Abstract
We present a systematic treatment of higher-order modes of vacuum-clad ultrathin optical fibers. We show that, for a given fiber, the higher-order modes have larger penetration lengths, larger effective mode radii, and larger fractional powers outside the fiber than the fundamental mode. We calculate, both analytically and numerically, the Poynting vector, propagating power, energy, angular momentum, and helicity (or chirality) of the guided light. The axial and azimuthal components of the Poynting vector can be negative with respect to the direction of propagation and the direction of phase circulation, respectively, depending on the position, the mode type, and the fiber parameters. The orbital and spin parts of the Poynting vector may also have opposite signs in some regions of space. We show that the angular momentum per photon decreases with increasing fiber radius and increases with increasing azimuthal mode order. The orbital part of angular momentum of guided light depends not only on the phase gradient but also on the field polarization, and is positive with respect to the direction of the phase circulation axis. Meanwhile, depending on the mode type, the spin and surface parts of angular momentum and the helicity of the field can be negative with respect to the direction of the phase circulation axis.
Highlights
Near-field optics using optical fibers is currently a highly active and productive area of research that has implications for optical communication, sensing, computing, and even quantum information
We find that the signs of the spin and surface parts of the transverse angular momentum density of the fundamental and higher-order modes depend on the direction of propagation
We have presented a systematic treatment of higher-order modes of vacuum-clad ultrathin optical fibers
Summary
Near-field optics using optical fibers is currently a highly active and productive area of research that has implications for optical communication, sensing, computing, and even quantum information. In a vacuum-clad nanofiber, the guided field penetrates an appreciable distance into the surrounding medium and appears as an evanescent wave carrying a significant fraction of the power and having a complex polarization pattern [5,6,7]. These fibers offer high transmission and strong confinement of guided light in the transverse plane of the fiber. In order to focus on the underlying physics of guided light in higher-order modes, we put the lengthy mathematical expressions for the mode functions and some analytical results in the appendixes
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