2010
DOI: 10.1364/ol.35.002233
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Management of the high-order mode content in large (40 μm) core photonic bandgap Bragg fiber laser

Abstract: Very large-mode-area Yb(3+)-doped single-mode photonic bandgap (PBG) Bragg fiber oscillators are considered. The transverse hole-burning effect is numerically modeled, which helps properly design the PBG cladding and the Yb(3+)-doped region for the high-order mode content to be carefully controlled. A ratio of the Yb(3+)-doped region diameter to the overall core diameter of 40% allows for single-mode emission, even for small spool diameters of 15 cm. Such a fiber was manufactured and subsequently used as the c… Show more

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Cited by 34 publications
(13 citation statements)
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“…Hence the FOM will experience the highest gain and dominate the modal distribution at the laser output. A few recent fiber designs include the chirally-coupled core fiber (HOMs are coupled to and shed from one or more satellite waveguides that form a helix around the fiber core) [11], photonic bandgap Bragg fiber (where only the FOM propagates with low loss) [12], solid photonic bandgap fibers (where bending loss is exacerbated on HOMs relative to the FOM) [13], leakage channel fibers (wherein all modes are lossy, but the loss is minimized for the FOM) [14], and selectively-doped triple clad fibers (where the FOM has the highest overlap with the active region in the fiber) [15]. While there is clearly no shortage of methods utilized to improve the beam quality from an LMA fiber, such fibers generally are quite complex in their cross-sectional geometries.…”
Section: Resultsmentioning
confidence: 99%
“…Hence the FOM will experience the highest gain and dominate the modal distribution at the laser output. A few recent fiber designs include the chirally-coupled core fiber (HOMs are coupled to and shed from one or more satellite waveguides that form a helix around the fiber core) [11], photonic bandgap Bragg fiber (where only the FOM propagates with low loss) [12], solid photonic bandgap fibers (where bending loss is exacerbated on HOMs relative to the FOM) [13], leakage channel fibers (wherein all modes are lossy, but the loss is minimized for the FOM) [14], and selectively-doped triple clad fibers (where the FOM has the highest overlap with the active region in the fiber) [15]. While there is clearly no shortage of methods utilized to improve the beam quality from an LMA fiber, such fibers generally are quite complex in their cross-sectional geometries.…”
Section: Resultsmentioning
confidence: 99%
“…Since the grating crosssection is no longer determined by the dopant concentration, more elaborate fiber grating designs are possible: e. g. grating structures within the cladding or highly localized intracore modifications. Especially the latter enable new grating designs that tap the huge potential of higher-order fiber modes [166,167]. Specially polarized feedback can be obtained, e. g. a fully radially polarized beam [168].…”
Section: Discussionmentioning
confidence: 99%
“…Among these fibers, 2D SC-PBGF [21] and Bragg fibers [24] are two possible options and, in the second case, the classical design has been recently revisited so as to improve the transmission properties of the fiber. More precisely, it has been proposed by our group to replace the high-index rings of classical Bragg fibers by discontinuous rings made of high index rods.…”
Section: Introductionmentioning
confidence: 99%