Wavelength flexibility through variable-period poling of optical fiber

1. A fiber laser system comprising:

a high power pump laser;

an optical fiber that is aligned to receive output from the high power pump laser;

a first pair of orthogonally opposed, periodic electrode structures aligned on opposite first and second sides of the optical fiber; and

a controller communicatively coupled to the first pair of periodic electrode structures and that performs dynamically adjustable period poling of the first pair of periodic electrode structures to achieve quasi-phase matching (QPM) with wavelength agility.

2. The fiber laser system of claim 1 , further comprising:

a seed laser that emits one of a seed laser beam at one of a signal wavelength and an idler wavelength; and

an optical combiner that combines the output from the high power pump laser and the seed laser, wherein the fiber laser system is configured as an optical parametric amplifier (OPA).

3. The fiber laser system of claim 1 , further comprising two opposing mirrors positioned on opposite axial sides of the optical fiber to form an optical cavity, wherein the fiber laser system is configured as an optical parametric oscillator (OPO).

4. The fiber laser system of claim 1 , wherein the optical fiber comprise a nonlinear optical crystal that generates an output containing a signal and an idler, wherein the fiber laser system is configured as an optical parametric generator (OPG).

5. The fiber laser system of claim 1 , wherein the controller activates: (i) a periodic first subset of the electrodes of one of the first pair of orthogonally opposed, periodic electrode structures; and (i) a corresponding periodic second subset of the electrodes of another of the first pair of orthogonally opposed, periodic electrode structures to dynamically adjust the period poling.

6. The fiber laser system of claim 1 , further comprising a second pair of orthogonally opposed, periodic electrode structures longitudinally aligned and unaligned to the first pair, the second pair having a different periodic length than the first pair, wherein the controller is communicatively coupled to the second pair to achieve QPM at two different signal wavelengths.

7. The fiber laser system of claim 1 , wherein the optical fiber comprises a fused silica solid core fiber.

8. The fiber laser system of claim 1 , wherein the optical fiber comprises a hollow-core photonic crystal fiber (HCPCF) that is filled with a fluid.

9. The fiber laser system of claim 8 , wherein the fluid comprises a gas.

10. The fiber laser system of claim 9 , further comprising an optical attenuator that attenuates at a Raman wavelength to attenuate Raman scattering parasitic process.

11. The fiber laser system of claim 9 , wherein the gas comprises a noble gas.

12. The fiber laser system of claim 11 , wherein the noble gas is xenon (Xe).

13. The fiber laser system of claim 8 , wherein the fluid comprises a liquid.

14. The fiber laser system of claim 8 , wherein the first and second pairs are rotated around the optical fiber at different azimuth angles at and have different electrode periods which phase match different wavelengths.

15. The fiber laser system of claim 1 , wherein the controller performs dynamically adjustable period poling of the first pair of periodic electrode structures to achieve QPM with wavelength agility:

in response to a first mode selection, activates the first pair of periodic electrode structures to achieve a first wavelength of output that is one of signal and idler wavelength; and

in response to a second mode selection, deactivates the first pair of periodic electrode structures to achieve a pump wavelength of output.