Photonic bandgap fiber and fiber laser device using same
AssigneesFujikura Ltd., National University Corporation Hokkaido University
InventorsMasahiro Kashiwagi, Kunimasa Saitoh
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Abstract
There is provided a photonic bandgap fiber used in a state in which at least a part of the photonic bandgap fiber is bent at radii of 15 cm or greater and 25 cm or less. A large number of high refractive index portions 57 are disposed in a nineteen-cell core type in three layers, and a V value is 1.5 or greater and 1.63 or less. In the high refractive index portions 57, conditions are defined that a relative refractive index difference is Δ% and a lattice constant is Λ μm so as to remove light in a higher mode at the bent portion as described above.
Claims5
A photonic bandgap fiber comprising:
- a core region;
- and
- a cladding region having a large number of high refractive index portions disposed in a triangular lattice shape to surround the core region, the high refractive index portions having a refractive index higher than a refractive index of the core region, the cladding region including a medium having a refractive index equal to the refractive index of the core region and provided among the high refractive index portions, the photonic bandgap fiber being used in a state in which at least a part of the photonic bandgap fiber is bent with a predetermined bending radius, wherein
- the large number of the high refractive index portions are disposed in a nineteen-cell core type in three layers,
- a V value is 1.5 or greater and 1.63 or less, and
- Expression (1) and Expression (2) below are satisfied where a relative refractive index difference of the high refractive index portions to the medium is defined as Δ%, a lattice constant is defined as Λ μm, and the predetermined bending radius is defined as R cm,
- AHOM+BHOM+CHOM2+DHOM3≦Δ≦AFM+BFM+CFM2+DFM3 (1)
- 15≦R≦25 (2)
- where
- AHOM==171.37687+2.093345R−0.1275714R2
- BHOM=−43.29906+0.530802R+0.011094R2
- CHOM=3.48397−0.098659R+0.000365R2
- DHOM=−0.09034+0.003584R−0.0000348R2
- AFM=89.98658−2.94759R+0.04246R2
- BFM=−17.33858+0.743907R−0.011185R2
- CFM=1.0904−0.054614R+0.0008568R2 and
- DFM=−0.02229+0.001232R−0.00002R2,
- wherein the V value is obtained by:
- V
- =
- π
- λ
-
- d
-
- n
- high
- 2
- -
- n
- low
- 2
- where λ is a use wavelength, d is a diameter of the respective high refractive index portions, nhigh is the refractive index of the high refractive index portions, and nlow is the refractive index of the medium provided among the high refractive index portions.
Dependencies are inferred from the claim text.