Chromatic dispersion compensator
View Patent ↗A chromatic dispersion compensator comprises a beam delay element, such as one or more Gires-Tournois etalon (GTEs); a beam director, such as a polarizing beam splitter (PBS), a prism polarizer, a dielectric polarizer or a crystal polarizer; and a polarization changer, such as one or more quarter-wave plates. The beam director directs an inbound optical beam based on its polarization toward the beam delay element whereat a first unit of group delay is induced. The optical beam traverses the beam delay element and enters a polarization changer whereat the optical beam obtains a new polarization. The optical beam traverses the polarization changer and re-enters the beam director whereupon a path change is induced on the optical beam based on its new polarization and the optical beam is redirected toward the beam delay element whereat a second unit of group delay is induced. The compensator is arranged to advantageously perform the referenced technique contemporaneously on two constituent optical beams (having different polarizations) of an inbound optical beam and eventually re-combine the two constituent optical beams into an outbound optical beam. The beam delay element may include one or more GTEs. Inducement of path changes and direction of the optical beam to the beam delay element may be assisted by one or more ninety degree mirrors. The referenced technique may be performed on an optical beam more than twice, such that a third, fourth, fifth, etc. delay is induced on the optical beam.
1. A chromatic dispersion compensator, comprising:
a polarization changer;
a beam delay element; and
a beam director,
wherein the polarization changer receives an optical beam having a unit of group delay induced thereon by the beam delay element and induces a change in polarization of the optical beam prior to transmitting the optical beam to the beam director, the change in polarization inducing a path change on the optical beam by the beam director whereupon the optical beam is redirected to the beam delay element whereat a further unit of group delay is induced on the optical beam,
wherein the beam director is a single polarizing beam splitter that is operatively coupled with a plurality of ninety degree mirrors to facilitate inducement of at least four units of group delay on the optical beam.
2. The compensator of claim 1 , wherein the optical beam is a portion of an input optical beam and wherein the compensator induces multiple units of group delay on other portions of the input optical beam and re-combines the optical beam with the other portions into an output optical beam.
3. The compensator of claim 1 , wherein the beam delay element comprises a Gires-Tournois etalon.
4. The compensator of claim 1 , wherein the beam delay element comprises a plurality of Gires-Tournois etalons.
5. The compensator of claim 1 , wherein the polarization changer comprises a quarter-wave plate.
6. The compensator of claim 1 , wherein the incidence of the optical beam into the beam delay element is substantially normal.
7. A method for chromatic dispersion compensation, comprising the steps of:
directing an optical beam to a delay element;
inducing a unit of group delay on the optical beam at the delay element;
changing a polarization of the optical beam;
inducing a path change on the optical beam based on the changed polarization;
redirecting the optical beam to the delay element; and
inducing a further unit of group delay on the optical beam at the delay element,
wherein a single polarizing beam splitter is operatively coupled with a plurality of ninety degree mirrors to facilitate inducement of at least four units of group delay on the optical beam.
8. The method of claim 7 , further comprising the step of re-combining the optical beam with other portions of an input optical beam upon which multiple units of group delay have been induced.
9. The method of claim 7 , wherein the beam delay element comprises a Gires-Tournois etalon.
10. The method of claim 7 , wherein the beam delay element comprises a plurality of Gires-Tournois etalons.
11. The method of claim 7 , wherein the changing step is performed by a quarter-wave plate.
12. The method of claim 7 , wherein the incidence of the optical beam into the beam delay element is substantially normal.