Optical waveguide and method for creating an asymmetrical optical filter device

Abstract

The invention is related to an optical waveguide device comprising

Description

BACKGROUND OF THE INVENTION

[0001] The invention is related to an optical waveguide device and method for creating an asymmetrical optical filter device. In particular the invention is related to an optical waveguide device with a special structure of core and inner and outer cladding so that an asymmetrical coupling of fundamental mode with the cladding modes of the device can be obtained.

[0002] The invention is also related to a method for creating an asymmetrical optical filter device by a special coupling of the fundamental mode with multiple cladding modes using special fiber design.

[0003] Bragg gratings in optical fibers have been known to be extremely useful features in the field of telecommunication for quite some years. Versatile filter and reflector systems can be carried out conveniently by use of such gratings. An important application is the optical gain equalization in long distance fiber lines. In order to compensate for the loss over long distances optical amplifiers are incorporated into the lines in certain spatial intervals. Unfortunately, in multiplexed systems the amplifier gain response usually is not flat over the whole range of all wavelength channels. Thus, a gain equalization by spatially succeeding filter systems is necessary. The filter characteristics, i.e. the “shape” of the filter, has to be optimized according to the characteristics of the fiber line, the amplifier systems and the wavelength range.

[0004] Slanted Bragg gratings SBG are used to couple light of certain over amplified wavelengths into the cladding modes of the fiber, while other wavelengths remain unaffected. The SBG is a standard fiber Bragg grating tilted during photo inscription with an angle between the grating fringes and the normal of the fiber axis. This SBG couples part of the fiber-guided mode into radiation modes or cladding modes in a counter-propagating direction. The envelope of couplings into the different cladding modes yields the filter shape. The envelope of couplings is defined by the specific fiber design. It is for example known from FR-A-9806904, to provide a photosensitive cladding to reduce the spectral width of the filter and a reduced photosensitivity in the core to decrease the back reflection into the fundamental mode, whereby the grating can be short (800 μm) or chirped to suppress the modulation due to coupling into discrete modes. By chirping the fringe period along the grating length, or by shortening the grating, each discrete filter corresponding to the coupling into each cladding mode is enlarged, so that they can overlap each other.

[0005] Especially in systems of a wide spectral range or in systems with very uneven spectral distribution, however, a single slanted Bragg grating often is not enough to yield a satisfying equalization of the amplifier gain. Thus, a chain of several slanted Bragg gratings with different characteristics can be concatenated one after the other to represent a row of spectrally succeeding filters. The succeeding fiber sections containing one filter each are spliced together.

[0006] In the U.S. Pat. No. 6,005,999 an optical filter is disclosed that offers a narrowband rejection filter that couples out of a forward propagating core mode. The design of this device allows the coupling of the fundamental mode to one cladding mode. The coupling to a single cladding mode allows to design the narrow band filters with for example a FWHM of around 0.3 nm. The filter characteristic is symmetric.

[0007] For a filter with a broader spectral width more than one cladding mode is coupled to the fundamental mode LP01. The French application 98 06 904 disclosed a filter having a symmetric shape, defined by the envelope of the cladding modes in the fiber. Often the gain equalization in transmission systems requires asymmetric shapes of fillers. Up to now solutions with symmetric concatenated filters are used.

SUMMARY OF THE INVENTION

[0008] The invention provides a solution to create asymmetrical shaped filters in one single Bragg grating written in a special designed fiber. The solution is realized by a fiber including a monomode core having a refraction index of nco, a photosensitivity of Sco and a radius Rco

[0009] and an internal cladding with a refractive index of ncl, a photosensitivity of Scl and a radius of Rcl

[0010] and an outer cladding surrounding the internal cladding with an refractive index that allows the existence of multiple cladding modes,

[0011] and a slanted Bragg grating with an effective tilt angle of θ written in core and inner cladding of the optical waveguide, coupling the fundamental mode into several cladding modes

[0012] where Rcl≦2.5 Rco and the Sco≦Scl

[0013] Preferably the device also comprises a Bragg grating wherein the slant angle θ is higher than 2.5°. In the most preferably embodiment the angle is selected to be between 4 and 5°. With this value an optimal coupling is obtained between fundamental and cladding modes.

[0014] Preferably the device also comprises a design where the ratio of photosensitivities Sco and Scl is between 20 and 90%. This allows to decrease the back-reflection into the fundamental mode.

[0015] Preferably the device also comprises a design where the photosensitivities Scoand Scl are equal. This allows, for systems permitting higher values of back-reflection into the fundamental mode, to realize filters wither higher contrast.

[0016] Preferably the device also comprises a design where the internal cladding is depressed or matched or have a positive refractive index.

[0017] Preferably the device also comprises a design where the core has a radius Rc>3 μm. In the most preferably embodiment the core has a radius equal to 4 μm. This is an important aspect for the filter so that it can be easily spliced to standard single mode fibers in telecommunication networks. The adaptation of core radius to the common used radius in single mode fibers helps to avoid losses in case of splices.

[0018] Preferably the device also comprises a design where the period of the slanted grating is uniform. In a preferably embodiment the length of this uniform grating is lower than 1 mm. The slanted grating with a uniform period is the easiest slanted grating to imprint in a fiber. With a long grating, the discrete cladding mode coupling arises clearly in the filter shape. Imprinting a short length slanted grating allows to smooth the spectrum. This is due to the fact that each unitary filter overlaps the adjacent unitary filter smoothing in result the transmission spectrum.

