Photonic Weyl Points

Weyl points are band degeneracies that occur in the momentum space of 3D periodic materials and are enforced by an integer topological charge known as the Chern number. Weyl materials are associated with a range of interesting physical phenomena directly connected to their non-trivial topological charge. For example, due to the bulk-boundary correspondence principle, these materials exhibit unique surface states whose dispersion does not span the entire Brillouin zone but instead terminates at Weyl points with opposite charges. Weyl points can carry arbitrary integer charges, and those with a charge greater than one are known to occur in the presence of certain non-symmorphic symmetries found in chiral structures.

In the photonic domain, Weyl points may enable the creation of large-volume single-mode lasing devices. Furthermore, they can mediate unique long-range interactions between embedded quantum emitters. However, due to fabrication challenges, experimental realization of photonic Weyl points at near-IR frequencies has remained elusive.

We experimentally observed charge-2 Weyl points at mid- and near-infrared wavelengths in a chiral woodpile photonic crystal. This photonic crystal was micro-printed using a low refractive index material via two-photon polymerization and was characterized using FTIR spectroscopy. Additionally, we experimentally demonstrated that when the protective symmetry is broken, a charge-2 Weyl point splits into charge-1 Weyl points. Importantly, this splitting can be restricted to high-symmetry directions in momentum space, resulting in unprecedented control over the location of Weyl points.

Recently, we also explored the consequences of placing Weyl points on non-orientable manifolds.

Observation of a charge-2 Weyl point (above) in a three-dimensional chiral woodpile photonic crystal (below)

FDTD simulation of corner states in a 2D higher-order topological photonic crystal

Theory of Topological Insulators

Topological insulators are a fascinating class of materials that have recently emerged as a prominent subject of study in condensed matter physics. They represent new phases of matter that possess unique properties at their surfaces, hinges, edges or corners, distinct from those in the bulk. This results ultimately from the underlying non-trivial topology of the electronic band structure rather than any specific material property. In the last decade, many of these topological ideas have been extended to other systems that host wave-like excitations (such as light propagating in photonic crystals and sound waves in acoustic metamaterials). I am broadly interested in extending the theory of topological phases to photonic crystals and quasicrystals, and finding novel occurrences of topology in condensed matter physics.

In our recent work, we developed a complete classification of topological phases in photonic crystals under crystalline symmetries and proposed a design strategy based on this classification. Using the invariants developed there, we also showed the existence of weak topological phases within Chern insulators and strong topological insulators.

Localization in Photonic Quasicrystals

Anderson localization is the ubiquitous phenomenon involving the localization of waves and the cessation of wave transport in disordered media. In three dimensions, a sharp transition separates the extended and localized regimes as a function of the strength of disorder. A similar transition can also occur in one-dimensional systems when random disorder is replaced by quasiperiodicity.

In photonics, the localization of light is particularly interesting, as it finds applications in various areas, including random nanolasing, the formation of photonic stop bands, the creation of high-Q nanocavities, and the reduction of crosstalk between components in telecommunication devices.

In our recent work, we demonstrated localization/delocalization transitions in one-dimensional photonic quasicrystals comprising alternating layers of silicon and silica. In particular, we observed a surprising and counterintuitive phenomenon within this system: a second transition of certain localized states to a delocalized regime upon increasing quasiperiodic disorder. The degree of localization of photonic states has a measurable effect on the transmission of light through these structures, enabling a clear experimental demonstration of these transitions. This result advances our understanding of localization physics in complex systems and the impact of quasiperiodicity on light transport in photonic devices.

A one-dimensional photonic quasicrystal fabricated using chemical vapour deposition

Point-defect localized bound state in the continuum in a two-dimensional photonic crystal

Bound States in the Continuum

Photonic crystals are lattices of dielectric materials, such as glasses or semiconductors, that enable fine control over the properties of light. They are known to possess band gaps, making them act as perfect mirrors for a range of frequencies. These band gaps have traditionally been utilized for trapping light to defects, creating one-dimensional waveguides and zero-dimensional nanocavities. However, the reliance on a band gap limits the choice of materials to those with a sufficiently high refractive index.

In this work, we propose a new method for trapping light within nanocavities embedded in two-dimensional photonic crystals that lack band gaps. We demonstrate that it is possible to engineer the photonic crystal and nanocavity such that a symmetry mismatch with the photonic crystal's modes prohibits light within the cavity from leaking away. This state of light is an example of a "bound state in the continuum", which is a localized state that co-exists with a continuum of propagating states of the photonic crystal. Furthermore, this state can be utilized to create slow-light modes in complex photonic crystal fibers. Our work enables the construction of nanocavities within photonic crystals made of versatile, low-index materials like glasses and polymers.

We also showed the existence of bound states in the continuum of a photonic crystal slab that lie in a "symmetry bandgap" of  a 3D photonic crystal environment within which the slab is embedded.