MODE FILTERING OPTICAL FIBRE

Abstract

A microstructured optical fiber has periodically arranged high-index rods embedded in a low-index background, a high-index ring surrounding the high-index rods, and a high-index core located at the center. The high-index rods and the low-index background forms a microstructured cladding region which supports the guidance of supermodes. The fundamental and the highest supermodes form a cladding-mode band, wherein at least the effective index of a core mode lies in the cladding-mode band. Also provided is

a technique for selectively filtering the fiber modes, to selectively filter out one or some of the high-order modes with the other modes still guided in the core with low loss. The cascade of optical fibers can filter out a group of fiber modes, marking guidance of a single high-order mode in a few-mode optical fiber possible.

Claims

1. A microstructured optical fiber comprising periodically arranged high-index rods embedded in a low-index background, a high-index ring surrounding the high-index rods, and a high-index core located at the center, wherein the high-index rods and the low-index background forms a microstructured cladding region which supports the guidance of supermodes, wherein the fundamental and the highest supermodes form a cladding-mode band, wherein at least the effective index of a core mode lies in the cladding-mode band, wherein the relationship between the refractive indexes of the core n.sub.core, the background n.sub.clad, the high-index rods n.sub.rod, and the high-index ring .sub.out meet the condition of n.sub.out>n.sub.clad, n.sub.core>n.sub.clad, and n.sub.rod>n.sub.clad, and wherein the core parameters should meet the condition of V>2.405 , where $V=\frac{2.Math..Math..Math.r_{\mathrm{core}}}{{}_0}.Math.{\left(n_{\mathrm{core}}^2-n_{\mathrm{clad}}^2\right)}^{1/2},$ r.sub.core is the core radius, and .sub.0 is the operating wavelength.

2. The microstructured optical fiber as claimed in claim 1, wherein the refractive index of the high-index ring is higher than the effective indexes of all the supermodes.

3. The microstructured optical fiber as claimed in claim 1, wherein the relationship between the inner diameter of the high-index ring d.sub.in, the radius of the high-index rods r.sub.rod, and the maximum center-to-center distance between the high-index rods and the core L.sub.max meets the condition of d.sub.inL.sub.maxr.sub.rod<4 m.

4. The microstructured optical fiber as claimed in claim 1, wherein the ring number of high-index rods N meets the condition of N3.

5. The microstructured optical fiber as claimed in claim 1, wherein the minimum center-to-center distance between the high-index rods and the core S.sub.min meets the condition of S.sub.min(r.sub.core+r.sub.rod)3 m and S.sub.min(R.sub.core+r.sub.rod)8 m.

6. The microstructured optical fiber as claimed in claim 3, wherein the relationship between the refractive index of the high-index ring n.sub.out and the effective index of the fundamental supermode n.sub.ceff meets the condition of n.sub.outn.sub.ceff>0.0005.

7. The microstructured optical fiber as claimed in claim 3, wherein the microstructured cladding is composed of 2 or 3 types of high-index rods, each type of high-index rods have the same radius, refractive index, and period, wherein the high-index rods of a type forms 1 to 3 regions, and the centers of the high-index rods in a region are fallen in a sector area.

8. The microstructured optical fiber as claimed in claim 7, wherein the cross-section of the optical fiber is of axial symmetry.

9. The microstructured optical fiber as claimed in claim 1, wherein the core is filled with high-index liquid.

10. The microstructured optical fiber as claimed in claim 1, wherein the high-index rods is replaced by high-index liquid.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0017] FIG. 1 is a cross-sectional diagram of an optical fiber according to an embodiment of the present invention;

[0018] FIG. 2 is a cross-sectional diagram of an optical fiber with high-index rods of two different sizes according to an embodiment of the present invention;

[0019] FIG. 3 is a cross-sectional diagram of another optical fiber with high-index rods of two different sizes according to an embodiment of the present invention;

[0020] FIG. 4 is the field distributions of the LP.sub.01 mode (a) and LP.sub.11 mode (b) for an optical fiber according to an embodiment of the present invention as shown in FIG. 1;

[0021] FIG. 5 is the effective indexes (a) and confinement losses (b) of the core modes for an optical fiber according to an embodiment of the present invention as shown in FIG. 1.

[0022] FIG. 6 is the transmission loss of the fundamental core mode as a function of transmission distance for an optical fiber according to an embodiment of the present invention as shown in FIG. 1.

[0023] FIG. 7 is the confinement losses of the core modes as functions of inner diameter of the high-index ring for an optical fiber according to an embodiment of the present invention as shown in FIG. 1;

[0024] FIG. 8 is the confinement losses of the core modes as functions of the refractive index of the high-index ring for an optical fiber according to an embodiment of the present invention as shown in FIG. 1;

[0025] FIG. 9 is the effective indexes (a) and confinement losses (b) of the core modes for an optical fiber according to an embodiment of the present invention as shown in FIG. 1.

