CN1434583A - Bragg grating with new sampling structure for compensating dispersion and polarization mode dispersion - Google Patents

Abstract

The present invention proposes a kind of reflective Bragg grating that is used for dispersion compensation in optical fiber communication, and it has effective refractive index perturbation as shown in (1) formula: Wherein z is the coordinate along grating direction, and Λ ₀ grating starting point period, Δn _dc is the average value of the effective index perturbation within one grating period, Δn _ac is the magnitude of the fast-varying component of the effective index perturbation, φ is an additional phase term, where F(z) is a novel The sampling structure with nonlinear type II chirp is shown in (2): Thus, the Bragg grating of the present invention does not depend on the chirp (type I chirp) caused by Δn _dc or φ varying with z Various group delay response spectra can be provided as required in a specific reflection band of the grating to compensate for dispersion, and the sampling period of the sampling structure F(z) is much longer than the grating period. Therefore, the overhead on the phase template is reduced and the control precision required in the manufacturing process is reduced, thereby reducing the manufacturing cost. At the same time, the present invention also overcomes the problem that the linear type II chirp in the prior art is difficult to be used for dispersion compensation alone, and can obtain a variety of actually required group delay responses in a certain specific reflection band of the grating spectrum, and when combined with Type I chirp, the group delay response spectrum of the grating can be tuned within a channel.

Description

The Bragg grating that is used for compensation of dispersion and polarization mode disperse with new sampling structure

Technical field

The present invention relates to fiber optic communication field, relate in particular to static dispersion compensation, dynamic dispersion compensation, dynamic polarization mould disperse compensation in the optical fiber communication.

Background of invention

In optical fiber telecommunications system, the carrier of information is a series of light pulse.Through after the transmission of certain distance, light pulse meeting broadening, thus making the decreased performance of system, message capacity also is restricted.Have multiple factor can cause optical pulse broadening, wherein very important two is chromatic dispersion and polarization mode disperse.

A light wave ripple bag passes to the receiving terminal required time from transmitting terminal and is known as group delay.Because CHROMATIC DISPERSION IN FIBER OPTICS, the light wave ripple with different center frequency wraps in transmitting speed difference in the optical fiber, so their group delay is also different.As shown in Figure 1, a light pulse is made of two ripple bags, and their centre frequency is respectively f ₁And f ₂Because their group delay τ ₁And τ ₂Difference, so bring in from reception, they have separated Δ τ=τ in time ₁-τ ₂This has just caused the optical pulse broadening of receiving at receiving terminal.

Have at optical fiber under the situation of polarization mode disperse, electric field component wraps in propagation velocity difference in the optical fiber at the light wave ripple of different directions polarization.As shown in Figure 2, a light pulse is made of two ripple bags, and their electric field component is respectively along x and y direction.Because their group delay τ ₁And τ ₂Difference, so bring in from reception, they have separated Δ τ=τ in time ₁-τ ₂This has just caused the optical pulse broadening of receiving at receiving terminal.

In the prior art, fiber grating has been suggested the influence that is used to eliminate chromatic dispersion and polarization mode disperse, and this is existing the description in appended reference paper D1-D4.Fig. 3 a is the structural representation of Fiber Bragg Grating FBG, wherein the sandwich layer of optical fiber is two kinds of dielectric materials that refractive index is different with covering, they constitute a fiber waveguide, the refractive index perturbation of the dash area indication cycle property in the sandwich layer, and its cycle is called as the grating cycle.The refractive index of covering and sandwich layer is converted into the effective refractive index n of waveguide usually _Eff, and the refractive index perturbation in the sandwich layer is converted into the effective refractive index perturbation of whole wave guide, is expressed as: ${\mathrm{\Δn}}_{\mathrm{eff}}\left(z\right)={\mathrm{\Δn}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\Δn}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\π}}{{\mathrm{\Λ}}_0}z+\mathrm{\φ}\left(z\right)]---\left(1\right)$ Wherein, z is along optical fiber coordinate longitudinally, Λ ₀Be the cycle of grating starting point, Be the effective refractive index perturbation at the mean value (be also referred to as the DC component of effective refractive index perturbation) of a grating in the cycle,

Be the amplitude (being also referred to as the alternating current component of effective refractive index perturbation) of the fast variation amount of effective refractive index perturbation,  is an additional phase term, represents warbling of grating cycle. With  can be the function of z.Fig. 3 b has represented the variation schematic diagram of the effective refractive index perturbation of three kinds of Fiber Bragg Grating FBGs with the optical fiber along slope coordinate, wherein, (A) is

With  all be the situation of constant; (B) be With Situation with the z variation; (C) be the situation that  changes with z.The centre wavelength that wraps in the vacuum when incident wave satisfies $\frac{2\mathrm{\π}(n_{\mathrm{eff}}+\stackrel{\‾}{\mathrm{\Δn}}\left(z\right))}{\mathrm{\λ}}-\frac{\mathrm{\πN}}{{\mathrm{\Λ}}_0}-\frac{1}{2}\frac{\mathrm{d\φ}\left(z\right)}{\mathrm{dz}}=0---\left(2\right)$ The time, it will be reflected.In the formula (2), N is a positive integer, and λ is inversely proportional to the centre frequency f of ripple bag: $\mathrm{\λ}\∝\frac{1}{f}---\left(3\right)$ Formula (2) is commonly referred to as phase-matching condition.

