Dispersion management system for soliton optical transmission system
A dispersion management system for soliton or soliton-like transmission systems comprises a length of optical fiber (L) in which a plurality of sections (I) made up of components (N,A) of opposite sign dispersions are concatenated together. The duration of the dispersion compensation phase is short in comparison with the propagation interval in the remainder of the system and that the path average dispersion is anomalous.
1. An optical communication system for transmitting a soliton or substantially soliton pulse, comprising
a plurality of dispersion elements, each dispersion element from the plurality of dispersion elements including at least a fiber length and a discrete dispersion compensator, the fiber length and discrete compensator having different dispersions, wherein the path average dispersion of the plurality of dispersion elements is anomalous.
2. The optical communication system of claim 1 , wherein the discrete dispersion compensator is fabricated from a highly dispersive material.
3. The optical communication system of claim 1 , wherein at least one of the discrete dispersion compensators is fabricated from a highly dispersive material.
4. The optical communication system of claim 1 , wherein the soliton or substantially soliton pulse has a time-bandwidth product greater than the time-bandwidth product of a Gaussian-shaped pulse.
5. The optical communication system of claim 1 , wherein the soliton or substantially soliton pulse has a time-bandwidth product greater than the time-bandwidth product of a Gaussian-shaped pulse.
6. An optical communication system comprising
a plurality of sections, each section including at least two dispersion elements that have dispersions of opposite sign, wherein the plurality of sections permits propagation of a stable or quasi-stable optical pulse, and wherein the optical pulse has a time-bandwidth product greater than a time-bandwidth product of an optical pulse that is Gaussian in shape.
7. The optical communication system of claim 6 , wherein the optical pulse alternately expands and compresses as it propagates through the sections.
8. The optical communication system of claim 6 , wherein the path average dispersion of the plurality of sections is zero or anomalous.
9. The optical communication system of claim 6 , wherein the difference between the dispersion magnitudes of the two dispersion elements is less than 12 ps 2 /Km.
10. The optical communication system of claim 9 , wherein the difference between the dispersion magnitudes of the two dispersion elements is less than 4 ps 2 /Km.
11. The optical communication system of claim 10 , wherein the difference between the dispersion magnitudes of the two dispersion elements is less than 0.1 ps 2 /Km.
12. The optical communication system of claim 6 , wherein the two dispersion elements of a section comprise an optical fiber length and a discrete dispersion compensator.
13. A method of optical communication comprising:
generating a plurality of optical pulses; and
launching the plurality of optical pulses through an optical communication system comprising a plurality of dispersion elements, each dispersion element from the plurality of dispersion elements including at least a fiber length and a discrete dispersion compensator, the fiber length and the discrete dispersion compensator having different dispersions, wherein the path average dispersion of the plurality of dispersion elements is zero or anomalous, such that the optical pulses are transmitted as soliton or substantially soliton pulses.
14. A method of optical communication comprising:
generating a plurality of optical pulses; and
launching the plurality of optical pulses through an optical communication system comprising a plurality of sections, each section including at least two dispersion elements that have dispersions of opposite sign, wherein the plurality of sections permits propagation of corresponding stable or quasi-stable optical pulses, and wherein the stable or quasi-stable optical pulses have a time-bandwidth product greater than a time-bandwidth product of optical pulses that are Gaussian in shape.