In-channel residual chromatic dispersion measurement
View Patent ↗A system generates optical pulses, that include two frequencies within one optical channel, at a first end of an optical link, and receives the optical pulses at a second end of the optical link. The system also sets a frequency difference for the two frequencies of the optical pulses, calculates a relative group delay difference for the two frequencies of the optical pulses, and calculates a residual chromatic dispersion of the channel based on the frequency difference and the calculated relative group delay difference.
1. A method, comprising:
generating, by a transmitter device, optical pulses, that include two frequencies within an optical channel,
where the generating includes:
separating, by an interferometer, light into two optical pulses that each correspond to a different one of the two frequencies;
tuning, by a tunable filter, the optical pulses to the optical channel;
splitting, by a beam splitter, the optical pulses into two portions,
outputting, by the beam splitter, at least a portion of the optical pulses to the optical channel;
receiving the optical pulses from the optical channel;
separating the two frequencies of the optical pulses within the optical channel;
measuring arrival times of the optical pulses;
calculating a relative group delay difference for the two frequencies of the optical pulses, based on the arrival times; and
calculating a residual chromatic dispersion of the channel based on the frequency difference and the calculated relative group delay difference.
2. The method of claim 1 , further comprising:
providing for display of the residual chromatic dispersion.
3. The method of claim 1 , where calculating the residual chromatic dispersion comprises:
calculating the residual chromatic dispersion by dividing the calculated relative group delay difference by the frequency difference.
4. A system, comprising:
a receiver device configured to:
receive optical pulses, that include two frequencies and a frequency difference, from a channel of an optical network,
separate the two frequencies of the optical pulses within the channel,
measure arrival times of the optical pulses,
calculate a relative group delay difference for the two frequencies of the optical pulses, based on the arrival times, and
calculate a residual chromatic dispersion of the channel based on the frequency difference and the calculated relative group delay difference; and
a transmitter device configured to generate the optical pulses to the channel, where the transmitter device comprises a tunable dual-frequency light source that generates the optical pulses;
where the tunable dual-frequency light source comprises:
an interferometer that receives light and separates the light into the two frequencies of the optical pulses;
a tunable filter that receives the optical pulses from the interferometer and tunes the optical pulses to the channel; and
a beam splitter that splits the optical pulses into two portions, and outputs at least a portion of the optical pulses to the channel.
5. The system of claim 4 , where the transmitter device comprises:
a driver that outputs one or more operating frequencies and one or more power levels; and
an optical modulator that interacts with the driver and the tunable dual-frequency light source to generate the optical pulses that includes two frequencies.
6. The system of claim 4 , where the tunable dual-frequency light source comprises one of:
a gas laser;
a chemical laser;
a dye laser;
a metal-vapor laser;
a solid-state laser; or
a semiconductor laser.
7. The system of claim 4 , further comprising:
a user interface that provides for display of the residual chromatic dispersion of the channel.
8. The system of claim 4 , where the processing logic is further configured to:
calculate the residual chromatic dispersion of the channel by dividing the calculated relative group delay difference by the frequency difference.
9. The system of claim 4 , where the optical network comprises a Dense Wavelength Division Multiplexing (DWDM)-based network.
10. A device comprising:
means for generating optical pulses, that include two frequencies within an optical channel,
where the means for generating include:
means for separating light into the two optical pulses that each correspond to a different one of the two frequencies,
means for tuning the optical pulses to the optical channel, and
means for splitting the optical pulses into two portions and outputting at least a portion of the optical pulses to the optical channel;
means for receiving the optical pulses from the optical channel;
means for separating the two frequencies of the optical pulses within the optical channel;
means for measuring arrival times of the optical pulses;
means for calculating a relative group delay difference for the two frequencies of the optical pulses, based on the arrival times; and
means for calculating a residual chromatic dispersion of the channel based on the frequency difference and the calculated relative group delay difference.
11. The device of claim 10 , where the means for generating further include:
means for reflecting light generated by a tunable dual-frequency light source, and
means for providing an optical gain to the light reflected by the means for reflecting.
12. The device of claim 10 , further comprising:
means for adjusting the means for separating and the means for tuning based on another portion of the optical pulses.
13. The device of claim 10 , further comprising:
means for displaying a representation of the residual chromatic dispersion.
14. The system of claim 4 , where the tunable dual-frequency light source further comprises:
an absorber that receives the optical pulses from the tunable filter and maintains oscillation of the optical pulses.
15. The system of claim 4 , where the tunable dual-frequency light source further comprises:
a mirror that reflects light generated by the tunable dual-frequency light source, and
a gain medium that receives the light reflected by the mirror and provides an optical gain to the light reflected by the mirror,
where the light received by the interferometer is the light to which the the gain medium provides the optical gain.
16. The system of claim 15 , where the tunable dual-frequency light source further comprises:
a wavelength locker that receives another portion of the optical pulses from the beam splitter and adjusts the interferometer and the tunable filter based on the other portion of the optical pulses.
17. The method of claim 1 , where the generating further includes:
reflecting, by a mirror, light generated by a tunable dual-frequency light source, and
providing, by a gain medium, an optical gain to the light reflected by the mirror.
18. The method of claim 1 , further comprising:
adjusting, by a wavelength locker, the interferometer and the tunable filter based on another portion of the optical pulses.