the coating layer 30. Therefore, the clad 20 causes lose of the light beam propagating therethrough than the core 10.

[0048] Incidentally, in one or more embodiments, n.sub.effd is defined as the difference between the effective refractive index of the light beam of x-th order LP mode and the refractive index of the clad 20. The difference between the effective refractive index of the light beam of mode 3 and the refractive index of the clad 20 is n.sub.effd in the example of FIG. 2. In this case, n.sub.effd is larger than n.sub.effc, and coupling of the light beams of up to x-th order LP mode propagating through the core with the light beam of the clad mode is suppressed. Thus, in the example of FIG. 2, coupling of the light beams of mode 1 to mode 3 propagating through the core with the light beam of the clad mode is suppressed.

[0049] As described above, the optical fiber 1 of one or more embodiments is an optical fiber that communicates using the light beams of up to x-th order LP mode (x is an integer of two or more) in a predetermined communication band, and the core 10 allows propagation of the light beams of (x+1)-th order LP mode and higher. Therefore, the light beams of up to x-th order LP mode used for communication can be firmly confined in the core 10, the effective refractive index differences between the light beams of up to x-th order mode can be reduced, and the light beams up to x-th order LP mode can be easily mode coupled with each other. Further, the light beam of the clad mode propagating through the clad 20 as a coupled member is coupled with the light beam of the highest order LP mode propagating through the core 10, and the light beams of (x+1)-th order LP mode and higher propagating through the core 10 are mode coupled with each other separately from the light beams of up to x-th order LP mode. Thus, it is possible to release the light beams of (x+1)-th order LP mode and higher, which are not used for communication, to the clad 20 to attenuate the light beams. Therefore, it is possible to suppress the influence of light beams of the LP modes that are not used for communication on light beams of the LP modes used for communication. Thus, according to the optical fiber 1 of one or more embodiments, light beams of a plurality of modes used for communication are mode coupled with each other while propagating properly.

[0050] In the example illustrated in FIGS. 1 and 2, the light beam of mode 4 and the light beam of mode 5 are regarded as the light beams of (x+1)-th order LP mode and higher, and the light beams of (x+1)-th order LP mode and higher are mode coupled with each other. However, when a light beam of only one mode is included in light beams of (x+1)-th order LP mode and higher includes, there is no concept of mode coupling of light beams of (x+1)-th order LP mode and higher. For example, when mode 5 does not exist in FIG. 2, and the light beam of mode 4 is coupled with the light beam of the clad mode, the light beam of mode 4 need not be coupled with a light beam of another mode in the core 10.

[0051] In addition, in one or more embodiments, the core 10 has a refractive index profile of a ring type. Therefore, the light beams up to the predetermined LP mode can easily be coupled with each other, and the effective refractive index of a light beam of the predetermined LP mode and the effective refractive index of a light beam of the LP mode next to the predetermined LP mode can be separated. For example, as in the above-described embodiments, a design that enables easy mode coupling of the light beam of the LP.sub.01 mode, the light beam of the LP.sub.11 mode, and the light beam of the LP.sub.21 mode with each other by making their effective refractive indexes close to each other, and enables suppression of mode coupling of the light beam of the LP.sub.02 mode and the light beams of up to the third LP mode by separating the effective refractive index of the light beam of the LP.sub.21 mode and the effective refractive index of the light beam of the LP.sub.02 mode, which is the fourth LP mode can be easily made.

[0052] Next, additional embodiments of the present invention will be described in detail with reference to FIGS. 3 to 5. Here, components that are identical or similar to those in the previously-described embodiments are indicated by the same reference numerals and the description thereof will not be repeated unless otherwise particularly mentioned.

[0053] FIG. 3 is a sectional view perpendicular to the longitudinal direction of the optical fiber according to one or more embodiments. As illustrated in FIG. 3, an optical fiber 2 is different from the optical fiber 1 of the previously-described embodiments in that the optical fiber 2 includes a side core 40 that is parallel to the core 10.