By formula (2) as can be known, if

Or  changes with z, and the ripple bag with different center frequency will be reflected at the diverse location of grating, so the time that they are detained in grating is just different.Grating with this design feature is known as to have and warbles.Hereinafter, by Or  changes warbling of causing with z and warbles originally being called the I type.

Be mapped to grating when a light wave ripple with centre frequency f wraps into, incide from it and leave the required time of grating and be known as the group delay response of grating in frequency f.If the difference of the group delay response of two ripple bags is τ among grating pair Fig. 1 ₂-τ ₁, just compensated by the caused chromatic dispersion of Transmission Fibers so.

If a kind of material has different effective refractive indexs to the light of different directions polarization, so this material just is called as and has birefringent characteristic.According to formula (2), if a grating is formed at and has birefringent waveguide, the ripple bag of tool different directions polarization will be reflected at the diverse location of grating, the corresponding difference of their group delay of grating pair.Therefore, the optical pulse broadening that is caused by the polarization mode disperse among Fig. 2 can be eliminated with this grating.

In the optical fiber telecommunications system of reality, the group delay of light wave ripple bag is a change at random in time, and when single channel speed was higher, system became responsive to this change at random, therefore needed dynamic (dynamically promptly) dispersion compensation.It is important that the problem of polarization mode disperse generally just seems in High Speed System, so polarization mode disperse compensation all is dynamic usually.The group delay response that so just requires Bragg grating to have is as shown in Figure 4 composed, and this is existing the description in appended reference paper D3 and D4, and wherein f and τ represent the centre frequency and the group delay value of incident wave bag respectively.The feature of this group delay response spectrum is that the value of group delay is the nonlinear function of the centre frequency of incident wave bag.Have the Bragg grating that non-linear I type warbles and just have such group delay response spectrum.

The method that produces Bragg grating in optical fiber is commonly known in the art.Described a kind of method of making grating in reference paper D5, as shown in Figure 5, phase mask 1 wherein is to use the glass plate of UV transparent is made, and its surface has periodic groove structure.Place on one section this surface of optical fiber 2 next-door neighbours, perpendicular to the ultraviolet light of phase mask incident by the periodicity groove structure diffraction of phase mask, + 1 and-1 order diffraction light in optical fiber, interfere, the style of interference is periodic, thereby the one section grating that exposes in optical fiber.

The method that multiple manufacturing has the Bragg grating that the I type warbles has been described in reference paper D6-D14, wherein described in reference paper D6 and the D7 in the method, warbling of phase mask surface groove is identical with warbling of grating, so the cycle of phase mask surface groove is non-constant, and such phase mask is than general phase mask costliness.Reference paper D8-D12 reported method be respectively in making the process of fiber grating curved fiber, stretching optical fiber, change effective refractive index average along the distribution of optical fiber, change strain along the distribution of optical fiber, in scanning ultraviolet light light beam moving fiber, these methods all need high-precision control device, and reference paper D13 and D14 reported method are respectively after grating forms, it is applied a strain gradient and temperature gradient, and this increases the complexity of grating encapsulation.

Proposed a kind of Bragg grating in the prior art, be called as the sampling Bragg grating with periodic sample structure.Fig. 6 a and 6b have represented the structure of uniform sampling Bragg grating, and its effective refractive index perturbation is by the envelope modulation of one-period, and the right that is to say formula (1) has been multiplied by the envelope function F (z) of one-period and has become ${\mathrm{\Δn}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\Δn}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\Δn}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\π}}{{\mathrm{\Λ}}_0}z+\mathrm{\φ}\left(z\right)\left]\right\}{F}^{\′}\left(z\right)---\left(4\right)$ F (z) is known as shan, and its cycle is known as the sampling period (representing with Z).As shown in Figure 7, a sampling Bragg grating has a plurality of zones of reflections, and they all are that a corresponding Fourier component by F (z) causes. Numeral 2,1,0 ,-1 and-2 wherein is respectively the corresponding Fourier leaf-size class of these five zones of reflections.

If sampling period Z changes with coordinate z, promptly Z is the function Z (z) of z, and F (z) just is known as has warbling of sampling period.This warbling is known as the II type hereinafter and warbles.At appended reference paper D15 to analyzing with having the chromatic dispersion that the I type is warbled and linear II type is warbled Bragg grating compensates a plurality of channels in the wavelength-division multiplexing fiber-optic communication system simultaneously.But it is linear that such II type is warbled, and it has only a variable element, and promptly Z is with the rate of change of z linear change.By the warble first order component and the high order component of the group delay response that produced of linear II type all is this parameter decision, so they can not be controlled respectively.This has just brought following problem: the first, and can not only warble and obtain actual required various group delay response spectrums by linear II type; The second, the high order component of group delay response becomes and can not ignore when Z is big with the rate of change of z linear change, and makes the shape of group delay response spectrum become irregular.Therefore, linear II type is warbled and is difficult to be utilized separately for dispersion compensation, even combine and be used under the situation of multichannel dispersion compensation warbling with the I type, the main contribution of the group delay response of Bragg grating is still come from the I type warble, the minute differences of the dispersion measure that only is used to compensate each interchannel and the II type is warbled.

