CN103760631B - A kind of Ge-doped double-core photonic crystal fiber - Google Patents
A kind of Ge-doped double-core photonic crystal fiber Download PDFInfo
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- CN103760631B CN103760631B CN201310688666.6A CN201310688666A CN103760631B CN 103760631 B CN103760631 B CN 103760631B CN 201310688666 A CN201310688666 A CN 201310688666A CN 103760631 B CN103760631 B CN 103760631B
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Abstract
The invention discloses a kind of Ge-doped double-core photonic crystal fiber, include quartz body, quartz body center mixes the conglobate Ge-doped region I of germanium structure, quartz body is provided with multiple big airport, multiple big airports are evenly distributed on around Ge-doped region I, in quartz body, also bias mixes the conglobate Ge-doped region II of germanium structure, is additionally provided with multiple little airport in quartz body, and multiple little airports are evenly distributed on around Ge-doped region II.
Description
Technical field
The present invention relates to field fiber, a kind of Ge-doped double-core photonic crystal fiber.
Background technology
In modern optical fiber telecommunications system, the loss of silica fibre is to limit transfer rate, transmission range and transmission
One of key factor of capacity boost.
The loss of optical fiber is that the luminous power caused due to the reason such as absorbed, scattering reduces phenomenon.The damage of optical fiber
Consumption make optical signal pulses in transmitting procedure gradually decay die down, cause optical fiber telecommunications system error code to increase, limit
Make the distance of optical signal pulses repeaterless transmission.The loss factor of silica fibre has decreased to substantially it at present
Theoretical boundary, the research without fiber manufacturing Material Field breaks through, under its loss value is difficult to further
Fall.It is true that widely used image intensifer solves restricted problem is lost in modern optical fiber telecommunications system.At present
Common image intensifer has semiconductor optical amplifier, parametric optical amplifier, all kinds of doping image intensifer and optical fiber to draw
Graceful amplifier (Fiber Raman Amplifier, FRA) etc..Wherein, FRA due to have noise coefficient low,
Gain band is flexible, can realize the many merits such as broadband amplification, it has also become modern wavelength-division multiplex (WDM) optical fiber
One of Primary Component of communication system.
The physical basis of FRA work is stimulated Raman scattering (Stimulited Raman Scattering, SRS)
Phenomenon.In general, in nonlinear optical medium, the high-octane laser of transmission will scatter, little by one
Portions incident power transfers to the luminous power that another frequency moves down, and the knots modification of frequency is determined by the character of medium,
This process is referred to as spontaneous Raman scattering.If the heavy pumping light of a weak signal light and a higher frequency exists simultaneously
Transmitting in nonlinear optical medium, and the frequency of flashlight is within the Raman gain bandwidth of medium, then due to
Raman scattering effect, weak signal light can obtain energy from heavy pumping light and be amplified, and this process is exactly SRS.
If using optical fiber as nonlinear dielectric, it is possible to make FRA.
The mathematical model of FRA stable state can be attributed to power below coupled-differential equations:
Wherein Pj、vjAnd αjPower, frequency and the attenuation quotient of Shij road light, n=n respectivelyp+ns, np
And nsIt is pump light and flashlight number, g respectivelyR(vi-vj) it is the Raman gain coefficienct of fiber medium used,
Z is the transmission direction of flashlight, AeffFor the effective core area of optical fiber, formula (2) define:
Wherein ψ represents the mould field intensity distribution of light wave, and subscript p and s represent pump light and flashlight, integration respectively
Subscript V of symbol represents the whole cross-sectional area that respective mode field is full of.γR=gR/AeffIt is defined as Raman gain
Efficiency, in general optical fiber, AeffVarying less with frequency of light wave, so γRAnd gRShape basic
Unanimously.S (j) is a sign flag, takes negative sign when taking positive sign, reverse transfer when jth road light forward transmits,
KeffIt is polarization correlation factor, typically takes 2.0.
When FRA is applied in WDM fiber communication system, there is in wider service band preferable gain
Spectrum flatness is to it basic demand, but due to drawing currently as the various optical fiber of FRA gain media
Graceful gain efficiency coefficient is the most uneven, only can not make with single pumping source so understanding according to formula (1) and formula (2)
Conventional FRA has smooth gain spectral in wider wave band.Traditional all kinds of fiber manufacturing FRA are utilized to there is also
Another one problem, owing to Raman gain coefficienct all ratios of traditional fiber are relatively low, so the optical fiber of general FRA
Length even to tens kms at tens kms, makes the FRA of discrete be difficult to reduce volume, limits discrete
FRA promotes the use of.