[0054] FIG. 4 is a diagram illustrating an example of a refractive index profile and effective refractive indexes of the optical fiber 2 of FIG. 3. As illustrated in FIG. 4, the refractive index of the side core 40 is higher than the refractive index of the clad 20. In one or more embodiments, the side core 40 is a single mode core in a predetermined communication band of the optical fiber 2. In FIG. 4, similarly to FIG. 2, the effective refractive indexes of light beams of modes propagating through the core 10 and the refractive index of the clad 20 are indicated by broken lines, and the effective refractive index of a light beam propagating through the side core 40 is indicated by a dotted line. Since the side core 40 is a single mode core as described above, the mode of light beam propagating through the side core 40 is indicated as mode 1.

[0055] In one or more embodiments, any of light beams of (x+1)-th order LP mode and higher propagating through the core 10 is coupled with a light beam propagating through the side core 40, and light beams of up to x-th order LP mode propagating through the core 10 are suppressed from coupling with the light beam propagating through the side core 40. In the example illustrated in FIG. 4, among the light beams of (x+1)-th order LP mode and higher, a light beam that is most likely to be coupled with the light beam propagating through the side core 40 is the light beam of mode 4, and the light beam of mode 3 is suppressed from being mode coupled with the light beam of mode 1 propagating through the side core 40.

[0056] Here, n.sub.effa and n.sub.effc are defined similarly to those in previously-described embodiments. In one or more embodiments, n.sub.effb is defined as the minimum value among differences between the effective refractive indexes of the light beams of (x+1)-th order LP mode and higher propagating through the core 10 and the effective refractive index of the light beam of the mode propagating through the side core 40. In the example illustrated in FIG. 4, the difference between the effective refractive index of the light beam of mode 4 propagating through the core 10 and the effective refractive index of the light beam of mode 1 propagating through the side core 40 is n.sub.effb. Further, n.sub.effd is defined as the minimum value among differences between the effective refractive index of the light beam of x-th order LP mode propagating through the core 10 and the effective refractive indexes of the light beams of the modes propagating through the side core 40. In the example illustrated in FIG. 4, the difference between the effective refractive index of the light beam of mode 3 and the effective refractive index of the light beam of mode 1 propagating through the side core 40 is n.sub.effd.

[0057] At this time, the light beam of (x+1)-th order LP mode propagating through the core 10 (the light beam of mode 4 in the example of FIG. 4) has to be coupled with the light beam propagating through the side core 40, and the light beam of x-th order LP mode (the light beam of mode 3 in the example of FIG. 4) has to be suppressed from being coupled with the light beam propagating through the side core 40. Thus, the relationship:

n.sub.effb<n.sub.effd

is satisfied.

[0058] In addition, as described above, the light beams of up to x-th order LP mode propagating through the core 10 have to be mode coupled with each other and the light beam of x-th order LP mode (the light beam of mode 3 in the example of FIG. 4) has to be suppressed from being coupled with the light beam propagating through the side core 40. Thus, the relationship:

n.sub.effa<n.sub.effd

is satisfied.

[0059] Similarly to the optical fiber 1 of previously-described embodiments, the relationship:

n.sub.effa<n.sub.effc

is satisfied.

[0060] In addition, as apparent from FIG. 4, the relationship:

n.sub.effb<n.sub.effc

is satisfied.

[0061] When the above conditions are satisfied, in the example of FIG. 4, the light beam of mode 4 can be coupled with the light beam propagating through the side core 40. In addition, since the light beams of (x+1)-th order LP mode and higher are mode coupled with each other separately from the light beams of up to x-th order LP mode, the light beam of mode 5 is coupled with the light beam of mode 4. Thus, the light beam of mode 5 can be coupled with the light propagating through the side core 40. As described above, in one or more embodiments, the side core 40 is a member through which a light beam to be coupled with unnecessary light beams, which are of LP modes not used for communication, propagates. Thus, the side core 40 can be regarded as a coupled member.

[0062] The side core 40 may lose light beams propagating therethrough than the core 10. There are some ways to make the side core 40 lose light beams as described above, and one of them is to distribute a hydroxyl group in a glass rod to be used as the side core 40 and make excessive oxygen to flow therethrough at the time of dehydration.