Summary of the invention

The objective of the invention is to warble and need complex structure and expensive phase mask, control precision in the manufacture process is required high or makes problem such as encapsulation complexity increase in order to solve the I type, and the linear II type problems such as being difficult to be utilized separately for dispersion compensation of warbling.

For this reason, the present invention proposes a kind of reflective Bragg grating with new sampling structure, described grating index perturbation is shown in following formula (4): ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;n}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\&Delta;n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left(z\right)\left]\right\}{F}^{\&prime;}\left(z\right)---\left(4\right)$ It is characterized in that F (z) warbles for non-linear II type, promptly its sampling period Z is non-linear with the variation along the coordinate z of grating.Or rather, this novel sampling structure can be represented with following shan: $F\left(z\right)=F^{\&prime;}\left(z^{\&prime;}\right)=F^{\&prime;}(z+\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z}^{p_n+1})---\left(5\right)$ Wherein F ' (z ') is the envelope of one-period, such as square wave, sine wave etc., starts from the starting point of grating, terminates in the terminal point of grating.Have sampling structure that non-linear II type as the formula (5) warbles and will be Fourier leaf-size class time additional equivalent phase item of effective refractive index perturbation contribution for the zone of reflections of m: ${\mathrm{\&phi;}}_e\left(z\right)=\frac{2\mathrm{m\&pi;}}{{\mathrm{<figure-callout\; id="0"\; label="Z"\; filenames="A0210338300211.png,A0210338300221.png"\; state="\{\{state\}\}">Z</figure-callout>}}_0}\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z}^{p_n+1}---\left(6\right)$ By formula (6) as can be known, the n order component of equivalent phase item is uniquely by relevant parameters a _nAnd p _nDecision.By setting one group of a _nAnd p _n(n=1,2,3 ...), in certain specific zone of reflections of grating, can obtain diversified group delay response spectrum.Therefore, by reasonably setting a in the formula (5) _nAnd p _n(n=1,2,3 ...) numerical value, can make the group delay response spectrum of Bragg grating compose consistent with actual required group delay response.Thereby can realize the purpose of dispersion compensation.

Basic ideas of the present invention be exactly according to reality required group delay response compose to determine sampling structure F (z) in the formula (5).As seen from formula (5), F (z) is with the one-period function F ' (z ') through following coordinate transform $z^{\&prime;}=z+\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z}^{p_n+1}---(7-a)$ Conversion and getting.Particularly, at first, from F ' (z '), choose N point (z ' _k, F ' (z ' _k)) (k gets N from 1), and guarantee that N is enough greatly so that choose 2 points at least in each cycle of F ' (z ').Secondly, with z ' _kAnd z _kSubstitution formula (7) obtains about z _kEquation ${z^{\&prime;}}_k=z_k+\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z_k}^{p_n+1}---(7-b)$ Then, separate this equation by the method for parsing commonly known in the art or numerical value and obtain z _k, make again F ' (z ' _k)=F (z _k), just can obtain corresponding point (z among the F (z) _k, F (z _k)), these points have just been represented sampling structure F (z).

Compose to determine p according to required group delay _nAnd a _n(n=1,2,3 ...) the flow chart of method.In step 1, the group delay response spectrum τ (λ) required according to reality reasonably chooses one group of p _nAnd a _n(n=1,2,3 ...) as initial value (for example examples of implementation 1 or 2 in " detailed Description Of The Invention "); Then, enter step 2, obtain to have accordingly the shan F (z) that non-linear II type is warbled by the shan F ' of one-period (z ') according to foregoing method of coordinates transform; Then, enter step 3, obtain to have (λ) as the group delay response spectrum τ ' of the Bragg grating of the described sampling structure of F (z) by numerical simulation or experiment; Then, enter step 4, relatively τ ' (λ) with τ (λ), see whether they conform in actual permissible accuracy; If conform to, then enter step 6, whole process finishes, otherwise returns step 5, revises p _nAnd a _n(n=l, 2,3 ...) value, repeat said process again.

Can compose according to needed group delay by above method and to obtain needed non-linear sampling structure function F (z), thereby obtain needed effective refractive index perturbation

Having the I type when proposing among the reference paper D15 warbles and compares with the Bragg grating that linear II type is warbled, Bragg grating proposed by the invention has non-linear II type and warbles, therefore it can be used for dispersion compensation, dynamic dispersion compensation and dynamic polarization mould disperse compensation, and no matter whether grating also has the I type simultaneously warbles.

Warble with the I type and to compare, the present invention has the following advantages: 1. because the periodicity groove structure that the II type is warbled and do not relied on the phase mask surface, so when utilization phase mask method is made this Bragg grating, the periodicity groove structure on phase mask surface can have the constant cycle, this has just increased the flexibility of design and manufacturing, and has reduced manufacturing cost because avoided using baroque phase mask; 2.F the sampling period (z) is generally than big 2 to 3 orders of magnitude of grating cycle, compares the accurate control that easier realization is warbled to the II type in manufacture process so warble with the I type.

Warble with linear II type and to compare, the present invention has the following advantages: can obtain the required group delay response spectrum of varied reality in certain specific zone of reflections of grating 1.; 2. can be utilized separately for dispersion compensation; 3. warble when combining with the I type, its effect is not limited to compensate the minute differences of the dispersion measure of each interchannel, and can adjust the group delay response spectrum of grating in a channel.