Summary of the invention
It is an object of the invention to provide a kind of Ge-doped double-core photonic crystal fiber, to solve Raman in prior art
Amplify and the loss restricted problem of optical fiber telecommunications system.
In order to achieve the above object, the technical solution adopted in the present invention is:
A kind of Ge-doped double-core photonic crystal fiber, it is characterised in that: include quartz body, in described quartz body
The heart mixes the conglobate Ge-doped region I of germanium structure, Ge-doped region I form fibre core I, be provided with in quartz body
Multiple big airports, multiple big airports are evenly distributed on around Ge-doped region I, and in quartz body, also bias is mixed
Enter the conglobate Ge-doped region II of germanium structure, Ge-doped region II form fibre core II, described Ge-doped region I
Diameter is more than Ge-doped region II, and Ge-doped region I concentration is different from Ge-doped region II concentration, quartz body
In be additionally provided with multiple little airport, multiple little airports are evenly distributed on around Ge-doped region II, described
Big airport diameter is more than little airport diameter.
The Ge-doped double-core photonic crystal fiber of described one, it is characterised in that: multiple big airports composition multi-turn
Regular hexagon centered by Ge-doped region I, big airport adjacent in each circle big airport of regular hexagon it
Between spacing the most equal, multiple little airports composition multi-turn regular hexagon centered by Ge-doped region II, respectively
Between little airport adjacent in the circle little airport of regular hexagon, spacing is the most equal, and big airport spacing is more than little
Airport spacing.
The invention discloses a kind of Ge-doped double-core photonic crystal fiber, by the parameter to this GD-TC-PCF
Design, its effective core area is Tong Bu with the change of wavelength and the tendency of changes of Raman gain coefficienct, thus it draws
Graceful gain efficiency coefficient becomes the most smooth.When using this optical fiber as the gain media of raman amplifier, its high and
Smooth raman gain efficiency coefficient improves the conversion efficiency of pumping source, only uses single pumping source with regard to energy simultaneously
Obtain wider, more smooth Raman amplifier gain spectrum.As can be seen here, utilize that the present invention's is novel
GD-TC-PCF manufacture raman amplifier can overcome well current optical fiber telecommunications system loss limit because of
Element, this is for improving the quality of FRA and promoting FRA to have important in the application further of fiber optic communication field
Meaning.
Accompanying drawing explanation
Fig. 1 is present configuration schematic diagram.
Fig. 2 is Ge-doped region II structural representation in the present invention.
Fig. 3 is that in the specific embodiment of the invention, Raman gain coefficienct and effective core area synchronize with wavelength is close
Situation of change schematic diagram.
Fig. 4 is fiber Raman amplifier gain spectral fluctuation situation schematic diagram in the specific embodiment of the invention.
Detailed description of the invention
As shown in Figure 1 and Figure 2.A kind of Ge-doped double-core photonic crystal fiber, includes quartz body 1, quartz
Body 1 center mixes the conglobate Ge-doped region I of germanium structure, Ge-doped region I form fibre core I, quartz body 1
In be provided with multiple big airport 2, multiple big airports 2 are evenly distributed on around Ge-doped region I, quartz
In body 1, also bias mixes the conglobate Ge-doped region II of germanium structure, Ge-doped region II form fibre core II, germanium
Doped region I diameter is more than Ge-doped region II, and Ge-doped region I concentration is with Ge-doped region II concentration not
With, quartz body 1 is additionally provided with multiple little airport 3, multiple little airports 3 are evenly distributed on Ge-doped district
Around the II of territory, big airport 2 diameter is more than little airport 3 diameter.
Multiple big airports 2 form multi-turn regular hexagon centered by Ge-doped region I, respectively enclose regular hexagon
Between big airport 2 adjacent in big airport 2, spacing is the most equal, and multiple little airports 3 form multi-turn with germanium
Regular hexagon centered by doped region II, little airport 3 adjacent in each circle little airport of regular hexagon 3
Between spacing the most equal, and big airport 2 spacing is more than little airport 3 spacing.
In the present invention, the diameter mixing germanium region of fibre core I and fibre core II is different, and germania concentration is the most different, bag
The diameter of the airport enclosing them is the most different, and larger-diameter fibre core I is at the center of whole optical fiber, less
The fibre core II of diameter is distributed prejudicially.Wherein λ and d is spacing and the diameter of little airport respectively, Λ and D divides
Not being spacing and the diameter of big airport, R and r represents the Ge-doped radius of two fibre core I and II respectively.
