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Radiation mode
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For an [[optical fiber]] or [[waveguide]], a '''radiation mode''' or '''unbound mode''' is a mode which is not confined by the fiber core. Such a mode has fields that are transversely oscillatory everywhere external to the waveguide, and exists even at the limit of zero [[wavelength]]. Specifically, a radiation mode is one for which :<math>\beta = \sqrt{n^2(a) k^2 -(l/a)^2}</math> where ''Ξ²'' is the imaginary part of the axial [[propagation constant]], integer ''l'' is the azimuthal index of the mode, ''n''(''r'') is the [[refractive index]] at radius ''r'', ''a'' is the [[Fiber_optics#Principle_of_operation|core]] radius, and ''k'' is the free-space wave number, ''k'' = 2Ο/''Ξ»'', where ''Ξ»'' is the wavelength. Radiation modes correspond to [[refracted ray]]s in the terminology of [[geometric optics]].
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