Abstract:We review our recent progress in the development of lead silicate glass fibers with high nonlinearity and tailored near-zero dispersion at telecommunication wavelengths, encompassing holey, all-solid microstructured and W-type fiber designs. The fabrication techniques and relative merits of each fiber design are described in detail. The optical properties of the fabricated fibers are assessed both experimentally and through accurate numerical simulations. The significant potential of lead silicate highly nonli… Show more
“…The nonlinear refractive index n 2 of the core and the cladding glasses are 41ϫ 10 −20 m 2 / W and 22ϫ 10 −20 m 2 / W at 1.55 m, respectively. 13 The effective nonlinearity ␥ ͑=2 n 2 / ͑ A ef f ͒͒ at 1.55 m of the fiber was therefore estimated to be 225 W −1 km −1 , which is 225 times higher than that of the conventional silica fiber ͑SMF28͒. The propagation loss in the fiber core was measured to be 5 dB/m at 1550 nm using cutback method.…”
Section: Lead Silicate Glass Microsphere Resonators With Absorption-lmentioning
We report the fabrication and characterization of a lead-silicate glass microsphere resonator. We show that at the wavelengths near 1555 nm high Q modes can be efficiently excited from a 109 μm diameter lead-silicate glass microsphere via evanescent coupling using a tapered silica fiber with a waist diameter of 2 μm. Resonances with Q-factors as high as 0.9×107 were observed. This is very close to the theoretical material-limited Q-factor and is the highest Q-factor reported so far from a nonlinear glass microsphere.
“…The nonlinear refractive index n 2 of the core and the cladding glasses are 41ϫ 10 −20 m 2 / W and 22ϫ 10 −20 m 2 / W at 1.55 m, respectively. 13 The effective nonlinearity ␥ ͑=2 n 2 / ͑ A ef f ͒͒ at 1.55 m of the fiber was therefore estimated to be 225 W −1 km −1 , which is 225 times higher than that of the conventional silica fiber ͑SMF28͒. The propagation loss in the fiber core was measured to be 5 dB/m at 1550 nm using cutback method.…”
Section: Lead Silicate Glass Microsphere Resonators With Absorption-lmentioning
We report the fabrication and characterization of a lead-silicate glass microsphere resonator. We show that at the wavelengths near 1555 nm high Q modes can be efficiently excited from a 109 μm diameter lead-silicate glass microsphere via evanescent coupling using a tapered silica fiber with a waist diameter of 2 μm. Resonances with Q-factors as high as 0.9×107 were observed. This is very close to the theoretical material-limited Q-factor and is the highest Q-factor reported so far from a nonlinear glass microsphere.
“…4. An asymmetric arc-fusion splicing configuration [20,27], i.e., moving the heating element along the silica fiber from the gap (see Fig. 10(a)), was adopted to splice the borosilicate dual-ASC fiber with a commercial high-NA small core silica fiber (Nufern UHNA4, NA=0.35).…”
Section: Connecting Of Dual-asc Fiber To All-solid Silica Fiber By Armentioning
confidence: 99%
“…The dual-core fiber preform was made by extrusion under a temperature around 600 o C. The extrusion method is a well-developed method for making non-silica glass (or so-called soft glass) HF [19] above the glass softening temperature, which is typically below 800 °C. It is very powerful in directly making microstructured preforms with glass features even as small as 7 µm [20]. But due to the lack of suitable die materials capable of working at temperatures above 1000 °C and at high pressures of 0.1-10 kN/cm 2 , the glass extrusion technology has not shown any success in making preforms using glasses with high softening temperature such as silica.…”
We demonstrate the fabrication of a novel type of optical fibers with multiple parallel airsuspended cores by the sheet-stacking method. Using this technique we have constructed optical fibers with up to 10 parallel micron-size suspended cores. No extra scattering loss from the fabrication process was observed in a fabricated dual air-suspended core fiber. The sheetstacking method opens the way towards using a wide range of optical glasses for manufacturing multiple parallel suspended-core specialty optical fibers with novel optical functionalities such as dispersion tunability. Fusion splicing has also been successfully used to connect such a multiple core fiber with a conventional silica fiber.
“…By choosing a glass with lower material loss than N-BK7, e.g., silica as the core, multiple ASC fibres with much lower loss can be fabricated. A commercial fusion splicer was used to splice the dual-ASC fibre to a commercial high NA silica fibre (Nufern UHNA4, NA=0.35) by the offset fusion splicing approach [5], see Fig. 3(c).…”
Section: Fabrication and Characterization Of Dual-asc Fibrementioning
Abstract:We demonstrate using a sheet-stacking method to fabricate nanomechanical optical fibres with long and thin spokes. This approach shows great advantage for manufacturing complex multi-material speciality optical fibres with novel photonic and nanomechanical functionalities.
2013 Optical Society of AmericaOCIS codes: 060.2280 Fiber design and fabrication; 060.4005 Microstructured fibers
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