Monolithic visible wavelength fiber laser
Fiber laser having a monolithic laser resonator having laser affected zones for providing laser beams having wavelengths below 800 nm and from between 400 nm to 800 nm. Methods of using femtosecond lasers to form fiber Bragg gratings, volume Bragg gratings, space gratings, and laser beam delivery patterns for changing the index of refraction within optical fibers.
1. A laser resonator for generating a laser beam in the wavelength region of about 400 nm to about 700 nm, the laser resonator comprising:
a) an optical fiber comprising a core and a cladding and having an all fiber feed-back mechanism, the feed-back mechanism comprising a first reflective member and a second reflective member: the first reflective member and the second reflective member located along a length of the optical fiber and defining a distance there between; and,
b) wherein, the second reflective member is a fiber Bragg grating, wherein the fiber Bragg grating is capable of providing feedback to the first Raman order; and wherein the fiber Bragg grating is incapable of providing feedback to the second Raman order.
2. The laser resonator of claim 1 , wherein the fiber Bragg grating is created in the optical fiber using femtosecond pulses to operate in the wavelength region of 400-700 nm.
3. The laser resonator of claim 2 , wherein the fiber Bragg grating is inscribed at an angle with respect to the normal of the optical wave direction in the optical fiber; whereby the fiber Bragg grating is capable of redirecting the propagating mode out of the core of the fiber.
4. The laser resonator of claim 2 , wherein the fiber Bragg grating is inscribed with a curved shape with respect to the normal of the optical wave direction in the optical fiber; whereby the fiber Bragg grating is capable of redirecting only n modes back into the core of the fiber, where n can vary from 1 to <4.
5. The laser resonator of claim 2 , wherein the fiber Bragg grating is inscribed in a pure fused silica core fiber.
6. The laser resonator of claim 2 , wherein the fiber Bragg grating is inscribed in a phosphorous doped core of a fiber.
7. The laser resonator of claim 2 , wherein the fiber Bragg grating is inscribed in a doped core.
8. The laser resonator of claim 2 , wherein the core is not doped with photosensitive dopants, whereby the core is free from photosensitive dopants;
and the laser resonator is capable of producing a laser beam at wavelengths below about 500 nm.
9. The laser resonator of claim 1 , wherein the core is pure fused silica core and the fiber Bragg grating is located in the core.
10. The laser resonator of claim 1 , wherein the core is a phosphorous doped core and the fiber Bragg grating is located in the core.
11. The laser resonator of claim 1 , wherein the core is not doped with photosensitive dopants, whereby the core is free from photosensitive dopants; and the laser resonator is capable of producing a laser beam at wavelengths below about 500 nm.
12. The laser resonator of claims 11 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating.
13. The laser resonator of claim 1 , wherein the fiber Bragg grating is inscribed at normal incidence to the optical wave direction in the optical fiber;
thereby providing feedback within the core of the optical fiber.
14. The laser resonator of claim 1 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating; and wherein the fiber-coupled volume Bragg grating is created using femtosecond laser pulses.
15. The laser resonator of claim 1 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating; and wherein the fiber-coupled volume Bragg grating is created in glass.
16. The laser resonator of claim 1 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating; and wherein the fiber-coupled volume Bragg grating is inscribed at normal incidence to the optical wave direction in glass; whereby the fiber-coupled volume Bragg grating is capable of providing feedback within the core of the optical fiber.
17. The laser resonator of claims 1 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating; wherein the fiber-coupled volume Bragg grating is inscribed at an angle with respect to the normal of the optical wave direction in the optical fiber; whereby the fiber-coupled Bragg grating is capable of redirecting the propagating mode out of the core of the fiber.
18. The laser resonator of claims 1 , wherein the fiber Bragg grating is a fiber-coupled volume Bragg grating; wherein the fiber-coupled volume Bragg grating is inscribed with a curved shape with respect to the normal of the optical wave direction in the optical fiber; whereby the fiber-coupled Bragg grating is capable of redirecting only n modes back into the core of the fiber, where n can vary from 1 to <4.
19. The laser resonator of claim 1 comprises a fiber optic endcap, and wherein the Bragg grating is located in the fiber optic endcap.