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b The constant electric field mode field emission plot.
The mode field was at the waterside of Taiwan MingDao University.
The numerator is the normalization factor of the nanocavity mode field.
This can be exploited tomographically, since TE210 mode field pattern penetrates less radially inwards than the TE110 mode.
Figure 4b shows that the constant electric field mode field emission characteristics in 1 × 10−3 Pa vacuum ambient.
The fundamental mode field profile of the proposed PCF for 50%, 655 %and80%0 % core porosities are shown in Fig. 2.
The physical explanation behind this phenomenon can be explained by the mode field profiles in Fig. 2.
Numerical results show that the mode field would exhibit a strong evanescent wave for TM mode in case the core layers are not many enough, even the TE mode field is well confined in the expanded core region.
The mode field area can be obtained in tapered region using a full vectorial H field technique.
The thermally expanded core technique can control the dopant concentration of the signal fiber, which can realize mode field match between the mode field sizes of the signal fiber and the output fiber.
Low transmission loss is realized by extending the mode field to the air holes adjacent to the solid material.
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