The accompanying drawing summary

Fig. 1 causes the optical pulse broadening schematic diagram by chromatic dispersion.

Fig. 2 causes the optical pulse broadening schematic diagram by the polarization mode disperse.

Fig. 3 a is the structural representation of Fiber Bragg Grating FBG of the prior art.

Fig. 3 b is the variation schematic diagram of the effective refractive index perturbation of three kinds of Fiber Bragg Grating FBGs of the prior art with the optical fiber along slope coordinate, wherein, (A) is With  all be the situation of constant; (B) be

With

Situation with the z variation; (c) be the situation that  changes with z.

Fig. 4 is the group delay response spectrum schematic diagram that is used for the Bragg grating of dynamic dispersion compensation and polarization mode disperse compensation in the prior art.

Fig. 5 makes the Fiber Bragg Grating FBG schematic diagram with phase mask in the prior art.

Fig. 6 a is the structural representation of the Fiber Bragg Grating FBG of uniform sampling of the prior art.

Fig. 6 b is that the effective refractive index perturbation of Fiber Bragg Grating FBG of uniform sampling of the prior art is with the variation schematic diagram of optical fiber along slope coordinate.

Fig. 7 is the group delay response spectrum of the Fiber Bragg Grating FBG of uniform sampling of the prior art.

Fig. 8 a is the structural representation that has the sampling Fiber Bragg Grating FBG that non-linear II type warbles according to of the present invention.

Fig. 8 b is transformed to a schematic diagram with shan F (z) that non-linear II type warbles according to the shan F ' with one-period of the present invention (z ').

Fig. 9 is the flow chart that obtains to have accordingly the sampling structure that non-linear II type warbles by the required group delay response of reality spectrum according to of the present invention.

Figure 10 a is a group delay response spectrum according to the sampling Bragg grating-1 grade zone of reflections of first embodiment.

Figure 10 b is the group delay response spectrum that only has the Bragg grating that linear I type warbles in the prior art, is incorporated herein by the comparison with Figure 10 (a).

Figure 11 is 20 ℃ and 100 ℃, no strain and has under the situation of 0.05% tensile strain in temperature, the group delay response spectrum according to-1 grade of zone of reflections of the sampling Bragg grating of second embodiment.

Figure 12 a is to be under the situation of 20 ℃ and 100 ℃ in temperature, the group delay response spectrum according to-1 grade of zone of reflections of the described sampling Bragg grating of the 3rd embodiment.

Figure 12 b is in no strain and has under the situation of 0.05% tensile strain, the group delay response spectrum according to-1 grade of zone of reflections of the described sampling Bragg grating of the 3rd embodiment.

Figure 13 be have only linear I type warble and with linear I type warble with the situation about combining of warbling according to the non-linear II type of first embodiment under, the group delay response of-1 grade of zone of reflections of Bragg grating spectrum.

Detailed Description Of The Invention

Fig. 8 a has described a kind of warble Bragg grating of sampling structure of non-linear II type that has,

Implement basic ideas of the present invention and be exactly required group delay response and compose to determine sampling structure F (z) in the formula (5) according to reality.From above-mentioned formula (5) as can be known, F (z) is with the one-period function F ' (z ') pass through as shown in the formula (7-a) coordinate transform $z^{\&prime;}=z+\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z}^{p_n+1}---(7-a)$ Conversion and getting.F ' (z ') be the periodic sample structure that is adopted usually, such as square wave, sine wave etc.Fig. 8 b has represented the method through the sampling structure F (z) that obtains having nonlinear II type suc as formula (5) described coordinate transform and warble with periodic sampling structure F ' (z '), and F ' wherein (z ') be a square wave.Particularly, at first, from F ' (z '), choose N point (z ' _k, F ' (z ' _k)) (k gets N from 1), and guarantee that N is enough greatly so that choose 2 points at least in each cycle of F ' (z ').Secondly, with z ' _kAnd z _kSubstitution formula (7) obtains about z _kEquation ${z^{\&prime;}}_k=z_k+\underset{n=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_n{z_k}^{p_n+1}---(7-b)$ Then, separate this equation by the method for parsing commonly known in the art or numerical value and obtain z _k, make again F ' (z ' _k)=F (z _k), just can obtain corresponding point (z among the F (z) _k, F (z _k)), these points have just been represented sampling structure F (z).

Fig. 9 shows according to required group delay and composes to determine p _nAnd a _n(n=1,2,3 ...) the flow chart of method.In step 1, the group delay response spectrum τ (λ) required according to reality reasonably chooses one group of p _nAnd a _n(n=1,2,3 ...) as initial value (for example examples of implementation 1 or 2 in " detailed Description Of The Invention "); Then, enter step 2, obtain to have accordingly the shan F (z) that non-linear II type is warbled by the shan F ' of one-period (z ') according to foregoing method of coordinates transform; Then, enter step 3, obtain to have (λ) as the group delay response spectrum τ ' of the Bragg grating of the described sampling structure of F (z) by numerical simulation or experiment; Then, enter step 4, relatively τ ' (λ) with τ (λ), see whether they conform in actual permissible accuracy; If conform to, then enter step 6, whole process finishes, otherwise returns step 5, revises p _nAnd a _n(n=1,2,3 ...) value, repeat said process again.

