Chromatic dispersion detection method and device for optical transmission network and storage medium
10153847 ยท 2018-12-11
Assignee
Inventors
- Jizheng Guo (Shenzhen, CN)
- Cheng Yu (Shenzhen, CN)
- Haitao Zhou (Shenzhen, CN)
- Xianjun Zeng (Shenzhen, CN)
Cpc classification
H04B10/6162
ELECTRICITY
H04B10/07951
ELECTRICITY
H04B10/25133
ELECTRICITY
International classification
Abstract
The disclosure discloses a Chromatic Dispersion (CD) detection method for an optical transmission network. Data of two polarization states orthogonal to each other is converted from time-domain data to frequency-domain data, extraction is performed on the frequency-domain data and a linear combination operation is performed on the extracted frequency-domain data, an argument of a CD value of the data of the two polarization states are obtained according to a result of the linear combination operation, and the CD value is estimated according to the argument of the CD value of the data of the two polarization states. The disclosure further discloses a CD detection device for the optical transmission network and a storage medium.
Claims
1. A Chromatic Dispersion (CD) estimation method for an optical transmission network comprising: receiving data of two polarization states orthogonal to each other from an In-phase/Quadrature (IQ) balance; converting the data of the two polarization states orthogonal to each other from time-domain data to frequency-domain data by adopting a discrete Fourier transform, with N=2.sup.t and t being a natural number greater than 2, and the frequency-domain data converted from the data of the two polarization states being set as X(k) and Y(k) respectively, k=0, 1, . . . , N1, then
2. The CD estimation method according to claim 1, wherein performing the linear combination operation on the extracted data from the frequency-domain data comprises: step a: obtaining two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U) as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in three different directions according to X.sup.U[k], X.sup.L[k], Y.sup.U[k] and Y.sup.L[k]:
R.sub.n[k]=X.sub.n.sup.(U)[k].Math.conj{X.sub.n.sup.(L)[k]}, where conj() is a conjugate operation, k=0, . . . N1 and n=1, 2, 3; step c: setting a first interval value as .sub.1=2 and a second interval value as .sub.2=32, and calculating accumulated values F.sub.1 and F.sub.2 corresponding to these two interval values in different directions according to R.sub.1[k], R.sub.2[k] and R.sub.3[k]:
3. The CD estimation method according to claim 2, wherein obtaining the argument of the CD value of the data of the two polarization states according to the result of the linear combination operation comprises: calculating arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states according to F.sub.1.sub._.sub.sum and F.sub.2.sub._.sub.sum respectively:
4. The CD estimation method according to claim 3, wherein estimating the CD value according to the argument of the CD value of the data of the two polarization states comprises: obtaining a CD estimation coefficient .sub.1 according to the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states, and estimating the CD value CD according to the CD estimation coefficient .sub.1:
CD=.sub.1delta_CD, where delta_CD=1000CN_fft/(2f.sup.2lambda.sup.2), C is a light velocity in an optical fibre, N_fft is a discrete Fourier transform length, f is a symbol rate, and lambda is a wavelength.
5. A Chromatic Dispersion (CD) estimation device for an optical transmission network comprising: a processor; and a memory for storing instructions executable by the processor; wherein the processor is configured to: receive data of two polarization states orthogonal to each other from an In-phase/Quadrature (IQ) balance; convert the data of the two polarization states orthogonal to each other from time-domain data to frequency-domain data by adopting a discrete Fourier transform, with N=2.sup.t and t being a natural number greater than 2, and the frequency-domain data converted from the data of the two polarization states being set as X(k) and Y(k) respectively, k=0, 1, . . . , N1, then
6. The CD estimation device according to claim 5, wherein the processor is configured to: 1): obtain two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U)as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in three different directions according to X.sup.U[k], X.sup.L[k], Y.sup.U[k] and Y.sup.L[k]:
R.sub.n[k]=X.sub.n.sup.(U)[k].Math.conj{X.sub.n.sup.(L)[k]}, where conj() is a conjugate operation, k=0, . . . N1 and n=1, 2, 3; 3): set a first interval value as .sub.1=2 and a second interval value as .sub.2=32, and calculate accumulated values F.sub.1 and F.sub.2 corresponding to these two interval values in different directions according to R.sub.1[k], R.sub.2[k] and R.sub.3[k]:
7. The CD estimation device according to claim 6, wherein the processor is configured to calculate arguments .sub.1 and .sub.2 of the CD value the data of the two polarization states according to F.sub.1.sub._.sub.sum and F.sub.2.sub._.sub.sum respectively:
8. The CD estimation device according to claim 7, wherein the processor is configured to obtain a CD estimation coefficient .sub.1 according to the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states, and estimate the CD value CD according to the CD estimation coefficient .sub.1:
CD=.sub.1delta_CD, where delta_CD=1000CN_fft/(2f.sup.2lambda.sup.2), C is a light velocity in an optical fibre, N_fft is a discrete Fourier transform length, f is a symbol rate, and lambda is a wavelength.
