All solid hybrid arrow fiber
An all solid hybrid waveguiding structure provides large mode area, acceptable losses of the desired core mode and very high losses of the undesired next higher order mode in the core. Embodiments of the waveguide include a hybrid of low index barriers providing confinement by total internal reflection, and further include high index rings that support guided modes only at effective indices different from that of the desired core mode.
1. An apparatus, comprising:
a length of background material of undoped optical material having an index of refraction (n bg );
a core comprising a length of a solid core material within said length of background material, wherein said core material comprises a rare-earth dopant and has an index of refraction (n core ); and
a length of a first set of solid optical material elements located within said length of background material and distributed around said core, wherein each solid optical material element of said first set of solid optical material elements comprises an outer solid ring region having an index of refraction (n ring )that is greater than n bg ,
wherein each solid optical material element of said first set of solid optical material elements comprises an outer wall, wherein light is partially confined to said core by glancing reflection from at least one said wall of said solid optical material elements.
2. The apparatus of claim 1 , wherein said undoped optical material comprises undoped glass.
3. The apparatus of claim 1 , wherein each solid optical material element of said first set of solid optical material elements comprises a solid glass element.
4. The apparatus of claim 1 , wherein said first set of solid optical material elements are distributed around said core and curve away from said core.
5. The apparatus of claim 1 , wherein said glancing reflection is enhanced for certain wavelengths by multiple reflections within said outer ring region of at least one solid optical material element of said first set of solid optical material elements.
6. The apparatus of claim 1 , wherein to obtain minimum losses in said solid core material at an operating wavelength A, said each outer solid ring region is set such that
2 tNA =( m+ ½)λ,
wherein
NA =√{square root over ( n ring 2 −n bg 2 )}
wherein t is the wall thickness of said each outer solid ring region, wherein said ring comprises a material specified by its numerical aperture NA which is a function of its index of refraction n ring and that of the background n bg and wherein m is an integer.
7. The apparatus of claim 1 , further comprising a length of a second set of optical material elements located within said background material and distributed around said core, wherein said second set of optical material elements comprises an index of refraction (n barrier ) below that of n bg .
8. The apparatus of claim 1 , wherein at least one solid optical material element of said first set of solid optical material elements has a diameter that tunes a mode of said outer solid ring region such that an unwanted higher order mode (HOM) in said core is coupled to a mode supported within the interior of at least one solid optical material element of said first set of solid optical material elements.
9. An apparatus, comprising:
a length of background material of undoped optical material having an index of refraction (n bg );
a core comprising a length of a solid core material within said length of background material, wherein said core material comprises a rare-earth dopant and has an index of refraction (n core ); and
a length of a first set of solid optical material elements located within said length of background material and distributed around said core, wherein each solid optical material element of said first set of solid optical material elements comprises an outer solid ring region having an index of refraction (n ring ) that is greater than n bg ,
wherein each said outer solid ring region of said first set of solid optical material elements comprises a diameter that brings at least one of its interior modes into resonance with at least one higher order mode (HOM) of said core, and thereby increases the propagation loss of said at least one HOM.
10. An apparatus, comprising:
a length of background material of undoped optical material having an index of refraction (n bg );
a core comprising a length of a solid core material within said length of background material, wherein said core material comprises a rare-earth dopant and has an index of refraction (n core ); and
a length of a first set of solid optical material elements located within said length of background material and distributed around said core, wherein each solid optical material element of said first set of solid optical material elements comprises an outer solid ring region having an index of refraction (n ring ) that is greater than n bg ,
wherein said core is co-doped with material to reduce its index to that of said undoped optical material.
11. The apparatus of claim 10 , wherein said core is co-doped with Fluorine to reduce the index of said core to that of said undoped optical material.
12. An apparatus, comprising:
a length of background material of undoped optical material having an index of refraction (n bg );
a core comprising a length of a solid core material within said length of background material, wherein said core material comprises a rare-earth dopant and has an index of refraction (n core );
a length of a first set of solid optical material elements located within said length of background material and distributed around said core, wherein each solid optical material element of said first set of solid optical material elements comprises an outer solid ring region having an index of refraction (n ring ) that is greater than n bg ; and
a length of a second set of optical material elements located within said background material and distributed around said core, wherein said second set of optical material elements comprises an index of refraction (n barrier ) below that of n bg .
13. The apparatus of claim 12 , wherein each optical material element of said second set of optical material elements comprises glass.
14. The apparatus of claim 12 , wherein at least one solid optical material element of said first set of solid optical material elements has a diameter that tunes a mode of said outer solid ring region such that an unwanted higher order mode (HOM) in said core is coupled to a mode supported within the interior of said at least one solid optical material element of said first set of solid optical material elements.
15. The apparatus of claim 12 , wherein each said outer solid ring region of said first set of solid optical material elements comprises a diameter that brings at least one of its interior modes into resonance with at least one higher order mode (HOM) of said core, and thereby increases the propagation loss of said at least one HOM.
16. An apparatus, comprising:
a length of background material of undoped optical material having an index of refraction (n bg );
a core comprising a length of a solid core material within said length of background material, wherein said core material comprises a rare-earth dopant and has an index of refraction (n core ); and
a length of a first set of solid optical material elements located within said length of background material and distributed around said core, wherein each solid optical material element of said first set of solid optical material elements comprises an outer solid ring region having an index of refraction (n ring ) that is greater than n bg ,
wherein at least one solid optical material element of said first set of solid optical material elements has a diameter that tunes a mode of said outer solid ring region such that an unwanted higher order mode (HOM) in said core is coupled to a mode supported within the interior of at least one solid optical material element of said first set of solid optical material elements.