Utilize said method can obtain following several Bragg grating that non-linear II type is warbled that has, the sampling structure of wherein described below first embodiment and second embodiment make the group delay response spectrum of Bragg grating be respectively incident wave bag centre wavelength once and quadratic function, and actual required group delay spectrum generally contains the once more with the secondary power composition of incident wave bag centre wavelength.Therefore, when using alternative manner shown in Figure 9, the p of available these two kinds of sampling structures _nAnd a _nAs the initial value of iteration, its advantage is to reduce number of iterations.

In first embodiment, the present invention proposes one and do not have the I type and warble but have the sampling Bragg grating that non-linear II type is warbled, its sampling structure is by making p in the formula (5) ₁=1 and a _n=0 (for n=2,3 ...) obtain, be shown below

F (z)=F ＇ (z+a ₁z ²) that is to say that (8-a) the sampling structure F (z) of this sampling Bragg grating is with the one-period function F ' (z ') coordinate transform through being shown below

Z ＇=z+a ₁z ²(8-b) conversion and getting.A wherein ₁Relevant with the group delay response spectrum that reality is required, can obtain by method shown in Figure 9.Figure 10 a has shown the group delay response spectrum (can be obtained by the described transfer matrix method simulation of reference paper D16) of-1 grade of zone of reflections of a this sampling Bragg grating.The F ' that uses when designing this grating (z ') be one-period Z ₀=0.5mm, duty ratio=0.5, value are 0 and 1 square wave, and get a in coordinate transform ₁=-2.5 * 10 ^-3Mm ^-1As can be seen from the figure, under first approximation, group delay response is the linear function of incident wave bag centre wavelength.Therefore, this grating can be used for the 2nd order chromatic dispersion in the static compensation optical fiber telecommunications system.Figure 10 b has shown a group delay response spectrum that only has the Bragg grating that linear I type warbles, and the chirp value of this grating is 0.083nm/cm.Figure 10 a and 10b are compared as can be seen, in the required wave-length coverage of reality, utilize the II type to warble and to obtain the group delay response spectrum of warbling equivalent with the I type.

In a second embodiment, the present invention proposes one not to have the I type and warbles but have the sampling Bragg grating that non-linear II type is warbled, and its sampling structure is by making p in the above-mentioned formula (5) ₁=1/2 and a _n=0 (for n=2,3 ...) obtain, promptly

F (z)=F ＇ (z+a ₁z ^3/2) that is to say that (9-a) the sampling structure F (z) of this sampling Bragg grating is with the one-period function F ' (z ') coordinate transform through being shown below

Z ＇=z+a ₁z ^3/2(9-b) conversion and getting.A wherein ₁Relevant with the group delay response spectrum that reality is required, can obtain by method shown in Figure 9.Figure 11 has shown the group delay response spectrum (being obtained by the described transfer matrix method simulation of reference paper D16) of-1 grade of zone of reflections of a this sampling Bragg grating.The F ' that uses when designing this grating (z ') be one-period Z ₀=0.5mm, duty ratio=0.5, value are 0 and 1 square wave, and get a in coordinate transform ₁=0.11 * 10 ^-1/2Mm ^-1/2As can be seen from Figure 11, under first approximation, group delay response is the quadratic function of incident wave bag centre wavelength.Therefore, this grating can be used for the third-order dispersion in the static compensation optical fiber telecommunications system.The group delay response spectrum that only has the Bragg grating that non-linear I type warbles among Figure 11 and the reference paper D6 is compared as can be seen, in the required wave-length coverage of reality, utilize the II type to warble to obtain and the warble group delay response spectrum of equivalence of I type.

Shown simultaneously also among Figure 11 that temperature with grating is elevated to 100 ℃ or its is produced group delay response spectrum after 0.05% the tensile strain.In both cases, group delay response spectrum all along the abscissa translation one segment distance, and variation has all taken place in the slope of the group delay of each wavelength correspondence spectrum.Therefore, this grating is added that one can be regulated the temperature of grating or can make grating produce the device of dynamic strain, it just can be used to dynamic dispersion compensation.

In the 3rd embodiment, the invention allows for a kind of like this Bragg grating, it have with second embodiment in the identical sampling structure of sampling Bragg grating, and not having the I type warbles, and the fiber waveguide at its place is to be made by the material with birefringent characteristic, thereby between the group delay response spectrum to the light of both direction polarization a relative translation is arranged.Figure 12 a and 12b have shown the group delay response spectrum of-1 grade of zone of reflections of a this sampling Bragg grating, wherein solid line and dotted line are represented the situation of two different polarization directions respectively, Figure 12 a is the comparison of temperature T when being 20 ℃ and 100 ℃, and Figure 12 b is that no strain and strain are 0.05% o'clock comparison.Except the fiber waveguide at place has the birefringent characteristic, other structure of this grating is all identical with grating among second embodiment.Therefore, see group delay response spectrum separately to the light of some direction polarizations, as broad as long with Figure 11.But on each wavelength, there is a difference in group delay response to the light of both direction polarization, and because the group delay response of two polarization directions is quadratic functions of incident wave bag centre wavelength under first approximation, so their difference is the linear function of incident wave bag centre wavelength.The temperature of grating is elevated to 100 ℃ or its is produced after 0.05% the tensile strain, the group delay response spectrum of two polarization directions all along the abscissa translation one segment distance, their difference also moves thereupon simultaneously.Therefore, this grating is added that one can be regulated the temperature of grating or can make grating produce the device of dynamic strain, it just can be used to dynamic polarization mould disperse compensation.This grating is used for dynamic dispersion compensation also has an advantage: it is the linear function of incident wave bag centre wavelength to the corresponding difference of the group delay of two polarization directions, and this helps reducing temperature and the tuning difficulty (and this point utilizes linear II type to warble and can't accomplish) of stress.