9. A non-transitory computer storage readable medium in which a computer program is stored, wherein when the computer program is executed, a processor is caused to: receive data of two polarization states orthogonal to each other from an In-phase/Quadrature (IQ) balance; convert the data of the two polarization states orthogonal to each other from time-domain data to frequency-domain data by adopting a discrete Fourier transform, with N=2.sup.t and t being a natural number greater than 2, and the frequency-domain data converted from the data of the two polarization states being set as X(k) and Y(k) respectively, k=0, 1, . . . , N1, then
10. The non-transitory computer storage readable medium according to claim 9, wherein performing, by the processor, the linear combination operation on the extracted data from the frequency-domain data comprises: step a: obtaining two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U)as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in three different directions according to X.sup.U[k], X.sup.L[k], Y.sup.U[k] and Y.sup.L[k]:
R.sub.n[k]=X.sub.n.sup.(U)[k].Math.conj{X.sub.n.sup.(L)[k]}, where conj() is a conjugate operation, k=0, . . . N1 and n=1, 2, 3; step c: setting a first interval value as .sub.1=2 and a second interval value as .sub.2=32, and calculating accumulated values F.sub.1 and F.sub.2 corresponding to these two interval values in different directions according to R.sub.1[k], R.sub.2[k] and R.sub.3[k]:
11. The non-transitory computer storage readable medium according to claim 10, wherein obtaining, by the processor, the argument of the CD value of the data of the two polarization states according to the result of the linear combination operation comprises: calculating arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states according to F.sub.1.sub._.sub.sum and F.sub.2.sub._.sub.sum respectively:
12. The non-transitory computer storage readable medium according to claim 11, wherein estimating, by the processor, the CD value according to the argument of the CD value of the data of the two polarization states comprises: obtaining a CD estimation coefficient .sub.1 according to the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states, and estimating the CD value CD according to the CD estimation coefficient .sub.1:
CD=.sub.1delta_CD, where delta_CD=1000CN_fft/(2f.sup.2lambda.sup.2), C is a light velocity in an optical fibre, N_fft is a discrete Fourier transform length, f is a symbol rate, and lambda is a wavelength.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1)
(2)
(3)
DETAILED DESCRIPTION
(4) In the embodiments of the disclosure, data of two polarization states orthogonal to each other is converted from time-domain data to frequency-domain data, extraction is performed on the frequency-domain data and a linear combination operation is performed on the extracted frequency-domain data, an argument of a CD value of the data of the two polarization states is obtained according to a result of the linear combination operation, and the CD value is estimated according to the argument of the CD value of the data of the two polarization states.
(5) The disclosure will be further described in detail below with reference to the drawings and specific embodiments.
(6) The embodiments of the disclosure implement a CD detection method for an optical transmission network. As shown in
(7) In Step 101: data of two polarization states orthogonal to each other is converted from time-domain data to frequency-domain data.
(8) In the step, a special algorithm of discrete Fourier transform, i.e. Fast Fourier Transform (FFT), is adopted for implementation, with N=2.sup.t and t being a natural number, and the frequency-domain data converted from the data of the two polarization states being set as X(k) and Y(k), k=0, 1, . . . , N1, then
(9)
(10) where
(11)
z(n) represents a sampled time-domain signal sequence, z(n)=x(n)+i.Math.y(n), and consists of the data x(n) and y(n) of the polarization states in two orthogonal dimensions, and Z(k) is a frequency-domain signal corresponding to the sequence z(n).
(12) In Step 102: extraction is performed on the frequency-domain data.
(13) In the step, the data is extracted from the frequency-domain data according to the following rules:
(14)
(15) where X.sup.U[k] represents upper sideband data extracted from X(k), X.sup.L[k] represents lower sideband data extracted from X(k), Y.sup.U[k] represents upper sideband data extracted from Y(k), Y.sup.L[k] represents lower sideband data extracted from Y(k),
(16)
and M may be also designated according to the specific precision requirement, where k=0, 1, . . . , M1.
(17) In Step 103: a linear combination operation is performed on the extracted frequency-domain data.
(18) Here, the following steps are included.
