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The effective mode area of the structure was calculated and compared with the mode area of conventional PCF's.
Here, we demonstrate mid-infrared (4 15 µm) plasmons in graphene nanostructures with dimensions as small as 50 nm (with a mode area of ∼1 × 10−3 µm2).
The single-mode large mode area of 100 12,000 μm2 could be achieved in the fiber.
According to simulation effective mode area of 1798 μm2 is achieved at an operating wavelength of 1.064 μm when no lower index rod is used.
We experimentally and numerically demonstrated that the tuning range can be increased by tailoring the effective mode area of the SRR and enhancing the interaction with graphene.
We numerically demonstrate propagation of 55.5-kW peak power, 1550-nm wavelength, 100-fs duration laser pulse through fundamental mode of 4-m long fiber having mode area of 1900 μm2.
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Dependence of effective mode area on the pitch and radius of high index rods are studied.
The designed fiber has effective mode areas of 16.04 μm2 and 16.06 μm2 for x-and y-polarization modes, respectively, at a wavelength of 1550 nm.
The geometric dependence of the mode characteristics of this structure is analyzed in detail, showing strong confinement and low loss with propagation lengths exceeding 14 mm at normalized mode areas of 1.72 × 10−2.
We evaluated the mode areas of various air gap widths for both substrate thicknesses, as shown in Figure 3.
Hence, in a size distribution, Jorgensen et al. (2002) reasoned that daughter cells would occupy the "left-of-mode" area of a cell size histogram of asynchronously dividing cells.
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