Optical compensator having compensation for Kerr effect phase noise
View Patent ↗A method and apparatus for reducing nonlinear phase noise that is induced in an optical transmission system by the interaction of optical amplifier noise and Kerr effect. The apparatus includes an intensity-scaled nonlinear phase noise compensator. The phase noise compensator reduces the nonlinear phase noise by rotating a phase estimate by a scaled signal strength estimate for the optical signal or by comparing a complex estimate to curved regions having scaled nonlinear decision boundaries. The scale factor is derived from the number of spans in the transmission system. Another embodiment of the phase noise compensator uses the scaled signal strength for re-modulating an optical signal.
1. An optical phase noise compensator, comprising:
an intensity scaler for receiving an optical signal having Kerr effect nonlinear phase noise accumulated over one or more spans and providing an electrical scaled signal strength, said optical signal using optical signal phase for carrying information; and
an optical phase modulator for modulating said received optical signal with said scaled signal strength for compensating said nonlinear phase noise and issuing an output optical signal using optical signal phase for carrying said information.
2. The compensator of claim 1 , wherein:
said phase noise is induced by fiber nonlinearity in said spans.
3. The compensator of claim 1 , wherein:
said phase noise is induced by additive noise in said spans.
4. The compensator of claim 1 , wherein:
the intensity scaler includes a signal strength estimator for estimating a signal strength of said received optical signal and a multiplier for multiplying said signal strength by a scale factor for providing said scaled signal strength.
5. The compensator of claim 4 , wherein:
said scale factor is a function of a number N of said spans.
6. The compensator of claim 5 , wherein:
said scale factor is approximately one half a nonlinear coefficient of an optical fiber (γ) times an effective nonlinear length for one of said spans (L eff ) times a sum of one plus said N.
7. The compensator of claim 4 , wherein:
said scale factor is approximately
γ
L
eff
N
+
1
2
·
E
0
2
+
(
2
N
+
1
)
σ
2
/
3
E
0
2
+
N
σ
2
where said N is the number of said spans, said γ is a nonlinear coefficient of an optical fiber, said L eff is an effective nonlinear length for one of said spans, said E 0 is a calculated power expected of said received optical signal without noise, and said σ 2 is a noise variance for one of said spans.
8. The compensator of claim 4 , wherein:
said scale factor is approximately one-half the ratio of a mean nonlinear phase shift and a mean signal power of said received optical signal, said mean phase shift due to Kerr effect.
9. The compensator of claim 1 , wherein:
said optical signal phase for carrying information is modulation selected from the group consisting of binary phase shift keying (BPSK), quadrature amplitude modulation (QAM), M-ary phase shift keying (MPSK), differential phase shift keying (DPSK), differential quadrature amplitude modulation, and frequency modulation.
10. A method for phase noise compensation comprising:
receiving an optical signal having Kerr effect nonlinear phase noise accumulated over one or more spans, said optical signal using optical signal phase for carrying information;
determining an electrical scaled signal strength for said received optical signal; and
phase modulating said received optical signal with said scaled signal strength for compensating said nonlinear phase noise and issuing an output optical signal using optical signal phase for carrying said information.
11. The method of claim 10 , wherein:
said phase noise is induced by fiber nonlinearity in said spans.
12. The method of claim 10 , wherein:
said phase noise is induced by additive noise in said spans.
13. The method of claim 10 , wherein:
the step of determining a scaled signal strength includes estimating a signal strength of said received optical signal; and multiplying said signal strength by a scale factor for providing said scaled signal strength.
14. The method of claim 13 , wherein:
said scale factor is a function of a number N of said spans.
15. The method of claim 14 , wherein:
said scale factor is approximately one half a nonlinear coefficient of an optical fiber (γ) times an effective nonlinear length for one of said spans (L eff ) times a sum of one plus said N.
16. The method of claim 13 , wherein:
said scale factor is approximately
γ
L
eff
N
+
1
2
·
E
0
2
+
(
2
N
+
1
)
σ
2
/
3
E
0
2
+
N
σ
2
where said N is the number of said spans, said γ is a nonlinear coefficient of an optical fiber, said L eff is an effective nonlinear length for one of said spans, said E 0 is a calculated power expected of said received optical signal without noise, and said σ 2 is a noise variance for one of said spans.
17. The method of claim 13 , wherein:
said scale factor is approximately one-half the ratio of a mean nonlinear phase shift and a mean signal power of said received optical signal, said mean phase shift due to Kerr effect.
18. The method of claim 10 , wherein:
said optical signal phase for carrying information is modulation selected from the group consisting of binary phase shift keying (BPSK), quadrature amplitude modulation (QAM), M-ary phase shift keying (MPSK), differential phase shift keying (DPSK), differential quadrature amplitude modulation, and frequency modulation.