(19) In Step 103a: two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U) as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in three different directions are obtained according to X.sup.U[k], X.sup.L[k], Y.sup.U[k] and Y.sup.L[k]:
(20)
(21) where k=0, 1, . . . , N1.
(22) In Step 103b: conjugate multiplication is performed on the two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U) as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in the three different directions to obtain a CD sub-sequence R.sub.1[k], R.sub.2[k] and R.sub.3[k] in the three different directions:
R.sub.n[k]=X.sub.n.sup.(U)[k].Math.conj{X.sub.n.sup.(L)[k]},
(23) where conj() is a conjugate operation, k=0, . . . N1 and n=1, 2, 3.
(24) In Step 103c: a first interval value is set as .sub.1=2 and a second interval value is set as .sub.2=32, and accumulated values F.sub.1 and F.sub.2 corresponding to these two interval values in different directions are calculated according to R.sub.1[k], R.sub.2[k] and R.sub.3[k]:
(25)
(26) In Step 103d: low-pass filtering is performed on a number T of accumulated values F.sub.1 and a number M of accumulated values F.sub.2 thus obtained to get
(27)
(28) where k1=0, 1, . . . , T1, and k2=0, 1, . . . , M1.
(29) In Step 103e: two registers Buffer1 and Buffer2 with a length L are constructed, Buffer1 stores
(30)
(31) here, a value of L may be configured, and may be selected from [16, 32, 64, 128], and a default value of L is 16.
(32) In Step 104: the argument of the CD value of the data of the two polarization states is obtained according to the result of the linear combination operation;
(33) particularly, the arguments .sub.1 and .sub.2 of the CD values of the data of the two polarization states are calculated respectively according to F.sub.1.sub._.sub.sum and F.sub.2.sub._.sub.sum:
(34)
(35) where both .sub.1 and .sub.2 belong to an interval [0,1).
(36) In Step 105: the CD value is estimated according to the argument of the CD value of the data of the two polarization states,
(37) particularly, a CD estimation coefficient .sub.1 is obtained according to the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states, and a specific process is as follows:
(38) m=floor(.sub.116), and
(39) u=.sub.116m,
(40) where floor() represents rounding down;
(41) .sub.2u=.sub.2u, and
(42) when .sub.2u0.5, u=.sub.21;
(43) when .sub.2u<0.5, u=.sub.2+1; and
(44) when 0.5.sub.2u<0.5, u=.sub.2;
(45) .sub.1=m+u,
(46) .sub.1=.sub.1/32, and
(47) if .sub.10.25, a value obtained by .sub.10.5 is reassigned to .sub.1; and
(48) the CD value CD is estimated according to the CD estimation coefficient .sub.1:
(49) CD=.sub.1delta_CD,
(50) where delta_CD=1000CN_fft/(2f.sup.2lambda.sup.2), C is a light velocity in an optical fibre, N_fft is an FFT transformation length, f is a symbol rate, lambda is a wavelength, and for specific values, refer to Table 1.
(51) TABLE-US-00001 TABLE 1 Name Range Description C About 3 10.sup.8 m/s Light velocity in optical fibre N_fft N FFT transformation length f 32 GHz, 28 GHz and the like Symbol rate lambda 1,529~1,561 nm (C waveband) Wavelength 1,529~1,568 nm (CE waveband) 1,570~1,605 nm (L waveband)
(52) In order to implement the abovementioned method, the disclosure further provides a CD detection device for an optical transmission network. As shown in
(53) the data conversion module 21 is configured to convert data of two polarization states orthogonal to each other from time-domain data to frequency-domain data;
(54) the data extraction module 22 is configured to perform extraction on the frequency-domain data, and send the extracted frequency-domain data to the linear combination operation module 23;
(55) the linear combination operation module 23 is configured to perform a linear combination operation on the extracted frequency-domain data, and send a result of the linear combination operation to the argument acquisition module 24;
(56) the argument acquisition module 24 is configured to obtain an argument of a CD value of the data of the two polarization states according to the result of the linear combination operation, and send the argument of the CD value to the CD estimation module 25; and
(57) the CD estimation module 25 is configured to estimate the CD value according to the argument of the CD value of the data of the two polarization states.
(58) The data conversion module 21 is specifically configured to convert the data of the two polarization states into the frequency-domain data by adopting a discrete Fourier transform, with N=2.sup.t and t being a natural number, and the frequency-domain data converted from the data of the two polarization states being set as X(k) and Y(k) respectively, k=0, 1, . . . , N1, then:
(59)
(60) where
(61)
z(n) represents a sampled time-domain signal sequence, z(n)=x(n)+i.Math.y(n), and consists of the data x(n) and y(n) of the polarization states in two dimensions orthogonal to each other, and Z(k) is a frequency-domain signal corresponding to the sequence z(n).
