High performance hollow-core optical-fiber filter for optical rotation sensing

1. A hollow-core optical-fiber filter comprising:

an optically-inactive-hollow-core optical fiber having a first end-face and an opposing second end-face, the first end-face and the second end-face setting a fiber length;

a first reflective end-cap positioned at the first end-face; and

a second reflective end-cap positioned at the second end-face, wherein at least one of the first reflective end-cap and the second reflective end-cap is a beveled end-cap, and wherein, when an optical beam from a laser is coupled into one of the first end-face or the second end-face, an optical output from the opposing end-face has a narrow linewidth and low frequency noise fluctuations.

2. The filter of claim 1 , wherein the first reflective end-cap includes a first reflective surface and wherein the second reflective end-cap includes a second reflective surface, wherein, when an optical beam from the laser is coupled into one of the first end-face or the second end-face, a resonant cavity is established between the first reflective surface and second reflective surface.

3. The filter of claim 1 , wherein the first reflective end-cap includes:

a first reflective surface having a first reflectivity;

a first anti-reflective surface opposing the first reflective surface, and wherein the second reflective end-cap includes:

a second reflective surface having a second reflectivity;

a second anti-reflective surface opposing the second reflective surface wherein, when an optical beam from the laser is coupled into one of the first end-face or the second end-face, a resonant cavity is established between the first reflective surface and second reflective surface.

4. The filter of claim 1 , wherein the first reflective end-cap is a first beveled end-cap, including:

a first surface having a first reflectivity; and

a second surface, wherein the first surface and the second surface of the first beveled end-cap are in planes that intersect at a first acute angle, and wherein the second reflective end-cap is a second beveled end-cap including:

a first surface having a second reflectivity; and

a second surface, wherein the first surface and the second surface of the second beveled end-cap are in planes that intersect at a second acute angle, when an optical beam from the laser is coupled into one of the first end-face or the second end-face, a resonant cavity is established between the first surface of the of the first beveled end-cap and the first surface of the second beveled end-cap.

5. The filter of claim 4 , wherein the second surface of the first beveled end-cap is coated with an anti-reflection coating, and wherein the second surface of the second beveled end-cap is coated with an anti-reflection coating.

6. The filter of claim 1 , wherein the fiber length, a first reflectivity of the first reflective end-cap, a second reflectivity of the second reflective end-cap, a mode field size of the hollow-core optical fiber, and a numerical aperture of the hollow-core optical fiber are selected to prevent generation of non-linear effects in the hollow-core optical fiber.

7. A method of generating at least one low-noise, coherent optical beam for use in a resonator-fiber-optic gyroscope system, the method comprising:

phase locking at least one slave laser to a master laser;

coupling an optical beam emitted from the at least one slave laser to a first end-face of a respective at least one hollow-core optical-fiber filter, the at least one hollow-core optical-fiber filter including;

an optically-inactive-hollow-core optical fiber having a first end-face and an opposing second end-face, the first end-face and the second end-face setting a fiber length;

a first reflective end-cap positioned at the first end-face; and

a second reflective end-cap positioned at the second end-face, wherein at least one of the first reflective end-cap and the second reflective end-cap is a beveled end-cap,

wherein a respective at least one low-noise, coherent optical beam is output from the second end-face of the at least one hollow-core optical-fiber filter; and

coupling the at least one low-noise, coherent optical beam output from the second end-face of the at least one hollow-core optical-fiber filter to at least one of two coil end-faces of a fiber resonator coil.

8. The method of claim 7 , wherein the at least one slave laser includes at a first slave laser and a second slave laser, wherein the at least one hollow-core optical-fiber filter further includes:

a first hollow-core optical-fiber filter wherein the first end-face is in contact a reflective coating on the first reflective end-cap and the second end-face is in contact with a reflective coating on the second reflective end-cap; and

a second hollow-core optical-fiber filter wherein the first end-face is in contact a reflective coating on a third reflective end-cap and the second end-face is in contact with a reflective coating on a fourth reflective end-cap, the method further comprising:

coupling the optical beam output from the first slave laser to the first end-face of the first hollow-core optical-fiber filter, wherein a first low-noise, coherent optical beam is output from the second end-face of the first hollow-core optical-fiber filter; and

coupling the optical beam output from the second slave laser to the first end-face of the second hollow-core optical-fiber filter, wherein a second low-noise, coherent optical beam is output from the second end-face of the second hollow-core optical-fiber filter.

9. The method of claim 8 , further comprising:

coupling the first low-noise, coherent optical beam to a first coil end-face of a fiber resonator coil; and

coupling the second low-noise, coherent optical beam to a second coil end-face of the fiber resonator coil.

10. The method of claim 9 , further comprising:

positioning the first coil end-face in a first groove in a silicon optical bench; and

positioning the second coil end-face in a second groove in the silicon optical bench.