[0063] Next, another example of the effective refractive indexes of the optical fiber 2 will be described. FIG. 5 is a diagram illustrating another example of the refractive index profile and the effective refractive indexes of the optical fiber 2 of FIG. 3. As illustrated in FIG. 5, this example is different from the example illustrated in FIG. 4 in a point that the effective refractive index of the light beam of mode 1 propagating through the side core 40 is between the effective refractive index of the mode 4 propagating through the core 10 and the effective refractive index of the light beam of mode 5. In this example, the effective refractive index of the light beam of mode 1 propagating through the side core 40 is made closer to the effective refractive index of the light beam of mode 4 than to the effective refractive index of the light beam of mode 5 propagating through the core 10. Even when the effective refractive index of the light beam of mode 1 propagating through the side core 40 is not between the effective refractive index of the light beam of x-th order mode propagating through the core 10 and the effective refractive index of the light beam of the (x+1)-th order mode, the light beam of mode 4 can be coupled with the light beam propagating through the side core 40, and the light beam of mode 5 can then be coupled with the light beam propagating through the side core 40 by being coupled with the light beam of mode 4 when the expressions presented in the example of FIG. 4 are satisfied.

[0064] Although not illustrated in particular, when the effective refractive index of the light beam of mode 1 propagating through the side core 40 is smaller than the effective refractive index of the light beam of mode 5, that is, the effective refractive index of the light beam of mode 1 is between the effective refractive index of the light beam of mode 5 and the refractive index of the clad 20, the same conditions as in previously-described embodiments can be applied by defining n.sub.effb as the difference between the effective refractive index of the light beam of mode 5 and the effective refractive index of the light beam of mode 1 propagating through the side core 40.

[0065] As described above, according to the optical fiber 2 of one or more embodiments, the side core 40 serves as a coupled member. Thus, it is possible to extract the light beam of (x+1)-th order LP mode and higher that have been moved to the side core 40 can be extracted from the side core 40. In addition, since the light beams of (x+1)-th order LP mode and higher propagating through the core 10 do not have to be coupled with the light beam of the clad mode propagating through the clad 20, the degree of freedom in designing the core 10 can be improved.

[0066] Also in one or more embodiments, in the examples illustrated in FIGS. 3 to 5, the light beam of mode 4 and the light beam of mode 5 are the light beams of (x+1)-th order LP mode and higher, and the light beams of (x+1)-th order LP mode and higher are mode coupled with each other. However, when a light beam of only one mode is included in light beams of (x+1)-th order LP mode and higher, there is no concept of mode coupling of light beams of (x+1)-th order LP mode and higher. For example, when mode 5 does not exist in FIGS. 4 and 5, the light beam of mode 4 need not be coupled with a light beam of another mode in the core 10.

[0067] Next, additional embodiments of the invention will be described in detail referring to FIG. 6. Here, components that are identical or similar to those in the previously-described embodiments are indicated by the same reference numerals and the description thereof will not be repeated unless otherwise particularly mentioned.

[0068] FIG. 6 is a sectional view perpendicular to the longitudinal direction of the optical fiber according to one or more embodiments. As illustrated in FIG. 6, an optical fiber 3 of one or more embodiments is a multi-core optical fiber including a plurality of cores 10, which are described in the previously-described embodiments, and a clad 20 that is similar to the clad 20 of the previously-described embodiments. Therefore, the light beams of (x+1)-th order LP mode and higher propagating through the cores 10 are coupled with a light beam of the clad mode propagating through the clad 20.

[0069] According to the optical fiber 3 of one or more embodiments, each of the cores 10 allows propagation of a light beam to be mode coupled. Thus, it is possible to realize an optical fiber capable of transmitting a higher amount of information.

[0070] Next, additional embodiments of the invention will be described in detail referring to FIG. 7. Here, components that are identical or similar to those in the previously-described embodiments are indicated by the same reference numerals and the description thereof will not be repeated unless otherwise particularly mentioned.

[0071] FIG. 7 is a sectional view perpendicular to the longitudinal direction of the optical fiber according to one or more embodiments. As illustrated in FIG. 7, an optical fiber 4 of one or more embodiments is a multi-core optical fiber including a plurality of cores 10 and a plurality of side cores 40, which are described in the previously-described embodiments, and a clad 20 that is similar to the clad 20 of the previously-described embodiments.