Bragg grating in the foregoing description all only has non-linear II type warbles, but the utilization that utilization that non-linear II type is warbled and I type are warbled is not repelled mutually.Therefore, in fact a Bragg grating can have these two kinds simultaneously and warbles, and the two complements one another.

In the 4th embodiment, we make a sampling Bragg grating have simultaneously that linear I type is warbled and above-mentioned first embodiment described in non-linear II type warble.Linear I type is warbled and can be obtained with the phase mask of band linear chrip commonly known in the art, but the specific I type that phase mask produced is warbled and is fixed, this slope that makes the group delay response of Bragg grating compose is also fixed, so if will obtain to have the group delay response spectrum of Different Slope, will use different phase masks, this has just increased the cost that spends in the research and production on the phase mask.Yet, because warbling, non-linear II type do not rely on phase mask, so have these two kinds simultaneously when warbling when a Bragg grating, can adjust the slope of group delay response spectrum by adjusting parameter that non-linear II type warbles.Figure 13 has shown that linear I type warbles and the warble group delay response spectrum of the Bragg grating before and after combining of the non-linear II type described in above-mentioned first embodiment, the no II type of the solid line representative situation of warbling wherein, and dash line and chain-dotted line are represented respectively and are had non-linear II type described in top first embodiment and warble and a ₁=5 * 10 ^-4Mm ^-1And a ₁=-5 * 10 ^-4Mm ^-1Situation.As can be seen from Figure 13, add that non-linear II type is warbled after, the slope of the corresponding spectrum of group delay has changed, and works as a ₁Slope reduces when getting positive number, and works as a ₁Slope increases when getting negative, and this has just increased the flexibility of design and manufacturing greatly, and has saved the expense on phase mask.

According to embodiments of the invention, the present invention proposes a kind of warble Bragg grating of sampling structure of non-linear II type that has, it does not rely on the I type and warbles and just can provide various group delay responses spectrum replenishing chromatic dispersion in certain specific zone of reflections of grating as required, and described non-linear II type is warbled sampling period of sampling structure F (z) much larger than the grating cycle.Save the expense on the phase mask thereby reduced, and made that required control precision reduces in the manufacturing process, thereby reduced manufacturing cost.Simultaneously, the present invention has also overcome the linear II type in the prior art and has warbled and be difficult to be utilized separately for the problem of dispersion compensation, in certain specific zone of reflections of grating, can obtain the required group delay response spectrum of varied reality, and warble when combining with the I type, can in a channel, adjust the group delay response spectrum of grating.However, it should be understood that the foregoing description only as schematic and nonrestrictive, can do various modification or improvement in the protection range of in described claim, determining of the present invention.

