Boris T. Kuhlmey1,2,
Ross C. McPhedran2 and C. Martijn de Sterke2
1 School of Physics, University of Sydney, NSW
2006, Australia
2 Institut Fresnel, Unité Mixte de Recherche du CNRS 6133, Faculté des Sciences et Techniques de Saint Jérôme, 13397 Marseille Cedex 20, France
Optics Letters 27, pp.
1684-1686 (2002)
©2002 Optical
Society of America
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FIG. 1:
Im(neff) as a function of wavelength/pitch, for a
structure of 8 rings of holes in silica at a wavelength of l =
1.55µm for several diameter on pitch ratios. Im(neff)
decreases monotonically with increasing d/L, as this parameter takes
the values 0.40 (1), 0.41, 0.42, 0.43, 0.45, 0.46, 0.48 0.49, 0.50, 0.55,
0.60, 0.65, 0.70, 0.75 (14). |
FIG.2:
Variation of different physical quantities during the transition, for a MOF with d/L = 0.55 used at l = 1.55 µm. Curves
(1) to (3) are Im(neff)
for 4, 8 and 10 rings, curves 4 to 7 are Q , Reff/L ,
Aeff/L2 and M as defined in the text, for 8 rings. The points (a-d) indicate
the position of the field plots of Fig. 3. |
|
FIG. 3: Density plots of the real part of the z
component of the Poynting vector of
the second mode, for four values of the pitch around the localization
transition, for a structure of 8 rings of holes with a diameter on pitch
ratio of d/L =0.55. (a): cladding filling state (l/L
= 0.81), (b,c):
transition states (b: l/L =
0.599, c: l/L = 0.537), (d) localized state l/L =0.445. The corresponding points are marked on Fig.
2. |
|
FIG. 4: Phase diagram of
the second mode. The different curves
correspond to different definitions of the transition point. In the
lower region the second mode is confined and the fiber is therefore dual
moded. The dashed vertical line shows the approximation to the limit of the
endlessly single mode regime. |
Fig. 1 ©
2002 Optical Society of America, Fig. 2-4 in
their color versions © 2002 by the authors. All rights reserved. Please feel
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