[0026] FIG. 10 is a cross-sectional diagram of another optical fiber according to an embodiment of the present invention;

[0027] FIG. 11 is the confinement losses of the core modes for an optical fiber according to an embodiment of the present invention as shown in FIG. 10;

DETAILED DESCRIPTION OF THE PRESENT INVENTION

[0028] FIG. 1 shows the cross-sectional diagram of an optical fiber according to an embodiment of the present invention. According to the invention there is provided a photonic bandgap cladding optical fiber comprising periodically arranged high-index rods embedded in a low-index background and a high-index core located at the center the core. The step-index core supports the guidance of higher-order modes. In addition, the high-index rods and the low-index background forms a microstructured cladding region which supports the guidance of supermodes.

[0029] According to the theory of photonic bandgap fiber, the guidance of lights in the microstructured cladding would be forbidden in the specified wavelength and mode index regions. Therefore, those core modes with effective indexes located in the bandgap region will be guided by the bandgap effect. Since the microstructured cladding is composed of high-index rods in the background of low index material, the microstructured cladding would be able to form cladding modes whose effective indexes are higher than that of the background index, which can be understood as the result of splitting the fundamental mode of a single rod into a large number of supermodes by bringing a large number of identical rods together. Therefore, if a core mode has low index difference with a supermode, then the core mode would couple with the supermode. Low-index difference between the two modes is a premier requirement for strong mode coupling. Therefore, as long as the number of high-index rods is large enough, there would be sufficient large number of cladding modes in the cladding mode band, if the effective index of a core mode lies in the cladding mode band, strong mode coupling would happen.

[0030] The high-index ring plays an important role on the elimination of core mode. In order to introduce leakage mechanism, the refractive index of the high-index ring should be higher than that of the background. Preferably the refractive index of the high-index ring should be higher than the effective indexes of all the supermodes. The index-guiding mechanism is therefore broken, and high leakage losses are introduce to the supermodes.

[0031] It is important to apply a high-index ring. In fact, if high-index ring is not introduced, then both the core modes and the cladding modes would have higher indexes than the background index, which means the core modes and cladding modes are guided based on index-guiding effect without confinement losses. To induce high leakage losses for the supermodes, the refractive index of the high-index ring should be higher than those of the supermodes, that is, the refractive index of the high-index ring n.sub.out should be higher than the effective index of the fundamental supermode n .sub.ceff. Preferably the relationship between the refractive index of the high-index ring n.sub.out and the effective index of the fundamental supermode n.sub.ceff may meet the condition of n.sub.outn.sub.ceff>0.0005.

[0032] The high-index ring should be closer to the high-index rods, in this way, the guidance of the supermodes by index guiding will be difficult, as a result, the supermodes will experience high leakage losses. Preferably the relationship between the inner diameter of the high-index ring d.sub.in, the maximum center-to-center distance between the high-index rods and the core L.sub.max should meet the condition of d.sub.inL.sub.maxr.sub.rod<4 m.

[0033] By applying two or more types of high-index rods, it is possible to filter out a few core modes. The high-index rods of a type forms 1 to 3 regions, and the high-index rods in a region are fallen in a sector area. A core mode, of which the effective index of a core mode lies in the cladding-mode band will couple with the supernodes in the region, and filtered out. Therefore, high-index rods of different types can filter out different core modes. FIGS. 2 and 3 show examples of the present invention with two types of high-index rods.

[0034] The core should be closer enough with the high-index rods, so that the coupling between the core mode and the supermodes are strong enough. It is also important that the distance should not be to closer so that the guided core mode would still keep a regular mode field. The center-to-center distance between the core and the high-index rods adjacent the core S.sub.min should meet the condition of S.sub.min(r.sub.core+r.sub.rod)3 m and S.sub.min(r.sub.core+r.sub.rod)8 m.

Embodiment 1

[0035] FIG. 1 is a cross-sectional diagram of an optical fiber according to an embodiment of the present invention. FIG. 4 show the field profiles of the LP.sub.01 and LP.sub.11 modes of this embodiment. The LP.sub.01 mode shows a strong coupling with the cladding mode. As a contrast, the LP.sub.11 mode is confined in the core, although it also has some energy located in the first ring of the high-index rods.

[0036] FIG. 5(a) show the effective indexes of the core modes for an optical fiber according to an embodiment of the present invention as shown in FIG. 1. In particular, curves A01 and A11 show the effective indexes of the LP.sub.01 and LP.sub.11 modes. Curves A2 and A3 are the upper and lower limits of the cladding mode band. Curve A4 is the upper edge of the bandgap. The lower limit of the cladding-mode band approaches the upper edge of the bandgap. The mode indexes of the cladding modes are following in a narrow index range for a fixed wavelength as the figure shows. Introducing more high-index rods will reduce the gap between the cladding mode index and the top boundary of the bandgap. Low-index difference between the two modes is a premier requirement for strong mode coupling. Since so many cladding modes exist in the narrow index range, if the effective index of the fundamental core mode lies in the cladding mode region, strong mode coupling would happen. As shown in FIG. 5(a), the LP.sub.11 mode index lies in the bandgap region, whereas the LP.sub.01 mode index lies in the cladding mode region for a wide wavelength range.