Reference paper: D1:F.Ouellette, " using the linear chrip Bragg grating filter in fiber waveguide to eliminate chromatic dispersion (Dispersion cancellation using linearly chirped Bragg grating filters inoptical waveguides); " Opt.Lett., vol.12, no.10, pp.847-849,1987.D2:K.O.Hill, F.Bilodeau, B.Malo, T.Kitagawa, S.Th é riault, D.C.Johnson, and J.Albert, " the chirped fiber Bragg grating (Chirpedin-fiber Bragg gratings for compensation of optical-fiber dispersion) that is used for the compensated fiber chromatic dispersion. " Opt.Lett., vol.19, no.17, pp.1314-1316,1994.D3:K.-M.Feng, J.X.Cai, V.Grubsky, D.S.Starodubov, M.I.Hayee, S.Lee, X.Jiang, A.E.Willner, and J.Feinberg, " utilizing the Fiber Bragg Grating FBG with non-linear chirp of the novel voltage tuning of a clock that the optical communication system of 10-Gb/s is carried out dynamic dispersion compensation (Dynamic dispersion compensation in a 10-Gb/s optical system using anovel voltage tuned nonlinearly chirped fiber Bragg grating), " IEEE Photon.Technol.Lett., vol.11, no.3, pp.373-375,1999.D4:S.Lee, R.Khosravani, J.Peng, V.Grubsky, D.S.Starodubov, A.E.Willner and J.Feinberg, " Fiber Bragg Grating FBG that utilization has birefringence and non-linear chirp carries out tunable polarization mode disperse compensation (Adjustable compensation of polarizationmode dispersion using a high-birefringence nonlinearly chirped fiber Bragggrating); " IEEE Photon.Technol.Lett., vol.11, no.10, pp.1277-1279,1999.D5:K.O.Hill and G.Meltz, " basic principle of Fiber Bragg Grating FBG and outline (FiberBragg grating technology fundamentals and overview), " J.LightwaveTechnol, .vol.15, no.8, pp.1263-1276,1997.D6:T.Komukai and M.Nakazawa, " being used for the manufacturing (Fabrication of non-linearly chirped fiber Bragggratings for higher-order dispersion compensation) of the Fiber Bragg Grating FBG with non-linear chirp of high-order dispersion compensation; " Opt.Commun., vol.154, no.1-3, pp.5-8,1998.D7:R.Kashyap, P.F.McKee, R.J.Campbell and D.L.Williams, " a kind of new method (Novel method of producing all fibrephotoinduced chirped gratings) of making the photic chirp grating of full optical fiber; " Electron.Lett., vol.30, no.12, pp.996-998,1994.D8:K.Sugden, L.Bennion, A.Molony, and N.J.Copner, " in exposure process, making optical-fiber deformation and the chirp grating (Chirped gratings produced inphotosensitive optical fibres by fibre deformation during exposure) that in light-sensitive optical fibre, produces, " Electron.Lett., vol.30, no.5, pp.440-442,1994.D9:K.C.Byron and H.N.Rourke, " making chirped fiber grating (Fabrication of chirped fibre gratings by novel stretch and writetechnique); " by the method that stretching writes Electron.Lett., vol.31, no.1, pp.60-61,1995.D10:J.A.R.Williams, L.A.Everall, L.Bennion, and N.J.Doran, " being used for the manufacturing (Fiber Bragg grating fabrication fordispersion slope compensation) of the Fiber Bragg Grating FBG of dispersion slope compensation; " IEEE Photon.Technol.Lett., vol.8, no.9, pp.1187-1189,1996.D11:M.A.Putnam, G.M.Williams, and E.J.Friebele, " manufacturing of the chirped fiber Bragg grating with strain gradient of taper (Fabrication of tapered; strain-gradientchirped fibre Bragg gratings), " Electron.Lett., vol.31 no.4, pp.309-310,1995.D12:W.H.Loh, M.J.Cole, M.N.Zervas, S.Barcelos, and R.I.Laming, " based on the baroque grating (Complex grating structures with uniform phase masks based on themoving fiber-scanning beam technique) of the even phase mask manufacturing of the utilization of moving fiber-scanning light beam method, " Opt.Lett., vol.20, no.20, pp.2051-2053.1995.D13:P.C.Hill and B.J.Eggleton, " warble (the Strain gradient chirp of fibre Bragg gratings) of the light Bragg grating that strain gradient causes; " Electron.Lett., vol.30, no.14, pp.1172-1174,1994.D14:J.Lauzon, S.Thibault, J.Martin, and F.Ouellette, " utilizing temperature gradient to produce the enforcement and the evaluation (Implementation andcharacterization of fiber Bragg gratings linearly chirped by a temperaturegradient) of the Fiber Bragg Grating FBG of linear chrip; " Opt.Lett., vol.19, no.23, pp.2027-2029,1994.D15:X.-f.Chen, Y.Luo, C.-c.Fan, T.Wu, and S.-z.Xie, " resolution table with sampling Bragg grating that the sampling period warbles is addressed its application (Analytical expression of sampled Bragg gratings with chirp in thesampling period and its application in dispersion management design in aWDM system) in the dispersion management of optical WDM communication system, " IEEE Photon.Technol.Lett., vol.12, no.8, pp.1013-1015,2000.D16:T.Erdogan, " fiber grating spectrum (Fiber grating spectra); " J:LightwaveTechnol., vol.15, no.8., pp.1277-1294,1997.

Claims (27)

1. An optical waveguide device, comprising: an optical waveguide for transporting optical energy and having an effective refractive index n _eff profile; A section formed on the optical waveguide is used to provide the required group delay spectrum effective refractive index perturbation region, wherein the refractive index perturbation is shown in the following formula (4): ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;\; n}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\&Delta;n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left(z\right)\left]\right\}f\left(z\right)---\left(4\right)$ Wherein z is the coordinate along the grating direction, the period of Λ ₀ grating starting point, The average value of the effective index perturbation over a grating period, is the magnitude of the fast-varying component of the effective refractive index perturbation,  is an additional phase term representing the chirp of the grating period, F(z) is called the sampling function, and its period is called the sampling period Z, where Features: F(z) is obtained by a periodic envelope function F'(z') through coordinate transformation, as shown in the following formula (5): $f\left(z\right)=f^{\&prime;}\left(z^{\&prime;}\right)=f^{\&prime;}(z+\underset{\mathrm{no}=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_{\mathrm{no}}{z}^{p_{\mathrm{no}}+1})---\left(5\right)$ 2. The optical waveguide device according to claim 1, characterized in that: a ₁ ≠0, and when n=2, 3, ..., a _n =0; and p ₁ =1, so that the sampling represented by the above formula (5) The function F(z) is: F(z)=F'(z+a ₁ z ² ) 3. The optical waveguide device of claim 2, characterized in that:

