Multi-helical PCF and OAM

The study of electromagnetic wave propagation in helical structures began in earnest in the 1940s, with the invention of the travelling-wave tube amplifier. In this device a microwave signal is guided along a helical wire that spirals around an axially propagating electron beam [Kompfner (1947)]. Since the physical distance over which the spiralling microwave signal travels is longer than the distance directly along the axis, its group and phase velocities are both effectively reduced. By appropriate design the velocity difference between the two waves can be adjusted, permitting the microwave signal to be amplified with power from the electron beam. In a similar manner, the geometrical stretching of the cladding structure in a t-PCF causes the effective optical path-length along the axis, and thus the effective refractive index, to increase topologically with radius ρ following the relationship n_eff(ρ) = n₀(1 + α²ρ²)^0.5 where n₀ is the index in the untwisted case and α the twist rate in rad/m.

This topological effect makes it possible for example to phase-match light guided in a central solid glass core (modal index nc) to the fundamental space-filling mode in the cladding (phase index nSM in the untwisted fibre) with the result that light can leak out into cladding modes at certain wavelengths. This results in a series of dips in the transmission spectrum, caused by anti-crossings between the core mode and leaky ring-shaped cladding modes carrying orbital angular momentum (OAM), each dip corresponding to a different OAM order [Wong (2012)]. Since the cladding light is diverted by the hollow channels into a spiral path, the azimuthal component of its wavevector must take values that yield a round-trip phase advance that is an integer multiple  of 2π, where  is the OAM order. This leads to a resonance condition that yields remarkably good agreement with experimental measurements, showing in particular that the dip wavelengths scale linearly with the twist rate. We have used the twist and strain sensitivity of these dips to construct an all-optical twist-strain transducer [Xi (2013)].

Understanding the physics of light propagation in t-PCF is quite challenging, because the natural coordinate system—helicoidal—is non-orthogonal. This led us to introduce a new concept: helical Bloch waves. The optical Bloch waves of any untwisted periodic structure are mathematically described by the product of a periodic function (with periodicities that match the structure) and a term representing the phase progression of the Bloch wave [Russell (1986)]. A convenient physical picture for the modes guided in a t-PCF can be constructed by generalising Bloch's theorem so that the azimuthally periodic function follows the twist. At any given value of z, the periodic function will repeat at angular intervals 360°/N, where N is the number of times the structure repeats over one complete revolution. The Bloch waves can then be calculated analytically using an expansion in terms of azimuthal harmonics of OAM order. Substituting this field Ansatz into Maxwell's equations allows the dispersion relation to be derived and the properties of the modes to be investigated [Xi (2014)]. To explore the properties of helical Bloch waves, we fabricated a t-PCF with a ring of six solid glass "satellite" cores around its axis. This structure supports 6 non-degenerate helical Bloch modes with different values of orbital angular momentum, in both left and right circularly polarised states [Russell (2017)]. To determine the OAM order of the modes guided through the t-PCF, the output was superimposed on to a divergent Gaussian beam and the resulting fringe pattern imaged using a CCD camera. The single- and double-spiral interference patterns below confirm that the fibre generates optical vortices and preserves the magnitude and sign of the OAM for all four modes. Similar experiments carried out at multiple wavelengths and for fibres up to 50 m long have confirmed that the t-PCFs preserve the magnitude and sign of the OAM.

We have discovered a new mechanism of light guidance, based on a t-PCF with no core [Beravat (2016)]. Cleaving the fibre and examining its cross-section reveals a complete absence of any structure at which light could be trapped. Nevertheless it supports a guided mode: the helical twist creates a topological channel within light is robustly trapped. This arises from the quadratic increase in optical path length with radius (see "Topology"), which produces a radial gradient in axial refractive index, creating a potential well within which light is confined by photonic bandgap effects. Using mathematical tools from general relativity [Russell (1999)], we have shown that the geodesics of the light follow closed spiral paths within the topological channel, forming modes that carry OAM. The effective area of these modes decreases with twist rate α, so that by varying the twist rate along the fibre, it would be possible to create fibres whose mode-field diameter changes with position. Unlike in conventional index-guiding fibres, where the guided mode shifts towards the outside of the bend ("normal cornering"), this highly unusual mode shifts inwards towards the bend ("anomalous cornering"). Hamiltonian optics shows that the mode may be viewed as having negative effective mass (caused by the opposite sign of the dispersion surface curvature), so that it moves in the opposite direction when subject to bend forces.