Embodiments of the invention: set single pumping wavelength as 1.495um, flashlight is commonly used in the range of fiber optic communication
C-band part, i.e. wave-length coverage is 1.530-1.565um altogether 35nm.Fig. 3 gives the effective fine of the present invention
Core area and the synchronous situation of Raman gain coefficienct change.It can be seen from figure 3 that photonic crystal fiber of the present invention has
Effect core area is the most consistent with Raman gain coefficienct variation tendency, close to parallel.So, with this photonic crystal light
Even if its gain spectral also can be the most smooth in the case of single pumping for the fine raman amplifier manufactured.For testing further
Demonstrate,prove this effect, single pumping this photonic crystal fiber to 5km that use wavelength is 1.495um, power is 0.5W
Carrying out pumping and constitute Raman Fiber Amplifier, the gain spectral of its C-band is as shown in Figure 4.From fig. 4, it can be seen that whole
The gain spectral fluctuation of individual C-band amplifier is the least, only 0.49dB.It addition, because fiber Raman amplifier
Amplify wave band only relevant with the wavelength of pumping, for different pumping wavelengths, by choosing different size air
Bore dia, airport spacing, Ge-doped radius and concentration, the photonic crystal fiber of the present invention can be used for S-band,
The Raman amplifiction of other band signal light such as L-band.
Claims (1)
1. a Ge-doped double-core photonic crystal fiber, it is characterized in that: include quartz body, described quartz body center mixes the conglobate Ge-doped region I of germanium structure, fibre core I is formed by Ge-doped region I, quartz body is provided with multiple big airport, multiple big airports are evenly distributed on around Ge-doped region I, in quartz body, also bias mixes the conglobate Ge-doped region II of germanium structure, fibre core II is formed by Ge-doped region II, described Ge-doped region I diameter is more than Ge-doped region II, and Ge-doped region I concentration is different from Ge-doped region II concentration, quartz body is additionally provided with multiple little airport, multiple little airports are evenly distributed on around Ge-doped region II, described big airport diameter is more than little airport diameter;
Described multiple big airport composition multi-turn regular hexagon centered by Ge-doped region I, between big airport adjacent in each circle big airport of regular hexagon, spacing is the most equal, multiple little airports composition multi-turn regular hexagon centered by Ge-doped region II, between little airport adjacent in each circle little airport of regular hexagon, spacing is the most equal, and big airport spacing is more than little airport spacing.
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CN101071189A (en) * | 2007-04-30 | 2007-11-14 | 电子科技大学 | Optical fiber |
CN101093338A (en) * | 2007-04-30 | 2007-12-26 | 电子科技大学 | Gain medium of Raman amplifier |
CN101196593A (en) * | 2006-12-04 | 2008-06-11 | 德雷卡通信技术公司 | Optical fiber |
CN102607609A (en) * | 2012-03-12 | 2012-07-25 | 天津理工大学 | Novel high-sensitivity photonic crystal fiber terahertz evanescent wave sensing device |
CN102819062A (en) * | 2012-07-31 | 2012-12-12 | 燕山大学 | Air hole square array fiber core annular doping four-core photonic crystal fiber |
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2013
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Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101196593A (en) * | 2006-12-04 | 2008-06-11 | 德雷卡通信技术公司 | Optical fiber |
CN101071189A (en) * | 2007-04-30 | 2007-11-14 | 电子科技大学 | Optical fiber |
CN101093338A (en) * | 2007-04-30 | 2007-12-26 | 电子科技大学 | Gain medium of Raman amplifier |
CN102607609A (en) * | 2012-03-12 | 2012-07-25 | 天津理工大学 | Novel high-sensitivity photonic crystal fiber terahertz evanescent wave sensing device |
CN102819062A (en) * | 2012-07-31 | 2012-12-12 | 燕山大学 | Air hole square array fiber core annular doping four-core photonic crystal fiber |
Non-Patent Citations (2)
Title |
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C band single pump photonic crystal fiber Raman amplifier;JIANG HaiMing, et al.;《Chinese Science Bulletin》;20100228;第55卷(第6期);555-559 * |
具有优良喇曼增益属性的新型非对称双芯光子晶体光纤;姜海明等;《中国科学》;20091231;第39卷(第7期);第1256-1260页 * |
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