(62) The data extraction module 22 is specifically configured to extract data from the frequency-domain data according to the following rules:
(63)
(64) where X.sup.U[k] represents upper sideband data extracted from X(k), X.sup.L[k] represents lower sideband data extracted from X(k), Y.sup.U[k] represents upper sideband data extracted from Y(k), Y.sup.L[k] represents lower sideband data extracted from Y(k),
(65)
and M may be also designated according to the specific precision requirement, where k=0, 1, . . . , M1.
(66) The linear combination operation module 23 is specifically configured to:
(67) 1): obtain two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U) as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in three different directions according to X.sup.U[k], X.sup.L[k], Y.sup.U[k] and Y.sup.L[k], estimation of the sequences in the three different directions can avoid influence of polarization mode dispersion on CD estimation:
(68)
(69) where k=0, 1, . . . , N1;
(70) 2): perform conjugate multiplication on the two groups of sequences X.sub.1.sup.(U), X.sub.2.sup.(U) and X.sub.3.sup.(U) as well as X.sub.1.sup.(L), X.sub.2.sup.(L) and X.sub.3.sup.(L) in the three different directions to obtain a CD sub-sequence R.sub.1[k], R.sub.2[k] and R.sub.3[k] in the three different directions:
R.sub.n[k]=X.sub.n.sup.(U)[k].Math.conj{X.sub.n.sup.(L)[k]},
(71) where conj() is a conjugate operation, k=0, . . . N1 and n=1, 2, 3;
(72) 3): set a first interval value as .sub.1=2 and a second interval value as .sub.2=32, and calculate accumulated values F.sub.1 and F.sub.2 corresponding to these two interval values in different directions according to R.sub.1[k], R.sub.2[k] and R.sub.3[k]:
(73)
(74) 4): perform low-pass filtering on a number T of accumulated values F.sub.1 and a number M of accumulated values F.sub.2 thus obtained to get
(75)
(76) where k1=0, 1, . . . , T1, and k2=0, 1, . . . , M1; and
(77) 5): construct two registers Buffer1 and Buffer2 with a length L, Buffer1 stores
(78) The argument acquisition module 24 is specifically configured to calculate the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states according to F.sub.1.sub._.sub.sum and F.sub.2.sub._.sub.sum respectively:
(79)
(80) where both .sub.1 and .sub.2 belong to an interval [0,1).
(81) The CD estimation module 25 is specifically configured to obtain a CD estimation coefficient .sub.1 according to the arguments .sub.1 and .sub.2 of the CD value of the data of the two polarization states, and estimate the CD value CD according to the CD estimation coefficient .sub.1:
CD=.sub.1delta_CD,
(82) where delta_CD=1000CN_fft/(2f.sup.2lambda.sup.2), C is a light velocity in an optical fibre, N_fft is an FFT transformation length, f is a symbol rate, and lambda is a wavelength.
(83) A position of the CD detection device for the optical transmission network in the optical transmission network is shown in
(84) If being implemented in form of a software function module and sold or used as an independent product, the CD detection method for the optical transmission network according to the embodiments of the disclosure may also be stored in a computer-readable storage medium. Based on such an understanding, the technical solutions of the embodiments of the disclosure naturally or parts contributing to a conventional art may be embodied in form of a software product, and the computer software product is stored in a storage medium, including a plurality of instructions to enable a piece of computer equipment (which may be a personal computer, a server, network equipment or the like) to execute all or part of the method of each embodiment of the disclosure. The storage medium includes various media capable of storing program codes such as a U disk, a mobile hard disk, a Read-Only Memory (ROM), a magnetic disk or an optical disk. Therefore, the embodiments of the disclosure are not limited to any specific hardware and software combination.
(85) Correspondingly, the embodiments of the disclosure further provide a computer storage medium in which a computer program is stored for execution of the CD detection method for the optical transmission network according to the embodiments of the disclosure.
(86) What are described above are only the particular embodiments of the disclosure and not intended to limit the scope of protection of the disclosure. Any modifications, equivalent replacements, improvements and the like made within the spirit and principle of the disclosure shall fall within the scope of protection of the disclosure.
INDUSTRIAL APPLICABILITY
(87) From each embodiment of the disclosure, the data of the two polarization states orthogonal to each other is converted into the frequency-domain data and a linear combination operation is performed, the argument of the CD value of the data of the two polarization states are obtained, and the CD value is estimated according to the argument of the CD value. Therefore, electric domain estimation may be performed on CD of the optical transmission network to implement CD detection of the optical transmission network.