(z) and (z) are constants respectively

and , so the effective refractive index perturbation shown in the above formula (4) is: ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;n}}_{\mathrm{dc}}+{\mathrm{\&Delta;\; n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left]\right\}{f}^{\&prime;}(z+a_1{z}^2)$ 4. The optical waveguide device according to claim 1, characterized in that: a ₁ ≠0, and when n=2, 3, ..., a _n =0; and p ₁ =1/2, thus the above formula (5) shows The sampling function F(z) is: F(z)=F'(z+a ₁ z ^3/2 ) 5. The optical waveguide device of claim 4, characterized in that: (z) and (z) are constants respectively

and , so the effective refractive index perturbation shown in the above formula (4) is: ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;n}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\&Delta;n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left]\right\}{f}^{\&prime;}(z+a_1{z}^{3/2})$ 6. The optical waveguide device according to claim 4, characterized in that said optical waveguide is made of a material having birefringence properties. 7. The optical waveguide device of claim 5, wherein the optical waveguide is made of a material having birefringence properties. 8. The optical waveguide device according to claim 4, characterized in that: said optical waveguide device further comprises a device for changing the temperature distribution in the optical waveguide and/or causing a longitudinal strain in the optical waveguide. 9. The optical waveguide device according to claim 5, characterized in that: said optical waveguide device further comprises a device for changing the temperature distribution in the optical waveguide and/or causing a longitudinal strain in the optical waveguide. 10. The optical waveguide device according to claim 6, characterized in that: said optical waveguide device further comprises a device for changing the temperature distribution in the optical waveguide and/or causing a longitudinal strain in the optical waveguide. 11. The optical waveguide device according to claim 7, characterized in that: said optical waveguide device further comprises a device for changing the temperature distribution in the optical waveguide and/or causing a longitudinal strain in the optical waveguide. 12. The optical waveguide device of claim 1, wherein said optical waveguide is an optical fiber. 13. The optical waveguide device of claim 2, wherein said optical waveguide is an optical fiber. 14. The optical waveguide device of claim 3, wherein said optical waveguide is an optical fiber. 15. The optical waveguide device of claim 4, wherein said optical waveguide is an optical fiber. 16. The optical waveguide device of claim 5, wherein said optical waveguide is an optical fiber. 17. The optical waveguide device of claim 6, wherein said optical waveguide is an optical fiber. 18. The optical waveguide device of claim 7, wherein said optical waveguide is an optical fiber. 19. The optical waveguide device of claim 8, wherein said optical waveguide is an optical fiber. 20. The optical waveguide device of claim 9, wherein said optical waveguide is an optical fiber. 21. The optical waveguide device of claim 10, wherein said optical waveguide is an optical fiber. 22. The optical waveguide device of claim 11, wherein said optical waveguide is an optical fiber. 23. A method for manufacturing an optical waveguide device, comprising the steps of: providing an optical waveguide for transmitting optical energy and having an effective refractive index n _eff distributed along the waveguiding direction, An effective refractive index perturbation zone for providing the required group delay spectrum is formed on a section of the optical waveguide, wherein the effective refractive index perturbation is shown in the following formula (4): ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;n}}_{\mathrm{dc}}\left(z\right)+{\mathrm{\&Delta;\; n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left(z\right)\left]\right\}f\left(z\right)---\left(4\right)$ Wherein z is the coordinate along the grating direction, the period of Λ ₀ grating starting point,

the average value of the effective index perturbation over one grating period (also called the DC component of the effective index perturbation), is the magnitude of the fast-varying component of the effective index perturbation (also known as the AC component of the effective index perturbation),  is an additional phase term representing the chirp of the grating period, and F(z) is called the sampling function, and its period is called the sampling period z, characterized by: According to the required group delay spectrum, F(z) is determined by a periodic envelope function F'(z') through coordinate transformation, as shown in the following formula (5): $f\left(z\right)=f^{\&prime;}\left(z^{\&prime;}\right)=f^{\&prime;}(z+\underset{\mathrm{no}=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_{\mathrm{no}}{z}^{p_{\mathrm{no}}+1})---\left(5\right)$ . 24. The method according to claim 23, characterized in that: determine the effective refractive index perturbation according to the required group delay spectrum The steps of the sampling function F(z) in include: Step 1, according to the required group delay response spectrum τ(λ), reasonably select a set of p _n and a _n (n=1, 2, 3, ...) as initial values; Step 2, calculate by the following formula ${\mathrm{\&Delta;n}}_{\mathrm{eff}}\left(z\right)=\{{\mathrm{\&Delta;n}}_{\mathrm{dc}}+{\mathrm{\&Delta;n}}_{\mathrm{ac}}\left(z\right)\cos [\frac{2\mathrm{\&pi;}}{{\mathrm{\&Lambda;}}_0}z+\mathrm{\&phi;}\left]\right\}{f}^{\&prime;}(z+\underset{\mathrm{no}=1}{\overset{\&infin;}{\mathrm{\&Sigma;}}}{a}_{\mathrm{no}}{z}^{p_{\mathrm{no}}+1})$ The group delay response spectrum τ'(λ) of the described Bragg grating with nonlinear sampling structure; Step 3, determining whether the difference between the calculated group delay response spectrum τ' (λ) and the required group delay response spectrum τ (λ) is within the required accuracy; Step 4, if not within the required precision, adjust the values of p _n and a _n (n=1, 2, 3, ...); Repeat steps 2 to 4 above until the difference between the calculated group delay response spectrum τ'(λ) and the required group delay response spectrum τ(λ) is within the required accuracy. 25. The method of claim 24, wherein: The step 1 is: a _n =0 (n=2, 3, . . . ) and p ₁ =1 are selected as initial values. 26. The method of claim 24, wherein: The step 1 is: select a _n =0 (n=2, 3, . . . ) and p ₁ =1/2 as initial values. 27. The method of any one of claims 23-26, characterized in that: said periodic sampling function F'(z') is a square wave.

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