[0037] The confinement losses of the core modes as functions of wavelength are shown in FIG. 5(b). The LP.sub.11 mode shows increased confinement loss as wavelength increases. The LP.sub.01 mode with effective index located at the cladding mode region shows a quite complex variation of confinement loss as the wavelength varies, which is owing to the fact that the LP.sub.01 mode will couple with different cladding modes at different situation. Therefore, the coupling efficiency would be different. The confinement loss of the LP.sub.01 mode reduces with the increase of index difference between the LP.sub.01 mode and the cladding modes. The wide operating bandwidth is owing to the existence of a large number of cladding modes in a narrow region, which ensures strong coupling as the core mode lies in the region.

[0038] The guiding mechanics of the LP.sub.11 mode in the fiber is different with that of a conventional bandgap fiber because the introduction of the high-index rods will actually increase the confinement loss of the LP.sub.11 mode in the proposed fiber. In another words, the high-index rods in the cladding do not contribute to the guiding of the LP.sub.11 mode at this situation. The main function of the periodic high-index rods would be forming the cladding modes in a specified region, so that the cladding modes will couple with the core modes whose effective indexes lie in the bandgap region and simultaneously avoid the coupling with the other core modes.

[0039] Curve C1 in FIG. 6 shows the transmission loss of the LP.sub.11 mode of an example without high-index ring. It shows the LP.sub.01 mode couples with the cladding supermodes periodically. Curve C2 in FIG. 6 shows the transmission loss of the LP.sub.01 mode of an example with high-index ring. The introduction of high-index ring can effective increase the confinement loss of the LP.sub.01 mode. Therefore, the high-index ring plays an important role on the elimination of the LP.sub.01 mode.

[0040] FIG. 7 shows the confinement losses of the core modes as functions of inner diameter of the high-index ring d.sub.in. We can see the microstructured cladding diameter d.sub.in should be small enough to break the index guiding mechanism of the cladding modes, so that the confinement loss of the LP.sub.01 mode could be high enough. FIG. 8 is the confinement losses of the core modes as functions of the refractive index of the high-index ring n.sub.out for an optical fiber according to an embodiment of the present invention. It shows the refractive index of the high-index ring has little influence on the confinement loss of the LP.sub.11 mode, whereas the LP.sub.01 mode would experience high loss as the refractive index of the high-index ring is higher enough. A basic criterion is the refractive index of the high-index ring should be higher than the effective indexes of the cladding modes. The fact that the LP.sub.11 mode has little interaction with the microstructured cladding leads to the weak influence by the variation of outer cladding index.

Embodiment 2

[0041] The configuration is shown in FIG. 1. The effective indexes and confinement losses of the core modes in the fiber as functions of wavelength are shown in FIG. 9. The core is able to support the guidance of the LP.sub.01, LP.sub.11, LP.sub.21, and LP.sub.02 modes. FIG. 9(a) shows the effective indexes of the core modes and the supermode hand. Curves F01, F11, F21, and F02 show the effective indexes of the LP.sub.01, LP.sub.11, LP.sub.21, and LP.sub.02 modes, respectively. Curves F30 and F40 are the upper and lower boundary of the supermode band. Curve F50 is the bandgap edge of the high-index rods. The effective index of the LP.sub.11 mode lies in the supermode band at wide bandwidth, whereas the index curves of the LP.sub.01, LP.sub.21, and LP.sub.02 modes lie out of the bandgap region.

[0042] Curves G01, G11, G21, and G02 show the confinement losses of the LP.sub.01, LP.sub.11, LP.sub.21, and LP.sub.02 modes. As shown in FIG. 9(a), the LP.sub.11 mode lies in the cladding mode band at wide wavelength range, which is why the high loss region of the LP.sub.H mode is so wide. The losses of the LP.sub.01 mode is always low, which is contributed to its high index contrast with the cladding modes. As for the LP.sub.21 and LP.sub.02 modes, the losses increase with the increase of wavelength.

Embodiment 3

[0043] The configuration is shown in FIG. 10. The ring number of high-index rods is N=4. The effective indexes and confinement losses of the core modes in the fiber as functions of wavelength are shown in FIG. 11. Curves H01, H 11, H 21, and H 02 show the confinement losses of the LP.sub.01, LP.sub.11, LP.sub.21, and LP.sub.02 modes.

[0044] Compared with the results of embodiment 2, the confinement losses of the LP.sub.21 and LP.sub.02 modes in the present embodiment are reduced effectively, while the LP.sub.11 mode still maintains a high loss.