[0072] According to the optical fiber 4 of one or more embodiments, each of the cores 10 allows propagation of a light beam to be mode coupled. Thus, it is possible to realize an optical fiber capable of transmitting a higher amount of information. The number of the side cores 40 may be the same as or different from the number of the cores 10. For example, in the example illustrated in FIG. 7, each of the side cores 40 is arranged adjacently to three of the cores 10 and can be coupled with light beams of (x+1)-th order LP mode and higher propagating through each of the cores 10 that are adjacent thereto.

(Design Examples of Optical Fiber)

[0073] Next, design examples of the optical fiber of the above-described embodiments will be described.

[0074] An optical fiber having the refractive index profile of FIG. 1 was designed. In this optical fiber, the radius r1 of the inner core 11 was set to 4.5 m, the radius of the outer periphery of the outer core 12 was set to 13.0 m, the refractive index of the inner core 11 was set equal to the refractive index of the clad 20, and the relative refractive index difference A of the outer core 12 to the clad 20 was set to 0.34%. This optical fiber was used as an optical fiber for communication at a wavelength of 1550 nm.

[0075] The LP modes of the light beams propagating through the core 10 at this wavelength were LP.sub.01 mode, LP.sub.11 mode, LP.sub.21 mode, LP.sub.31 mode, LP.sub.02 mode, and LP.sub.12 mode. The effective refractive indexes n.sub.eff of the light beams of the modes were as presented in Table 1. Accordingly, the effective refractive index differences n.sub.eff between the light beams of LP modes that are adjacent to each other are as presented in Table 1.

TABLE-US-00001 TABLE 1 mode n.sub.eff n.sub.eff LP.sub.01 1.45379166 3.834 10.sup.4 LP.sub.11 1.45340825 8.908 10.sup.4 LP.sub.21 1.45251749 1.203 10.sup.3 LP.sub.31 1.45131469 6.354 10.sup.4 LP.sub.02 1.45067933 5.737 10.sup.4 LP.sub.12 1.45010567 1.057 10.sup.4 Clad 1.45000000

[0076] From Table 1, a larger effective refractive index difference of the effective refractive index difference between the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode and the effective refractive index difference between the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21 mode light beam is 8.90810.sup.4. In addition, the effective refractive index difference between the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is 1.20310.sup.3. Therefore, a coupling amount of the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is suppressed compared to a coupling amount of the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode, and a coupling amount of the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21 mode. A larger effective refractive index difference of the effective refractive index difference between the light beam of the LP.sub.31 mode and the light beam of the LP.sub.02 mode and the effective refractive index difference between the light beam of the LP.sub.02 mode and the light beam of LP.sub.12 mode is 6.35410.sup.4 (, which is smaller than the larger effective refractive index difference of the effective refractive index difference between the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode and the effective refractive index difference between the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21 mode). Therefore, a coupling amount of the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is suppressed compared to a coupling amount of the light beam of the LP.sub.31 mode and the light beam of the LP.sub.02 mode, and a coupling amount of the light beam of the LP.sub.02 mode and the light beam of the LP.sub.12 mode. In addition, a difference between the effective refractive index of the light beam of the LP.sub.12 mode and the refractive index of the clad 20 is 1.05710.sup.4. Therefore, the light beam of the LP.sub.12 mode is coupled with the light beam of the clad mode propagating through the clad 20, and thus propagates through the clad 20. Therefore, through this optical fiber, the light beams of three LP modes having the first to third highest effective refractive indexes propagate while being mode coupled with each other, and the light beams of three LP modes having the first to third lowest effective refractive indexes are mode coupled with each other, coupled with the light beam of the clad mode, and then lost.

[0077] Next, additional design examples of the optical fiber of the above-described embodiments will be described.

[0078] An optical fiber having the refractive index profile of FIG. 1 was designed. In this optical fiber, the radius r1 of the inner core 11 was set to 3.4 m, the radius of the outer periphery of the outer core 12 was set to 9.5 m, the refractive index of the inner core 11 was set equal to the refractive index of the clad 20, and the relative refractive index difference A of the outer core 12 to the clad 20 was set to 0.60%. This optical fiber was used as an optical fiber for communication at a wavelength of 1550 nm.