11. The method of claim 10 , further comprising:

positioning the second end-face and the second reflective end-cap of the first hollow-core optical-fiber filter in a first etched region in the silicon optical bench; and

positioning the second end-face and the fourth reflective end-cap of the second hollow-core optical-fiber filter in a second etched region in the silicon optical bench.

12. The method of claim 9 , wherein coupling the first low-noise, coherent optical beam to the first coil end-face of a fiber resonator coil comprises:

coupling the first low-noise, coherent optical beam to the first coil end-face positioned in a first groove in a silicon optical bench via at least one ball lens positioned in a first etched region of the silicon optical bench; and

wherein coupling the second low-noise, coherent optical beam to a second coil end-face of the fiber resonator coil comprises:

coupling the second low-noise, coherent optical beam to the second coil end-face positioned in a second groove in the silicon optical bench via at least one ball lens positioned in a second etched region of the silicon optical bench.

13. The method of claim 12 , wherein the at least one ball lens positioned in the first etched region of the silicon optical bench includes a first ball lens and a second ball lens and wherein the at least one ball lens positioned in the second etched region of the silicon optical bench includes a third ball lens and a fourth ball lens, the method further comprising:

positioning the first ball lens and the second ball lens to collimate the low-noise, coherent optical beam propagating there between; and

positioning the third ball lens and the fourth ball lens to collimate the low-noise, coherent optical beam propagating there between.

14. The method of claim 8 , wherein the at least one slave laser further includes a third slave laser further, wherein the at least one hollow-core optical fiber-filter further includes a third hollow-core optical-fiber filter, and wherein the first end-face of the third hollow-core optical-fiber filter is in contact a reflective coating on a fifth reflective end-cap and the second end-face of the third hollow-core optical-fiber filter is in contact with a reflective coating on a sixth reflective end-cap, the method further comprising:

coupling the optical beam output from the third slave laser to the first end-face of the third hollow-core optical-fiber filter, wherein a third low-noise, coherent optical beam is output from the second end-face of the third hollow-core optical-fiber filter; and

coupling the third low-noise, coherent optical beam to a first coil end-face of the fiber resonator coil.

15. A resonator-fiber-optic gyroscope comprising:

a frequency stabilized master laser emitting a reference optical beam having low phase noise;

at least two slave lasers arranged so that the reference optical beam controls the respective at least two slave lasers;

at least two hollow-core optical-fiber filters arranged so that optical beams emitted from the at least two slave lasers are coupled to the respective hollow-core optical-fiber filters, wherein low-noise, coherent optical beams are output from the respective hollow-core optical-fiber filters; and

a fiber resonator coil having a first coil end-face and a second coil end-face,

wherein an optical beam output from one of the at least two hollow-core optical-fiber filters is coupled to the first coil end-face of the fiber resonator coil, and

wherein an optical beam output from another one of the at least two hollow-core optical-fiber filters is coupled to the second coil end-face of the fiber resonator coil.

16. The resonator-fiber-optic gyroscope of claim 15 , wherein the at least two hollow-core optical-fiber filters each comprise a hollow-core optical fiber having a first end-face and an opposing second end-face, the first end-face and the second end-face setting a fiber length, the first end-face in contact a first reflective coating on a first reflective end-cap and the second end-face in contact a second reflective coating on a second reflective end-cap, wherein the fiber length, the first reflective coating on the first reflective end-cap, the second reflective coating on the second reflective end-cap, a mode field size of the hollow-core optical fiber, and a numerical aperture of the hollow-core optical fiber are selected to prevent generation of non-linear effects in the hollow-core optical fibers of the at least two hollow-core optical-fiber filters.

17. The resonator-fiber-optic gyroscope of claim 15 , wherein the optical beam emitted from a first slave laser is coupled to a first end-face of a first hollow-core optical-fiber filter, wherein a first low-noise, coherent optical beam output from a second end-face of the first hollow-core optical-fiber filter is coupled to the first coil end-face of the fiber resonator coil, and

wherein the optical beam emitted from a second slave laser is coupled to a first end-face of a second hollow-core optical-fiber filter, wherein a second low-noise, coherent optical beam output from a second end-face of the second hollow-core optical-fiber filter is coupled to the second coil end-face of the fiber resonator coil.

18. The resonator-fiber-optic gyroscope of claim 17 , wherein the optical beam emitted from a third slave laser is coupled to a first end-face of a third hollow-core optical-fiber filter, wherein a third low-noise, coherent optical beam output from a second end-face of the third hollow-core optical-fiber filter is coupled to the first coil end-face of the fiber resonator coil.

19. The resonator-fiber-optic gyroscope of claim 15 , further comprising:

a silicon optical bench including grooves to position optical elements configured to align and direct the low-noise, coherent optical beams output from the at least two hollow-core optical-fiber filters to the first coil end-face and the second coil end-face.

20. The resonator-fiber-optic gyroscope of claim 19 , wherein the optical elements include at least one optically transparent ball lens positioned in a respective at least one etched region in the silicon optical bench.