[0019] Preferably the device also comprises a design where the period of the slanted grating is chirped. The chirping of the grating period smoothes the mode structure of the filter.

[0020] Without a chirp the discrete cladding mode coupling arises clearly in the filter shape. Imprinting a slanted grating with a chirped period allows to smooth the spectrum. This is due to the fact that each unitary filter overlaps the adjacent unitary filter smoothing in result the transmission spectrum.

[0021] The method to create a asymmetrical shaped optical filter bases on the fact that the coupling into cladding modes can be influenced by a design rule.

DESCRIPTION OF THE INVENTION

[0022] Preferred embodiments and examples are described in the figures and in the following description.

[0023] FIG. 1 is a graphical representation of the radial refractive index distribution and the radial photosensitivity

[0024] FIG. 2 is a second representation of a refractive index distribution

[0025] FIG. 3 is a simulation of mode coupling and the resulting filter shapes.

[0026] FIG. 1 a illustrates the radial distribution of refractive indices for a first embodiment of the invention. The refractive indexes n show in a schematic way the situation in a fiber with depressed inner cladding. In this embodiment the refractive index of the core nco has a higher absolute value than the refractive index of the outer cladding. The refractive index of the outer cladding has a higher value than the refractive index of the inner cladding. This forms a depressed well and the total index step is defined as difference between nco and ncl.

[0027] FIG. 1 b illustrates the function of photosensitivity versus the radius R of the fiber. The photosensitivity in the core Sco has a lower value than the photosensitivity in the inner cladding region.

[0028] FIG. 2 illustrates a second embodiment of the inventional fiber. The refractive index profile is the profile of a index matched inner cladding. The profile of the photosensitivity remain as shown in FIG. 1b.

[0029] FIG. 3 shows the results of a simulation with all relevant parameters of the optical fiber to obtain a asymmetric shape of filter.

[0030] The used fiber has a:

[0031] Core radius of 4 μm

[0032] Step index of 6.5 10−3

[0033] Depressed cladding Dn 10−3

[0034] Photosensitivity ratio between core and cladding 50%

[0035] For the grating:

[0036] Photoinduced modulation 10−3

[0037] Period of the grating is chirped with 2 nm/cm

[0038] Length of the grating 10 mm

[0039] The simulation with the parameters above mentioned shows the overlap integrals between fundamental and cladding modes and the resulting transmission spectrum.

[0040] FIG. 3 a starts with a radius of the cladding of 20 μm. The resulting transmission spectrum 3b is symmetric. Reducing the cladding radius in 3c to a value of 10 μm the coupling becomes asymmetric and the transmission curve shifts to a asymmetric function. With a cladding radius of only 6 μm the result is clearly asymmetric in FIG. 3f.

[0041] This example is calculated with a tilt angle θ of 5°. If this angle is decreased the shape of the filter will be more asymmetric.

[0042] A set of optimal parameters for the design of an asymmetric filter allows to create the dependence that the fundamental mode is differently coupled into symmetric cladding mode LP0m and asymmetric cladding modes LP1m−1 for m=2,3,4. Therefore the symmetry of the coupling is broken.

[0043] The optical asymmetric filter is used in transmission systems as passive components for equalization of signal strengths over a wavelength range. The filters are especially used for optical fiber amplifying systems to achieve flat gain spectra for a wavelength comb.

Claims

1. An optical waveguide device comprising a length of fiber including a monomode core having a refractive index of nco, a photosensitivity of Sco and a radius Rco and an internal cladding with a refractive index of ncl, a photosensitivity of Scl and a radius of Rcl, and an outer cladding surrounding the internal cladding with a refractive index that allows the existence of multiple cladding modes, and a slanted Bragg grating with an effective tilt angle of θ written in core and inner cladding of the optical waveguide, coupling the fundamental mode into several cladding modes where Rcl≦2.5 Rco and the Sco≦Scl.

2. An optical waveguide according to claim 1 wherein the slant angle θ is higher than 2.5°.

3. An optical waveguide according to claim 1 wherein photosensitive dopant is Germanium.

4. An optical waveguide according to claim 1, wherein the ratio of photosensitivities Sco and Scl is between 20 and 90%.

5. An optical waveguide according to claim 1, wherein the photosensitivities Sco and Scl are equal.

6. An optical waveguide according to claim 1 where the internal cladding is depressed or matched or have a positive refractive index.

7. An optical waveguide according to claim 1 where the core has a radius Rc>3 μm.

8. An optical waveguide according to claim 1 where the period of the slanted grating is uniform.

9. An optical waveguide according to claim 1 where the period of the slanted grating is chirped.

10. Method for creating an asymmetrical optical filter device with a piece of fiber comprising a core, an inner and an outer cladding, where the refractive indices are adapted in a way that the fundamental mode LP01 is coupled with different strengths to the symmetric cladding modes LP0m and the asymmetric cladding modes LP1m−1 where m=2,3,4, . . .

11. Method according to claim 9 where the strength of coupling into cladding modes LP0m is different then the strength into cladding modes LP1m−1.

12. Transmission system using at least one optical device according to claim 1.