[0079] The LP modes of the light beams propagating through the core 10 were LP.sub.01 mode at this wavelength are LP.sub.11 mode, LP.sub.21 mode, LP.sub.31 mode, and LP.sub.02 mode. The effective refractive indexes n.sub.eff of the light beams of the modes were as presented in Table 2. Accordingly, the effective refractive index differences n.sub.eff between the light beams of LP modes that are adjacent to each other are as presented in Table 2.

TABLE-US-00002 TABLE 2 mode n.sub.eff n.sub.eff LP.sub.01 1.45659030 7.044 10.sup.4 LP.sub.11 1.45588591 1.636 10.sup.3 LP.sub.21 1.45425014 2.212 10.sup.3 LP.sub.31 1.45203784 1.152 10.sup.3 LP.sub.02 1.45088601 8.860 10.sup.4 Clad 1.45000000

[0080] From Table 2, a larger effective refractive index difference of the effective refractive index difference between the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode and the effective refractive index difference between the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21 mode light beam is 1.63610.sup.3. In addition, the effective refractive index difference between the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is 2.21210.sup.3. Therefore, a coupling amount of the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is suppressed compared to a coupling amount of the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode, and a coupling amount of the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21 mode. The effective refractive index difference between the light beam of the LP.sub.31 mode and the light beam of the LP.sub.02 mode is 1.15210.sup.3 (, which is smaller than the larger effective refractive index difference of the effective refractive index difference between the light beam of the LP.sub.01 mode and the light beam of the LP.sub.11 mode and the effective refractive index difference between the light beam of the LP.sub.11 mode and the light beam of the LP.sub.21). Therefore, a coupling amount of the light beam of the LP.sub.21 mode and the light beam of the LP.sub.31 mode is suppressed compared to a coupling amount of the light beam of the LP.sub.31 mode and the light beam of the LP.sub.02 mode. In addition, a difference between the effective refractive index of the light beam of the LP.sub.02 mode and the refractive index of the clad 20 is 8.86010.sup.4. Therefore, the light beam of the LP.sub.02 mode is coupled with the light beam of the clad mode propagating through the clad 20, and thus propagates through the clad 20. Therefore, through this optical fiber, the light beams of three LP modes having the first to third highest effective refractive indexes propagates while being mode coupled with each other, and the light beams of two LP modes having the first and second lowest effective refractive indexes are mode coupled with each other, coupled with the light beam of the clad mode, and then lost.

[0081] Although the invention has been described above by reference to the above-described embodiments as examples, the invention is not limited thereto.

[0082] For example, in the optical fibers 1 to 4 of the above-described embodiments, the number of modes of light beams up to x-th order mode is not particularly limited as long as it is two or more. In addition, the number of modes of light beams of (x+1)-th order mode and higher is not particularly limited as long as it is one or more.

[0083] In the above-described embodiments, the side core 40 is a single mode core, but the side core 40 may be a core that allows propagation of light beams of a plurality of modes. In this case, only one of the light beams of the plurality of modes propagating through the side core 40 has to be coupled with a light beams of any one of the (x+1)-th LP order mode and higher propagating through the core 10.

[0084] In the above-described embodiments, each core 10 has a refractive index profile of a ring type, but the core 10 may be a core having a refractive index profile of a step type, in which the refractive index is constant along the radial direction, or a core having a refractive index that increases toward the center axis.

[0085] In the above-described embodiments, each core 10 is directly surrounded by the clad 20, but a trench layer having a refractive index lower than that of the clad 20 may be formed between the core 10 and the clad 20.

[0086] In the above-described embodiments, cases where the number of the cores 10 is seven is described, but in an optical fiber having a plurality of cores 10, the number of the cores 10 is not limited as long as it is two or more.

[0087] As described above, according to one or more embodiments of the present invention, an optical fiber capable of allowing appropriate propagation of light beams of a plurality of modes while making them mode coupled can be provided, and can be used in the field of optical communication.

[0088] 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.

EXPLANATION OF LETTERS OR NUMERALS

[0089] 1 to 4 . . . optical fiber [0090] 10 . . . core (signal light propagation core) [0091] 11 . . . inner core [0092] 12 . . . outer core [0093] 30 . . . coating layer [0094] 40 . . . side core